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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
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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
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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 + Beryllium Monofluoride gas
-
298.15
205.752
8711.0
–170624.0
94.857
–198906.0
BeF Beryllium Fluoride
-
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
!
!
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( g @ Beryllium Fluoride gas
¡ ¢
£¤¢ ¥¦ £ ¢ - §
¨© £¢
¨© ¡¢
¨©ª ¢
298.15
227.278
10880.0
–796588.0
14.989
–801057.0
BeH g @ 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
94TCRAS
94TCRAS
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
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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
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DF is P
Th
ha
ing
mod
ified
us
a de
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PD
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F so
-
93THDA
94TCRAS
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
BeS ! g "$# Beryllium Sulphide gas %
(
)*
+,* -. + * - /
01 +*
01 )*
01 2 *
298.15
210.289
8778.0
263592.0
168.719
213288.0
Be3 C # Diberyllium Carbide%
(
)*
01 +*
01 )*
0142 *
298.15 2400.00
16.318
–90793.0
–8.424
–88281.4
Landolt-B¨ornstein New Series IV/19A
co df.
sp art
n of
rsio
w.
ww
en s be
DF is P
Th
ha
ing
mod
ified
us
a de
mo
ve
AR
TS
PD
m are
ftw
F so
13
& 85JANAF'
& 85JANAF'
05768 +*
05768 )*
type
75312.0
31.380
)9;:
SGTE
14
Thermodynamic Properties of Inorganic Materials: Pure Substances
Be< Cl=?> g @BA Diberyllium Tetrachloride gas C
F
GH
IJH KL I H - M
NO IH
NO GH
NOQP H
298.15
366.333
22641.0
–819621.0
–98.825
–790156.0
O(BeF)> g @BA Diberyllium Difluoride Oxide gas C
F
G H
I JH K L I M H -
NO I H
NO G H
NO P H
298.15
298.910
16585.4
–1204573.6
–25.452
–1196980.0
SGTE
co df.
sp art
n of
rsio
w.
ww
en s be
DF is P
Th
ha
ing
mod
ified
us
a de
mo
ve
AR
TS
PD
m are
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F so
D 94TCRASE
D 85JANAFE
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
BeR FS?T g U$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 Og g B Triberyllium Trioxide gas
-
298.15
273.341
13321.9
–1054368.0
–62.880
–1035620.0
Be O? g B Tetraberyllium Tetraoxide gas
-
4
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
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F so
17
85JANAF
85JANAF
SGTE
18
Thermodynamic Properties of Inorganic Materials: Pure Substances
Be Og g B Pentaberyllium Pentaoxide gas
¡ - ¢
£¤
£¤
£¤4¥
298.15
323.282
19087.4
–2112920.0
–237.086
–2042230.0
Be¦ O¦g g B Hexaberyllium Hexaoxide gas
¡ ¢ -
£¤
£¤
£¤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
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F so
85JANAF
85JANAF
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
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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
298.15 564.00
123.428
–55772.7
8.623
–58343.8
BiI g $ Bismuth Monoiodide gas
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
73Bar
type
1297.0
2.300
93THDA
SGTE
26
Thermodynamic Properties of Inorganic Materials: Pure Substances
BiIf Bismuth Triiodide
298.15 682.00
224.681
–150624.0
–6.262
–148757.0
BiIn¤ g ¥$ Bismuth Triiodide gas
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
¡\
¡_
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
ÁÊËÌÃÀ
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
ÜáâãÚÛ
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
CHBrF% g
= Bromodifluoromethane gas
298.15
295.225
13169.0
-
–422000.0
94TCRAS "
–54.751
–405676.0
CBrF I g
Bromodifluoroiodomethane gas
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
-
–325000.0
–0.082
94TCRAS
–324975.0
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
CBrF g Bromotrifluoromethane gas
¡¢£
¤
298.15
297.822
14468.3
-
¥ ¦
85JANAF ¥ ¦
–648938.4
"
–88.209
¥ ¦ §
–622639.0
CHBrI¨© g Bromodiiodomethane gas
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
¡¢£
-
¤
¥ ¦
165000.0
39
