Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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الصفحة 136
Fokker - Planck equation for an inverse - square force . Phys . Rev. , 107 , 1-6 , 1957 . [ 37 ] A. V. Bobylev and V. A. Chuyanov . On the numerical solution of Landau's kinetic equation . Zh . Vychisl . Mat . & Mat .
Fokker - Planck equation for an inverse - square force . Phys . Rev. , 107 , 1-6 , 1957 . [ 37 ] A. V. Bobylev and V. A. Chuyanov . On the numerical solution of Landau's kinetic equation . Zh . Vychisl . Mat . & Mat .
الصفحة 194
The following result concerns the t - evolution of the limiting solutions . ... v , t ) = n ( x , t ) 8 ( u ( x , t ) - v ) in T2 ↓ R ∞ for every σ = o ( v ) € C1 ( Rd ; R ) with ( 1 ) EL ( Rd ) if the solution of ( 18.10 ) ...
The following result concerns the t - evolution of the limiting solutions . ... v , t ) = n ( x , t ) 8 ( u ( x , t ) - v ) in T2 ↓ R ∞ for every σ = o ( v ) € C1 ( Rd ; R ) with ( 1 ) EL ( Rd ) if the solution of ( 18.10 ) ...
الصفحة 199
Additionally , if n¡ ( x ) x € L1 ( R ) we can show that the solution of this example is a renormalized solution in the sense of Theorem 18.1 . This follows from the fact that for T1 € ( -1 , 0 ) , T2 € ( 7 , 37 ) , w Є Co ( R2 × ( T1 ...
Additionally , if n¡ ( x ) x € L1 ( R ) we can show that the solution of this example is a renormalized solution in the sense of Theorem 18.1 . This follows from the fact that for T1 € ( -1 , 0 ) , T2 € ( 7 , 37 ) , w Є Co ( R2 × ( T1 ...
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