The Ground Myth Dr. Bruce Archambeault IBM Distinguished Engineer - - PowerPoint PPT Presentation

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The Ground Myth Dr. Bruce Archambeault IBM Distinguished Engineer - - PowerPoint PPT Presentation

The Ground Myth Dr. Bruce Archambeault IBM Distinguished Engineer IEEE Fellow IBM Research Triangle Park, NC Barch@us.ibm.com October 2007 IEEE IEEE Outline Electromagnetics Skin Effect Inductance Ground


slide-1
SLIDE 1

The “Ground” Myth

  • Dr. Bruce Archambeault

IBM Distinguished Engineer IEEE Fellow

IBM Research Triangle Park, NC Barch@us.ibm.com October 2007

IEEE IEEE

slide-2
SLIDE 2

October 2007

  • Dr. Bruce Archambeault

2

Outline

  • Electromagnetics
  • Skin Effect
  • Inductance
  • Ground
  • Return Current Path
slide-3
SLIDE 3

October 2007

  • Dr. Bruce Archambeault

3

Electromagnetics

In the Beginning

  • Electric and Magnetic effects not

connected

  • Electric and magnetic effects were due to

‘action from a distance’

  • Faraday was the 1st to propose a

relationship between electric lines of force and time-changing magnetic fields

– Faraday was very good at experiments and ‘figuring out’ how things work

slide-4
SLIDE 4

October 2007

  • Dr. Bruce Archambeault

4

Maxwell

  • Maxwell was

impressed with Faraday’s ideas

  • Discovered the

mathematical link between the “electro” and the “magnetic”

  • Scotland’s greatest

contribution to the world (next to Scotch)

slide-5
SLIDE 5

October 2007

  • Dr. Bruce Archambeault

5

Maxwell’s Equations – Differential Form

t B E t D J H ∂ ∂ ∂ ∂ − = × ∇ + = × ∇

A difference in Magnetic Field across a small piece of space A difference in Electric Field across a small piece of space A change in Electric Flux Density with respect to time A change in Magnetic Flux Density with respect to time

slide-6
SLIDE 6

October 2007

  • Dr. Bruce Archambeault

6

Maxwell’s Equations are not Hard!

  • Change in H-field across space ¡ Change

in E-field (at that point) with time

  • Change in E-field across space ¡ Change

in H-field (at that point) with time

  • (Roughly speaking, and ignoring

constants)

slide-7
SLIDE 7

October 2007

  • Dr. Bruce Archambeault

7

Current Flow

  • Most important concept of EMC
  • Current flow through metal changes as

frequency increases

  • DC current

– Uses entire conductor – Only resistance inhibits current

  • High Frequency

– Only small part of conductor (near surface) is used – Resistance is small part of current inhibitor – Inductance is major part of current inhibitor

slide-8
SLIDE 8

October 2007

  • Dr. Bruce Archambeault

8

Skin Depth

  • High frequency current flows only near the

metal surface at high frequencies

Frequency Skin Depth Skin Depth 60 Hz 260 mils 8.5 mm 1 KHz 82 mils 2.09 mm 10 KHz 26 mils 0.66 mm 100 KHz 8.2 mils 0.21 mm 1 MHz 2.6 mils 0.066 mm 10 MHz 0.82 mils 0.021 mm 100 MHz 0.26 mils 0.0066 mm 1 GHz 0.0823 mils 0.0021 mm

µσ π δ f 1 =

slide-9
SLIDE 9

October 2007

  • Dr. Bruce Archambeault

9

Current Migrates to Outer Portions of the Conductor at High Frequencies

Resistance is determined by the area of the copper conductor actually used at each frequency!

slide-10
SLIDE 10

October 2007

  • Dr. Bruce Archambeault

10

S21 Skin Effect Loss ONLY-- Comparison for Microstrip (1 cm Long) Various Widths -- 50 ohms (FR4, 4.2, 0.021) Trace Thickness = 0.6mil

