beryllium chloride


Gas phase thermochemistry 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.

Quantity Value Units Method Reference Comment
Δfgas-360.24kJ/molReviewChase, 1998Data last reviewed in June, 1965
Quantity Value Units Method Reference Comment
gas,1 bar252.13J/mol*KReviewChase, 1998Data last reviewed in June, 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) 2000. - 6000.
A 58.38688
B 3.263616
C -0.865561
D 0.072876
E -0.721397
F -380.2055
G 317.7915
H -360.2424
ReferenceChase, 1998
Comment Data last reviewed in June, 1965

Condensed phase thermochemistry 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.

Quantity Value Units Method Reference Comment
Δfliquid-491.31kJ/molReviewChase, 1998Data last reviewed in June, 1965
Quantity Value Units Method Reference Comment
liquid,1 bar79.71J/mol*KReviewChase, 1998Data last reviewed in June, 1965
Quantity Value Units Method Reference Comment
Δfsolid-496.22kJ/molReviewChase, 1998β phase; Data last reviewed in June, 1965

Liquid 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) 688. - 2000.
A 121.4201
B -1.464710×10-8
C 1.015642×10-8
D -2.323154×10-9
E -5.387780×10-10
F -536.2675
G 203.0784
H -491.3146
ReferenceChase, 1998
Comment Data last reviewed in June, 1965

Solid 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. - 688.298. - 688.
A 57.52260-2.666730
B 48.35270325.9030
C -28.26600-439.9610
D 5.565141206.4320
E -0.6352580.354212
F -517.4160-499.9580
G 128.63301.985951
H -496.2220-490.9300
ReferenceChase, 1998Chase, 1998
Comment β phase; Data last reviewed in June, 1965 α phase; Data last reviewed in June, 1965

Gas phase ion energetics 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:
LLK - Sharon G. Lias, Rhoda D. Levin, and Sherif A. Kafafi
RDSH - Henry M. Rosenstock, Keith Draxl, Bruce W. Steiner, and John T. Herron

Ionization energy determinations

IE (eV) Method Reference Comment
11.15PELee and Potts, 1979LLK
12.5 ± 1.0EIFarber and Srivastava, 1974LLK
12.4 ± 0.4EIHildenbrand and Theard, 1969RDSH
12.75 ± 0.02PELee and Potts, 1979Vertical value; LLK

Appearance energy determinations

Ion AE (eV) Other Products MethodReferenceComment
Be+20.4 ± 0.4?EIHildenbrand and Theard, 1969RDSH
BeCl+14.3 ± 0.5ClEIHildenbrand and Theard, 1969RDSH

Vibrational and/or electronic energy levels

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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: Marilyn E. Jacox

State:   X


Vib. 
sym. 
 No.   Approximate 
 type of mode 
 cm-1   Med.   Method   References

Πu 2 Bend 238 s Ne IR Snelson, 1968
Σu+ 3 Asym. stretch 1122 s Ne IR Snelson, 1966
Snelson, 1968
3 Asym. stretch 1108 s Ar IR Snelson, 1966
3 Asym. stretch 1100 s Kr IR Snelson, 1966

Additional references: Jacox, 1994, page 84; Buchler, Stauffer, et al., 1964

Notes

sStrong

References

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Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.

Chase, 1998
Chase, M.W., Jr., NIST-JANAF Themochemical Tables, Fourth Edition, J. Phys. Chem. Ref. Data, Monograph 9, 1998, 1-1951. [all data]

Lee and Potts, 1979
Lee, E.P.F.; Potts, A.W., An investigation of the valence shell electronic structure of alkaline earth halides by using Ab initio S. C. F. calculations and photoelectron spectroscopy, Proc. R. Soc. London A:, 1979, 365, 395. [all data]

Farber and Srivastava, 1974
Farber, M.; Srivastava, R.D., Dissociation energies of BeF and BeCl and the heat of formation of BeClF, J. Chem. Soc. Faraday Trans. 1, 1974, 70, 1581. [all data]

Hildenbrand and Theard, 1969
Hildenbrand, D.L.; Theard, L.P., Mass spectrometric measurement of the dissociation energies of BeCi and BeCl2, J. Chem. Phys., 1969, 50, 5350. [all data]

Snelson, 1968
Snelson, A., Infrared spectra of the beryllium halides, J. Phys. Chem., 1968, 72, 1, 250, https://doi.org/10.1021/j100847a046 . [all data]

Snelson, 1966
Snelson, A., Infrared Spectra of Some Alkaline Earth Halides by the Matrix Isolation Technique, J. Phys. Chem., 1966, 70, 10, 3208, https://doi.org/10.1021/j100882a031 . [all data]

Jacox, 1994
Jacox, M.E., Vibrational and electronic energy levels of polyatomic transient molecules, American Chemical Society, Washington, DC, 1994, 464. [all data]

Buchler, Stauffer, et al., 1964
Buchler, A.; Stauffer, J.L.; Klemperer, W., None, J. Am. Chem. Soc., 1964, 86, 21, 4544, https://doi.org/10.1021/ja01075a007 . [all data]


Notes

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