08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 1 Transmission Lines Transmission line effects must be considered when length is comparable.

Slides:



Advertisements
Similar presentations
Note 2 Transmission Lines (Time Domain)
Advertisements

RF Communication Circuits
Waves and Transmission Lines Wang C. Ng. Traveling Waves.
Waves and Transmission Lines TechForce + Spring 2002 Externship Wang C. Ng.
EMLAB 1 Transmission line. EMLAB 2 An apparatus to convey energy or signal from one place to another place. Transmitter to an antenna connections between.
11/24/2004EE 42 fall 2004 lecture 361 Lecture #36: Transmission lines Last lecture: –Transmission lines –Balanced and unbalanced –Propagation This lecture:
Characteristic Impedance Contnd. Air Dielectric Parallel Line Coaxial Cable Where: D = spacings between centres of the conductors r = conductor radius.
EEE 498/598 Overview of Electrical Engineering
EKT241 – ELECTROMAGNETICS THEORY
Chapter Fourteen: Transmission Lines
Derivation and Use of Reflection Coefficient
UNIVERSITI MALAYSIA PERLIS
Prof. D. R. Wilton Note 2 Transmission Lines (Time Domain) ECE 3317.
ELCT564 Spring /9/20151ELCT564 Chapter 2: Transmission Line Theory.
Chapter 2: Transmission Line Theory
EELE 461/561 – Digital System Design
July, 2003© 2003 by H.L. Bertoni1 I. Introduction to Wave Propagation Waves on transmission lines Plane waves in one dimension Reflection and transmission.
Distributed constants Lumped constants are inadequate models of extended circuit elements at high frequency. Examples are telephone lines, guitar strings,
Lecture 6 Last lecture: Wave propagation on a Transmission line Characteristic impedance Standing wave and traveling wave Lossless transmission.
Lecture 2 Transmission lines 1.Transmission line parameters, equations 2.Wave propagations 3.Lossless line, standing wave and reflection coefficient.
EEE340Lecture 411 Half-wave Calibration and measurement which is from We obtain also (9.115) (9.118) (9.119) (9.116) (9.117)
Prof. Ji Chen Notes 13 Transmission Lines (Impedance Matching) ECE Spring 2014.
G Practical MRI 1 – 26 th March 2015 G Practical MRI 1 Review of Circuits and Electronics.
Advanced Microwave Measurements
1 Basics of Microwave Measurements Steven Anlage
ENE 428 Microwave Engineering
1 ENE 429 Antenna and Transmission lines Theory Lecture 4 Transmission lines.
Lecture 4.  1.5 The terminated lossless transmission line What is a voltage reflection coefficient? Assume an incident wave ( ) generated from a source.
ECE 546 – Jose Schutt-Aine 1 ECE 546 Lecture -04 Transmission Lines Spring 2014 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois.
© H. Heck 2008Section 5.41 Module 5:Advanced Transmission Lines Topic 4: Frequency Domain Analysis OGI ECE564 Howard Heck.
© H. Heck 2008Section 2.31 Module 2:Transmission Lines Topic 3: Reflections OGI ECE564 Howard Heck.
Chapter 2. Transmission Line Theory
Prof. Ji Chen Notes 9 Transmission Lines (Frequency Domain) ECE Spring 2014.
Transmission Line Theory
10. Transmission Line 서강대학교 전자공학과 윤상원 교수
Prof. D. R. Wilton Notes 6 Transmission Lines (Frequency Domain) ECE 3317 [Chapter 6]
CHAPTER 4 TRANSMISSION LINES.
Lossless Transmission Line If Then: All TEM, L’C’=µε Selected conductors: High conductivities Dielectric materials: negligible conductivities.
Note 3 Transmission Lines (Bounce Diagram)
Lecture 9 Smith Chart Normalized admittance z and y are directly opposite each other on.
Penn ESE370 Fall DeHon 1 ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 35: December 5, 2012 Transmission Lines.
1 RS ENE 428 Microwave Engineering Lecture 5 Discontinuities and the manipulation of transmission lines problems.
Notes 8 Transmission Lines (Bounce Diagram)
1.  Transmission lines or T-lines are used to guide propagation of EM waves at high frequencies.  Examples: › Transmitter and antenna › Connections.
Prof. David R. Jackson Notes 13 Transmission Lines (Impedance Matching) ECE 3317 [Chapter 6]
So far, we have considered plane waves in an infinite homogeneous medium. A natural question would arise: what happens if a plane wave hits some object?
Prof. Ji Chen Notes 6 Transmission Lines (Time Domain) ECE Spring 2014.
Lecture 2. Review lecture 1 Wavelength: Phase velocity: Characteristic impedance: Kerchhoff’s law Wave equations or Telegraphic equations L, R, C, G ?
Lecture 3.
Chapter 2. Transmission Line Theory
Chapter 2 Transmission Line Theory (2.1 ~ 2.5) 전자파연구실 1.
Chapter9 Theory and Applications of Transmission Lines.
1 John McCloskey NASA/GSFC Chief EMC Engineer Code 565 Building 23, room E Fundamentals of EMC Transmission Lines.
Figure 11.1 Figure 11.1 Basic transmission line circuit, showing voltage and current waves initiated by closing switch S 1.
HDT, 1998: Resistance, Inductance, Capacitance, Conductance per Unit Length Lossless case.
Smith Chart & Matching Anurag Nigam.
High Speed Signal Integrity Analysis
S- Parameters.
Characteristic Impedance Contnd.
Day 37: December 1, 2014 Transmission Lines Modeling and Termination
Day 37: December 2, 2013 Transmission Lines Modeling and Termination
ENE 428 Microwave Engineering
Applied Electromagnetic Waves Notes 6 Transmission Lines (Time Domain)
Notes 8 Transmission Lines (Bounce Diagram)
Notes 11 Transmission Lines
Notes 10 Transmission Lines (Reflection and Impedance)
Microwave Engineering
Voltage Reflection Coefficient
N-port Network Port reference Line Impedance Port Voltage & Current.
4th Week Seminar Sunryul Kim Antennas & RF Devices Lab.
Presentation transcript:

