the three most confusing topics in signal integrity
play

The Three Most Confusing Topics in Signal Integrity and how not to - PDF document

Slide -1 Bogatin: 3 Confusing Topics The Three Most Confusing Topics in Signal Integrity and how not to be confused with Dr. Eric Bogatin, Signal Integrity Evangelist, Bogatin Enterprises, www.beTheSignal.com eric@beTheSignal.com IEEE EMC


  1. Slide -1 Bogatin: 3 Confusing Topics The Three Most Confusing Topics in Signal Integrity and how not to be confused with Dr. Eric Bogatin, Signal Integrity Evangelist, Bogatin Enterprises, www.beTheSignal.com eric@beTheSignal.com IEEE EMC Distinguished Lecturer Series Slide -2 Bogatin: 3 Confusing Topics Overview • Why do we care? • Specific examples: � Characteristic Impedance � Differential Impedance � Inductance • Got your own? Send me a note IEEE EMC Distinguished Lecturer Series

  2. Slide -3 Bogatin: 3 Confusing Topics What are the Designer’s Most Important Tools? To Here Or Here From Here ? Creativity and intuition are the key ingredients to the design process IEEE EMC Distinguished Lecturer Series Slide -4 Bogatin: 3 Confusing Topics What Does it Mean to Refer to a Cable as a “50 Ohm Cable”? 3 foot long 50 Ohm coax Ω IEEE EMC Distinguished Lecturer Series

  3. Slide -5 Bogatin: 3 Confusing Topics What is the Most Important Electrical Quality the Signal Cares About? Ans: the instantaneous impedance V signal V Signal path V V in Return path GROUND IEEE EMC Distinguished Lecturer Series Slide -6 Bogatin: 3 Confusing Topics Electrical Model of a Lossless Transmission Line ∂ ∂ ∂ ∂ ( ) ( ) ( ) ( ) I x , t = − C V x , t Telegraphers’ equation V x , t = − L I x , t ∂ x ∂ t ∂ x ∂ t 2 2 2 2 ∂ 1 ∂ ∂ 1 ∂ ( ) ( ) ( ) ( ) V x , t = V x , t I x , t = I x , t Wave equation 2 2 2 2 ∂ t LC ∂ x ∂ t LC ∂ x L Z 0 = TD = LC derive C IEEE EMC Distinguished Lecturer Series

  4. Slide -7 Bogatin: 3 Confusing Topics “…be the signal” Charging up a transmission line + + + + + - - - - - V Z = Instantaneous Impedance, I IEEE EMC Distinguished Lecturer Series Slide -8 Bogatin: 3 Confusing Topics Geometry, Current and Impedance Line width increases, capacitance ______________, impedance______________ increases decreases Line width decreases, capacitance ______________, impedance ______________ decreases increases Dielectric thickness increases, capacitance ___________, impedance, ___________ decreases increases IEEE EMC Distinguished Lecturer Series

  5. Slide -9 Bogatin: 3 Confusing Topics What Does it Mean to Have a 50 Ohm Line? Verrrry longgggg 50 Ohm coax Ω IEEE EMC Distinguished Lecturer Series Slide -10 Bogatin: 3 Confusing Topics The Input Impedance of a Transmission Line is Time Dependent open Impedance (Ohms) Characteristic impedance Time Round trip Many round trip time of time of flights flight IEEE EMC Distinguished Lecturer Series

  6. Slide -11 Bogatin: 3 Confusing Topics “…the impedance” of a Transmission Line is Ambiguous • The input impedance of the transmission line - may be time dependent • The instantaneous impedance of the transmission line • The Characteristic impedance of the transmission line IEEE EMC Distinguished Lecturer Series Slide -12 Bogatin: 3 Confusing Topics 2 nd topic: Differential Impedance • What is differential impedance and how does coupling affect it? Difference signal IEEE EMC Distinguished Lecturer Series

  7. Slide -13 Bogatin: 3 Confusing Topics A Secret to Minimize Confusion About Differential Impedance Differential mode Think: : Think Common mode Differential signals Differential signals Common signals Common signals Odd mode Odd mode Even mode Even mode IEEE EMC Distinguished Lecturer Series Slide -14 Bogatin: 3 Confusing Topics Essential Principle Differential impedance is the instantaneous impedance the differential signal sees IEEE EMC Distinguished Lecturer Series

