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Liouville theorem and related forms

2 Liouville theorem and related forms The Helmholtz-Lagrange relation given in equ. (4.46) is related to many other forms which all state certain conservation laws (the Clausius theorem, Abbe s relation, the Liouville theorem). The most important one in the present context is the Liouville theorem [Lio38] which describes the invariance of the volume in phase space. The content of this theorem will be discussed and represented finally in a slightly different form which allows a new access to the luminosity introduced in equ. (4.14). [Pg.388]

The applications of the Helmholtz-Lagrange relation given in equ. (4.46) to an arbitrary conjugate object-image pair characterized by left (/) and right (r), respectively, leads to [Pg.388]

The product y a is called the emittance, and when divided by a factor of n it is termed the normalized emittance. Equ. (10.39) states that the (normalized) emittance remains constant, provided an ideal optical system, i.e., without intensity losses, is given. [Pg.388]

In the context of conservation relations another form will be added. If equ. (10.39b) is squared, one can introduce an area A to replace y2, a solid angle 2 to replace a2 and a so-called brightness B which is proportional to (see below). This gives [Pg.389]

In optical radiometry with plane solid surfaces the product 2, at the lens input represents the luminosity Lopt  [Pg.389]




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