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Figure A2.5.25. Coexistence-curve diameters as functions of reduced temperature for Ne, N2, C2H4, and SFg. Dashed lines indicate linear fits to the data far from the critical point. Reproduced from [19] Pestak M W, Goldstein R E, Chan M H W, de Bniyn J R, Balzarini D A and Ashcroft N W 1987 Phys. Rev. B 36 599, figure 3. Copyright (1987) by the American Physical Society. Figure A2.5.25. Coexistence-curve diameters as functions of reduced temperature for Ne, N2, C2H4, and SFg. Dashed lines indicate linear fits to the data far from the critical point. Reproduced from [19] Pestak M W, Goldstein R E, Chan M H W, de Bniyn J R, Balzarini D A and Ashcroft N W 1987 Phys. Rev. B 36 599, figure 3. Copyright (1987) by the American Physical Society.
Figure A2.5.29. Peak positions of the liquid-vapour heat capacity as a fiinction of methane coverages on graphite. These points trace out the liquid-vapour coexistence curve. The frill curve is drawn for p = 0.127. Reproduced from [31] Kim H K and Chan M H W Phys. Rev. Lett. 53 171 (1984) figure 2. Copyright (1984) by the American Physical Society. Figure A2.5.29. Peak positions of the liquid-vapour heat capacity as a fiinction of methane coverages on graphite. These points trace out the liquid-vapour coexistence curve. The frill curve is drawn for p = 0.127. Reproduced from [31] Kim H K and Chan M H W Phys. Rev. Lett. 53 171 (1984) figure 2. Copyright (1984) by the American Physical Society.
Figure A3.14.12. The first experimental observation of a Turing pattern in a gel strip reactor. Solutions containing separate components of the CIMA/CDIMA reaction are flowed along each edge of the strip and a spatial pattern along the horizontal axis develops for a range of experimental conditions. (Reprinted with pennission from [38], The American Physical Society.)... Figure A3.14.12. The first experimental observation of a Turing pattern in a gel strip reactor. Solutions containing separate components of the CIMA/CDIMA reaction are flowed along each edge of the strip and a spatial pattern along the horizontal axis develops for a range of experimental conditions. (Reprinted with pennission from [38], The American Physical Society.)...
Proceedings of the biannual Conference of the American Physical Society Topical Group on Shock Compression Science, the most recent of which is ... [Pg.1967]

Binder K and Ciccotti G (ed) 1996 Monte Carlo and Molecular Dynamics of Condensed Matter Systems vol 49 (Bologna Italian Physical Society)... [Pg.2280]

Car R 1996 Molecular dynamics from first principles Monte Carlo and Moleoular Dynamios of Condensed Matter Systems vo 49 ed K Binder and G Ciccotti (Bologna Italian Physical Society) pp 601-34... [Pg.2289]

R. A. E, C. Paley and N. Wiener, Fourier Transforms in the Complex Domam, American Physical Society, New York, 1934. [Pg.176]

A. Diusdale and R. Moore, Niscometry and Its Measurement, The Institute of Physics and the Physical Society, Reinhold PubUshing Corp., New York, 1963. [Pg.208]

Jeanloz, R., and Grover, R. (1988), Birch-Murnaghan and Us-Up Equations of State, in Proceedings of the American Physical Society Topical Conference on Shock Waves in Condensed Matter, Monterey, CA, 1987 (edited by Schmidt S.C. and N.C. Holmes), Plenum, New York, pp. 69-72. [Pg.112]

Thadhani, N.N., Shock-Induced Chemical Synthesis of Intermetallic Compounds, presented at the American Physical Society Topical Conference on Shock Compression of Condensed Matter, Albuquerque, NM, August 14-17, 1989. [Pg.374]

Nabarro, F.R.N (1948) Report, Conference on the Strength of Solids (Physical Society, London) p. 75. [Pg.184]

Of course, many other professional societies have played their part in this successful reaching out between specialisms. As outlined above, the big metallurgical societies have broadened resolutely, and the American Physical Society and American Chemical Society are now much more hospitable to their members in industry than they apparently were 30 years ago. [Pg.512]

Miller, C.W., Power sourees for irradiation processing the linear accelerator. In Charlesby, A. (Ed.), Radiation Sources. The MacMillan Company, New York, 1964, pp. 197-219. Sehonberg, R.G., Radiation considerations for operation of a portable 6-MeV Electron Linear Accelerator. Proceedings 20th Midyear Topical Symposium, Health Physics Society, Reno, NV, February 8-12, 1987, p. 297. [Pg.1038]

