Copper monofluoride


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-12.55kJ/molReviewChase, 1998Data last reviewed in December, 1977
Quantity Value Units Method Reference Comment
gas,1 bar226.49J/mol*KReviewChase, 1998Data last reviewed in December, 1977

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 1500.1500. to 6000.
A 33.7347652.10544
B 8.325868-10.16766
C -6.1035362.542886
D 1.636351-0.156636
E -0.208962-9.517137
F -23.63081-44.04957
G 263.9163274.4269
H -12.55200-12.55200
ReferenceChase, 1998Chase, 1998
Comment Data last reviewed in December, 1977 Data last reviewed in December, 1977

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
Δfsolid-280.33kJ/molReviewChase, 1998Data last reviewed in December, 1977
Quantity Value Units Method Reference Comment
solid64.82J/mol*KReviewChase, 1998Data last reviewed in December, 1977

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. to 2000.
A 46.65327
B 33.62384
C -20.88138
D 4.276090
E -0.274197
F -296.4879
G 110.5965
H -280.3284
ReferenceChase, 1998
Comment Data last reviewed in December, 1977

Constants of diatomic molecules

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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: Klaus P. Huber and Gerhard H. Herzberg

Data collected through August, 1975

Symbols used in the table of constants
SymbolMeaning
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)
Diatomic constants for 63Cu19F
StateTeωeωexeωeyeBeαeγeDeβereTrans.ν00
C 1Π 20258.47 645.07 HQ 4.19  [0.3746] 1   (0.00000051)  [1.7561] C ↔ X R 20269.62 Z
Ritschl, 1927; missing citation
B 1Σ+ 19717.5 657.0 2 3.92  0.3716 0.0032 3  (0.00000048)  1.7632 B ↔ X R 19734.66 Z
Ritschl, 1927; missing citation
A 1Π 17543.4 649.2 4 HQ 4.00  [0.3675] 5     [1.7730] A ↔ X R 17556.7 HQ
Ritschl, 1927; Woods, 1943
X 1Σ+ 0 622.65 HQ 3.95  0.3794029 0.0032298 0.0000123 0.000000563  1.744930 6  
Hoeft, Lovas, et al., 1970; Honerjager and Tischer, 1974

Notes

1Λ-type doubling Δνef = +0.0010J(J+1).
2From bandheads, taking into account head-origin separations.
3Slight modification of the analysis of the 1-1 band in Woods, 1943.
40-0 sequence only. Constants recalculated assuming that the lower state is X 1Σ+.
5From a partial rotational analysis, assuming that the lower state is X 1Σ+.
6Microwave sp. 8
7Thermochemical value (mass.spectrom.) Hildenbrand, 1968. See also Kent, McDonald, et al., 1966.
8μel(v=0) = 5.77 D. Values for eqQ(Cu) in Hoeft, Lovas, et al., 1970, magnetic constants from Zeeman effect measurements in Honerjager and Tischer, 1974.

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]

Ritschl, 1927
Ritschl, R., Uber den bau einer klasse von absorptionsspektren, Z. Phys., 1927, 42, 172. [all data]

Woods, 1943
Woods, L.H., Rotational analysis of the emission spectrum of CuF, Phys. Rev., 1943, 64, 259. [all data]

Hoeft, Lovas, et al., 1970
Hoeft, J.; Lovas, F.J.; Tiemann, E.; Torring, T., The rotational spectra and dipole moments of AgF and CuF by microwave absorption, Z. Naturforsch. A, 1970, 25, 35. [all data]

Honerjager and Tischer, 1974
Honerjager, R.; Tischer, R., Magnetische Konstanten der Molekeln CuF und GaF, Z. Naturforsch. A, 1974, 29, 1919. [all data]

Hildenbrand, 1968
Hildenbrand, D.L., Dissociation energy of copper monofluoride, J. Chem. Phys., 1968, 48, 2457. [all data]

Kent, McDonald, et al., 1966
Kent, R.A.; McDonald, J.D.; Margrave, J.L., Mass spectrometric studies at high temperatures. IX. The sublimation pressure of copper(II) fluoride, J. Phys. Chem., 1966, 70, 874. [all data]


Notes

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