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Three-dimensional wideband electromagnetic modeling on massively parallel computers

机译:大规模并行计算机上的三维宽带电磁建模

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A method is presented for modeling the wideband, frequency domain electromagnetic (EM) response of a three-dimensional (3-D) earth to dipole sources operating at frequencies where EM diffusion dominates the response (less than 100 kHz) up into the range where propagation dominates (greater than 10 MHz). The scheme employs the modified form of the vector Helmholtz equation for the scattered electric fields to model variations in electrical conductivity, dielectric permitivity and magnetic permeability. The use of the modified form of the Helmholtz equation allows for perfectly matched layer (PML) absorbing boundary conditions to be employed through the use of complex grid stretching. Applying the finite difference operator to the modified Helmholtz equation produces a linear system of equations for which the matrix is sparse and complex symmetrical. The solution is obtained using either the biconjugate gradient (BICG) or quasi-minimum residual (QMR) methods with preconditioning; in general we employ the QMR method with Jacobi scaling preconditioning due to stability. In order to simulate larger, more realistic models than has been previously possible, the scheme has been modified to run on massively parallel (MP) computer architectures. Execution on the 1840-processor Intel Paragon has indicated a maximum model size of 280 × 260 × 200 cells with a maximum flop rate of 14.7 Gflops. Three different geologic models are simulated to demonstrate the use of the code for frequencies ranging from 100 Hz to 30 MHz and for different source types and polarizations. The simulations show that the scheme is correctly able to model the air-earth interface and the jump in the electric and magnetic fields normal to discontinuities. For frequencies greater than 10 MHz, complex grid stretching must be employed to incorporate absorbing boundaries while below this normal (real) grid stretching can be employed.
机译:提出了一种方法,用于建模三维(3-D)地球对偶极子源的宽带频域电磁(EM)响应,该偶极子源在EM扩散主导响应(小于100 kHz)的频率范围内达到传播占主导地位(大于10 MHz)。该方案将矢量Helmholtz方程的修改形式用于散射电场,以模拟电导率,介电常数和磁导率的变化。亥姆霍兹方程的修改形式的使用允许通过使用复杂的网格拉伸来采用完美匹配的层(PML)来吸收边界条件。将有限差分算子应用于修改后的亥姆霍兹方程,可生成线性方程组,其矩阵稀疏且对称。可以使用双共轭梯度(BICG)或准最小残留(QMR)方法进行预处理来获得溶液。通常,由于稳定​​性,我们采用带有Jacobi标度预处理的QMR方法。为了模拟比以前可能更大,更现实的模型,已对该方案进行了修改,使其可以在大规模并行(MP)计算机体系结构上运行。 1840处理器Intel Paragon上的执行表明最大型号为280×260×200个单元,最大翻转率为14.7 Gflops。对三种不同的地质模型进行了仿真,以演示该代码在100 Hz至30 MHz频率范围内以及不同源类型和极化情况下的使用。仿真表明,该方案能够正确地模拟空地界面以及垂直于不连续面的电场和磁场中的跃变。对于大于10 MHz的频率,必须采用复杂的网格拉伸来合并吸收边界,而低于此正常(实际)网格拉伸则可以采用。

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