Compounds from BeBr to ZrCl2

Landolt-Börnstein Numerical Data and Functional Relationships in Science and Technology New Series / Editor in Chief: W. Martienssen

Group IV: Physical Chemistry Volume 19

Thermodynamic Properties of Inorganic Materials compiled by SGTE Subvolume A Pure Substances Heat Capacities, Enthalpies, Entropies and Gibbs Energies, Phase Transition Data

Part 2 Compounds from BeBr to ZrCl2 Editor Lehrstuhl für Theoretische Hüttenkunde, Rheinisch-Westfälische Technische Hochschule Aachen Authors Scientific Group Thermodata Europe (SGTE)

13

ISSN 0942-7996 (Physical Chemistry) ISBN 3-540-65344-9 Springer-Verlag Berlin Heidelberg New York Library of Congress Cataloging in Publication Data Zahlenwerte und Funktionen aus Naturwissenschaften und Technik, Neue Serie Editor in Chief: W. Martienssen Vol. IV/19A2: Editor: Lehrstuhl für Theoretische Hüttenkunde, Rheinisch-Westfälische Technische Hochschule Aachen At head of title: Landolt-Börnstein. Added t.p.: Numerical data and functional relationships in science and technology. Tables chiefly in English. Intended to supersede the Physikalisch-chemische Tabellen by H. Landolt and R. Börnstein of which the 6th ed. began publication in 1950 under title: Zahlenwerte und Funktionen aus Physik, Chemie, Astronomie, Geophysik und Technik. Vols. published after v. 1 of group I have imprint: Berlin, New York, Springer-Verlag Includes bibliographies. 1. Physics--Tables. 2. Chemistry--Tables. 3. Engineering--Tables. I. Börnstein, R. (Richard), 1852-1913. II. Landolt, H. (Hans), 1831-1910. III. Physikalisch-chemische Tabellen. IV. Title: Numerical data and functional relationships in science and technology. QC61.23 502'.12 62-53136 This work is subject to copyright. All rights are reserved, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilm or in other ways, and storage in data banks. Duplication of this publication or parts thereof is permitted only under the provisions of the German Copyright Law of September 9, 1965, in its current version, and permission for use must always be obtained from SpringerVerlag. Violations are liable for prosecution act under German Copyright Law. © Springer-Verlag Berlin Heidelberg 1999 Printed in Germany The use of general descriptive names, registered names, trademarks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. Product Liability: The data and other information in this handbook have been carefully extracted and evaluated by experts from the original literature. Furthermore, they have been checked for correctness by authors and the editorial staff before printing. Nevertheless, the publisher can give no guarantee for the correctness of the data and information provided. In any individual case of application, the respective user must check the correctness by consulting other relevant sources of information. Cover layout: Erich Kirchner, Heidelberg Typesetting: Authors and Redaktion Landolt-Börnstein, Darmstadt Printing: Computer to plate, Mercedes-Druck, Berlin Binding: Lüderitz & Bauer, Berlin SPIN: 10705961

63/3020 - 5 4 3 2 1 0 – Printed on acid-free paper

Editors I. Hurtado and D. Neuschütz Lehrstuhl für Theoretische Hüttenkunde Rheinisch-Westfälische Technische Hochschule Aachen D-52056 Aachen, Germany http://www.lth.rwth-aachen.de/

Authors Scientific Group Thermodata Europe (SGTE) Chairman: P.J. Spencer Grenoble Campus 1001 Avenue Centrale, BP 66 F-38402 Saint Martin d'Hères, France http://www.sgte.org/

Member Organisations of SGTE: The present series of books is the result of a collective work carried out during many years by many individuals. Since a complete list of all contributors is an impossible task, only a contact person is mentioned under each member organisation. AEA Technology plc Materials and Chemical Process Assessment P.K. Mason 220, Harwell Laboratory, Didcot, Oxfordshire, United Kingdom, OX11 0RA http://www.aeat.co.uk/mcpa/ GTT Technologies Gesellschaft für Technische Thermochemie und -physik mbH K. Hack Kaiserstraße 100 D-52134 Herzogenrath, Germany http://gttserv.lth.rwth-aachen.de/gtt/ Institut National Polytechnique de Grenoble Laboratoire de Thermodynamique et Physico-Chimie Métallurgiques I. Ansara F-38402 Saint Martin d'Hères, France http://www.inpg.fr/LTPCM/ IRSID Department of Physical Chemistry J. Lehmann Voie Romaine - BP 30320 F-57283 Maizières-lès-Metz, France

Max-Planck-Institut für Metallforschung und Institut für Nichtmetallische Anorganische Materialen der Universität Stuttgart Pulvermetallurgisches Laboratorium H.J. Seifert Heisenbergstraße 5 D-70569 Stuttgart, Germany http://wwwmf.mpi-stuttgart.mpg.de/abteilungen/aldinger/aldinger.html National Physical Laboratory Centre for Materials Measurement and Technology A.T. Dinsdale Queens Road, Teddington, Middlesex, United Kingdom, TW11 0LW http://www.npl.co.uk/npl/cmmt/mtdata/mts.htm Rheinisch-Westfälische Technische Hochschule Aachen Lehrstuhl für Theoretische Hüttenkunde E. Münstermann D-52056 Aachen, Germany http://www.lth.rwth-aachen.de/ Royal Institute of Technology Department of Materials Science and Engineering J. Ågren S-10044 Stockholm, Sweden http://www.met.kth.se/tc/ Thermo-Calc AB B. Sundman Björnnägen 21 S-11347 Stockholm, Sweden http://www.thermocalc.se/ THERMODATA B. Cheynet Grenoble Campus 1001 Avenue Centrale, BP 66 F-38402 Saint Martin d'Hères, France http://www.thermodata.asso.fr/ Université Paris-Sud XI Faculté de Pharmacie Laboratoire de Chimie Physique Minérale et Bioinorganique, EA 401 Y. Feutelais 5 rue J.B. Clément F-92296 Châtenay-Malabry, France http://www.u-psud.fr/

In preparing the data for publication in this Series, the editors has been assisted particularly by: A.T. Dinsdale (Data Manager for Elements), I. Ansara (Data Manager for Pure Substances), B. Sundman (Data Manager for Solutions), J.A.J. Robinson (SGTETab software).

Preface

Thermodynamic data for inorganic materials are fundamental for the optimisation of existing process parameters and for investigating suitable parameters for carrying out potential new processes. With the aid of such data, considerable time and costs can be saved by calculating the conditions necessary to produce a material of the required composition and specified purity, with a minimum usage of energy and input materials and with a minimum release of harmful substances to the environment. The reliability of such calculations depends, of course, on the accuracy of the thermodynamic data used and one difficulty facing the user of published thermodynamic tables has been the wide selection of such compilations available. A further difficulty in using such tabulations is the need to maintain compatibility if it is found necessary to use values from more than one compilation. Different standard states, different tabulated functions and even different values for the same substance can quickly lead to uncertainty and errors in application of the numbers. Nearly all currently available compilations of thermodynamic data relate to pure substances. Very few publications of solution properties for inorganic materials exist. There are very, very few processes however, for which the reactants and products can be regarded as simple stoichiometric compounds. Even very small amounts of dissolved gases or other impurities in a product material can seriously impair its properties. On the other hand, many materials in use today are comprised of several deliberately alloyed constituents to achieve desired mechanical and physical properties. Only by including the thermodynamic solution properties of the dissolved species can full account be taken of reactions such as those between an alloy melt and a slag phase, or those involved in forming precipitated phases in a multicomponent alloy, or in vapour deposition of complex coatings on an alloy substrate, etc.. For almost 20 years, members of SGTE have been working together to try to overcome some of these problems by together producing self-consistent and compatible thermodynamic datasets, not only for pure inorganic substances, but also for mixtures of substances in the form of alloys, slags, salt systems, aqueous solutions, etc. Major advantages of the SGTE data are their self-consistency, the fact that they are produced with careful attention to a well-defined quality procedure and that the expertise of SGTE members in various areas of inorganic chemistry and materials science (ferrous and non-ferrous metallurgy, ceramics, slags, nuclear, aqueous, etc.) allows review of the numbers by highly qualified scientists in the fields concerned. The SGTE evaluated data forming this series provide a self-consistent progression from elements and stoichiometric compounds (Volume A) to binary systems including solution phases (Volume B). The possibility to continue to ternary and multicomponent systems is also forseen. The data in the latter would be so presented as to correspond to potential application themes (steels, light alloys, nickel-base alloys, etc.). The fundamental equations used in evaluating the data are given in the introduction to the volumes and the models used in representing the data are described. Each book is accompanied by a CD-ROM allowing computer tabulation of any required function at any temperature, or for selected temperature ranges, for the substances or systems in that volume. Graphical representations are also possible, including phase diagrams for the systems. The first set of four books (subvolume A) will be accompanied by software which also allows calculation, tabulation and plotting of the thermodynamic properties of reaction of substances selected from any of the Parts 1 to 4.

Information on more comprehensive software, allowing complex equilibrium calculations involving not only pure substances, but also solution phases of different types, can be obtained from SGTE members. A list of the SGTE membership is presented in the cover pages of this Volume. In presenting the data in this Series, SGTE would like to give sincere acknowledgement to the contributions of a number of scientists whose efforts have been invaluable in establishing the present SGTE databases. The names are as follows: Prof. E. Bonnier, Dr. M.H. Rand, Prof. O. Kubaschewski, Dr. M. Olette, Prof. O. Knacke, Prof. M. Hillert, Prof. I. Barin, Dr. H.L. Lukas, Dr. C. Bernard, Dr. T.I. Barry, Dr. T.G. Chart and Dr. G.P. Jones. The skilled evaluations originating from members of THERMOCENTER, Russian Academy of Science, are also gratefully acknowledged.

Dr. P.J. Spencer Chairman of SGTE

Ithaca, August 1999

Survey of volume IV/19 Thermodynamic Properties of Inorganic Materials compiled by SGTE Pure Substances

Subvolume A

Elements and Compounds from AgBr to Ba3N2 Compounds from BeBr to ZrCl2

Part 1 Part 2

(tentative) Compounds from Cl3- to GeCompounds from H- to Te-

Part 3 Part 4

Binary Systems From Ag- to AuFrom B- to CoFrom Cr- to GeFrom Hf- to Y-

Ternary and multicomponent Systems (application oriented, i.e. Light Alloys, Solders, Steels,...)

Subvolume B Part 1 Part 2 Part 3 Part 4

Subvolume C

Introduction

XI

Introduction

The data presented in this series, dealing with pure inorganic substances (IV/19A), binary systems (IV/19B) and ternary and multicomponent systems (IV/19C) have been evaluated and compiled by SGTE. SGTE is a consortium of European laboratories working together to develop high quality thermodynamic databases for a wide variety of inorganic and metallurgical systems [87Ans, 91Din]. The SGTE element data [91Din] conform to the 1990 International Temperature Scale and over the last years have formed the basis for most assessments of binary, ternary and higher order systems appearing in the open literature.

m o

Members of SGTE have played a principle role in promoting the concept of “computational thermochemistry“ as a time and cost-saving basis for guiding materials development and processing in many different areas of technology. At the same time, through organisation of workshops and participation in CODATA Task Groups, SGTE members have contributed significantly to the broader international effort to unify thermodynamic data and assessment methods. are

c . f

ftw o s The SGTE data can be obtained via members and their agents world-wide for use withFcommercially available software developed by some of the members, to enable users to undertake PDcalculations of S complex chemical equilibria efficiently and reliably. RT A of The SGTE Member organisations are (January 1999): n o i ers v France: - Institut National Polytechnique (LTPCM),eGrenoble mo - Association THERMODATA, Grenoble ad g - IRSID, Maizières-lès-Metz sin u - Université de Paris Sud (LCP) d ifie d mo Technische Hochschule (LTH), Aachen Germany: - Rheinisch-Westfälische n ee - MPI fürbMetallforschung (PML), Stuttgart s - GTT-Technologies, Aachen a Fh D sP i h Sweden: - Royal Institute of Technology (MSE), Stockholm T

d p

s t r a

. w

w w

- Thermo-Calc AB, Stockholm

United Kingdom:

Landolt-Börnstein New Series IV/19A

-National Physical Laboratory (CMMT), Teddington -AEA Technology plc, Harwell

SGTE

XII

Introduction

1 Basic equations and functions used

1.1 Heat capacity The heat capacity of the elements and the pure substances in a defined state is represented by a power series of the form C p = a + b ⋅ T + c ⋅ T 2 + d ⋅ T −2

(1)

It is often necessary to use several temperature ranges, without discontinuities, in order to represent the assessed Cp values as accurately as possible. Plots of Cp are presented for each substance, whilst calculated values for selected temperatures or temperature intervals can be obtained using the software accompanying the volumes. It can sometimes be necessary to extrapolate the thermodynamic properties of the solid phases of an element beyond the temperature ranges where the phases are stable. In the SGTE treatment of such data for the liquid phase, it has been assumed that the heat capacity of the liquid should approach that of the SER-phase (Standard Element Reference-phase, which is usually the phase stable at 298.15 K) and similarly, that the heat capacity of all solid phases above the melting temperature should approach that of the liquid. This excludes a proper treatment of glass transformations, but represents a pragmatic solution to the difficulties associated with necessary extrapolations and removes the possibility of phases becoming incorrectly stable at high or low temperatures. The resulting additional T 7 and T -9 temperature terms used are presented in equation (7) below. Alternative extrapolation methods have been used for some elements and new methods are being reviewed for incorporation into the SGTE databases shortly [95Sun].

1.2. Enthalpies of formation and transition and standard entropy The enthalpy of formation at 298.15 K, ( ∆ f H 0 (298 K), and the standard entropy at 298.15 K, S 0 (298 K), are presented for each substance, together with the enthalpies and temperatures of polymorphic transformations, ∆ trs H and Ttrs. A reference pressure of 100 kPa is used. In addition, the value of H(298.15 K)-H(0 K) is given when available.

1.3. Gibbs energy As most thermodynamic calculations relating to reactions and phase equilibria involving inorganic materials are made assuming constant temperature and pressure, the Gibbs energy is often the most suitable function to describe the thermodynamic properties of the substances involved. The molar Gibbs energy of a pure element i, 0 Gi (T) , referred to the enthalpy of its standard reference state at 298.15 K,

0

H i (298.15K) , is denoted by GHSERi. This quantity is described as a function of

temperature by the following equation: SGTE

Landolt-Börnstein New Series IV/19A

Introduction

XIII

GHSER i = 0 Gi (T)− 0 H i (298K ) = a + b ⋅ T + c ⋅ T ⋅ lnT + d ⋅ T 2 + e ⋅ T 3 + f ⋅ T −1

(2)

The same basic equation is also used to describe the Gibbs energy of pure stoichiometric substances. N.B. It is important to recognise that GHSER (normally shortened to G) is not the Gibbs energy of formation at a particular temperature. ∆ f G includes contributions from the entropy of the elements at T and changes in the enthalpy of the elements between 298.15 K and T. From the Gibbs energy, all important thermodynamic properties can be calculated by combining appropriate partial derivatives. In particular the first and second derivatives of equation (2) with respect to temperature are related to the absolute entropy and heat capacity of the substance at the temperature concerned. Experimental values for heat capacity can thus be directly correlated with the coefficients c, d, e and f. S = − b − c − c ⋅ lnT − 2d ⋅ T − 3e ⋅ T 2 + f ⋅ T −2 Using

G = H −T ⋅S

(3) (4)

H = a − c ⋅ T − d ⋅ T 2 − 2e ⋅ T 3 + 2f ⋅ T −1

(5)

C p = −c − 2d ⋅ T − 6e ⋅ T 2 − 2f ⋅ T −2

(6)

Taking into account the need to extrapolate the data for a phase to metastable ranges, as discussed in Section 1.1., equation (2) is modified to give: GHSER i = 0 Gi (T)− 0 H i (298K ) = a + b ⋅ T + c ⋅ T ⋅ lnT + d ⋅ T 2 + e ⋅ T 3 + f ⋅ T −1 + g ⋅ T 7 + h ⋅ T −9

(7)

1.3.1. Influence of magnetic behaviour For substances which display a magnetic ordering (e.g. the elements Cr, Fe, Ni, Mn), the term GHSER is considered for a paramagnetic state and the magnetic contribution is treated explicitly. Thus an additional term is added to the molar Gibbs energy of the magnetic phase. This is equal to: G mag = RTln(β + 1) ⋅ f( τ)

(8)

where τ is T/Tc, Tc being the critical temperature for magnetic ordering and ß the average magnetic moment per atom expressed in Bohr magnetons. The function f(τ) is given as: τ < 1:

f(τ) = 1-[79 τ-1/140p+(474/497)(1/p-1)(τ 3/6+ τ9/135+ τ 15/600)]/A

τ > 1:

f(τ) = -[ τ /10+ τ /315+ τ /1500]/A

(10)

A = 518/1125+(11692/15975)(1/p-1)

(11)

-5

-15

-25

(9)

with

These equations were derived by Hillert et al. [78Hil] from an expression of the magnetic heat capacity, C pmag , proposed by Inden [81Ind]. The value of p depends on the structure. For example, p has a value of 0.28 for fcc and hcp metals and 0.40 for bcc metals [81Ind]. Gibbs energy equations for the pure elements, of the form given in equation (7), have been published previously as the SGTE data for the pure elements by Dinsdale [91Din].

Landolt-Börnstein New Series IV/19A

SGTE

XIV

Introduction

1.4 Gibbs energy of formation 1.4.1 Binary compounds The Gibbs energy of formation of a binary compound AaBb is expressed as: GA a Bb − a⋅0 H A (298.15K) − b⋅0 H B (298.15K) = f(T )

(12)

The expression for f(T) is identical to that given by equation (7). Equation (12) can be transformed by applying equation (2) for each component f (T ) = GA

a Bb

= ∆ f GA The term ∆ f GA

a Bb

(T ) − a⋅0 GA (T ) − b⋅0 GB (T ) + a GHSERA + b GHSER B = a Bb

(T ) + a GHSERA + b GHSERB

(13)

(T ) is the Gibbs energy of formation of the compound referred to the stable elements

at temperature T. 1.4.2 Gaseous species An expression identical to equation (12) is used to describe the Gibbs energy of formation of gaseous species, with an additional term RT lnP, where P is the total pressure. The reference state for each vapour species is taken to be the pure component at 0.1 MPa pressure.

2 Definitions and reference information The definitions given here, which are relevant to the volumes of tabulated data and accompanying software, are intended to explain the meaning of words commonly used in metallurgical and inorganic thermochemistry; they are not necessarily generally used definitions in all cases. Atom An atom is the smallest possible state of division of an element. Component (see System) Compound A compound is composed of at least two different elements. The phase is not defined. A compound in crystalline form may be made up of individual molecules or it may have extended ionic, covalent or metallic bonding. For example the overall composition of rock salt is governed by the fact that there are equal numbers of Na+ and Cl - ions on two sublattices. The use of the word compound normally implies a stoichiometric composition (i.e. the amounts of the elements are in simple ratio). Element An element cannot be broken down to a simpler chemical form by non-nuclear processes. The phase is not defined and the element may be present as atoms or molecules, e.g. gaseous O, O2 and O3 are different molecular forms of the element oxygen. SGTE

Landolt-Börnstein New Series IV/19A

Introduction

XV

Equilibrium At chemical equilibrium the phases present, their composition and internal speciation is such as to minimise the Gibbs energy at a fixed pressure or the Helmholtz energy at fixed volume. When the Gibbs energy is minimum the chemical potentials (partial molar Gibbs energies with respect to composition) of the components are equalised throughout the system, i.e. in every phase. Thus equilibrium can be computed either by minimisation of Gibbs energy or equalisation of chemical potentials. Ion An ion is an atom or molecule carrying electric charge. Isomer Isomers are molecules with the same formula but different structures. SGTE distinguishes between isomers by appending a tag to the formula, e.g. C2Cl2H2_trans and C2Cl2H2_cis. Isotope Isotopes of the same element have the same atomic number but differing atomic weights. For most elements, and for most purposes, the differences in chemical behaviour are insignificant. Hydrogen is an exception and the SGTE substance database incorporates data for deuterium, tritium and some of their compounds using the symbols D and T. Model The word "model", as used in conjunction with the SGTE data, applies to any mathematical description of the properties of a phase, a unary or an interaction as a function of one or more variables such as temperature, pressure, composition and internal distribution of components. The mathematical model is strongly linked to the phase and takes account of structural features of phases for example multiple sublattices and solution on individual sublattices. Within a single phase the same model must be used to describe the mixing between all binary and, if necessary, higher order combinations of unaries. This entails that care must be taken when developing data for a multicomponent system that models and reference states are consistent. "Model" may also have a more restrictive definition in which the parameters in the mathematical description are given definite numerical values. Molecule A molecule is a chemically bonded group of similar or different atoms, eg Cl2 or NH3. The word molecule is most often used for species in the gas phase, but it can be used for species (q.v.) in other phases, including crystalline phases, provided the molecule behaves as a single entity. Phase A phase is chemically and structurally homogeneous and is distinguishable from other phases by its name, structure and properties (mechanical, physical and chemical). Crystalline phases have a definite periodic structure, often with sublattices. In order to define phases uniquely, phase names like fcc and alpha are insufficient. For this reason SGTE has coupled the Pearson symbol to the crystal class for metallic phases, e.g. Fe. Reference state Enthalpy data for all substances are ultimately referred to the enthalpy of the elements in their standard reference states. This corresponds to the stable phase at 1 atm. (101325 Pa) and 298.15 K. (Phosphorous, for which the red allotrope is more easy to prepare and define in a chemically pure form than is the stable white form, is an exception). Thus, for example, the enthalpy of liquid water is referred to gaseous O2 and H2, both at 101325 Pa, via the equation: H2 + 0.5 O2 = H2O Landolt-Börnstein New Series IV/19A

(14) SGTE

XVI

Introduction

However, the entropy and heat capacity of liquid water are properties of water itself. The enthalpy and entropy of liquid water are defined by: T ∫298.15 C p (H2O)dT

(15)

T ∫298.15 C p (H2O)/T dT

(16)

H(H2O) = ∆fH298.15(H2O) + S(H2O) = S298.15(H2O) +

Solution A solution is a homogeneous mixture within a single phase. Local ordering may be present. A phase that includes a variable proportion of unoccupied sites is also a solution but the vacancies do not constitute a component. The data for solutions are defined by reference to the unaries from which they are constituted using the model and data describing the ideal and non-ideal mixing between these unaries. Species A species is an atom, ion or molecule and corresponds to an identifiable constituent of a phase, for example a gaseous molecule or an ion occupying a sublattice. State of matter The states of matter relevant to these tables are solid, liquid and gas. Substance "Substance" denotes any quantity of material having a definite identity. Thus the term comprises anything from an atom or ion upwards. In the SGTE data presented here, a more restricted sense is implied, namely a unary, a stoichiometric compound or a pure gas. System and component A chemical system is defined by a set of chemical entities known as components. In the simplest case these are the elements comprising the system. However, they may also be compounds of these elements, in which case they may be fewer or, less commonly, greater in number than the number of elements. For the example of the three elements C, H and O, the number of components might be 1, ethanol; 2, ethanolwater; 3, C-H-O; or 4, methanol-ethanol-water-benzene, etc. Systems may be closed or open. In closed systems the total amount of the components is fixed, whereas in open systems the composition can adjust to meet some external constraint. Unary The word "unary" is used to define the constituents of a phase. For example in a liquid phase the unaries might be H2O and C2H5OH. The data for these unaries are those of the pure liquids. Unaries are not necessarily experimentally accessible. For example Ni is unstable but data for it are required to model the solution of nickel in the bcc phase of steels. Moreover, to meet the requirements of models for ionic phases with sublattices a unary may carry charge. For example the formation of an inverse spinel AB2O4 might be modelled by the mixing of the four unaries, A3+(A3+)2O4<spinel>, A3+(B2+)2O4<spinel>, B2+(A3+)2O4<spinel> and B2+(B2+)2O4<spinel> which respectively have charges of +1 -1, 0 and -2 only one of which, even in principle, could have an independent existence. Vacancies Sites in crystalline structures are not always 100% populated, indeed interstitial sites may have a very low occupancy. SGTE modelling considers the unoccupied sites as vacancies, which are denoted by Va.

SGTE

Landolt-Börnstein New Series IV/19A

Introduction

XVII

3 Content of the tables 3.1 Tabulated values The following standard format has been used to present the evaluated thermodynamic values for all inorganic substances: At the head of the page on the left hand side is the chemical formula and name for the substance concerned and on the right hand side a reference or references to the major source of the evaluated data contained in the table below. The table itself contains the following: T (Temperature in K) So (Standard entropy in J K-1 mol-1) - the entropy of the substance at 298.15 K and 100 kPa. H298-H0 (Enthalpy in J mol-1) - the difference in the enthalpy of the substance between 298.15 K and 0 K (when available) ∆f Ho (Standard enthalpy of formation in J mol-1) - the change in enthalpy resulting from the formation of the substance at 298.15K from the appropriate proportions of its pure elemental components in their standard reference states, also at 298.15K ∆f So (Standard entropy of formation in J K-1 mol-1) - the change in entropy resulting from the formation of the substance at 298.15 K from the appropriate proportions of its pure elemental components in their standard reference states, also at 298.15 K ∆f Go (Standard Gibbs energy of formation in J mol-1) - the change in Gibbs energy resulting from the formation of the substance at 298.15 K from the appropriate proportions of its pure elemental components in their standard reference states, also at 298.15 K ∆trs Ho (Enthalpy of transition in J mol-1) - the enthalpy difference between two different stable phases of the substance at the transition temperature corresponding to the value of T in the first column ∆trs So (Entropy of transition in J K-1 mol-1) - the entropy difference between two different stable phases of the substance at the transition temperature corresponding to the value of T in the first column type (nature of the transition) abbreviated information on the nature of the phase transition concerned S-S - solid/solid transition S-L - solid/liquid transition For the elements the information is more detailed including the name of the phases.

Landolt-Börnstein New Series IV/19A

SGTE

XVIII

Introduction

3.2 Figures There are generally two figures accompanying the tabulated values. These are - a plot of the heat capacity, Cp , (in J K-1 mol-1) as a function of temperature (K) for the complete range of temperature for which data are available. The plot comprises curves for the different phases of the substance if phase transitions occur in the temperature range concerned. - a plot of the enthalpy of formation, ∆fH , and Gibbs energy of formation, ∆fG , (in kJ mol-1 or MJ mol-1) as a function of temperature. Phase transitions in the substance and in the elemental components of the substance are reflected in the different curves. The maximum temperature may be limited by the maximum temperature of one of the component of the substance. For the elements in its reference state the second figure is replaced by a table with several properties, including a short version of the SGTE phase designation (i.e. A_MON_Pu instead of ALPHA_MONOCLINIC_Pu) the Strukturbericht, prototype, Pearson symbol and space group [86Mas, 91Din] the atomic number and atomic weight [96IUPAC, 97IUPAC]. The number in parentheses indicates the uncertainty in the last digit. the density [98Pre]

4 Accompanying software, SGTETab( for Windows)

INSTALL

SGTETab is a program for tabulating and plotting the thermodynamic properties for pure substances or a chemical reaction using data stored in the SGTE pure substance database. It has been designed for use under the Windows9x or Windows NT operating systems as a full Windows program providing dialogue boxes, menus and context sensitive help in order to guide the user to ask for the table or plot required. As a Windows program it provides printer support. On executing SGTETab first click the ∆H button which opens the tabulation window containing various simple dialogue boxes allowing you to define: -

the substance (in a compact way, e.g. Be6Li2O10 instead of Li2O.3B2O3) or equation the units of temperature, pressure and energy the thermodynamic function to be plotted the range of temperatures to be covered by the calculations the fixed pressure for the calculations the name of the file where tabulated results are to be saved

The substance or equation is defined using the standard chemical nomenclature for the element names, eg mixture of upper and lower case characters Ag, B, Na, AgCl, CaBr2. If the substance is entered without a phase identifier a crystalline state is assumed with no defined phase name. However if data for a particular phase are to be used, the phase name should be entered immediately after the substance within angular brackets e.g. C. If data for gaseous species are required the phase identifier g is used e.g. H2, CH2. Equations are entered with the list of reactants and products separated by an equals sign e.g.:

SGTE

Landolt-Börnstein New Series IV/19A

Introduction

XIX

Ca + Cl2 = CaCl2 The amount of each of the reactants or products could be a fraction or a non-integer if required e.g.: C +0.5O2 = CO Na + 1/2Cl2 = NaCl SGTETab also provides a facility to balance chemical equations automatically. e.g.: Fe2(SO4) 3 = Fe3O4 + SO2 + O2 will auto-balance to give the chemical equation: Fe2(SO4) 3 = 2/3Fe3O4 + 3SO2 +5/3O2 Both tabular and graphical output is provided on clicking the PLOT button. The graphical output may be minimised for comparison with other graphical output, saved on disk or printed out on a connected printer. Optionally the printed information may be sent to a file as specified in the results file dialogue box. By default SGTETAB assumes that the units of energy are joules, temperature in K and pressure in Pa but alternative units may be selected using by clicking on the arrow in the appropriate dialogue box. The default temperature range over which calculations are carried out is 300 to 3000 K in steps of 50 K but this may be truncated depending on the upper temperature range of one or more of the compounds in the chemical equation. The user may, however, select a range of temperatures and step size depending on his own interest. The default pressure is 105 Pa but again this may be changed by the user if he/she wishes to investigate the properties of a chemical reaction or a pure substance at other pressures. A number of different thermodynamic functions may be plotted as a function of temperature including the heat capacity at constant pressure, Cp (the default), enthalpy, H, entropy, S, the Gibbs energy, G, and a function beta. When looking at data for individual substances the heat capacity and entropy represent absolute values while the values of the enthalpy and Gibbs energy are relative to the SGTE defined reference, Hser, the enthalpies of the elements in their standard reference state at 298.15 K. If a chemical reaction is being considered these functions become the change in properties arising from the chemical reaction ie ∆Cp, ∆S, ∆H and ∆G. The function beta for a pure substance is defined as: G/RTln10 where G is the Gibbs energy relative to HSER as defined above. For a chemical reaction the function beta now represents ∆G/RTln10 or the logarithm (base 10) of the equilibrium constant at constant pressure i.e. log10Kp. While SGTETab gives useful information about the stability of individual substances under ranges of conditions it is worth remembering that more powerful facilities are also available from SGTE members to use the data to model chemical and phase equilibria of much greater complexity.

Landolt-Börnstein New Series IV/19A

SGTE

XX

Introduction

References 78Hil 81Ind 87Ans 91Din 95Sun 98Pre

87Mas 96IUPAC 97IUPAC

SGTE

M. Hillert and M. Jarl: CALPHAD 2 (1978) 227-238. G. Inden: Physica 103B (1981) 82-100. I. Ansara and B. Sundman: in "Computer Handling and Dissemination of Data", P. Glaeser (ed.), CODATA, Elsevier, 1987, p. 154-158. A.T. Dinsdale: CALPHAD 15 (1991) 317-425. B. Sundman, F. Aldinger: 1995 Ringberg Workshop on Unary Data, CALPHAD 19 (1995) 433. B. Predel: "Phase Equilibria, Crystallographic and Thermodynamic Data of Binary Alloys, Pu-Re ... Zn-Zr", O. Madelung (ed.), Landolt-Börnstein New Series IV/5J, Springer-Verlag, Berlin Heidelberg (1998) T. Massalski (ed.): "Binary Alloy Phase Diagrams", ASM International, Materials Park, Ohio, USA. IUPAC, Pure Appl. Chem. 68 (1996) 2339-2359. IUPAC, Pure Appl. Chem. 69 (1997) 2471-2473.

Landolt-Börnstein New Series IV/19A

References

LVII

References 67Kub 69Stu

"Metallurgical Thermochemistry" (Fourth edition), O. Kubaschewski, E.LL. Evans and C.B. Alcock, Pergamon Press Ltd. (1967). "The Chemical Thermodynamics of Organic Compounds", D.R. Stull, E. Westrum Jr. and G. Sinke, Wiley & Sons Publ. (1969). "Thermochemical Properties of Inorganic Substances", I. Barin, O. Knacke (1973), and 'Supplement 1977', I. Barin, O. Knacke and O. Kubaschewski, Springer-Verlag Berlin, Heidelberg and Verlag Stahleisen mbH, Düsseldorf. "Thermodynamic Data for Inorganic Sulphides, Selenides and Tellurides", K.C. Mills, Butterworths & Co. Ltd. London (1974). "Thermodynamic Properties of Halides", L.B. Pankratz,, Bur. Mines. Bull. 674 (1984). "JANAF Thermochemical Tables" (Third edition), M.W. Chase, Jr., C.A. Davies, J.R. Downey, Jr., D.J. Frurip, R.A. McDonald, and A.N. Syverud, Journal of Physical and Chemical Reference Data, vol. 14, Supplement No. 1, The American Chemical Society and American Institute of Physics for the National Bureau of Standards (1985). "Thermochemical Properties of Inorganic Substances", Eds. O. Knacke, O. Kubaschewski and K. Hesselmann, Springer-Verlag Berlin, Heidelberg and Verlag Stahleisen mbH, Düsseldorf (1991). "Thermochemical Data of Pure Substances" (Second edition), I. Barin, VCH Verlagsgesellschaft mbH, Weinheim (1993). THERMODATA, Grenoble Campus, 1001 Avenue Centrale, BP 66, F-38402 Saint re a Martin d'Hères, France. w oft V.A. "CODATA Key Values for Thermodynamics", Eds. J.D. Cox, D.D. Wagman, s Medvedev, Hemisphere Publ. Corp. (1989). DF P Scientific Group Thermodata Europe (SGTE), Grenoble Campus, TS 1001 Avenue R Centrale, BP 66, F-38402 Saint Martin d'Hères, France. f A IVTAN Association, Glushko Thermocenter of the Russian Academy of o Sciences, Izhorskaya 13/19, 127412 Moscow, Russia. ion s r see [94SGTE] ve o see [94TCRAS] em (Fourth edition), M.W. Chase, Jr., Journal of "NIST-JANAF Thermochemical Tables" d Physical and Chemical Reference g a Data, Monograph n° 9, The American Chemical n i Society and American Institute us of Physics (1998). d see [93THDA] e i

73Bar

74Mil 84Pan 85JANAF

91Kna

m o

93Bar

c . f d

93THDA 94CODATA

p ts

94SGTE 94TCRAS

r .a

95SGTE 96TCRAS 98JANAF

w w

99THDA

w

is Th

en

if

d mo

e sb

a

h DF

P

Landolt-Börnstein New Series IV/19A

SGTE

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeBr g






 

298.15

229.587

BeBr





298.15 781.00

w

ww

en s be

DF is P

Th

ha

in

ified

mod

us

mo

om

f.c

pd

de ga

n of

rsio

ve

AR

TS

PD

are

ftw

F so

   

 - 

 

 

 

8971.0

132447.0

143.982

89518.8

Beryllium Bromide 

 

   

 - 

 

 

 

108.000

14900.0

–358000.0

–53.710

–341986.0

Landolt-B¨ornstein New Series IV/19A

ts .ar

Beryllium Monobromide gas 

1

 94TCRAS

 

 ! 

