Modeling of CollisionsEditions Scientifiques et Medicales Elsevier, 1998 - 222 من الصفحات |
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الصفحة 208
... B1 , B2 . Then for all e , λ > 0 the functional Eελ has a unique minimizer ( √ne , √√pe ) in Ce which solves the associated Euler - Lagrange equations : n2 A√ne = √neV ( V + Tn logne - E1 ) , En2 A√pe = √peV ( -V + Tp log p - E1 ...
... B1 , B2 . Then for all e , λ > 0 the functional Eελ has a unique minimizer ( √ne , √√pe ) in Ce which solves the associated Euler - Lagrange equations : n2 A√ne = √neV ( V + Tn logne - E1 ) , En2 A√pe = √peV ( -V + Tp log p - E1 ...
الصفحة 210
... B1 , B2 and let λ > 0. For e≥ 0 let ( no , pa ) be the unique minimizer of EEλ in CE and let Vε be the solution of - \ 2AV¤ nε − pε − C , √2 Vε = 0. Then there exists an M * > 1 such that for all e≥ 0 , and 0 < M ≤ no , p ≤ M ...
... B1 , B2 and let λ > 0. For e≥ 0 let ( no , pa ) be the unique minimizer of EEλ in CE and let Vε be the solution of - \ 2AV¤ nε − pε − C , √2 Vε = 0. Then there exists an M * > 1 such that for all e≥ 0 , and 0 < M ≤ no , p ≤ M ...
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