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Question 10.1: A parallel-plate waveguide as shown in Fig. 10.3 has an air ......

A parallel-plate waveguide as shown in Fig. 10.3 has an air gap of d[m].

(a) Show that the TE modes expressed by Eq. (10-4b) are mutually orthogonal

such that  \int_{y=0}^{y= d}{\pmb{E}_{m} \pmb{\cdot }\pmb{E}^{*}_{n} dy }= 0   for mn.

\boxed{\pmb{E} = – j 2 E_{o} \pmb{a}_{x} \sin (k_{y} y) e^{- j k_{z}z}}                                                                  (10-4b)

(b) Find the orthonormal set in TE modes satisfying

\int_{y=0}^{y= d}{\pmb{E}_{m} \pmb{\cdot }\pmb{E}^{*}_{m} dy = 1}.

10.3
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(a) Upon using Eq. (10-4b), we write

\int_{y=0}^{y= d}{\pmb{E}_{m} \pmb{\cdot }\pmb{E}^{*}_{n} dy} = 4 E^{2}_{o} \int_{y=0}^{y= d}{\sin \left\lgroup\frac{m\pi }{d}y \right\rgroup \sin \left\lgroup\frac{n\pi }{d}y \right\rgroup dy} \\   \quad \quad \quad \quad \quad \quad \quad = 2 E^{2}_{o} \int_{y=0}^{y= d}{\left[\cos \left\{ (m – n)\frac{\pi y}{d}\right\} – \cos \left\{(m + n)\frac{\pi y}{d} \right\} \right] dy} \\ \quad \quad \quad \quad \quad \quad \quad   = 0

(b) Assuming m = n in part (a) we have

\int_{y=0}^{y= d}{\pmb{E}_{m} \pmb{\cdot }\pmb{E}^{*}_{m} dy} = 2 d E^{2}_{o}

Dividing Eq. (10-4b) by \sqrt{2 d E^{2}_{o}} , the orthonormal set in TE modes is

\boxed{\pmb{E}_{m} = – j \sqrt{\frac{2}{d} } \pmb{a}_{x} \sin \left\lgroup\frac{m \pi }{d} y \right\rgroup e^{- j k_{z}z}}            (m = 1,2,3,…)              (10-19)

If an electromagnetic field is propagating in a parallel-plate waveguide, which is known to have no longitudinal component of E, then its electric field can be expanded in terms of the orthonormal set given in Eq. (10-19).

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