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单词 Liouville's Phase Space Theorem
释义

Liouville's Phase Space Theorem

States that for a nondissipative Hamiltonian System, phase space density (the Area between phase spacecontours) is constant. This requires that, given a small time increment ,

(1)


(2)

the Jacobian be equal to one:
 
  
 (3)

Expressed in another form, the integral of the Liouville Measure,
(4)

is a constant of motion. Symplectic Maps of Hamiltonian Systems must therefore be Area preserving (and have Determinants equal to 1).

See also Liouville Measure, Phase Space


References

Chavel, I. Riemannian Geometry: A Modern Introduction. New York: Cambridge University Press, 1994.


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