18000.0

23.047

 94TCRAS type

#"%$

SGTE

2

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeBr&(' g )+* Beryllium Bromide gas ,

/

0 1

231 45  2 1 - 6

78 21

78 01

789 1

298.15

273.236

12837.0

–234063.0

111.526

–267314.0

BeCO:;* Beryllium Carbonate,

/

0 1

2 31 4 5 2 6 1 -

78 2 1

78 0 1

789 1

298.15

52.000

9200.0

–1045000.0

–270.963

–964213.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

- 94TCRAS.

- 94TCRAS.

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeC<(= g >@? Monoberyllium Dicarbide gas A

D

E F

GHF IJ  G F - K

LM GF

LM EF

LMN F

298.15

218.643

10196.0

564840.0

197.659

505908.0

BeCl = g >@? Beryllium Monochloride gas A

D

E F

G HF I J G K F -

LM G F

LM E F

LMN F

298.15

218.097

8861.0

56693.0

97.058

27755.3

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

3

B 85JANAFC

B 94TCRASC

SGTE

4

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeClF O g P@Q Beryllium Chloride Fluoride gas R

U

V W

XYW Z[  X W - \

]^ XW

]^ VW

]^_ W

298.15

246.493

11702.6

–573208.0

24.059

–580381.0

BeCl`;Qa – Beryllium ChlorideR

U

V W

]^ XW

]^ V W

]^_ W

298.15 688.00

82.676

–490783.2

–149.903

–446090.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

S 85JANAFT

S 94SGTET

]bcd XW

]b c!d VW

type

8660.9

12.589

Vfehg

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeCli;jk – Beryllium Chloride l

o

p q

rstq

rsp q

rsuq

298.15 676.00 688.00

75.814

–496222.4

–156.765

–449483.0

BeCli|{ g }+j Beryllium Chloride gas l

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

m 94SGTEn

rvwxtq

rv w!xpq

type

6819.9 8660.9

10.089 12.589

pfy%p pfyhz

o

p q

t~q €  t q - 

r s tq

r s pq

r s uq

298.15

250.258

12081.0

–361539.0

17.679

–366810.0

Landolt-B¨ornstein New Series IV/19A

5

m 94TCRASn

SGTE

6

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeF ‚ g ƒ+„ Beryllium Monofluoride gas …

ˆ

‰ Š

‹ŒŠ Ž  ‹ Š - 

‘ ‹Š

‘ ‰Š

‘’ Š

298.15

205.752

8711.0

–170624.0

94.857

–198906.0

BeF“”„ Beryllium Fluoride …

ˆ

‰ Š

‹ŒŠ Ž  ‹ Š - 

‘ ‹Š

‘ ‰Š

‘’ Š

298.15 493.00 823.00

53.350

8468.0

–1027000.0

–158.939

–979612.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

† 94TCRAS‡

• –!— ‹Š

•–!— ‰Š

175.0 4770.0

0.355 5.796

† 94TCRAS‡ type

‰f˜%‰ ‰f˜%‰

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeF™(š g ›@œ Beryllium Fluoride gas 

 

¡ ¢

£¤¢ ¥¦  £ ¢ - §

¨© £¢

¨© ¡¢

¨©ª ¢

298.15

227.278

10880.0

–796588.0

14.989

–801057.0

BeH š g ›@œ Beryllium Monohydride gas 

 

¡ ¢

£ ¤¢ ¥ ¦ £ § ¢ -

¨© £ ¢

¨© ¡ ¢

¨©ª ¢

298.15

176.821

8648.0

342252.0

101.981

311846.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

7

ž 94TCRASŸ

ž 94TCRASŸ

SGTE

8

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeH«;¬ Beryllium Hydride ­

°

± ²

³´² µ¶  ³ ² - ·

¸¹ ³²

¸¹ ±²

¸¹º ²

298.15

24.100

4200.0

–19000.0

–116.080

15609.3

BeH«|» g ¼½¬ Beryllium Hydride gas ­

°

± ²

¸¹ ³ ²

¸¹ ± ²

¸¹¾º ²

298.15

173.327

125520.0

33.147

115637.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

® 94TCRAS¯

® 94SGTE¯

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeI ¿ g À+Á Beryllium Monoiodide gas Â

Å

Æ Ç

ÈÉÇ ÊË  È Ç - Ì

ÍÎ ÈÇ

ÍÎ ÆÇ

ÍÎÏ Ç

298.15

237.292

9096.0

169991.7

169.722

119389.0

BeIÐÑÁ Beryllium Iodide Â

Å

Æ Ç

ÍÎ ÈÇ

ÍÎ ÆÇ

ÍÎÏ Ç

298.15 753.00

120.499

–211710.4

–5.140

–210178.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

9

à 85JANAFÄ

à 85JANAFÄ

ÍÒÓ!Ô ÈÇ

ÍÒÓ!Ô ÆÇ

type

20920.0

27.782

ÆfÕhÖ

SGTE

10

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeI×(Ø g Ù@Ú Beryllium Iodide gas Û

Þ

ß à

áâà ãä  á à - å

æç áà

æç ßà

æçè à

298.15

291.521

13631.5

–64015.2

165.882

–113473.0

BeN Ø g Ù½Ú Beryllium Mononitride gas Û

Þ

ß à

á âà ã ä á å à -

æç á à

æç ß à

æçè à

298.15

208.774

8723.6

426688.5

103.468

395839.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ü 85JANAFÝ

Ü 85JANAFÝ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeO é Beryllium Oxide ê

í

îï

ðñï òó  ð ï - ô

õö ðï

õö îï

õö÷ ï

298.15 2373.00 2851.00

13.770

2837.0

–609400.0

–98.303

–580091.0

BeO þ g ÿ@é Beryllium Oxide gas ê

í

î ï

ðñï òó  ð ï - ô

õ ö ðï

õ ö îï

õ ö÷ ï

298.15

197.624

8686.0

136398.4

85.550

110892.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

11

õøùú ðï

õø ù!ú îï

264.0 86000.0

0.111 30.165

ë 94TCRASì type

î#ûüî î#û%ý

ë 85JANAFì

SGTE

12

BeSO

 298.15 863.00 908.00




Thermodynamic Properties of Inorganic Materials: Pure Substances

Beryllium Sulphate 







 





77.969

–1200808.0

–373.895

–1089330.0

 



type

945.6 19551.8

1.096 21.533

 




BeS Beryllium Sulphide 





  







298.15

34.000

5500.0

–236000.0

–7.570

–233743.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

 93THDA

 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeS ! g "$# Beryllium Sulphide gas %

(

)*

+,* -.  + * - /

01 +*

01 )*

01 2 *

298.15

210.289

8778.0

263592.0

168.719

213288.0

Be3 C # Diberyllium Carbide%

(

)*

01 +*

01 )*

0142 *

298.15 2400.00

16.318

–90793.0

–8.424

–88281.4

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

13

& 85JANAF'

& 85JANAF'

05768 +*

05768 )*

type

75312.0

31.380

)9;:

SGTE

14

Thermodynamic Properties of Inorganic Materials: Pure Substances

Be< Cl=?> g @BA Diberyllium Tetrachloride gas C

F

GH

IJH KL  I H - M

NO IH

NO GH

NOQP H

298.15

366.333

22641.0

–819621.0

–98.825

–790156.0

O(BeF) g @BA Diberyllium Difluoride Oxide gas C

F

G H

I JH K L I M H -

NO I H

NO G H

NO P H

298.15

298.910

16585.4

–1204573.6

–25.452

–1196980.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

D 94TCRASE

D 85JANAFE

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BeR FS?T g U$V Diberyllium Tetrafluoride gas W

Z

[\

]^\ _`  ] \ - a

bc ]\

bc [\

bc4d \

298.15

323.161

19834.0

–1731716.0

–101.417

–1701480.0

BeR O T g UBV Diberyllium Monoxide gas W

Z

[ \

] ^\ _ ` ] a \ -

bc ] \

bc [ \

bc4d \

298.15

220.832

9924.4

–62760.0

99.258

–92353.9

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

15

X 94TCRASY

X 85JANAFY

SGTE

16

Thermodynamic Properties of Inorganic Materials: Pure Substances

Bee Oegf g hBi Diberyllium Dioxide gas j

m

no

pqo rs  p o - t

uv po

uv no

uv w o

298.15

247.618

11405.6

–410032.0

23.471

–417030.0

Bex Neyi Beryllium Nitride j

m

no

pqo rs  p o - t

uv po

uv no

uvQw o

298.15 1673.0 2473.0

34.400

7124.0

–588000.0

–185.982

–532820.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

k 85JANAFl

k 94TCRASl

uz{| po

uz7{| no

16000.0 111000.0

9.564 44.885

type

n~}n n~}€

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Be Og‚ g ƒB„ Triberyllium Trioxide gas …

ˆ

‰Š

‹ŒŠ Ž  ‹ Š - 

‘ ‹Š

‘ ‰Š

‘ ’ Š

298.15

273.341

13321.9

–1054368.0

–62.880

–1035620.0

Be“ O“?‚ g ƒB„ Tetraberyllium Tetraoxide gas …

ˆ

‰ Š

‹ ŒŠ  Ž ‹  Š -

‘ ‹ Š

‘ ‰ Š

‘4’ Š

298.15

302.579

16526.8

–1589920.0

–145.715

–1546480.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

17

† 85JANAF‡

† 85JANAF‡

SGTE

18

Thermodynamic Properties of Inorganic Materials: Pure Substances

Be” O”g• g –B— Pentaberyllium Pentaoxide gas ˜

›

œ

žŸ  ¡  ž  - ¢

£¤ ž

£¤ œ

£¤4¥ 

298.15

323.282

19087.4

–2112920.0

–237.086

–2042230.0

Be¦ O¦g• g –B— Hexaberyllium Hexaoxide gas ˜

›

œ 

ž Ÿ   ¡ ž ¢  -

£¤ ž 

£¤ œ 

£¤4¥ 

298.15

343.197

21476.5

–2661024.0

–329.244

–2562860.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

™ 85JANAFš

™ 85JANAFš

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiBr g






 

298.15

267.467

BiBr





298.15 492.00

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 





53408.8

134.627

13269.8

Bismuth Tribromide 

 

 





181.586

–276144.0

–103.464

–245296.0

Landolt-B¨ornstein New Series IV/19A

sp art

Bismuth Monobromide 

19

 93THDA

 73Bar

 



type

21714.9

44.136



SGTE

20

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiBr! g "$# Bismuth Tribromide gas %

(

) *

+ ,-*

+ ,)*

+ ,.*

298.15

384.410

–156900.0

99.360

–186524.0

BiCl # Bismuth Monochloride %

(

) *

+ ,- *

+,) *

+ ,. *

298.15

92.885

–127612.0

–75.390

–105135.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

& 93THDA'

& 94SGTE'

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiCl / g 0$1 Bismuth Monochloride gas 2

6 7

8 9:7

8 967

8 9;7

298.15

255.082

25104.0

86.808

–777.7

5

6 7

8 9: 7

8 96 7

8 9; 7

298.15

102.508

–371120.8

–168.340

–320930.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

3 73Bar4

5

BiOCl 1 Bismuth Chloride Oxide 2

21

3 73Bar4

SGTE

22

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiCl<>= Bismuth Trichloride ?

B

C D

E FGD

E FCD

E FHD

298.15 507.00

171.544

–378652.0

–219.810

–313116.0

BiCl
B

C D

E FGD

E FCD

E FQHD

298.15

357.423

–265265.6

–33.931

–255149.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

@ 73BarA

E IJKGD

E IJKCD

type

23639.6

46.626

CLM

@ 93THDAA

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiF R g S$T Bismuth Monofluoride gas U

X

Y Z

[\]_Z ^`  [ Z - a

b c [Z

b c YZ

b cd Z

298.15

244.198

9258.0

28660.0

86.068

2998.7

BiFefT Bismuth Trifluoride U

X

Y Z

b c [Z

b c YZ

b cd Z

298.15 922.00

122.591

–910438.4

–238.328

–839381.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

23

V 94TCRASW

V 94SGTEW

b ghi [Z

b ghi YZ

type

21589.4

23.416

Yjk

SGTE

24

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiFlnm g oqp Bismuth Trifluoride gas r

u

v w

x yzw

x yvw

x yQ{w

298.15

317.759

–709188.0

–43.160

–696320.0

BiH m g o$p Bismuth Monohydride gas r

u

v w

z |_w } ~ z  w -

x yz w

xyv w

x y{ w

298.15

214.635

8671.0

202012.0

92.560

174415.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

s 94SGTEt

s 94TCRASt

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiI € Bismuth Monoiodide 

„

… †

‡ ˆ‰†

‡ˆ… †

‡ ˆŠ†

298.15 564.00

123.428

–55772.7

8.623

–58343.8

BiI ‘ g ’$€ Bismuth Monoiodide gas 

„

… †

‡ ˆ‰†

‡ ˆ…†

‡ ˆŠ†

298.15

275.417

74554.7

160.612

26668.1

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

25

‚ 73Barƒ

‡ ‹Œ‰†

‡‹ŽŒ…†

type

1297.0

2.300

……

‚ 93THDAƒ

SGTE

26

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiI“f” Bismuth Triiodide •

˜

™ š

› œš

› œ™š

› œžš

298.15 682.00

224.681

–150624.0

–6.262

–148757.0

BiI“n¤ g ¥$” Bismuth Triiodide gas •

˜

™ š

› œš

›œ™ š

› œžš

298.15

408.384

–16317.6

177.440

–69221.5

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

– 73Bar—

› Ÿ ¡\š

› Ÿ ¡_™š

type

39120.4

57.361

™¢£

– 93THDA—

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiO ¦ g §$¨ Bismuth Monoxide gas ©

¬

­ ®

¯ °±®

¯°­ ®

¯ °²®

298.15

246.407

125687.0

87.099

99718.6

BiS ¦ g §q¨ Bismuth Monosulphide gas ©

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ª 94SGTE«

¬

­ ®

± ³_® ´ µ ± ¶ ® -

¯ °± ®

¯°­ ®

¯ °² ®

298.15

257.872

9485.0

176548.0

169.067

126141.0

Landolt-B¨ornstein New Series IV/19A

27

ª 94TCRAS«

SGTE

28

Thermodynamic Properties of Inorganic Materials: Pure Substances

Bi· O·n¸ g ¹qº Dibismuth Dioxide gas »

¾

¿ À

Á ÂÃÀ

Á¿ À

Á ÂÄÀ

298.15

347.375

–25261.6

28.758

–33835.8

Bi· OÅfº Dibismuth Trioxide »

¾

¿ À

Ã\Æ_À ÇÈ  Ã À - É

Á ÂÃÀ

Á ¿À

Á ÂÄÀ

298.15 1003.0 1098.0

149.810

21530.0

–578010.0

–271.381

–497098.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¼ 94SGTE½

ÁʎËÌÃÀ

¼ 94TCRAS½ Á ÊËÌ¿À

29800.0 14700.0

29.711 13.388

type

¿\Íο ¿\ÍÐÏ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BiÑ OÒnÓ g ÔqÕ Dibismuth Trioxide gas Ö

Ù

Ú Û

Ü ÝÞÛ

Ü ÝÚÛ

Ü ÝQßÛ

298.15

341.994

–222380.0

–79.197

–198768.0

BiÑ SÒàÕ Bismuth Sulphide Ö

Ù

ÚÛ

Ü ÝQÞ\Û

Ü ÝÚÛ

Ü ÝQßÛ

298.15 1050.00

200.414

–155644.8

–9.266

–152882.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

29

× 94SGTEØ

× 73BarØ

Ü áâãÞÛ

ÜáŽâãÚÛ

type

78240.8

74.515

Úäå

SGTE

30

Thermodynamic Properties of Inorganic Materials: Pure Substances

Biæ Oç!è g éqê Tribismuth Tetraoxide gas ë

î

ï ð

ñ òóð

ñ òïð

ñ òôð

298.15

432.428

–409745.7

–148.071

–365598.0

Biç Oõnè g éqê Tetrabismuth Hexaoxide gas ë

î

ï ð

ñ òó ð

ñ òï ð

ñ òô ð

298.15

507.812

–807896.0

–334.569

–708144.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ì 94SGTEí

ì 94SGTEí

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBr ö g ÷ùø Carbon Monobromide gas ú

ý

þ ÿ

\ÿ
 ÿ

 

298.15

234.560

9615.0

490413.0

-

ÿ

 

þÿ

152.713

  

þ ÿ

298.15

310.685

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ÿ




-

13787.0



ÿ

 

ÿ

–230000.0

 

þ ÿ

–49.436

û 94TCRASü ÿ

444882.0

CHBrClF ö g ÷$ø Bromochlorofluoromethane gas ú

ý

31

  

ÿ

û 94TCRASü

–215261.0

SGTE

32

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBrClFI  g  Bromochlorofluoroiodomethane gas  



 

 

298.15

353.555

18148.0

-



!

!

–125000.0

"

0.705

! #

 94TCRAS 

–125210.0

CBrClF$% g & Bromochlorodifluoromethane gas  

  

298.15

318.718

15528.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 

-

 



!





–435000.0

!

 

–77.457

 94TCRAS ! #



–411906.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHBrClI ' g () Bromochloroiodomethane gas * -

./

0/ 123

0/ 4

298.15

338.095

15967.0

-

0/

5 6

."/

5 6

60000.0

21.299

+ 94TCRAS, 5 6 7

/

53649.7

CH8 BrCl ' g () Bromochloromethane gas * -

. / 0

298.15

287.284

12191.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

/ 123

-

0 4

/

5 6

0

/

–45000.0

5 6

33

+ 94TCRAS, . /

–36.783

5 6 7

/

–34033.3

SGTE

34

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBrClI9%: g ;=< Bromochlorodiiodomethane gas > A

BC

DC EFG

DC H

298.15

382.350

20377.0

-

DC

I J

I J

170000.0

B"C

72.825

? 94TCRAS@ I JLK

C

148287.0

CFCl9 Br : g ;&< Bromodichlorofluoromethane gas > A

B C D

298.15

330.766

16730.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

C EFG

-

D H

C

I J

D

C

–235000.0

I J

B C

–75.554

? 94TCRAS@ I J K

C

–212473.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHBrClM%N g OP Bromodichloromethane gas Q T

UV

WV XYZ

WV [

298.15

316.472

14730.0

-

WV

\ ]

\ ]

–45000.0

U"V

–53.794

R 94TCRASS \ ] ^

V

–28961.3

CBrClM I N g O=P Bromodichloroiodomethane gas Q T

U V W

298.15

361.912

19084.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

V XYZ

-

W [

V

\ ]

W

V

60000.0

\ ]

U V

–1.084

35

R 94TCRASS \ ] ^

V

60323.0

SGTE

36

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBrCl_%` g a=b Bromotrichorobromomethane gas c f

gh

ih jkl

ih m

298.15

333.574

17984.0

-

ih

n o

n o

–43000.0

g"h

–82.892

d 94TCRASe h

n o p

–18285.9

CHBrFI ` g ab Bromofluoroiodomethane gas c f

g h i

298.15

325.273

14761.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

h jkl

-

i m

h

n o

i

h

–120000.0

n o

g h

18.622

d 94TCRASe n o p

h

–125552.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHq BrF r g s=t Bromofluoromethane gas u x

yz

{z |}~

{z 

298.15

276.276

11622.0

-

{z

€ 

v 94TCRASw € 

–215000.0

y"z

–37.646

€  ‚

z

–203776.0

CBrFIq%r g s=t Bromofluorodiiodomethane gas u x

y z {

298.15

373.226

19333.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

z |}~

-

{ 

z

€ 

{

z

–15000.0

37

€ 

y z

73.845

v 94TCRASw € L‚

z

–37017.0

SGTE

38

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHBrFƒ%„ g …=† Bromodifluoromethane gas ‡ Š

‹Œ

Œ Ž

Œ ‘

298.15

295.225

13169.0

-

Œ

’ “

’ “

–422000.0

ˆ 94TCRAS‰ ‹"Œ

–54.751

Œ

’ “ ”

–405676.0

CBrFƒ I „ g …† Bromodifluoroiodomethane gas ‡ Š

‹ Œ 

298.15

342.623

16988.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Œ Ž

-

 ‘

Œ

’ “



Œ

–325000.0

’ “

‹ Œ

–0.082

ˆ 94TCRAS‰ ’ “ ”

Œ

–324975.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBrF•—– g ˜™ Bromotrifluoromethane gas š 

žŸ

 Ÿ ¡¢£

 Ÿ ¤

298.15

297.822

14468.3

-

 Ÿ

¥ ¦

› 85JANAFœ ¥ ¦

–648938.4

ž"Ÿ

–88.209

¥ ¦ §

Ÿ

–622639.0

CHBrI¨©– g ˜™ Bromodiiodomethane gas š 

ž Ÿ  

298.15

355.142

16621.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ÿ ¡¢£

-

  ¤

Ÿ

¥ ¦

 

Ÿ

165000.0

39

› 94TCRASœ ¥ ¦

ž Ÿ

91.816

¥ ¦L§

Ÿ

137625.0

SGTE

40

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHª BrI « g ¬­ Bromoiodomethane gas ® ±

²³

´³ µ¶·

´³ ¸

298.15

307.087

12924.0

-

´³

¹ º

¯ 94TCRAS° ¹ º

60000.0

²"³

36.491

¹ º »

³

49120.4

CH¼ Br « g ¬=­ Bromomethane gas ® ±

² ³ ´

298.15

245.913

10612.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

³ µ¶·

-

´ ¸

³

¹ º

´

¯ 94TCRAS° ³

–36400.0

¹ º

² ³

–31.954

¹ º »

³

–26872.9

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBrI½%¾ g ¿=À Bromotriiodomethane gas Á Ä

ÅÆ

ÇÆ ÈÉÊ

ÇÆ Ë

298.15

395.269

21839.0

-

ÇÆ

Ì Í

 94TCRASÃ Ì Í

275000.0

Å"Æ

139.214

Æ

Ì Í Î

233493.0

BrCN ¾ g ¿=À Cyanogen Bromide gas Á Ä

Å Æ Ç

298.15

248.363

11075.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Æ ÈÉÊ

-

Ç Ë

Æ

Ì Í

Ç

Æ

186188.0

41

 85JANAFÃ Ì Í

Å Æ

70.711

Ì ÍLÎ

Æ

165106.0

SGTE

42

Thermodynamic Properties of Inorganic Materials: Pure Substances

CÏ H Ð Br Ñ g Ò=Ó Bromoethane gas Ô ×

ØÙ

ÚÙ ÛÜÝ

ÚÙ Þ

298.15

287.394

13573.0

-

Õ 94TCRASÖ ÚÙ

ß à

ß à

–63597.0

Ø"Ù

–126.895

Ù

ß à á

–25763.3

CaBr Ñ g Ò&Ó Calcium Monobromide gas Ô ×

Ø Ù Ú

298.15

253.122

9856.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ù ÛÜÝ

-

Ú Þ

Ù

ß à

Ú

Ù

–24868.0

Õ 94TCRASÖ ß à

Ø Ù

135.429

ß à á

Ù

–65246.2

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaBr â OH ãåä g æçâ Calcium Bromide Hydroxide gas ã ê

ëì

íì îïð

íì ñ

298.15

312.309

15986.0

-

íì

ò ó

ò ó

–480578.0

ë"ì

26.702

è 94TCRASé ì

ò ó ô

–488539.0

CdBr ä g æ&â Cadmium Monobromide gas ã ê

ë ì í

298.15

263.906

10055.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ì îïð

-

í ñ

ì

ò ó

í

ì

66321.0

ò ó

43

è 94TCRASé ë ì

136.001

ò óLô

ì

25772.3

SGTE

44

Thermodynamic Properties of Inorganic Materials: Pure Substances

BrCl õ g ö÷ Bromine Chloride gas ø û

üý

þý ÿ


298.15

240.045

9407.0

þý 

-

ù 94TCRASú

þý





14790.0

ü"ý

52.401

 

ý

–833.2

CoBr õ g ö&÷ Cobalt Monobromide gas ø û

ü ý þ

298.15

255.293

9986.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ý ÿ


-

þ 

ý



þ

ý

218299.0

ù 96TCRASú  

ü ý

149.148

 

ý

173831.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

45

CrBr  g  Chromium Monobromide gas  



 


298.15

268.326

9868.0

-

 





181481.0

 

 94TCRAS 

168.678





131190.0

CsBr Cesium Bromide  



 


298.15 910.00

112.940

13135.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 94TCRAS

-

 





–405600.0





–48.395

!



"$#

%$

 "&#'%



–391171.0 23600.0

25.934

type )(+*

SGTE

46

Thermodynamic Properties of Inorganic Materials: Pure Substances

CsBr , g -/. Cesium Bromide gas 0 3

45

65 7
89

298.15

267.530

10406.0

-

65 :

;<

65

–206829.0

1 94TCRAS2 ;<

45

106.195

5

;
–238491.0

CuBr . Copper Monobromide 0 3

45

65 78
9

298.15 657.00 741.00 759.00

96.100

12104.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

65 :

;<

1 96TCRAS2 65

–105000.0

; <

45

–13.155

;< =

5

;>$?'@

65

;>$?'@

45

–101078.0 4600.0 2150.0 5100.0

7.002 2.901 6.719

type 4BA+4 4BA+4 4BADC

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CuBr E g FHG Copper Monobromide gas I L

MN

ON P
QR

298.15

248.303

9759.0

ON S

-

ON

TU

J 96TCRASK T U

107235.0

MN

139.048

N

TU V

65777.8

BrF E g FG Bromine Monofluoride gas I L

M N O

298.15

228.985

9021.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

N P
QR

-

O S

N

TU

O

N

–58851.0

47

J 94TCRASK T U

M N

51.486

TUWV

N

–74201.4

SGTE

48

Thermodynamic Properties of Inorganic Materials: Pure Substances

BrFXZY g [/\ Bromine Trifluoride gas ] `

ab

cb d
ef

cb g

298.15

292.433

14275.8

-

cb

hi

^ 85JANAF_ hi

–255588.0

ab

–87.855

hi!j

b

–229394.0

BrFkZY g [/\ Bromine Pentafluoride gas ] `

a b c

298.15

323.687

19179.5

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

b d
ef

-

c g

b

hi

c

b

–428717.7

^ 85JANAF_ hi

a b

–259.391

hi j

b

–351380.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SBrFlZm g no Sulphur Bromide Pentafluoride gas p s

tu

vu w
xy

vu z

298.15

333.654

19434.7

-

vu

{|

{|

–972821.8

tu

–281.494

q 85JANAFr {| }

u

–888895.0

FeBr m g n/o Iron Monobromide gas p s

t u v

298.15

264.850

11379.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

u w
xy

-

v z

u

{|

v

49

q 96TCRASr u

224202.0

{ |

t u

161.465

{| }

u

176061.0

SGTE

50

Thermodynamic Properties of Inorganic Materials: Pure Substances

GaBr ~ g /€ Gallium Monobromide gas  „

…†

‡† ˆ
‰Š

298.15

251.827

9932.0

‡† ‹

-

‡†

Œ

‚ 94TCRASƒ Œ 

–17968.0

…†

134.995

†

Œ Ž

–58216.8

GeBr ~ g H€ Germanium Monobromide gas  „

… † ‡

298.15

257.221

9864.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

† ˆ
‰Š

-

‡ ‹

†

Œ

‡

†

137439.0

Œ 

‚ 94TCRASƒ … †

150.026

Œ Ž

†

92708.7

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

HBr  g /‘ Hydrogen Bromide gas ’ •

–—

˜— ™
š›

298.15

198.697

8648.0

˜— œ

-

“ 94TCRAS”

˜—

ž

 ž

–36290.0

–—

57.252

žWŸ

—

–53359.7

SrBr ‘ OH ’  g /‘ Strontium Bromide Hydroxide gas ’ •

– — ˜

298.15

328.430

16476.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

— ™
š›

-

˜ œ

—

ž

˜

51

—

–480928.0

ž

– —

28.718

ž Ÿ

“ 94TCRAS” —

–489490.0

SGTE

52

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiH¡ Br ¢ g £¤ Bromosilane gas ¥ ¨

©ª

«ª ¬
­®

298.15

262.463

11769.6

-

«ª ¯

°±

¦ 85JANAF§ «ª

–78240.8

° ±

©ª

–28.472

°± ²

ª

–69751.9

NH³ Br ¤ Ammonium Bromide¥ ¨

©ª

«ª ¬
­®

298.15 411.00

112.842

16953.6

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

«ª ¯

¦ 85JANAF§ °±

ǻ

–271541.6

°±

©ª

–320.428

°± ²

ª

° ´&µ'¶

ǻ

°´$µ'¶

©ª

–176006.0 3221.7

7.839

type ©B·+©

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

HgBr ¸ g ¹/º Mercury Monobromide gas » ¾

¿À

ÁÀ Â
ÃÄ

ÁÀ Å

298.15

271.546

10250.8

-

ÁÀ

ÆÇ

¼ 85JANAF½ Æ Ç

104181.6

¿À

110.134

À

ÆÇ È

69157.5

IBr ¸ g ¹º Iodine Bromide gas » ¾

¿ À Á

298.15

258.809

9911.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

À Â
ÃÄ

-

Á Å

À

53

¼ 94TCRAS½ ÆÇ

Á

À

40807.0

ÆÇ

¿ À

124.635

ÆÇWÈ

À

3647.2

SGTE

54

Thermodynamic Properties of Inorganic Materials: Pure Substances

InBr É Indium Monobromide Ê

Ë 73BarÌ

Í

ÎÏ

ÐÑ ÒÏ

ÐÑÎÏ

ÐÑ!Ó Ï

298.15 558.00

114.223

–175309.6

–19.532

–169486.0

ÐÔ$Õ$Ö ÒÏ

Ð Ô&Õ'ÖÎÏ

24267.2

43.490

InBr Ù g ÚÉ Indium Monobromide gas Ê Í

ÎÏ

ÒÏ Û
ÜÝ

298.15

259.614

10084.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

ÒÏ Þ

type ÎB×DØ

Ë 94TCRASÌ

ÐÑWÒÏ

Ð Ñ ÎÏ

ÐÑ Ó Ï

–54116.0

125.859

–91640.9

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

55

KBr ß Potassium Bromide à ã

äå

æå ç
èé

298.15 1007.00

95.920

12210.0

-

æå ê

á 94TCRASâ ëì

æå

–393450.0

ëì

äå

–44.865

å

ëì!í

ëî$ï$ð

25520.0

ã

äå

æå ç
èé

298.15

250.534

10109.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

æå ê

ëì

æå

–179251.0

ë î&ï'ð

äå

–380073.0

KBr ó g ô/ß Potassium Bromide gas à

sp art

æå

25.343

type ä)ñ+ò

á 94TCRASâ ëì

äå

109.749

ëì!í

å

–211973.0

SGTE

56

Thermodynamic Properties of Inorganic Materials: Pure Substances

LiBr õ Lithium Bromide ö

÷ 94TCRASø

ù

úû

üû ýþ
ÿ

298.15 823.00

74.010

10476.0

-

üû


 üû


 úû




–351160.0

–31.215

–341853.0

û

LiBr  g õ Lithium Bromide gas ö ù

úû

üû ý
þÿ

298.15

224.334

9173.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

üû


  üû


  úû

17660.0

21.458

type

 ú

÷ 94TCRASø


 üû


 úû




–151163.0

119.109

–186675.0

û

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MgBr  g  Magnesium Monobromide gas 





"! $# - %  &

'( %

'( )

'(* 

298.15

244.972

9588.0

6164.0

136.196

–34442.8

MnBr  Manganese Monobromide gas 



 

 "! $# -  & 

'(  

'(  

'(+* 

298.15

264.223

9839.8

81000.0

155.898

34519.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

57

 94TCRAS

 95SGTE

SGTE

58

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoBr , g -. Molybdenum Monobromide gas /