  8. Slide -15 Bogatin: 3 Confusing Topics The Differential Signal Differential signal V = 0v � � � 1v � V = 1v � � � � 0v 1 2 +1 Difference voltage = 2v : -1v � � � +1v � -1 What is the impedance the difference signal sees? What is the impedance the difference signal sees? IEEE EMC Distinguished Lecturer Series Slide -16 Bogatin: 3 Confusing Topics Differential Impedance and Series Impedances What is the equivalent impedance between the two signal lines? with no coupling: with no coupling: Z diff Z diff = Z 0 + Z 0 Z 0 Z 0 Z diff = 2 x Z 0 What happens to the impedance of one line when we turn on coupling? IEEE EMC Distinguished Lecturer Series

  9. Slide -17 Bogatin: 3 Confusing Topics Other Line Is Tied Low Z 0 , Second Trace Pegged Low 58 Single-Ended Impedance (Ohms) 56 54 52 50 Z 0 , Second Trace Pegged Low 48 46 44 42 40 0 5 10 15 20 25 30 35 40 45 50 Edge to Edge Spacing Between the Traces (mils) IEEE EMC Distinguished Lecturer Series Slide -18 Bogatin: 3 Confusing Topics Other Line Driven Opposite 58 s) hm 56 pedance (O 54 V diff = V 1 – V 2 Z 0 , Second Trace Pegged Low 52 50 Single-Ended Im 48 +1 v -1 v 46 44 Z 0 , Both Traces Driven Opposite 42 return 40 0 5 10 15 20 25 30 35 40 45 50 ODD MODE Edge to Edge Spacing Between the Traces (mils) IEEE EMC Distinguished Lecturer Series

  10. Slide -19 Bogatin: 3 Confusing Topics Relating the Modes’ Impedance to the Impedance the Signals See What is the equivalent impedance between the two signal lines? with coupling: with coupling: Z differential Z odd Z odd = Z 2 x Z differenti al odd decrease decrease As coupling increases, differential impedance will: _______________ IEEE EMC Distinguished Lecturer Series Slide -20 Bogatin: 3 Confusing Topics What’s Inductance? � � � � IEEE EMC Distinguished Lecturer Series

  11. Slide -21 Bogatin: 3 Confusing Topics Deficiencies with Text Book Definitions • Too mathematical to provide insight • Deals with coils, not traces on a board IEEE EMC Distinguished Lecturer Series Slide -22 Bogatin: 3 Confusing Topics Inductance Principles -1 wire carrying a current Rings of magnetic field lines are Rings of magnetic field lines are around all current carrying around all current carrying conductors conductors Right hand rule photo source: Halliday and Resnick, Physics, 1962 What influences the total number of rings of field lines? IEEE EMC Distinguished Lecturer Series

  12. Slide -23 Bogatin: 3 Confusing Topics Inductance Principles -2 2. Inductance is the number of rings of magnetic field 2. Inductance is the number of rings of magnetic field lines around a conductor, per amp of current lines around a conductor, per amp of current through it through it Units: Webers/amp = Henry nH more common Inductance is a measure of the efficiency of a conductor to create rings of magnetic field lines at the cost of current - high inductance, lots of field lines Many flavors of inductance: self � � mutual self mutual � partial loop � loop partial total, net or effective total, net or effective IEEE EMC Distinguished Lecturer Series Slide -24 Bogatin: 3 Confusing Topics Inductance Plays a Pivotal Role in Signal Integrity • Signal propagation: � loop self inductance • Discontinuities: � loop self inductance • Cross talk: � loop mutual inductance • PDN and rail collapse: � loop self inductance • Ground bounce: � total inductance of the return path Hacking interconnects: performance � physical design • � Partial self and partial mutual inductance IEEE EMC Distinguished Lecturer Series

  13. Slide -25 Bogatin: 3 Confusing Topics Most Important Principle (#3) of Inductance V � � I � � � � B � � ?B � � � V � 1831 Christmas lecture to the Royal Society: Faraday demonstrates “switching noise” Michael Faraday's discovery: Induction : dB/dt � V � I Changing magnetic field Changing lines around a conductor induce a voltage, which drives a current. IEEE EMC Distinguished Lecturer Series Slide -26 Bogatin: 3 Confusing Topics Summary • Why do we care? • Specific examples: � Characteristic Impedance � Differential Impedance � Inductance • Got your own? Send me a note IEEE EMC Distinguished Lecturer Series

  14. Slide -27 Bogatin: 3 Confusing Topics ����������� ���������� IEEE EMC Distinguished Lecturer Series

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend