Electromagnetics, Microwave Circuit, and Antenna Design for Communications Engineering, Second Edition

Figure 7.26 shows a circular waveguide with inner diameter 2 a. We investigate the lossless circular waveguide with a perfectly conducting wall and free-space inner region. To investigate the TM and TE modes of the circular cylindric waveguide we derive the fields either from an electric Hertz form ? e or a magnetic Hertz form ? m exhibiting only a z-component
| (7.297a) | |
| (7.297b) | |
For both cases the Helmholtz equation (3.28) has the following form:
| (7.298) | |
with
. With (A.157) we obtain for circular cylindric coordinates
| (7.299) | |
We seek solutions for waves propagating in the positive z-direction and choose the separation formulation
| (7.300) | |
From this it follows that
| (7.301) | |
We introduce the parameter k c given by
| (7.302) | |
and obtain
| (7.303) | |
The first two terms of this equation are dependent on r only, whereas the third term only depends on ?. This equation therefore can be fulfilled only if the sum of the first two terms and the last term as well as the third term each are independently constant. Therefore we set the third term equal to - n 2 and obtain
| (7.304) | |
The solution of this equation is
| (7.305) | |
Since f( ?) is periodic with 2 ?, the parameter n must be an integer. Furthermore A' = 0 without loss of generality, since both solutions in (7.305) only are distinguished...