Matlab工具用于电磁场计算,采用有限元法。_Matlab tool for electromagnetic fiel

上传者: xinkai1688 | 上传时间: 2026-02-27 22:02:13 | 文件大小: 99.23MB | 文件类型: ZIP
Matlab工具用于电磁场计算,采用有限元法。_Matlab tool for electromagnetic field calculation using the finite element method..zip Matlab工具在电磁场计算领域的应用广泛,其中采用有限元法的工具尤其引人注目。有限元法是一种强大的数值分析技术,专门用于解决工程和物理问题中的边界值问题。它通过将复杂的连续域离散化成有限个小的元素,并在这些元素上进行近似求解,从而计算出整个域的物理量分布。 Matlab作为一种高级数学计算和仿真软件,为工程师和科学家们提供了一个功能强大的平台来实现有限元分析。Matlab中包含了专门用于电磁场仿真和计算的工具箱,这些工具箱经过精心设计,可以高效地进行电磁场分析,包括但不限于静磁场、时变磁场以及电磁波传播等问题。 使用Matlab进行有限元分析时,首先需要建立数学模型,这包括定义几何形状、物理属性以及边界条件。在模型构建完成后,将连续的求解域划分成有限元素网格,这一过程称为网格划分。Matlab提供了丰富的函数和命令来实现高质量的网格划分。 接下来,根据电磁场理论和有限元法原理,将麦克斯韦方程组等电磁理论基础方程转化为适合于有限元法的矩阵方程。Matlab的计算内核将对这些矩阵方程进行求解,得到各节点上的电场、磁场或者电磁波的分布情况。 Matlab工具的电磁场计算功能不仅限于理论计算,它还可以进行电磁兼容性分析、天线设计、高频电磁场仿真、微波器件分析等多种实际工程应用。通过与Matlab强大的绘图和可视化工具结合,用户可以获得直观的电磁场分布图像,这在教学和研究中具有很高的实用价值。 为了更方便地使用Matlab进行电磁场有限元分析,一些第三方开发者和研究团队开发了专门针对Matlab平台的电磁仿真工具包。这些工具包提供了更多专门的函数和命令,甚至预设的仿真模板,使得用户可以更快捷地搭建仿真模型,进行电磁场分析和设计。 在实际使用中,用户需要熟悉Matlab编程语言以及电磁场理论,这样才能充分利用Matlab强大的仿真计算功能,解决复杂的电磁场问题。此外,对Matlab的持续学习和研究也是必要的,这将有助于用户不断提升仿真分析的效率和准确性。 Matlab工具在电磁场计算中发挥着重要作用,尤其是采用了有限元法进行求解,使得工程师和科学家能够处理各种复杂的电磁场问题,并且在实际应用中取得了显著的成效。通过Matlab平台,用户可以深入分析和优化电磁场相关的工程问题,推动技术的进步。