2

34

56"4 7$8 - % 5 94

:; 5%4

:; 3)4

:;< 4

298.15

251.060

9889.0

460000.0

146.395

416352.0

NBr , g -=. Nitrogen Monobromide gas /

2

3 4

5 6"4 $7 8 - 5 9 4

:; 5 4

:; 3 4

:;+< 4

298.15

235.485

8987.2

300758.5

63.575

281804.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

0 94TCRAS1

0 85JANAF1

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

NOBr > g ?A@ Nitrosyl Bromide gas B

E

FG

HI"G J$K - % H LG

MN H%G

MN F)G

MNO G

298.15

273.521

11652.4

82131.9

–0.963

82419.0

NaBr @ Sodium Bromide B

E

F)G

HI"G J$K - % H LG

MN H%G

MN F)G

MNO G

298.15 1020.00

86.930

11590.0

–361160.0

–40.475

–349092.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

59

C 85JANAFD

MP Q R H%G

MPSQR F)G

26230.0

25.716

C 94TCRASD type

FUTWV

SGTE

60

Thermodynamic Properties of Inorganic Materials: Pure Substances

NaBr X g Y=Z Sodium Bromide gas [

^

_`

ab"` c$d - % a e`

fg a%`

fg _)`

fgh `

298.15

241.221

9821.0

–145929.0

113.816

–179863.0

NiBr X g YAZ Nickel Monobromide gas [

^

_ `

a b"` $c d - a e `

fg a `

fg _ `

fgh `

298.15

256.784

10313.0

203161.0

150.883

158175.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

\ 94TCRAS]

\ 96TCRAS]

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

BrO i g jAk Bromine Monoxide gas l

o

pq

rs"q t$u - % r vq

wx r%q

wx p)q

wx+y q

298.15

232.709

9009.0

125837.0

54.030

109728.0

PuOBr k Plutonium Bromide Oxide l

o

p q

wx r q

wx p q

wxy q

298.15

119.244

–888681.6

–113.895

–854724.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

61

m 94TCRASn

m 73Barn

SGTE

62

Thermodynamic Properties of Inorganic Materials: Pure Substances

PBr z g {| Phosphorus Monobromide gas }

€

‚

ƒ„"‚ …$† - % ƒ ‡‚

ˆ‰ ƒ%‚

ˆ‰ )‚

ˆ‰Š ‚

298.15

249.212

9506.0

162464.7

132.017

123104.0

PbBr z g {| Lead Monobromide gas }

€

 ‚

ƒ „"‚ $… † - ƒ ‡ ‚

ˆ‰ ƒ ‚

ˆ‰  ‚

ˆ‰+Š ‚

298.15

272.741

10146.0

64822.0

131.836

25515.1

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

~ 85JANAF

~ 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

RbBr ‹ Rubidium BromideŒ



‘

’“"‘ ”$• - % ’ –‘

—˜ ’%‘

—˜ )‘

—˜™ ‘

298.15 965.00

110.100

13060.0

–394770.0

–42.781

–382015.0

RbBr Ÿ g  =‹ Rubidium Bromide gas Œ



‘

’“"‘ ”$• - % ’ –‘

—˜ ’%‘

—˜ )‘

—˜™ ‘

298.15

261.128

10319.0

–191511.0

108.247

–223785.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

63

—š › œ ’%‘

—šS›œ )‘

23300.0

24.145

 94TCRASŽ type

UWž

 94TCRASŽ

SGTE

64

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiBr ¡ g ¢£ Silicon Monobromide gas ¤

§

¨©

ª«"© ¬$­ - % ª ®©

¯° ª%©

¯° ¨)©

¯°± ©

298.15

247.285

10035.0

175158.0

152.370

129729.0

SnBr ¡ g ¢=£ Tin Monobromide gas ¤

§

¨ ©

ª «"© $¬ ­ - ª ® ©

¯° ª ©

¯° ¨ ©

¯°+± ©

298.15

264.827

9986.0

75644.0

137.542

34635.9

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¥ 94TCRAS¦

¥ 94TCRAS¦

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SrBr ² g ³´ Strontium Monobromide gas µ

¸

¹º

»¼"º ½$¾ - % » ¿º

ÀÁ »%º

ÀÁ ¹)º

ÀÁÂ º

298.15

263.874

10107.0

–63917.0

132.075

–103295.0

TBr ² g ³´ Tritium Bromide gas µ

¸

¹ º

» ¼"º $½ ¾ - » ¿ º

ÀÁ » º

ÀÁ ¹ º

ÀÁ+Â º

298.15

207.909

8682.0

–37370.0

55.140

–53810.1

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

65

¶ 94TCRAS·

¶ 94TCRAS·

SGTE

66

Thermodynamic Properties of Inorganic Materials: Pure Substances

TiBr à Titanium Monobromide Ä

Ç

ÈÉ

Ê%Ë$É Ì"Í -  Ê ÎÉ

ÏÐ Ê%É

ÏÐ È)É

ÏÐÑ É

298.15

75.000

11000.0

–206084.0

–31.825

–196595.0

TiBr Ò g Ó=Ã Titanium Monobromide gas Ä

Ç

È É

Ê Ë"É $Ì Í - Ê Î É

ÏÐ Ê É

ÏÐ È É

ÏÐÑ É

298.15

259.098

9861.0

191700.0

152.273

146300.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Å 94TCRASÆ

Å 94TCRASÆ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

TlBr Ô Thallium Monobromide Õ

Ø

ÙÚ

ÛÜÝ%Ú

ÛÜ$Ù)Ú

ÛÜÞÚ

298.15 733.00

122.591

–172673.7

–17.814

–167362.0

TlBr ä g åÔ Thallium Monobromide gas Õ

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ö 73Bar×

Ûß à áÝ%Ú

ÛßSàá$Ù)Ú

type

16401.3

22.376

Ù âã

Ø

ÙÚ

Ýæ"Ú ç$è - % Ý éÚ

ÛÜ+Ý%Ú

ÛÜÙ)Ú

ÛÜÞÚ

298.15

267.530

10201.0

–34329.0

127.125

–72231.3

Landolt-B¨ornstein New Series IV/19A

67

Ö 94TCRAS×

SGTE

68

Thermodynamic Properties of Inorganic Materials: Pure Substances

WBr ê g ëAì Tungsten Monobromide gas í

ð

ñò

óô"ò õ$ö - % ó ÷ò

øù ó%ò

øù ñ)ò

øùú ò

298.15

277.260

9903.0

586000.0

168.537

535751.0

ZnBr ê g ëì Zinc Monobromide gas í

ð

ñ ò

ó ô"ò $õ ö - ó ÷ ò

øù ó ò

øù ñ ò

øù+ú ò

298.15

255.656

9932.0

69808.0

137.920

28687.2

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

î 94TCRASï

î 96TCRASï

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

ZrBr g






 

298.15

265.205

CBr



g


298.15

  

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

   

 - 

 

 

 

10590.0

348730.0

149.919

304032.0

Carbon Dibromide gas 

288.459

Landolt-B¨ornstein New Series IV/19A

sp art

Zirconium Monobromide gas 

     -

 

  

 

12197.0

336627.0

130.507

297716.0

69

 94TCRAS

 94TCRAS

SGTE

70

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBr ClF  g  Dibromochlorofluoromethane gas

#

$ %

&'% ()  & % - *

+, &%

+, $%

+,.- %

298.15

343.080

17498.0

–175000.0

–27.806

–166710.0

CHBr Cl  g  Dibromochloromethane gas

#

$ %

& '% ( ) & * % -

+, & %

+, $ %

+,- %

298.15

328.020

15291.0

10000.0

–6.812

12030.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

! 94TCRAS"

! 94TCRAS"

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBr/ ClI 0 g 12 Dibromochloroiodomethane gas 3

6

7 8

9:8 ;<  9 8 - =

>? 98

>? 78

>?A@ 8

298.15

373.301

19886.0

115000.0

45.740

101363.0

CBr/ Cl/B0 g 12 Dibromodichloromethane gas 3

6

7 8

9 :8 ; < 9 = 8 -

>? 9 8

>? 7 8

>?A@ 8

298.15

348.483

18692.0

10000.0

–32.548

19704.2

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

71

4 94TCRAS5

4 94TCRAS5

SGTE

72

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHBrC F D g EGF Dibromofluoromethane gas H

K

L M

NOM PQ  N M - R

ST NM

ST LM

STU M

298.15

316.919

14359.0

–175000.0

–7.767

–172684.0

CBrC FI D g EF Dibromofluoroiodomethane gas H

K

L M

N OM P Q N R M -

ST N M

ST L M

STAU M

298.15

366.285

18984.0

–70000.0

48.869

–84570.3

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

I 94TCRASJ

I 94TCRASJ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CV BrV F W g XY Dibromodifluoromethane gas Z

]

^ _

`a_ bc  ` _ - d

ef `_

ef ^_

ef.g _

298.15

325.407

16280.0

–380000.0

–35.334

–369465.0

CHBrV I W g XY Dibromoiodomethane gas Z

]

^ _

` a_ b c ` d _ -

ef ` _

ef ^ _

efAg _

298.15

347.169

16226.0

110000.0

65.808

90379.5

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

73

[ 94TCRAS\

[ 94TCRAS\

SGTE

74

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHh Brhji g kl Dibromomethane gas m

p

q r

str uv  s r - w

xy sr

xy qr

xyz r

298.15

293.425

12630.0

10000.0

4.793

8571.0

CBrh IhBi g kl Dibromodiiodomethane gas m

p

q r

s tr u v s w r -

xy s r

xy q r

xyz r

298.15

385.765

21080.0

220000.0

111.674

186704.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

n 94TCRASo

n 94TCRASo

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C{ H| Br{j} g ~G 1,1–Dibromoethane gas €

ƒ

„ …

†‡… ˆ‰  † … - Š

‹Œ †…

‹Œ „…

‹Œ …

298.15

327.649

16322.0

–41003.0

–97.405

–11961.7

CaBr{Ž Calcium Bromide €

ƒ

„…

†‡… ˆ‰  † … - Š

‹Œ †…

‹Œ „…

‹Œ …

298.15 1015.00

130.000

17000.0

–683800.0

–63.798

–664779.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

75

 94TCRAS‚

 94TCRAS‚

‹‘“’ †…

‹”“’ „…

29100.0

28.670

type

„–•˜—

SGTE

76

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaBr™jš g ›œ Calcium Bromide gas 

 

¡ ¢

£¤¢ ¥¦  £ ¢ - §

¨© £¢

¨© ¡¢

¨©.ª ¢

298.15

310.128

15603.0

–387197.0

116.330

–421881.0

CdBr™«œ Cadmium Bromide 

 

¡ ¢

¨© £¢

¨© ¡¢

¨©.ª ¢

298.15 841.00

138.825

–315264.4

–65.185

–295829.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ž 94TCRASŸ

ž 73BarŸ

¨¬”­”® £¢

¨¬‘­“® ¡¢

type

33346.5

39.651

¡–¯˜°

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdBr±j² g ³µ´ Cadmium Bromide gas ¶

¹

º »

¼½» ¾¿  ¼ » - À

ÁÂ ¼»

Á º»

ÁÂ.Ã »

298.15

309.733

15407.0

–139613.0

105.723

–171134.0

CoBr±Ž´ Cobalt Dibromide ¶

¹

º »

¼½» ¾¿  ¼ » - À

ÁÂ ¼»

Á º»

ÁÂ.Ã »

298.15 648.00 951.00

135.000

17800.0

–215400.0

–47.250

–201312.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

77

· 94TCRAS¸

ÁÄ”Å”Æ ¼»

ÁÄ‘Å“Æ º»

170.0 43000.0

0.262 45.216

· 96TCRAS¸ type

ºÈÇɺ ºÈÇËÊ

SGTE

78

Thermodynamic Properties of Inorganic Materials: Pure Substances

CoBrÌjÍ g ÎÏ Cobalt Dibromide gas Ð

Ó

Ô Õ

Ö×Õ ØÙ  Ö Õ - Ú

ÛÜ ÖÕ

ÛÜ ÔÕ

ÛÜAÝ Õ

298.15

322.562

16147.0

–6053.0

140.312

–47887.0

CrBrÌ«Ï Chromium Dibromide Ð

Ó

ÔÕ

Ö×Õ ØÙ  Ö Õ - Ú

ÛÜ ÖÕ

ÛÜ ÔÕ

ÛÜÝ Õ

298.15 1115.00

140.000

18000.0

–298000.0

–35.753

–287340.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ñ 96TCRASÒ

Ñ 94TCRASÒ

Ûޑߓà ÖÕ

Ûޔߓà ÔÕ

45000.0

40.359

type

Ԗá˜â

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CrBrãjä g åæ Chromium Dibromide gas ç

ê

ë ì

íîì ïð  í ì - ñ

òó íì

òó ëì

òóô ì

298.15

314.432

15092.0

–50908.0

138.679

–92255.1

Csã Brãjä g åæ Dicesium Dibromide gas ç

ê

ë ì

í îì ï ð í ñ ì -

òó í ì

òó ë ì

òóô ì

298.15

413.791

22113.0

–565829.0

91.121

–592997.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

79

è 94TCRASé

è 94TCRASé

SGTE

80

Thermodynamic Properties of Inorganic Materials: Pure Substances

CuBrõ«ö Copper Dibromide ÷

ú

û ü

ýþü ÿ
ý ü



298.15

130.000

16700.0

–138500.0

-

ýü



–55.360

CuBrõ  g µö Copper Dibromide gas ÷

ú

û ü

ý þü
ÿ ý  ü -



298.15

318.345

14294.0

42094.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ý ü

ûü



û ü

132.985



ü

ø 96TCRASù

–121994.0



ü

ø 96TCRASù

2444.5

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

81

Cu Br  g  Dicopper Dibromide gas  



 


298.15

363.483

20154.0

-



!"



 96TCRAS !"

15626.0

#

144.973

!"$



–27597.7

EuBr % Europium Dibromide  



298.15 956.00

136.817

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

!"



–719648.0

 93THDA !"

#

–96.186

!"$



!&('()



!*&+',)

#

–690970.0 25145.8

26.303

type .-0/

SGTE

82

Thermodynamic Properties of Inorganic Materials: Pure Substances

EuBr12 g 34 Europium Dibromide gas 5

6 93THDA7

8

9:

;<>=:

;<
9#:

;<?*:

298.15

337.340

–372376.0

104.337

–403484.0

FeBr1@4 Iron Dibromide 5 8

9:

=: AB
C

298.15 650.00 964.00

140.700

18100.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

6 96TCRAS7

-

=: D

;<=:

;<
9#:

;<?*:

–244700.0

–38.790

–233135.0

;E(F(G=:

;*E+F,G>9#:

480.0 43000.0

0.738 44.606

type 9IHJ9 9IHLK

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

FeBrMON g PRQ Iron Dibromide gas S V

WX

YX Z[
\

YX ]

298.15

317.303

16504.0

-

T 96TCRASU YX

^_

^*_

–52296.0

W#X

137.813

^_>`

X

–93384.9

GaBrMON g PRQ Gallium Dibromide gas S V

W X Y

298.15

323.439

14025.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

X Z[
\

-

Y ]

X

^_

83

Y

X

–149180.0

T 94TCRASU ^_

W X

130.502

^_`

X

–188089.0

SGTE

84

Thermodynamic Properties of Inorganic Materials: Pure Substances

Gaa Brab g cd Digallium Dibromide gas e h

ij

kj lm
n

kj o

298.15

379.760

20793.0

-

kj

pq

f 94TCRASg pq

–136963.0

i#j

146.096

j

pqr

–180522.0

GeBra b g cd Digermanium Dibromide gas e h

i j k

298.15

319.165

14193.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

j lm
n

-

k o

j

pq

k

j

–60963.0

p*q

f 94TCRASg i j

135.865

pq>r

j

–101471.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

85

SiHs Brs t g uv Dibromosilane gas w z

{|

}| ~
€

298.15

310.048

14271.6

-

}| 

‚ƒ

x 85JANAFy

}|

‚ƒ

–190372.0

{#|

8.348

‚ƒ>„

|

–192861.0

HgBrs@v Mercury Dibromide w z

{|

298.15 514.00

170.314

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

‚ƒ

}|

–169452.0

x 85JANAFy ‚ƒ

{#|

–67.203

‚ƒ„

|

‚…(†(‡

}|

‚*…+†,‡

{#|

–151603.0 17907.5

34.839

type {.ˆ0‰

SGTE

86

Thermodynamic Properties of Inorganic Materials: Pure Substances

HgBrŠO‹ g ŒR Mercury Dibromide gas Ž ‘

’“

”“ •–
—

”“ ˜

298.15

320.231

15656.5

-

™š

”“

 85JANAF ™*š

–85454.0

’#“

82.714

™š›

–112303.0

HgŠ BrŠœ Dimercury Dibromide Ž ‘

’ “

298.15

218.752

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

™š

”

“

–204179.2

“

 85JANAF ™š

’ “

–104.071

™š>›

“

–177525.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

InBr ž g Ÿ  Indium Dibromide gas ¡ ¤

¥¦

§¦ ¨©
ª

§¦ «

298.15

333.551

14424.0

-

§¦

¬­

¢ 94TCRAS£ ¬­

–149729.0

¥#¦

123.691

¦

¬­®

–186607.0

In Br ž g Ÿ¯  Diindium Dibromide gas ¡ ¤

¥ ¦ §

298.15

398.287

21435.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¦ ¨©
ª

-

§ «

¦

¬­

§

¦

–196305.0

87

¢ 94TCRAS£ ¬­

¥ ¦

130.777

¬­®

¦

–235296.0

SGTE

88

Thermodynamic Properties of Inorganic Materials: Pure Substances

K° Br° ± g ²³ Dipotassium Dibromide gas ´ ·

¸¹

º¹ »¼
½

º¹ ¾

298.15

376.369

20952.0

-

º¹

¿À

µ 94TCRAS¶ ¿À

–538744.0

¸#¹

94.799

¿À>Á

¹

–567008.0

Li° Br° ± g ²¯³ Dilithium Dibromide gas ´ ·

¸ ¹ º

298.15

317.527

16958.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¹ »¼
½

-

º ¾

¹

¿À

º

¹

–495826.0

µ 94TCRAS¶ ¿À

¸ ¹

107.077

¿ÀÁ

¹

–527751.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

89

MgBrψ Magnesium Bromide Ä Ç

ÈÉ

ÊÉ ËÌ
Í

298.15 984.00

117.000

15500.0

-

ÊÉ Î

Å 94TCRASÆ ÏÐ

ÊÉ

–526000.0

ÏÐ

È#É

–67.881

É

ÏÐÑ

ÏÒ(Ó(Ô

39300.0

Ç

ÈÉ

ÊÉ ËÌ
Í

298.15

296.427

14757.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

ÊÉ Î

ÏÐ

ÊÉ

–306743.0

Ï*Ò+Ó,Ô

È#É

–505761.0

MgBrÂ × g Øà Magnesium Bromide gas Ä

sp art

ÊÉ

39.939

type ÈIÕLÖ

Å 94TCRASÆ ÏÐ

È#É

111.546

ÏÐÑ

É

–340000.0

SGTE

90

Thermodynamic Properties of Inorganic Materials: Pure Substances

MnBrÙœÚ Manganese Dibromide Û

Ü 93THDAÝ

Þ

ßà

áâ>ãà

áâ
ß#à

áâä*à

298.15 971.00

138.072

–384928.0

–46.358

–371106.0

MnBrÙ ê g ë¯Ú Manganese Dibromide gas Û

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

á*å+æ,ç
ß#à

33472.0

34.472

type ß.è0é

Ü 93THDAÝ

Þ

ßà

áâ>ãà

áâ
ß#à

áâä*à

298.15

318.089

–175309.6

133.659

–215160.0

SGTE

áå(æ(ç>ãà

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoBrìœí Molybdenum Dibromide î ñ

òó

ôó õö
÷

ôó ø

298.15

130.000

19000.0

-

ï 94TCRASð

ôó

ùú

ùú

–234000.0

ò#ó

–50.770

ó

ùúû

–218863.0

MoBrì ü g ýí Molybdenum Dibromide gas î ñ

ò ó ô

298.15

318.941

15215.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ó õö
÷

-

ô ø

ó

ùú

ô

91

ó

170000.0

ù*ú

ï 94TCRASð ò ó

138.171

ùú>û

ó

128804.0

SGTE

92

Thermodynamic Properties of Inorganic Materials: Pure Substances




Naþ Brþ ÿ g

Disodium Dibromide gas 





298.15

351.041

     - 

 

 

 

19591.0

–480849.0

96.231

–509540.0

 94TCRAS




NiBrþ Nickel Bromide 





     - 

 

 

 

298.15 1236.00

122.360

16680.0

–211900.0

–59.646

–194117.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 96TCRAS

 

 

56000.0

45.307

type

 "!

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

NiBr#%$ g &(' Nickel Bromide gas )

,

-.

/ 0 . 12  / . - 3

45 /.

45 -.

456 .

298.15

316.872

15070.0

9490.0

134.866

–30720.3

ThBr# O ' Thorium Dibromide Oxide )

,

- .

45 / .

45 - .

4576 .

298.15

130.959

–1129680.0

–175.624

–1077320.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

93

* 96TCRAS+

* 73Bar+

SGTE

94

Thermodynamic Properties of Inorganic Materials: Pure Substances

UBr8 O 9 Uranium Dibromide Oxide :

=

>?

@AB?

@A>?

@A7C?

298.15

157.737

–1004160.0

–147.246

–960258.0

PbD Br8 O8E9 Trilead Dibromide Dioxide :

=

> ?

@AB ?

@A> ?

@AC ?

298.15

284.203

–741823.2

–267.554

–662052.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

; 73Bar<

; 94SGTE<

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

UBrF OFEG Uranium Dibromide Dioxide H

K

LM

NOPM

NOLM

NO7QM

298.15

169.452

–1157294.4

–238.105

–1086300.0

PbR BrF OSEG Tetralead Dibromide Trioxide H

K

L M

NOP M

NOL M

NOQ M

298.15

349.473

–970269.6

–369.657

–860056.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

95

I 93THDAJ

I 94SGTEJ

SGTE

96

Thermodynamic Properties of Inorganic Materials: Pure Substances

PbBrTVU Lead Bromide W

Z

[\

] ^ \ _`  ] \ - a

bc ]\

bc [\

bced \

298.15 644.00

161.130

19233.8

–277399.2

–55.880

–260739.0

PbBrTnm g o(U Lead Bromide gas W

Z

[\

] ^ \ _`  ] \ - a

bc ]\

bc [\

bced \

298.15

339.386

14987.1

–104390.8

122.376

–140877.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

bfgh ]\

bfgh [\

16443.1

25.533

X 85JANAFY type

[jilk

X 85JANAFY

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

PdBrpVq Palladium Bromide r

u

vw

xyzw

xyvw

xye{w

298.15

141.001

–103344.8

–49.032

–88725.9

PtBrpVq Platinum Bromide r

u

v w

xyz w

xyv w

xy{ w

298.15

154.808

–80332.8

–39.033

–68695.1

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

97

s 94SGTEt

s 73Bart

SGTE

98

Thermodynamic Properties of Inorganic Materials: Pure Substances

Rb| Br|~} g € Dirubidium Dibromide gas ‚

…

†‡

ˆ ‰ ‡ Š‹  ˆ ‡ - Œ

Ž ˆ‡

Ž †‡

Ž ‡

298.15

398.368

21696.0

–551802.0

92.606

–579412.0

SBr|n} g (€ Sulphur Dibromide gas ‚

…

† ‡

Ž ˆ ‡

Ž † ‡

Ž ‡

298.15

301.650

–12552.0

117.370

–47545.9

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ƒ 94TCRAS„

ƒ 93THDA„

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

S Br~‘ g ’“ Disulphur Dibromide gas ”

—

˜™

š›œ™

š›˜™

š›7™

298.15

350.519

30961.6

134.169

–9040.9

SeBrn‘ g ’(“ Selenium Dibromide gas ”

—

˜ ™

š›œ ™

š›˜ ™

š› ™

298.15

317.089

–20920.0

122.913

–57566.5

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

99

• 93THDA–

• 93THDA–

SGTE

100

Thermodynamic Properties of Inorganic Materials: Pure Substances

Sež BržnŸ g  ¡ Diselenium Dibromide gas ¢

¥

¦§

¨©ª§

¨©¦§

¨©7«§

298.15

378.134

29288.0

141.992

–13046.9

SiBržnŸ g  ¡ Silicon Dibromide gas ¢

¥

¦ §

ª ¬ § ­ ® ª ¯ § -

¨©7ª §

¨©¦ §

¨©« §

298.15

304.715

13317.0

–51000.0

133.695

–90861.2

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

£ 93THDA¤

£ 94TCRAS¤

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SnBr°V± Tin Dibromide ²

µ

¶·

¸¹º·

¸¹¶·

¸¹e»·

298.15 505.00

149.787

–259993.8

–53.603

–244012.0

SnBr°~Á g ± Tin Dibromide gas ²

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

³ 73Bar´

¸¼½¾º·

¸¼½¾¶·

type

17991.2

35.626

¶ ¿"À

µ

¶·

º Ã · ÄÅ  º · - Æ

¸¹7º·

¸¹¶·

¸¹e»·

298.15

329.041

14595.0

–118975.0

125.651

–156438.0

Landolt-B¨ornstein New Series IV/19A

101

³ 94TCRAS´

SGTE

102

Thermodynamic Properties of Inorganic Materials: Pure Substances

SrBrÇVÈ Strontium Bromide É

Ì

ÍÎ

ÏÐÑÎ

ÏÐÍÎ

ÏÐeÒÎ

298.15 918.00 930.00

135.101

–717556.0

–72.803

–695850.0

SrBrÇnØ g Ù(È Strontium Bromide gas É

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ÏÓÔÕÑÎ

ÏÓÔÕÍÎ

type

12133.6 10460.0

13.217 11.247

Í ÖlÍ Í Ö"×

Ì

ÍÎ

Ñ Ú Î ÛÜ  Ñ Î - Ý

Ï Ð ÑÎ

Ï Ð ÍÎ

Ï Ð ÒÎ

298.15

326.403

16334.0

–406726.0

118.499

–442056.0

SGTE

Ê 73BarË

Ê 94TCRASË

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

TiBrÞVß Titanium Dibromide à

ã

äå

æ ç å èé  æ å - ê

ëì æå

ëì äå

ëìeí å

298.15

113.000

16300.0

–396000.0

–69.930

–375150.0

TiBrÞnî g ïðß Titanium Dibromide gas à

ã

ä å

æ ç å è é æ ê å -

ëì æ å

ëì ä å

ëìeí å

298.15

305.696

14789.0

–107709.0

122.766

–144312.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

103

á 94TCRASâ

á 94TCRASâ

SGTE

104

Thermodynamic Properties of Inorganic Materials: Pure Substances

Tlñ Brñnò g ó(ô Dithallium Dibromide gas õ

ø

ùú

û ü ú ýþ  û ú - ÿ


ûú


ùú


 ú

298.15

414.830

21856.0

–164328.0

134.020

–204286.0

VBrñVô Vanadium Dibromide õ

ø

ù ú


û ú


ù ú


 ú

298.15

125.520

–364426.0

–57.580

–347259.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ö 94TCRAS÷

ö 91Kna÷

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

VBr g  Vanadium Dibromide gas 









298.15

125.629

–347272.0

–57.471

–330137.0



 

   -  ! 

" 

 

 

298.15

325.979

15465.0

298000.0

141.151

255916.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

94SGTE



WBr g  Tungsten Dibromide gas 

105

94TCRAS

SGTE

106

Thermodynamic Properties of Inorganic Materials: Pure Substances

ZnBr#%$ Zinc Bromide &

)

*+

,-.+ /0 -  , 1+

23 ,+

23 *+

234 +

298.15 675.00

132.000

16670.0

–329000.0

–61.841

–310562.0

ZnBr#@? g A $ Zinc Bromide gas &

)

*+

,-.+ /0 -  , 1+

23 ,+

23 *+

234 +

298.15

300.801

14944.0

–184726.0

106.960

–216616.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

257678 ,+

2596:8 *+

15650.0

23.185

' 96TCRAS( type

*<;>=

' 96TCRAS(

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

ZrBrBDC Zirconium Dibromide E

H

IJ

KLJ MN -  K OJ

PQ K-J

PQ IJ

PQR J

298.15 1100.00

135.000

17000.0

–420000.0

–56.391

–403187.0

ZrBrBZ g [C Zirconium Dibromide gas E

H

IJ

K-LJ MN -  K OJ

PQ KJ

PQ IJ

PQR J

298.15

317.101

15406.0

–20791.0

125.710

–58271.4

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

107

F 94TCRASG

PS9T:U KJ

PS7T:U IJ

28000.0

25.455

type

IWVYX

F 94TCRASG

SGTE

108

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBr\] g ^ _ Carbon Tribromide gas `

c

de

f-ge hi -  f je

kl fe

kl de

klm e

298.15

334.571

15582.0

235000.0

100.514

205032.0

CBr\ Cl ] g ^ _ Tribromochloromethane gas `

c

d e

f ge h i - f j e

kl f e

kl d e

klm e

298.15

357.610

19568.0

65000.0

12.014

61418.2

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

a 94TCRASb

a 94TCRASb

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBrn F o g p q Tribromofluoromethane gas r

u

vw

x-yw z{ -  x |w

}~ xw

}~ vw

}~ w

298.15

345.718

18243.0

–120000.0

10.267

–123061.0

CHBrno g pq Tribromomethane gas r

u

v w

x yw z { - x | w

}~ x w

}~ v w

}~ w

298.15

330.669

15907.0

60000.0

31.272

50676.3

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

109

s 94TCRASt

s 94TCRASt

SGTE

110

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBr€ I  g ‚ ƒ Tribromoiodomethane gas „

‡

ˆ‰

Š-‹‰ Œ -  Š Ž‰

 Š‰

 ˆ‰

"‘ ‰

298.15

378.318

20856.0

170000.0

86.191

144302.0

C’ H € Br€ g ‚ƒ 1,1,1–Tribromoethane gas „

‡

ˆ ‰

Š ‹‰ Œ  - Š Ž ‰

 Š ‰

 ˆ ‰

"‘ ‰

298.15

354.233

19919.0

–4602.0

–81.586

19722.9

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

… 94TCRAS†

… 94TCRAS†

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeBr“D” Cerium Bromide •

˜

™š

›œ-š

›œ™š

›œ"žš

298.15 1005.00

182.004

–887008.0

–115.765

–852493.0

CeBr“¤ g ¥ ” Cerium Bromide gas •

˜

™š

›œš

›œ™š

›œžš

298.15

398.368

–597056.8

100.599

–627050.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

111

– 73Bar—

›Ÿ7 :¡-š

›Ÿ7 :¡™š

type

51881.6

51.623

™W¢Y£

– 93THDA—

SGTE

112

Thermodynamic Properties of Inorganic Materials: Pure Substances

CoBr¦§ g ¨ © Cobalt Tribromide gas ª

­

®¯

°-±¯ ²³ -  ° ´¯

µ¶ °¯

µ¶ ®¯

µ¶· ¯

298.15

377.778

19277.0

–26064.0

119.423

–61670.0

CrBr¦D© Chromium Tribromide ª

­

®¯

°±¯ ²³ -  ° ´¯

µ¶ °-¯

µ¶ ®¯

µ¶· ¯

298.15 1085.00

159.700

21020.0

–400000.0

–92.158

–372523.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

« 96TCRAS¬

« 94TCRAS¬

µ¸9¹:º °¯

µ¸7¹:º ®¯

60000.0

55.300

type

®W»Y¼

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CrBr½¾ g ¿ À Chromium Tribromide gas Á

Ä

ÅÆ

Ç-ÈÆ ÉÊ -  Ç ËÆ

ÌÍ ÇÆ

ÌÍ ÅÆ

ÌÍÎ Æ

298.15

382.779

19729.0

–141291.0

130.921

–180325.0

CuBr½¾ g ¿ÏÀ Copper Tribromide gas Á

Ä

Å Æ

ÌÍ Ç Æ

ÌÍ Å Æ

ÌÍÎ Æ

298.15

451.981

–151531.0

190.516

–208333.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

113

 94TCRASÃ

 91KnaÃ

SGTE

114

Thermodynamic Properties of Inorganic Materials: Pure Substances

CuÐ BrÐ@Ñ g Ò Ó Tricopper Tribromide gas Ô

×

ØÙ

Ú-ÛÙ ÜÝ -  Ú ÞÙ

ßà ÚÙ

ßà ØÙ

ßàá Ù

298.15

458.065

30231.0

–148561.0

130.300

–187410.0

DyBrÐÑ g Ò Ó Dysprosium Bromide gas Ô

×

Ø Ù

ßà Ú Ù

ßà Ø Ù

ßàá Ù

298.15

404.096

–540154.0

100.825

–570215.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Õ 96TCRASÖ

Õ 93THDAÖ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

ErBrâã g äå Erbium Bromide gas æ

é

êë

ìíîë

ìíêë

ìíïë

298.15

403.375

–546012.0

101.882

–576388.0

EuBrâ%å Europium Tribromide æ

é

ê ë

ìíî ë

ìíê ë

ìíï ë

298.15

182.841

–753120.0

–126.267

–715473.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

115

ç 93THDAè

ç 93THDAè

SGTE

116

Thermodynamic Properties of Inorganic Materials: Pure Substances

FeBrðòñ Iron Tribromide ó

ö

÷ø

ù-úø ûü -  ù ýø

þÿ ùø

þÿ ÷ø

þÿ
ø

298.15

173.000

21800.0

–262600.0

–82.595

–237974.0

FeBrð g Ïñ Iron Tribromide gas ó

ö

÷ ø

ù úø û ü - ù ý ø

þÿ ù ø

þÿ ÷ ø

þÿ
ø

298.15

380.234

19346.0

–121940.0

124.639

–159101.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ô 96TCRASõ

ô 96TCRASõ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

117

GaBr Gallium Bromide 

94SGTE







 




298.15 396.00

179.912

–386601.6

–89.130

–360027.0



 

11715.2

29.584

GaBr# g $% Gallium Bromide gas  



& ')(*

298.15

359.410

19037.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

 +

type

"!

