Rectangular Waveguide Theory

Understanding electromagnetic wave propagation in hollow conducting tubes

Introduction

A rectangular waveguide is a hollow metallic tube of rectangular cross-section used to guide electromagnetic waves at microwave frequencies (typically 1 GHz to 100 GHz). Unlike transmission lines that support TEM modes, waveguides support only TE (Transverse Electric) and TM (Transverse Magnetic) modes.

Dimensions
a = Wide dimension (m)
b = Narrow dimension (m)
a > b
Materials
Copper, Aluminum, or Brass with silver or gold plating for low loss
Applications
Radar systems, Satellite communication, Microwave ovens, Particle accelerators

Waveguide Geometry & Coordinates

a (Wide wall) b (Narrow wall) x y z (propagation) Hollow interior

Coordinate System

  • x: Transverse direction (0 to a)
  • y: Transverse direction (0 to b)
  • z: Propagation direction

Standard Waveguide Sizes (WR-90 example):

a = 22.86 mm (0.9 inch)

b = 10.16 mm (0.4 inch)

Frequency range: 8.2 - 12.4 GHz (X-band)

Modal Analysis

TE Modes (Transverse Electric)

Electric field entirely transverse (Ez = 0). Magnetic field has z-component.

Ez = 0
Hz ≠ 0
TEmn modes: m,n = 0,1,2,... (not both zero)

TM Modes (Transverse Magnetic)

Magnetic field entirely transverse (Hz = 0). Electric field has z-component.

Hz = 0
Ez ≠ 0
TMmn modes: m,n = 1,2,3,... (both non-zero)

Cutoff Frequency & Wavenumber

Cutoff wavenumber:

kc = √[(mπ/a)² + (nπ/b)²]

Cutoff frequency:

fc = (c/2π) × kc
= (c/2) × √[(m/a)² + (n/b)²]

Guide wavelength:

λg = λ0 / √[1 - (fc/f)²]
= 2π / β

Phase constant:

β = √[k² - kc²]
where k = 2πf√(με)

Dominant Mode: TE₁₀

The TE₁₀ mode is the dominant (lowest cutoff frequency) mode in rectangular waveguides. It has the lowest attenuation and is most commonly used.

Cutoff frequency fc = c/(2a)
Cutoff wavelength λc = 2a
Field pattern Half-sine variation in x, uniform in y
E-field (into/out of page) H-field (dots = out, crosses = in)

Cross-sectional view of TE₁₀ mode fields

Attenuation & Power Handling

Conductor Loss

αc = (Rs)/(a³bβkη) × [2bπ² + a³k²] (TE₁₀)

Rs = Surface resistance = √(πfμ/σ)

Dielectric Loss

αd = (k²tanδ)/(2β)

tanδ = Loss tangent of filling material

Power Capacity

Pmax = (ab/4η) × Ebr² × √[1-(fc/f)²]

Ebr = Breakdown field strength (~3 MV/m for air)