The series of Proceedings of the American Physical Society Topical Conferences on Shock Compresion of Condensed Matter provides an especially rich collection of data by many authors. Table 1.3 gives a summary of those reference sources. [Pg.10]

Table 1.3. Proceedings, American Physical Society topical conferences on shock waves in condensed matter. Table 1.3. Proceedings, American Physical Society topical conferences on shock waves in condensed matter.
FIG. 2 Phase diagram in the M-z plane for a square lattice (MC) and for a Bethe lattice q = A). Dashed lines Exact results for the Bethe lattice for the transition lines from the gas phase to the crystal phase, from the gas to the demixed phase and from the crystal to the demixed phase full lines asymptotic expansions. Symbols for MC transition points from the gas phase to the crystal phase (circles), from the gas to the demixed phase (triangles) and from the crystal to the demixed phase (squares). (Reprinted with permission from Ref. 190, Fig. 7. 1995, American Physical Society.)... [Pg.87]

FIG. 5 Relative difference x of the lattice constants of Ne and Ne as a function of temperature. Lines are experimental values [346], symbols are PIMC results, the error bars of the lO x( ) fata values are about 0.03. (Reprinted with permission from Ref. 288, Fig. 8. 1995, American Physical Society.)... [Pg.96]

FIG. 8 PIMC results (symbols) of the imaginary-time correlations G r) versus imaginary time for densities p = 0.1,0.2,..., 0.7 from bottom to top the temperature is T = 1. The full line shows the results for Q r) according to the lowest-order virial expansion the dashed lines give the MF values of Q r) for the densities p = 0.7, 0.6, and 0.5 from top to bottom. (Reprinted with permission from Ref. 175, Fig. 1. 1996, American Physical Society.)... [Pg.104]

FIG. 13 Herringbone order parameter and total energy for N2 (X model with Steele s corrugation). Quantum simulation, full line classical simulation, dotted line quasiharmonic theory, dashed line Feynman-Hibbs simulation, triangles. The lines are linear connections of the data. (Reprinted with permission from Ref. 95, Fig. 4. 1993, American Physical Society.)... [Pg.116]

FIG. 14 Phase diagram of the quantum APR model in the Q -T plane. The solid curve shows the line of continuous phase transitions from an ordered phase at low temperatures and small rotational constants to a disordered phase according to the mean-field approximation. The symbols show the transitions found by the finite-size scaling analysis of the path integral Monte Carlo data. The dashed line connecting these data is for visual help only. (Reprinted with permission from Ref. 328, Fig. 2. 1997, American Physical Society.)... [Pg.119]

A. P. Young. In K. Binder, G. Cicotti, eds. Monte Carlo and Moleeular Dynamies of Condensed Matter Systems. Bologne Italian Physical Society, 1996, pp. 285-307. [Pg.290]

V. Degiorgio, M. Corti, eds. Physics of Amphiphiles Micelles, Vesicles and Microemulsions. Amsterdam Italian Physical Society, North-Holland, 1985. [Pg.740]

Geller, H. S., and Goldstein, D. B. (1999). Equipment Efficiency Standards Mitigating Global Climate Change at a Profit. Physics Society. 28(2). [Pg.82]

In an obituaiy talk given at the Physical Society of Berlin in 1889, Hermann Helmholtz stressed that Clausius s strict formulation of the mechanical heat theory is one of the most surprising and interesting achievements of the old and new physics, because of the absolute generality independent of the nature of the physical body and since it establishes new, unforeseen relations between different branches of physics. [Pg.238]

Allison, S. K., et al. (lO.S.S). Memorial Symposium m Honor of Enrico Fermi held on April 29, 1955 at meeting of the American Physical Society m Washington, U.C. Reviews of Modern Physics 27 249-275. [Pg.501]

J.J., as Thomson was commonly called, received the 1906 Nobel Prize in Physics in recognition of the great merits of his theoretical and experimental investigations of the conduction of electricity by gases . He was knighted in 1908, received the Order of Merit in 1912 and was successively President of the Physical Society, the Royal Society and the Institute of Physics. [Pg.1134]


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See also in sourсe #XX -- [ Pg.154 ]

See also in sourсe #XX -- [ Pg.42 , Pg.46 , Pg.62 , Pg.88 , Pg.147 , Pg.157 ]




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