94TCRAS

,

 



–292963.0

90.368

–319906.0

SGTE

118

Thermodynamic Properties of Inorganic Materials: Pure Substances

GdBr-/. Gadolinium Bromide 0

1 93THDA2

3

45

67
8&5

6745

67,95

298.15 1058.00

189.954

–828850.0

–106.450

–797112.0

GdBr-@? g AB. Gadolinium Bromide gas 0

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

6:;<)45

38136.7

36.046

type 4

=">

1 93THDA2

3

45

6785

6745

67
95

298.15

398.932

–531368.0

102.528

–561937.0

SGTE

6:;<8&5

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

GeBr
g  

 

298.15

363.167

18549.0

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

ve

AR

TS

PD

m are

ftw

F so



-



 94TCRAS

 

 



–119030.0

103.762

–149967.0

Tribromosilane gas 

 85JANAF





   

-







298.15

348.043

17823.8

–302921.6

35.578

–313529.0

Landolt-B¨ornstein New Series IV/19A

mo

Germanium Tribromide gas 



SiHBr
g 

sp art



119

SGTE

120

Thermodynamic Properties of Inorganic Materials: Pure Substances

HoBr Holmium Bromide

! 93THDA"

#

$%

&'( %

&'$%

&'*)+%

298.15 1192.00

194.138

–840984.0

–109.196

–808427.0

&,.-0/( %

&,.-0/$%

50082.1

42.015

type

$2143

InBr5 Indium Bromide #

$%

( 6% 78

298.15 693.00

175.000

24500.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

! 94TCRAS"

-

(9 %

&'*(%

&'$%

&')+%

–399000.0

–110.965

–365916.0

&+,:-0/(%

&,.-0/$%

26000.0

37.518

type

$2143

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

InBr;< g =?> Indium Bromide gas @ C

DE

F GE HI

298.15

373.471

19912.0

-

FJ E

A 94TCRASB

KL FE

KL DE

KLM E

–256588.0

87.506

–282678.0

IrBr;5> Iridium Tribromide @

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

A 94SGTEB

C

D E

KL F E

KL D E

KLM E

298.15

129.570

–176639.0

–134.250

–136612.0

Landolt-B¨ornstein New Series IV/19A

121

SGTE

122

Thermodynamic Properties of Inorganic Materials: Pure Substances

LaBrN5O Lanthanum Bromide P

Q 73BarR

S

TU

VWX U

VWTU

VW*Y+U

298.15 1061.00

182.004

–870272.0

–103.213

–839499.0

LaBrN_ g `aO Lanthanum Bromide gas P

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

VZ.[0\TU

53973.6

50.871

type

T2]4^

Q 93THDAR

S

TU

VWXU

VWTU

VWY+U

298.15

383.703

–603751.2

98.486

–633115.0

SGTE

VZ.[0\X U

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Lib Brbc g dae Trilithium Tribromide gas f i

jk

l mk no

298.15

401.346

26036.0

-

lp k

g 94TCRASh

qr lk

qr jk

qrs k

–824640.0

85.671

–850183.0

MoBrb5e Molybdenum Tribromide f

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

g 94TCRASh

i

j k

l mk n o l p k -

qr l k

qr j k

qrs k

298.15

170.000

24000.0

–284000.0

–86.875

–258098.0

Landolt-B¨ornstein New Series IV/19A

123

SGTE

124

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoBrtu g v?w Molybdenum Tribromide gas x {

|}

~ } €

298.15

373.220

18757.0

-

~‚ }

y 94TCRASz

ƒ„ ~}

ƒ+„ |}

ƒ„… }

–20000.0

116.345

–54688.3

NbBrt O u g v?w Niobium Tribromide Oxide gas x {

| }

~ } €  ~ ‚ } -

ƒ„ ~ }

ƒ„ | }

ƒ„… }

298.15

390.740

22230.0

–595000.0

23.581

–602031.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

y 94TCRASz

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

125

NdBr†5‡ Neodymium Bromide ˆ

‰ 93THDAŠ

‹

Œ

Ž

ŽŒ

Ž‘+

298.15 955.00

194.138

–873201.0

–105.263

–841817.0

Ž’.“0”*

Ž’.“0”Œ

45312.7

47.448

NiBr†— g ˜a‡ Nickel Tribromide gas ˆ ‹

Œ

 ™ š›

298.15

374.290

19105.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

-

œ 

type

Œ2•4–

‰ 96TCRASŠ

Ž*

ŽŒ

Ž*‘+

23299.0

116.179

–11339.8

SGTE

126

Thermodynamic Properties of Inorganic Materials: Pure Substances

POBrŸž g  a¡ Phosphorus Tribromide Oxide gas ¢ ¥

¦§

¨ ©§ ª«

298.15

359.841

19848.9

-

¨¬ §

£ 85JANAF¤

­® ¨§

­® ¦§

­®¯ §

–406559.3

–12.135

–402941.0

TaOBrž g  a¡ Tantalum Tribromide Oxide gas ¢ ¥

¦ §

¨ ©§ ª « ¨ ¬ § -

­® ¨ §

­® ¦ §

­®¯ §

298.15

397.733

22748.0

–611501.0

25.372

–619066.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

£ 94TCRAS¤

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

UOBr°± Uranium Tribromide Oxide ²

³ 91Kna´

µ

¶·

¸¹º·

¸¹¶·

¸¹»+·

298.15

205.016

–953998.0

–176.072

–901502.0

VOBr°¼ g ½?± Vanadium Tribromide Oxide gas ²

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

³ 94TCRAS´

µ

¶ ·

º ¾· ¿ À º Á · -

¸¹*º ·

¸¹¶ ·

¸¹» ·

298.15

380.081

21540.0

–509609.0

18.302

–515066.0

Landolt-B¨ornstein New Series IV/19A

127

SGTE

128

Thermodynamic Properties of Inorganic Materials: Pure Substances

PBrÂÃ g Ä?Å Phosphorus Bromide gas Æ É

ÊË

Ì ÍË ÎÏ

298.15

348.243

17752.7

-

ÌÐ Ë

Ç 85JANAFÈ

ÑÒ ÌË

ÑÒ ÊË

ÑÒÓ Ë

–145896.1

78.840

–169402.0

PBr S à g ÄaÅ Phosphorus Tribromide Sulphide gas Æ É

Ê Ë

Ì ÍË Î Ï Ì Ð Ë -

ÑÒ Ì Ë

ÑÒ Ê Ë

ÑÒÓ Ë

298.15

372.837

21187.8

–281039.3

71.363

–302316.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ç 85JANAFÈ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

129

PbBrÔÕ g Öa× Lead Tribromide gas Ø Û

ÜÝ

Þ ßÝ àá

298.15

385.248

19968.0

-

Þâ Ý

Ù 94TCRASÚ

ãä ÞÝ

ãä ÜÝ

ãäå Ý

–104010.0

92.133

–131479.0

PrBrÔ5× Praseodymium Bromide Ø Û

ÜÝ

ãä ÞÝ

ãä ÜÝ

ãäå Ý

298.15 966.00

192.464

–891192.0

–109.782

–858460.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ù 93THDAÚ ãæ.ç0è ÞÝ

ãæ.ç0è ÜÝ

47278.8

48.943

type

Ü2é4ê

SGTE

130

Thermodynamic Properties of Inorganic Materials: Pure Substances

PrBrëì g í?î Praseodymium Bromide gas ï

ð 93THDAñ

ò

óô

õö÷ô

õöóô

õöø+ô

298.15

401.154

–594546.4

98.908

–624036.0

PtBrë5î Platinum Tribromide ï ò

ó ô

õö÷ ô

õöó ô

õöø ô

298.15

179.912

–127612.0

–90.034

–100768.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ð 73Barñ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

131

PuBrù5ú Plutonium Bromideû

ü 73Barý

þ

ÿ




ÿ

 

298.15 954.00

191.209

–831779.2

–91.567

–804478.0

ReBrù5ú Rhenium Tribromide û

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

  ÿ

type

58576.0

61.400

ÿ

ü 94SGTEý

þ

ÿ




ÿ

 

298.15

184.096

–164431.2

–80.701

–140370.0

Landolt-B¨ornstein New Series IV/19A

  

SGTE

132

Thermodynamic Properties of Inorganic Materials: Pure Substances

RhBr Rhodium Tribromide 






!

"

 #

298.15

188.280

–210873.6

–71.591

–189529.0

SbBr Antimony Bromide 






!

"

 #

298.15 370.00

210.037

–259408.0

–63.800

–240386.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 73Bar

 94TCRAS

$%&!

$%&"

type

14644.0

39.578

'(

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SbBr)+* g ,.- Antimony Bromide gas /

2

3
4

56794 8":  5 4 - ;

<= 54

<= 34

<= > 4

298.15

374.536

19748.5

–194556.0

100.699

–224579.0

ScBr)- Scandium Bromide /

2

3 4

<= 5 4

<= 3 4

<= > 4

298.15

167.360

–745965.4

–95.599

–717463.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

133

0 84Pan1

0 94SGTE1

SGTE

134

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiBr?A@ g B.C Silicon Tribromide gas D

G

H
I

J6K9I L"M  J I - N

OP JI

OP HI

OP Q I

298.15

351.319

17461.0

–157000.0

104.194

–188065.0

SnBr?+@ g B.C Tin Tribromide gas D

G

H I

J K9I "L M J N I -

OP J I

OP H I

OPQ I

298.15

373.595

19280.0

–158716.0

94.100

–186772.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

E 94TCRASF

E 94TCRASF

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

TbBrR+S g T.U Terbium Bromide gas V

Z
[

\]^[

\]"Z[

\] _[

298.15

402.439

–540572.8

142.054

–582926.0

Y

Z [

^ `9[ "a b ^ c [ -

\]d^ [

\]"Z [

\] _ [

298.15

176.500

22970.0

–549000.0

–82.535

–524392.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

W 93THDAX

Y

TiBrRU Titanium Tribromide V

135

W 94TCRASX

SGTE

136

Thermodynamic Properties of Inorganic Materials: Pure Substances

TiBreAf g gih Titanium Tribromide gas j

m

n
o

p6q9o r"s  p o - t

uv po

uv no

uv w o

298.15

367.027

18999.0

–362971.0

107.992

–395169.0

TmBreAf g gxh Thulium Bromide gas j

m

n o

uv p o

uv n o

uvw o

298.15

401.188

–545593.6

98.858

–575068.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

k 94TCRASl

k 93THDAl

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

UBryz Uranium Tribromide {

~

€

‚ ƒ6€

‚"€

‚„€

298.15 1000.00

188.280

–720903.2

–90.235

–694000.0

VBryz Vanadium Tribromide {

~


€

‚ƒ€

‚"€

‚„€

298.15

142.256

–447688.0

–116.949

–412820.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

137

| 93THDA}

…†‡dƒ€

…†‡"€

type

43932.0

43.932

ˆ‰

| 93THDA}

SGTE

138

Thermodynamic Properties of Inorganic Materials: Pure Substances

VBrŠA‹ g Œ. Vanadium Tribromide gas Ž

‘

’
“

”•–“

”•"’“

”•—“

298.15

142.365

–447688.0

–116.840

–412852.0

WBrŠ˜‹ g Œx Tungsten Tribromide gas Ž

‘

’ “

– ™9“ "š › – œ “ -

”•d– “

”•"’ “

”•d— “

298.15

382.013

19324.0

60000.0

121.080

23900.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 94SGTE

 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

ZrBrž Zirconium Tribromide Ÿ

¢

£¤

¥¦9¤ §9¨  ¥ ¤ - ©

ª« ¥6¤

ª« £¤

ª«¬ ¤

298.15 1000.00

170.000

21000.0

–600000.0

–97.496

–570932.0

ZrBrA² g ³xž Zirconium Tribromide gas Ÿ

¢

£
¤

¥6¦9¤ §"¨  ¥ ¤ - ©

ª« ¥¤

ª« £¤

ª« ¬ ¤

298.15

378.767

19792.0

–340742.0

111.271

–373917.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

139

  94TCRAS¡

ª­®¯ ¥¤

ª­®¯ £¤

33000.0

33.000

type

£°±

  94TCRAS¡

SGTE

140

Thermodynamic Properties of Inorganic Materials: Pure Substances

CBr´+µ g ¶.· Carbon Tetrabromide gas ¸

»

¼
½

¾6¿9½ À"Á  ¾ ½ - Â

ÃÄ ¾½

ÃÄ ¼½

ÃÄdÅ ½

298.15

358.057

20365.0

120000.0

47.895

105720.0

CdÆ Br´Çµ g ¶.· Dicadmium Tetrabromide gas ¸

»

¼ ½

¾ ¿9½ "À Á ¾ Â ½ -

ÃÄ ¾ ½

ÃÄ ¼ ½

ÃÄÅ ½

298.15

487.284

31775.0

–291000.0

79.264

–314633.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¹ 94TCRASº

¹ 94TCRASº

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CoÈ BrÉ+Ê g Ë.Ì Dicobalt Tetrabromide gas Í

Ð

Ñ
Ò

Ó6Ô9Ò Õ"Ö  Ó Ò - ×

ØÙ ÓÒ

ØÙ ÑÒ

ØÙ Ú Ò

298.15

478.535

29865.0

–183707.0

114.035

–217707.0

CrBrÉ+Ê g Ë.Ì Chromium Tetrabromide gas Í

Ð

Ñ Ò

Ó Ô9Ò "Õ Ö Ó × Ò -

ØÙ Ó Ò

ØÙ Ñ Ò

ØÙÚ Ò

298.15

418.368

24493.0

–215000.0

90.405

–241954.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

141

Î 96TCRASÏ

Î 94TCRASÏ

SGTE

142

Thermodynamic Properties of Inorganic Materials: Pure Substances

CuÛ BrÜÇÝ g Þ.ß Dicopper Tetrabromide gas à

ã

ä
å

æ6ç9å è"é  æ å - ê

ëì æå

ëì äå

ëìdí å

298.15

449.060

28550.0

–65152.0

78.340

–88509.1

CuÜ BrÜÇÝ g Þ.ß Tetracopper Tetrabromide gas à

ã

ä å

æ ç9å "è é æ ê å -

ëì æ å

ëì ä å

ëì í å

298.15

564.761

42202.0

–236854.0

127.741

–274940.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

á 96TCRASâ

á 96TCRASâ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Feî Brï+ð g ñ.ò Diiron Tetrabromide gas ó

ö

÷
ø

ù6ú9ø û"ü  ù ø - ý

þÿ ùø

þÿ ÷ø

þÿ
ø

298.15

479.438

29412.0

–264640.0

120.458

–300555.0

Gaî BrïÇð g ñ.ò Digallium Tetrabromide gas ó

ö

÷ ø

ù ú9ø "û ü ù ý ø -

þÿ ù ø

þÿ ÷ ø

þÿ ø

298.15

471.802

30591.0

–415819.0

85.928

–441438.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

143

ô 96TCRASõ

ô 94TCRASõ

SGTE

144

Thermodynamic Properties of Inorganic Materials: Pure Substances

GeBr Germanium Bromide 



 

298.15 299.25

250.000

30300.0

-

 

 94TCRAS 



–348000.0





–85.510






co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so



12000.0





 

298.15

396.187

23963.0

-

 





–291000.0

 !



–322505.0

GeBr'& g () Germanium Bromide gas 

SGTE



40.100

type

#"%$

 94TCRAS 



60.677





–309091.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

HfBr*+ Hafnium Bromide ,

- 93THDA.

/

0 1

2341

2301

2351

298.15

238.488

–767346.0

–109.492

–734701.0

HfBr*76 g 89+ Hafnium Bromide gas , /

0 1

234

298.15

418.928

–656888.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

145

1

- 93THDA.

230 1

235

1

70.948

–678041.0

SGTE

146

Thermodynamic Properties of Inorganic Materials: Pure Substances

In: Br;'< g =9> Diindium Tetrabromide gas ? B

C D

ED FGH

ED I

298.15

496.369

31798.0

-

ED

JK

@ 94TCRASA JK

–436508.0

CD

76.649

D

JKL

–459361.0

Mg: Br;'< g =9> Dimagnesium Tetrabromide gas ? B

C D E

298.15

461.341

30965.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

D FGH

-

E I

D

JK

E

D

–767764.0

JK

C D

91.579

@ 85JANAFA JKL

D

–795068.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoBrMON Molybdenum Tetrabromide P S

T U

VU WXY

VU Z

298.15

217.000

29000.0

-

VU

[\

Q 94TCRASR [\

–304000.0

TU

–115.980

U

[\]

–269421.0

MoBrM'^ g _)N Molybdenum Tetrabromide gas P S

T U V

298.15

459.456

26310.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

U WXY

-

V Z

U

[\

V

U

–206000.0

147

[\

T U

126.476

Q 94TCRASR [\
]

U

–243709.0

SGTE

148

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ni` Bra'b g c)d Dinickel Tetrabromide gas e h

i j

kj lmn

kj o

298.15

470.330

29256.0

-

kj

pq

f 96TCRASg pq

–163702.0

ij

106.318

j

pq
r

–195401.0

PbBra'b g c9d Lead Tetrabromide gas e h

i j k

298.15

427.717

25871.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

j lmn

-

k o

j

pq

k

j

–182434.0

f 94TCRASg pq

i j

58.497

pqr

j

–199875.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

PtBrsOt Platinum Tetrabromideu

v 73Barw

x

y z

{|}z

{|yz

{|
~z

298.15

251.040

–140582.4

–95.011

–112255.0

SiBrsOt Silicon Bromide u

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

v 73Barw

x

y z

{|}

298.15

278.085

–461495.2

Landolt-B¨ornstein New Series IV/19A

149

z

{|y z

{|
~

z

–45.145

–448035.0

SGTE

150

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiBr'€ g )‚ Silicon Bromide gas ƒ †

‡ ˆ

‰ˆ Š‹Œ

298.15

379.368

22313.0

-

‰ˆ 

Ž

„ 94TCRAS… ‰ˆ

–415800.0

Ž

‡ˆ

56.138

Ž

ˆ

–432538.0

SnBrO‚ Tin Tetrabromide ƒ †

‡ ˆ

‰ˆ Š‹Œ

298.15 302.25

260.000

31260.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

‰ˆ 

„ 94TCRAS… Ž

‰ˆ

–388000.0

Ž

‡ˆ

–95.600

Ž


ˆ

Ž‘’“

‰ˆ

Ž‘ ’!“

‡ˆ

–359497.0 12150.0

40.199

type ‡#”%•

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

151

SnBr–˜— g ™)š Tin Tetrabromide gas › ž

Ÿ  

¡  ¢£¤

298.15

413.228

25043.0

-

¡  ¥

¦§

œ 94TCRAS

¡ 

¦§

–324217.0

Ÿ 

57.628

¦§¨

 

–341399.0

TeBr–Oš Tellurium Tetrabromide› ž

Ÿ  

298.15 653.00

243.509

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

¦§

¡ 

–194974.4

œ 73Bar ¦§

Ÿ 

–110.132

¦§¨

 

¦©ª!«

¡ 

¦©ª!«

Ÿ 

–162139.0 24685.6

37.803

type Ÿ­¬¯®

SGTE

152

Thermodynamic Properties of Inorganic Materials: Pure Substances

ThBr°²± Thorium Tetrabromide ³

´ 73Barµ

¶

· ¸

¹º»¸

¹º·¸

¹º¼¸

298.15 693.00 952.00

228.028

–965667.2

–128.192

–927447.0

ThBr°˜Ã g Ä)± Thorium Tetrabromide gas ³ ¶

· ¸ ¹

298.15

429.890

–760580.1

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

º »

¸ ¹

º · ¸

73.670

¹½¾!¿À»¸

¹½¾!¿·¸

4184.0 54392.0

6.038 57.134

type ·­Á%· ·­Á¯Â

´ 93THDAµ ¹

º ¼

¸

–782545.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

153

TiBrÅOÆ Titanium TetrabromideÇ Ê

Ë Ì

ÍÌ ÎÏÐ

298.15 311.40

243.600

28610.0

-

ÍÌ Ñ

ÒÓ

È 94TCRASÉ ÍÌ

–618000.0

ÒÓ

ËÌ

–91.540

Ì

ÒÓ
Ô

12890.0

Ê

Ë Ì

ÍÌ ÎÏÐ

298.15

400.407

23913.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ÍÌ

-

ÍÌ Ñ

ÒÓ

ÍÌ

–549697.0

ÒÕ Ö!×

ËÌ

–590707.0

TiBrÅ'Ú g ÛÜÆ Titanium Tetrabromide gas Ç

sp art

ÒÕÖ×

41.394

type Ë#Ø%Ù

È 94TCRASÉ ÒÓ

ËÌ

65.267

ÒÓÔ

Ì

–569156.0

SGTE

154

Thermodynamic Properties of Inorganic Materials: Pure Substances

UBrÝOÞ Uranium Tetrabromide ß

à 73Bará

â

ã ä

åæçä

åæãä

åæèä

298.15 792.15

234.304

–826340.0

–120.316

–790468.0

UBrÝ'î g ï)Þ Uranium Tetrabromide gas ß

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

åéê!ëãä

55228.8

69.720

type ã­ì¯í

à 93THDAá

â

ã ä

åæçä

åæãä

åæ
èä

298.15

458.559

–593299.6

103.939

–624289.0

SGTE

åéê!ëÀçä

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

VBrð'ñ g ò)ó Vanadium Tetrabromide gas ô

õ 94SGTEö

÷

ø ù

úûüù

úûøù

úûýù

298.15

334.829

–393296.0

–0.481

–393153.0

WBrðó Tungsten Tetrabromide ô ÷

ø ù ü

298.15

228.000

32000.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ù þÿ


-

ü



ù

úûÀü

155

õ 94TCRASö ù

–265000.0

úûø ù

úûý

ù

–109.038

–232490.0

SGTE

156

Thermodynamic Properties of Inorganic Materials: Pure Substances 

WBr g  



 


298.15

456.957

26675.0

Zn Br g 

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so



 

-





94TCRAS



–155000.0



119.919



–190754.0

Dizinc Tetrabromide gas 





298.15

466.761

30612.0

SGTE

sp art

Tungsten Tetrabromide gas 




-

 





–469742.0

96TCRAS





79.079



–493319.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

157

ZrBr"! Zirconium Bromide# &

'(

)( *+
,

298.15 723.00

220.000

27000.0

-

)( -

$ 94TCRAS% ./

)(

–759500.0

./

'(

–123.601

./0

(

30000.0

&

'(

)( *+
,

298.15

414.480

24953.4

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

)(

-

)( -

./

)(

–644754.4

.17365

'(

type

–722648.0

ZrBr< g =>! Zirconium Bromide gas #

sp art

.214365

41.494

'98;:

$ 85JANAF% ./

'(

70.879

./0

(

–665887.0

SGTE

158

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoBr?@ g ACB Molybdenum Pentabromide gas D G

HI

JI KL
M

298.15

449.404

28021.0

-

JI N

OP

JI

OP

–220000.0

HI

E 94TCRASF

40.319

OPQ

I

–232021.0

NbBr?RB Niobium PentabromideD G

HI

298.15 527.00

258.780

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

OP

JI

–556053.6

E 85JANAFF OP

HI

–158.015

OPQ

I

OS7T6U

JI

OS7T6U

HI

–508941.0 24016.2

45.572

type H9V;W

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

159

NbBrXY g Z\[ Niobium Pentabromide gas ] `

ab

cb de
f

298.15

449.253

29426.1

-

cb g

hi

cb

^ 85JANAF_ hi

–443587.7

ab

32.458

hij

b

–453265.0

TaBrXR[ Tantalum Pentabromide] `

ab

298.15 513.00

305.432

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

hi

cb

–598312.0

^ 73Bar_ hi

ab

–116.565

hij

b

hk7l6m

cb

hk7l6m

ab

–563558.0 37656.0

73.404

type a9n;o

SGTE

160

Thermodynamic Properties of Inorganic Materials: Pure Substances

TaBrpq g rCs Tantalum Pentabromide gas t w

xy

zy {|
}

zy ~

298.15

457.685

30125.0

-

€

zy

u 94TCRASv €

–485000.0

xy

35.688

€

–495640.0

UBrpRs Uranium Pentabromidet w

x y

298.15

292.880

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

€

z

y

–810858.8

y

u 93THDAv €

x y

–137.845

€

y

–769760.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

161

VBr‚ƒ g „C… Vanadium Pentabromide gas † ‰

Š‹

Œ‹ Ž


298.15

437.898

28512.0

-

Œ‹ 

‘’

Œ‹

‡ 94TCRASˆ ‘’

–393753.0

Š‹

26.483

‘’“

‹

–401649.0

WBr‚”… Tungsten Pentabromide† ‰

Š‹

298.15 559.00

271.960

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

‘’

Œ‹

–311708.0

‡ 85JANAFˆ ‘’

Š‹

–141.183

‘’“

‹

‘•7–6—

Œ‹

‘•7–6—

Š‹

–269614.0 17154.4

30.688

type Š9˜;™

SGTE

162

Thermodynamic Properties of Inorganic Materials: Pure Substances

WBršœ› g >ž Tungsten Pentabromide gas Ÿ ¢

£¤

¥¤ ¦§
¨

¥¤ ©

298.15

461.404

30020.2

-

¥¤

ª«

  85JANAF¡ ª«

–199158.4

£¤

48.261

¤

ª«¬

–213547.0

C­ Br®› g >ž Hexabromoethane gas Ÿ ¢

£ ¤ ¥

298.15

461.785

31880.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¤ ¦§
¨

-

¥ ©

¤

ª«

¥

¤

–133051.0

  94TCRAS¡ ª«

£ ¤

–6.329

ª«¬

¤

–131164.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Fe¯ Br°± g ²C³ Diiron Hexabromide gas ´ ·

¸¹

º¹ »¼
½

º¹ ¾

298.15

595.811

41483.0

-

º¹

¿À

µ 96TCRAS¶ ¿À

–386089.0

¸¹

84.621

¹

¿ÀÁ

–411319.0

Ga¯ Br°± g ²C³ Digallium Hexabromide gas ´ ·

¸ ¹ º

298.15

568.118

41151.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¹ »¼
½

-

º ¾

¹

¿À

º

¹

–673689.0

163

¿À

µ 94TCRAS¶ ¸ ¹

30.034

¿ÀÁ

¹

–682644.0

SGTE

164

Thermodynamic Properties of Inorganic Materials: Pure Substances

In BrÃÄ g Å>Æ Diindium Hexabromide gas Ç Ê

ËÌ

ÍÌ ÎÏ
Ð

ÍÌ Ñ

298.15

603.447

43096.0

-

ÍÌ

ÒÓ

È 94TCRASÉ ÒÓ

–628684.0

ËÌ

31.517

Ì

ÒÓÔ

–638081.0

MoBrÃÄ g ÅCÆ Molybdenum Hexabromide gas Ç Ê

Ë Ì Í

298.15

487.944

35205.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ì ÎÏ
Ð

-

Í Ñ

Ì

ÒÓ

Í

Ì

–180000.0

ÒÓ

Ë Ì

2.754

È 94TCRASÉ ÒÓÔ

Ì

–180821.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

WBrÕ”Ö Tungsten Hexabromide ×

Ø 85JANAFÙ

Ú

ÛÜ

ÝÞßÜ

ÝÞ
ÛÜ

ÝÞà2Ü

298.15

313.800

–343088.0

–175.448

–290778.0

WBr՜á g â>Ö Tungsten Hexabromide gas × Ú

Û Ü ß

298.15

482.692

35204.2

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ü ãä
å

-

ß æ

Ü

ÝÞçß

165

Ü

–243090.4

Ø 85JANAFÙ ÝÞ
Û Ü

ÝÞà

Ü

–6.556

–241136.0

SGTE

166

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaCN
Calcium Cyanamide 



 

   - 

   

 

 

298.15

81.588

12100.0

–157.353

–303704.0

–350619.0

CaCO
Calcium Carbonate



 

   - 

   

 

 

298.15 1603.0

91.71

14480.0

–263.340

–1128090.0

SGTE co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–1206600.0

 93Bar

 

 94TCRAS    type

36000.0

22.458

!#"

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdCO$% Cadmium Carbonate&

* +

,-/.+

,-* +

,-0+

298.15

92.466

–751864.8

–272.796

–670531.0

)

* +

. 4+ 5 6 - . 7 + ,-8. +

,-/* +

,-/0 +

298.15

224.552

9396.0

107.271

407577.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

' 73Bar(

)

CCl 1 g 23% Carbon Monochloride gas &

439560.0

167

' 94TCRAS(

SGTE

168

Thermodynamic Properties of Inorganic Materials: Pure Substances

CClF 9 g :3; Chlorofluoromethylene gas <

?

@ A

BCA DE -  B F A GH BA

GH @A

GH/I A

298.15

259.032

10929.0

40.356

13843.9

25876.0

CHClF 9 g :J; Chlorofluoromethyl gas <

?

@ A

B CA D E - B F A GH B A

GH @ A

GH/I A

298.15

268.502

11146.0

–15.514

–78515.5

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–83141.0

= 94TCRAS>

= 94TCRAS>

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHClFI K g LJM Chlorofluoroiodomethane gas N

Q

R S

TUS VW -  T X S YZ TS

YZ RS

YZ[ S

298.15

313.013

14062.0

–29.073

–166332.0

–175000.0

CH\ ClF K g LJM Chlorofluoromethane gas N

Q

R S

T US V W - T X S YZ T S

YZ R S

YZ[ S

298.15

264.421

11252.0

–84.935

–244677.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–270000.0

169

O 94TCRASP

O 94TCRASP

SGTE

170

Thermodynamic Properties of Inorganic Materials: Pure Substances

CClFI]_^ g `ba Chlorofluorodiiodomethane gas c

f

g h

ijh kl -  i m h no ih

no gh

no8p h

298.15

359.089

18426.0

24.274

–77237.3

–70000.0

COClF ^ g `Ja Carbonyl Fluoride Chloride gas c

f

g h

i jh k l - i m h no i h

no g h

nop h

298.15

277.023

11903.5

–44.227

–413582.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–426768.0

d 94TCRASe

d 85JANAFe

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CClFqsr g t3u Chlorodifluoromethyl gas v

y

z {

|}{ ~ -  | € { ‚ |{

‚ z{

‚ƒ {

298.15

287.348

12432.0

–32.722

–265244.0

–275000.0

CHClFq_r g t3u Chlorodifluoromethane gas v

y

z {

| }{ ~  - | € { ‚ | {

‚ z {

‚/ƒ {

298.15

280.915

12367.0

–104.495

–443845.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–475000.0

171

w 94TCRASx

w 94TCRASx

SGTE

172

Thermodynamic Properties of Inorganic Materials: Pure Substances

CClF„ I … g †3‡ Chlorodifluoroiodomethane gas ˆ

‹

Œ 

Ž ‘ -  Ž ’  “” Ž

“” Œ

“”• 

298.15

329.098

16207.0

–49.042

–365378.0

–380000.0

CClF–s… g †3‡ Chlorotrifluoromethane gas ˆ

‹

Œ 

Ž   ‘ - Ž ’  “” Ž 

“” Œ 

“”/• 

298.15

285.419

13791.0

–136.046

–667238.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–707800.0

‰ 94TCRASŠ

‰ 94TCRASŠ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHCl — g ˜J™ Chloromethylene gas š



ž Ÿ

 ¡Ÿ ¢£ -    ¤ Ÿ ¥¦  Ÿ

¥¦ žŸ

¥¦8§ Ÿ

298.15

234.880

10154.0

52.258

292699.0

308280.0

CHClI¨©— g ˜3™ Chlorodiiodomethane gas š



ž Ÿ

  ¡Ÿ ¢ £ -   ¤ Ÿ ¥¦   Ÿ

¥¦ ž Ÿ

¥¦8§ Ÿ

298.15

342.806

15820.0

44.046

96867.8

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

110000.0

173

› 94TCRASœ

› 94TCRASœ

SGTE

174

Thermodynamic Properties of Inorganic Materials: Pure Substances

COHCl ª g «­¬ Formylchloride gas ®

±

² ³

´µ³ ¶· -  ´ ¸ ³ ¹º ´³

¹º ²³

¹º» ³

298.15

259.065

11006.0

–26.130

–156417.0

–164208.0

CH¼ Cl ª g «3¬ Chloromethyl gas ®

±

² ³

´ µ³ ¶ · - ´ ¸ ³ ¹º ´ ³

¹º ² ³

¹º8» ³

298.15

243.475

10980.0

–4.486

118210.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

116872.0

¯ 94TCRAS°

¯ 94TCRAS°

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CH½ ClI ¾ g ¿­À Chloroiodomethane gas Á

Ä

Å Æ

ÇÈÆ ÉÊ -  Ç Ë Æ ÌÍ ÇÆ

ÌÍ ÅÆ

ÌÍ/Î Æ

298.15

295.546

12508.0

–10.485

8126.1

5000.0

CHÏ Cl ¾ g ¿3À Chloromethane gas Á

Ä

Å Æ

Ç ÈÆ É Ê - Ç Ë Æ ÌÍ Ç Æ

ÌÍ Å Æ

ÌÍ/Î Æ

298.15

234.392

10416.0

–78.910

–58343.1

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

–81870.0

175

 94TCRASÃ

 94TCRASÃ

SGTE

176

Thermodynamic Properties of Inorganic Materials: Pure Substances

CClIÐ_Ñ g ÒbÓ Chlorotriiodomethane gas Ô

×

Ø Ù

ÚÛÙ ÜÝ -  Ú Þ Ù ßà ÚÙ

ßà ØÙ

ßà8á Ù

298.15

385.465

21037.0

93.975

196981.0

225000.0

ClCN Ñ g Ò3Ó Cyanogen Chloride gas Ô

×

Ø Ù

Ú ÛÙ Ü Ý - Ú Þ Ù ßà Ú Ù

ßà Ø Ù

ßà8á Ù

298.15

236.334

10685.9

23.247

131015.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

137946.5

Õ 94TCRASÖ

Õ 85JANAFÖ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

COCl â g ãJä Carbonyl Monochloride gas å

è

é ê

ëìê íî -  ë ï ê ðñ ëê

ðñ éê

ðñ8ò ê

298.15

265.190

11551.0

45.335

–29516.6

–16000.0

CClósâ g ã3ä Carbon Dichloride gas å

è

é ê

ë ìê í î - ë ï ê ðñ ë ê

ðñ é ê

ðñ8ò ê

298.15

265.030

11461.0

36.209

215434.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

226230.0

177

æ 94TCRASç

æ 94TCRASç

SGTE

178

Thermodynamic Properties of Inorganic Materials: Pure Substances

CClô F õ g ö3÷ Dichlorofluoromethyl gas ø

û

ü ý

þÿ
ý  - þ ý



þý

298.15

298.911

13217.0

–105000.0



–31.305

CHClô F õ g ö3÷ Dichlorofluoromethane gas ø

û

ü ý

þ ÿ
ý  - þ  ý



298.15

293.302

13294.0

–280000.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

þ ý

üý



üý

–102.253

 

ù 94TCRASú ý

–95666.6

 

ý

ù 94TCRASú

–249513.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CCl FI g  Dichlorofluoroiodomethane gas  



 


 

298.15

341.560

17381.0

-







–180000.0

 

–46.725

 94TCRAS  !