94TCRAS ¥ ¦
91.816
¥ ¦L§
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
65 789
298.15
267.530
10406.0
-
65 :
;<
65
–206829.0
1 94TCRAS2 ;<
45
106.195
5
;
–238491.0
CuBr . Copper Monobromide 0 3
45
65 789
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 PQR
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 PQR
-
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 def
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 def
-
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 wxy
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 wxy
-
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
298.15
251.827
9932.0
-
94TCRAS
–17968.0
134.995
–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
-
137439.0
94TCRAS
150.026
92708.7
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
HBr g / Hydrogen Bromide gas
298.15
198.697
8648.0
-
94TCRAS
–36290.0
57.252
W
–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
-
51
–480928.0
28.718
94TCRAS
–489490.0
SGTE
52
Thermodynamic Properties of Inorganic Materials: Pure Substances
SiH¡ Br ¢ g £¤ Bromosilane gas ¥ ¨
©ª
ǻ ¨
298.15
262.463
11769.6
-
«ª ¯
°±
¦ 85JANAF§ «ª
–78240.8
° ±
©ª
–28.472
°± ²
ª
–69751.9
NH³ Br ¤ Ammonium Bromide¥ ¨
©ª
ǻ ¨
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
°´$µ'¶
©ª
–176006.0 3221.7
7.839
type ©B·+©
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
HgBr ¸ g ¹/º Mercury Monobromide gas » ¾
¿À
ÁÀ ÂÃÄ
ÁÀ Å
298.15
271.546
10250.8
-
ÁÀ
ÆÇ
¼ 85JANAF½ Æ Ç
104181.6
¿À
110.134
À
ÆÇ È
69157.5
IBr ¸ g ¹º Iodine Bromide gas » ¾
¿ À Á
298.15
258.809
9911.0
Landolt-B¨ornstein New Series IV/19A
co df.
sp art
n of
rsio
w.
ww
en s be
DF is P
Th
ha
ing
mod
ified
us
a de
mo
ve
AR
TS
PD
m are
ftw
F so
À ÂÃÄ
-
Á Å
À
53
¼ 94TCRAS½ ÆÇ
Á
À
40807.0
ÆÇ
¿ À
124.635
ÆÇWÈ
À
3647.2
SGTE
54
Thermodynamic Properties of Inorganic Materials: Pure Substances
InBr É Indium Monobromide Ê
Ë 73BarÌ
Í
ÎÏ
ÐÑ ÒÏ
ÐÑÎÏ
ÐÑ!Ó Ï
298.15 558.00
114.223
–175309.6
–19.532
–169486.0
ÐÔ$Õ$Ö ÒÏ
Ð Ô&Õ'ÖÎÏ
24267.2
43.490
InBr Ù g ÚÉ Indium Monobromide gas Ê Í
ÎÏ
ÒÏ ÛÜÝ
298.15
259.614
10084.0
SGTE
co df.
sp art
n of
rsio
w.
ww
en s be
DF is P
Th
ha
ing
mod
ified
us
a de
mo
ve
AR
TS
PD
m are
ftw
F so
-
ÒÏ Þ
type ÎB×DØ
Ë 94TCRASÌ
ÐÑWÒÏ
Ð Ñ ÎÏ
ÐÑ Ó Ï
–54116.0
125.859
–91640.9
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
55
KBr ß Potassium Bromide à ã
äå
æå çèé
298.15 1007.00
95.920
12210.0
-
æå ê
á 94TCRASâ ëì
æå
–393450.0
ëì
äå
–44.865
å
ëì!í
ëî$ï$ð
25520.0
ã
äå
æå çèé
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 ýþÿ
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 ýþÿ
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 }
"
$ - %
%
)
298.15
249.212
9506.0
162464.7
132.017
123104.0
PbBr z g {| Lead Monobromide gas }
" $
-
+
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 Bromide
" $ - %
%
)
298.15 965.00
110.100
13060.0
–394770.0
–42.781
–382015.0
RbBr g = Rubidium Bromide gas
" $ - %
%
)
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
%
S )
23300.0
24.145
94TCRAS type
UW
94TCRAS
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
-
298.15
327.649
16322.0
–41003.0
–97.405
–11961.7
CaBr{ Calcium Bromide
-
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
CaBrj g Calcium Bromide gas
¡ ¢
£¤¢ ¥¦ £ ¢ - §
¨© £¢
¨© ¡¢
¨©.ª ¢
298.15
310.128
15603.0
–387197.0
116.330
–421881.0
CdBr« 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
94TCRAS
73Bar
¨¬® £¢
¨¬® ¡¢
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±´ 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¸
ÁÄÅÆ ¼»
ÁÄÅÆ 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
ÛÞßà ÖÕ
ÛÞßà ÔÕ
45000.0
40.359
type
Ôáâ
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:
=: ABC
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 lmn
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 lmn
-
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
-
}|
x 85JANAFy
}|
–190372.0
{#|
8.348
>
|
–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
}|
–169452.0
x 85JANAFy
{#|
–67.203
|
((
}|
*
+,
{#|
–151603.0 17907.5
34.839
type {.0
SGTE
86
Thermodynamic Properties of Inorganic Materials: Pure Substances
HgBrO g R Mercury Dibromide gas