  • 1
  • 0.9
  • 0.8
  • 0.7
  • 0.6
  • 0.5
  • 0.4
  • 0.3
  • 0.2
  • 0.1

0.1 1 10 100 Frequency (GHz) Loss (dB) 1 Mil Wide uStrip 2 Mil Wide uStrip 4 Mil Wide uStrip 6 Mil Wide uStrip 8 Mil Wide uStrip

slide-11
SLIDE 11

October 2007

  • Dr. Bruce Archambeault

11

S21 Dielectric Loss ONLY-- Comparison for Microstrip (1 cm Long) Various Widths -- 50 ohms (FR4, 4.2, 0.021) Trace Thickness = 0.6mil

  • 1
  • 0.9
  • 0.8
  • 0.7
  • 0.6
  • 0.5
  • 0.4
  • 0.3
  • 0.2
  • 0.1

0.1 1 10 100 Frequency (GHz) Loss (dB) 1 Mil Wide uStrip 2 Mil Wide uStrip 4 Mil Wide uStrip 6 Mil Wide uStrip 8 Mil Wide uStrip

slide-12
SLIDE 12

October 2007

  • Dr. Bruce Archambeault

12 S21 Loss Comparison Between Stripline and Microstrip (1 cm Long) 6 mil wide -- 50 ohms (FR4, 4.2, 0.021) Trace Thickness = 0.6mil

  • 2
  • 1.8
  • 1.6
  • 1.4
  • 1.2
  • 1
  • 0.8
  • 0.6
  • 0.4
  • 0.2

0.1 1 10 100 Frequency (GHz) S21 Mag (dB) 6 mil Wide uStrip 6 mil Wide StripLine

slide-13
SLIDE 13

October 2007

  • Dr. Bruce Archambeault

13 S21 Loss Comparison for 6 Mil Wide Microstrip Loss (1 cm Long) Various Dielectric Loss -- 50 ohms (FR4, 4.2) Trace Thickness = 0.6mil

  • 1
  • 0.9
  • 0.8
  • 0.7
  • 0.6
  • 0.5
  • 0.4
  • 0.3
  • 0.2
  • 0.1

0.1 1 10 100 Frequency (GHz) S21 Mag (dB) Skin Only Diel (.010) Only Diel (.021) Only Diel (.029) Only Diel (.021) + Skin

slide-14
SLIDE 14

October 2007

  • Dr. Bruce Archambeault

14

At High Frequencies

  • Resistive loss and dielectric loss are

present

  • Inductance will usually dominate
slide-15
SLIDE 15

October 2007

  • Dr. Bruce Archambeault

15

Inductance

  • Current flow through metal =>

inductance!

  • Fundamental element in EVERYTHING
  • Loop area first order concern
  • Inductive impedance increases with

frequency and is MAJOR concern at high frequencies

fL X L π 2 =

slide-16
SLIDE 16

October 2007

  • Dr. Bruce Archambeault

16

Current Loop => Inductance

Courtesy of Elya Joffe

slide-17
SLIDE 17

October 2007

  • Dr. Bruce Archambeault

17

Inductance Definition

  • Faraday’s Law

∫ ∫∫

⋅ ∂ ∂ − = ⋅ S d t B dl E

t B A V ∂ ∂ − =

V B Area = A

  • For a simple rectangular loop

The minus sign means that the induced voltage will work against the current that

  • riginally created the magnetic field!
slide-18
SLIDE 18

October 2007

  • Dr. Bruce Archambeault

18

Self Inductance

  • Isolated circular loop

        − ≈ 2 8 ln r a a L µ

        + − + − + + + + =

2 2

1 1 2 1 1 2 1 1 ln 2 p p p p p a L π µ

  • Isolated rectangular loop

Note that inductance is directly influenced by loop AREA and only less influenced by conductor size!