–166069.0

CCl F" g  Dichlorodifluoromethane gas  

  

298.15

300.902

14881.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 


-

 









–486000.0



179

 94TCRAS  

–130.708

 !



–447029.0

SGTE

180

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHCl#%$ g &(' Dichloromethyl gas ) ,

-.

/. 0
12

/. 3

298.15

277.830

12360.0

-

* 94TCRAS+

/.

45

45

73895.0

- .

–16.331

.

4576

78764.1

CHCl# I $ g &' Dichloroiodomethane gas ) ,

- . /

298.15

324.118

14906.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

. 0
12

-

/ 3

.

45

/

.

5000.0

45

* 94TCRAS+ - .

–28.112

45 6

.

13381.7

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CH8 Cl8:9 g ;< Dichloromethane gas = @

AB

CB D
EF

CB G

298.15

270.359

11854.0

-

HI

CB

> 94TCRAS? HJI

–95000.0

A B

–89.142

HI K

A B

298.15

329.181

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

HI

C

B

–428441.6

HI

A B

–179.810

HI K

B

–68422.3

SiH(CHL )Cl8M9 g ;< Methyldichlorosilane gas = @

181

> 94SGTE? B

–374831.0

SGTE

182

Thermodynamic Properties of Inorganic Materials: Pure Substances

CClN IN"O g PQ Dichlorodiiodomethane gas R U

VW

XW Y
Z[

XW \

298.15

362.090

19407.0

-

XW

]^

S 94TCRAST

]J^

115000.0

V W

17.130

]^7_

W

109893.0

COClN%O g P(Q Phosgene gas R U

V W X

298.15

283.852

12865.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

W Y
Z[

-

X \

W

S 85JANAFT ]^

X

W

–220078.4

]^

V W

–47.542

]^ _

W

–205904.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CCl`"a g bc Carbon Trichloride gas d g

hi

ji k
lm

ji n

298.15

300.330

13939.0

-

e 94TCRASf

ji

op

op

80000.0

h i

op7q

–40.030

i

91935.1

CCl` F a g bc Trichlorofluoromethane gas d g

h i j

298.15

309.779

16063.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

i k
lm

-

j n

i

op

j

183

i

–285000.0

e 94TCRASf op

h i

–131.976

op q

i

–245651.0

SGTE

184

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHClr%s g t(u Trichloromethane gas v y

z{

|{ }
~

|{ €

298.15

296.353

14302.0

-

‚

w 94TCRASx

|{

z {

‚

–102700.0

‚ ƒ

–109.347

–70098.0

Si u CHr„v Clr"s g tu Methyltrichlorosilane gas v y

z {

298.15

351.147

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

‚

|

{

–606680.0

‚

z {

–204.043

‚ ƒ

{

w 94SGTEx {

–545844.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CCl… I † g ‡ˆ Trichloroiodomethane gas ‰ Œ

Ž

Ž 
‘’

Ž “

298.15

340.604

18282.0

-

”•

Ž

Š 94TCRAS‹ ”•

10000.0

 Ž

”•7–

–57.826

 Ž

298.15

216.396

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

”•



Ž

–128005.0

Ž

27240.8

CCl—˜ˆ Carbon Tetrachloride‰ Œ

185

Š 94SGTE‹ ”•

 Ž

–235.504

”• –

Ž

–57789.5

SGTE

186

Thermodynamic Properties of Inorganic Materials: Pure Substances

CCl™Mš g ›œ Carbon Tetrachloride gas   

¡¢

£¢ ¤
¥¦

298.15

309.461

17158.0

-

£¢ §

¨©

£¢

ž 94TCRASŸ ¨J©

–95600.0

¡ ¢

¨© ª

–142.439

–53131.8

CoCO«¬œ Cobalt Carbonate  

¡ ¢

298.15

88.701

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¨©

£

¢

–711280.0

¢

ž 73BarŸ ¨J©

¡ ¢

–254.802

¨© ª

¢

–635311.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

187

Cs­ CO®°¯ Cesium Carbonate± ´

µ¶

·¶ ¸¹
º

298.15 1066.0

204.47

25727.0

-

·¶ »

² 94TCRAS³ ¼½

·¶

–1134900.0

¼½

µ ¶

–279.452

¶

¼½ ¾

31000.0

´

µ¶

·¶ ¸
¹º

298.15

388.519

21179.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

·¶

-

·¶ »

¼½

·¶

–806448.0

¼¿ÁÀÃÂ

µ¶

–1051580.0

Cs­ CO®"Ç g ȯ Cesium Carbonate gas ±

sp art

¼¿ÁÀÃÂ

29.081

type µÄÆÅ

² 94TCRAS³ ¼½

µ ¶

–95.404

¼½ ¾

¶

–778003.0

SGTE

188

Thermodynamic Properties of Inorganic Materials: Pure Substances

CuCN É Copper Cyanide gas Ê Í

ÎÏ

ÐÏ ÑÒ
Ó

ÐÏ Ô

298.15

90.002

12052.0

-

Ë 85JANAFÌ ÕÖ

ÐÏ

ÕÖ

94977.0

Î Ï

ÕÖ ×

–44.695

108303.0

CuCOØ°É Copper CarbonateÊ Í

Î Ï

298.15

87.864

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ÕÖ

Ð

Ï

–596220.0

Ï

Ë 73BarÌ ÕJÖ

Î Ï

–258.748

ÕÖ ×

Ï

–519074.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CF Ù g ÚÛ Carbon Monofluoride gas Ü ß

àá

âá ã
äå

298.15

213.031

9065.0

âá æ

-

âá

çè

Ý 94TCRASÞ çJè

244072.0

à á

105.895

á

çè é

212500.0

CHF Ù g ÚêÛ Fluoromethylene gas Ü ß

à á â

298.15

234.870

9982.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

á ã
äå

-

â æ

á

çè

189

â

Ý 94TCRASÞ á

105286.0

çJè

à á

62.394

çè7é

á

86683.4

SGTE

190

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHFIë%ì g í(î Fluorodiiodomethane gas ï ò

óô

õô ö
÷ø

õô ù

298.15

332.720

14759.0

-

õô

úû

ð 94TCRASñ úJû

–65000.0

ó ô

44.104

úû7ü

ô

–78149.8

COHF ì g íêî Formylfluoride gas ï ò

ó ô õ

298.15

246.802

10443.3

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ô ö
÷ø

-

õ ù

ô

úû

õ

ð 85JANAFñ ô

–376560.0

úû

ó ô

–28.248

úû ü

ô

–368138.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances




Fluoromethyl gas     -    

   

298.15

236.524

–1.293

CHý F þ g ÿ

10592.0

–32000.0




Fluoroiodomethane gas     -         

298.15

286.264

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–165000.0

–9.622

 94TCRAS

–31614.6

CHý FI þ g ÿ

11968.0

191

 94TCRAS

–162131.0

SGTE

192

Thermodynamic Properties of Inorganic Materials: Pure Substances

  
 Fluoromethane gas ! "# $ % # &' - $( # )* $#

)* "#

)*,+ #

298.15

–80.335

–231048.0

CH F g

222.822

10135.0

–255000.0

- g
  Fluorotriiodomethane gas ! "# $ % # &' - $ ( # )* $ # )* " # )*+ #

CFI

298.15

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

373.196

19825.0

45000.0

91.851

 94TCRAS

 94TCRAS

17614.6

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

. /
0 Cyanogen Fluoride gas1 4 56 7 8 6 9: - 7; 6 <= 76 <= 56 <=> 6

FCN g

298.15

225.401

10271.7

35982.4

22.459

. /?0 Carbonyl Monofluoride gas1 4 56 7 8 6 9: - 7 ; 6 <= 7 6 <= 5 6 <=> 6 248.484

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

10393.1

–171544.0

38.774

2 85JANAF3

29286.2

COF g

298.15

193

2 85JANAF3

–183104.0

SGTE

194

Thermodynamic Properties of Inorganic Materials: Pure Substances

@-A g
B C Carbon Difluoride gasD G HI J K I LM - JN I OP JI

OP HI OPQ I

298.15

32.297

CF

240.828

10355.4

–182004.0

OP H I

OP,Q I

298.15

–15.370

–249417.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–191633.0

@RA g S B C Difluoromethyl gasD G HI J K I LM - J N I OP J I

CHF

258.501

11051.0

–254000.0

E 85JANAFF

E 94TCRASF

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

T U S V W Difluoroiodomethane gasX [ \] ^ _ ] `a - ^b ] cd ^] cd \]

cd,e ]

298.15

–357236.0

CHF I g

305.900

13855.0

–365000.0

T T-U g
V W Difluoromethane gasX [ \] ^ _ ] `a - ^ b ] cd ^ ]

cd \ ]

cd,e ]

298.15

–92.518

–423074.0

CH F

246.693

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–26.041

10690.1

–450658.6

195

Y 94TCRASZ

Y 85JANAFZ

SGTE

196

Thermodynamic Properties of Inorganic Materials: Pure Substances

f f-g g S h i Difluorodiiodomethane gasj m no p q o rs - pt o uv po uv no uvw o

CF I

298.15

346.507

17604.0

–260000.0

21.837

uv,w o

298.15

–623330.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–266511.0

fRg g S h i Carbonyl Difluoride gasj m no p q o rs - p t o uv p o uv n o

COF

258.894

11116.9

–638896.8

–52.210

k 94TCRASl

k 85JANAFl

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

x-y g
z { Carbon Trifluoride gas|  € ‚ ƒ  „… - ‚†  ‡ˆ ‚

‡ˆ €

‡ˆ,‰ 

298.15

–44.847

–456910.0

CF

265.078

11522.7

–470281.6

xRy g S z { Trifluoromethane gas|  € ‚ ƒ  „… - ‚ †  ‡ˆ ‚ 

‡ˆ € 

‡ˆ‰ 

298.15

–115.591

–662236.0

CHF

259.674

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

11565.0

–696700.0

197

} 85JANAF~

} 94TCRAS~

SGTE

198

Thermodynamic Properties of Inorganic Materials: Pure Substances

Š Š ‹
Œ  Trifluoromethylsilane gasŽ ‘ ’“ ”•–“ ”•’“ ”•—“

 93THDA

CF H Si g

298.15

314.202

–1232711.0

–210.553

–1169930.0

Š ‹ Œ
 Trifluoroiodomethane gasŽ ‘ ’“ – ˜ “ ™š - – › “ ”•– “ ”•’ “

”•,— “

298.15

–571246.0

CF I g

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

307.777

15025.0

–589200.0

–60.218

 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

œž g
Ÿ   Tetrafluoromethane gas¡ ¤ ¥¦ § ¨ ¦ ©ª - §« ¦ ¬­ §¦

¬­ ¥¦

¬­® ¦

298.15

–149.866

–888517.0

CF

261.454

12730.0

–933200.0

¯ 
Ÿ   Trifluoromethyl Oxygen Fluoride gas¡ ¤ ¥¦ § ¨ ¦ ©ª - § « ¦ ¬­ § ¦ ¬­ ¥ ¦ ¬­® ¦

CF OF g

298.15

322.533

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

13702.6

–764835.2

–191.360

199

¢ 94TCRAS£

¢ 85JANAF£

–707781.0

SGTE

200

Thermodynamic Properties of Inorganic Materials: Pure Substances

° ±ž² g
³ ´ Trifluoromethyl Sulphur Pentafluoride gasµ ¸ ¹º » ¼ º ½¾ - »¿ º ÀÁ »º ÀÁ ¹º ÀÁ º

CF SF

298.15

379.301

24083.1

ÀÁ ¹ º

ÀÁ, º

298.15

–247.857

–666669.0

SGTE

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–469.667

°Ã´ Iron Carbonateµ ¸ ¹º ÀÁ » º

FeCO

sp art

–1717050.8

92.885

–740568.0

¶ 85JANAF·

–1577020.0

¶ 94SGTE·

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ä Å
Æ Methine gasÇ Ê ËÌ Í Î Ì ÏÐ - ÍÑ Ì ÒÓ ÍÌ

ÒÓ ËÌ

ÒÓÔ Ì

298.15

111.955

563991.0

CH g

183.037

8625.0

597370.0

ÕÖÄ g × Å Æ Triiodomethane gasÇ Ê ËÌ Í Î Ì ÏÐ - Í Ñ Ì ÒÓ Í Ì

ÒÓ Ë Ì

ÒÓÔ Ì

298.15

110.256

187127.0

CHI

355.546

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

17113.0

220000.0

201

È 94TCRASÉ

È 94TCRASÉ

SGTE

202

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ø ?Ù Ú Hydrogen Isocyanate gasÛ ßà á â à ãä - áå à æç áà æç ßà

HNCO g

Þ

298.15

NaHCO

Þ

298.15 800.00

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

238.225

10962.1

–101671.2

–31.236

éêÚ Sodium Hydrogen CarbonateÛ ßà á â à ãä - áå à æç áà æç ßà 101.700

15940.0

–950810.0

–328.403

Ü 85JANAFÝ

æç,è à –92358.2

æçè à

æëíìïî áà æëðìïî ßà

–852897.0 25000.0

31.250

Ü 94SGTEÝ type

ßòñôó

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

õ öø÷ Formyl gasù ü ýþ ÿ þ - ÿþ



298.15

42000.0

HCO g




224.338



9989.0

õ ?ö ÷ Carboxyl gasù ýþ ÿ þ -ÿ þ

COOH g

ü

298.15




251.731

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

10813.0





ÿþ

ÿþ

–213000.0



ýþ



50.682



203

ú 94TCRASû þ

26889.0

ýþ

–24.498



þ

ú 94TCRASû

–205696.0

SGTE

204

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHP g  Methinophosphide gas  



 

298.15

215.062

9351.2

 

-

 85JANAF





 

149912.7

!

121.130



 "

131258.0

CH#$ g % Methylene gas  

  

298.15

194.895

9939.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 

-

 

 94TCRAS 







390421.0

 

 

58.473

&"



372987.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CH' I'$( g )%* Diiodomethane gas + .

/0

10 234

10 5

298.15

309.945

13243.0

-

, 94TCRAS10

67

6 7

121000.0

/!0

57.384

67&8

0

103891.0

H' CO ( g )%* Formaldehyde gas + .

/ 0 1

298.15

218.760

10020.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

0 234

-

1 5

0

67

205

1

, 94TCRAS0

–108700.0

67

/ 0

–20.236

678

0

–102667.0

SGTE

206

Thermodynamic Properties of Inorganic Materials: Pure Substances

HCOOH 9 Formic Acid :

; 93THDA<

=

>?

@A B?

@A>!?

@A C ?

298.15

128.993

–422793.2

–212.576

–359414.0

CHD$E g F%9 Methyl gas : =

> ? B

298.15

193.956

10365.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

? GHI

; 94TCRAS<

-

B J

?

@A&B

?

146300.0

@ A > ?

@A&C ?

–7.806

148627.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHK I L g M%N Iodomethane gas O R

ST

UT VWX

UT Y

298.15

253.906

10815.0

-

P 94TCRASQ UT

Z[

Z[

14400.0

S!T

–5.925

Z[ \

T

16166.7

CH]^L g M%N Methane gas O

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

P 94TCRASQ

R

S T U

298.15

186.368

10016.0

Landolt-B¨ornstein New Series IV/19A

T VWX

-

207

U Y

T

Z[

U

T

–74600.0

Z [

S T

–80.734

Z[ \

T

–50529.2

SGTE

208

Thermodynamic Properties of Inorganic Materials: Pure Substances

CH_ OH ` Methanol a

b 73Barc

d

ef

gh if

ghe!f

gh j f

298.15

126.692

–238697.2

–242.983

–166252.0

CH_ OH k g l` Methanol gas a d

e f i

298.15

239.865

11441.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

f mno

-

i p

f

b 94TCRASc gh&i

f

–201000.0

ghe f

gh j f

–129.810

–162297.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CI q g r%s Carbon Monoiodide gas t w

xy

zy {|}

298.15

241.315

9494.0

zy ~

-

u 94TCRASv

zy

€

 €

570201.0

x!y

177.504

y

€ 

517278.0

ICN q g r%s Cyanogen Iodide gas t w

x y z

298.15

257.338

11468.3

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

y {|}

-

z ~

y

€

209

z

u 85JANAFv y

225936.0

 €

x y

97.721

€&

y

196800.0

SGTE

210

Thermodynamic Properties of Inorganic Materials: Pure Substances

CI‚$ƒ g „%… Carbon Diiodide gas † ‰

Š‹

Œ‹ Ž

Œ‹ 

298.15

304.318

12643.0

-

‡ 94TCRASˆ Œ‹

‘’

‘ ’

468397.0

Š!‹

182.437

‹

‘’ “

414003.0

CI”$ƒ g „%… Carbon Triiodide gas † ‰

Š ‹ Œ

298.15

361.026

16831.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

‹ Ž

-

Œ 

‹

‘’

Œ

‡ 94TCRASˆ ‹

405987.0

‘ ’

Š ‹

181.076

‘’ “

‹

351999.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CI•^– g —%˜ Tetraiodomethane gas ™ œ

ž

Ÿž  ¡¢

Ÿž £

298.15

391.891

22331.0

-

š 94TCRAS› Ÿž

¤¥

¤ ¥

340000.0

!ž

153.871

ž

¤¥ ¦

294123.0

IrC – g —%˜ Iridium Monocarbide gas ™ œ

 ž Ÿ

298.15

239.309

8752.9

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ž  ¡¢

-

Ÿ £

ž

¤¥

211

Ÿ

ž

761655.4

š 93THDA› ¤ ¥

 ž

198.062

¤¥ ¦

ž

702603.0

SGTE

212

Thermodynamic Properties of Inorganic Materials: Pure Substances

KCN § Potassium Cyanide ¨ «

¬­

®­ ¯°±

298.15 895.00

127.779

17342.7

-

®­ ²

© 85JANAFª ³´

®­

³´

–113470.1

¬!­

³´µ

–38.449

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

³¶¸·¸¹

®­

14644.0

«

¬­

®­ ¯°±

298.15

253.145

12455.8

-

®­ ²

³´

®­

79496.0

³ ¶º·»¹

¬!­

–102007.0

KCN À g Á§ Potassium Cyanide gas ¨

SGTE

­

16.362

type ¬½¼¿¾

© 85JANAFª ³´

¬!­

86.918

³´ µ

­

53581.5

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

213

KÂ COÃÅÄ Potassium CarbonateÆ É

ÊË

ÌË ÍÎÏ

298.15 693.00 1173.0

155.5

22665.0

-

ÌË Ð

Ç 94TCRASÈ ÌË

ÑÒ

Ñ Ò

–1151500.0

Ê!Ë

–287.322

Ë

ÑÒÓ

Ñ ÔºÕ»Ö

2100.0 27614.4

É

ÊË

ÌË ÍÎÏ

298.15

345.638

19516.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

ÌË Ð Ñ

Ò

ÌË

–811649.0

ÑÔ¸Õ»Ö

Ê!Ë

–1065830.0

KÂ COÃÜÛ g ÝÞÄ Potassium Carbonate gas Æ

sp art

ÌË

3.030 23.542

type Ê×ØÊ Ê×ÚÙ

Ç 94TCRASÈ Ñ

Ò

Ê!Ë

–97.185

Ñ

Ò Ó

Ë

–782673.0

SGTE

214

Thermodynamic Properties of Inorganic Materials: Pure Substances

Liß COàâá Lithium Carbonateã

ä 94SGTEå

æ

ç!è

éê ëè

éêç!è

éê&ì è

298.15 623.00 683.00 1005.00

90.165

–1215870.0

–281.537

–1131930.0

éí¸î¸ï&ëè

é íºî»ï ç!è

560.7 2238.4 44768.8

0.900 3.277 44.546

type çñðòç çñðòç çñð¿ó

MgCOàôá Magnesium Carbonateã æ

çè

ëè õö÷

298.15 1263.0

65.09

11630.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

ëè ø

é

ê ëè

–1096000.0

ä 94TCRASå é ê ç!è

é

ê ì è

–281.043

–1012210.0

é íºî»ï ëè

é

í¸î»ï ç!è

59000.0

46.714

type çùÚó

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MnCOúÅû Manganese Carbonateü







  


 


298.15

85.772

–894957.6

–259.910

–817465.0




ÿ

298.15

202.643

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ý 67Kubþ

ÿ

CN g %û Carbon Nitride gas ü

215

ý 94TCRASþ

 
   
-




 





8672.0

440287.0

101.096

410145.0

SGTE

216

Thermodynamic Properties of Inorganic Materials: Pure Substances

NaCN Sodium Cyanide






      - 

 

 

 

298.15 835.00

118.467

19422.0

–90709.0

–34.377

–80459.4

NaCN ! g "





298.15

243.363

SGTE co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Sodium Cyanide gas


      - 

 

 

 

12125.2

94265.5

90.516

67278.3

 

 

8786.0

10.522

 98JANAF type

 

 85JANAF

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CNO # g $&% Carbon Nitride Oxide gas '

+,

- . , /0  - , - 1

23 -,

23 +,

2354 ,

298.15

232.381

10221.0

177496.0

28.260

169070.0

*

+,

-. , / 0  - , - 1

23 - ,

23 +,

234 ,

298.15 723.15 1123.15

138.796

20811.2

-1130767.8

-277.266

-1048100

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

( 94TCRAS)

*

Na6 CO78% Sodium Carbonate'

217

29:; -,

( 85JANAF) 29:; +,

690.4 29664.6

0.955 26.412

type

+ <=+ +

SGTE

218

Thermodynamic Properties of Inorganic Materials: Pure Substances

NiCO@BA Nickel CarbonateC

F

GH

IJKH

IJGH

IJMLH

298.15

85.354

–679900.0

–257.904

–603006.0

CO N g OPA Carbon Monoxide gas C

F

G H

K Q H R S K T H -

IJ5K H

IJG H

IJL H

298.15

197.665

8673.4

–110528.7

89.350

–137168.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

D 73BarE

D 85JANAFE

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

COS U g VPW Carbon Oxide Sulphide gas X

[

\]

^ _ ] `a  ^ ] - b

cd ^]

cd \]

cde ]

298.15

231.644

9942.0

–141700.0

91.258

–168909.0

COfgU g VPW Carbon Dioxide gas X

[

\ ]

^ _ ] ` a ^ b ] -

cd ^ ]

cd \ ]

cde ]

298.15

213.783

9365.0

–393510.0

2.894

–394373.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

219

Y 94TCRASZ

Y 94TCRASZ

SGTE

220

Thermodynamic Properties of Inorganic Materials: Pure Substances

PbCOh8i Lead Carbonatej

m

no

pqro

pqno

pqso

298.15

130.959

–699146.4

–247.303

–625413.0

Rbt COh8i Rubidium Carbonatej

m

no

ruo v w r o - x

pqro

pqno

pqso

298.15 576.00 1146.0

181.33

24480.0

–1132600.0

–285.684

–1047420.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

k 67Kubl

pyz{5ro

k 94TCRASl pyz{no

1300.0 30000.0

2.257 26.178

type

n |=n n |?}

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SrCO~€ Strontium Carbonate

„

…†

‡ˆ† ‰ Š  ‡ † - ‹

Œ ‡ †

Œ …†

ŒMŽ †

298.15 1198.0 1767.0

97.20

15120.0

–1226000.0

–271.956

–1144920.0

ZnCO~8 Zinc Carbonate

„

…†

Œ  ‡†

Œ  …†

Œ Ž †

298.15

82.425

–812742.0

–272.668

–731446.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

221

Œ‘’ ‡†

‚ 94TCRASƒ Œ’ …†

16700.0 40000.0

13.940 22.637

type

… “”… … “=•

‚ 94SGTEƒ

SGTE

222

Thermodynamic Properties of Inorganic Materials: Pure Substances

PbCO–g— PbO ˜ Lead Carbonate—Lead Oxide (1/1) ™

œ

ž

Ÿ ¡ž

Ÿ ž

Ÿ ¢ž

298.15

204.179

–816716.8

–341.457

–714911.0

CP £ g ¤P˜ Carbon Monophosphide gas ™

œ

 ž

¡ ¥ ž ¦ § ¡ ¨ ž -

Ÿ 5¡ ž

Ÿ  ž

Ÿ ¢ ž

298.15

216.254

8715.0

520162.0

169.421

469649.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

š 73Bar›

š 94TCRAS›

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CP©gª g «P¬ Carbon Diphosphide gas ­

°

±²

³´µ²

³´±²

³´¶²

298.15

263.919

402082.4

175.999

349608.0

CS ª g «P¬ Carbon Monosulphide gas ­

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

® 94SGTE¯

°

± ²

µ · ² ¸ ¹ µ º ² -

³´5µ ²

³´± ²

³´¶ ²

298.15

210.554

8708.0

279775.0

172.742

228272.0

Landolt-B¨ornstein New Series IV/19A

223

® 94TCRAS¯

SGTE

224

Thermodynamic Properties of Inorganic Materials: Pure Substances

CS»8¼ Carbon Disulphide ½

À

ÁÂ

ÃÄÅÂ

ÃÄÁÂ

ÃÄÆÂ

298.15

151.335

89412.1

81.453

65126.9

CS»gÇ g Èɼ Carbon Disulphide gas ½

À

Á Â

Å Ê Â Ë Ì Å Í Â -

ÃÄ5Å Â

ÃÄÁ Â

ÃÄÆ Â

298.15

237.882

10664.0

116700.0

168.000

66610.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¾ 67Kub¿

¾ 94TCRAS¿

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CSe Î g ÏÉÐ Carbon Monoselenide gas Ñ

Ô

ÕÖ

× Ø Ö ÙÚ  × Ö - Û

ÜÝ ×Ö

ÜÝ ÕÖ

ÜÝÞ Ö

298.15

222.740

8761.3

364091.7

175.032

311906.0

CSeßàÎ g ÏPÐ Carbon Diselenide gas Ñ

Ô

Õ Ö

× Ø Ö Ù Ú × Û Ö -

ÜÝ × Ö

ÜÝ Õ Ö

ÜÝÞ Ö

298.15

263.450

11757.0

242839.4

173.776

191028.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

225

Ò 93THDAÓ

Ò 93THDAÓ

SGTE

226

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiC áâ – Silicon Carbideã

æ

çè

éêè ë ì é è - í

îï éè

îï çè

îïð è

298.15

16.485

3252.0

–71546.0

–8.067

–69140.8

SiC áMñ – Silicon Carbideã

æ

ç è

é êè ë ì é í è -

îï é è

îï ç è

îïð è

298.15

16.610

327.0

–73220.0

–7.942

–70852.1

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ä 85JANAFå

ä 85JANAFå

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiC ò g óPô Silicon Carbide gas õ

ø

ùú

û ü ú ýþ  û ú - ÿ


ûú


ùú


 ú

298.15

226.209

9217.0

734950.0

201.657

674826.0

Si C ò g óÉô Disilicon Carbide gas õ

ø

ù ú

û ü ú ý þ û ÿ ú -


û ú


ù ú


 ú

298.15

261.895

11582.0

554098.0

218.533

488942.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

227

ö 94TCRAS÷

ö 94TCRAS÷

SGTE

228

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaC  Calcium Dicarbide











298.15 720.00

70.291

–59412.8

17.219

–64546.6

 94SGTE





type

5564.7

7.729



CaCO"! MgCO# Calcium Carbonate—Magnesium Carbide (1/1) $&%('*)'&+-,.0/*









1

298.15

117.989

–2326304.0

–583.195

–2152420.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 93THDA

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeC2#3 Cerium Dicarbide4

7

89

:;<9

:;89

:;=9

298.15

79.078

–62760.0

–1.860

–62205.4

C2 Cl > g ?@3 Dicarbon Monochloride gas 4

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

5 94SGTE6

7

8 9

< AC9 B D - < E 9

:;1< 9

:;8 9

:;= 9

298.15

241.943

10780.0

534090.0

118.920

498634.0

Landolt-B¨ornstein New Series IV/19A

229

5 94TCRAS6

SGTE

230

Thermodynamic Properties of Inorganic Materials: Pure Substances

CF ClF G g H@I Chlorofluoroacetylene gas J

M

NO

PQRCO ST -  P UO

VW PO

VW NO

VWX O

298.15

266.381

13876.0

33773.0

41.963

21261.7

CF ClFYZG g H@I Chlorotrifluoroethylene gas J

M

N O

P RCO S T - P U O

VW P O

VW N O

VWX O

298.15

322.383

17128.0

–515200.0

–104.824

–483947.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

K 94TCRASL

K 94TCRASL

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C[ HCl \ g ]@^ Chloroacetylene gas _

b

cd

eQfCd gh -  e id

jk ed

jk cd

jk1l d

298.15

241.991

11786.3

213802.4

53.627

197813.0

C[ H m Cl \ g ]@^ Chloroethylene gas _

b

c d

e fCd g h - e i d

jk e d

jk c d

jk1l d

298.15

264.019

11819.0

23000.0

–55.025

39405.6

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

231

` 85JANAFa

` 94TCRASa

SGTE

232

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cn ClnZo g prq Dichloroacetylene gas s

v

wx

yQzCx {| -  y }x

~ yx

~ wx

~1€ x

298.15

272.023

14564.5

209618.4

37.460

198450.0

Cn H ClnZo g p@q 1,1–Dichloroethane gas s

v

w x

y zCx { | - y } x

~ y x

~ w x

~€ x

298.15

305.170

15445.0

–130122.0

–190.753

–73249.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

t 85JANAFu

t 94TCRASu

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C‚ ClƒZ„ g …r† Dicarbon Trichloride gas ‡

Š

‹Œ

QŽCŒ  -   ‘Œ

’“ Œ

’“ ‹Œ

’“” Œ

298.15

328.160

16150.0

190279.0

–17.942

195629.0

C‚ Clƒ F „ g …@† Trichlorofluoroethylene gas ‡

Š

‹ Œ

 ŽCŒ   -  ‘ Œ

’“  Œ

’“ ‹ Œ

’“” Œ

298.15

342.587

18732.0

–166000.0

–104.910

–134721.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

233

ˆ 94TCRAS‰

ˆ 94TCRAS‰

SGTE

234

Thermodynamic Properties of Inorganic Materials: Pure Substances

C• Cl– F–Z— g ˜r™ Trichlorotrifluoroethane gas š



žŸ

 ¡¢Ÿ

 ¡žŸ

 ¡£Ÿ

298.15

364.410

–742241.6

–285.876

–657008.0

C• HCl –"— g ˜@™ Trichloroethylene gas š



ž Ÿ

¢ ¤CŸ ¥ ¦ - ¢ § Ÿ

 ¡1¢ Ÿ

 ¡ž Ÿ

 ¡£ Ÿ

298.15

324.960

16610.0

–19100.0

–86.482

6684.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

› 93THDAœ

› 94TCRASœ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C¨ H © Cl©Zª g «@¬ 1,1,1–Trichloroethane gas ­

°

±²

³Q´C² µ¶ -  ³ ·²

¸¹ ³²

¸¹ ±²

¸¹º ²

298.15

320.137

18000.0

–142298.0

–221.985

–76113.0

C¨ Cl»¼ª g «r¬ Tetrachloroethylene gas ­

°

± ²

³ ´C² µ ¶ - ³ · ²

¸¹ ³ ²

¸¹ ± ²

¸¹½º ²

298.15

343.415

19911.7

–12426.5

–114.227

21630.3

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

235

® 94TCRAS¯

® 85JANAF¯

SGTE

236

Thermodynamic Properties of Inorganic Materials: Pure Substances

C¾ H ¾ Cl¿¼À g Á@ 1,1,1,2–Tetrachloroethane gas Ã

Æ

ÇÈ

ÉQÊCÈ ËÌ -  É ÍÈ

ÎÏ ÉÈ

ÎÏ ÇÈ

ÎÏÐ È

298.15

355.971

20402.0

–149369.0

–232.351

–80093.5

C¾ ClÑZÀ g Ár Pentachloroethyl gas Ã

Æ

Ç È

É ÊCÈ Ë Ì - É Í È

ÎÏ É È

ÎÏ Ç È

ÎÏÐ È

298.15

396.502

23964.0

39000.0

–172.679

90484.4

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ä 94TCRASÅ

Ä 94TCRASÅ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CÒ HCl Ó"Ô g Õ@Ö Pentachloroethane gas ×

Ú

ÛÜ

ÝQÞCÜ ßà -  Ý áÜ

âã ÝÜ

âã ÛÜ

âãä Ü

298.15

381.542

23351.0

–145603.0

–252.979

–70177.2

CÒ ClåZÔ g ÕrÖ Hexachloroethane gas ×

Ú

Û Ü

Ý ÞCÜ ß à - Ý á Ü

âã Ý Ü

âã Û Ü

âãä Ü

298.15

398.624

27129.0

–141500.0

–282.097

–57392.8

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

237

Ø 94TCRASÙ

Ø 94TCRASÙ

SGTE

238

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cæ F ç g è@é Dicarbon Fluoride gas ê

í

îï

ðQñCï òó -  ð ôï

õö ðï

õö îï

õö÷ ï

298.15

231.031

10367.0

388855.0

118.153

353628.0

Cæ HF ç g è@é Fluoroacetylene gas ê

í

î ï

ð ñCï ò ó - ð ô ï

õö ð ï

õö î ï

õö÷ ï

298.15

231.569

11446.0

41700.0

53.350

25793.5

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ë 94TCRASì

ë 94TCRASì

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cø H ù F ú g û@ü Fluoroethylene gas ý

298.15




     -

 




 

252.669

11336.0

–140100.0

–56.229

–123335.0

Cø H  F ú g û@ü Fluoroethane gas ý

298.15




     -

  




 

265.092

12834.0

–263174.0

–174.486

–211151.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

239

þ 94TCRASÿ

þ 94TCRASÿ

SGTE

240

Thermodynamic Properties of Inorganic Materials: Pure Substances

C F g  Difluoroacetylene gas 





!"# $  ! - %

&' !