298.15
320.231
15656.5
-
85JANAF *
–85454.0
#
82.714
–112303.0
Hg Br Dimercury Dibromide
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
–204179.2
85JANAF
–104.071
>
–177525.0
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
InBr g Indium Dibromide gas ¡ ¤
¥¦
§¦ ¨©ª
§¦ «
298.15
333.551
14424.0
-
§¦
¬
¢ 94TCRAS£ ¬
–149729.0
¥#¦
123.691
¦
¨
–186607.0
In Br g ¯ 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 »¼½
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 »¼½
-
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
MgBrÂÃ Magnesium Bromide Ä Ç
ÈÉ
ÊÉ ËÌÍ
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 ËÌÍ
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
MnBrÙÚ Manganese Dibromide Û
Ü 93THDAÝ
Þ
ßà
áâ>ãà
áâß#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,çß#à
33472.0
34.472
type ß.è0é
Ü 93THDAÝ
Þ
ßà
áâ>ãà
áâß#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
MoBrìí 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
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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
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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
-
298.15
398.368
21696.0
–551802.0
92.606
–579412.0
SBr|n} g ( Sulphur Dibromide gas
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
94TCRAS
93THDA
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
S Br~ g Disulphur Dibromide gas
7
298.15
350.519
30961.6
134.169
–9040.9
SeBrn g ( Selenium Dibromide gas
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
Se Brn g ¡ Diselenium Dibromide gas ¢
¥
¦§
¨©ª§
¨©¦§
¨©7«§
298.15
378.134
29288.0
141.992
–13046.9
SiBrn 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 Tribromoiodomethane gas
- -
"
298.15
378.318
20856.0
170000.0
86.191
144302.0
C H Br g 1,1,1–Tribromoethane gas
-
"
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
CeBrD Cerium Bromide
-
"
298.15 1005.00
182.004
–887008.0
–115.765
–852493.0
CeBr¤ g ¥ Cerium Bromide gas
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
7 :¡-
7 :¡
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
678&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
6795
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
~}
+ |}
}
–20000.0
116.345
–54688.3
NbBrt O u g v?w Niobium Tribromide Oxide gas x {
| }
~ } ~ } -
~ }
| }
}
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
NdBr5 Neodymium Bromide
93THDA
+
298.15 955.00
194.138
–873201.0
–105.263
–841817.0
.0*
.0
45312.7
47.448
NiBr g a Nickel Tribromide gas
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
-
type
24
96TCRAS
*
*+
23299.0
116.179
–11339.8
SGTE
126
Thermodynamic Properties of Inorganic Materials: Pure Substances
POBr g a¡ Phosphorus Tribromide Oxide gas ¢ ¥
¦§
¨ ©§ ª«
298.15
359.841
19848.9
-
¨¬ §
£ 85JANAF¤
® ¨§
® ¦§
®¯ §
–406559.3
–12.135
–402941.0
TaOBr 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
34
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
HI
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
no
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 {
~
6
"
298.15 1000.00
188.280
–720903.2
–90.235
–694000.0
VBryz Vanadium Tribromide {
~
"
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}
d
"
type
43932.0
43.932
| 93THDA}
SGTE
138
Thermodynamic Properties of Inorganic Materials: Pure Substances
VBrA g . Vanadium Tribromide gas
"
298.15
142.365
–447688.0
–116.840
–412852.0
WBr g x Tungsten Tribromide gas
9 " -
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 Zirconium Tribromide
¢
£¤
¥¦9¤ §9¨ ¥ ¤ - ©
ª« ¥6¤
ª« £¤
ª«¬ ¤
298.15 1000.00
170.000
21000.0
–600000.0
–97.496
–570932.0
ZrBrA² g ³x Zirconium Tribromide gas
¢
£¤
¥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 ¸
»
¼½
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
ÑÒ
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
äå
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
pqr
–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
298.15
379.368
22313.0
-
94TCRAS
–415800.0
56.138
–432538.0
SnBrO Tin Tetrabromide
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
-
94TCRAS
–388000.0
–95.600
!
