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17-Phys-A3 Electromagnetics · December 2017

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.

Question 4: Rectangular Waveguide Cutoff Frequencies (equal value)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

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.

  1. 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 $c/(2\times1.5)=3\times10^8/3=1\times10^8$.
  2. Dominant mode, TE$_{10}$ ($m=1,n=0$, along the wide wall $a=2.25$ cm $=0.0225$ m): $$f_{c,10}=10^8\times\frac{1}{0.0225}=\boxed{4.44\ \text{GHz}}.$$
  3. 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: $$f_{c,11}=10^8\sqrt{\left(\frac{1}{0.0225}\right)^2+\left(\frac{1}{0.01}\right)^2}=10.94\ \text{GHz}.$$
  4. 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).
εᵣ = 2.25a = 2.25 cmb = 1 cm
Dielectric-filled rectangular waveguide cross-section, $a=2.25$ cm × $b=1$ cm, $\varepsilon_r=2.25$.
Final results
ModeCutoff frequency
TE$_{10}$ (lowest)4.44 GHz
TE$_{20}$ (2nd lowest)8.89 GHz
TE$_{01}$ (3rd lowest)10.00 GHz
TE$_{11}$/TM$_{11}$ (for reference, 4th)10.94 GHz