Hydrogen bromide
- Formula: BrH
- Molecular weight: 80.912
- IUPAC Standard InChIKey: CPELXLSAUQHCOX-UHFFFAOYSA-N
- CAS Registry Number: 10035-10-6
- Chemical structure:
This structure is also available as a 2d Mol file or as a computed 3d SD file
The 3d structure may be viewed using Java or Javascript. - Other names: Hydrobromic acid; Anhydrous hydrobromic acid; HBr; Hydrogen bromide, anhydrous-; Acide bromhydrique; Acido bromidrico; Bromowodor; Bromwasserstoff; Broomwaterstof; UN 1048; UN 1788; Hydrogen monobromide
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- Information on this page:
- Other data available:
- Reaction thermochemistry data: reactions 1 to 50, reactions 51 to 76
- Ion clustering data
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Gas phase thermochemistry data
Go To: Top, Phase change data, Henry's Law data, Gas phase ion energetics data, IR Spectrum, Mass spectrum (electron ionization), Constants of diatomic molecules, References, Notes
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔfH°gas | -36.29 ± 0.16 | kJ/mol | Review | Cox, Wagman, et al., 1984 | CODATA Review value |
ΔfH°gas | -36.44 | kJ/mol | Review | Chase, 1998 | Data last reviewed in September, 1965 |
Quantity | Value | Units | Method | Reference | Comment |
S°gas,1 bar | 198.700 ± 0.004 | J/mol*K | Review | Cox, Wagman, et al., 1984 | CODATA Review value |
S°gas,1 bar | 198.70 | J/mol*K | Review | Chase, 1998 | Data last reviewed in September, 1965 |
Gas Phase Heat Capacity (Shomate Equation)
Cp° = A + B*t + C*t2 + D*t3 +
E/t2
H° − H°298.15= A*t + B*t2/2 +
C*t3/3 + D*t4/4 − E/t + F − H
S° = A*ln(t) + B*t + C*t2/2 + D*t3/3 −
E/(2*t2) + G
Cp = heat capacity (J/mol*K)
H° = standard enthalpy (kJ/mol)
S° = standard entropy (J/mol*K)
t = temperature (K) / 1000.
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Temperature (K) | 298. to 1100. | 1100. to 6000. |
---|---|---|
A | 31.71409 | 32.88913 |
B | -13.69992 | 2.822116 |
C | 23.35567 | -0.478035 |
D | -9.008529 | 0.032464 |
E | -0.028758 | -3.174958 |
F | -45.57464 | -52.46318 |
G | 240.0428 | 230.8597 |
H | -36.44306 | -36.44306 |
Reference | Chase, 1998 | Chase, 1998 |
Comment | Data last reviewed in September, 1965 | Data last reviewed in September, 1965 |
Phase change data
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Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data compiled as indicated in comments:
TRC - Thermodynamics Research Center, NIST Boulder Laboratories, Chris Muzny director
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
Tfus | 186.1 | K | N/A | Dreisbach, 1955 | Uncertainty assigned by TRC = 0.02 K; TRC |
Tfus | 187.2 | K | N/A | Maass and Russell, 1918 | Uncertainty assigned by TRC = 1. K; TRC |
Tfus | 187.15 | K | N/A | Beckmann and Waentig, 1910 | Uncertainty assigned by TRC = 1.5 K; TRC |
Antoine Equation Parameters
log10(P) = A − (B / (T + C))
P = vapor pressure (bar)
T = temperature (K)
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Temperature (K) | A | B | C | Reference | Comment |
---|---|---|---|---|---|
134.3 to 206.7 | 4.02419 | 695.466 | -33.542 | Stull, 1947 | Coefficents calculated by NIST from author's data. |
206.7 to 343.8 | 4.15585 | 754.969 | -25.086 | Stull, 1947 | Coefficents calculated by NIST from author's data. |
Henry's Law data
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Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data compiled by: Rolf Sander
Henry's Law constant (water solution)
kH(T) = k°H exp(d(ln(kH))/d(1/T) ((1/T) - 1/(298.15 K)))
k°H = Henry's law constant for solubility in water at 298.15 K (mol/(kg*bar))
d(ln(kH))/d(1/T) = Temperature dependence constant (K)
k°H (mol/(kg*bar)) | d(ln(kH))/d(1/T) (K) | Method | Reference | Comment |
---|---|---|---|---|
0.72 | 6100. | C | N/A | missing citation refer to missing citation and missing citation but this value cannot be found there. |
