酷热
发表于 2025-3-26 23:51:43
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垄断
发表于 2025-3-27 04:00:54
Fabian Birkmann,Henning Urbat,Stefan Milius last part of the book is devoted to rapidly oscillating perturbations extended over the whole domain or its boundary. At first glance the problems collected here essentially differ from those studied in the preceding chapters. Nevertheless, one can follow an analogy in the iterative procedures for
INTER
发表于 2025-3-27 06:11:59
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coagulate
发表于 2025-3-27 12:53:15
Ackermannian Completion of Separatorss played by a partial differential operator acting on functions in . variables. As a model we take the problem of the propagation of heat in a fine wire-cloth. On its segments there are given some ordinary second order differential equations. At the nodes, the sum of the flows rates is equal to zero
技术
发表于 2025-3-27 16:04:07
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才能
发表于 2025-3-27 20:52:52
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共同确定为确
发表于 2025-3-28 00:18:00
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babble
发表于 2025-3-28 02:47:52
Elliptic Boundary Value Problems with Rapidly Oscillating Coefficients last part of the book is devoted to rapidly oscillating perturbations extended over the whole domain or its boundary. At first glance the problems collected here essentially differ from those studied in the preceding chapters. Nevertheless, one can follow an analogy in the iterative procedures for
outset
发表于 2025-3-28 08:59:52
Paradoxes of Limit Passage in Solutions of Boundary Value Problems When Smooth Domains Are Approximahis purpose we use an asymptotic approach. Though the techniques have a broader field of applications, we restrict ourselves to studying some particular boundary value problems in the theory of thin plates. More precisely, we consider a number of questions related to the known paradox that goes back
破裂
发表于 2025-3-28 11:46:03
Homogenization of a Differential Operator on a Fine Periodic Net of Curvess played by a partial differential operator acting on functions in . variables. As a model we take the problem of the propagation of heat in a fine wire-cloth. On its segments there are given some ordinary second order differential equations. At the nodes, the sum of the flows rates is equal to zero