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and a vapor–liquid coexistence curve, as well as a reasonable estimate of the supercritical point can be also simulated from this approach. NPH simulation can be carried out using
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Kioupis, L. I.; Arya, G.; Maginn E. I. Pressure-enthalpy driven molecular dynamics for thermodynamic property calculation II: applications.
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is also kept as a constant. It was developed by physicist H. C. Andersen in 1980. The ensemble adds another
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of a system to which the coordinates of all particles are relative. The volume
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and inversion curve can be computed directly from a single
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560:. Using isoenthalpic-isobaric ensemble of
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572:simulation. A complete vapor-compression
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417:-ensemble, where the number of particles
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227:Grand potential / Landau free energy
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349:that maintains constant enthalpy
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391:applied. It is also called the
16:Statistical-mechanical ensemble
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332:isoenthalpic-isobaric ensemble
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1039:. You can help Knowledge by
699:Principle of maximum entropy
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1091:Statistical mechanics stubs
632:Other Statistical Ensembles
601:Journal of Chemical Physics
69:Indistinguishable particles
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723:Statistical thermodynamics
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566:Joule–Thomson coefficient
564:, it was shown that the
983:Condensed matter physics
966:Statistical field theory
549:{\displaystyle H=E+PV\,}
841:Mathematical approaches
830:Lennard-Jones potential
746:thermodynamic potential
112:Thermodynamic ensembles
64:Spin–statistics theorem
877:conformal field theory
644:Fluid Phase Equilibria
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370:and constant pressure
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1086:Statistical ensembles
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792:Ferromagnetism models
685:Statistical mechanics
603:72, 2384-2393 (1980).
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217:Helmholtz free energy
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513:{\displaystyle PV\,}
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484:becomes a dynamical
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1031:This article about
971:elementary particle
736:partition functions
646:200, 93–110 (2002).
574:refrigeration cycle
562:Lennard-Jones fluid
477:{\displaystyle V\,}
456:{\displaystyle V\,}
431:{\displaystyle N\,}
410:{\displaystyle NPH}
384:{\displaystyle P\,}
363:{\displaystyle H\,}
154:Isothermal–isobaric
57:Particle statistics
998:information theory
905:correlation length
900:Critical exponents
887:Critical phenomena
868:stochastic process
848:Boltzmann equation
741:equations of state
619:2007-06-22 at the
612:Hwee, Chiang Soo.
570:molecular dynamics
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1041:expanding it
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959:Applications
910:size scaling
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950:von Neumann
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812:percolation
275:von Neumann
84:Fermi–Dirac
1080:Categories
807:Heisenberg
588:References
334:(constant
239:Scientists
200:Potentials
930:Boltzmann
853:H-theorem
731:Ensembles
496:given by
270:Ehrenfest
250:Boltzmann
130:Canonical
940:Tsallis
617:Archived
486:variable
347:ensemble
340:pressure
336:enthalpy
265:Einstein
212:Enthalpy
177:Einstein
935:Shannon
922:Entropy
578:GROMACS
245:Maxwell
784:Models
692:Theory
582:LAMMPS
280:Tolman
166:Models
1035:is a
993:chaos
945:Rényi
802:Potts
797:Ising
556:is a
488:with
290:Fermi
285:Debye
260:Gibbs
187:Potts
182:Ising
172:Debye
1037:stub
875:and
580:and
492:and
330:The
255:Bose
151:NPT
143:NPH
135:µVT
127:NVT
119:NVE
1082::
748::
584:.
1068:e
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1043:.
767:G
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757:H
752:U
677:e
670:t
663:v
543:V
540:P
537:+
534:E
531:=
528:H
507:V
504:P
471:V
450:V
425:N
405:H
402:P
399:N
378:P
357:H
319:e
312:t
305:v
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