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Day 36: November 26, 2013 Transmission Line Introduction and Analysis

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Presentation on theme: "Day 36: November 26, 2013 Transmission Line Introduction and Analysis"— Presentation transcript:

1 Day 36: November 26, 2013 Transmission Line Introduction and Analysis
ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 36: November 26, 2013 Transmission Line Introduction and Analysis Penn ESE370 Fall DeHon

2 Next few Lectures/Lab See in action in lab (last Friday) Where arise?
General wire formulation Lossless Transmission Line End of Transmission Line? Termination Discuss Lossy Implications Penn ESE370 Fall DeHon

3 Where Transmission Lines Arise
Penn ESE370 Fall DeHon

4 Transmission Lines Cable: coaxial PCB Twisted Pair (Cat5) Strip line
Microstrip line Twisted Pair (Cat5) Penn ESE370 Fall DeHon

5 Transmission Lines How did the coaxial cables behave in lab on Friday?
How differ from Ideal equipotential? RC-wire on chip? Penn ESE370 Fall DeHon

6 Transmission Lines This is what wires/cables look like
Aren’t an ideal equipotential Signals do take time to propagate Maintain shape of input signal Within limits Shape and topology of wiring effects how signals propagate …and the noise effects they see Penn ESE370 Fall DeHon

7 Transmission Lines Need theory/model to support Reason about behavior
Understand what can cause noise Engineer high performance communication Penn ESE370 Fall DeHon

8 Wire Formulation Penn ESE370 Fall DeHon

9 Wires In general, our “wires” have distributed R, L, C components
Penn ESE370 Fall DeHon

10 RC Wire When R dominates L
We have the distributed RC Wires we saw on Day 24 Typical of on-chip wires in Ics What is RC response to step? Penn ESE370 Fall DeHon

11 Transmission Line When resistance is negligible
Have LC wire = Lossless Transmission Line No energy dissipation (loss) through R’s More typical of Printed Circuit Board wires Penn ESE370 Fall DeHon

12 Build Intuition from LC
What did one LC do? What will chain do? Penn ESE370 Fall DeHon

13 Intuitive: Lossless Pulses travel as waves without distortion
(up to a characteristic frequency) Penn ESE370 Fall DeHon

14 SPICE Simulation Penn ESE370 Fall DeHon

15 SPICE Simulation Penn ESE370 Fall DeHon

16 Pulse Response SPICE Penn ESE370 Fall DeHon

17 Contrast RC Wire Penn ESE370 Fall DeHon

18 Contrast Penn ESE370 Fall DeHon

19 Visualization See: Penn ESE370 Fall DeHon

20 Model Need to understand Voltage as a function of position and time
Position along wire Want to get V(x,t) Also I(x,t) Penn ESE370 Fall DeHon

21 Setup Relations i is a position Position: x=i × Δx So Vi is V(x=iΔx)
Ici Penn ESE370 Fall DeHon

22 Setup Relations Vi-Vi-1 = Ici= Ii-Ii+1= Ii+1 Ii Vi-1 Vi Vi+1 Ici
Penn ESE370 Fall DeHon

23 Setup Relations Vi-Vi-1 = -Ldii/dt Ici=CdVi/dt i is spatial dimension
Ii-Ii+1=Ici i is spatial dimension Vi at different positions Ii+1 Ii Vi-1 Vi Vi+1 Ici Penn ESE370 Fall DeHon

24 Setup Relations Vi-Vi-1 = -Ldii/dt Ici=CdVi/dt Ii-Ii+1=Ici Ii+1 Ii
Penn ESE370 Fall DeHon

25 Reduce to Single Equation
Eliminate Ici? Ii-Ii+1=Ici=CdVi/dt Take derivative with respect to time dii/dt - dii+1/dt=Cd2Vi/dt Penn ESE370 Fall DeHon

26 Reduce to Single Equation
dii/dt - dii+1/dt=Cd2Vi/dt Vi-Vi-1 = -Ldii/dt Vi+1-Vi = -Ldii+1/dt Eliminate Is ? Vi-Vi-1 -(Vi+1-Vi )= -Ldii/dt + Ldii+1/dt d2V/dx =LCd2V/dt Penn ESE370 Fall DeHon

27 Implication d2V/dx = LCd2V/dt V(x,t) = A+Be(x-wt)
Wave equation V(x,t) = A+Be(x-wt) Be(x-wt)=LCw2Be(x-wt) w=1/sqrt(LC) What is w? Penn ESE370 Fall DeHon

28 Light Cycle Context http://www.youtube.com/watch?v=GNfs6v7i7eY
Penn ESE370 Fall DeHon

29 Light Cycle Example What is the position of a cycle at time t
Start at x=0 Travel at v Light Cycle is step function at x=0 Cycle creates trail of height 1 F(0, t=0)=1, F(x>0,t=0)=0  F(x,t=0)=1-u(x) Penn ESE370 Fall DeHon

30 Light Cycle Example Light Cycle is step function at x=0
Cycle creates trail of height 1 F(0, t=0)=1, F(x>0,t=0)=0  F(x,t=0)=1-u(x) When does cycle reach position x>0? What is F(x,t)? t=0 x=0 t=t1 x=0 x=? Penn ESE370 Fall DeHon

31 Implication d2V/dx = LCd2V/dt V(x,t) = A+Be(x-wt)
Wave equation V(x,t) = A+Be(x-wt) Be(x-wt)=LCw2Be(x-wt) w=1/sqrt(LC) What is w? Penn ESE370 Fall DeHon

32 Implication d2V/dx = LCd2V/dt V(x,t) = A+Be(x-wt)
Wave equation V(x,t) = A+Be(x-wt) Be(x-wt)=LCw2Be(x-wt) w=1/sqrt(LC) Rate of propagation Penn ESE370 Fall DeHon

33 Propagation Rate in Example
L=1uH C=1pF What is w ? Penn ESE370 Fall DeHon

34 Signal Propagation Penn ESE370 Fall DeHon

35 Propagation Be(x-wt+x)=LCw2Be(x-wt) w=1/sqrt(LC) Rate of propagation
Delay linear in length Compare RC wire delay quadratic in length Penn ESE370 Fall DeHon

36 Contrast RC Wire Penn ESE370 Fall DeHon

37 Propagation From Day 35 we know for wire: CL = em
Be(wt+x)=LCw2Be(wt+x) w=1/sqrt(LC) Rate of propagation Delay linear in length Compare RC wire delay quadratic in length From Day 35 we know for wire: CL = em w=1/sqrt(em)=c0/sqrt(ermr) Where c0=speed of light in vacuum=30cm/ns Penn ESE370 Fall DeHon

38 Idea Signal propagate as wave down transmission line
Delay linear in wire length Speed Penn ESE370 Fall DeHon

39 Admin HW8 out Back here on Monday
Includes writeup for previous and this lab Also three questions Back here on Monday Penn ESE370 Fall DeHon


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