Abstract
This work develops the Helmholtz potential A(ρ, T) for He4 below 0.8 K. Superfluid terms, related to temperature and momentum gradients, are neglected with negligible loss of accuracy in the derived state properties (specific heats, first sound velocity, expansivity, compressibility, etc.). Retained terms are directly related to a bulk fluid compressibility plus phonon and roton excitations in this quantum fluid. The bulk fluid compressibility is found from the empirical equation c 31 ≈ c 310 + b; P, where c1 is the velocity of first sound, P is the pressure, and c10 and b are constants; this empirical equation is found to apply also to other helium temperature ranges and to other fluids. The phonon excitations lead to a single temperature-dependent term in A(ρ ,T) up to 0.3 K, with only two more terms added up to 0.8 K. The roton potential, negligible below about 0.3 K, is a single term first derived 60 years ago but little used in more recent work. The final A(ρ ,T) is shown to fit available experimental specific heat data to about ±2% or better. The magnitude of the pressure-independent Gruneisen parameter below 0.3 K is typical of highly compressed normal liquids. Extension of the equation above 0.8 K is hampered by lack of data between 0.8 and 1.2 K
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References
J. Maynard (1976) Phys Rev B 14 3868 Occurrence Handle10.1103/PhysRevB.14.3868
M.S. Mongiovi (1993) Phys Rev B 48 6276 Occurrence Handle10.1103/PhysRevB.48.6276
L. Landau (1941) J. Phys. 5 71
L. Landau (1947) J. Phys. 11 91
R.J. Donnelly P.H. Roberts (1977) J. Low. Temp. Phys. 27 687 Occurrence Handle10.1007/BF00655704
J.S. Brooks R.J. Donnelly (1977) J. Phys. Chem. Ref. Data 6 51
McCarty R.D. (1980). NBS Tech Note 1029.
N.E. Phillips C.G. Waterfield J.K. Hoffer (1970) Phys. Rev. Letters 25 1260 Occurrence Handle10.1103/PhysRevLett.25.1260
N. E. Phillips, private communication (Univ. of California).
D.S. Greywall (1978) Phys Rev B 18 2127 Occurrence Handle10.1103/PhysRevB.18.2127
D.S. Greywall (1979) Phys Rev B 21 1329 Occurrence Handle10.1103/PhysRevB.21.1329
R.J. Donnelly C.F. Barenghi (1998) J. Phys. Chem. Ref. Data 27 1217
H. Preston Thomas (1990) Metrologia 27 3 Occurrence Handle10.1088/0026-1394/27/1/002
M. Durieux R.L. Rusby (1983) Metrologia 19 67 Occurrence Handle10.1088/0026-1394/19/2/004
Abraham B.M., Eckstein Y., Ketterson J.B., Kuchnir M., Roach P.R. Phys Rev. A1: 250 (1970); Erratum: Phys. Rev.A2:550 (1970)
H.J. Maris (1991) Phys. Rev. Lett. 66 45 Occurrence Handle10.1103/PhysRevLett.66.45 Occurrence Handle10043138
J.J. Niemela R.J. Donnelly (1995) J. Low Temp. Phys. 98 1 Occurrence Handle10.1007/BF00754064
W.M. Whitney C.E. Chase (1967) Phys Rev. 158 200 Occurrence Handle10.1103/PhysRev.158.200
V. Arp J.M. Persichetti G.B. Chen (1984) J. Fluids Eng. 106 193
A.D.B. Woods P.A. Hilton R. Scherm W.G. Stirling (1977) J. Phys. C 10 45 Occurrence Handle10.1088/0022-3719/10/3/002
V. Arp (1990) J. Low Temp. Phys. 79 1 Occurrence Handle10.1007/BF00683459
E.R. Grilly R.L. Mills (1962) Ann Phys. 18 250 Occurrence Handle10.1016/0003-4916(62)90069-6
V. Arp (to be published).
J.A. Lipa D.R. Swanson J.A. Nissen T.C.P. Chui U.E. Israelsson (1996) Phys. Rev. Lett. 76 944 Occurrence Handle10.1103/PhysRevLett.76.944 Occurrence Handle10061591
M. Strosser M. Monnigmann V. Dohm (2000) Physica B 284-288 41 Occurrence Handle10.1016/S0921-4526(99)02006-2
B.E. Gammon (1976) J. Chem. Phys. 64 2556
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Arp, V. He4 State Equation Below 0.8 K. Int J Thermophys 26, 1477–1493 (2005). https://doi.org/10.1007/s10765-005-8098-1
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DOI: https://doi.org/10.1007/s10765-005-8098-1