Abstract
The specific heat at constant pressure, C p, of aluminum measured by Ditmars, Plint, and Shukla has been reduced to the volume V 0 appropriate for 0 K employing the Murnaghan equation. The C v0 thus obtained is compared with the theoretical C v0 calculated in the harmonic and the lowest-order anharmonic approximation from three different pseudopotentials (Harrison, Ashcroft, and Dagens-Rasolt-Taylor) as well as a phenomenological Morse potential. The higher-order (λ 4) anharmonic contributions are calculated from the same nearest-neighbor Morse potential as in the lowest-order anharmonic theory. The role of the vacancy and the higher-order anharmonic contributions to C v0 has been examined and we conclude that the λ 4 contributions to C v0 are much smaller than the vacancy contribution. After removal of the vacancy contribution, the reduced C v0 is found to be in excellent agreement with the Ashcroft and Harrison pseudopotentials as well as the Morse potential including the λ 2 and λ 4 contributions to C v0.
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References
R. C. Shukla and C. A. Plint, Int. J. Thermophys. 1:299 (1980).
D. A. Ditmars, C. A. Plint, and R. C. Shukla, Int. J. Thermophys. 6:499 (1985).
A. J. Leadbetter, J. Phys. C (Proc. Phys. Soc.) 1:1481 (1968).
C. R. Brooks and R. E. Bingham, J. Phys. Chem. Solids 29:1553 (1968).
Y. Takahashi, Private communication, 4 Dec. 1981.
J. C. Slater, Introduction to Chemical Physics (McGraw-Hill, New York, 1939), Chap. XIII.
W. C. Overton, J. Chem. Phys. 37:2975 (1962).
R. C. Shukla and C. A. Plint, in Proceedings of the Eighth Symposium on Thermophysical Properties of Solids and of Selected Fluids for Energy Technology, J. V. Sengers, ed. (ASME, New York, 1982), p. 77.
F. D. Murnaghan, Proc. Natl. Acad. Sci. 30:244 (1944).
R. C. Shukla and E. R. Cowley, Phys. Rev. B3:4055 (1971).
W. C. Overton, J. Chem. Phys. 37:116 (1962).
D. B. Fraser and A. C. Hollis-Hallett, Can. J. Phys. 43:193 (1965).
D. F. Gibbons, Phys. Rev. 112:136 (1958).
R. O. Simmons and R. W. Balluffi, Phys. Rev. 117:52 (1960).
G. N. Kamm and G. A. Alers, J. Appl. Phys. 35:327 (1964).
D. Gerlich and E. S. Fisher, J. Phys. Chem. Solids 30:1197 (1969).
R. E. Schmunk and C. S. Smith, J. Phys. Chem. Solids 9:100 (1959).
A. J. Leadbetter, J. Phys. C (Proc. Phys. Soc.) 1:1489 (1968).
N. E. Phillips, Phys. Rev. 114:676 (1959).
G. Grimvall, J. Phys. Chem. Solids 29:1221 (1968).
N. W. Ashcroft and J. W. Wilkins, Phys. Lett. 14:285 (1965).
R. C. Shukla and L. Wilk, Phys. Rev. B10:3660 (1974).
R. C. Shukla and R. A. MacDonald, High Temp. High Press. 12:291 (1980).
R. A. MacDonald and W. M. MacDonald, Phys. Rev. B24:1715 (1981).
W. TriftshÄuser, Phys. Rev. B12:4634 (1975).
W. A. Harrison, Pseudopotentials in the Theory of Metals (Benjamin, New York, 1966).
N. W. Ashcroft, Phys. Lett. 23:48 (1966).
L. Dagens, M. Rasolt, and R. Taylor, Phys. Rev. B11:2726 (1975).
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Shukla, R.C., Plint, C.A. & Ditmars, D.A. Aluminum. II. Derivation of C v0from C p and comparison to C v0 calculated from anharmonic models. Int J Thermophys 6, 517–532 (1985). https://doi.org/10.1007/BF00508894
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DOI: https://doi.org/10.1007/BF00508894