–359497.0 12150.0
40.199
type #%
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
151
SnBr g ) Tin Tetrabromide gas
¡ ¢£¤
298.15
413.228
25043.0
-
¡ ¥
¦§
94TCRAS
¡
¦§
–324217.0
57.628
¦§¨
–341399.0
TeBrO Tellurium Tetrabromide
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
73Bar ¦§
–110.132
¦§¨
¦©ª!«
¡
¦©ª!«
–162139.0 24685.6
37.803
type ¬¯®
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
ÒÓÔ
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
åæèä
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 KLM
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 def
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 g C
Vanadium Pentabromide gas
298.15
437.898
28512.0
-
94TCRAS
–393753.0
26.483
–401649.0
WBr
Tungsten Pentabromide
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
–311708.0
85JANAF
–141.183
76
76
–269614.0 17154.4
30.688
type 9;
SGTE
162
Thermodynamic Properties of Inorganic Materials: Pure Substances
WBr g > Tungsten Pentabromide gas ¢
£¤
¥¤ ¦§¨
¥¤ ©
298.15
461.404
30020.2
-
¥¤
ª«
85JANAF¡ ª«
–199158.4
£¤
48.261
¤
ª«¬
–213547.0
C Br® g > Hexabromoethane gas ¢
£ ¤ ¥
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 »¼½
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 »¼½
-
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 ÎÏÐ
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 ÎÏÐ
-
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
WBrÕÖ Tungsten Hexabromide ×
Ø 85JANAFÙ
Ú
ÛÜ
ÝÞßÜ
ÝÞÛÜ
ÝÞà2Ü
298.15
313.800
–343088.0
–175.448
–290778.0
WBrÕá 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 ãäå
-
ß æ
Ü
ÝÞçß
165
Ü
–243090.4
Ø 85JANAFÙ ÝÞÛ 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{
{
298.15
287.348
12432.0
–32.722
–265244.0
–275000.0
CHClFq_r g t3u Chlorodifluoromethane gas v
y
z {
| }{ ~ - | { | {
z {
/ {
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
-
298.15
329.098
16207.0
–49.042
–365378.0
–380000.0
CClFs
g 3 Chlorotrifluoromethane gas
-
/
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
94TCRAS
94TCRAS
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
CHCl g J Chloromethylene gas
¡ ¢£ - ¤ ¥¦
¥¦
¥¦8§
298.15
234.880
10154.0
52.258
292699.0
308280.0
CHClI¨© g 3 Chlorodiiodomethane gas
¡ ¢ £ - ¤ ¥¦
¥¦
¥¦8§
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
94TCRAS
94TCRAS
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
þÿý - 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 ÿý - 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 ) ,
-.
