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Circular Waveguides in ANSYS Module

Nov 23, 2024

ANSYS Module on Circular Waveguides

Overview

  • Focus on governing equations of circular waveguides.
  • Review of previous module: rectangular waveguide using AEDT HFSS simulation.

Circular Waveguide Definition

  • Circular cross-section, generally in the xy-plane, uniform along the z-axis.
  • Radius defined as A.
  • Can be empty or filled with dielectric material (lossless with relative permittivity ε and permeability μ).
  • Walls made of PEC (Perfect Electroconductor) or metal.
  • Modes: Only TE (Transverse Electric) and TM (Transverse Magnetic) modes exist; no TEM mode.

Maxwell's Equations

  1. Represented in phasor format for a source-free region.
  2. Fields have components along x, y, and z axes in Cartesian coordinates.
  3. Use cylindrical coordinates (ρ, φ):
    • ρ ranges from 0 to A
    • φ ranges from 0 to 2π
  4. Transverse components: Eρ, Eφ, Hρ, Hφ; longitudinal components: EZ, HZ.
  5. Propagation along the z-axis: variation expressed as e^(jβz), where β is the propagation constant (lossless dielectric).

Expansion of Maxwell's Equations

  • Express transverse components in terms of longitudinal components.
  • kc: Cut-off wave number defined; k: wave number in the medium, given by
    • k = ω√(με) = 2π/λ.

Wave Equation Derivation

  • General longitudinal function φ derived for solutions.
  • TE case: E = 0; TM case: H = 0.
  • Wave equation expressed in cylindrical coordinates.
  • Using separation of variables, terms grouped into equations dependent on one variable.
  • Separation constant defined as and .

Bessel's Differential Equation

  • Reduced to Bessel's differential equation; general solutions involve Bessel functions (first and second kind).
  • C5 must be zero for cylindrical waveguides.
  • General function solution: includes constants A and B.

Boundary Conditions and Cut-off Wave Number

  • For TE case: tangential electric field must be zero at conductor surface.
  • Cut-off wave number derived using boundary conditions:
    • Jn(Kc * A) = 0.
  • TM case similar with E and H components.*

Mode Definitions

  • Modes categorized using indices TE_n,m and TM_n,m.
  • m: number of half-cycles along radial direction, always >= 1.
  • n: number of full cycle variations along circumference, can be 0.
  • TE11 mode has the lowest cutoff frequency (dominant mode), followed by TM01 and TE21 modes.

Conclusion

  • Understanding governing equations is crucial for designing waveguides.
  • Upcoming module: Simulating a circular waveguide in ANSYS Electronic Desktop HFSS using physical model geometry.
  • Additional resources: ANSYS Course.