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1.
平行板-偏心圆柱耦合传输线的特性阻抗   总被引:1,自引:0,他引:1  
提出用保角变换边界元组合法计算平行板-偏心圆柱耦合传输线的特性阻抗。通过对三种基本偏心结构的计算,获得平行板-偏心圆柱耦合传输线的特性阻抗数据。这些数据不仅可为平行板-偏心圆柱耦合传输线的准确设计提供理论依据,而且可为同轴传输线的加工制作精度提供理论参考。  相似文献   

2.
利用数值保角变换,研究内圆外矩同轴传输线内TEM波的场结构,利用软件MATLAB、HFSS绘制其场结构图,并给出特性阻抗的计算公式.研究结论对于计算该传输线的衰减常数、了解其功率容量、考虑功率耦合及设计有关的有源器件具有一定的参考价值.  相似文献   

3.
朱柯斌  聂在平  孙向阳 《物理学报》2013,62(6):60202-060202
信号传输是随钻测井的重要组成部分, 也是随钻测井进一步发展的瓶颈.针对这个问题, 研究了由NovatekTM提出的基于钻杆内有线传输, 钻杆间电磁耦合传输的随钻信号高速传输方法.首先, 针对钻杆间的电磁耦合结构的对称性, 采用了高效的数值模式匹配法对该耦合结构进行了电磁建模; 然后, 为了优化钻杆间耦合结构的耦合性能, 利用上述的电磁建模方法对该耦合结构进行了仿真分析, 分析了该耦合结构各个参数对耦合性能的影响, 并得出了一些有意义的结论, 该结论能够指导随钻测井信号钻杆间耦合传输的优化设计.另外, 钻杆内传输线利用矩形传输线设计, 设计出了50 Ω 特性阻抗的矩形传输线, 并计算了相关损耗.最后, 通过仿真和实验验证了优化设计的钻杆间耦合传输结构具有非常好的传输性能, 并且仿真和实验结果符合良好. 关键词: 随钻信号传输 数值模式匹配 电磁耦合 矩形传输线  相似文献   

4.
通过求解拉普拉斯方程,研究斜平板传输线内TEM波的场结构并进行仿真,讨论平板倾斜角度对其传输性能的影响,并将其特性阻抗数值与平行平板传输线的情况予以比较,得到其特性阻抗随平板倾斜角度增大的结论.研究结论对定量计算实际生产中出现的工艺偏差,提高平板传输线的质量,具有一定的参考价值.  相似文献   

5.
提出了一种基于时域反射原理的平行板传输线特性阻抗仿真计算方法,利用该方法借助CST软件构建模型对平行板传输线的特性阻抗值进行了仿真计算,同时重点研究了下极板展宽结构对特性阻抗值的影响。以仿真计算结果为基础,对原有特性阻抗公式进行了修正,提出了包含下极板展宽结构在内的不对称结构的平行板传输线阻抗计算公式,该公式可作为计算有界波模拟器等电磁脉冲模拟装置特性阻抗的参考公式。  相似文献   

6.
特种截面传输线特性阻抗计算的一种方法   总被引:2,自引:0,他引:2       下载免费PDF全文
曾令儒 《物理学报》1982,31(6):709-721
本文提出用圆或椭圆图形逼近多角形边界、计及其角形外导体边界的电荷角效应影响和取截面边界尺寸上、下限几何平均值的方法,计算特种截面传输线特性阻抗,得到了矩形外导体-椭圆内导体、圆形外导体-正三角形内导体、圆形外导体-正五边形内导体、圆形外导体-正六边形内导体、椭圆外导体-矩形内导体等五种新型传输线和九种现有传输线特性阻抗的初等函数计算公式,通过计算数值与有关文献的精确值比较,证实了本文方法及其特性阻抗计算公式的准确性。 关键词:  相似文献   