/. 012
/. 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
. 012
-
/ 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 DEF
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 YZ[
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 YZ[
-
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 klm
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 klm
-
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
–109.347
–70098.0
Si u CHrv 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
{
w 94SGTEx {
–545844.0
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
CCl
I g Trichloroiodomethane gas
298.15
340.604
18282.0
-
94TCRAS
10000.0
7
–57.826
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
–128005.0
27240.8
CCl Carbon Tetrachloride
185
94SGTE
–235.504
–57789.5
SGTE
186
Thermodynamic Properties of Inorganic Materials: Pure Substances
CClM g Carbon Tetrachloride gas
¡¢
£¢ ¤¥¦
298.15
309.461
17158.0
-
£¢ §
¨©
£¢
94TCRAS ¨J©
–95600.0
¡ ¢
¨© ª
–142.439
–53131.8
CoCO«¬ 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
¢
73Bar ¨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¶
·¶ ¸¹º
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 ÑÒÓ
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 ãäå
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 ãäå
-
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|
-
,
298.15
–44.847
–456910.0
CF
265.078
11522.7
–470281.6
xRy g S z { Trifluoromethane gas|
-
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
Trifluoromethylsilane gas
93THDA
CF H Si g
298.15
314.202
–1232711.0
–210.553
–1169930.0
Trifluoroiodomethane gas -
,
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
g Tetrafluoromethane gas¡ ¤ ¥¦ § ¨ ¦ ©ª - §« ¦ ¬ §¦
¬ ¥¦
¬® ¦
298.15
–149.866
–888517.0
CF
261.454
12730.0
–933200.0
¯ 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
° ±² 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 ÅÆ 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
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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
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mo
ve
AR
TS
PD
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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$ g %
Carbon Diiodide gas
298.15
304.318
12643.0
-
94TCRAS
468397.0
!
182.437
414003.0
CI$ g %
Carbon Triiodide gas
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
-
94TCRAS
405987.0
181.076
351999.0
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
CI^ g % Tetraiodomethane gas
¡¢
£
298.15
391.891
22331.0
-
94TCRAS
¤¥
¤ ¥
340000.0
!
153.871
¤¥ ¦
294123.0
IrC g % Iridium Monocarbide gas
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
¡¢
-
£
¤¥
211
761655.4
93THDA ¤ ¥
198.062
¤¥ ¦
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
-
M
298.15 1198.0 1767.0
97.20
15120.0
–1226000.0
–271.956
–1144920.0
ZnCO~8 Zinc Carbonate
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
94TCRAS
16700.0 40000.0
13.940 22.637
type
=
94SGTE
SGTE
222
Thermodynamic Properties of Inorganic Materials: Pure Substances
PbCOg PbO Lead Carbonate—Lead Oxide (1/1)
¡
¢
298.15
204.179
–816716.8
–341.457
–714911.0
CP £ g ¤P Carbon Monophosphide gas
¡ ¥ ¦ § ¡ ¨ -
5¡
¢
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
73Bar
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 ClZ g
r Dicarbon Trichloride gas
QC -
298.15
328.160
16150.0
190279.0
–17.942
195629.0
C Cl F g
@ Trichlorofluoroethylene gas
C -
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
94TCRAS
94TCRAS
SGTE
234
Thermodynamic Properties of Inorganic Materials: Pure Substances
C Cl FZ g r Trichlorotrifluoroethane gas
¡¢
¡
¡£
298.15
364.410
–742241.6
–285.876
–657008.0
C HCl " g @ Trichloroethylene gas
¢ ¤C ¥ ¦ - ¢ §
¡1¢
¡
¡£
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
93THDA
94TCRAS
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
-
y
298.15
332.185
20254.7
–1343900.8
–287.666
–1258130.0
CCH | g }~ Ethynyl gas
-
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
-
y
298.15
240.591
11866.0
610438.0
67.962
590175.0
C H * g > Ethyne ¡£¢¥¤§¦*¨ª©¬« ¦®¦¯¡ gas
-
y
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
¿À ¸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
¿À ¸ 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
óô 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
23
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
EF
G HI F
GHEF
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
YZ
[\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
mn
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 {
~
298.15
277.622
431914.3
183.958
377067.0
Si(CH
)
Cl x g y)z Trimethylchlorosilane gas {
~
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 g ) Tricarbon Dioxide gas
-
O
298.15
276.642
13945.0
–97600.0
54.269
–113780.0
Si(CH ) g T Tetramethylsilane gas
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
94TCRAS
94SGTE
SGTE
258
Thermodynamic Properties of Inorganic Materials: Pure Substances
C N g ) 3–Cyano–2–Propynylidyne gas
£
¤¥
¦§¥ ¨© ¦ ¥ - ª
« ¬ ¦ ¥
«¬ ¤¥
« ¬ ¥
298.15
285.004
15516.0
790000.0
166.231
740438.0
C N®9 g T 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
ÉÊ
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
Þß
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
òó
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 GeO
Calcium Oxide—Germanium Oxide (1/1)
,
298.15
87.362
–1285324.0
–293.037
–1197960.0
CaH g P
Calcium Monohydride gas
-
L
,
L
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
91Kna
94TCRAS
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
CaI(OH) g Calcium Hydroxide Iodide gas
¡¢ £¤ ¡ - ¥
¦§ ¡
¦§
¦§¨
298.15
319.795
16181.0
–394721.0
52.224
–410292.0
Ca(OH) g P Calcium Monohydroxide gas
¡ ¢ £ ¤ ¡ ¥ -
¦§ ¡
¦§
¦§¨
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
94TCRAS
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
ÀÍÐ
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 Sulphate
(
298.15 1473.00 1733.00
106.692
–1437622.4
–377.260
–1325140.0
CaO UO` Calcium Oxide—Uranium Trioxide (1/1)
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
-.
