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Question 10.8: How many component plane-waves does the TE10 mode contain in......

How many component plane-waves does the TE_{10} mode contain in a rectangular waveguide with dimensions a and b?

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For the TE_{10} mode, let us rewrite Eq. (10-74) as

\boxed{H_{z}(x,y) = H_{o} \cos \left\lgroup\frac{m\pi }{a} x \right\rgroup \cos \left\lgroup\frac{n\pi }{b}y \right\rgroup }                ( m,n = 0,1,2,…)                     (10-74)

H_{z} = H_{o} \cos \left\lgroup\frac{\pi }{a}x \right\rgroup = H_{o} \frac{1}{2} (e^{j\pi x/a} +e^{- j\pi x/a})                                          (10-89)

As can be seen from Eq. (10-75), the TE_{10} mode has no E_{x}– and no H_{y}component. Rewriting Eq. (10-75c) for the TE_{10} mode, we have

\boxed{E_{x} =\frac{j\omega \mu }{h^{2}} \left\lgroup\frac{n\pi }{b} \right\rgroup H_{o} \cos \left\lgroup \frac{m\pi }{a}x \right\rgroup \sin \left\lgroup\frac{n\pi }{b}y \right\rgroup}    (m,n = 0,1,2,…)   (10-75a) \\ \boxed{E_{y} = – \frac{j\omega \mu }{h^{2}} \left\lgroup \frac{m\pi }{a} \right\rgroup H_{o} \sin \left\lgroup\frac{m\pi }{a}x \right\rgroup \cos \left\lgroup\frac{n\pi }{b}y \right\rgroup }                                                               (10-75b) \\\boxed{H_{x} = \frac{\gamma }{h^{2}} \left\lgroup\frac{m \pi }{a} \right\rgroup H_{o} \sin \left\lgroup \frac{m\pi }{a}x \right\rgroup \cos \left\lgroup \frac{n\pi }{b} y\right\rgroup}                                                              (10-75c)\\ \boxed{H_{y} = \frac{\gamma }{h^{2}} \left\lgroup\frac{n \pi }{b} \right\rgroup H_{o} \cos \left\lgroup \frac{m\pi }{a}x \right\rgroup \sin \left\lgroup \frac{n\pi }{b} y\right\rgroup}                                                    (10-75d) \\  \\ H_{x} = \frac{\gamma }{h^{2}} \left\lgroup\frac{\pi }{a} \right\rgroup H_{o} \sin \left\lgroup \frac{\pi }{a}x \right\rgroup = \frac{\gamma }{h^{2}} \left\lgroup\frac{\pi }{a} \right\rgroup H_{o} \frac{1}{2j} (e^{j\pi x/a} +e^{- j\pi x/a})                        (10-90)

Combining Eq. (10-89) and Eq. (10-90), assuming a lossless waveguide( \gamma = j\beta _{10}  ), the magnetic field phasor is

\pmb{H} =\left\{H_{x}(x, y) \pmb{a}_{x} + H_{y} (x,y) \pmb{a}_{y} +H_{z} (x,y) \pmb{a}_{z}\right\} e^{-j\beta _{10}z}

From the above equation, we see that the mode TE_{10} comprises two plane waves of the form e^{j \pi x/a -j\beta _{10}z}  and e^{- j \pi x/a -j\beta _{10}z} .

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