文件下载

资源详情

[{"title":"( 477 个子文件 99.23MB ) Matlab工具用于电磁场计算,采用有限元法。_Matlab tool for electromagnetic fiel","children":[{"title":"figure_2.eps <span style='color:#111;'> 1.04MB </span>","children":null,"spread":false},{"title":"figure_2.eps <span style='color:#111;'> 304.25KB </span>","children":null,"spread":false},{"title":"figure_5.eps <span style='color:#111;'> 179.71KB </span>","children":null,"spread":false},{"title":"figure_3.eps <span style='color:#111;'> 140.25KB </span>","children":null,"spread":false},{"title":"figure_1.eps <span style='color:#111;'> 124.80KB </span>","children":null,"spread":false},{"title":"figure_1.eps <span style='color:#111;'> 123.64KB </span>","children":null,"spread":false},{"title":"figure_3.eps <span style='color:#111;'> 96.32KB </span>","children":null,"spread":false},{"title":"figure_5.eps <span style='color:#111;'> 94.27KB </span>","children":null,"spread":false},{"title":"figure_4.eps <span style='color:#111;'> 79.45KB </span>","children":null,"spread":false},{"title":"figure_6.eps <span style='color:#111;'> 75.98KB </span>","children":null,"spread":false},{"title":"figure_4.eps <span style='color:#111;'> 45.10KB </span>","children":null,"spread":false},{"title":"figure_6.eps <span style='color:#111;'> 42.68KB </span>","children":null,"spread":false},{"title":"gmsh_win.exe <span style='color:#111;'> 57.20MB </span>","children":null,"spread":false},{"title":"capacitor_rotsym.geo <span style='color:#111;'> 1.20KB </span>","children":null,"spread":false},{"title":"capacitor_cylinder.geo <span style='color:#111;'> 1.10KB </span>","children":null,"spread":false},{"title":"spheres_over_conducting_plate.geo <span style='color:#111;'> 969B </span>","children":null,"spread":false},{"title":"electrodes_over_plate.geo <span style='color:#111;'> 920B </span>","children":null,"spread":false},{"title":"cylindrical_electrodes_over_plate.geo <span style='color:#111;'> 920B </span>","children":null,"spread":false},{"title":"cylinder_electrodes.geo <span style='color:#111;'> 917B </span>","children":null,"spread":false},{"title":"long_solenoid.geo <span style='color:#111;'> 718B </span>","children":null,"spread":false},{"title":"charged_sphere_surface_charge.geo <span style='color:#111;'> 705B </span>","children":null,"spread":false},{"title":"current_loop_quadratic.geo <span style='color:#111;'> 698B </span>","children":null,"spread":false},{"title":"charged_sphere.geo <span style='color:#111;'> 665B </span>","children":null,"spread":false},{"title":"ferromagnetic_cylinder_in_B_field.geo <span style='color:#111;'> 650B </span>","children":null,"spread":false},{"title":"Stromleiter.geo <span style='color:#111;'> 622B </span>","children":null,"spread":false},{"title":"wire_in_plane.geo <span style='color:#111;'> 620B </span>","children":null,"spread":false},{"title":"charged_cylinder.geo <span style='color:#111;'> 615B </span>","children":null,"spread":false},{"title":"current_loop.geo <span style='color:#111;'> 614B </span>","children":null,"spread":false},{"title":"metal_plates.geo <span style='color:#111;'> 497B </span>","children":null,"spread":false},{"title":"simple_capacitor.geo <span style='color:#111;'> 407B </span>","children":null,"spread":false},{"title":"capacitor.geo <span style='color:#111;'> 407B </span>","children":null,"spread":false},{"title":"cylindric_capacitor.geo <span style='color:#111;'> 371B </span>","children":null,"spread":false},{"title":".gitattributes <span style='color:#111;'> 66B </span>","children":null,"spread":false},{"title":".gitignore <span style='color:#111;'> 6B </span>","children":null,"spread":false},{"title":"gmsh_lnx <span style='color:#111;'> 69.45MB </span>","children":null,"spread":false},{"title":"arrow.m <span style='color:#111;'> 58.17KB </span>","children":null,"spread":false},{"title":"arrow.m <span style='color:#111;'> 58.17KB </span>","children":null,"spread":false},{"title":"clr.m <span style='color:#111;'> 11.18KB </span>","children":null,"spread":false},{"title":"get_elefant_B.m <span style='color:#111;'> 9.63KB </span>","children":null,"spread":false},{"title":"even_stream_data.m <span style='color:#111;'> 7.42KB </span>","children":null,"spread":false},{"title":"even_stream_data.m <span style='color:#111;'> 7.42KB </span>","children":null,"spread":false},{"title":"even_stream_taper.m <span style='color:#111;'> 5.22KB </span>","children":null,"spread":false},{"title":"even_stream_taper.m <span style='color:#111;'> 5.22KB </span>","children":null,"spread":false},{"title":"even_stream_texture.m <span style='color:#111;'> 5.13KB </span>","children":null,"spread":false},{"title":"even_stream_texture.m <span style='color:#111;'> 5.13KB </span>","children":null,"spread":false},{"title":"even_stream_arrow.m <span style='color:#111;'> 4.93KB </span>","children":null,"spread":false},{"title":"even_stream_arrow.m <span style='color:#111;'> 4.93KB </span>","children":null,"spread":false},{"title":"contourx.m <span style='color:#111;'> 4.50KB </span>","children":null,"spread":false},{"title":"contourx.m <span style='color:#111;'> 4.50KB </span>","children":null,"spread":false},{"title":"even_stream_demo.m <span style='color:#111;'> 3.78KB </span>","children":null,"spread":false},{"title":"even_stream_demo.m <span style='color:#111;'> 3.78KB </span>","children":null,"spread":false},{"title":"getElementFun.m <span style='color:#111;'> 3.73KB </span>","children":null,"spread":false},{"title":"even_stream_line.m <span style='color:#111;'> 3.33KB </span>","children":null,"spread":false},{"title":"even_stream_line.m <span style='color:#111;'> 3.33KB </span>","children":null,"spread":false},{"title":"bluewhitered.m <span style='color:#111;'> 3.06KB </span>","children":null,"spread":false},{"title":"compare_solutions.m <span style='color:#111;'> 2.90KB </span>","children":null,"spread":false},{"title":"generateFiles.m <span style='color:#111;'> 2.49KB </span>","children":null,"spread":false},{"title":"parseGmesh.m <span style='color:#111;'> 2.43KB </span>","children":null,"spread":false},{"title":"calcA.m <span style='color:#111;'> 2.18KB </span>","children":null,"spread":false},{"title":"parseRegions.m <span style='color:#111;'> 2.11KB </span>","children":null,"spread":false},{"title":"calc_exact_E.m <span style='color:#111;'> 2.02KB </span>","children":null,"spread":false},{"title":"dispMesh.m <span style='color:#111;'> 1.94KB </span>","children":null,"spread":false},{"title":"dispMesh.m <span style='color:#111;'> 1.90KB </span>","children":null,"spread":false},{"title":"dispMeshUI.m <span style='color:#111;'> 1.87KB </span>","children":null,"spread":false},{"title":"dispMeshUI.m <span style='color:#111;'> 1.87KB </span>","children":null,"spread":false},{"title":"display.m <span style='color:#111;'> 1.65KB </span>","children":null,"spread":false},{"title":"evalED.m <span style='color:#111;'> 1.57KB </span>","children":null,"spread":false},{"title":"evalBH.m <span style='color:#111;'> 1.56KB </span>","children":null,"spread":false},{"title":"integrateNeumann.m <span style='color:#111;'> 1.53KB </span>","children":null,"spread":false},{"title":"display.m <span style='color:#111;'> 1.53KB </span>","children":null,"spread":false},{"title":"integrateNeumannSecOrder.m <span style='color:#111;'> 1.45KB </span>","children":null,"spread":false},{"title":"calcJ.m <span style='color:#111;'> 1.30KB </span>","children":null,"spread":false},{"title":"evalE.m <span style='color:#111;'> 1.27KB </span>","children":null,"spread":false},{"title":"evalB.m <span style='color:#111;'> 1.27KB </span>","children":null,"spread":false},{"title":"calcElementMats.m <span style='color:#111;'> 1.23KB </span>","children":null,"spread":false},{"title":"calcTriED.m <span style='color:#111;'> 1.21KB </span>","children":null,"spread":false},{"title":"evalH.m <span style='color:#111;'> 1.19KB </span>","children":null,"spread":false},{"title":"calcTriBH.m <span style='color:#111;'> 1.18KB </span>","children":null,"spread":false},{"title":"calcW.m <span style='color:#111;'> 1.10KB </span>","children":null,"spread":false},{"title":"generateRegionsFile.m <span style='color:#111;'> 1.08KB </span>","children":null,"spread":false},{"title":"getIntegralFun.m <span style='color:#111;'> 1.08KB </span>","children":null,"spread":false},{"title":"getBFun.m <span style='color:#111;'> 1.08KB </span>","children":null,"spread":false},{"title":"calcBH.m <span style='color:#111;'> 1.07KB </span>","children":null,"spread":false},{"title":"getFuns.m <span style='color:#111;'> 1.06KB </span>","children":null,"spread":false},{"title":"getEFun.m <span style='color:#111;'> 1.06KB </span>","children":null,"spread":false},{"title":"initConfigParams.m <span style='color:#111;'> 1.05KB </span>","children":null,"spread":false},{"title":"extractLT.m <span style='color:#111;'> 1.04KB </span>","children":null,"spread":false},{"title":"evalA.m <span style='color:#111;'> 1020B </span>","children":null,"spread":false},{"title":"calcTriPointED.m <span style='color:#111;'> 1005B </span>","children":null,"spread":false},{"title":"mat2struct.m <span style='color:#111;'> 986B </span>","children":null,"spread":false},{"title":"calcED.m <span style='color:#111;'> 982B </span>","children":null,"spread":false},{"title":"calcTriPointBH.m <span style='color:#111;'> 982B </span>","children":null,"spread":false},{"title":"calcTriE.m <span style='color:#111;'> 967B </span>","children":null,"spread":false},{"title":"integrateKsecOrd.m <span style='color:#111;'> 945B </span>","children":null,"spread":false},{"title":"integrateKas.m <span style='color:#111;'> 945B </span>","children":null,"spread":false},{"title":"gaussIntData.m <span style='color:#111;'> 923B </span>","children":null,"spread":false},{"title":"integrateRsecOrd.m <span style='color:#111;'> 911B </span>","children":null,"spread":false},{"title":"neumannIntegrationFunDerivatives.m <span style='color:#111;'> 889B </span>","children":null,"spread":false},{"title":"integrateR.m <span style='color:#111;'> 889B </span>","children":null,"spread":false},{"title":"calcTriB.m <span style='color:#111;'> 857B </span>","children":null,"spread":false},{"title":"......","children":null,"spread":false},{"title":"<span style='color:steelblue;'>文件过多,未全部展示</span>","children":null,"spread":false}],"spread":true}]

评论信息

免责申明

【只为小站】的资源来自网友分享,仅供学习研究,请务必在下载后24小时内给予删除,不得用于其他任何用途,否则后果自负。基于互联网的特殊性,【只为小站】 无法对用户传输的作品、信息、内容的权属或合法性、合规性、真实性、科学性、完整权、有效性等进行实质审查;无论 【只为小站】 经营者是否已进行审查,用户均应自行承担因其传输的作品、信息、内容而可能或已经产生的侵权或权属纠纷等法律责任。
本站所有资源不代表本站的观点或立场,基于网友分享,根据中国法律《信息网络传播权保护条例》第二十二条之规定,若资源存在侵权或相关问题请联系本站客服人员,zhiweidada#qq.com,请把#换成@,本站将给予最大的支持与配合,做到及时反馈和处理。关于更多版权及免责申明参见 版权及免责申明