Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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الصفحة 64
Collision operators ( 4-18 ) can be written as a fo 6C0 % = 3√ / Fπavas 11 3 { Ao ( 51 ) + 80 ( 1 ) } SCO ab Bo w2 aw na ( including a = b case ) , where A and Bo are " universal " operators . Ao is a differential operator and Bo is ...
Collision operators ( 4-18 ) can be written as a fo 6C0 % = 3√ / Fπavas 11 3 { Ao ( 51 ) + 80 ( 1 ) } SCO ab Bo w2 aw na ( including a = b case ) , where A and Bo are " universal " operators . Ao is a differential operator and Bo is ...
الصفحة 74
Equations ( 4-32 ) give , to first perturbation order , = mi Ti T (黒) A ( ) = Collision operators ( 4-20 ) can be written as while B ... Фт w3 w3 aw Фт д το δω ότι 489 1 a w3 aw C gives back the operator formerly defined in ( 6-3 ) .
Equations ( 4-32 ) give , to first perturbation order , = mi Ti T (黒) A ( ) = Collision operators ( 4-20 ) can be written as while B ... Фт w3 w3 aw Фт д το δω ότι 489 1 a w3 aw C gives back the operator formerly defined in ( 6-3 ) .
الصفحة 171
This means that feq is still a maxwellian ( 12.12 ) . Now , in order to write the limit let us set : The same computation , as in section 15.1 , holds true here except the effect of the collision operator . We obtain ƏtU + div F ( U ) ...
This means that feq is still a maxwellian ( 12.12 ) . Now , in order to write the limit let us set : The same computation , as in section 15.1 , holds true here except the effect of the collision operator . We obtain ƏtU + div F ( U ) ...
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