&' 

&'(

298.15

249.565

13266.0

–144659.0

35.292

–155181.0

C H) F* g  1,1–Difluoroethane gas 

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 94TCRAS





! "# $ ! % -

&' !

&' 

&'(

298.15

282.529

13972.0

–500825.0

–193.104

–443251.0

SGTE

sp art

 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C+ F,- g ./ Dicarbon Trifluoride gas 0

3

45

675 8 9  6 5 - :

;< 65

;< 45

;<= 5

298.15

297.638

14163.0

–228174.0

–18.029

–222799.0

C+ HF,- g .>/ Trifluoroethylene gas 0

3

4 5

6 75 8 9 6 : 5 -

;< 6 5

;< 4 5

;<= 5

298.15

292.659

14327.0

–491000.0

–88.349

–464659.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

241

1 94TCRAS2

1 94TCRAS2

SGTE

242

Thermodynamic Properties of Inorganic Materials: Pure Substances

C? H @ F@*A g BC 1,1,1–Trifluoroethane gas D

G

HI

JKI L M  J I - N

OP JI

OP HI

OPQ I

298.15

287.405

15287.0

–745589.0

–224.282

–678719.0

CF@ CN A g B>C Trifluoroacetonitrile gas D

G

H I

J KI L M J N I -

OP J I

OP H I

OPQ I

298.15

298.529

15895.0

–495385.6

–112.944

–461711.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

E 94TCRASF

E 85JANAFF

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CR FSUT g VW Tetrafluoroethylene gas X

[

\]

^_] ` a  ^ ] - b

cd ^]

cd \]

cde ]

298.15

300.010

16330.2

–658561.6

–117.052

–623663.0

CR H R FST g VW 1,1,1,2–Tetrafluoroethane gas X

[

\ ]

^ _] ` a ^ b ] -

cd ^ ]

cd \ ]

cde ]

298.15

316.319

16951.0

–895794.0

–231.423

–826795.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

243

Y 85JANAFZ

Y 94TCRASZ

SGTE

244

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cf Fgh g ij Pentafluoroethyl gas k

n

op

qrp s t  q p - u

vw qp

vw op

vwx p

298.15

348.690

19098.0

–896000.0

–169.766

–845384.0

Cf HFgh g i>j Pentafluoroethane gas k

n

o p

q rp s t q u p -

vw q p

vw o p

vwyx p

298.15

333.832

18735.0

–1104576.0

–249.964

–1030050.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

l 94TCRASm

l 94TCRASm

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cz F{| g }~ Hexafluoroethane gas 

‚

ƒ„

…†„ ‡ ˆ  … „ - ‰

Š‹ …„

Š‹ ƒ„

Š‹yŒ „

298.15

332.185

20254.7

–1343900.8

–287.666

–1258130.0

CCH | g }~ Ethynyl gas 

‚

ƒ „

… †„ ‡ ˆ … ‰ „ -

Š‹ … „

ŠŽ‹ ƒ „

Š‹Œ „

298.15

209.734

9856.0

569000.0

132.910

529373.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

245

€ 85JANAF

€ 94TCRAS

SGTE

246

Thermodynamic Properties of Inorganic Materials: Pure Substances

CHCN  g ‘ Methine Cyanide gas ’

•

–—

˜™— š ›  ˜ — - œ

ž ˜—

Žž –—

žyŸ —

298.15

240.591

11866.0

610438.0

67.962

590175.0

C  H  * g >‘ Ethyne ¡£¢¥¤§¦*¨ª©¬« ¦­®¦¯¡ gas ’

•

– —

˜ ™— š › ˜ œ — -

ž ˜ —

Žž – —

žyŸ —

298.15

200.926

10009.0

227400.0

58.762

209880.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

“ 94TCRAS”

“ 94TCRAS”

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C° H ° O ± g ²>³ Oxirene gas ´

·

¸¹

º»¹ ¼ ½  º ¹ - ¾

¿À º¹

¿ŽÀ ¸¹

¿ÀyÁ ¹

298.15

245.556

11925.0

170000.0

0.819

169756.0

C° H Â*± g ²>³ Ethenyl gas ´

·

¸ ¹

º »¹ ¼ ½ º ¾ ¹ -

¿À º ¹

¿ŽÀ ¸ ¹

¿ÀyÁ ¹

298.15

232.839

10283.0

260000.0

25.335

252446.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

247

µ 94TCRAS¶

µ 94TCRAS¶

SGTE

248

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cà HÄÅ g Æ>Ç Ethene ÈÊÉËÍÌÏάÐÑÒÓÑ¯È gas Ô

×

ØÙ

ÚÛÙ Ü Ý  Ú Ù - Þ

ßà ÚÙ

ßà ØÙ

ßàyá Ù

298.15

219.316

10518.0

52400.0

–53.528

68359.4

Cà HÄ OÃâÇ Acetic Acid Ô

×

Ø Ù

ßà Ú Ù

ßà Ø Ù

ßàá Ù

298.15

159.829

–484089.0

–318.162

–389229.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Õ 94TCRASÖ

Õ 93THDAÖ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cã H ä*å g æ>ç Ethyl gas è

ë

ìí

îïí ð ñ  î í - ò

óô îí

óŽô ìí

óôõ í

298.15

250.521

11810.0

107000.0

–87.663

133137.0

Cã H ä I å g æ>ç Iodoethane gas è

ë

ì í

î ïí ð ñ î ò í -

óô î í

óô ì í

óôõ í

298.15

295.630

13844.0

–8368.0

–100.623

21632.9

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

249

é 94TCRASê

é 94TCRASê

SGTE

250

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cö H ÷*ø g ù>ú Ethane gas û

þ

ÿ


  -

 

 ÿ

 

298.15

229.161

11884.0

–84000.0

–174.363

–32013.7

Cö H  OH ú Ethanol û

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ü 93THDAý

þ

ÿ

 

 ÿ

 

298.15

160.707

–277608.4

–345.390

–174630.0

SGTE

sp art

ü 94TCRASý

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C H  OH  g  Ethanol gas 






!"# $ -

% & 

% & 

% &' 

298.15

281.621

14126.0

–234800.0

–224.476

–167872.0

Si(CH( ) O  g ) Dimethylsiloxane gas 



 

% & 

% &  

% &' 

298.15

304.705

–184096.0

–220.202

–118443.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

251

 94TCRAS

 93THDA

SGTE

252

Thermodynamic Properties of Inorganic Materials: Pure Substances

C* H + O*-, Ethyleneglycol .

1

2
3

4 56 3

4 523

4 573

298.15

166.942

–454926.3

–441.729

–323225.0

C* H + O*98 g :), Ethyleneglycol gas .

1

2 3

4 56 3

4 52 3

4 57 3

298.15

323.658

–389321.2

–285.013

–304345.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

/ 99THDA0

/ 99THDA0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiH; (CH< );9= g >@? Dimethylsilane gas A

E
F

G HI F

GHE
F

G HJF

298.15

300.102

–71964.8

–252.912

3440.9

D

E F

I KF L M I N F -

G HOI F

G HE F

G HJ F

298.15

373.126

24786.0

–8368.0

40.671

–20494.1

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

B 93THDAC

D

K; (CN);9= g >@? Dipotassium Dicyanide gas A

253

B 85JANAFC

SGTE

254

Thermodynamic Properties of Inorganic Materials: Pure Substances

CP NP9Q g RTS Dicyanogen gas U

X

Y
Z

[\Z ]^ [ Z - _

` a [ Z

`a YZ

` aOb Z

298.15

242.201

12715.0

309100.0

39.106

297441.0

NaPcS CN UdP9Q g R)S Disodium Dicyanide gas U

X

Y Z

[ \Z ] ^ [ _ Z -

` a [ Z

` a Y Z

` ab Z

298.15

347.097

23179.4

–8786.4

41.402

–21130.4

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

V 94TCRASW

V 85JANAFW

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ce O f g g)h Dicarbon Monoxide gas i

l

m
n

opn qr o n - s

t u o n

tu mn

t uv n

298.15

233.608

10483.0

291043.0

119.551

255399.0

Ce P f g g)h Dicarbon Monophosphide gas i

l

m n

t u o n

tu m n

t uv n

298.15

242.183

636804.8

189.609

580273.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

255

j 94TCRASk

j 94SGTEk

SGTE

256

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cw Pw9x g y@z Dicarbon Diphosphide gas {

~


€

 ‚ƒ €

‚
€

 ‚„€

298.15

277.622

431914.3

183.958

377067.0

Si(CH… )… Cl x g y)z Trimethylchlorosilane gas {

~

 €

 ‚ƒ €

 ‚ €

 ‚„ €

298.15

361.774

–354384.8

–373.861

–242918.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

| 94SGTE}

| 94SGTE}

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C† O ‡‰ˆ g Š)‹ Tricarbon Dioxide gas Œ




‘

’“‘ ”• ’ ‘ - –

— ˜ ’ ‘

—˜ ‘

— ˜O™ ‘

298.15

276.642

13945.0

–97600.0

54.269

–113780.0

Si(CH† )š›ˆ g ŠT‹ Tetramethylsilane gas Œ



 ‘

— ˜ ’ ‘

— ˜  ‘

— ˜™ ‘

298.15

361.189

–286604.0

–464.669

–148063.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

257

 94TCRASŽ

 94SGTEŽ

SGTE

258

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cœ N  g ž)Ÿ 3–Cyano–2–Propynylidyne gas  

£

¤
¥

¦§¥ ¨© ¦ ¥ - ª

« ¬ ¦ ¥

«¬ ¤¥

« ¬­ ¥

298.15

285.004

15516.0

790000.0

166.231

740438.0

Cœ N®9 g žTŸ 2–Butynedinitrile gas  

£

¤ ¥

¦ §¥ ¨ © ¦ ª ¥ -

« ¬ ¦ ¥

«¬ ¤ ¥

« ¬O­ ¥

298.15

290.119

17736.0

533460.0

75.540

510938.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¡ 94TCRAS¢

¡ 85JANAF¢

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ni ¯ CO °²±-¯ Nickel Tetracarbonyl °

µ

¶
·

¸¹· º» ¸ · - ¼

½ ¾ ¸ ·

½ ¾ ¶·

½ ¾¿ ·

298.15

319.561

33934.0

–631784.0

–143.497

–589000.0

Ni ¯ CO °²±9À g Á)¯ Nickel Tetracarbonyl gas °

µ

¶ ·

¸ ¹· º » ¸ ¼ · -

½ ¾ ¸ ·

½ ¾ ¶ ·

½ ¾¿ ·

298.15

415.505

30493.0

–601575.5

–47.553

–587398.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

259

³ 93THDA´

³ 85JANAF´

SGTE

260

Thermodynamic Properties of Inorganic Materials: Pure Substances

Fe  CO ÃdÄÅ Iron Pentacarbonyl Ã

È

É
Ê

Ë ÌÍ Ê

Ë ÌÉÊ

Ë ÌÎÊ

298.15

337.649

–763998.4

–231.209

–695064.0

Fe  CO ÃdÄÐÏ g Ñ) Iron Pentacarbonyl gas Ã

È

É Ê

Í ÒÊ Ó Ô Í Õ Ê -

Ë ÌOÍ Ê

Ë ÌÉ Ê

Ë ÌÎ Ê

298.15

439.287

33145.6

–727848.6

–129.570

–689217.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Æ 73BarÇ

Æ 85JANAFÇ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CÖ N × g Ø)Ù 4–Cyano–1,3–Butadiynyl gas Ú

Ý

Þ
ß

àáß âã à ß - ä

å æ à ß

åæ Þß

å æç ß

298.15

304.559

18370.0

830000.0

180.044

776320.0

Cè H Ö Cl Ù Monochlorobenzol Ú

Ý

Þ ß

å æ à ß

å æ Þ ß

å æç ß

298.15

194.100

11698.5

–278.591

94760.6

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

261

Û 94TCRASÜ

Û 93THDAÜ

SGTE

262

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cé H ê Cl ë g ì)í Monochlorobenzol gas î

ñ

ò
ó

ô õö ó

ô õòó

ô õ÷ó

298.15

297.424

52772.8

–175.267

105029.0

SiH í Cé Hêøî Clù9ë g ì)í Phenyldichlorosilane gas î

ñ

ò ó

ô õö ó

ô õò ó

ô õ÷ ó

298.15

392.359

–266520.8

–276.022

–184225.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ï 93THDAð

ï 94SGTEð

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Si ú Cû Hüøý Clþ9ÿ g )ú Phenyltrichlorosilane gas ý





  

  

 

298.15

420.936

–468608.0

–293.644

–381058.0

Cr ú CO ý²û ú Chromium Hexacarbonyl ý



 

  

   

  

298.15

320.076

–928848.0

–353.360

–823494.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

263


94SGTE


73Bar

SGTE

264

Thermodynamic Properties of Inorganic Materials: Pure Substances

C H  Benzene





  

  

 

298.15

171.540

49036.5

–254.952

125050.0

C H  g ! Benzene gas 



 

  

   

  

298.15

269.308

82926.9

–157.184

129791.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 91Kna

 69Stu

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

C" H " O # g $!% Phenol gas &

)

*+

, -. +

,- *+

, -0/+

298.15

315.709

–96358.0

–213.356

–32745.8

Mo % CO &1"2% Molybdenum Hexacarbonyl &

)

* +

, -. +

, - * +

, -/ +

298.15

327.189

–984495.2

–351.264

–879766.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

265

' 93THDA(

' 67Kub(

SGTE

266

Thermodynamic Properties of Inorganic Materials: Pure Substances

Mo CO
 g 

Molybdenum Hexacarbonyl gas








 



298.15

490.110

–912098.6

–188.343

–855944.0

W CO
 Tungsten Hexacarbonyl






298.15

332.210

–951860.0

SGTE co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so



 93THDA

 91Kna

 

 

–350.301

–847418.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaCl g




Calcium Monochloride gas 



 

298.15

241.632

CaCl(OH) g




 

298.15

300.311

Landolt-B¨ornstein New Series IV/19A co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so



   

 - 

 

 

 

9595.0

–103773.0

88.505

–130161.0

Calcium Chloride Hydroxide gas 

     -

 

  

 

15665.0

–548229.0

–20.730

–542048.0

267

 94TCRAS

 94TCRAS

SGTE

268

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaCl Calcium Chloride 

298.15 1045.0

! "

#$" %&  # " - '

() #"

() !"

()* "

108.368

15273.0

–795390.0

–156.299

–748789.0

CaCl65 g 78 Calcium Chloride gas 

298.15

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

! "

#$" %&  # " - '

() #"

() !"

()* "

290.257

15116.8

–471536.8

25.590

–479166.0

(,+.-0/ #"

 94CODATA (+1-0/ !"

28547.0

27.318

type

!243

 85JANAF

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaCl9 O : Calcium Dichloride Oxide ;

? @

ABC@

AB?@

ABD,@

298.15

112.968

–746425.6

–254.273

–670614.0

>

? @

C H@ I J C K @ -

ABLC @

AB? @

ABD @

298.15

229.134

9132.0

–276403.0

86.151

–302089.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

< 73Bar=

>

CaF E g FG: Calcium Monofluoride gas ;

269

< 94TCRAS=

SGTE

270

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaF(OH) M g NPO Calcium Fluoride Hydroxide gas Q

T

U V

WXV YZ  W V - [

\] WV

\] UV

\]^ V

298.15

290.526

15040.0

–688676.0

–20.370

–682603.0

CaF_`O Calcium Fluoride Q

T

U V

WXV YZ  W V - [

\] WV

\,] UV

\]^ V

298.15 1424.0 1691.0

68.45

11640.0

–1228000.0

–175.927

–1175550.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

R 94TCRASS

\,a.b0c WV

R 96TCRASS \a1b0c UV

0.0 30000.0

0.000 17.741

type

UdeU Ud4f

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaFgih g jGk Calcium Fluoride gas l

p q

rsq tu  r q - v

wx rq

wx pq

wxy q

298.15

273.793

12656.6

–784500.0

29.416

–793270.0

o

pq

wx rq

wx pq

w,xy q

298.15 1489.00

145.185

–1476533.6

–361.257

–1368820.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

m 85JANAFn

o

CaO z Feg O{k Calcium Oxide—Diiron Trioxide (1/1) l

271

m 73Barn

w,|.}0~ rq

w|1}0~ pq

type

108365.6

72.777

p€‚

SGTE

272

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaO ƒ GeO„†… Calcium Oxide—Germanium Oxide (1/1) ‡

Š

‹ Œ

ŽŒ

Ž‹Œ

Ž,Œ

298.15

87.362

–1285324.0

–293.037

–1197960.0

CaH ‘ g ’P… Calcium Monohydride gas ‡

Š

‹ Œ

 “Œ ” •  – Œ -

ŽL Œ

,Ž‹ Œ

ŽL Œ

298.15

201.842

8705.0

229409.0

94.914

201110.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ˆ 91Kna‰

ˆ 94TCRAS‰

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaI(OH) — g ˜š™ Calcium Hydroxide Iodide gas ›

ž

Ÿ  

¡¢  £¤  ¡   - ¥

¦§ ¡ 

¦§ Ÿ 

¦§¨  

298.15

319.795

16181.0

–394721.0

52.224

–410292.0

Ca(OH) — g ˜P™ Calcium Monohydroxide gas ›

ž

Ÿ  

¡ ¢  £ ¤ ¡ ¥   -

¦§ ¡  

¦§ Ÿ  

¦§¨  

298.15

238.849

11050.0

–173260.0

29.347

–182010.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

273

œ 94TCRAS

œ 94TCRAS

SGTE

274

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaSO©iª¬­« H­ O ® Calcium Sulphite—Water (1/ ­« ) ¯

²

³ ´

µ¶·´

µ¶³´

µ¶L¸,´

298.15

121.298

–1311700.8

–376.707

–1199390.0

CaHPO¹® Calcium Hydrogen Phosphate ¯

²

³ ´

µ ¶· ´

µ ¶³ ´

µ ¶¸ ´

298.15

111.378

–1814391.6

–446.916

–1681140.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

° 93THDA±

° 73Bar±

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaHº†» Calcium Hydride ¼

¿

À Á

ÂÃÁ ÄÅ  Â Á - Æ

ÇÈ ÂÁ

Ç,È ÀÁ

ÇÈÉ Á

298.15 1053.0 1273.0

41.400

6770.0

–177000.0

–130.868

–137982.0

Ca » OH ¼Òº†» Calcium Hydroxide ¼

¿

ÀÁ

ÂÃÁ ÄÅ  Â Á - Æ

Ç È ÂÁ

Ç È ÀÁ

Ç ÈÉ Á

298.15 1023.00

83.400

14160.0

–985900.0

–294.015

–898239.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

275

ÇÊ1Ë1Ì ÂÁ

Ç,Ê.Ë0Ì ÀÁ

6700.0 22000.0

6.363 17.282

½ 94TCRAS¾ type

ÀÎÍÏÀ ÀÎÍÑÐ

½ 94TCRAS¾

Ç Ê.Ë0Ì ÂÁ

Ç Ê1Ë0Ì ÀÁ

29000.0

28.348

type

À€Í‚Ð

SGTE

276

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ca Ó OH ÔÒÕ×Ö g ØGÓ Calcium Hydroxide gas Ô

Û

Ü Ý

ÞßÝ àá  Þ Ý - â

ãä ÞÝ

ãä ÜÝ

ãäå Ý

298.15

292.040

16592.0

–598292.0

–85.375

–572837.0

Ca Ó NOæçÔÒÕéè 2HÕ O Ó Calcium Nitrate—Water (1/2) Ô

Û

Ü Ý

ãä Þ Ý

ãä Ü Ý

ã,äå Ý

298.15

269.399

–1540758.0

–1045.750

–1228970.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ù 94TCRASÚ

Ù 93THDAÚ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaHPOê6ë 2Hì O í Calcium Hydrogen Phosphate—Water (1/2) î

ñ

ò ó

ôõöó

ôõòó

ôõL÷,ó

298.15

189.535

–2421168.0

–835.278

–2172130.0

Ca í NOøçîÒìéë 3Hì O í Calcium Nitrate—Water (1/3) î

ñ

ò ó

ôõö ó

ôõò ó

ô,õ÷ ó

298.15

319.201

–1838001.9

–1229.200

–1471520.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

277

ï 93THDAð

ï 93THDAð

SGTE

278

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ca ù NOúçûÒüéý 4Hü O ù Calcium Nitrate—Water (1/4) û

298.15




 




  

375.301

–2132329.5

–1406.350

–1713030.0

CaI  g Gù Calcium Monoiodide gas û

298.15

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so




       -

 




 

261.300

10008.1

–5045.9

161.642

–53239.6

þ 93THDAÿ

þ 85JANAFÿ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaI Calcium Iodide 





 ! " #   - $

%&  

%& 

%&(' 

298.15 1056.3

145.300

17970.0

–536400.0

–12.427

–532695.0

CaI43 g 56 Calcium Iodide gas 





 ! " #   - $

%&  

%& 

%&(' 

298.15

327.562

16012.2

–258152.8

169.835

–308789.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

279

%)+*+,  

% )-*., 

41800.0

39.583

 94TCRAS type

0/21

 85JANAF

SGTE

280

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaO 7 MgO 8 Calcium Oxide—Magnesium Oxide (1/1) 9

<

=>

?@A >

?@ =>

?@B >

298.15

66.316

–1243066.4

–213.090

–1179530.0

Ca 8 NOCD9FE8 Calcium Nitrate 9

<

= >

?@A >

?@ = >

?@B >

298.15

193.217

–936797.6

–655.423

–741383.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

: 73Bar;

: 93THDA;

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaO G Calcium Oxide H

K

LM

N O M PQ N R M -

ST N M

S T LM

ST(U M

298.15 3172.0

38.100

6750.0

–634920.0

–106.061

–603298.0

CaO [ g \]G Calcium Oxide gas H

K

LM

N OM P Q N M - R

ST N M

ST LM

STU M

298.15

219.715

8953.0

38011.0

75.553

15484.7

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

281

SV+W+X N M

S V-W.X LM

80000.0

25.221

I 94TCRASJ type

L0Y2Z

I 94TCRASJ

SGTE

282

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaO^`_ Calcium Dioxide a

d

ef

ghi f

g h ef

gh(j f

298.15

83.680

–658980.0

–163.055

–610365.0

CaSOk_ Calcium Sulphite a

d

e f

ghi f

gh e f

ghj f

298.15

101.253

–1171520.0

–280.125

–1088000.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

b 73Barc

b 73Barc

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaO l TiOmon Calcium Oxide—Titanium Dioxide (1/1) p

s

tu

vwx u

vw tu

vwy u

298.15 1530.00

93.722

–1658537.6

–286.307

–1573180.0

CaO l ZrOmon Calcium Oxide—Zirconium Dioxide (1/1) p

s

tu

vwx u

vw tu

vwy u

298.15

93.722

–1765229.6

–294.768

–1677340.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

283

q 73Barr

vz+{+|x u

v z-{.|tu

type

1502.1

0.982

t~}t

q 93THDAr

SGTE

284

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaSO€‚ Calcium Sulphateƒ

†

‡ˆ

‰Š(‹ ˆ

‰Š ‡ˆ

‰ ŠŒ ˆ

298.15 1473.00 1733.00

106.692

–1437622.4

–377.260

–1325140.0

CaO ” UO•` Calcium Oxide—Uranium Trioxide (1/1) ƒ

†

‡ˆ

‰ Š‹ ˆ

‰ Š ‡ˆ

‰ Š Œ ˆ

298.15 1025.00

143.093

–1998278.4

–358.989

–1891250.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

„ 93THDA…

‰ -Ž.‹ ˆ

‰+Ž. ‡ˆ

type

5000.0 25400.0

3.394 14.657

‡‘2‡ ‡‘“’

„ 73Bar…

‰ -Ž. ‹ ˆ

‰ +Ž. ‡ˆ

type

920.5

0.898

‡‘2‡

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaO – WO—™˜ Calcium Oxide—Tungsten Trioxide (1/1) š



žŸ

 ¡¢ Ÿ

 ¡ žŸ

 ¡£ Ÿ

298.15

126.357

–1622973.6

–358.143

–1516190.0

CaO – V¤ O¥˜ Calcium Oxide—Divanadium Pentaoxide (1/1) š



ž Ÿ

 ¡¢ Ÿ

 ¡ ž Ÿ

 ¡£ Ÿ

298.15

179.075

–2335508.8

–539.734

–2174590.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

285

› 73Barœ

› 93THDAœ

SGTE

286

Thermodynamic Properties of Inorganic Materials: Pure Substances

CaS ¦ Calcium Sulphide §

ª

«¬

­ ®¬ ¯ ° ­ ¬ - ±

²³ ­ ¬

²³ «¬

²³(´ ¬

298.15 2800.00

56.500

9010.0

–475000.0

–17.158

–469884.0

CaS º g »6¦ Calcium Sulphide gas §

ª

«¬

­ ®¬ ¯ ° ­ ¬ - ±

²³ ­ ¬

² ³ «¬

²³´ ¬

298.15

232.613

9360.0

121486.0

158.955

74093.6

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

²µ+¶+· ­ ¬

² µ-¶.· «¬

70000.0

25.000

¨ 94TCRAS© type

«0¸2¹

¨ 94TCRAS©

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Fe¼ O½4¾ 2CaO ¿ Diiron Trioxide—Calcium Oxide (1/2) À

Ã

ÄÅ

ÆÇ(È Å

ÆÇ ÄÅ

Æ ÇÉ Å

298.15 1723.00

188.698

–2130074.5

–461.906

–1992360.0

ÄÅ

ÆÇÈ Å

ÆÇ ÄÅ

ÆÇÉ Å

298.15

120.499

–2315007.2

–391.781

–2198200.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Á 73BarÂ

Æ Ê-Ë.ÌÈ Å

ÆÊ+Ë.Ì ÄÅ

type

151042.4

87.662

đ͓Î

2CaO ¾ SiO¼™¿ Silicon Oxide—Calcium Oxide (1/2) ÏÑÐ ÒÓ ÔÕÓ ÖØ×ÙÀ

Ã

287

Á 73BarÂ

SGTE

288

Thermodynamic Properties of Inorganic Materials: Pure Substances

PÚ OÛ4Ü 2CaO Ý Phosphorus Oxide—Calcium Oxide (1/2) Þ

á

âã

äå(æ ã

äå âã

ä åç ã

298.15 1413.00 1626.00

189.242

–3336740.0

–694.134

–3129780.0

ä è-é.êæ ã

äè+é.ê âã

type

6694.4 100834.4

4.738 62.014

â‘ë2â â‘ë“ì

VÚ O ÛíÜ 2CaO Ý Divanadium Pentaoxide—Calcium Oxide (1/2) Þ

á

âã

ä å æ ã

ä å âã

ä å ç ã

298.15

220.497

–3088628.8

–642.474

–2897080.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ß 73Barà

ß 93THDAà

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MgO î 2SiOïíî 3CaO ð Magnesium Oxide—Silicon Oxide– –Calcium Oxide (1/1/3) óõô÷ö4øÑùûú üýúþFöÙÿ

298.15




 




 

253.132

–4564325.5

–762.511

–4336980.0

Ca Nïð Calcium Nitride ÿ

298.15




 




 

107.947

–439320.0

–208.428

–377177.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

289

ñ 93THDAò

ñ 73Barò

SGTE

290

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiO 3CaO  Silicon Oxide—Calcium Oxide (1/3) 





 

 

 

298.15

168.615

–2926708.0

–487.827

–2781260.0

WO 3CaO  Tungsten Trioxide—Calcium Oxide (1/3) 



 

 

  

  

298.15

194.974

–2930473.5

–577.849

–2758190.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 73Bar

 73Bar

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

291

2TiO ! 3CaO " Titanium Oxide—Calcium Oxide (2/3) #

&

'(

)*+ (

)* '(

)* ,(

298.15

234.722

–3999067.2

–669.497

–3799460.0

Ca-." PO/0#12" Tricalcium Bis(Phosphate)#

&

'(

)*3+4(

)* '(

)*,(

298.15 1373.00

235.978

–4117056.0

–791.568

–3881050.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

$ 73Bar%

$ 73Bar%

)57698+ (

)5:698 '(

type

15480.8

11.275

'<;='

SGTE

292

Thermodynamic Properties of Inorganic Materials: Pure Substances

V> O ?@ 3CaO A Divanadium Pentaoxide—Calcium Oxide (1/3) B

E

FG

HIJ G

HI FG

HI KG

298.15

274.889

–3782545.2

–732.243

–3564230.0

CaL P>2A Calcium Phosphide B

E

F G

HIJ G

HI F G

HI3K G

298.15

123.846

–506264.0

–83.096

–481489.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

C 93THDAD

C 73BarD

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

3TiO MN 4CaO O Titanium Oxide—Calcium Oxide (3/4) P

S

TU

VWX U

VW TU

VW YU

298.15

328.444

–5664717.5

–955.803

–5379740.0

5CaO N 6SiOM0N 3HM O O Calcium Oxide—Silicon Oxide—Water (5/6/3) P

S

T U

VWX U

VW T U

VWY U

298.15

513.168

–9935745.0

–2251.140

–9264570.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

293

Q 73BarR

Q 93THDAR

SGTE

294

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdCl Z g []\ Cadmium Monochloride gas ^

a

bc

d4egc f h d c - i

jk d c

jk bc

jkl c

298.15

252.232

9707.0

27339.0

88.893

835.7

CdClm2\ Cadmium Chloride ^

a

bc

jk d c

jk bc

jkl c

298.15 841.00

115.478

–391622.4

–159.401

–344097.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

_ 94TCRAS`

_ 94SGTE`

jn:o9p d c

jn:o9p bc

type

30124.8

35.820

b
Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdCltu g vxw Cadmium Chloride gas y

|

}~

4€g~  ‚  ~ - ƒ

„…  ~

„… }~

„…† ~

298.15

286.087

14426.0

–194434.0

11.208

–197776.0

CdF u g v]w Cadmium Monofluoride gas y

|

} ~

 €g~  ‚  ƒ ~ -

„…  ~

„… } ~

„… † ~

298.15

240.576

9219.0

–62316.0

87.382

–88368.8

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

295

z 94TCRAS{

z 94TCRAS{

SGTE

296

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdF‡2ˆ Cadmium Fluoride ‰

Œ

Ž

‘ Ž

 Ž

’Ž

298.15 1333.00

83.262

–700401.6

–171.327

–649320.0

CdF‡˜ g ™šˆ Cadmium Fluoride gas ‰

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

“:”9• ‘ Ž

“:”9• Ž

type

51881.6

38.921

<–s—

Œ

Ž

‘4›gŽ œ  ‘ Ž - ž

 ‘ Ž

 Ž

’Ž

298.15

264.944

13155.0

–393245.0

10.355

–396332.0

SGTE

Š 94SGTE‹

Š 94TCRAS‹

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdH Ÿ g  ]¡ Cadmium Monohydride gas ¢

¥

¦§

¨4©g§ ª « ¨ § - ¬

­® ¨ §

­® ¦§

­®¯ §

298.15

218.309

8834.0

260837.0

101.169

230673.0

Cd(OH) Ÿ g  ]¡ Cadmium Monohydroxide gas ¢

¥

¦ §

¨ ©g§ ª « ¨ ¬ § -

­® ¨ §

­® ¦ §

­® ¯ §

298.15

250.038

11055.0

–78767.0

30.324

–87808.2

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

297

£ 94TCRAS¤

£ 94TCRAS¤

SGTE

298

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cd ° OH ±1²³° Cadmium Hydroxide ±

¶

·¸

¹ º ¸ »g¼ 4 ¹ ¸ - ½

¾¿ ¹ ¸

¾¿ ·¸

¾¿3À ¸

298.15

92.000

13800.0

–561500.0

–295.627

–473359.0

Cd ° OH ±1²ÂÁ g Ú° Cadmium Hydroxide gas ±

¶

· ¸

¹ ºg¸ » ¼ ¹ ½ ¸ -

¾¿ ¹ ¸

¾¿ · ¸

¾¿À ¸

298.15

283.920

16971.0

–406426.0

–103.707

–375506.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

´ 94TCRASµ

´ 94TCRASµ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdI Ä g Å]Æ Cadmium Monoiodide gas Ç

ËÌ

Í4ÎgÌ Ï Ð Í Ì - Ñ

ÒÓ Í Ì

ÒÓ ËÌ

ÒÓ Ô Ì

298.15

271.708

10272.0

82440.0

161.838

34187.9

Ê

ËÌ

ÒÓ Í Ì

ÒÓ ËÌ

ÒÓÔ Ì

298.15 663.00

161.084

–203342.4

–6.855

–201299.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

È 94TCRASÉ

Ê

CdIÕ2Æ Cadmium Iodide Ç

299

È 94SGTEÉ

ÒÖ:×9Ø Í4Ì

ÒÖ:×9Ø ËÌ

type

20710.8

31.238

Ë<ÙsÚ

SGTE

300

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdIÛÜ g ÝxÞ Cadmium Iodide gas ß

â

ãä

å4ægä ç è å ä - é

êë å ä

êë ãä

êëì ä

298.15

324.774

15913.0

–60167.0

156.835

–106927.0

Cd Þ NOíîßïÛ2Þ Cadmium Nitrate ß

â

ãä

êë å ä

êë ãä

êëì ä

298.15 431.00

207.945

–456955.0

–650.907

–262887.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

à 94TCRASá

à 91Knaá

êð:ñ9ò å ä

êð:ñ9ò ãä

type

2928.8

6.795

ã<ó=ã

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdO ô Cadmium Oxide õ

ùú

ûüý ú

ûü ùú

ûüþú

298.15

54.810

–259408.0

–99.563

–229723.0

ø

ù ú

ý
ú  ý  ú

ûü ý ú

ûüù ú

ûü þ ú

298.15

231.564

8955.0

127000.0

77.190

103986.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

ö 73Bar÷

ø

CdO ÿ g ]ô Cadmium Oxide gas õ -

301

ö 94TCRAS÷

SGTE

302

Thermodynamic Properties of Inorganic Materials: Pure Substances 

CdSeO Cadmium Selenite





 



298.15 953.00

120.081

–581994.4

–281.405

–498093.0

CdSO#

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so



Cadmium Sulphate



 

58576.0

61.465

type

"!