+.
type
5000.0 25400.0
3.394 14.657
2
73Bar
-.
+.
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)
¡¢
¡
¡£
298.15
126.357
–1622973.6
–358.143
–1516190.0
CaO V¤ O¥ Calcium Oxide—Divanadium Pentaoxide (1/1)
¡¢
¡
¡£
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
73Bar
93THDA
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
ÄÍÎ
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
âë2â âëì
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
|
}~
4g~ ~ -
~
}~
~
298.15
286.087
14426.0
–194434.0
11.208
–197776.0
CdF u g v]w Cadmium Monofluoride gas y
|
} ~
g~ ~ -
~
} ~
~
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
CdF2 Cadmium Fluoride
298.15 1333.00
83.262
–700401.6
–171.327
–649320.0
CdF g 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
:9
type
51881.6
38.921
<s
4g -
298.15
264.944
13155.0
–393245.0
10.355
–396332.0
SGTE
94SGTE
94TCRAS
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
CdH g ]¡ Cadmium Monohydride gas ¢
¥
¦§
¨4©g§ ª « ¨ § - ¬
® ¨ §
® ¦§
®¯ §
298.15
218.309
8834.0
260837.0
101.169
230673.0
Cd(OH) 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 ð 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~ Cll 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 g
Cadmiun Tetrafluoride gas
2
298.15
387.266
24481.0
-
94TCRAS
–798000.0
–121.912
–761652.0
Cd I g
Cadmiun Tetraiodide gas
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
-
–95000.0
307
94TCRAS
181.123
–149002.0
SGTE
308
Thermodynamic Properties of Inorganic Materials: Pure Substances
CeCl Cerium Chloride
93THDA
7¡2
¢
298.15 1080.00
150.959
–1053531.0
–253.113
–978065.0
CeClª© 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
£;¤¥
53137.0
49.201
type §¦?¨
93THDA
¡
7¢
298.15
370.711
–722995.0
–33.361
–713048.0
SGTE
£¤¥¡
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
CeIÍÎ Cerium Iodide Ï
Ð 93THDAÑ
Ò
ÓÔ
ÕÖ7×2Ô
ÕÖÓÔ
ÕÖØÔ
298.15 1033.00
214.639
–649774.9
–29.024
–641122.0
CeIÍªÞ g ßÎ Cerium 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 ìà 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
þÿý
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
LMN
–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
LMN
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
Li 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
# -
298.15
262.681
12330.2
–569024.0
17.076
–574115.0
SO ClF g
) Sulphur Chloride Fluoride Dioxide gas
# -
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
85JANAF
85JANAF
SGTE
324
Thermodynamic Properties of Inorganic Materials: Pure Substances
ClO F g Chlorine Fluoride Trioxide gas
¡ ¢# £ ¤ ¡ - ¥
¦ § ¡
¦§
¦ §<¨
298.15
278.986
13296.8
–21422.1
–241.669
50631.4
PClF g Phosphorus Monochloride Monofluoride gas
¡ ¢# £ ¤ ¡ ¥ -
¦ § ¡
¦ §
¦ §¨
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
85JANAF
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 âã 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 õö 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
ÿþ 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}
298.15 513.15
184.180
25237.9
-
–295767.0
~ 85JANAF
#
–694.819
H
9623.2
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
-
217568.0
st
#
–88606.7
HfCl g ({ Hafnium Monochloride gas }
sp art
qq
18.753
type vw
~ 93THDA
#
102.074
H
187134.0
SGTE
336
Thermodynamic Properties of Inorganic Materials: Pure Substances
HgCl Mercury Monochloride gas
298.15
96.265
11738.2
-
85JANAF
–132463.3
#
–100.581
–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
-
78450.0
85JANAF
–100.581
H
–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
NO
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 tu 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
-
X
298.15 1073.80
72.115
10611.0
–411120.0
–90.725
–384070.0
NaCl g
Sodium Chloride gas