radius wire side

  • f

length p =

slide-19
SLIDE 19

October 2007

  • Dr. Bruce Archambeault

19

Partial Inductance

  • Simply a way to break the overall loop

into pieces in order to find total inductance

L3 L4 L2 L1

L total=Lp11+ Lp22 + Lp33 + Lp44 - 2Lp13 - 2Lp24

slide-20
SLIDE 20

October 2007

  • Dr. Bruce Archambeault

20

Decoupling Capacitor Mounting

  • Keep as to planes as close to capacitor

pads as possible

Height above Planes Via Separation

Inductance Depends

  • n Loop AREA
slide-21
SLIDE 21

October 2007

  • Dr. Bruce Archambeault

21

Important Points About Inductance

  • Inductance is everywhere
  • Loop area most important
  • Inductance is everywhere
slide-22
SLIDE 22

October 2007

  • Dr. Bruce Archambeault

22

‘Ground’

  • Ground is a place where

potatoes and carrots thrive!

  • ‘Earth’ or ‘reference’ is more descriptive
  • Original use of “GROUND”
  • Inductance is everywhere

fL X L π 2 =

slide-23
SLIDE 23

October 2007

  • Dr. Bruce Archambeault

23

What we Really Mean when we say ‘Ground’

  • Signal Reference
  • Power Reference
  • Safety Earth
  • Chassis Shield Reference
slide-24
SLIDE 24

October 2007

  • Dr. Bruce Archambeault

24

‘Ground’ is NOT a Current Sink!

  • Current leaves a driver on a

trace and must return (somehow) to its source

  • This seems basic, but it is often

forgotten, and is most often the cause of EMC problems

slide-25
SLIDE 25

October 2007

  • Dr. Bruce Archambeault

25

‘Grounding’ Needs Low Impedance at Highest Frequency

  • Steel Reference Plate

– 4 milliohms/sq @ 100KHz – 40 milliohms/sq @ 10 MHz – 400 milliohms/sq @ 1 GHz

  • A typical via is about 2

nH

– @ 100 MHz Z = 1.3 ohms – @ 500 MHz Z = 6.5 ohms – @ 1000 MHz Z = 13 ohms – @ 2000 MHz Z = 26 ohms

slide-26
SLIDE 26

October 2007

  • Dr. Bruce Archambeault

26

Single-point ‘Ground’? Vs Multi-point ‘Ground’?

  • Which do I want?
  • Which do I get?
slide-27
SLIDE 27

October 2007

  • Dr. Bruce Archambeault

27

Single Point ‘Ground’ Myth

  • At high frequencies, inductance makes

this impossible!

  • At high frequencies, parasitic capacitance

makes this impossible!

  • Depends on the amount of ‘Ground’ error

your system can stand…...

slide-28
SLIDE 28

October 2007

  • Dr. Bruce Archambeault

28

Single-Point Ground Concept

GND via

Board A Board B Metal Enclosure

GND via GND via GND via GND via GND planes

slide-29
SLIDE 29

October 2007

  • Dr. Bruce Archambeault

29

Reality Overcomes Single-Point Ground Intentions

GND via

Board A Board B Metal Enclosure

GND via GND via GND via GND via GND planes

slide-30
SLIDE 30

October 2007

  • Dr. Bruce Archambeault

30

Where did the Term “GROUND” Originate?

  • Original Teletype connections
  • Lightning Protection
slide-31
SLIDE 31

October 2007

  • Dr. Bruce Archambeault

31

Ground/Earth Teletype Receiver Teletype Transmitter

slide-32
SLIDE 32

October 2007

  • Dr. Bruce Archambeault

32

Ground/Earth Teletype Receiver Teletype Transmitter

slide-33
SLIDE 33

October 2007

  • Dr. Bruce Archambeault

33

Lightning striking house

FIG 7 Lightning

slide-34
SLIDE 34

October 2007

  • Dr. Bruce Archambeault

34

Lightning effect without rod

slide-35
SLIDE 35

October 2007

  • Dr. Bruce Archambeault

35

Lightning effect with rod

Lightning rod Lightning

slide-36
SLIDE 36

October 2007

  • Dr. Bruce Archambeault

36

What we Really Mean when we say ‘Ground’

