Analysis Methods for RF, Microwave, and Millimeter-Wave - download pdf or read online

By Cam Nguyen

ISBN-10: 0471017507

ISBN-13: 9780471017509

ISBN-10: 0471200670

ISBN-13: 9780471200673

Collect the paintings of others within the box, write a booklet approximately it, improve it with a number of mathematical appendices, ship it to the editor, and you will get 2 hundred pages+ of thick conception, void of functional curiosity for the layout engineer.

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Additional resources for Analysis Methods for RF, Microwave, and Millimeter-Wave Planar Transmission Line Structures

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At y D 0 and b). 2 Series-Form Green’s Function We consider again the Sturm–Liouville Eq. 67 where ˛i and ˇi (i D 1, 2) are constants. Accordingly, the Green’s function G x; x 0 must satisfy Eq. 69 n. 70 and the same boundary conditions for G x; x 0 in Eqs. 69). 72 is the Kronecker delta function. 73 nD1 where an is the amplitude coefficient. Multiplying both sides of Eq. 74 a Now multiplying Eq. 32) by ˚n x and Eq. 75 SOLUTIONS OF GREEN’S FUNCTION 51 whose left-hand side vanishes upon using Eqs.

At y D 0 and b). 2 Series-Form Green’s Function We consider again the Sturm–Liouville Eq. 67 where ˛i and ˇi (i D 1, 2) are constants. Accordingly, the Green’s function G x; x 0 must satisfy Eq. 69 n. 70 and the same boundary conditions for G x; x 0 in Eqs. 69). 72 is the Kronecker delta function. 73 nD1 where an is the amplitude coefficient. Multiplying both sides of Eq. 74 a Now multiplying Eq. 32) by ˚n x and Eq. 75 SOLUTIONS OF GREEN’S FUNCTION 51 whose left-hand side vanishes upon using Eqs.

36) can be found within the interval [a, b]. As a demonstration of the procedure for finding the Green’s function in closed form, we consider a shielded microstrip line as shown in Fig. 2. The shield and strip are assumed to be perfect conductors, and the strip thickness is negligible. We assume there exists a current source J on the strip. We wish to find the closed-form Green’s function and the z component of the electric field, Ez . The electric field component Ezi in region i (i D 0, 1) is produced by the current component Jz .

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Analysis Methods for RF, Microwave, and Millimeter-Wave Planar Transmission Line Structures by Cam Nguyen


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