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
28158.0
26.223
85JANAF type
94TCRAS
SGTE
348
Thermodynamic Properties of Inorganic Materials: Pure Substances
NaClO Sodium Perchlorate
¡ ¢£
¡ ¢
¡ ¢¤
298.15 581.00
142.256
–382752.3
–430.878
–254286.0
NbClO©ª Niobium Chloride Dioxide
¡ ¢£
¡¢
¡ ¢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
93THDA
¡ ¥¦§+£
¡ ¥¦§
type
13974.6
24.053
¨
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
ÄÅ
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
ÓÔ
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
Þß
à áâß
àáÞß
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
ïð
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
-
298.15
237.837
9884.0
142363.0
107.487
110316.0
SnCl | g }j~ Tin Monochloride gas
-
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 ' Strontium Monochloride gas
-
298.15
252.467
9800.0
–127867.0
85.233
–153279.0
TCl g ' Tritium Chloride gas
-
#
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 g ' Tantalum Monochloride gas ¡
¤
¥¦
§¨© ¦
§¨ ¥¦
§¨ª¦
298.15
259.266
359824.0
106.255
328144.0
TiCl g ' 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
-
f
298.15
335.428
19047.0
–232.930
–1052550.0
–1122003.0
FeClz~ Iron Dichloride
-
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
42830.0
45.084
96TCRAS type
!#
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
FeCl g W Iron Dichloride gas
¡ - ¢ £¤
£¤
£¤'¥
298.15
293.837
15584.0
43.478
–158779.0
–145816.0
GaCl g W Gallium Dichloride gas
¡ - ¢ £¤
£¤
£¤'¥
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
96TCRAS
94TCRAS
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
HfClËÌ 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
HgClÝÞ Mercury Chloride ß
â
ã ä
åæ'çä
åæãä
åæ'èä
298.15 550.00
144.494
–230120.0
–163.892
–183443.0
HgClÝð 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
þÿý - 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 <
=>
?> @AB
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 [
\]
`] mno
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
MoCl O Molybdenum Dichloride Oxide
298.15
125.000
18000.0
-
–530000.0
94TCRAS
–229.212
–461660.0
MoCl O g Molybdenum Dichloride Oxide gas
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
-
–310000.0
–13.568
94TCRAS H
–305955.0
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
385
MoCl OW Molybdenum Dichloride Dioxide
298.15 449.00
135.60
19600.0
-
¡
¢£
–724000.0
¢F£
–321.186
94TCRAS ¢£H¤
¢¥K¦K§
17000.0
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
-
¡
¢£
–633039.2
¢£
–119.007
¢F¥M¦N§
–628238.0
MoCl O"ª g « Molybdenum Dichloride Dioxide gas
sp art
¢£ ¤
37.862
type P¨R©
85JANAF
–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 ËÌÍ
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 àáâ
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 òóô
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 òóô
-
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
-
7
298.15
353.921
19501.6
–671532.0
–106.923
–639653.0
SnCl} OJ~ g L Tin Dichloride Tetraoxide gas
-
7
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
85JANAF
93THDA
Landolt-B¨ornstein New Series IV/19A
Thermodynamic Properties of Inorganic Materials: Pure Substances
PClJ g Phosphorus Dichloride gas
-
H
¡
298.15
285.122
12249.0
–54292.0
20.954
–60539.4
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
¢g£j¤
¢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
<
298.15
305.663
–112968.0
33.363
–122915.0
ThCl|2 Thorium Dichloride
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
TiCl2 Titanium Dichloride
298.15 1308.0
87.350
13300.0
-
A
94TCRAS
–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
HI
<
–465373.0
TiCl+ g m Titanium Dichloride gas
sp art
FF
26.223
type KM
94TCRAS
<
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