  • Signal Reference
  • Power Reference
  • Safety Earth
  • Chassis Shield Reference

Circuit “Ground” Chassis “Ground” Digital “Ground”

D

Analog “Ground”

A

slide-37
SLIDE 37

October 2007

  • Dr. Bruce Archambeault

37

slide-38
SLIDE 38

October 2007

  • Dr. Bruce Archambeault

38

Schematic with Return Current Shown

IC1 IC2 IC3 Return currents on ground Signal trace currents

slide-39
SLIDE 39

October 2007

  • Dr. Bruce Archambeault

39

Actual Current Return is 3-Dimensional

Ground Layer Signal Trace IC Ground Vias Ground Layer Signal Trace IC Ground Via BOARD STACK UP: Ground Layer Signal Trace CURRENT LOCATION:

slide-40
SLIDE 40

October 2007

  • Dr. Bruce Archambeault

40

Low Frequency Return Currents Take Path of Least Resistance

Ground Plane Driver Receiver

slide-41
SLIDE 41

October 2007

  • Dr. Bruce Archambeault

41

High Frequency Return Currents Take Path of Least Inductance

Ground Plane Driver Receiver

slide-42
SLIDE 42

October 2007

  • Dr. Bruce Archambeault

42

Microstrip Transmission Line Stripline Transmission Line

Dielectric Reference Planes Signal Trace

Traces/nets over a Reference Plane

slide-43
SLIDE 43

October 2007

  • Dr. Bruce Archambeault

43

Signal Traces Reference Planes (Power, “Ground”, etc.)

Traces/nets and Reference Planes in Many Layer Board Stackup

slide-44
SLIDE 44

October 2007

  • Dr. Bruce Archambeault

44

Microstrip Electric/Magnetic Field Lines

(8mil wide trace, 8 mils above plane, 65 ohm)

Electric Field Lines

Vcc

slide-45
SLIDE 45

October 2007

  • Dr. Bruce Archambeault

45

Microstrip Electric/Magnetic Field Lines

Common Mode 8 mil wide trace, 8 mils above plane, 65/115 ohm)

Electric Field Lines

Vcc

slide-46
SLIDE 46

October 2007

  • Dr. Bruce Archambeault

46

Microstrip Electric/Magnetic Field Lines

Differential Mode 8 mil wide trace, 8 mils above plane, 65/115 ohm)

Electric Field Lines

Vcc

slide-47
SLIDE 47

October 2007

  • Dr. Bruce Archambeault

47

Electric/Magnetic Field Lines

Symmetrical Stripline

Vcc GND

slide-48
SLIDE 48

October 2007

  • Dr. Bruce Archambeault

48

Electric/Magnetic Field Lines

Symmetrical Stripline (Differential)

Vcc GND

slide-49
SLIDE 49

October 2007

  • Dr. Bruce Archambeault

49

Electric/Magnetic Field Lines

Asymmetrical Stripline

Vcc GND

slide-50
SLIDE 50

October 2007

  • Dr. Bruce Archambeault

50

Electric/Magnetic Field Lines

Asymmetrical Stripline (Differential)

slide-51
SLIDE 51

October 2007

  • Dr. Bruce Archambeault

51

What About Pseudo-Differential Nets?

  • So-called differential traces are NOT truly

differential

– Two complementary single-ended drivers

  • Relative to ‘ground’

– Receiver is differential

  • Senses difference between two nets (independent
  • f ‘ground’)
  • Provides good immunity to common mode noise
  • Good for signal quality/integrity
slide-52
SLIDE 52

October 2007

  • Dr. Bruce Archambeault

52

Pseudo-Differential Nets Current in Nearby Plane

  • Balanced/Differential currents have

matching current in nearby plane

– No issue for discontinuities

  • Any unbalanced (common mode) currents

have return currents in nearby plane that must return to source!

