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Consider an air-filled rectangular waveguide with dimensions a = 2.286 cm and b = 1.016 cm. At 10 GHz operating frequency, the value of the propagation constant (per meter) of the corresponding propagating mode is __________

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Concept:

The propagation constant is given by \({\rm{\gamma }} = \sqrt {{{\left( {\frac{{{\rm{m\pi }}}}{{\rm{a}}}} \right)}^2} + {{\left( {\frac{{{\rm{n\pi }}}}{{\rm{b}}}} \right)}^2} - {{\rm{k}}^2}}\)

Application:

\({{\rm{f}}_{{\rm{c}},10}} = \frac{{\rm{c}}}{{2{\rm{a}}}} = 6.56{\rm{\;GHz}}\)

\({{\rm{f}}_{{\rm{c}},01}} = \frac{{\rm{c}}}{{2{\rm{b}}}} = 14.76{\rm{\;GHz}}\)

So, 10 GHz can propagate only in TE10 node.

Now, the free space propagation constant will be:

\({\rm{k}} = \frac{{\rm{\omega }}}{{\rm{c}}} = \frac{{2{\rm{\pi }} \times 100 \times {{10}^8}}}{{3 \times {{10}^8}}} \)

\(k= \frac{{200{\rm{\pi }}}}{3}\)

Now, the propagation constant will be:

\({\rm{\gamma }} = \sqrt {{{\left( {\frac{{{\rm{m\pi }}}}{{\rm{a}}}} \right)}^2} + {{\left( {\frac{{{\rm{n\pi }}}}{{\rm{b}}}} \right)}^2} - {{\rm{k}}^2}}\)

With m = 1 and n = 0, we get:

\( {\rm{\gamma }} = \sqrt {{{\left( {\frac{{\rm{\pi }}}{{2.286 \times {{10}^{ - 2}}}}} \right)}^2} - {{\left( {\frac{{200{\rm{\pi }}}}{3}} \right)}^2}}\)

\({\rm{\gamma }}\)  = j158.05 m-1

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