7.
开关振荡器是宽带高功率电磁脉冲的重要产生方式之一,以开关激励同轴振荡器为例,采用理论计算和电磁仿真为主要手段,从传输线特性阻抗与开关振荡器储能、传输线特性阻抗与天线阻抗关系及传输线特性阻抗和开关导通阻抗关系三个方面进行了研究。研究结果表明:传输线阻抗越小,振荡器储能越高;天线阻抗与传输线阻抗比值越大,输出信号品质因数越大,频谱上能量越集中,带宽越小,能量效率随比值增大呈现先增大后减小趋势;传输线特性阻抗很小时,开关阻抗对输出振荡信号影响增大,此时随特性阻抗减小,输出信号中心频率降低,品质因数减小,频谱上能量分散,带宽较宽。  相似文献   

8.
林为干  钟祥礼 《物理学报》1963,19(4):249-258
本文提出对于传输线的特性阻抗的一个新计算方法,即利用变分法的一个定理求出特性阻抗的准确值的上限及下限,但在计算过程中不是应用变分法的常用方法来进行处理,而是利用函数变换法来进行处理。这种方法可以估计特性阻抗的准确值的上限及下限,如果上下限值差别不大,则其平均值即可取作此特性阻抗的近似值,并且准确度很高。文中对于具有圆柱形内导体的矩形线、对称全矩形线、槽形线及平板线的特性阴抗分别进行计算,并举例求出数值与已发表的文献进行比较,最后对多心电续的特性阻抗也进行近似计算。 关键词:  相似文献   

9.
目前,针对空间电磁场作用有耗介质层上传输线的电磁耦合,仍缺乏有效的数值分析方法.因此,本文提出一种高效的时域混合算法,很好地解决了有耗介质层上传输线电磁耦合建模难的问题.首先,对经典传输线方程进行改进,推导了适用于有耗介质层上多导体传输线电磁耦合分析的修正传输线方程.然后,结合时域有限差分方法和相应插值技术,求解修正传输线方程,获得多导线及其端接负载上的电压和电流响应,并实现空间电磁场辐射与多导线瞬态响应的同步计算.最后,通过相应计算实例的数值模拟,与CST软件的仿真结果进行对比,验证了时域混合算法的正确性和高效性.  相似文献   

10.
设计研制了一种低阻抗传输线向高阻抗超宽带天线馈电的馈电结构,理想情况下,该馈电方法可实现特性阻抗为50Ω的同轴传输线向特性阻抗为200Ω的超宽带天线匹配馈电。分别用TEM喇叭天线和抛物反射面天线进行了实验验证,结果表明,与同轴线直接馈电相比,采用该匹配馈电结构后,TEM喇叭天线的辐射场强提高了15%,反射面天线的辐射场强提高了27%。  相似文献   

11.
在进行感应电压叠加装置设计时, 为了使初级脉冲形成与传输系统产生的快前沿高压脉冲均匀耦合到次级传输线, 需要建立感应腔的二维电路模型对电磁波在角向传输线中的传播过程进行分析, 并基于电路计算结果优化设计角向传输线阻抗分布规律,使次级传输线中电流能够均匀分布。由于角向传输线结构复杂, 没有精确求解阻抗值的解析公式, 介绍了一种基于电报方程和瞬态电磁场仿真求解复杂结构传输线阻抗值的方法, 采用该方法对等宽度和变化宽度两种结构角向传输线阻抗值进行了评估。研究结果表明,相比于三平板传输线阻抗计算公式, 采用微带传输线阻抗计算公式对角向传输线阻抗值进行求解结果更加精确。  相似文献   