– All normal concerns for single-ended nets apply!

slide-53
SLIDE 53

October 2007

  • Dr. Bruce Archambeault

53

Pseudo-Differential Nets

  • Not really ‘differential’, since more closely

coupled to nearby plane than each other

  • Slew and rise/fall variation cause common

mode currents!

slide-54
SLIDE 54

October 2007

  • Dr. Bruce Archambeault

54 Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec rise/fall time

0.2 0.4 0.6 0.8 1 1.2 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (nsec) Voltage Complementary -- Line1 Complementary -- Line 2 Skew=2ps Skew=6ps Skew = 10ps Skew = 20ps Skew = 30ps Skew =40ps Skew =50ps Skew =60ps

slide-55
SLIDE 55

October 2007

  • Dr. Bruce Archambeault

55 Common Mode Voltage From Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec rise/fall time

  • 0.6
  • 0.4
  • 0.2

0.2 0.4 0.6 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (nsec) Voltage Balanced Skew=2ps Skew=6ps Skew =10ps Skew =20ps Skew =30ps Skew =40ps Skew =50ps

slide-56
SLIDE 56

October 2007

  • Dr. Bruce Archambeault

56 Common Mode Current From Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec Rise/fall Time

  • 100
  • 80
  • 60
  • 40
  • 20

20 40 60 80 100 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (nsec) Level (ma) Balanced Skew=2ps Skew=6ps Skew =10ps Skew =20ps Skew =30ps Skew =40ps Skew =50ps Skew =60ps

slide-57
SLIDE 57

October 2007

  • Dr. Bruce Archambeault

57 Common Mode Current From Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec Rise/fall Time

50 60 70 80 90 100 110 120 130 140 150 1.E+08 1.E+09 1.E+10 1.E+11 Frequency (Hz) Level (dBuA) Skew=2ps Skew=6ps Skew =10ps Skew =20ps Skew =30ps Skew =40ps Skew =50ps Skew =60ps

slide-58
SLIDE 58

October 2007

  • Dr. Bruce Archambeault

58 Differential Voltage Pulse with Rise/Fall Variation/Unbalance 1 Gbit/sec with 95 psec Nominal Rise/Fall Time

0.2 0.4 0.6 0.8 1 1.2 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns)

Level (volts)

Original Pulse rise=95ps Complementary Pulse Rise=90ps Complementary Pulse Rise=80ps Complementary Pulse Rise=105ps Complementary Pulse Rise=115ps

slide-59
SLIDE 59

October 2007

  • Dr. Bruce Archambeault

59 Common Mode Voltage From Differential Voltage Pulse with Various Rise/Fall Unbalance 1 Gbit/sec with 95 psec Nominal Rise/Fall Time

  • 0.2
  • 0.15
  • 0.1
  • 0.05

0.05 0.1 0.15 0.2 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) Voltage Complementary Pulse Rise=90ps Complementary Pulse Rise=80ps Complementary Pulse Rise=105ps Complementary Pulse Rise=115ps

slide-60
SLIDE 60

October 2007

  • Dr. Bruce Archambeault

60 Common Mode Current From Differential Voltage Pulse with Various Rise/Fall Unbalance 1 Gbit/sec with 95 psec Nominal Rise/fall Time

  • 60
  • 40
  • 20

20 40 60 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) Current (ma) Complementary Pulse Rise=90ps Complementary Pulse Rise=80ps Complementary Pulse Rise=105ps Complementary Pulse Rise=115ps

slide-61
SLIDE 61

October 2007

  • Dr. Bruce Archambeault

61 Common Mode Current From Differential Voltage Pulse with Various Rise/Fall Unbalance 1 Gbit/sec with Nominal 95 psec Rise/fall Time