93THDA







 



298.15

123.010

–933450.4

–371.154

–822791.0

SGTE

sp art

73Bar

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

303

CdO $ WO%'& Cadmium Oxide—Tungsten Trioxide (1/1) ( +

,-

./0-

./,-

./1-

298.15

154.808

–1181394.2

–339.904

–1080050.0

) 73Bar*

CdS & Cadmium Sulphide ( +

,-

02345

298.15 1748.00

72.180

9802.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

06

) 94TCRAS* ./0-

./,-

./71-

–149400.0

–11.690

–145915.0

.89:0-

.8;9:,-

34000.0

19.451

type ,=

SGTE

304

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdS @ g ACB Cadmium Sulphide gas D G

HI

J2I KLM

298.15

244.981

9561.0

-

JI N

OP

JI

175658.0

E 94TCRASF OP

HI

161.111

OPQ

I

127623.0

CdSb B Cadmium Antimonide D G

HI

298.15 729.00

95.604

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

OP

JI

–13347.0

E 73BarF OP

HI

–1.718

OPQ

I

ORST

JI

ORST

HI

–12834.8 35564.0

48.785

type H=UWV

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

305

CdSe X Cadmium SelenideY \

]^

_2^ `ab

298.15 1509.00

86.680

11160.0

-

_^ c

Z 94TCRAS[ de

_^

–144800.0

de

]^

–7.086

^

def

dghi

_2^

dghi

]^

–142687.0 30000.0

]^

_2^ `ab

298.15 1365.00

95.000

11770.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

_^ c

]

19.881

CdTe X Cadmium Telluride Y \

type j"k

Z 94TCRAS[ de

_^

–100800.0

de

]^

–6.021

def

^

dghi

_^

dghi

]^

–99004.8 45000.0

32.967

type ]

j"k

SGTE

306

Thermodynamic Properties of Inorganic Materials: Pure Substances

CdTe l g mon Cadmium Telluride gas p s

tu

v2u wxy

vu z

298.15

266.296

10171.3

-

vu

{|

q 93THDAr {|

242672.0

tu

165.275

{|}

u

193395.0

Cd~ Cl€l g mon Cadmiun Tetrachloride gas p s

t u v

298.15

439.553

28967.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

u wxy

-

v z

u

{|

v

u

–400000.0

q 94TCRASr {|

t u

–110.205

{|}

u

–367142.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cd F‚„ƒ g …‡† Cadmiun Tetrafluoride gas ˆ ‹

Œ

Ž2 ‘

Ž ’

298.15

387.266

24481.0

-

Ž

“”

‰ 94TCRASŠ “”

–798000.0

Œ

–121.912

“”•



–761652.0

Cd I‚„ƒ g …‡† Cadmiun Tetraiodide gas ˆ ‹

Œ  Ž

298.15

517.001

33100.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 ‘

-

Ž ’



“”

Ž



–95000.0

307

‰ 94TCRASŠ “”

Œ 

181.123

“”•



–149002.0

SGTE

308

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeCl–˜— Cerium Chloride ™

š 93THDA›

œ

ž

Ÿ 7¡2ž

Ÿ ž

Ÿ ¢ž

298.15 1080.00

150.959

–1053531.0

–253.113

–978065.0

CeCl–ª© g «‡— Cerium Chloride gas ™

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ÿ£;¤¥ž

53137.0

49.201

type §¦?¨

š 93THDA›

œ

ž

Ÿ ¡ž

Ÿ ž

Ÿ 7¢ž

298.15

370.711

–722995.0

–33.361

–713048.0

SGTE

Ÿ£¤¥¡ž

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

309

CrCeO¬˜­ Chromium Cerium Trioxide ®

¯ 93THDA°

±

²³

´µ¶³

´µ²³

´µ·³

298.15

105.018

–1540130.0

–295.700

–1451970.0

CeF¬˜­ Cerium Fluoride ® ±

²³

´µ7¶2³

´µ²³

´µ·³

298.15 1710.00

115.269

–1688913.0

–258.368

–1611880.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¯ 93THDA° ´¸;¹º¶³

´¸¹º²³

55647.0

32.542

type ²

»"¼

SGTE

310

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeF½ª¾ g ¿oÀ Cerium Fluoride gas Á

 93THDAÃ

Ä

ÅÆ

ÇÈÉÆ

ÇÈÅÆ

ÇÈÊÆ

298.15

337.101

–1248506.0

–36.536

–1237610.0

CeHËÌÀ Cerium Dihydride Á Ä

Å Æ

ÇÈÉ

298.15

55.773

–193300.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Æ

 94SGTEà ÇÈÅ Æ

ÇÈ7Ê Æ

–144.361

–150260.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

311

CeI͘ΠCerium Iodide Ï

Ð 93THDAÑ

Ò

ÓÔ

ÕÖ7×2Ô

ÕÖÓÔ

ÕÖØÔ

298.15 1033.00

214.639

–649774.9

–29.024

–641122.0

CeIÍªÞ g ߇ΠCerium Iodide gas Ï

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ÕÙÚÛÓÔ

51044.8

49.414

type Ó

Ü"Ý

Ð 93THDAÑ

Ò

ÓÔ

ÕÖ×Ô

ÕÖÓÔ

ÕÖ7ØÔ

298.15

427.342

–371957.6

183.679

–426722.0

Landolt-B¨ornstein New Series IV/19A

ÕÙÚÛ×Ô

SGTE

312

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeN à Cerium Nitride á

â 73Barã

ä

åæ

çèéæ

çèåæ

çè7êæ

298.15

44.350

–326352.0

–120.909

–290303.0

CeO ë g ì‡à Cerium Monoxide gas á ä

å æ é

298.15

246.104

9444.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

æ íîï

-

é ð

æ

çèé

â 94TCRASã æ

–130701.0

çèå æ

çèê æ

74.076

–152787.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeO ñóò ôöõÌ÷ Cerium Dioxide (Oxygen deficient)ø û

üý

þÿ
ý

þÿüý

þÿý

298.15

69.036

–995792.0

–176.844

–943066.0

CeO ñóò Ì÷ Cerium Dioxide (Oxygen deficient)ø û

ü ý

þÿ


298.15

67.781

–1033448.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ý

þÿü ý

þÿ
 ý

–189.383

–976984.0

313

ù 73Barú

ù 73Barú

SGTE

314

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeO  Cerium Dioxide

 94TCRAS



 

298.15 2753.0

62.30

10370.0

-

 







–1090400.0





–212.301

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

"!$#





298.15

78.241





–456474.4

%!$#



–1027100.0 80000.0

CeS  Cerium Monosulphide

SGTE



29.059

type &('

 73Bar 



–23.283






–449533.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CeS ) g *,+ Cerium Monosulphide gas 0

12

32 456

32 7

298.15

253.158

9510.2

-

89

32

. 93THDA/ 89

120039.0

12

89
:

151.634

2

74829.3

Ce; O; S + Dicerium Dioxide Monosulphide 0

1 2

298.15

130.541

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

89

3

2

–1696612.0

89

315

1 2

–245.584

. 91Kna/ 89<:

2

–1623390.0

SGTE

316

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ce= O>@? Cerium Oxide A

B 94TCRASC

D

EF

GF HIJ

298.15 2523.0

144.40

21170.0

-

GF K

LM

GF

LM

–1799700.0

EF

LM
N

–302.229

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

LO%P$Q

GF

120000.0

D

EF

298.15

287.441

LM

GF

–3951788.0

LO%P$Q

EF

–1709590.0

Ce=U? SOVWAT> ? Cerium Sulphate A

SGTE

F

47.562

type ERTS

B 73BarC LM

EF

–1178.560

LM
N

F

–3600400.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ce S




Cerium Sulphide 



298.15

Ce
S





298.15

 

 





180.330

–1188256.0

–54.788

–1171920.0

Tricerium Tetrasulphide 

 

 

 

 

255.224

–1652680.0

–81.418

–1628410.0

Landolt-B¨ornstein New Series IV/19A co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

317

 73Bar

 73Bar

SGTE

318

Thermodynamic Properties of Inorganic Materials: Pure Substances

CoCl  g  Cobalt Monochloride gas 



 

 !# " $    - %

& ' 

&' 

& '( 

298.15

243.863

9707.0

192378.0

102.283

161882.0

CrCl  g ) Chromium Monochloride gas 



 

 !# " $  %  -

& '  

&'  

& '( 

298.15

258.166

9563.0

155543.0

123.083

118846.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 96TCRAS

 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CrOCl * g +, Cromium Chloride Oxide gas -

0

1 2

3 4#2 5 6  3 2 - 7

8 9 32

8 9 12

8 9: 2

298.15

288.713

11922.0

–101059.0

51.057

–116282.0

CrO; Cl * g +), Cromium Chloride Dioxide gas -

0

1 2

3 4#2 5 6 3 7 2 -

8 9 3 2

8 9 1 2

8 9<: 2

298.15

311.144

14639.0

–342683.0

–29.086

–334011.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

319

. 94TCRAS/

. 94TCRAS/

SGTE

320

Thermodynamic Properties of Inorganic Materials: Pure Substances

CsCl = Cesium Chloride >

A

B C

D E#C F G  D C - H

I J DC

I J BC

I J
298.15 743.00 919.00

101.170

12450.0

–442310.0

–95.600

–413807.0

CsCl W g X= Cesium Chloride gas >

A

B C

D E#C F G D H C -

I JD C

I JB C

I JK C

298.15

256.078

10131.0

–242229.0

59.308

–259912.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

I LNMNO DC

ILPMQO BC

2930.0 20380.0

3.943 22.176

? 94TCRAS@ type

BSRTB BSRVU

? 94TCRAS@

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CuCl Y Copper Monochloride Z

]

^ _

`a_ b#c ` d _ -

e f `_

ef ^_

e fg _

298.15 685.00 696.00

87.740

11400.0

–137000.0

–56.950

–120021.0

CuCl o g p)Y Copper Monochloride gas Z

]

^ _

` a#_ b c ` d _ -

e f` _

e f^ _

e fg _

298.15

237.099

9471.0

76304.0

92.410

48752.1

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

e hNiQj ` _

e hNiQj ^_

6500.0 7080.0

9.489 10.172

321

[ 96TCRAS\ type

^lkV^ ^lknm

[ 96TCRAS\

SGTE

322

Thermodynamic Properties of Inorganic Materials: Pure Substances

ClF q g r)s Chlorine Fluoride gas t

w

x y

z {#y | }  z y - ~

 € zy

€ xy

 €‚ y

298.15

217.940

8908.0

–55700.0

5.006

–57192.5

Liƒ ClF q g r)s Dilithium Chloride Fluoride gas t

w

x y

z {#y | } z ~ y -

 € z y

 € x y

 € y

298.15

268.040

13422.0

–753957.0

–3.134

–753023.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

u 94TCRASv

u 85JANAFv

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MgClF „ g …† Magnesium Chloride Fluoride gas ‡

Š

‹ Œ

 Ž#Œ     Œ - ‘

’ “ Œ

’ “ ‹Œ

’ “” Œ

298.15

262.681

12330.2

–569024.0

17.076

–574115.0

SO• ClF „ g …)† Sulphur Chloride Fluoride Dioxide gas ‡

Š

‹ Œ

 Ž#Œ    ‘ Œ -

’ “  Œ

’ “ ‹ Œ

’ “” Œ

298.15

302.847

14702.6

–556472.0

–147.304

–512553.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

323

ˆ 85JANAF‰

ˆ 85JANAF‰

SGTE

324

Thermodynamic Properties of Inorganic Materials: Pure Substances

ClO– F — g ˜š™ Chlorine Fluoride Trioxide gas ›

ž

Ÿ  

¡ ¢#  £ ¤  ¡   - ¥

¦ § ¡ 

¦§ Ÿ 

¦ §<¨  

298.15

278.986

13296.8

–21422.1

–241.669

50631.4

PClF — g ˜™ Phosphorus Monochloride Monofluoride gas ›

ž

Ÿ  

¡ ¢#  £ ¤ ¡ ¥   -

¦ § ¡  

¦ § Ÿ  

¦ §¨  

298.15

279.489

11630.0

–283175.0

25.467

–290768.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

œ 85JANAF

œ 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiClF © g ª)« Silicon Monochloride Monofluoride gas ¬

¯

° ±

² ³#± ´ µ  ² ± - ¶

· ¸ ²±

· ¸ °±

· ¸¹ ±

298.15

275.142

11833.0

–377825.0

43.398

–390764.0

POClFº»© g ª)« Phosphorus Chloride Difluoride Oxide gas ¬

¯

° ±

² ³#± ´ µ ² ¶ ± -

· ¸ ² ±

· ¸ ° ±

· ¸¹ ±

298.15

301.696

14196.3

–971399.3

–156.294

–924800.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

325

­ 94TCRAS®

­ 85JANAF®

SGTE

326

Thermodynamic Properties of Inorganic Materials: Pure Substances

PClF¼¾½ g ¿ÁÀ Phosphorus Monochloride Difluoride gas Â

Å

Æ Ç

È É#Ç Ê Ë  È Ç - Ì

Í Î ÈÇ

Í Î ÆÇ

Í Î<Ï Ç

298.15

295.062

13876.0

–735066.0

–60.355

–717071.0

ClFÐѽ g ¿)À Chlorine Trifluoride gas Â

Å

Æ Ç

È É#Ç Ê Ë È Ì Ç -

Í Î È Ç

Í Î Æ Ç

Í ÎÏ Ç

298.15

281.605

13648.2

–158866.5

–134.118

–118879.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

à 94TCRASÄ

à 85JANAFÄ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

PClFÒÑÓ g ÔÁÕ Phosphorus Monochloride Tetrafluoride gas Ö

Ù

Ú Û

Ü Ý#Û Þ ß  Ü Û - à

á â ÜÛ

á â ÚÛ

á â‚ã Û

298.15

326.828

18320.0

–1364898.0

–231.387

–1295910.0

ClFäÑÓ g Ô)Õ Chlorine Pentafluoride gas Ö

Ù

Ú Û

Ü Ý#Û Þ ß Ü à Û -

á â Ü Û

á â Ú Û

á âã Û

298.15

310.734

17928.4

–238488.0

–307.778

–146724.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

327

× 94TCRASØ

× 85JANAFØ

SGTE

328

Thermodynamic Properties of Inorganic Materials: Pure Substances

SClFåÑæ g ç)è Sulphur Monochloride Pentafluoride gas é

ì

í î

ï ð#î ñ ò  ï î - ó

ô õ ïî

ô õ íî

ô õ‚ö î

298.15

318.937

18329.0

–1047000.0

–331.645

–948120.0

FeCl æ g ç÷è Iron Monochloride gas é

ì

í î

ï ð#î ñ ò ï ó î -

ô õ ï î

ôõ í î

ô õö î

298.15

253.178

11029.0

191933.0

114.359

157837.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ê 94TCRASë

ê 96TCRASë

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

FeClO ø Iron Chloride Oxide ù

ü

ý þ

ÿ
þ  ÿ  þ



298.15

82.550

12940.0

–407600.0

-

ÿþ

 

ý þ

ÿ 
þ  ÿ  þ



298.15

276.209

12455.0

–981.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

ÿ þ



–158.843

FeClO g ø Iron Chloride Oxide gas ù

ü

ýþ



ý þ

34.816

 

þ

329

ú 96TCRASû

–360241.0

þ

ú 96TCRASû

–11361.4

SGTE

330

Thermodynamic Properties of Inorganic Materials: Pure Substances

GaCl  g  Gallium Monochloride gas  



 

298.15

240.251

9609.0

-



!"



 94TCRAS ! "

–69622.0

#

87.984

!"$

–95854.6

GdOCl  Gadolinium Chloride Oxide  

 

298.15

95.395

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

!"





–983658.4

! "

 

–186.807



 94TCRAS !"$



–927962.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

GeCl % g &(' Germanium Monochloride gas ) ,

-.

/. 012

298.15

245.901

9599.0

/. 3

-

/.

45

45

69031.0

* 94TCRAS+

-#.

103.271

.

456

38240.6

HCl % g &' Hydrogen Chloride gas ) ,

- . /

298.15

186.901

8640.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

. 012

-

/ 3

.

45

/

331

* 94TCRAS+ .

–92310.0

4 5

- .

10.021

456

.

–95297.9

SGTE

332

Thermodynamic Properties of Inorganic Materials: Pure Substances

HClO 7 g 8(9 Hydrogen Monoxochlorate gas : =

>?

@? ABC

@? D

298.15

236.583

10224.0

-

@?

EF

E F

–75741.0

; 94TCRAS<

>#?

–42.870

EFHG

?

–62959.3

Sr(OH)Cl 7 g 8I9 Strontium Chloride Hydroxide gas : =

> ? @

298.15

319.841

16036.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

? ABC

-

@ D

?

EF

@

?

–533698.0

EF

> ?

–15.306

EFG

; 94TCRAS< ?

–529135.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

HSOJ Cl K g LIM Hydrogen Chlorotrioxosulphate gas N Q

RS

TS UVW

TS X

298.15

310.001

16035.0

-

TS

YZ

YZ

–550000.0

O 94TCRASP

R#S

YZH[

–206.669

R S T

298.15

251.329

10665.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

S UVW

-

T X

S

YZ

T

S

54945.0

YZ

S

–488382.0

SiHCl K g L(M Silicon Chloride Hydride gas N Q

333

O 94TCRASP R S

55.639

YZH[

S

38356.1

SGTE

334

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiH\ Cl ] g ^I_ Monochlorosilane gas `

a 94SGTEb

c

de

fgHhe

fgd#e

fgi e

298.15

250.731

–200832.0

–75.638

–178280.0

NHj Cl _ Ammonium Chloride ` c

de

he klm

298.15 457.70 793.20

94.860

22698.2

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

he n

a 85JANAFb

fgHhe

f gHd#e

fgi e

–314553.1

–373.845

–203091.0

foqpqrhe

f osptrHd#e

3949.7 10585.5

8.629 13.345

type dvuwd dvuyx

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

335

NHz ClOz|{ Ammonium Perchlorate} €

‚

ƒ‚ „…†

298.15 513.15

184.180

25237.9

-

ƒ‚ ‡

ˆ‰

ƒ‚

–295767.0

~ 85JANAF ˆ‰

#‚

–694.819

ˆ‰HŠ

‚

9623.2

€

‚

ƒ‚ „…†

298.15

257.174

9556.3

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ƒ‚

-

ƒ‚ ‡

ˆ‰

ƒ‚

217568.0

ˆ ‹sŒt

#‚

–88606.7

HfCl  g ({ Hafnium Monochloride gas }

sp art

ˆ‹qŒq

18.753

type vŽw

~ 93THDA ˆ ‰

#‚

102.074

ˆ‰HŠ

‚

187134.0

SGTE

336

Thermodynamic Properties of Inorganic Materials: Pure Substances

HgCl ‘ Mercury Monochloride gas ’ •

–—

˜— ™š›

298.15

96.265

11738.2

-

˜— œ

ž

“ 85JANAF”

˜—

 ž

–132463.3

–#—

–100.581

—

žŸ

–104663.0

HgCl   g ¡‘ Mercury Monochloride gas ’ •

– — ˜

298.15

259.957

9845.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

— ™š›

-

˜ œ

—

ž

˜

—

78450.0

“ 85JANAF” ž

– —

–100.581

žHŸ

—

–104663.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

337

ClI ¢ Chlorine Iodide £

¤ 85JANAF¥

¦

§¨

©¨ ª«¬

298.15 300.53

97.927

12163.0

-

©¨ ­

®¯

©¨

–35422.0

®¯

§#¨

–71.682

¨

®¯°

11602.0

¦

§¨

©¨ ª«¬

298.15

247.571

9555.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

©¨

-

©¨ ­

® ±s²t³

§#¨

–14050.0

ClI ¸ g ¹I¢ Chlorine Iodide gas £

sp art

®±q²q³

38.605

type §µ´·¶

¤ 94TCRAS¥ ®¯

©¨

17393.0

®¯

§#¨

77.962

®¯H°

¨

–5851.4

SGTE

338

Thermodynamic Properties of Inorganic Materials: Pure Substances

InCl º Indium Monochloride »

¼ 73Bar½

¾

¿À

ÁÂHÃÀ

Á ¿À

ÁÂHÄ À

298.15 393.00 498.00

94.977

–186188.0

–74.213

–164062.0

ÁÅqÆtÇÃÀ

ÁÅqÆtÇ¿#À

6903.6 9204.8

17.566 18.484

InCl Ê g ËIº Indium Monochloride gas » ¾

¿ À Ã

298.15

248.271

9752.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

À ÌÍÎ

-

à Ï

À Á

 Ã

À

–72148.0

type ¿µÈy¿ ¿µÈ·É

¼ 94TCRAS½ Á

 ¿ À

79.081

Á

 Ä

À

–95726.1

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

339

KCl Ð Potassium ChlorideÑ Ô

Õ#Ö

×Ö ØÙÚ

298.15 1044.00

82.555

11367.9

-

×Ö Û

Ò 85JANAFÓ ÜÝ

×Ö

–436684.1

ÜÝ

Õ#Ö

–93.664

Ö

ÜÝÞ

26283.9

Ô

ÕÖ

×Ö ØÙÚ

298.15

239.091

9885.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

×Ö

-

×Ö Û

ÜÝ

×Ö

–214575.0

Ü ßsàtá

Õ#Ö

–408758.0

KCl ä g åÐ Potassium Chloride gas Ñ

sp art

Üßqàqá

25.176

type Õvâyã

Ò 94TCRASÓ ÜÝ

Õ#Ö

62.871

ÜÝHÞ

Ö

–233320.0

SGTE

340

Thermodynamic Properties of Inorganic Materials: Pure Substances

KClOæ|ç Potassium Perchlorateè ë

ìí

îí ïðñ

298.15 572.70

151.042

21070.6

-

îí ò

óô

é 85JANAFê îí

óô

–430115.2

ì#í

óôHõ

–435.471

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ó ös÷tø

îí

13765.4

ë

ìí

298.15

82.843

óô

îí

–1020477.6

óô

ì#í

–188.172

óöq÷tø

ì#í

–300279.0

LaClO ç Lanthanum Monooxochlorate è

SGTE

í

24.036

type ìµùyì

é 73Barê óôHõ

í

–964374.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

LiCl ú Lithium Chloride û

ü 85JANAFý

þ

ÿ




  -

 

 ÿ

 

298.15 883.00

59.300

9305.2

–408266.4

–81.359

–384009.0

LiCl  g Iú Lithium Chloride gas û

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

  

  ÿ

19832.2

22.460

type

 ÿ

ü 94TCRASý

þ

ÿ




    -

 

 ÿ

 

298.15

212.857

9060.0

–193780.0

72.198

–215306.0

Landolt-B¨ornstein New Series IV/19A

341

SGTE

342

Thermodynamic Properties of Inorganic Materials: Pure Substances

LiClO  g 

$

 Lithium Monooxochlorate gas ! %
& ' ()& '(%
& ' (+*&

298.15

256.421

–14225.6

LiClO,- Lithium Perchlorate!

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–18157.6

$

%
&

' ()&

' (%&

' (*&

298.15 509.00

125.520

–380744.0

–425.433

–253901.0

SGTE

sp art

13.188

" 93THDA#

" 85JANAF#

' ./0+)&

' ./0%&

type

29288.0

57.540

%12

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MgCl 3 g 465 Magnesium Monochloride gas 7

:

;
<

= >< ?@  = < - A

B C =<

BC ;<

B C+D <

298.15

233.420

9363.0

–54705.0

89.210

–81302.8

MnCl 3 g 465 Manganese Monochloride gas 7

:

; <

= >< ? @ = A < -

B C = <

B C ; <

B C+D <

298.15

253.804

9550.0

11983.0

110.044

–20826.8

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

343

8 94TCRAS9

8 94TCRAS9

SGTE

344

Thermodynamic Properties of Inorganic Materials: Pure Substances

MnClOEGF g H6I Manganese Chloride Trioxide gas J

M

N
O

P QO RS  P O - T

U V PO

UV NO

U VXW O

298.15

311.115

16806.0

436565.0

–140.365

478415.0

MoCl F g H6I Molybdenum Monochloride gas J

M

N O

P QO R S P T O -

U V P O

UV N O

U VW O

298.15

258.600

9507.0

420000.0

118.501

384669.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

K 94TCRASL

K 94TCRASL

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoClO Y g Z

_

[ Molybdenum Chloride Oxide gas \ `
a b ca de bf a g h ba gh `a g h+i a

-

298.15

296.270

12011.0

–40000.0

53.597

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

] 94TCRAS^

–55979.9

MoClOjkY g Zl[ Molybdenum Chloride Dioxide gas \

_

` a

b ca d e b f a -

g h b a

g h ` a

g hXi a

298.15

317.441

14661.0

–370000.0

–27.806

–361710.0

Landolt-B¨ornstein New Series IV/19A

345

] 94TCRAS^

SGTE

346

NOCl m g n

Thermodynamic Properties of Inorganic Materials: Pure Substances

s

o Nitrosyl Chloride gas p t
u v wu xy vz u { | vu

{ | tu

{ |+} u

298.15

261.583

–48.335

67109.2

-

11364.0

52698.0

NO~ Cl m g n6o Nitryl Chloride gas p

s

t u

v wu x y v z u -

{ | v u

{ | t u

{ |} u

298.15

272.234

12221.0

12500.0

–140.258

54317.9

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

q 94TCRASr

q 94TCRASr

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

NaCl  Sodium Chloride€

ƒ

„…

† ‡… ˆ‰  † … - Š

‹ Œ †…

‹ Œ „…

‹ ŒX …

298.15 1073.80

72.115

10611.0

–411120.0

–90.725

–384070.0

NaCl – g —

ƒ

 Sodium Chloride gas € „
… † ‡… ˆ‰ †Š … ‹ Œ †…

‹ Œ „…

‹ Œ …

298.15

229.794

66.954

–201507.0

-

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

9615.0

–181545.0

347

‹ Ž †…

‹Ž‘ „…

28158.0

26.223

 85JANAF‚ type

„“’•”

 94TCRAS‚

SGTE

348

Thermodynamic Properties of Inorganic Materials: Pure Substances

NaClO˜š™ Sodium Perchlorate›

ž

Ÿ
 

¡ ¢£ 

¡ ¢Ÿ 

¡ ¢¤ 

298.15 581.00

142.256

–382752.3

–430.878

–254286.0

NbClO©ª™ Niobium Chloride Dioxide ›

ž

Ÿ
 

¡ ¢£ 

¡¢Ÿ
 

¡ ¢X¤ 

298.15

89.956

–983240.0

–263.001

–904826.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

œ 93THDA

¡ ¥¦§+£ 

¡ ¥¦§Ÿ 

type

13974.6

24.053

Ÿ¨•Ÿ

œ 93THDA

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

NdClO « Neodymium Chloride Oxide ¬

°
±

² ³´±

² ³°±

² ³µ±

298.15

94.558

–1011272.8

–190.641

–954433.0

¯

« Nickel Monochloride gas ¬ ° ± ´ ¸± ¹º ´ » ± ² ³+´ ±

²³° ±

² ³µ ±

298.15

245.453

104.118

139190.0

-

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

­ 73Bar®

¯

NiCl ¶ g ·

10028.0

170233.0

349

­ 96TCRAS®

SGTE

350

Thermodynamic Properties of Inorganic Materials: Pure Substances

ClO ¼ g ½¿¾ Chlorine Monoxide gas À

Ã

Ä
Å

Æ ÇÅ ÈÉ  Æ Å - Ê

Ë Ì ÆÅ

ËÌ ÄÅ

Ë Ì+Í Å

298.15

225.101

9522.0

101627.0

10.988

98350.9

PuClO ¾ Plutonium Chloride Oxide À

Ã

Ä Å

Ë Ì Æ Å

Ë Ì Ä Å

Ë ÌÍ Å

298.15

108.784

–931776.8

–159.790

–884135.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Á 94TCRASÂ

Á 73BarÂ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SbClO Î Antimony Chloride Oxide Ï

Ò

Ó
Ô

Õ Ö×Ô

Õ ÖÓÔ

Õ ÖØÔ

298.15

107.529

–380744.0

–152.106

–335394.0

SmClO Î Samarium Chloride Oxide Ï

Ò

Ó Ô

Õ Ö× Ô

Õ ÖÓ Ô

Õ Ö+Ø Ô

298.15

100.416

–1000394.0

–183.193

–945775.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

351

Ð 73BarÑ

Ð 91KnaÑ

SGTE

352

Thermodynamic Properties of Inorganic Materials: Pure Substances

TiClO Ù Titanium Chloride Oxide Ú

Ý

Þ
ß

à áâß

àáÞ
ß

à áXãß

298.15

73.220

–765672.0

–171.613

–714506.0

TiClO ä g å6Ù Titanium Chloride Oxide gas Ú

Ý

Þ ß

â æß ç è â é ß -

à á+â ß

à áÞ ß

à áã ß

298.15

263.668

12142.0

–244261.9

18.835

–249878.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Û 94SGTEÜ

Û 85JANAFÜ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

UClO ê Uranium Chloride Oxide ë

ï
ð

ñ òóð

ñ òïð

ñ òôð

298.15

102.508

–833871.2

–161.805

–785629.0

î

ï ð

ó ÷ð ø ù ó ú ð -

ñ ò+ó ð

ñòï ð

ñ ò+ô ð

298.15

303.325

12041.0

105000.0

56.594

88126.5

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ì 91Knaí

î

WClO õ g ö¿ê Tungsten Chloride Oxide gas ë

353

ì 94TCRASí

SGTE

354

Thermodynamic Properties of Inorganic Materials: Pure Substances

ClOûkü g ýlþ Chlorine Dioxide gas ÿ





     - 

  

 

 

298.15

256.878

10800.0

105000.0

–59.808

122832.0

TaClOûªþ Tantalum Chloride Dioxide ÿ



 

  

  

 

298.15

97.906

–1046000.0

–260.253

–968406.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

94TCRAS


93THDA


Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

UClO Uranium Chloride Dioxide 



! 

 

#"

298.15

112.550

–1169428.0

–254.337

–1093600.0



 

! (  ) * ! +  -

#! 

  

," 

298.15

322.790

14625.0

–265000.0

–26.514

–257095.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 91Kna



WClO%$ g &' Tungsten Chloride Dioxide gas 

355

 94TCRAS

SGTE

356

Thermodynamic Properties of Inorganic Materials: Pure Substances

PCl - g .'/ Phosphorus Monochloride gas 0

3

45

67 5 8 9 6 5 - :

;< 6 5

;< 45

;<= 5

298.15

236.880

9291.0

134624.0

102.491

121526.0

PbCl - g .'/ Lead Monochloride gas 0

3

4 5

6 7 5 8 9 6 : 5 -

;< 6 5

;< 4 5

;<#= 5

298.15

261.302

9787.0

8820.0

84.963

–16511.6

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

1 94TCRAS2

1 94TCRAS2

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

RbCl > Rubidium Chloride ?

B

CD

E F D G H  E D - I

JK E D

JK CD

JKL D

298.15 997.00

95.230

12160.0

–435220.0

–93.086

–407467.0

RbCl V g W'> Rubidium Chloride gas ?

