共查询到19条相似文献,搜索用时 375 毫秒
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为提高大区域森林环境电波传播特性预测的准确性,研究抛物方程(PE)法在森林环境电波传播特性预测中的应用,提出了基于抛物方程的森林模型。该模型采用PE法实现准确快速求解,考虑森林在垂直方向上的非均匀性,引入森林分层模型,将森林分为树冠、树干两个均匀有耗介质层,并根据森林区域的特性参数确定各有耗介质层的等效介电常数,相比于传统将森林等效为一个给定介电常数的均匀有耗介质层,能够更准确地描述森林对电波传播的影响。将其应用于三种常见绿叶林的电波传播特性预测中,仿真结果表明,该模型能够反映不同区域、不同植被种类的森林对电波传播的影响差异,有效预测大区域森林环境电波传播特性。 相似文献
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为提高部分森林覆盖山区电波传播特性预测的时效性,提出了一种基于宽角抛物方程(PE)的快速预测算法。采用PE通过分步傅里叶变换(SSFT)求解;在SSFT步进迭代过程中,根据传播路径上森林的等效介电常数、地形的起伏情况,动态选择PE的水平步长。通过对部分森林覆盖的不规则地形条件下的电波传播特性进行仿真,探讨了该方法的可行性和有效性。结果表明:相比于均匀大步长算法,该方法更准确;而相比于均匀小步长算法,该方法能够保证抛物方程的计算精确度,同时极大地提高计算效率。 相似文献
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风驱海浪随机起伏变化是海面环境的典型特征之一, 而较大的风浪通常会给海面无线通信带来重要的影响.传统的抛物方程(Parabolic Equationmethod, PE)模型在预测粗糙海面的电波传播时, 未能充分考虑海浪的电磁散射以及阴影效应等.针对以上不足, 文中基于三维抛物方程, 引入动力学分形方法, 对传统的抛物方程模型进行了改进研究.相比传统的Miller-Brown近似方法, 改进后的预测模型能更好地反映出海浪几何特征对电磁波传播的影响.最后以舰载雷达的有效探测范围为计算背景, 对粗糙海面的电波传播特性进行了仿真分析, 结果表明了该模型在区域级海面环境电波预测的可行性. 相似文献
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采用双向抛物方程(two-way parabolic equation,2WPE)法来预测复杂海洋环境中的电波传播特性,用双向有限差分(two-way finite-difference,2WFD)法求解2WPE,考虑了海岛等不规则地形引起的电波后向传播和大气波导的影响,并在前向和后向电波传播预测中引入一种改进的分形海面模型来模拟起伏波动的实际海面边界,且能模拟海面的大尺度浪涌特性和毛细波细微结构特性.在典型的数值算例中,我们将采用改进分形模型处理海面边界时计算得到的双向电波传播因子和采用Miller-Brown模型处理海面边界时计算得到的双向电波传播因子进行对比和分析,数值分析结果表明,在相同风速条件下,采用改进分形模型处理海面边界时计算得到的双向电波传播因子波动更剧烈,能更准确地反映出实际起伏波动海面对电磁波传播的影响. 相似文献
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G. K. Theofilogiannakos T. V. Yioultsis T. D. Xenos 《Wireless Personal Communications》2007,43(2):495-510
An efficient, full-wave computational technique to investigate the electromagnetic wave propagation within a complex building
environment, resulting from contemporary indoor communication systems, is proposed. Unlike a standard ray-tracing technique,
this new methodology is based on the parabolic wave equation (PE), appropriately modified to deal with the extremely wide-angle
propagation cases, encountered in a typical wireless system of this kind. It is also successfully applied to model the field
in the presence of walls, doors or other penetrable structures, taking into account the exact geometric configuration of the
environment under consideration. Next, the PE technique is significantly enhanced by an integral equation formulation, in
which the computed field in the interior of the walls and other obstacles is used as a secondary equivalent current source
and a corrected version of the electromagnetic field is recalculated in the whole indoor environment. This combined approach
has all the advantages of a full wave method, does not call for a highly dense mesh, and it also has moderate requirements
of computational resources. 相似文献
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A parabolic equation method (PEM)-based discrete algorithm is proposed and is used to obtain the field distribution in the evaporation duct space. This method not only improves the computing speed, but also provides the flexibility to adjust the simulation accuracy. Numerical simulation of the wave propagation in the oceanic waveguide structure is done. In addition, the initial field distribution and progressive steps are determined. The loss model in the waveguide is solved through the numerical solution. By comparing the characteristics of the radio wave propagation in the duct and in the normal atmospheric structure, we analyses the radio transmission over the horizon detection in the oceanic waveguide. 相似文献