12.
1~30 MHz传输线变压器的实频设计   总被引:1,自引:0,他引:1       下载免费PDF全文
 介绍了Guanella型传输线变压器的工作原理,利用电报方程分析了其阻抗变换特性和平衡到不平衡转换特性。为在巴伦低阻端获得最佳的输入阻抗,根据测量得到的实频负载阻抗来确定传输线的特性阻抗,设计了在1~30 MHz频带内可用于450 Ω到50 Ω,600.0 Ω到66.7 Ω变换的9∶1传输线变压器巴伦。受绕组间距的限制,600.0到66.7 Ω巴伦实际的传输线特性阻抗难以达到仿真所要求的值,但巴伦输入阻抗的仿真结果与实测结果仍有较好的一致性。实际测量的结果表明,这两款变压器的工作带宽(驻波比小于1.6)大于30∶1,在1~30 MHz的频带内插入损耗小于0.3 dB。  相似文献   

13.
Broadband conventional- and dual-composite right/left-handed (C/D-CRLH) transmission line metamaterials are presented. The extended transmission line theory for these structures is developed and the fundamental C-CRLH and D-CRLH properties are described comparatively in terms of dispersion/attenuation diagrams and Bloch/characteristic impedances with subsequent transmission characteristics. A D-CRLHstructure, implemented in microstrip technology, is demonstrated experimentally for the first time and shown to have potential for unique applications. As an illustration of such applications, a novel double-band coupled-line coupler constituted of one C-CRLH and one D-CRLH transmission line is demonstrated and explained by generalized coupled-mode theory. PACS 81.05.Zx; 84.40.Az; 41.20.Jb; 84.30.-r  相似文献   

14.
An efficient hybrid field solution to the general multilayer substrates transmission line problems with full shielded and half open cross-sectional geometry is presented by using the waveguide modes coupling and decoupling procedure in the spectral domain. Modal transverse transmission lines corresponding to the LSE and LSM modes are taken into account so that the Green's elements for the edge conditions can be derived by a simple iterative method. In this paper, we analyze not only the propagation constants and characteristic impedances but also the available transmission power capacity and power distribution of most commonly used structures. Normalized eigenmode power levels characterizing the propagation features are computed.  相似文献   

15.
椭圆外导体-矩形内导体同轴线的特性阻抗   总被引:5,自引:0,他引:5       下载免费PDF全文
本文提出用图形逼近和取尺寸上、下限值的几何平均值的方法,计算椭圆外导体-矩形内导体同轴线特性阻抗。矩形截面内导体的内切共焦椭圆和外接共焦椭圆,通过保角变换,变成同心圆。矩形变成近于矩形的闭合曲线,二同心圆分别为它的最小值和最大值,取二者的几何平均值,与同轴椭圆截面外导体同时变成的同心圆,构成一个标准同轴线,得到了特性阻抗公式。并由此推导出椭圆外导体-微带内导体、圆形外导体-方形内导体、圆形外导体-矩形内导体及圆形外导体-微带内导体等各种同轴线的特性阻抗的初等函数表示式。给出了上述几种同轴线的特性阻抗准确数值。 关键词:  相似文献   

16.
This paper describes a theoretical and experimental study of surface- and helicon-wave-heated plasma sources in which standing waves are set up in the cavity between the closed end plate to a plasma vessel and a wave launcher while travelling waves propagate from the opposite side of the launcher into a region which is long compared with the attenuation distance of the waves. We model the situation as a lossy transmission line of finite length coupled at the launcher to a lossy transmission line of infinite extent. RF power applied to the launcher divides in the ratio of the input impedances of the two transmission lines. For a conducting end plate, the power delivered to the travelling waves is a maximum when the cavity length is an odd number of 1/4 wavelengths long for which its input impedance is a maximum. Similarly, for an insulated end plate, the power delivered to the travelling waves is a maximum for a cavity with a length equal to an integer number of half wavelengths for which its input impedance is again a maximum.   相似文献   

