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Phase Volume

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Phase Volume 

the volume in phase space. For a mechanical system with N degrees of freedom, the elementary phase volume is equal to dpdq = dpldq1 . . . dpNdqN, where q1, . . .,qN are the generalized coordinates and p1, . . .,pN are the generalized momenta of the system. The phase volume of a finite phase region G is equal to the 2N-dimensional integral Gdpdq. If the system is described by Hamilton’s equations of motion, then the system’s phase volume remains constant when the system moves (Liouville’s theorem). This makes it possible to introduce normalized distribution functions in phase space.



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Therefore, many variables, such as the composition and concentration of rubber (1), (4), (5), particle size (1), (2), (6), (7), acrylonitrile content (2), (8), grafting level (2), (6), (9), rubber phase volume (2), matrix molecular weight (4), strain rate (4), temperature (1), (4), (6), etc.
1 contains more than 20,000 diagrams previously published in phase volumes produced as part of the ACerS-NIST Phase Equilibria Diagrams Program: Volumes I through XIV; Annuals 91, 92 and 93; High Tc Superconductors I & II; Zirconium & Zirconia Systems; and Electronic Ceramics.
 
 
 
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