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来源：百度知道 编辑：UC知道 时间：2024/05/12 06:56:11
IV. PROPOSED MODEL OF INCIDENT FIELD COUPLING
In the previous section, it was observed that the modified Lie formula approximates a distributed lossy MTL system with a cascade of lossless MTLs and lossy lumped networks. Based on this concept, incident electromagnetic fields are first analyzed with their coupling to lossless MTL sections. The effect of line losses on the incident field coupling is then accounted by the interspersed lumped network sections. For the purpose of illustration, consider the kth MLF cell (among the cascade of m MLF cells) as shown in Fig. 2. Here, for simplicity, the scattered
voltages corresponding to this MLF cell are represented as .
Fig. 2. Basic kth MLF cell (without EMI coupling)
Next, for uniform plane wave incident fields, the field coupling to this MLF cell can be formulated as follows. For the first lossless section of this cell, the solution of telegrapher’s equations (1) can be expressed as (8) After some manipulations, above (8
In the previous section, it was observed that the modified Lie formula approximates a distributed lossy MTL system with a cascade of lossless MTLs and lossy lumped networks. Based on this concept, incident electromagnetic fields are first analyzed with their coupling to lossless MTL sections. The effect of line losses on the incident field coupling is then accounted by the interspersed lumped network sections. For the purpose of illustration, consider the kth MLF cell (among the cascade of m MLF cells) as shown in Fig. 2. Here, for simplicity, the scattered
voltages corresponding to this MLF cell are represented as .
Fig. 2. Basic kth MLF cell (without EMI coupling)
Next, for uniform plane wave incident fields, the field coupling to this MLF cell can be formulated as follows. For the first lossless section of this cell, the solution of telegrapher’s equations (1) can be expressed as (8) After some manipulations, above (8
4. 计画了附带的领域联结的模型
在早先的区段中, 一般观察公式用无损失的 MTLs 和耗损集总网络的一个小瀑布接近一个被分配的耗损 MTL 系统的被修正的谎言。 基于这一项观念,事件电磁场以对无损失的 MTL 区段的他们联结被首先分析。 线损失对附带的领域联结的效果被被散布的集总网络区段然后解释。 为了例证,考虑如图 2 所显示的 kth MLF 细胞 (在 m MLF 细胞的小瀑布之中). 这里,为单纯, 那离散的
对这一个 MLF 细胞符合的电压被表现当做。
图 2. 基本 kth MLF 细胞 (没有 EMI 联结)
下一个, 为统一的飞机波事件领域,对这一个 MLF 细胞的领域联结依下列各项可能被制定。 对于这一个细胞的第一无损失的区段，报务员的相等 (1) 的解决可能在一些处理之后被表示成 (8), 当同样地，为 kth MLF 细胞 (图 2) 的第二无损失的区段，我们有 (10) 的时候 , 上方 (8) 可能被单一化在 (9)-(10),, 而且表现
同等物来源为附带的领域联结在 kth MLF 细胞会计中埋入。 (图 3)省略细节预定空间缺乏, 它可能被看到这些同等物来源被给被 (11) 复杂的广阔在哪里那
事件电场和 P 是基于 p.u.l 的一个不变的矢量。 排成一行叁数。 被计画的方式利益是那,感应来源的所有领域可能被及时分析地制定领域和可能被如在药料方面像模拟器一样的简单延迟来源。 也, 来源需要到只有被计算为那
首先 MLF 细胞, 藉由另一个来源只是被延迟的复制品。 对计算的储蓄这一个领引当提供重要的速度- 向上的而且保证全球的短暂模拟的安定时候。
它算术地可能被在被计画的方式中的联合近似值错误是 ( 细节省略预定空间缺乏)