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首页> 外文期刊>Computer Modeling in Engineering & Sciences >A Direct Integral Equation Method for a Cauchy Problem for the Laplace Equation in 3-Dimensional Semi-Infinite Domains
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A Direct Integral Equation Method for a Cauchy Problem for the Laplace Equation in 3-Dimensional Semi-Infinite Domains

机译:三维半无限域中拉普拉斯方程柯西问题的直接积分方程方法

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摘要

We consider a Cauchy problem for the Laplace equation in a 3-dimensional semi-infinite domain that contains a bounded inclusion. The canonical situation is the upper half-space in IR~3 containing a bounded smooth domain. The function value of the solution is specified throughout the plane bounding the upper half-space, and the normal derivative is given only on a finite portion of this plane. The aim is to reconstruct the solution on the surface of the bounded inclusion. This is a generalisation of the situation in Chapko and Johansson (2008) to three-dimensions and with Cauchy data only partially given. We represent the solution in terms of a sum of a layer potential over the surface over the inclusion with an unknown density and a layer potential involving a Green's function and a known density (the given data on the plane). The Cauchy problem is then reduced to identifying the unknown density. To construct it, we match up the data on the finite portion of the plane, where both function values and the normal derivative are specified, and this gives rise to a integral equation of the first kind over the (bounded) surface of the inclusion having a smooth kernel. We show that this boundary integral equation is uniquely solvable for a certain class of data in the usual Sobolev and Holder type spaces. To numerically solve this equation, we employ Weinert's method [Wienert (1990)]. This involves rewriting the integral equation over the unit sphere under the assumption that the surface of the inclusion can be mapped one-to-one to the unit sphere. The density is then represented in terms of a linear combination of spherical harmonics, and this generates a linear system to solve for the coefficients in this representation. Due to the ill-posedness of the Cauchy problem, Tikhonov regularization is incorporated. Numerical results are given as well, showing that accurate reconstructions of the solution and its normal derivative can be obtained on the surface of the inclusion with small computational effort. We also investigate the case when the normal derivative is given throughout the plane and the function value is only specified at a finite portion, and compare the accuracy of the reconstructions.
机译:我们考虑包含有界夹杂物的3维半无限域中Laplace方程的Cauchy问题。典型的情况是IR〜3中的上半部空间包含有界的平滑域。解的函数值在整个上半空间的平面上指定,并且仅在该平面的有限部分上给出法线导数。目的是在有界夹杂物的表面上重建解。这是Chapko和Johansson(2008)的情况到三维的概括,仅提供了部分柯西数据。我们用包含未知密度的夹杂物表面上的层电势与涉及格林函数和已知密度(平面上给定数据)的层电势之和表示解决方案。然后将柯西问题简化为识别未知密度。为了构造它,我们在平面的有限部分上匹配数据,在该有限部分上指定了函数值和正态导数,这在包含物的(有界)表面上产生了第一类积分方程。光滑的内核。我们表明,对于通常的Sobolev和Holder类型空间中的特定类别的数据,此边界积分方程是唯一可求解的。为了用数值方法求解这个方程,我们采用了韦纳特的方法[Wienert(1990)]。这涉及在假设夹杂物的表面可以一对一映射到单位球体的假设下,在单位球体上重写积分方程。然后用球谐函数的线性组合表示密度,这将生成一个线性系统来求解该表示形式的系数。由于柯西问题的不适定性,因此合并了Tikhonov正则化。还给出了数值结果,表明可以用较少的计算量在包裹体的表面上获得溶液及其正态导数的精确重建。我们还研究了在整个平面上给出法线导数并且仅在有限部分指定函数值的情况,并比较了重建的准确性。

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