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Slide -1 Bogatin: 3 Confusing Topics IEEE EMC Distinguished Lecturer Series 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 [email protected] Slide -2 Bogatin: 3 Confusing Topics IEEE EMC Distinguished Lecturer Series Overview Why do we care? Specific examples: Characteristic Impedance Differential Impedance Inductance Got your own? Send me a note

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Page 1: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -1Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

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

[email protected]

Slide -2Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Overview

• Why do we care?

• Specific examples:

Characteristic Impedance

Differential Impedance

Inductance

• Got your own? Send me a note

Page 2: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -3Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

What are the Designer’s Most Important Tools?

From Here To Here Or Here

?

Creativity and intuition are the key ingredients to the design process

Slide -4Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

What Does it Mean to Refer to a Cable as a “50 Ohm Cable”?

Ω

3 foot long 50 Ohm coax

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Slide -5Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

What is the Most Important Electrical Quality the Signal Cares About?

GROUND

VVsignal

Signal path

Return pathVVin

Ans: the instantaneous impedance

Slide -6Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Electrical Model of a Lossless Transmission Line

( ) ( )t,xIt

Lt,xVx ∂

∂−=

∂ ( ) ( )t,xVt

Ct,xIx ∂

∂−=

( ) ( )t,xVxLC

1t,xV

t 2

2

2

2

∂=

∂ ( ) ( )t,xIxLC

1t,xI

t 2

2

2

2

∂=

Telegraphers’ equation

Wave equation

C

LZ0 = LCTD =derive

Page 4: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -7Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

“…be the signal”

+ + + + +

- - - - -

Charging up a transmission line

Instantaneous Impedance, I

VZ =

Slide -8Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Geometry, Current and Impedance

Line width decreases, capacitance ______________, impedance ______________

Dielectric thickness increases, capacitance ___________, impedance, ___________

Line width increases, capacitance ______________, impedance______________decreases

increases

increases

decreases

decreases

increases

Page 5: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -9Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

What Does it Mean to Have a 50 Ohm Line?

Ω

Verrrry longgggg 50 Ohm coax

Slide -10Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

The Input Impedance of a Transmission Line is Time Dependent

Imp

ed

an

ce (

Oh

ms)

TimeMany round trip time of flights

open

Round trip time of flight

Characteristic impedance

Page 6: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -11Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

“…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

Slide -12Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

2nd topic: Differential Impedance

• What is differential impedance and how does coupling affect it?

Difference signal

Page 7: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -13Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Differential mode

Common mode

A Secret to Minimize Confusion About Differential Impedance

ThinkThink::

Differential signalsDifferential signals

Common signalsCommon signals

Odd modeOdd mode

Even modeEven mode

Slide -14Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Essential Principle

Differential impedance is the instantaneous impedance the

differential signal sees

Page 8: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -15Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

The Differential Signal

What is the impedance the difference signal sees?What is the impedance the difference signal sees?

V = 0v1vV = 1v0v

Differential signal

1

2

Difference voltage = 2v : -1v +1v

-1

+1

Slide -16Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Zdiff

Differential Impedance and Series Impedances

What is the equivalent impedance between the two signal lines?

Zdiff = Z0 + Z0

Zdiff = 2 x Z0

with no coupling:with no coupling:

Z0 Z0

What happens to the impedance of one line when we turn on coupling?

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Slide -17Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Other Line Is Tied Low

Z0, Second Trace Pegged Low

40

42

44

46

48

50

52

54

56

58

0 5 10 15 20 25 30 35 40 45 50

Edge to Edge Spacing Between the Traces (mils)

Sin

gle

-En

ded

Im

pe

dan

ce (O

hm

s)

Z0, Second Trace Pegged Low

Slide -18Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Other Line Driven Opposite

40

42

44

46

48

50

52

54

56

58

0 5 10 15 20 25 30 35 40 45 50

Edge to Edge Spacing Between the Traces (mils)

Sin

gle

-Ended Im

pedance (O

hm

s)

Z0, Second Trace Pegged Low

Z0, Both Traces Driven Opposite

return

+1 v -1 v

Vdiff = V1 – V2

ODD MODE

Page 10: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -19Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Relating the Modes’ Impedance to the Impedance the Signals See

ZoddZodd

Zdifferential

oddaldifferenti Zx2Z =

What is the equivalent impedance between the two signal lines?

with coupling:with coupling:

As coupling increases, differential impedance will: _______________decreasedecrease

Slide -20Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

What’s Inductance?

Page 11: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -21Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Deficiencies with Text Book Definitions

• Too mathematical to provide insight

• Deals with coils, not traces on a board

Slide -22Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Inductance Principles -1

photo source: Halliday and Resnick, Physics, 1962

wire carrying a current

Rings of magnetic field lines are Rings of magnetic field lines are around all current carrying around all current carrying

conductorsconductors

What influences the total number of rings of field lines?

Right hand rule

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Slide -23Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

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 itthrough it

Units: Webers/amp = Henry

nH more common

Many flavors of inductance:

self self mutualmutual

loop loop partialpartial

total, net or effectivetotal, net or effective

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

Slide -24Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

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

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Slide -25Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Most Important Principle (#3) of Inductance

1831 Christmas lecture to the Royal Society:

Faraday demonstrates “switching noise”

Michael Faraday's discovery:

Induction: dB/dt V I

ChangingChanging magnetic field

lines around a conductor

induce a voltage, which

drives a current.

V I B ?B V

Slide -26Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Summary

• Why do we care?

• Specific examples:

Characteristic Impedance

Differential Impedance

Inductance

• Got your own? Send me a note

Page 14: Bogatin: 3 Confusing Topics Slide -1web.mst.edu/~jfan/slides/Bogatin1.pdf · Bogatin: 3 Confusing Topics Slide -18 IEEE EMC Distinguished Lecturer Series Other Line Driven Opposite

Slide -27Bogatin: 3 Confusing Topics

IEEE EMC Distinguished Lecturer Series

Thanks for listening!