25. | 650. | Q | N/A | Only the tabulated data between T = 273. K and T = 303. K from missing citation was used to derive kH and -Δ kH/R. Above T = 303. K the tabulated data could not be parameterized by equation (reference missing) very well. The partial pressure of water vapor (needed to convert some Henry's law constants) was calculated using the formula given by missing citation. The quantities A and α from missing citation were assumed to be identical. |
1.3×10+9/KA | 10000. | T | N/A | For strong acids, the solubility is often expressed as kH = ([H+] * [A-]) / p(HA). To obtain the physical solubility of HA, the value has to be divided by the acidity constant KA. missing citation corrects erroneous data from missing citation. |
7.1×10+8/KA | 10000. | T | N/A |
Gas phase ion energetics data
Go To: Top, Gas phase thermochemistry data, Phase change data, Henry's Law data, IR Spectrum, Mass spectrum (electron ionization), Constants of diatomic molecules, References, Notes
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data evaluated as indicated in comments:
HL - Edward P. Hunter and Sharon G. Lias
L - Sharon G. Lias
Data compiled as indicated in comments:
B - John E. Bartmess
LLK - Sharon G. Lias, Rhoda D. Levin, and Sherif A. Kafafi
RDSH - Henry M. Rosenstock, Keith Draxl, Bruce W. Steiner, and John T. Herron
View reactions leading to HBr+ (ion structure unspecified)
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
IE (evaluated) | 11.68 ± 0.03 | eV | N/A | N/A | L |
Quantity | Value | Units | Method | Reference | Comment |
Proton affinity (review) | 584.2 | kJ/mol | N/A | Hunter and Lias, 1998 | HL |
Quantity | Value | Units | Method | Reference | Comment |
Gas basicity | 557.7 | kJ/mol | N/A | Hunter and Lias, 1998 | HL |
Ionization energy determinations
IE (eV) | Method | Reference | Comment |
---|---|---|---|
11.71 | PE | Kimura, Katsumata, et al., 1981 | LLK |
11.66 ± 0.02 | PI | Tiedemann, Anderson, et al., 1979 | LLK |
11.67 | EVAL | Huber and Herzberg, 1979 | LLK |
11.645 ± 0.005 | PE | Delwiche, Natalis, et al., 1973 | LLK |
11.677 ± 0.004 | DER | Haugh and Bayes, 1971 | LLK |
11.67 ± 0.01 | PE | Lempka, Passmore, et al., 1968 | RDSH |
11.71 ± 0.01 | PE | Frost, McDowell, et al., 1967 | RDSH |
11.68 ± 0.03 | PI | Watanabe, 1957 | RDSH |
De-protonation reactions
Quantity | Value | Units | Method | Reference | Comment |
---|---|---|---|---|---|
ΔrH° | 1353.69 ± 0.21 | kJ/mol | D-EA | Blondel, Cacciani, et al., 1989 | gas phase; reported: 27129.170±0.015 cm-1; B |
ΔrH° | 1353. ± 8.8 | kJ/mol | G+TS | Taft and Bordwell, 1988 | gas phase; B |
ΔrH° | 1341.4 | kJ/mol | N/A | Check, Faust, et al., 2001 | gas phase; F-; ; ΔS(acid)=19.2; ΔS(EA)=6.4; B |
Quantity | Value | Units | Method | Reference | Comment |
ΔrG° | 1331.8 ± 0.63 | kJ/mol | H-TS | Blondel, Cacciani, et al., 1989 | gas phase; reported: 27129.170±0.015 cm-1; B |
ΔrG° | 1331. ± 8.4 | kJ/mol | IMRE | Taft and Bordwell, 1988 | gas phase; B |
ΔrG° | 1319.6 | kJ/mol | N/A | Check, Faust, et al., 2001 | gas phase; F-; ; ΔS(acid)=19.2; ΔS(EA)=6.4; B |
IR Spectrum
Go To: Top, Gas phase thermochemistry data, Phase change data, Henry's Law data, Gas phase ion energetics data, Mass spectrum (electron ionization), Constants of diatomic molecules, References, Notes
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data compiled by: Coblentz Society, Inc.
Gas Phase Spectrum
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Notice: Except where noted, spectra from this collection were measured on dispersive instruments, often in carefully selected solvents, and hence may differ in detail from measurements on FTIR instruments or in other chemical environments. More information on the manner in which spectra in this collection were collected can be found here.
Notice: Concentration information is not available for this spectrum and, therefore, molar absorptivity values cannot be derived.
Additional Data
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Owner | COBLENTZ SOCIETY Collection (C) 2018 copyright by the U.S. Secretary of Commerce on behalf of the United States of America. All rights reserved. |
---|---|
Origin | DOW CHEMICAL COMPANY |
Source reference | COBLENTZ NO. 8757 |
Date | 1964 |
State | GAS (600 mmHg DILUTED TO A TOTAL PRESSURE OF 600 mmHg WITH N2) |
Instrument | DOW KBr FOREPRISM |
Instrument parameters | GRATING CHANGED AT 5.0, 7.5, 15.0 MICRON |
Path length | 5 CM |
Resolution | 4 |
Sampling procedure | TRANSMISSION |
Data processing | DIGITIZED BY NIST FROM HARD COPY (FROM TWO SEGMENTS) |
Mass spectrum (electron ionization)
Go To: Top, Gas phase thermochemistry data, Phase change data, Henry's Law data, Gas phase ion energetics data, IR Spectrum, Constants of diatomic molecules, References, Notes
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data compiled by: NIST Mass Spectrometry Data Center, William E. Wallace, director
Spectrum
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Additional Data
View image of digitized spectrum (can be printed in landscape orientation).
Due to licensing restrictions, this spectrum cannot be downloaded.
Owner | NIST Mass Spectrometry Data Center Collection (C) 2014 copyright by the U.S. Secretary of Commerce on behalf of the United States of America. All rights reserved. |
---|---|
Origin | Chemical Concepts |
NIST MS number | 157480 |
Constants of diatomic molecules
Go To: Top, Gas phase thermochemistry data, Phase change data, Henry's Law data, Gas phase ion energetics data, IR Spectrum, Mass spectrum (electron ionization), References, Notes
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data compiled by: Klaus P. Huber and Gerhard H. Herzberg
Data collected through December, 1976
Symbol | Meaning |
---|---|
State | electronic state and / or symmetry symbol |
Te | minimum electronic energy (cm-1) |
ωe | vibrational constant – first term (cm-1) |
ωexe | vibrational constant – second term (cm-1) |
ωeye | vibrational constant – third term (cm-1) |
Be | rotational constant in equilibrium position (cm-1) |
αe | rotational constant – first term (cm-1) |
γe | rotation-vibration interaction constant (cm-1) |
De | centrifugal distortion constant (cm-1) |
βe | rotational constant – first term, centrifugal force (cm-1) |
re | internuclear distance (Å) |
Trans. | observed transition(s) corresponding to electronic state |
ν00 | position of 0-0 band (units noted in table) |
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
---|---|---|---|---|---|---|---|---|---|---|---|---|
Numerous absorption bands above 11400 cm-1, tentatively assigned to higher members of two Rydberg series starting with L and M and converging to A 2Σ+ of Hbr+; I.P.[A 2Σ+, v=0]=123373 cm-1 (15.2964 eV). | ||||||||||||
M (1Σ+) | (109473) | [1308] 1 | M ← X | 108814 | ||||||||
↳missing citation | ||||||||||||
L (1Σ+, 1Π) | (104201) | [1262] 2 | L ← X | 103519 | ||||||||
↳missing citation | ||||||||||||
3 | ||||||||||||
↳Barrow and Stamper, 1961; Stamper, 1962 | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
K 6 1 | (83902) | (2518) 4 | [8.195] | [22.0E-4] | [1.4375] | K ← X R | 83847.9 5 Z | |||||
↳Stamper, 1962 | ||||||||||||
J 6 1 | (81243) | (2502) 4 | [8.027] 7 | [3.61E-4] | [1.453] | J ← X R | 81180.7 8 Z | |||||
↳missing citation | ||||||||||||
I 6 1 | 80436 | (2525) 4 | [8.169] 9 | [10.4E-4] | [1.440] | I ← X R | 80385.6 10 Z | |||||