50 55 60 65 70 75 80 85 90 1.E+08 1.E+09 1.E+10 1.E+11 Frequency (Hz) Level (dBua) Complementary Pulse Rise=90ps Complementary Pulse Rise=80ps Complementary Pulse Rise=105ps Complementary Pulse Rise=115ps

slide-62
SLIDE 62

October 2007

  • Dr. Bruce Archambeault

62

Pseudo-Differential Net Summary

  • Small amounts of skew can cause

significant common mode current

  • Small amount of rise/fall time deviation

can cause significant amount of common mode current

  • Discontinuities (vias, crossing split planes,

etc) and convert significant amount of differential current into common mode current

slide-63
SLIDE 63

October 2007

  • Dr. Bruce Archambeault

63

Return Current vs.. “Ground”

  • For high frequency signals, “Ground” is a

concept that does not exist

  • The important question is “where does

the return current flow?”

slide-64
SLIDE 64

October 2007

  • Dr. Bruce Archambeault

64

Referencing Nets (Where does the Return Current Flow??)

  • Microstrip/Stripline across split in

reference plane

  • Microstrip/Stripline through via (change

reference planes)

  • Mother/Daughter card
slide-65
SLIDE 65

October 2007

  • Dr. Bruce Archambeault

65

  • Don’t Cross Splits with Critical Signals!!!

– Bad practice – Stitching capacitor required across split to allow return current flow

  • must be close to crossing
  • must have low inductance
  • limited frequency effect --- due to inductance

– Major source of Common Mode current!

Microstrip/Stripline Across Split in Reference Plane

slide-66
SLIDE 66

October 2007

  • Dr. Bruce Archambeault

66

Splits in Reference Plane

  • Power planes often have splits
  • Return current path interrupted
  • Consider spectrum of clock signal
  • Consider stitching capacitor

impedance

  • High frequency harmonics not

returned directly

slide-67
SLIDE 67

October 2007

  • Dr. Bruce Archambeault

67

Split Reference Plane Example

PWR GND

slide-68
SLIDE 68

October 2007

  • Dr. Bruce Archambeault

68

Split Reference Plane Example

With Stitching Capacitors

PWR GND

Stitching Capacitors Allow Return current to Cross Splits ???

slide-69
SLIDE 69

October 2007

  • Dr. Bruce Archambeault

69

Capacitor Impedance

Measured Impedance of .01 uf Capacitor

0.1 1.0 10.0 100.0 1.E+06 1.E+07 1.E+08 1.E+09 Frequency (Hz) Impednace (ohms)

slide-70
SLIDE 70

October 2007

  • Dr. Bruce Archambeault

70

Frequency Domain Amplitude of Intentional Current Harmonic Amplitude From Clock Net

40 60 80 100 120 140 160 200 400 600 800 1000 1200 1400 1600 1800 2000 freq (MHz) level (dBuA)

slide-71
SLIDE 71

October 2007

  • Dr. Bruce Archambeault

71

MoM Microstrip Model Current Distribution Example

slide-72
SLIDE 72

October 2007

  • Dr. Bruce Archambeault

72

MoM Microstrip Model Current Distribution Example

slide-73
SLIDE 73

October 2007

  • Dr. Bruce Archambeault

73

Emissions From Board

  • Far field emissions not important unless it

is an unshielded product

  • Near field emissions above board ARE

important

  • Example of emissions from board with

critical net crossing split reference plane

slide-74
SLIDE 74

October 2007

  • Dr. Bruce Archambeault

74

Near Field Radiation from Microstrip on Board with Split in Reference Plane

Comparison of Maximum Radiated E-Field for Microstrip With and without Split Ground Reference Plane

