On the Equation of State of an Imperfect Hard Core Gas |
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Page 12
... potential , j , to have the strength J up to the end of its range , z , and 0 outside . Then we have v ( 0 ) = Jz . The temperature scale is determined by the strength of the potential multiplied by its range since the Curie point is ...
... potential , j , to have the strength J up to the end of its range , z , and 0 outside . Then we have v ( 0 ) = Jz . The temperature scale is determined by the strength of the potential multiplied by its range since the Curie point is ...
Page 54
... potential where the numbers in parentheses denote the exponents of the attractive and repulsive parts . See for example , Hirschfelder , Curtiss and Bird , op . cit . , p162 The last coefficient was obtained by numerical integration ...
... potential where the numbers in parentheses denote the exponents of the attractive and repulsive parts . See for example , Hirschfelder , Curtiss and Bird , op . cit . , p162 The last coefficient was obtained by numerical integration ...
Page 56
... potential ( Lennard - Jones potential with hard core ) and experimental results 33 . боро KTC PV C C a3 ε KTC Experiment 3.09 1.28 .292 K - L - A 2.59 1.43 .358 Molecular 3.04 1.42 418 Field Table 4.1 Comparison of Some Dimensionless ...
... potential ( Lennard - Jones potential with hard core ) and experimental results 33 . боро KTC PV C C a3 ε KTC Experiment 3.09 1.28 .292 K - L - A 2.59 1.43 .358 Molecular 3.04 1.42 418 Field Table 4.1 Comparison of Some Dimensionless ...
Contents
ISING MODEL OF FERROMAGNETISM | 4 |
THREE DIMENSIONAL LATTICE | 21 |
WEAK ATTRACTIVE TAIL | 39 |
4 other sections not shown
Common terms and phrases
applied magnetic field attractive tail base points BRARY Brout calculation canonical ensemble cluster expansion coefficient configurations CORNE CORNELL LIBRARY CORNELL UNIVERSITY CORNELL critical temperature Curie point Curie temperature defined denote Diagrams Occuring diagrams of Figure dotted line diagram dotted lines connected Equation equivalent external dotted factor ferromagnetism Figure A.1 fluctuations Fourier transform free energy given grand ensemble grand partition function hard core gas Identical Diagrams infinite interaction internal dotted lines irreducible graphs Ising model isotherms lattice gas LIBRARY CORNELL CORNELL LIBRARY LIBRARY line vertex loops Mayer molecular field theory non-crossing obtained overcounting phase transition Phys potential pressure r₁-r real gas reducible Reducibly linked graphs renormalized result ri-rj ring graphs saddle parameter solid lines spherical model spins sum rule summation theorem Theory of Condensation tion UNIVER UNIVERSITY CORNELL UNIVERSITY unlinked vertex containing vertices W(pva