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多層基板で直交する異層線路間での妨害結合におけるモデル化と解析手法に関する研究

机译:多层基板上不同正交层线间干扰耦合的建模与分析方法研究

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摘要

In this thesis, main target has been to obtain a novel circuit model for the couplingbetween two orthogonally intersecting strip conductors in configuration of strip line and/ormicrostrip line on different layers. Such circuit models would make it easy to understandthe coupling mechanism, and then one might avoid time-consuming works to estimate inadvance the coupling of high-risk probability in various configurations in real products.First, we have proposed a circuit model for discussing the crosstalk problem betweendouble strip lines model and double microstrip lines model crossing orthogonally and verifiedthe effective of the proposed model. The proposed model is based on telegrapher’sequations for the coupling of external fields to a transmission line. Coupling betweencrossing lines are caused by the electric field in a field concept and mutual capacitance in acircuit concept. Instead of obtaining the electric field, the scalar potential for strip line andmicrostrip line is approximated by using an electric image method. Taking account of thefields caused by the lines in terms of line voltages and currents at the line end terminals,we have proposed a novel four-port circuit network model, an ABCD matrix expression, inthe frequency-domain. In three different geometries, strip lines, embedded microstrip lines,and embedded-and-surface microstrip lines, we have confirmed the proposed approachesby comparing the results of the experiment and the calculation, which were in the goodagreement.Next, a lumped circuit model has been proposed for assessing the crosstalk between twostrip lines, embedded microstrip lines, and embedded-and-surface microstrip lines whichare intersecting orthogonally. Additionally, we have proposed two determination methods for the equivalent lumped capacitance by estimating a proposed error estimate and by estimatingphysical dimension of line systems. The proposed modeling approach was comparedto experimental results with good agreement. Furthermore, the analysis time was dramaticallydecreased by using the proposed method compared with one by using a 3-dimentionalfull wave analysis. The crosstalk between orthogonally intersecting lines is dominated bythe electric field, and is represented by a mutual capacitance in a circuit concept. Themutual capacitance is distributed near the intersecting point, so it can be modeled as alumped mutual capacitance. To estimate the lumped mutual capacitance, the total distributedmutual capacitance was placed at the intersection of the two orthogonal strip linesor microstrip lines. And in these evaluation models, the optimal phase progressions of thepropagating voltage wave on the transmission line of strip line model, embedded microstripline model and embedded-and-surface microstrip line model have been clear around ±40from the intersecting point. Moreover, we verify the circuit model for geometry of consumerproducts and we have made the design curves of equivalent mutual lumped capacitances.Additionally, we have discussed circuit models in the time-domain for the interferencecoupling between orthogonally intersecting two strip lines sandwiched by two referenceplanes. The circuit model proposed here was for making an inverse Laplace transform easy.The interference coupling in the time-domain was obtained in an analytical expression. Weverified the proposed models by comparing the time-domain results of the experiment withthose of the calculation, which were in good agreements.Finally, the coupling between two transmission lines intersecting in an arbitrary directionon different layers has been studied. In this thesis, the theory is developed on the assumptionthat transmission-line parameters, such as characteristic impedance and propagationconstant, correspond to those of isolated lines. In the transmission-line model for stripsintersecting at non-right angles, there is magnetic-field coupling in addition to the electric-fieldcoupling discussed previously. The magnetic-field generated from an infinite-lengthline can be derived from the vector magnetic potential. Then, the linking magnetic flux,which is the coupling-source component, can be estimated. Thus, the mutual inductanceand capacitance distributed along the lines can be formulated. By checking the distributionprofile, a circuit in terms of equivalent lumped inductance and capacitance elements wasproposed.
机译:在本文中,主要目标是获得一种新颖的电路模型,用于在不同层上的带状线和/或微带线的配置中两个正交相交的带状导体之间的耦合。这样的电路模型可以很容易地理解耦合机制,然后可以避免耗时的工作来估计实际产品中各种配置中高风险概率的耦合提前。首先,我们提出了一种电路模型来讨论串扰。双带线模型与双微带线模型正交交叉的问题,验证了所提模型的有效性。提议的模型基于电报员的公式,用于将外部场耦合到传输线。交叉线之间的耦合是由电场概念中的电场和电路概念中的互电容引起的。带电线和微带线的标量电势不是通过获取电场来计算的,而是通过电成像法进行估算的。考虑到线路末端的线路电压和电流,由线路引起的磁场,我们提出了一种新颖的四端口电路网络模型,即频域中的ABCD矩阵表达式。在三种不同的几何形状,带状线,嵌入式微带线以及嵌入式和表面微带线中,通过比较实验结果和计算结果,我们已经确认了所提出的方法。提出了用于评估正交相交的双带线,嵌入式微带线以及嵌入式和表面微带线之间的串扰的方法。另外,我们通过估算一个拟议的误差估算和估算线路系统的物理尺寸,为等效集总电容提出了两种确定方法。所提出的建模方法与实验结果进行了比较,吻合良好。此外,与使用三维全波分析方法相比,使用该方法可以大大减少分析时间。正交相交线之间的串扰由电场控制,并且在电路概念中由互电容表示。互电容分布在相交点附近,因此可以将其建模为集总互电容。为了估算集总互电容,将总分布互电容放在两条正交带状线或微带线的交点处。在这些评估模型中,带状线模型,嵌入式微带线模型和嵌入式表面微带线模型在传输线上的相交点上,传播电压波的最佳相位变化在±40左右清晰。此外,我们验证了消费品几何形状的电路模型,并绘制了等效的相互集总电容的设计曲线。此外,我们还讨论了时域中正交相交的两条带状线(夹在两个参考平面之间)之间的干扰耦合的电路模型。这里提出的电路模型是为了使拉普拉斯逆变换变得容易。通过解析表达式获得了时域的干扰耦合。通过比较实验的时域结果和计算结果,验证了所提出的模型,两者吻合良好。最后,研究了在不同层上以任意方向相交的两条传输线之间的耦合。本文在假设传输线参数(例如特性阻抗和传播常数)与隔离线的参数相对应的前提下发展了该理论。在用于以非直角相交的条带的传输线模型中,除了前面讨论的电场耦合之外,还存在磁场耦合。从无限长线产生的磁场可以从矢量磁势中得出。然后,可以估计作为耦合源分量的链接磁通量。因此,可以制定沿线分布的互感和电容。通过检查分布曲线,提出了一种等效等效集总电感和电容元件的电路。

著录项

  • 作者

    荒木 健次; Kenji Araki;

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  • 年度 2016
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  • 原文格式 PDF
  • 正文语种 en
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