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 1 Transmission Lines Transmission line effects must be considered when length is comparable to ¼ wavelength We will ignore the energy loss on transmission lines Concentrate on time-domain description rather than frequency domain egeg + - zgzg zlzl i i e xd l

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 2 Transmission Lines C:Capacitance / Unit Length [F/m] L:Inductance / Unit Length [H/m] R:Conductor Resistance / Unit Length [Ω/m] G:Insulation Conductance /Unit Length [ /m] Note G ≠ 1/R ! Ω

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 3 Transmission Lines By KVL: In the limit as :

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 4 Transmission Lines By KCL: In the limit as :

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 5 Lossless Case Take partial derivative w.r.t. x in (1) and partial derivative w.r.t. t in (2), then substitute. Recognize as wave equations

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 6 Lossless Case Show that the solution is in the form.

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 7 Interpretation is a wave traveling to right with velocity is a wave traveling to left with velocity Solving for i, we obtain is characteristic of line

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 8 Interpretation Note: Each traveling wave direction, e and i are related by z 0.

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 9 Reflections Look at terminations with real impedances  frequency independent Wave of voltage and current traveling to right At termination zlzl z0z0 e - + elel + - ilil

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 10 Reflections Hence, there must be reflected waves e - and i - such that In terms of voltage Reflection coefficient

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 11 Reflections Special cases: –z l = z 0  k=0 Matched, no reflections. Line looks infinite. –z l = 0, short circuit  k = -z 0 /z 0 = -1 –z l =, open circuit  k = 1 8

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 12 Multiple Reflections R=3z 0 z0z0 t=0 x=0 x=l E Hitting load, a wave of E/2 is produced E t=.3T E t=1.3T 3E/2 E t=2.3T 3E/2 Arriving wave of E/2 is reflected toward load T2T3T4T5T Voltage at load 1.5E.75E 1.125E.9375E 6T 7T E

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 13 Time-Space (Bounce) Diagram Mark reflection coefficients Write initial voltages Write wave amplitudes Update –Wave amplitudes when reflected –Voltages as waves cross x k 0 =-1k l =.5 e=E e=0 e=E E E/2 -E/2 -E/4 E/4 E/8 T 2T 3T 4T 5T e=3E/2 e=3E/4 e=9E/8 Time

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 14 Example 3z 0 E z0z0 Magnitude of the first wave: x k 0 =.5k l =1 e=E/4 e=0 e=5E/8 e=13E/16 E/4 E/8 E/16 T 2T 3T 4T 5T e=E/2 e=3E/4 e=7E/8 Time z0z0 t=0 k 0 =.5 E R=3z 0 l k l =1 E t At x=0 T2T3T 4T 5T

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 15 Reflections in Digital Lines Consider one source and one load Option 1: Do not terminate either end. Ringing will stop eventually. –Pro:Simple, no additional power loss –Con:Limited speed

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 16 Reflections in Digital Lines Option 2: Matched termination at the end –Pro:No reflections –Con:Excessive power consumption For z 0 =150Ω, power consumption 135mW Reduce by duty factor (0.5 for regular lines, 0.05 for floppy drives) Multiply by number of lines z0z0 Open-collector driver

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 17 Reflections in Digital Lines Option 3: Matched termination at the source end –Pro:Can be run at the same speed as load termination If receiver has very high input impedance, full voltage appears at the receiver No power dissipated at constant voltage level –Con:Special, high input impedance line receivers required (not suited for standard TTL) Look at multiple terminations z0z0

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 18 Reflection in Digital Lines Problem for multiple receivers –Assume the ideal case, where taps are infinitely short and have infinite impedances –Even for this case, intermediate taps do not get full signal immediately z0z0 E x k 0 =0k l =1 e=.5E e=0 E/2 T 2T e=E E t At x=.5L.5TT1.5T 2T

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 19 Reflection and Transmission at Junctions e 1 +, i 1 + e 1 -, i 1 - e 2 +, i 2 + e 3 +, i 3 +

08 - Winter 2005 ECE ECE 766 Computer Interfacing and Protocols 20 Reflection and Transmission at Junctions 3/2 L 2/3 L L z0z0 t=0 T 2T 3T 4T k=0 k=1 E/2 -E/6 2E/9 E/3 2E/9 E/3 -E/9 Many multiple reflections, eventually come to rest