↳missing citation | ||||||||||||
g (3Σ-)0+ | (79253.2) 11 | [7.63] 12 | -17E-4 | [1.49] | g ← X R | 77940.0 Z | ||||||
↳missing citation; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
F 1Δ | (78322.3) 11 | [8.20] | [1.437] | F ← X R | 77009.1 Z | |||||||
↳missing citation | ||||||||||||
f1 3Δ1 | (76814) 11 | [2299.7] Z | 8.027 | 0.213 | 1.453 | f1 ← X R | 76650.9 Z | |||||
↳Barrow and Stamper, 1961; missing citation | ||||||||||||
D 1Π | (76310) 13 | [2405.5] Z | 8.125 | 0.21 | 1.444 | D ← X R | 76199.4 Z | |||||
↳missing citation; missing citation | ||||||||||||
d0 3Π0 | (76193) | [2418.5] Z | [7.624] 14 | (0.32) | [1.4904] | d0 ← X R | 76088.8 Z | |||||
↳Barrow and Stamper, 1961; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
E (3Σ+)0+ | (76691) 11 | [7.34] 15 | [1.519] | E ← X R | 75378 | |||||||
↳Ginter and Tilford, 1971 | ||||||||||||
V 1Σ+ | (75800) 16 | (790) 17 | V ↔ X 18 R | (74900) | ||||||||
↳Stamper and Barrow, 1961; missing citation | ||||||||||||
f2 3Δ2 | [75533.8] 11 | [8.675] 19 | [16.5E-4] 19 | [1.397] 5 | f2 ← X R | 74220.6 Z | ||||||
↳Barrow and Stamper, 1961; missing citation | ||||||||||||
f3 3Δ3 | [75403.1] 11 20 | [7.41] | [-7.6E-4] | [1.512] 5 | f3 ← X R | 74089.9 Z | ||||||
↳missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
e 3Σ+ | [75053] 11 21 | e ← X R | 73740 | |||||||||
↳Ginter and Tilford, 1971 | ||||||||||||
d1 3Π1 | [74855] 13 22 | d1 ← X R | 73542 | |||||||||
↳Barrow and Stamper, 1961; Ginter and Tilford, 1971 | ||||||||||||
d2 3Π2 | [74753] 13 22 | d2 ← X R | 73440 | |||||||||
↳Barrow and Stamper, 1961; Ginter and Tilford, 1971 | ||||||||||||
C 1Π | 70578 23 | 2552 Z | 52 | 7.89 | 0.30 | 1.465 | C ← X 24 R | 70527.6 Z | ||||
↳Barrow and Stamper, 1961; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
b0 3Π0 0+ | (68998) 23 | [2452] | [7.996] 25 | [1.455] | b0 ← X R | 68911.2 Z | ||||||
↳Barrow and Stamper, 1961; missing citation | ||||||||||||
b0 3Π0 0- | b0 ← X R | 68904 26 H | ||||||||||
↳Barrow and Stamper, 1961; missing citation | ||||||||||||
b1 3Π1 | (67180) 23 | [2444.2] Z | 8.148 25 | 0.292 | 1.442 | b1 ← X R | 67088.4 Z | |||||
↳missing citation; missing citation | ||||||||||||
b2 3Π2 | [67663.0] 23 | [7.805] 25 | [1.473] | b2 ← X R | 66349.8 Z | |||||||
↳Barrow and Stamper, 1961; missing citation | ||||||||||||
State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
A (1Π) 28 | 27 | A ← X | ||||||||||
↳Bates, Halford, et al., 1935; Goodeve and Taylor, 1935; Datta and Chakravarty, 1941; Romand, 1949; Huebert and Martin, 1968 | ||||||||||||
X 1Σ+ | 0 | 2648.975 29 Z | 45.2175 30 | -0.0029 | 8.464884 X | 0.23328 31 | 3.4575E-4 32 | 1.414435 33 | ||||
↳Rank, Fink, et al., 1965 | ||||||||||||
Rotation spectrum 34 35 | ||||||||||||
↳Hansler and Oetjen, 1953; Jones and Gordy, 1964; Van Dijk and Dymanus, 1969 | ||||||||||||
Raman sp. 36 | ||||||||||||
↳Cherlow, Hyatt, et al., 1975 | ||||||||||||
Mol. beam el. reson. 37 | ||||||||||||
↳Dabbousi, Meerts, et al., 1973 |
Notes
1 | v=0...4 observed. Assigned as 4pσ4pπ4 6sσ. 40 |
2 | v=0...3 observed. Assigned as 4pσ4pπ4 5pσ and/or 5pπ. 40 |
3 | Further absorption bands of doubtful assignment between 75200 and 83600 cm-1. |
4 | From the observed HBr-DBr isotope shift assuming that the observed bands are 0-0 bands. |
5 | Band [37] of Stamper, 1962. |
6 | I, J, K correspond to absorption bands with clear analogues in DBr. |
7 | Ω-type doubling, Δνef = +0.142J(J+1)- ...; B and D represent average values. |
8 | Band [28] of Barrow and Stamper, 1961. Sharp P, Q, R branches; the Q levels appear to be predissociated for J«gte»14. |
9 | missing note |
10 | Band [26] of Barrow and Stamper, 1961. |
11 | Configuration ... σ2π3 5pπ. |
12 | Perturbed at high J. |
13 | Configuration ... σ2π3 5pσ. |
14 | Slightly diffuse lines. |
15 | Perturbed. |
16 | Derived from H+ + Br-; configuration ... σπ4σ*. |
17 | Bands in emission above 46500 cm-1, in absorption above 75700. Incomplete analysis. |
18 | Heavily perturbed extensive band system. Absorption lines above 75923 cm-1 are diffuse. B' varies irregularly between 3.4 and 4.5 cm-1. |
19 | Average values for the two Ω-type doubling components. |
20 | Weak transition. |
21 | Very diffuse, unresolved band. |
22 | Diffuse band, rotational structure unresolved. |
23 | Configuration ... σ2π3 5sσ. |
24 | Very strong absorption, lines are diffuse. |
25 | Diffuse rotational structure. |
26 | Diffuse Q head. |
27 | Continous absorption statring at ~35000 with maximum at 56400 cm-1. |
28 | Configuration ... σ2π3 σ*. |
29 | These are Y10 and Y01 values; applying Dunham corrections Rank, Fink, et al., 1965 obtain we = 2649.215, Be = 8.465065. Additional corrections (adiabatic, non-adiabatic) are discussed by Bunker, 1972. The microwave B0 values of Jones and Gordy, 1964 was included in the evaluation of Be. See also 42 37 |
30 | missing note |
31 | +0.0008735(v+1/2)2 - 0.000120(v+1/2)3. |
32 | -0.0397E-4(v+1/2) + 0.0038(v+1/2)2; Hv = 7.63E-9 - 0.55E-9(v+1/2). |
33 | Rot.-vibr. Sp. 42 35 |
34 | Absolute intensities have been measured by Chamberlain and Gebbie, 1965. |
35 | For observations and measurements of pressure-induced bands and pure rotation lines (ΔJ=2) see Atwood, Vu, et al., 1967, Weiss and Cole, 1967. The pressure broadening of the lines has been studied by Babrov, 1964, Pourcin, Bachet, et al., 1967. |
36 | Raman cross sections in gaseous HBr. |
37 | The following constants (as well as corresponding values for H79Br) are given in Dabbousi, Meerts, et al., 1973: -μel(v=0,J=1) = 0.8265 D [in a later paper van Dijk and Dymanus, 1974 derive 0.8282 D from Stark effect of rotation spectrum]; -quadrupole and other hyperfine coupling constants; -gJ = 0.3712. These constants supersede earlier values of Schurin and Rollefson, 1957, Jones and Gordy, 1964, Tokuhiro, 1967, Van Dijk and Dymanus, 1969, van Dijk and Dymanus, 1970. |
38 | From D00(H2), D00(Br2), and ΔHf0 (HBr;from gaseous H2,Br2). |
39 | Average value from photoionization Watanabe, 1957 and photoelectron spectra Frost, McDowell, et al., 1967, Lempka, Passmore, et al., 1968; refers to X 2Π3/2 of the ion. A more recent paper Delwiche, Natalis, et al., 1972 gives 11.645 eV. |
40 | Strongly broadened by preionization; estimated lifetime against preionization 9.5E-15 s Terwilliger and Smith, 1975. |
41 | From R, P branches. Δνef = -0.04lJ(J+1). |
42 | In absorption the 1-0, 2-0, 3-0, 3-1, 4-0, 5-0, 6-0 bands have been studied Naude and Verleger, 1950, Thompson, Williams, et al., 1952, Plyler, 1960, Rank, Fink, et al., 1965, Bernage, Niay, et al., 1973; in emission 1-0, 2-1, 3-2, 4-3 Mould, Price, et al., 1960, James and Thibault, 1965. The constants in the table are from Rank, Fink, et al., 1965, those of James and Thibault, 1965, Bernage, Niay, et al., 1973 are very similar and of comparable accuracy. See also Ogilvie and Koo, 1976. Absolute intensities have been measured Babrov, 1964, Babrov, Shabott, et al., 1965, Rao and Lindquist, 1968, Gustafson and Rao, 1970 and the dipole moment function has been calculated; Urquhart, Clark, et al., 1972 give for H79Br[D, ]: μel(r) = +0.788 + 0.315(r-re) + 0.575(r-re)2; see also Jacobi, 1967, Tipping and Herman, 1970, Rao, 1971. |
References
Go To: Top, Gas phase thermochemistry data, Phase change data, Henry's Law data, Gas phase ion energetics data, IR Spectrum, Mass spectrum (electron ionization), Constants of diatomic molecules, Notes
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Cox, Wagman, et al., 1984
Cox, J.D.; Wagman, D.D.; Medvedev, V.A.,
CODATA Key Values for Thermodynamics, Hemisphere Publishing Corp., New York, 1984, 1. [all data]
Chase, 1998
Chase, M.W., Jr.,
NIST-JANAF Themochemical Tables, Fourth Edition,
J. Phys. Chem. Ref. Data, Monograph 9, 1998, 1-1951. [all data]
Dreisbach, 1955
Dreisbach, R.R.,
Physical Properties of Chemical Compounds, Advances in Chemistry Series No. 15, Am. Chem. Soc.: Washington, D. C., 1955. [all data]
Maass and Russell, 1918
Maass, O.; Russell, J.,
Unsaturation and molecular compound formation,
J. Am. Chem. Soc., 1918, 40, 1561-1573. [all data]
Beckmann and Waentig, 1910
Beckmann, E.; Waentig, P.,
Cryoscopic Measurements at Low Temperatures,
Z. Anorg. Chem., 1910, 67, 17. [all data]
Stull, 1947
Stull, Daniel R.,
Vapor Pressure of Pure Substances. Organic and Inorganic Compounds,
Ind. Eng. Chem., 1947, 39, 4, 517-540, https://doi.org/10.1021/ie50448a022
. [all data]
Hunter and Lias, 1998
Hunter, E.P.; Lias, S.G.,
Evaluated Gas Phase Basicities and Proton Affinities of Molecules: An Update,
J. Phys. Chem. Ref. Data, 1998, 27, 3, 413-656, https://doi.org/10.1063/1.556018
. [all data]
Kimura, Katsumata, et al., 1981
Kimura, K.; Katsumata, S.; Achiba, Y.; Yamazaki, T.; Iwata, S.,
Ionization energies, Ab initio assignments, and valence electronic structure for 200 molecules
in Handbook of HeI Photoelectron Spectra of Fundamental Organic Compounds, Japan Scientific Soc. Press, Tokyo, 1981. [all data]
Tiedemann, Anderson, et al., 1979
Tiedemann, P.W.; Anderson, S.L.; Ceyer, S.T.; Hirooka, T.; Ng, C.Y.; Mahan, B.H.; Lee, Y.T.,
Proton affinities of hydrogen halides determined by the molecular beam photoionization method,
J. Chem. Phys., 1979, 71, 605. [all data]
Huber and Herzberg, 1979
Huber, K.P.; Herzberg, G.,
Molecular Spectra and Molecular Structure. IV. Constants of Diatomic Molecules,, Van Nostrand Reinhold Co., 1979, ,1. [all data]
Delwiche, Natalis, et al., 1973
Delwiche, J.; Natalis, P.; Momigny, J.; Collin, J.E.,
On the photoelectron spectra of HBr DBr,
J. Electron Spectrosc. Relat. Phenom., 1973, 1, 219. [all data]
Haugh and Bayes, 1971
Haugh, M.J.; Bayes, K.D.,
Predissociation and dissociation energy of HBr+,
J. Phys. Chem., 1971, 75, 1472. [all data]
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Electrical anharmonicities of diatomic molecules,
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Notes
Go To: Top, Gas phase thermochemistry data, Phase change data, Henry's Law data, Gas phase ion energetics data, IR Spectrum, Mass spectrum (electron ionization), Constants of diatomic molecules, References
- Symbols used in this document:
IE (evaluated) Recommended ionization energy S°gas,1 bar Entropy of gas at standard conditions (1 bar) Tfus Fusion (melting) point d(ln(kH))/d(1/T) Temperature dependence parameter for Henry's Law constant k°H Henry's Law constant at 298.15K ΔfH°gas Enthalpy of formation of gas at standard conditions ΔrG° Free energy of reaction at standard conditions ΔrH° Enthalpy of reaction at standard conditions - Data from NIST Standard Reference Database 69: NIST Chemistry WebBook
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