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Unformatted text preview: Cunningham ECE329 Lecture 3334 Transmission Lines Lectures 33 & 34 Cunningham ECE329 Lecture 3334 Starting Point: Uniform Plane Wave http://www.phy.ntnu.edu.tw/java/emWave/emWave.html Cunningham ECE329 Lecture 3334 Starting Point: Uniform Plane Waves • Consider E and H that are – Perpendicular to each other – Perpendicular to the direction of propagation – Magnitude is constant (“uniform”) in the plane perpendicular to the propagation direction – And for perfect dielectric media: • E and H are in phase • No attenuation in zdirection E = E x ( z , t ) a x H = H y ( z , t ) a y x y z E H propagation Cunningham ECE329 Lecture 3334 Parallel Plate Transmission Line • If we place the conducting sheets in the uniform plane wave, some of the wave enters the box and is guided by it z x y Imagine a rectangular box made of perfect conductors on the upper and lower surfaces, filled by perfect dielectric medium x,y=0 x=d y=w z=0 z=l E x H y Cunningham ECE329 Lecture 3334 Parallel Plate Transmission Line x,y=0 x=d y=w z=0 z=l E x H y E x H y x=0 x=d y=w y=0 ε Cross section of the transmission line so wave is propagating into the page Cunningham ECE329 Lecture 3334 Take a look at boundary conditions E x H y x=0 x=d y=w y=0 ε Perfect conductor Perfect dielectric E y =0, D x =0, H y =0, B x =0 E y =0, D x = ρ s , H y =J s a z , B x =0 The E and H fields inside the transmission line result in the formation of charge and current on the upper and lower surfaces ++++++++++           −ρ s ρ s J s a zJ s a z " s = # E x J s = H y r a z Cunningham ECE329 Lecture 3334 TL Voltage x=d y=w E x H y −ρ s + ρ s V ( z , t ) = ( d ) E x ( z , t ) Cunningham ECE329 Lecture 3334 TL Current x=d y=w E x H yJ s a z J s a z I ( z , t ) = wH y ( z , t ) Cunningham ECE329...
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This note was uploaded on 01/17/2011 for the course ECE 305 taught by Professor Staff during the Summer '08 term at Michigan State University.
 Summer '08
 STAFF

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