Question 4 of 8: Rectangular Waveguide Cutoff Frequencies
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
98-Phys-A3, Electromagnetics — National Exam, December 2017. 3-hour closed-book exam (Casio or Sharp approved calculators only); any FIVE of the eight questions constitute a complete paper and only the first five as they appear in a candidate's answer book are marked, each of equal value. Aids given on the paper: ε0 = 8.85×10-12 F/m, μ0 = 4π×10-7 H/m. All eight printed questions are solved below as a complete study resource.
Reference texts: Sadiku, Elements of Electromagnetics (7th ed.) — plane waves and boundaries, transmission lines, waveguides, antennas; Hayt & Buck, Engineering Electromagnetics (9th ed.) — magnetic forces and torque, transmission-line transients; Pozar, Microwave Engineering (4th ed.) — transmission-line theory, stub matching, rectangular waveguide cutoff; Balanis, Antenna Theory (4th ed.) — infinitesimal-dipole far field.
Given. Rectangular waveguide, inside dimensions $a=2.25$ cm (broad wall) $\times$ $b=1$ cm (narrow wall), filled with a lossless dielectric $\varepsilon_r=2.25$ ($\mu_r=1$).
Find. The cutoff frequencies of the three lowest-order propagating modes.
Approach. Use the dielectric-filled rectangular-waveguide cutoff formula for TE$_{mn}$/TM$_{mn}$ modes and evaluate it for the low-order $(m,n)$ combinations, keeping in mind $a>b$ makes the $x$-direction (along $a$) the "easy" one.
Cutoff formula. For a guide filled with dielectric $\varepsilon_r$ (non-magnetic),
$$f_{c,mn}=\frac{1}{2\pi\sqrt{\mu_0\varepsilon_0\varepsilon_r}}\sqrt{\left(\frac{m\pi}{a}\right)^2+\left(\frac{n\pi}{b}\right)^2}=\frac{c}{2\sqrt{\varepsilon_r}}\sqrt{\left(\frac{m}{a}\right)^2+\left(\frac{n}{b}\right)^2}.$$
With $\sqrt{\varepsilon_r}=\sqrt{2.25}=1.5$, the prefactor is $c/(2\times1.5)=3\times10^8/3=1\times10^8$.
Dominant mode, TE$_{10}$ ($m=1,n=0$, along the wide wall $a=2.25$ cm $=0.0225$ m):
$$f_{c,10}=10^8\times\frac{1}{0.0225}=\boxed{4.44\ \text{GHz}}.$$
Next modes. TE$_{20}$ ($m=2,n=0$):
$$f_{c,20}=10^8\times\frac{2}{0.0225}=8.89\ \text{GHz}.$$
TE$_{01}$ ($m=0,n=1$, along the narrow wall $b=1$ cm $=0.01$ m):
$$f_{c,01}=10^8\times\frac{1}{0.01}=10.00\ \text{GHz}.$$
TE$_{11}$/TM$_{11}$ ($m=1,n=1$), for comparison:
$$f_{c,11}=10^8\sqrt{\left(\frac{1}{0.0225}\right)^2+\left(\frac{1}{0.01}\right)^2}=10.94\ \text{GHz}.$$
Rank the modes. $4.44<8.89<10.00<10.94$ GHz, so the three lowest propagating modes are TE$_{10}$, TE$_{20}$, and TE$_{01}$ (TE$_{11}$/TM$_{11}$ is the fourth).
Dielectric-filled rectangular waveguide cross-section, $a=2.25$ cm × $b=1$ cm, $\varepsilon_r=2.25$.