Download Analysis Methods for RF, Microwave, and Millimeter-Wave by Cam Nguyen PDF

By Cam Nguyen

Bring together the paintings of others within the box, write a booklet approximately it, increase 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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features a myriad of illustrations, homework difficulties, references, and numerical examples

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Detailing the lively and passive elements of microwaves, Microwave Engineering: innovations and basics covers every little thing from wave propagation to mirrored image and refraction, guided waves, and transmission strains, delivering a entire figuring out of the underlying rules on the middle of microwave engineering. This encyclopedic textual content not just encompasses approximately all features of microwave engineering, but in addition supplies all topics—including microwave new release, dimension, and processing—equal emphasis. jam-packed with illustrations to help in comprehension, the book:

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

Sample text

71b where j D mn or kl. Imposing these conditions on Eq. 73b S S 30 FUNDAMENTALS OF ELECTROMAGNETIC THEORY for two different TM and TE modes, respectively, provided that they have different cutoff wave numbers; that is, they are nondegenerate modes. The relationship described by Eq. 73) is known as the orthogonality condition between the scalar potentials. It states that the scalar electric or magnetic potentials of two nondegenerate modes are always orthogonal to each other. It should be noted that, due to Neumann’s and Dirichlet’s conditions, this orthogonality only holds for waveguides with perfectly conducting walls.

43) to the familiar Laplace’s Eq. 23) used WAVE TYPES AND SOLUTIONS 23 under the static condition. Note that both e x, y, z and h x, y, z are now identical to V x, y, z . We can also write the wave equations for the field vector potentials in the plane transverse to the propagating direction. 45b yez D yet x, y eš where h and e are the corresponding propagation constants, with the š signs indicating the Ýz-directions of propagation, respectively. 47b h e 2 x, y C kc,h h 2 x, y C kc,e e where yht x, y and yet x, y are the transverse magnetic and electric vector potentials, respectively.

9 Verify the power orthogonality relationship for nondegenerate modes in a lossless rectangular waveguide. 10 The electric and magnetic fields of the eigenmodes existing in planar transmission lines are normally determined approximately. 100) does not hold. Show also that, if these fields were calculated with a good accuracy, the orthogonality relation is well satisfied. 11 Derive the constant C in Eq. 108). 85) for TM and TE modes, respectively. 86) for hybrid modes. 103) for a lossless waveguide.

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