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MANIFOLD DERIVATIVE IN THE LAPLACE-BELTRAMI EQUATION

机译:Laplace-Beltrami方程中的流形导数

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This paper is concerned with the derivative of the solution with respect to the manifold, more precisely with the shape tangential sensitivity analysis of the solution to the Laplace-Beltrami boundary value problem with homogeneous Dirichlet boundary conditions. The domain is an open subset omega of a smooth compact manifold Gamma of R-N. The flow of a vector field V(t,.) changes omega in omega(t) (and Gamma in Gamma(t)). The relative boundary gamma(t) of omega(t) in Gamma(t) is smooth enough and gamma(omega(t)) is the solution in omega(t) of the Laplace-Dirichlet problem with zero boundary value on gamma(t). The shape tangential derivative is characterized as being the solution of a similar non homogeneous boundary value problem; that element gamma(Gamma)'(omega; V) can be simply defined by the restriction to omega of <(gamma)over dot>-V(Gamma)gamma.V where <(gamma)over dot> is the material derivative of gamma and del(Gamma)gamma is the tangential gradient of gamma. The study splits in two parts whether the relative boundary gamma of omega is empty or not. In both cases the shape derivative depends on the deviatoric part of the second fundamental form of the surface, on the field V(0) through its normal component on omega and on the tangential field V(0)(Gamma) through its normal component on the relative boundary gamma. We extend the structure results for the shape tangential derivative making use of intrinsic geometry approach and intensive use of extension operators. (C) 1997 Academic Press. [References: 18]
机译:本文关注与流形有关的解的导数,更确切地说,涉及具有齐次Dirichlet边界条件的Laplace-Beltrami边值问题的解的形状切向敏感性分析。该域是R-N的光滑紧流形Gamma的开放子集Ω。向量场V(t ,.)的流在omega(t)中改变omega(在Gamma(t)中改变gamma)。 gamma(t)中omega(t)的相对边界gamma(t)足够光滑,并且gamma(omega(t))是在gamma(t)上具有零边界值的Laplace-Dirichlet问题的omega(t)中的解)。形状切向导数的特征是类似的非齐次边值问题的解;元素γ(γ)'(ω; V)可以简单地通过对<γover over点>-Vγγ.V的ω的限制来定义,其中<γover dot>是gamma和del(Gamma)gamma是伽玛的切向梯度。这项研究分为两个部分,即ω的相对边界伽玛是否为空。在这两种情况下,形状导数均取决于表面的第二基本形式的偏斜部分,取决于通过其在ω上的法向分量的场V(0)和通过其在ω的法向分量的切线场V(0)(Gamma)。相对边界伽玛。我们利用固有几何方法和大量使用扩展算符来扩展形状切向导数的结构结果。 (C)1997学术出版社。 [参考:18]

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