Anand K. Verma - Introduction To Modern Planar Transmission Lines

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rovides a comprehensive discussion of planar transmission lines and their applications, focusing on physical understanding, analytical approach, and circuit models
Planar transmission lines form the core of the modern high-frequency communication, computer, and other related technology. This advanced text gives a complete overview of the technology and acts as a comprehensive tool for radio frequency (RF) engineers that reflects a linear discussion of the subject from fundamentals to more complex arguments. 
Introduction to Modern Planar Transmission Lines: Physical, Analytical, and Circuit Models Approach  Emphasizes modeling using physical concepts, circuit-models, closed-form expressions, and full derivation of a large number of expressions Explains advanced mathematical treatment, such as the variation method, conformal mapping method, and SDA Connects each section of the text with forward and backward cross-referencing to aid in personalized self-study 
 is an ideal book for senior undergraduate and graduate students of the subject. It will also appeal to new researchers with the inter-disciplinary background, as well as to engineers and professionals in industries utilizing RF/microwave technologies.

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The impedance matrix could be obtained for a general linear two‐port network, shown in Fig (3.1). The wave entering the port is the incident voltage ( картинка 283) or the incident current ( картинка 284) wave. The reflected voltage ( картинка 285) and reflected current ( waves are also present at the ports The total port voltage V n or current - фото 286) waves are also present at the ports. The total port voltage (V n) or current (I n) is the sum of the incident and reflected voltage or current:

(3.1.1) In equation 311 n 1 2 is the port number ie port1 port2 The - фото 287

In equation (3.1.1), n = 1, 2 is the port number, i.e. port‐1, port‐2. The power entering the network is taken as a positive quantity for the incident wave, so the power coming out of the network, i.e. the power of the reflected wave, is taken as a negative quantity. The reflected voltage ( картинка 288) is positive. To maintain the negative direction of power flow, the reflected current wave ( картинка 289) is taken as negative in the above equation. At each port, the current entering the port from outside is positive, whereas the current leaving the port is negative. For the linear networks, the voltage at any port is a combined response of the currents applied to all ports. On using the superposition of the voltage responses, the following set of equations is written:

Figure 31 Twoport network to determine Z and Y parameters 312 - фото 290

Figure 3.1 Two‐port network to determine [Z] and [Y] parameters.

(3.1.2) Introduction To Modern Planar Transmission Lines - изображение 291

Equation (3.1.2)is written in a more compact matrix form:

(3.1.3) Introduction To Modern Planar Transmission Lines - изображение 292

where [V] and [I] are the column matrices. The two‐port impedance matrix is

(3.1.4) The Z parameter can be easily extended to the Nport networks B1 B3B5 - фото 293

The [Z] parameter can be easily extended to the N‐port networks [B.1, B.3–B.5]. The Z‐parameters are the open‐circuited parameters . The coefficient of the matrix can be defined in terms of the open circuit condition at the ports:

(3.1.5) All the ports are opencircuited except the i thport at which the matrix - фото 294

All the ports are open‐circuited, except the i thport at which the matrix element Z iiis defined. For instance, in the case of a two‐port network, Z 11is obtained when current I 1is applied to port‐1 and the voltage response is also obtained at the port‐1, while keeping the port‐2 open‐circuited, i.e. I 2= 0. The coefficient, Z 11, is known as the self‐impedance of the network. These are the diagonal elements of a [Z] matrix. The off‐diagonal elements of a [Z] matrix are defined as follows:

(3.1.6) In this case the current excitation is applied at the portj and the voltage - фото 295

In this case, the current excitation is applied at the port‐j and the voltage response is obtained at the port‐i. All other ports are kept open‐circuited allowing I k= 0, except at the port‐j. For instance, in the case of a two‐port network to evaluate Z 12, the current source is applied at the port‐2, and the voltage response is obtained at the port‐1, while keeping the port‐1 open‐circuited. The coefficient Z 12is the mutual impedance that describes the coupling of port‐2 with the port‐1. A network can have Z 11= Z 22, i.e. both of the ports are electrically identical. Such a network is known as the symmetrical network. Furthermore, the voltage response of a network at the port‐1 due to the current at the port‐2 can be identical to the voltage response at the port‐2, due to the current at the port‐1. This kind of network is a reciprocal network. It has a Z 12= Z 21. If Z 12= Z 21= 0, the ports are isolated one.

Example 3.1

Figure (3.2)shows lumped elements T‐network. Determine the [Z] parameter of the network.

Solution

For the port‐2 open‐circuited, I 2= 0. The voltage at the port‐1 is

Likewise for the port1 opencircuited I 1 0 and the parameters are Z 22 Z - фото 296

Likewise, for the port‐1 open‐circuited, I 1= 0, and the parameters are Z 22= Z B+ Z C, Z 12= Z C.The [Z] matrix description of a T‐network is

(3.1.7) Figure 32 Lumped Tnetwork The given circuit is asymmetrical However it is - фото 297

Figure 32 Lumped Tnetwork The given circuit is asymmetrical However it is - фото 298

Figure 3.2 Lumped T‐network.

The given circuit is asymmetrical. However, it is a reciprocal circuit. It becomes symmetrical for Z A= Z B.

Example 3.2

Determine the [Z]‐parameter of a section of the transmission line of length ℓ shown in Fig (3.3).

Solution

Let the port‐2 be open‐circuited and an incident voltage Introduction To Modern Planar Transmission Lines - изображение 299is applied at the port‐1. The voltage wave reaches to the port‐2 and reflects from there. It reaches the port‐1 as the voltage wave Introduction To Modern Planar Transmission Lines - изображение 300. The maximum of the voltage wave occurs at the port‐2. The total port voltages are given below:

Thus the Z parameters are obtained as follows The following Z matrix of - фото 301

Thus, the [Z] parameters are obtained as follows:

The following Z matrix of a line section is obtained by keeping in view that - фото 302

The following [Z] matrix of a line section is obtained by keeping in view that the uniform transmission line is a symmetrical and reciprocal network:

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