Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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الصفحة 23
ď3UB , Properties The general properties of a binary collision term can be explicitly checked with Landau's term [ 8 ] . Particle number conservation ( 1-7 ) is obvious : the collision term ( 2-1 ) is a divergence in velocity space .
ď3UB , Properties The general properties of a binary collision term can be explicitly checked with Landau's term [ 8 ] . Particle number conservation ( 1-7 ) is obvious : the collision term ( 2-1 ) is a divergence in velocity space .
الصفحة 82
... exp ( − v ; ) ( 글루 ) , Even it is not absolutely necessary [ 47 ] , it is very useful to choose a velocity meshing such that properties ( 8-4 ) are kept after discretizing : N Σ ( ómv2Av ) ; = 1 , j = 1 N Σ ...
... exp ( − v ; ) ( 글루 ) , Even it is not absolutely necessary [ 47 ] , it is very useful to choose a velocity meshing such that properties ( 8-4 ) are kept after discretizing : N Σ ( ómv2Av ) ; = 1 , j = 1 N Σ ...
الصفحة 197
1 ( 1 << t ) , t > 1 . x Figure 1 : Characteristics of example 1 . x costui sint , ( t , x ) = ( t , x ) = -x sin tu cost . = ( harmonic oscillator ) , Example 2 : Let the potential V = V ( x ) = u1 ( x ) = u = const . , and n¡ ( x ) ...
1 ( 1 << t ) , t > 1 . x Figure 1 : Characteristics of example 1 . x costui sint , ( t , x ) = ( t , x ) = -x sin tu cost . = ( harmonic oscillator ) , Example 2 : Let the potential V = V ( x ) = u1 ( x ) = u = const . , and n¡ ( x ) ...
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