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kernel of integral equation相关的网络例句

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与 kernel of integral equation 相关的网络例句 [注:此内容来源于网络,仅供参考]

Subsequently,Bihari\'s inequality is generalized to the equation with fractional integral kernel.With the help of the new inequality,we further weaken the condition on equations with special integral kernels,and obtain the corresponding results.

然后,将Bihari不等式推广至具有分式积分核的情形,利用新的不等式对具有特殊积分核的方程条件做了进一步减弱,建立了相应的存在唯一性和正则性结论。

The general Fredholm integral equation of the first kind with logarithmic kernel in 2 dimensions does not always have unique solution, especially for the unbounded problem, it depends on the asymptotic behaviour at infinity.

对二维问题,一般的带对数积分核第一类Fredholm 积分方程并不总是唯一可解的,特别是对外边值问题,解在无穷远处的形态有很大的影响。

On this base,we discuss a class of singular integral equation with Hilbert kernel having solutions with singularity of order one, the solvable conditions for general equation are given and solutions for responding characteristic eq...

在以上工作的基础之上,我们提出了一类不同于文献[13]的解具一阶奇性的Hilbert核奇异积分方程,给出了完全方程的Noether定理和特征方程的解和可解条件。

The direct method of solution for non-normal type of singular integral equation with Hubert kernel is discussed. Their solution have form of integral and the condition of solution have form of the system of equations.

给出了具有Hilbert核非正则型奇异积分方程的直接解法,对核密度函数k在附加某些条件下,得出了方程积分形式的解和方程组形式的可解条件。

It is shown that the kernel of the integral equation characters the boundary of scatterer, which is determined by solving it by virtual of regularity method, meanwhile, some numerical tests are given.

并给出了正交各向异性介质识别的数值实验。

From the Maxwell equation in EMT sensing subsystem, two kinds of 3D electromagnetic integral solutions are obtained under material field distribution and with Dyadic Green function as integral kernel.

从EMT传感子系统的Maxwell方程出发,得到了两类物场分布情况下的以并矢格林函数为积分核的三维电磁积分解。

The research achievement are acquired as follows: 1From mathematical models for inverse scattering in two dimensional homogenous media including Dirichlet, Neumann, Robin,all kinds of probable mixed boundaries and cracks, direct and inverse scattering are discussed, and ill-posed integral equation and indicator function method are formulated for the diverse of boundary identification. It is shown that the kernel of the integral equation characters the boundary of scatterer, which is determined by solving it by virtual of regularity method, meanwhile, some numerical tests are given.

本研究取得了如下研究成果: 1)在二维均匀介质逆散射各种边界识别的数学模型(包括Dirichlet,Neumann,Robin,各种可能的混合边界问题,裂纹问题)下,分别考虑了正散射问题和逆散射问题,推导了上述各种边界识别的不适定积分方程以及指示函数方法,由于积分方程的核充分表征了散射物的边界,由此说明只要利用正则化方法求解该积分方程,就可以确定散射物的边界,并给出了一些数值实验。

The Neumann boundary value prob-lem is firstly reduced into the equivalent natural boundary integral equation withthe kernel possessing 2nd-order singularity,and then the corresponding variationalproblem on the boundary is obtained.By applying Quak trigonometric wavelet basisBjsee(1.2.3as boundary elements and the method of expanding kernel functionto its Galerkin discretization,we obtain simple computational formulae of the en-tries in the stiffness matrix.

首先,我们将Neumann边值问题归化为等价的带有2阶强奇性核的自然边界积分方程,然后化为边界上相应的变分形式,以Hermite插值Quak三角小波基Bj见(1.2.3作为边界元并利用积分核函数展开法将其离散,得到了十分简单的刚度矩阵系数的计算公式,而且刚度矩阵具有十分简单的形式,它是分块循环对角阵。

The method is to add a term into the original singular kernel while it subtracts its analytical solution from the original equation. Since the singularity of Green's function can be eliminated by such a mathematical technique, shape function does not need to be supposed while solving the unknown. The calculation can be directly applied to the real shape of the object by taking the integral points distributed on the object as nodes that satisfy boundary conditions.

由於格林函数的奇异性经过数学上的技巧加以消除,因此当求解未知数时已经不需要再假设形状函数,即可直接使用物体真实的外型来做计算,也就是直接将物体上分布的积分点视为满足边界条件的节点。

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