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Lecture 17 Metallic Waveguides Dispersion Relations

Lecture 17 Metallic Waveguides Dispersion Relations. 6.013. ELECTROMAGNETICS AND APPLICATIONS. Luca Daniel. Outline. Review of Fundamental Electromagnetic Laws Electromagnetic Waves in Media and Interfaces Digital & Analog Communications TEM transmission lines (cables and IC/PCB traces)

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Lecture 17 Metallic Waveguides Dispersion Relations

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  1. Lecture 17Metallic Waveguides Dispersion Relations 6.013 ELECTROMAGNETICS AND APPLICATIONS Luca Daniel

  2. Outline • Review of Fundamental Electromagnetic Laws • Electromagnetic Waves in Media and Interfaces • Digital & Analog Communications • TEM transmission lines (cables and IC/PCB traces) • Digital communications (transients) • RF communications (matching loads to amplifiers) • RLC resonators (application: e.g. filters) • TEM resonators (application: e.g. microwave filters) • Metallic waveguides • Parallel plate waveguide • Cut off and dispersion relation • Rectangular waveguides • Cavity Resonators Today

  3. Parallel Plate Waveguides – Cut off and Dispersion kz = k sin  kx = k cos  Propagation condition (kz must be real)  k  Dispersion Relations Cut off frequency 2 TE2 slope=vg=d/dkz TE1 1 slope=vp =/kz kz

  4. TE10 Rectangular Waveguide Mode + + - - Add Sidewalls to TE1 Parallel Plate Waveguide  TE10: Surface charge s a Power flow b Surface current a Sidewall slots that will NOT stop current b

  5. Rectangular Waveguide Modes b b a a b b a a b b a a TE10 TE11 power What modes are these? • identify which lines are E and H • find the field that is always orthogonal to the waveguide propagation z • count half wavelenghts • determine the direction of power flow TM11 power

  6. Rectangular Waveguide Modes – Cut off and Dispersion Propagation condition (kz must be real) b a  Dispersion Relations Cut off frequencies TE20 20 11 TM11 TE11 01 TE01 slope=vg=d/dkz 10 TE10 slope=vp =/kz kz

  7. Rectangular Waveguide Design y b Cutoff Frequencies: x a TEm0 TE0n m Want b a/2 so that f01 f20 = n/a (f01 = n/2b) 4 Evanescence Propagation 3 TE20 TM20 Single propagating mode (if a  2b) [TE10] 2 TE10 1 0 f 2n/2a = f20 n/2a = f10 n/2b = f01

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