17.
Saffar S  Abdullah A 《Ultrasonics》2012,52(1):169-185
The effective ultrasonic energy radiation into the air of piezoelectric transducers requires using multilayer matching systems with accurately selected acoustic impedances and the thickness of particular layers. One major problem of ultrasonic transducers, radiating acoustic energy into air, is to find the proper acoustic impedances of one or more matching layers. This work aims at developing an original solution to the acoustic impedance mismatch between transducer and air. If the acoustic impedance defences between transducer and air be more, then finding best matching layer(s) is harder. Therefore we consider PZT (lead zirconate titanate piezo electric) transducer and air that has huge acoustic impedance deference. The vibration source energy (PZT), which is used to generate the incident wave, consumes a part of the mechanical energy and converts it to an electrical one in theoretical calculation. After calculating matching layers, we consider the energy source as layer to design a transducer. However, this part of the mechanical energy will be neglected during the mathematical work. This approximation is correct only if the transducer is open-circuit. Since the possibilities of choosing material with required acoustic impedance are limited (the counted values cannot always be realized and applied in practice) it is necessary to correct the differences between theoretical values and the possibilities of practical application of given acoustic impedances. Such a correction can be done by manipulating other parameters of matching layers (e.g. by changing their thickness). The efficiency of the energy transmission from the piezoceramic transducer through different layers with different thickness and different attenuation enabling a compensation of non-ideal real values by changing their thickness was computer analyzed (base on genetic algorithm). Firstly, three theoretical solutions were investigated. Namely, Chebyshev, Desilets and Souquet theories. However, the obtained acoustic impedances do not necessarily correspond to a nowadays available material. Consequently, the values of the acoustic impedances are switched to the nearest values in a large material database. The switched values of the acoustic impedances do not generally give efficient transmission coefficients. Therefore, we proposed, in a second step, the use of a genetic algorithm (GA) to select the best acoustic impedances for matching layers from the material database for a narrow band ultrasonic transducer that work at frequency below the 2.5 MHz by considering attenuation. However this bank is rich, the results get better. So the accuracy of the propose method increase by using a lot of materials with exact data for acoustic impedance and their attenuation, especially in high frequency. This yields highly more efficient transmission coefficient. In fact by using increasing number of layer we can increase our chance to find the best sets of materials with valuable both in acoustic impedance and low attenuation. Precisely, the transmission coefficient is almost equal to unity for the all studied cases. Finally the effect of thickness on transmission coefficient is investigated for different layers. The results showed that the transmission coefficient for air media is a function of thickness and sensitive to it even for small variation in thickness. In fact, the sensitivity increases when the differences of acoustic impedances to be high (difference between PZT and air).  相似文献   

18.
A novel 35GHz 3dB power divider using coupled transmission line is presented. Unlike conventional Wilkinson divider circuit, only the 50 transmission lines are used in the design. The impedance matching can be achieved by coupled transmission line even mode characteristic impedance. The predicated and measured performances agree well.  相似文献   

19.
Waves in periodic media, whose propagation is governed by nearest neighbour interaction, are investigated. The reflection and transmission coefficients are derived for a plane wave incident from medium 1 upon medium 2, without invoking common approximations. The derivation is valid for a class of waves including magneto- and electro-inductive waves, waves on short loaded dipoles, nanoparticles, coupled waveguides and acoustic waves in monatomic media. For this last case hitherto unknown microscopic reflection and transmission coefficients are derived and shown to reduce in the continuous limit to the well-known expressions in terms of acoustic impedances.  相似文献   

20.
水下水平阵对空中运动声源的线谱探测   总被引:2,自引:1,他引:1       下载免费PDF全文
由于空气、海水介质声阻抗差异巨大,空中声源辐射的噪声透射入水的能量损失很大,加之水中声源目标的干扰,从水下探测空中声源相对困难。海试数据分析表明,空中高速运动声源噪声透射入水后信号较弱,在频繁存在干扰的水下声场环境中,常规宽带波束形成方法难以生效.针对空中声源普遍存在线谱的特点,首先利用线谱识别、提取与跟踪以及线谱加密技术对水下水平阵接收信号进行线谱分析,再通过剔除强干扰目标的线谱,成功分离出包含空中声源的线谱信号,实现对空中运动声源的探测,最远距离达16.8 km。通过理论和实验数据分析,验证了探测结果的正确性.   相似文献   

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