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Day 37: December 1, 2014 Transmission Lines Modeling and Termination
ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 37: December 1, 2014 Transmission Lines Modeling and Termination Penn ESE370 Fall DeHon
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Transmission Line Agenda
See in action in lab Where arise? General wire formulation Lossless Transmission Line Impedance End of Transmission Line? Termination Discuss Lossy Implications Penn ESE370 Fall DeHon
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From Day 36 Signal propagate as wave down transmission line
V(x,t) = A+Be(x-wt) Delay linear in wire length Speed Penn ESE370 Fall DeHon
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Wire “Resistance” What is the resistance at Vi ? Q to charge Vi?
Ii given velocity w? R = Vi/Ii? Ii+1 Ii Vi-1 Vi Vi+1 Ici Penn ESE370 Fall DeHon
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Wire “Resistance” Q=CV I = dQ/dt Moving at rate w I=wCV R=V/I=1/(wC)
Ii+1 Ii Vi-1 Vi Vi+1 Ici Penn ESE370 Fall DeHon
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Impedance Z0 =R= 1/wC = 1/(C/sqrt(LC)) Ii+1 Ii Vi-1 Vi Vi+1 Ici
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Impedance Assuming infinitely long wire,
how look different at Vi, Vi+1, Vi+2 ? Ii+1 Ii Vi-1 Vi Vi+1 Ici Penn ESE370 Fall DeHon
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Impedance Transmission line has a characteristic impedance
Looks to driving circuit like a resistance Penn ESE370 Fall DeHon
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Infinite Lossless Transmission Line
Transmission line looks like resistive load Input waveform travels down line at velocity Without distortion Z0 Penn ESE370 Fall DeHon
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End of Line What happens at the end of the transmission line?
Short Circuit Hint: what must happen in steady state? Terminate with R=Z0 Open Circuit Penn ESE370 Fall DeHon
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Short Penn ESE370 Fall DeHon
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Terminate R=Z0 Penn ESE370 Fall DeHon
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Open Penn ESE370 Fall DeHon
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Longer LC (open) 40 Stages L=100nH C=1pF Stage delay?
Drive with 2ns Pulse No termination (open circuit) Penn ESE370 Fall DeHon
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Pulse Travel RC V1,V3,V4,V5,V6 about 10 stages apart
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Analyze End of Line Penn ESE370 Fall DeHon
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Analyze End of Line Incident wave Vi=Ii×Z0 @ T-e Vi is voltage on line
Vt is what goes forward Voltage seen by end of line at T Vr is the delta voltage that starts moving back towards source at T+e Penn ESE370 Fall DeHon
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Analyze End of Line Incident wave Vi=Ii×Z0 KCL @ end KVL @ end
V=IR relationships? Which resistances go with each V? Relate all three V’s using R, Z0 Penn ESE370 Fall DeHon
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Analyze End of Line Incident wave Vi=Ii×Z0 KCL: Ii=Ir+It KVL: Vi+Vr=Vt
Vr=Ir×Z Ir=Vr/Z0 Vt=It×R It=Vt/R Ii=Vi/Z0 Penn ESE370 Fall DeHon
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Analyze End of Line Vi+Vr=Vt Eliminate Vt
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Analyze End of Line Vi+Vr=Vt Penn ESE370 Fall DeHon
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Analyze End of Line Vi+Vr=Vt Penn ESE370 Fall DeHon
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Reflection Sanity check with previous Short Matched Open
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Pulse Travel RC Penn ESE370 Fall DeHon
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Visualization http://www.williamson-labs.com/xmission.htm
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Back to Source Penn ESE370 Fall DeHon
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Back at Source? What happens at source? Depends on how terminated
Looks like at sink end Penn ESE370 Fall DeHon
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R≠Z0 What happens? 75 W termination on 50 W line
“Short-Circuit” source? Penn ESE370 Fall DeHon
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Simulation For these, with direct drive from voltage source
Source looks like short circuit (not typical of CMOS) Source cannot be changed Penn ESE370 Fall DeHon
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Transmission Line Symbole
Specify delay and impedance Need reference Penn ESE370 Fall DeHon
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Simulation For these, with direct drive from voltage source
Source looks like short circuit (not typical of CMOS) Source cannot be changed Penn ESE370 Fall DeHon
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50W line, 75W termination Penn ESE370 Fall DeHon
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Step Response Penn ESE370 Fall DeHon
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Idea Signal propagate as wave down transmission line
Delay linear in wire length Speed Impedance Behavior at end of line depends on termination Both src and sink are “ends” Penn ESE370 Fall DeHon
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Admin HW8 Thursday Finals 2010—2013 online
Good, but maybe too long Lectures Wednesday and Friday Andre out next week (12/8-17) Last office hour tomorrow Ron topic review Monday Dec. 8th classtime (last day of classes) Penn ESE370 Fall DeHon
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