Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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النتائج 1-3 من 70
الصفحة 89
Let's recall that Lorentz model ( Z → ∞ , section 8.2 ) gives αo ( ∞ ) 3π 32 = ~ 0.2945 , Bo ( ∞ ) = 70 ( 00 ) Our results for 0 < Z < 1 , which are useful for ionic transport , are new . At the Z0 limit , ao ( 0 ) = 1 ( section 8.2 ) ...
Let's recall that Lorentz model ( Z → ∞ , section 8.2 ) gives αo ( ∞ ) 3π 32 = ~ 0.2945 , Bo ( ∞ ) = 70 ( 00 ) Our results for 0 < Z < 1 , which are useful for ionic transport , are new . At the Z0 limit , ao ( 0 ) = 1 ( section 8.2 ) ...
الصفحة 121
Since Aa3 is defined up to a factor ( should we point that , if InA≈ 10 , a factor 2 imprecision on A gives only a 7 % error on the logarithm ? ) , it may be obtained in the simplest cases by qualitative arguments ; unfortunately ...
Since Aa3 is defined up to a factor ( should we point that , if InA≈ 10 , a factor 2 imprecision on A gives only a 7 % error on the logarithm ? ) , it may be obtained in the simplest cases by qualitative arguments ; unfortunately ...
الصفحة 172
It gives b 1 √ ( § - E. , w ) + Y ( E - E. , w ) w [ feqw · Vzƒeq + feqw · Vzfeq ] d \ = this component is } S1 ( § − { x , w ) + - h = 1 = { div2 / ( § - E. , w ) Y feq feq w ® wải A ( w b ▽ x [ Y ( p ( x ) , p ( x ) ) p2 ( x ) T ...
It gives b 1 √ ( § - E. , w ) + Y ( E - E. , w ) w [ feqw · Vzƒeq + feqw · Vzfeq ] d \ = this component is } S1 ( § − { x , w ) + - h = 1 = { div2 / ( § - E. , w ) Y feq feq w ® wải A ( w b ▽ x [ Y ( p ( x ) , p ( x ) ) p2 ( x ) T ...
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