Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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الصفحة 34
Physically , the above inequality requires that the momentum given . by the field between two collisions is small compared to the one given in a collision ; we recognize here in particular the necessary condition for neglecting runaway ...
Physically , the above inequality requires that the momentum given . by the field between two collisions is small compared to the one given in a collision ; we recognize here in particular the necessary condition for neglecting runaway ...
الصفحة 146
where the internal energy is now given by : 12 / 2 The pressure tensor P in the momentum equation ( 12.18 ) is given by : Then , we have e ( t , x ) And the energy flux is obtained as follows . It is with = 1 1 } } , \ §12 € ƒ ( t , x .
where the internal energy is now given by : 12 / 2 The pressure tensor P in the momentum equation ( 12.18 ) is given by : Then , we have e ( t , x ) And the energy flux is obtained as follows . It is with = 1 1 } } , \ §12 € ƒ ( t , x .
الصفحة 194
For given σ € Co ( Rd ) the weak formulation of ( 18.18 ) reads : T2 - √ ( 18.18a ) ( 18.18b ) D ' ( Rd × ( T1 , T2 ) ) for ... of the Vlasov equation ( 18.10 ) with the test function w ( x , t ) o ( v ) where w is given by ( 18.19 ) .
For given σ € Co ( Rd ) the weak formulation of ( 18.18 ) reads : T2 - √ ( 18.18a ) ( 18.18b ) D ' ( Rd × ( T1 , T2 ) ) for ... of the Vlasov equation ( 18.10 ) with the test function w ( x , t ) o ( v ) where w is given by ( 18.19 ) .
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