By Ramesh Garg

ISBN-10: 1596933852

ISBN-13: 9781596933859

ISBN-10: 1596933860

ISBN-13: 9781596933866

In achieving optimum microwave process functionality via gaining knowledge of the rules and strategies underlying latest strong computational instruments and advertisement software program in electromagnetics. This authoritative source will give you transparent and whole clarification of this crucial electromagnetics wisdom, supplying you with the analytical historical past you must comprehend such key techniques as mother (method of moments), FDTD (Finite distinction Time area) and FEM (Finite point Method), and Green's services. This finished publication contains all math essential to grasp the cloth. in addition, it beneficial properties a number of solved difficulties that aid determine your realizing of key options during the booklet.

To continue you from being slowed down with advanced mathematical info (vector calculus) and coding, this entire quantity areas emphasis at the research of the scalar wave equation in Cartesian coordinates. The ebook additionally comprises a number of selection questions, applicable for self research or classes, that aid make clear recommendations with none mathematical burden. jam-packed with over 1,300 equations, many of the difficulties awarded within the e-book should be solved utilizing not anything greater than calculator.

**Software incorporated **

**CD-ROM-Included! comprises time-saving Matlab® resource code for the issues awarded within the ebook which might be simply changed that will help you resolve related difficulties within the box.
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**Extra info for Analytical and Computational Methods in Electromagnetics**

**Sample text**

It may be positive, negative, or simply zero. Let us consider these possibilities. Case 1: C > 0. In this case, C may be expressed as C = k 2. 17b) and Case 2: C < 0. For this case, C may be expressed as C = −k 2. 18b) and 34 Analytical Methods and Orthogonal Functions Case 3: C = 0. 19) Out of the three possible solutions described above, only case 2 can satisfy the boundary conditions at x = 0 and x = a because sin (kx) and cos (kx) can have infinite number of zeros. 18). 10c) is satisfied if B 2 = 0.

29) Wave Equation for Guided Waves. The wave equation for the guided waves can be simplified because the direction of propagation is specified with an assumed propagation constant along this direction. Let us consider guided waves in transmission lines/waveguides and assume that the direction of propagation is z. 30) where ٌt is the transverse (to the z-axis) operator. 32) 2 = ٌt + ␥ 2 2 where ٌt is the transverse Laplacian operator. 34) 14 Basic Principles of Electromagnetic Theory The quantities k c and c are called the cutoff wave number and cutoff frequency, respectively, since they reduce to the corresponding parameters at the cutoff (␥ = 0).

8 (a) Conducting wedge of angle ␣ . (b) Semi-infinite strip of conductor thickness t and a rectangular metal block with ␣ = /2. 65) where A, v, and 0 are the constants to be determined. 13c); that is, nˆ . 15 Classification of Methods of Analysis 21 When the internal angle of the wedge is less than , v is less than 1 and E , and therefore, charge density become singular at the edge, whereas E and E z remain finite. For the half-plane or semi-infinite strip, ␣ = 0, v = 1/2; and s ϰ 1/ 1/2.

### Analytical and Computational Methods in Electromagnetics by Ramesh Garg

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