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The two-dimensional (2-D) parabolic equation (PE) is widely used for making radiowave propagation predictions in the troposphere. The effects of transverse terrain gradients, propagation around the sides of obstacles, and scattering from large obstacles to the side of the great circle path are not modeled, leading to prediction errors in many situations. In this paper, these errors are addressed by extending the 2-D PE to three dimensions. This changes the matrix form of the PE making it difficult to solve. A novel iterative solver technique, which is highly efficient and guaranteed to converge, is presented. In order to confine the domain of computation, a three-dimensional (3-D) rectangular box is placed around the region of interest. A new second-order nonreflecting boundary condition is imposed on the surface of this box and its angular validity is established. The boundary condition is shown to keep unwanted fictitious reflections to an acceptable level in the domain of interest. The terrain boundary conditions for this 3-D PE method are developed and an original technique for incorporating them into the matrix form of the iterative solver is described. This is done using the concept of virtual field points below the ground. The prediction accuracy of the 3-D PE in comparison to the 2-D PE is tested both against indoor scaled frequency measurements and very high frequency (VHF) field trials 相似文献
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抛物方程方法的亚网格模型及其应用研究 总被引:1,自引:0,他引:1
该文在抛物方程非均匀网格技术的基础上,提出了抛物方程方法的亚网格模型,并给出了该亚网格模型的具体构建方法,以快速准确地求解大尺度复杂电磁环境中存在关键目标的电波传播问题。通过对存在强散射体的复杂电磁环境中电磁波的分布特性进行模拟,探讨了抛物方程亚网格技术的高效性。结果表明:与细网格相比,亚网格技术使得抛物方程的计算速度提升了4.57倍,网格空间数下降了86.64%,且较非均匀网格具有更高的计算精度。可见,抛物方程的亚网格模型能够极大地提升抛物方程的仿真效率。 相似文献
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为了解决遥感遥测、自动导航、电子战等领域中常常涉及到障碍物定位问题,在单向抛物方程法的逆算法的基础上提出了双向抛物方程法的逆算法。应用该逆算法对大气波导环境中的障碍物进行了探测和定位,采用插值法分析了大气波导对障碍物定位精确度的影响。仿真结果表明,通过双向抛物方程法的逆算法可以对传播路径上的障碍物进行探测和定位,而且大气折射率变化会对定位精确度产生较大影响。 相似文献
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The Fourier split-step method is a one-way marching-type algorithm to efficiently solve the parabolic equation for modeling electromagnetic propagation in troposphere. The main drawback of this method is that it characterizes only forward-propagating waves, and neglects backward-propagating waves, which become important especially in the presence of irregular surfaces. Although ground reflecting boundaries are inherently incorporated into the split-step algorithm, irregular surfaces (such as sharp edges) introduce a formidable challenge. In this paper, a recursive two-way split-step algorithm is presented to model both forward and backward propagation in the presence of multiple knife-edges. The algorithm starts marching in the forward direction until the wave reaches a knife-edge. The wave arriving at the knife-edge is partially-reflected by imposing the boundary conditions at the edge, and is propagated in the backward direction by reversing the paraxial direction in the parabolic equation. In other words, the wave is split into two components, and the components travel in their corresponding directions. The reflected wave is added to the forward-wave in each range step to obtain the total wave. The wave-splitting is performed each time a wave is incident on one of the knife-edges. This procedure is repeated until convergence is achieved inside the entire domain. 相似文献