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The quasistationary phase field equations with Neumann boundary conditions

机译:具有Neumann边界条件的准静态相场方程

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摘要

We prove that the quasistationary phase field equations partial derivative(t)(u + phi) - Delta u = f, - 2 epsilon Delta phi + 1/epsilon W'(phi) = u, where W(t) = (t(2) - 1)(2) is a double-well potential, admit a solution, when the space dimension n less than or equal to 3, and that the solutions converge for epsilon --> 0 to solutions of the Stefan problem with Gibbs-Thomson law. (C) 2000 Academic Press. [References: 25]
机译:我们证明了准静态相位场方程偏导数(t)(u + phi)-δu = f,-2 epsilonδphi + 1 / epsilon W'(phi)= u,其中W(t)=(t( 2)-1)(2)是双阱势,当空间维数n小于或等于3且该解收敛于epsilon时,接纳一个解-> 0到Gibbs的Stefan问题的解-汤姆森定律。 (C)2000学术出版社。 [参考:25]

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