微波EDA網(wǎng)-關(guān)于我們 微波EDA網(wǎng)-出版的圖書(shū)專(zhuān)著 微波EDA網(wǎng)培訓(xùn)課程列表 射頻工程師養(yǎng)成培訓(xùn)學(xué)習(xí)教程
  • 1
  • 2
  • 3
  • 4
   
您現(xiàn)在的位置: 微波EDA網(wǎng) >> CST >> CST設(shè)計(jì)實(shí)例 >> 正文

CST諧振腔體設(shè)計(jì)分析—CST2013設(shè)計(jì)實(shí)例

文章來(lái)源: CST    錄入: mweda.com   

    Eigenmode Calculation with JDM 
 

    CST MICROWAVE STUDIO offers the possibility to choose the JDM eigenmode solver.  This solver is recommended only if a small number of eigenmodes are required (5 modes or less).  Since this is a tutorial, it is convenient to reset the mesh settings to the initial values of the mesh adaptation to speed up the calculation.  Open the Mesh Properties dialog for the hexahedral mesh by selecting Home: Mesh Global Properties  : and set both Lines per wavelength and Lower mesh limit equal to 10.

    There may be old results present from the previous solver run that will be overwritten when changing the mesh.  In this case, the following warning message appears:

     Press OK to acknowledge deletion of the previous results.

     The solvers parameters are specified in the solver control dialog box that can be opened again by selecting Home: Simulation  Start Simulation . Select from the Method drop down menu the eigenmode solver JDM and reduce the number of Modes to 5.  With these settings the solver will calculate 5 modes starting from the lowest resonance frequency.

    Before starting the eigenmode solver, you may select the Specials button in order to change the desired accuracy for the eigenmodes.  In this case, the value of 1e-6 is sufficient and you can leave the box unchanged by pressing the OK button. 

    Finally, press the Start button.  A few progress bars will appear in the status bar again, keeping you informed of the current status of your calculation (e.g. matrix calculation, eigenmode analysis). After the solver has finished, the resonance frequencies of the first five modes are displayed in the main view.  

     In order to review the solver time required to achieve these results, you can display the solver log-file by selecting Results  > View Logfiles > Solver Logfile from the main menu.  Please scroll down the text to obtain the  timing information . The solver time required for the calculation is comparable to the AKS eigenmode solver. 

    Please note: In contrast to the AKS eigenmode solver, the JDM requires no guess of the highest eigenfrequency and the eigenmodes are calculated to a prescribed accuracy.  The visualization of modes, Q-factor calculation and mesh adaptation are carried out as for the AKS eigenmode solver. 

    In contrast to AKS, the JDM does not currently support TST mesh cells.  Furthermore, the AKS solver should be used if many modes have to be calculated.  The JDM eigenmode solver is able to calculate eigenmodes of lossy structures (const. complex permittivity).  However, if you require the Q-factors and the losses are small, it is advisable to calculate the eigenmodes of the loss-free structure first.  This is done by default, see the < i>Consider losses in postprocessing only check box.  Afterwards, you can compute the Q-factors by the post-processing step described previously.

上一頁(yè)  [1] [2] [3] [4] [5] [6] [7] 

  • CST微波工作室教學(xué)培訓(xùn)視頻教程

    CST中文視頻教程,資深專(zhuān)家講解,視頻操作演示,從基礎(chǔ)講起,循序漸進(jìn),并結(jié)合最新工程案例,幫您快速學(xué)習(xí)掌握CST的設(shè)計(jì)應(yīng)用...【詳細(xì)介紹

推薦課程

射頻工程師學(xué)習(xí)培訓(xùn)教程

主站蜘蛛池模板: 动漫美女羞羞漫画| 国内精品一区二区三区在线观看| 国产区在线观看视频| 下面一进一出好爽视频| 涩涩涩在线视频| 国产精品99久久精品爆乳| A毛片毛片看免费| 成人精品一区二区户外勾搭野战| 久久精品无码精品免费专区 | 久久99精品久久久久久噜噜 | 国产精品国产精品国产专区不卡| 丰满少妇被猛男猛烈进入久久| 校园春色亚洲欧美| 亚洲激情第二页| 男人天堂综合网| 制服美女视频一区| 芬兰bbw搡bbbb搡bbbb| 国产成人高清在线播放| tube欧美巨大| 成人精品一区二区电影| 久久久久无码中| 日韩欧美卡一卡二卡新区| 亚洲人成在线观看| 欧美成人黄色片| 亚洲欧美精品久久| 特级毛片全部免费播放| 免费看的黄网站| 精品无人区乱码麻豆1区2区 | 69xxxx日本| 国产精品酒店视频| 中文字幕乱理片免费完整的| 日本精a在线观看| 亚洲激情视频图片| 狠狠色综合网站久久久久久久| 国产原创中文字幕| 国产精品婷婷久青青原| 天天操天天干天天舔| 久久婷婷五月综合97色| 最新无码a∨在线观看| 亚洲一区二区三区在线播放| 欧美性生恔XXXXXDDDD|