B

CD

EF D G H E D - I

JK E D

JK CD

JKL D

298.15

249.689

10057.0

–223323.0

61.374

–241622.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

JMONQP ED

JMONQP CD

24400.0

24.473

357

@ 94TCRASA type

CSRUT

@ 94TCRASA

SGTE

358

Thermodynamic Properties of Inorganic Materials: Pure Substances

SCl X g Y'Z Sulphur Monochloride gas [

^

_`

ab ` c d a ` - e

fg a `

fg _`

fg#h `

298.15

237.326

9819.8

156464.9

93.716

128523.0

Si Cl X g YjZ Disulphur Monochloride gas [

^

_ `

a b ` c d a e ` -

fg a `

fg _ `

fg#h `

298.15

292.148

12472.5

78558.8

116.469

43833.7

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

\ 85JANAF]

\ 85JANAF]

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SbCl k g ljm Antimony Monochloride gas n

q

rs

tu s v w t s - x

yz t s

yz rs

yz#{ s

298.15

247.802

9937.0

–26024.5

90.741

–53078.8

ScCl k g l'm Scandium Monochloride gas n

q

r s

t u s v w t x s -

yz t s

yz r s

yz#{ s

298.15

234.337

9393.6

167000.0

88.154

140717.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

359

o 93THDAp

o 95SGTEp

SGTE

360

Thermodynamic Properties of Inorganic Materials: Pure Substances

SiCl | g }'~ Silicon Monochloride gas 

‚

ƒ„

…† „ ‡ ˆ … „ - ‰

Š‹ … „

Š‹ ƒ„

Š‹Œ „

298.15

237.837

9884.0

142363.0

107.487

110316.0

SnCl | g }j~ Tin Monochloride gas 

‚

ƒ „

… † „ ‡ ˆ … ‰ „ -

Š‹ … „

Š‹ ƒ „

Š‹Œ „

298.15

253.411

9644.0

34659.0

90.691

7619.3

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

€ 94TCRAS

€ 94TCRAS

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SrCl  g Ž' Strontium Monochloride gas 

“

”•

–— • ˜ ™ – • - š

›œ – •

›œ ”•

›œ •

298.15

252.467

9800.0

–127867.0

85.233

–153279.0

TCl  g Ž' Tritium Chloride gas 

“

” •

– — • ˜ ™ – š • -

›œ – •

›œ ” •

›œ# •

298.15

196.237

8671.0

–94065.0

8.034

–96460.3

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

361

‘ 94TCRAS’

‘ 94TCRAS’

SGTE

362

Thermodynamic Properties of Inorganic Materials: Pure Substances

TaCl ž g Ÿ'  Tantalum Monochloride gas ¡

¤

¥¦

§¨© ¦

§¨ ¥¦

§¨ª¦

298.15

259.266

359824.0

106.255

328144.0

TiCl ž g Ÿ'  Titanium Monochloride gas ¡

¤

¥ ¦

© « ¦ ¬ ­ © ® ¦ -

§¨#© ¦

§¨¥ ¦

§¨ª ¦

298.15

247.659

9590.0

150795.0

105.399

119370.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¢ 93THDA£

¢ 94TCRAS£

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

TlCl ¯ Thallium Chloride °

³

´µ

¶· µ ¸ ¹ ¶ µ - º

»¼ ¶ µ

»¼ ´µ

»¼,½ µ

298.15 704.00

111.240

12680.0

–204100.0

–64.600

–184840.0

TlCl Æ g Ç'¯ Thallium Chloride gas °

³

´µ

¶· µ ¸ ¹ ¶ µ - º

»¼ ¶ µ

»¼ ´µ

»¼#½ µ

298.15

256.364

9862.0

–66918.0

80.524

–90926.4

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

363

»¾O¿OÀ ¶ µ

»¾Á¿QÀ ´µ

15560.0

22.102

± 94TCRAS² type

´ÃÂÅÄ

± 94TCRAS²

SGTE

364

Thermodynamic Properties of Inorganic Materials: Pure Substances

UCl È g É'Ê Uranium Monochloride gas Ë

Î

ÏÐ

ÑÒ Ð Ó Ô Ñ Ð - Õ

Ö× Ñ Ð

Ö× ÏÐ

Ö×Ø Ð

298.15

265.911

10378.0

189424.0

104.171

158365.0

WCl È g ÉÙÊ Tungsten Monochloride gas Ë

Î

Ï Ð

Ñ Ò Ð Ó Ô Ñ Õ Ð -

Ö× Ñ Ð

Ö× Ï Ð

Ö×Ø Ð

298.15

266.018

9483.0

553000.0

121.861

516667.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ì 94TCRASÍ

Ì 94TCRASÍ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

ZnCl Ú g ÛjÜ Zinc Monochloride gas Ý

à

áâ

ãä â å æ ã â - ç

èé ã â

èé áâ

èéê â

298.15

244.079

9545.0

28778.0

90.909

1673.6

ZrCl Ú g Û'Ü Zirconium Monochloride gas Ý

à

á â

ã ä â å æ ã ç â -

èé ã â

èé á â

èéê â

298.15

253.711

10220.0

267727.0

102.990

237020.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

365

Þ 96TCRASß

Þ 94TCRASß

SGTE

366

Thermodynamic Properties of Inorganic Materials: Pure Substances

CoClëíì Cobalt Dichloride î

ñ

òó

ô õ ó ö ÷  ô ó - ø

ùú ô ó

ùú òó

ùú,û ó

298.15 1010.0

109.20

15800.0

–311100.0

–143.919

–268191.0

 g j ì Cobalt Dichloride gasî

CoClë

ñ

298.15

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

òó

ôõ ó ö ÷ ô ó - ø

ùú ô ó

ùú òó

ùú#û ó

297.939

15149.0

–93751.0

44.820

–107114.0

ùüOýOþ ô ó

ùüÁýQþ òó

46000.0

45.545

ï 96TCRASð type




òÃÿ

ï 96TCRASð

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

CrCl
Chromium Dichloride 



 

   - 

   

 

 

298.15 1097.0

115.30

15030.0

–131.322

–356246.0

CrCl%$ g &




Chromium Dichloride gas  

   -      

' 

298.15

290.059

–147269.0

Landolt-B¨ornstein New Series IV/19A co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–395400.0

14112.0

–134318.0

43.437

367

 

 

45000.0

41.021

 94TCRAS type

!#"

 94TCRAS

SGTE

368

Thermodynamic Properties of Inorganic Materials: Pure Substances

CrCl( O ) g *,+ Chromium Dichloride Oxide gas -

0

1 2

342 56 -  3 7 2 89 32

89 12

89: 2

298.15

335.123

16431.0

–14.073

–336944.0

–341140.0

CrCl( O(%) g *,+ Chromium Dichloride Dioxide gas -

0

1 2

3 42 5 6 - 3 7 2 89 3 2

89 1 2

89': 2

298.15

329.522

18042.0

–122.247

–481552.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–518000.0

. 94TCRAS/

. 94TCRAS/

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Cs; Cl;%< g =,> Dicesium Dichloride gas ?

B

C D

EFD GH -  E I D JK ED

JK CD

JK'L D

298.15

384.577

20944.0

–8.962

–641986.0

–644658.0

CuCl;> Copper Dichloride ?

B

C D

EFD GH -  E I D JK ED

JK CD

JKL D

298.15 675.00 871.00

108.07

14983.0

–148.159

–173726.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–217900.0

369

@ 94TCRASA

JMNO ED

JMNO CD

700.0 15000.0

1.037 17.222

@ 96TCRASA type

C!PQC C!P#R

SGTE

370

Thermodynamic Properties of Inorganic Materials: Pure Substances

CuClS%T g UWV Copper Dichloride gas X

[

\ ]

^_] `a -  ^ b ] cd ^]

cd \]

cdfe ]

298.15

295.590

13393.0

39.361

–43225.5

–31490.0

ClS CuS%T g UWV Dicopper Dichloride gas X

[

\ ]

^ _] ` a - ^ b ] cd ^ ]

cd \ ]

cdfe ]

298.15

339.833

19087.0

50.454

–55144.9

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–40102.0

Y 96TCRASZ

Y 96TCRASZ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

PClg OF h g ikj Phosphorus Dichloride Fluoride Oxide gas l

o

p q

rsq tu -  r v q wx rq

wx pq

wx'y q

298.15

320.386

16430.6

–147.748

–722332.0

–766383.3

PClg F h g i,j Phosphorus Dichloride Fluoride gas l

o

p q

r sq t u - r v q wx r q

wx p q

wxy q

298.15

307.919

14868.0

–57.642

–494721.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–511907.0

371

m 85JANAFn

m 94TCRASn

SGTE

372

Thermodynamic Properties of Inorganic Materials: Pure Substances

PClz F{%| g },~ Phosphorus Dichloride Trifluoride gas 

‚

ƒ „

…†„ ‡ˆ -  … ‰ „ Š‹ …„

Š‹ ƒ„

Š‹fŒ „

298.15

335.428

19047.0

–232.930

–1052550.0

–1122003.0

FeClz~ Iron Dichloride 

‚

ƒ „

…†„ ‡ˆ -  … ‰ „ Š‹ …„

Š‹ ƒ„

Š‹Œ „

298.15 950.00

118.06

16100.0

–132.299

–301855.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

€ 94TCRAS

–341300.0

ŠŽ …„

ŠŽ ƒ„

42830.0

45.084

€ 96TCRAS type

ƒ!‘#’

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

FeCl“•” g –W— Iron Dichloride gas ˜

›

œ 

žŸ  ¡ -  ž ¢  £¤ ž

£¤ œ

£¤'¥ 

298.15

293.837

15584.0

43.478

–158779.0

–145816.0

GaCl“•” g –W— Gallium Dichloride gas ˜

›

œ 

ž Ÿ   ¡ - ž ¢  £¤ ž 

£¤ œ 

£¤'¥ 

298.15

302.925

13513.0

39.119

–232642.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–220979.0

373

™ 96TCRASš

™ 94TCRASš

SGTE

374

Thermodynamic Properties of Inorganic Materials: Pure Substances

Ga¦ Cl¦%§ g ¨W© Digallium Dichloride gas ª

­

® ¯

°±¯ ²³ -  ° ´ ¯ µ¶ °¯

µ¶ ®¯

µ¶'· ¯

298.15

353.531

19488.0

48.998

–235582.0

–220973.0

GeCl¦•§ g ¨W© Germanium Dichloride gas ª

­

® ¯

° ±¯ ² ³ - ° ´ ¯ µ¶ ° ¯

µ¶ ® ¯

µ¶'· ¯

298.15

295.825

13277.0

41.656

–183420.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

–171000.0

« 94TCRAS¬

« 94TCRAS¬

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MgCl¸•¹ H ¸ O º Magnesium Chloride—Water (1/1) »

¿ À

ÁÂ'ÃÀ

Á¿À

ÁÂ'ÄÀ

298.15

137.235

–966629.5

–351.768

–861750.0

¾

¿ À

à ÇÀ È É - Ã Ê À ÁÂfà À

Á¿ À

ÁÂÄ À

298.15

286.705

13363.7

–85.864

–288200.0

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

¼ 93THDA½

¾

SiH¸ Cl¸%Å g Æ,º Dichlorosilane gas »

–313800.0

375

¼ 93THDA½

SGTE

376

Thermodynamic Properties of Inorganic Materials: Pure Substances

HfClËÌ Hafnium Dichloride Í

Ð

Ñ Ò

ÓÔ'ÕÒ

ÓÔÑÒ

ÓÔ'ÖÒ

298.15

129.704

–543920.0

–136.935

–503093.0

HfClË•× g ØWÌ Hafnium Dichloride gas Í

Ð

Ñ Ò

Õ ÙÒ Ú Û - Õ Ü Ò ÓÔfÕ Ò

ÓÔÑ Ò

ÓÔ'Ö Ò

298.15

298.136

14284.2

31.497

–247879.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Î 73BarÏ

–238488.0

Î 93THDAÏ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

HgClÝÞ Mercury Chloride ß

â

ã ä

åæ'çä

åæãä

åæ'èä

298.15 550.00

144.494

–230120.0

–163.892

–183443.0

HgClݕð g ñWÞ Mercury Chloride gas ß

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

åéêëãä

type

19413.8

35.298

ãíìïî

ã ä

çòä óô -  ç õ ä åæfçä

åæãä

åæèä

298.15

294.801

14543.6

–13.585

–144431.0

Landolt-B¨ornstein New Series IV/19A

à 85JANAFá

åéêëfçä

â

–146293.6

377

à 85JANAFá

SGTE

378

Thermodynamic Properties of Inorganic Materials: Pure Substances

Hgö Clö÷ Dimercury Dichloride ø

û

ü ý

þÿ
ý  - þ ý



þý

298.15

192.535

23476.4

–264926.7

InClö÷ Indium Dichloride ø

û

ü ý



298.15

122.173

–362752.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

þ ý





üý

–158.556

üý

 

–201.157

 

ý

ù 85JANAFú

–209327.0

ý

ù 73Barú

–315479.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

InCl  g  Indium Dichloride gas  



 


 

298.15

314.203

13956.0

-

 94TCRAS







–201484.0

 

33.474



 !

–211464.0

In Cl " g # Diindium Dichloride gas  

  

298.15

372.418

20224.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 


-

 







379



–232177.0

 94TCRAS 

 

34.039

 !



–242326.0

SGTE

380

Thermodynamic Properties of Inorganic Materials: Pure Substances

K$ Cl$"% g &' Dipotassium Dichloride gas ( +

,-

./
01

.2

298.15

352.858

20133.4

-

.-

34

) 85JANAF* 34

–617642.1

, -

0.419

-

34 5

–617767.0

Li$ Cl$"% g &#' Dilithium Dichloride gas ( +

, .

298.15

288.776

15485.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

/
01

-

. 2

-

34

.

-

–598546.3

) 85JANAF* 34

, -

7.457

34 5

-

–600770.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

381

MgCl687 Magnesium Chloride 9 <

=>

?> @A
B

298.15 987.00

89.620

13770.0

-

?> C

: 94TCRAS;

DE

?>

–644300.0

DFE

= >

–166.130

>

DEHG

43100.0

<

=>

?> @
AB

298.15

277.023

14284.2

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

?>

-

?> C

DE

?>

–392459.2

DFIMJNL

= >

–594768.0

MgCl6 S g T7 Magnesium Chloride gas 9

sp art

DIKJKL

43.668

type =PORQ

: 85JANAF; DE

= >

21.273

DE G

>

–398802.0

SGTE

382

Thermodynamic Properties of Inorganic Materials: Pure Substances

MnClUWV Manganese Dichloride X

Y 94SGTEZ

[

\]

^_ `]

^_\ ]

^_ aF]

298.15 923.00

118.198

–481996.8

–137.101

–441120.0

^bKcNde`]

^bKcNd\ ]

37656.0

40.797

MnClU j g klV Manganese Dichloride gas X [

\]

`] m
no

298.15

296.384

14371.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

`] p

type \gfih

Y 94TCRASZ

^_e`]

^_\ ]

^_ aF]

–261704.0

41.085

–273953.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoClq8r Molybdenum Dichloride s v

wx

yx z{
|

298.15

95.000

14000.0

-

yx }

~

t 94TCRASu

yx

~F

–290000.0

w x

–156.639

~H€

x

–243298.0

MoClq  g ‚r Molybdenum Dichloride gas s v

w x y

298.15

296.097

14269.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

x z
{|

-

y }

x

~

y

383

x

110000.0

~F

t 94TCRASu w x

44.458

~e€

x

96744.8

SGTE

384

Thermodynamic Properties of Inorganic Materials: Pure Substances

MoClƒ O „ Molybdenum Dichloride Oxide … ˆ

‰Š

‹Š Œ
Ž

‹Š 

298.15

125.000

18000.0

-

‹Š

‘

‘

–530000.0

† 94TCRAS‡ ‰ Š

–229.212

Š

‘ ’

–461660.0

MoClƒ O “ g ”„ Molybdenum Dichloride Oxide gas … ˆ

‰ Š ‹

298.15

340.645

16496.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Š Œ
Ž

-

‹ 

Š

‘

‹

Š

–310000.0

‘

‰ Š

–13.568

† 94TCRAS‡ ‘H’

Š

–305955.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

385

MoCl• O•W– Molybdenum Dichloride Dioxide — š

›œ

œ žŸ
 

298.15 449.00

135.60

19600.0

-

œ ¡

¢£

œ

–724000.0

¢F£

› œ

–321.186

˜ 94TCRAS™ ¢£H¤

œ

¢¥K¦K§

17000.0

š

›œ

œ ž
Ÿ 

298.15

337.779

18401.2

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

œ ¡

¢£

œ

–633039.2

¢£

› œ

–119.007

¢F¥M¦N§

› œ

–628238.0

MoCl• O•"ª g «– Molybdenum Dichloride Dioxide gas —

sp art

œ

¢£ ¤

37.862

type ›P¨R©

˜ 85JANAF™ œ

–597557.0

SGTE

386

Thermodynamic Properties of Inorganic Materials: Pure Substances

Na¬ Cl¬"­ g ®¯ Disodium Dichloride gas ° ³

´µ

¶µ ·
¸¹

¶µ º

298.15

325.445

18447.3

-

»¼

¶µ

± 85JANAF² »¼

–566095.2

´ µ

–0.234

»¼ ½

–566025.0

NbCl¬¾¯ Niobium Dichloride ° ³

´ µ

298.15

117.152

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

»¼

¶

µ

–407103.2

µ

± 93THDA² »¼

´ µ

–142.197

»¼ ½

µ

–364707.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

387

NbCl¿ O À Niobium Dichloride Oxide Á

 93THDAÃ

Ä

ÅÆ

ÇÈ ÉÆ

ÇÈÅ Æ

ÇÈ ÊFÆ

298.15

121.336

–774040.0

–240.586

–702309.0

NiCl¿8À Nickel Chloride Á Ä

Å Æ

ÉÆ ËÌ
Í

298.15 1304.00

98.10

14420.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

 96TCRASÃ

-

ÉÆ Î

ÇÈ ÉÆ

ÇFÈ Å Æ

ÇÈHÊFÆ

–304800.0

–154.775

–258654.0

ÇÏKÐKÑeÉÆ

ÇFÏMÐNÑ Å Æ

77900.0

59.739

type ÅPÒRÓ

SGTE

388

Thermodynamic Properties of Inorganic Materials: Pure Substances

NiClÔÖÕ g ×lØ Nickel Chloride gas Ù Ü

ÝÞ

ßÞ à
áâ

ßÞ ã

298.15

294.364

14230.0

-

äå

Ú 96TCRASÛ ßÞ

äFå

–73990.0

Ý Þ

äåeæ

41.489

Þ

–86359.9

NpClÔ O Ø Neptunium Dichloride Oxide Ù Ü

Ý Þ

298.15

140.164

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

äå

ß

Þ

–1028427.2

äå

Ý Þ

–235.948

Ú 73BarÛ äåeæ

Þ

–958079.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Clç O è g éê Dichlorine Oxide gas ë î

ïð

ñð ò
óô

ñð õ

298.15

267.965

11694.3

-

ì 85JANAFí

ñð

ö÷

ö÷

87864.0

ï ð

ö÷eø

–57.688

ð

105064.0

SClç O è g éê Sulphur Dichloride Oxide gas ë î

ï ð ñ

298.15

307.415

14831.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

ð ò
óô

-

ñ õ

ð

ö÷

ñ

389

ð

–212000.0

ö÷

ì 94TCRASí ï ð

–50.307

ö÷Hø

ð

–197001.0

SGTE

390

Thermodynamic Properties of Inorganic Materials: Pure Substances

TeClù O ú g ûü Tellurium Dichloride Oxide gas ý

298.15

þ 93THDAÿ




     -

 




 

334.829

16627.2

–184096.0

–40.044

–172157.0

ThClù O ü Thorium Dichloride Oxide ý

298.15

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

þ 73Barÿ




  




 

133.051

–1235953.6

–244.401

–1163090.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

TiCl O  g  Titanium Dichloride Oxide gas 





! "    - #

$% 

$% 

$%& 

298.15

321.010

16706.7

–545551.8

–35.362

–535008.0

UCl O  Uranium Dichloride Oxide 



 

$%  

$%  

$%& 

298.15

138.323

–1066920.0

–237.529

–996101.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

391

 85JANAF

 93Bar

SGTE

392

Thermodynamic Properties of Inorganic Materials: Pure Substances

WCl' O ( Tungsten Dichloride Oxide )

,

-.

/0. 1 2  / . - 3

45 /.

45 -.

4576 .

298.15

150.000

22000.0

–613000.0

–208.270

–550904.0

WCl' O 8 g 9( Tungsten Dichloride Oxide gas )

,

- .

/ 0. 1 2 / 3 . -

45 / .

45 - .

456 .

298.15

336.816

16496.0

–224000.0

–21.455

–217603.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

* 94TCRAS+

* 94TCRAS+

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

Pb: Cl; O;=< Trilead Dichloride Dioxide >

BC

DE7FC

DE BC

DE7GHC

298.15

258.262

–835963.2

–364.364

–727328.0

A

B C

F MC N O F P C -

DEF C

DE B C

DE7G C

298.15

311.094

16028.9

–354803.2

–149.202

–310319.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

? 94SGTE@

A

SCl; O;JI g KL< Sulphur Dichloride Dioxide gas >

393

? 85JANAF@

SGTE

394

Thermodynamic Properties of Inorganic Materials: Pure Substances

SnClQ OQSR g TLU Tin Dichloride Dioxide gas V

Y

Z[

\][ ^ _  \ [ - `

ab \[

ab Z[

ab7c [

298.15

340.059

18401.2

–564421.6

–139.347

–522875.0

UClQ O QdU Uranium Dichloride Dioxide V

Y

Z[

ab \[

ab Z[

abc [

298.15 850.00

150.624

–1243484.0

–327.802

–1145750.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

W 93THDAX

W 91KnaX

aegfgh \[

aHeifjh Z[

type

44057.5

51.832

Zlknm

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

UClo O oSp g qr Uranium Dichloride Dioxide gas s

v

wx

yz7{x

yz wx

yz7|Hx

298.15

372.485

–973901.0

–105.941

–942315.0

WClo Oo=r Tungsten Dichloride Dioxide s

v

w x

yz7{ x

yz w x

yz7| x

298.15

200.832

–780316.0

–260.012

–702793.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

395

t 91Knau

t 85JANAFu

SGTE

396

Thermodynamic Properties of Inorganic Materials: Pure Substances

WCl} O}J~ g L€ Tungsten Dichloride Dioxide gas 

„

…†

‡ˆ† ‰ Š  ‡ † - ‹

Œ ‡†

Œ …†

Œ7Ž †

298.15

353.921

19501.6

–671532.0

–106.923

–639653.0

SnCl} OJ~ g L€ Tin Dichloride Tetraoxide gas 

„

… †

‡ ˆ† ‰ Š ‡ ‹ † -

Œ ‡ †

Œ … †

Œ7Ž †

298.15

379.347

22765.1

–702075.2

–305.206

–611078.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

‚ 85JANAFƒ

‚ 93THDAƒ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

PClJ‘ g ’“ Phosphorus Dichloride gas ”

˜™

š›™ œ   š ™ - ž

Ÿ  š™

ŸH  ˜™

Ÿ ¡ ™

298.15

285.122

12249.0

–54292.0

20.954

–60539.4

—

˜™

Ÿ  š™

Ÿ  ˜™

Ÿ 7¡ ™

298.15 774.00

135.980

–359405.6

–151.899

–314117.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

• 94TCRAS–

—

PbCl=“ Lead Chloride ”

397

• 85JANAF–

Ÿ¢g£j¤ š™

Ÿ¢g£j¤ ˜™

type

21882.3

28.272

˜¦¥¨§

SGTE

398

Thermodynamic Properties of Inorganic Materials: Pure Substances

PbCl©Jª g «¬ Lead Chloride gas ­

°

±²

³´² µ ¶  ³ ² - ·

¸¹ ³²

¸¹ ±²

¸¹7º ²

298.15

315.616

14002.0

–175548.0

27.737

–183818.0

PdCl©=¬ Palladium Dichloride ­

°

±²

¸¹ ³²

¸¹ ±²

¸¹7º ²

298.15 952.00

103.763

–173175.8

–157.139

–126325.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

® 94TCRAS¯

® 73Bar¯

¸»g¼j½ ³²

¸»g¼j½ ±²

type

18409.6

19.338

±¦¾¨¿

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

PdClÀJÁ g ÂÃ Palladium Dichloride gas Ä

Ç

ÈÉ

ÊË7ÌÉ

ÊHË ÈÉ

ÊËÍHÉ

298.15

313.700

121545.2

52.798

105803.0

PtClÀdà Platinum Dichloride Ä

Ç

È É

ÊË7Ì É

ÊË È É

ÊË7Í É

298.15

129.704

–110876.0

–135.006

–70624.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

399

Å 73BarÆ

Å 73BarÆ

SGTE

400

Thermodynamic Properties of Inorganic Materials: Pure Substances

RbÎ ClÎJÏ g ÐLÑ Dirubidium Dichloride gas Ò

Õ

Ö×

ØÙ× Ú Û  Ø × - Ü

ÝÞ Ø×

ÝÞ Ö×

ÝÞ7ß ×

298.15

374.467

20785.0

–618373.0

–2.164

–617728.0

RhClÎJÏ g ÐLÑ Rhodium Dichloride gas Ò

Õ

Ö ×

ÝÞ Ø ×

ÝHÞ Ö ×

ÝÞß ×

298.15

288.387

126775.2

33.752

116712.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ó 94TCRASÔ

Ó 94SGTEÔ

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SClà=á Sulphur Dichloride â

æç

èé7êç

èHé æç

èé7ëHç

298.15

183.678

–49790.0

–71.471

–28480.9

å

æ ç

ê îç ï ð ê ñ ç -

èéê ç

èHé7æ ç

èéë ç

298.15

281.630

12443.2

–17572.8

26.481

–25468.1

Landolt-B¨ornstein New Series IV/19A

w

ww

en s be

DF is P

Th

ha

in

de ga

ified

mod

us

mo

om

f.c

pd

ts .ar

n of

rsio

ve

AR

TS

PD

are

ftw

F so

ã 85JANAFä

å

SClàJì g íLá Sulphur Dichloride gas â

401

ã 85JANAFä

SGTE

402

Thermodynamic Properties of Inorganic Materials: Pure Substances

Sò Clòdó Disulphur Dichloride ô

÷

øù

úû7üù

úHû øù

úû7ýHù

298.15

221.752

–58157.6

–65.467

–38638.6

Sò Clòÿþ g ó Disulphur Dichloride gas ô

÷

ø ù

ü
ù  ü  ù

úûü ù

úHû7ø ù

úûý ù

298.15

327.215

16480.8

–16736.0

39.996

–28660.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

õ 73Barö

-

õ 85JANAFö

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances 

SeCl  g

Selenium Dichloride gas

73Bar











298.15

295.709

–33472.0

30.664

–42614.5



Se Cl Diselenium Dichloride 

 



298.15

246.856

–83680.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so



403

73Bar  

 

–60.155

–65744.8

SGTE

404

Thermodynamic Properties of Inorganic Materials: Pure Substances

Se Cl  g 

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

ve

AR

TS

PD

m are

ftw

F so

" 74Mil#

%&

'()&

'(%&

'(*&

298.15

353.908

–21756.8

46.897

–35739.1



Silicon Dichloride gas !

$

% & )

298.15

281.612

12529.0

SGTE

mo

Diselenium Dichloride gas !

$

SiCl+ g 

sp art



& ,-.

-

) /

&

'()

" 94TCRAS# &

–163069.0

'(% &

'(* &

39.723

–174912.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

405

SmCl021 Samarium Dichloride 3

4 73Bar5

6

78

9:;8

9:7<8

9:=8

298.15

127.612

–818390.4

–164.963

–769207.0

SnCl021 Tin Dichloride 3 6

78

;8 >?@

298.15 520.20

134.10

17330.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

4 94TCRAS5

-

;A8 B

9:;8

9:7<8

9:C=8

–333000.0

–140.159

–291212.0

9DFEFG;8

9DHEIG7<8

14520.0

27.912

type 7KJML

SGTE

406

Thermodynamic Properties of Inorganic Materials: Pure Substances

SnClNPO g Q R

Tin Dichloride gas S

V

WX

YAX Z[\

298.15

305.898

13682.0

-

YX ]

^_

T 94TCRASU YX

–202648.0

^_

W<X

31.639

^_`

X

–212081.0

SrClNaR Strontium Chloride S V

WX

YAX Z[\

298.15 1000.0 1147.0

114.809

16242.3

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

YX ]

T 85JANAFU ^_

YX

–828850.4

^_

W<X

–163.964

^_`

X

^bHcId

YX

^bFcId

W<X

–779965.0 6008.2 16221.4

6.008 14.142

type WAefW WAehg

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

SrCli j g kml Strontium Chloride gas n q

rs

tAs uvw

298.15

316.336

14447.4

TaCli+j g k l

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

yz

ts

o 85JANAFp yz

–473210.4

r<s

37.563

Tantalum Dichloride gas n

q

r s

298.15

298.387

Landolt-B¨ornstein New Series IV/19A

ts x

-

yz

t

s

–66944.0

yz

r s

33.836

407

yz{

s

–484410.0

o 93THDAp yz{

s

–77032.2

SGTE

408

Thermodynamic Properties of Inorganic Materials: Pure Substances

TeCl|+} g ~m Tellurium Dichloride gas €

 93THDA‚

ƒ

„…

†‡ˆ…

†‡„<…

†‡‰…

298.15

305.663

–112968.0

33.363

–122915.0

ThCl|2 Thorium Dichloride € ƒ

„ …

†‡ˆ

298.15

125.353

–718392.8

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

…

 93THDA‚ †‡„ …

†‡‰ …

–149.526

–673812.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

409

TiClŠ2‹ Titanium Dichloride Œ 

‘

’‘ “”•

298.15 1308.0

87.350

13300.0

-

’A‘ –

 94TCRASŽ —˜

’‘

–515000.0

—˜

<‘

–166.449

‘

—˜C™

34300.0



‘

’A‘ “”•

298.15

283.542

13987.0

Landolt-B¨ornstein New Series IV/19A

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

’‘

-

’‘ –

—˜

’‘

–225018.0

—šH›Iœ

<‘

–465373.0

TiClŠ+Ÿ g  m‹ Titanium Dichloride gas Œ

sp art

—šF›Fœ

26.223

type KMž

 94TCRASŽ —˜

<‘

29.743

—˜™

‘

–233886.0

SGTE

410

Thermodynamic Properties of Inorganic Materials: Pure Substances

Tl¡ Cl¡+¢ g £¥¤ Dithallium Dichloride gas ¦ ©

ª«

¬A« ­®¯

298.15

389.686

20697.0

UCl¡+¢ g £

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¬«

±²

±²

–238148.0

ª<«

38.007

«

±²³

–249480.0

Uranium Dichloride gas ¦

©

ª « ¬

298.15

339.207

16435.0

SGTE

sp art

¤

¬« °

-

§ 94TCRAS¨

« ­®¯

-

¬ °

«

±²

¬

«

–159110.0

§ 94TCRAS¨ ±²

ª «

65.928

±²³

«

–178766.0

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

411

VCl´2µ Vanadium Dichloride ¶ ¹

º»

¼» ½¾¿

298.15 1623.0

99.420

14340.0

VCl´+É g Ê

co df. n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

¼A» À

ÁÂ

¼»

–451000.0

ÁÂ

º<»

–154.549

»

ÁÂCÃ

ÁÄFÅFÆ

¼»

µ

Vanadium Dichloride gas ¶

¹

º»

¼A» ½¾¿

298.15

306.784

13768.0

-

¼» À

ÁÂ

¼»

–187993.0

ÁÄHÅIÆ

º<»

–404921.0 35000.0

Landolt-B¨ornstein New Series IV/19A

sp art

-

· 94TCRAS¸

21.565

type ºKÇMÈ

· 94TCRAS¸ ÁÂ

º<»

52.815

ÁÂÃ

»

–203740.0

SGTE

412

Thermodynamic Properties of Inorganic Materials: Pure Substances

WClËÍÌ Tungsten Dichloride Î

Ï 85JANAFÐ

Ñ

ÒÓ

ÔÕÖÓ

ÔÕÒ<Ó

ÔÕ×Ó

298.15

130.541

–257316.0

–125.156

–220001.0

WClËÙØ g ÚmÌ Tungsten Dichloride gas Î Ñ

Ò Ó Ö

298.15

309.412

14627.3

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

Ó ÛÜÝ

-

Ö Þ

Ó

ÔÕÖ

Ó

–12552.0

Ï 85JANAFÐ ÔÕÒ Ó

ÔÕ× Ó

53.715

–28567.1

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

413

YbClß2à Ytterbium Dichloride á

â 93THDAã

ä

åæ

çèéæ

çèå<æ

çèêæ

298.15

130.541

–799562.4

–152.369

–754134.0

ZnClß2à Zinc Chloride á ä

åæ

éæ ëìí

298.15 598.00

111.50

15050.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

â 96TCRASã

-

éAæ î

çèéæ

çèå<æ

çèCêæ

–416000.0

–153.210

–370320.0

çïFðFñéæ

çïHðIñå<æ

10300.0

17.224

type åKòMó

SGTE

414

Thermodynamic Properties of Inorganic Materials: Pure Substances

ZnClôPõ g ö ÷

Zinc Chloride gas ø

û

üý

þAý ÿ


298.15

276.367

13959.0

-

þý 

ù 96TCRASú



þý

–268091.0



ü<ý

11.657

 

ý

–271567.0

ZrClô2÷ Zirconium Dichloride ø û

üý

þý ÿ


298.15 995.00

110.00

15000.0

SGTE

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

þAý 



ù 94TCRASú þý

–500000.0

 

ü<ý

–152.260



ý

  

þý

  

ü<ý

–454604.0 27000.0

27.136

type ü

Landolt-B¨ornstein New Series IV/19A

Thermodynamic Properties of Inorganic Materials: Pure Substances

ZrCl g  Zirconium Dichloride gas  

"!

#$! %
&'

298.15

310.580

13722.0

Landolt-B¨ornstein New Series IV/19A

co df.

sp art

n of

rsio

w.

ww

en s be

DF is P

Th

ha

ing

mod

ified

us

a de

mo

ve

AR

TS

PD

m are

ftw

F so

-

#(! )

*+

#(!

–118982.0

415

 94TCRAS *+

,!

48.320

*+ -

!

–133389.0

SGTE