20 30 40 50 60 70 80 90 100 110 120 10 100 1000 Frequency (MHz) Maximum Radiated E-Field (dBuv/m) No-Split Split

slide-75
SLIDE 75

October 2007

  • Dr. Bruce Archambeault

75

With “Perfectly Connected” Stitching Capacitors Across Split

Comparison of Maximum Radiated E-Field for Microstrip With and without Split Ground Reference Plane and Stiching Capacitors

20 30 40 50 60 70 80 90 100 110 120 10 100 1000 Frequency (MHz) Maximum Radiated E-Field (dBuv/m) No-Split Split Split w/ one Cap Split w/ Two Caps

slide-76
SLIDE 76

October 2007

  • Dr. Bruce Archambeault

76

Stitching Caps with Via Inductance

Comparison of Maximum Radiated E-Field for Microstrip With and without Split Ground Reference Plane and Stiching Capacitors

20 30 40 50 60 70 80 90 100 110 120 10 100 1000 Frequency (MHz) Maximum Radiated E-Field (dBuv/m) No-Split Split Split w/ one Cap Split w/ Two Caps Split w/One Real Cap Split w/Two Real Caps

slide-77
SLIDE 77

October 2007

  • Dr. Bruce Archambeault

77 Example of Common-Mode Noise Voltage Across Split Plane

  • Vs. Stitching Capacitor Distance to Crossing Point

5 10 15 20 25 200 400 600 800 1000 1200 1400 1600 1800 2000 Distance (mils) Gap Voltage

100MHz 200MHz 300MHz 400MHz 500MHz 600MHz 700MHz 800MHz 900MHz 1000MHz

slide-78
SLIDE 78

October 2007

  • Dr. Bruce Archambeault

78

Are Stitching Capacitors Effective ???

  • YES, at low frequencies
  • No, at high frequencies
  • Need to limit the high frequency current

spectrum

  • Need to avoid split crossings with ALL

critical signals

slide-79
SLIDE 79

October 2007

  • Dr. Bruce Archambeault

79

Pin Field Via Keepouts??

Return Current must go around entire keep out area --- just as bad as a slot Return current path deviation minimal s d Recommend s/d > 1/3

slide-80
SLIDE 80

October 2007

  • Dr. Bruce Archambeault

80

Changing Reference Planes

Six-Layer PCB Stackup Example

Signal Layer Signal Layer Signal Layer Signal Layer Plane Plane

slide-81
SLIDE 81

October 2007

  • Dr. Bruce Archambeault

81

Microstrip/Stripline through via (change reference planes)

Trace Via

slide-82
SLIDE 82

October 2007

  • Dr. Bruce Archambeault

82

How can the Return Current Flow When Signal Line Goes Through Via??

What happens to Return Current in this Region?

Return Current

slide-83
SLIDE 83

October 2007

  • Dr. Bruce Archambeault

83

How can the Return Current Flow When Signal Line Goes Through Via??

  • Current can NOT go from one side of the

plane to the other through the plane

– skin depth

  • Current must go around plane at via hole,

through decoupling capacitor, around second plane at the second via hole!

  • Use displacement current between planes
slide-84
SLIDE 84

October 2007

  • Dr. Bruce Archambeault

84

Return Current without Intentional Path

GND PWR

slide-85
SLIDE 85

October 2007

  • Dr. Bruce Archambeault

85

Return Current Across Reference Plane Change

With Decoupling Capacitor (on Top)

Return Current Decoupling Capacitor Reference Planes Displacement Current

Common-Mode Current

slide-86
SLIDE 86

October 2007

  • Dr. Bruce Archambeault

86

RF Current @ 700 MHz with One Capacitor 0.5” from Via

slide-87
SLIDE 87

October 2007

  • Dr. Bruce Archambeault

87

RF Current @ 700 MHz with One Capacitor 0.5” from Via

(expanded view)

slide-88
SLIDE 88

October 2007

  • Dr. Bruce Archambeault

88

Bad

Signal Layer Signal Layer Signal Layer Signal Layer Reference Plane Reference Plane

Bad

Signal Layer Signal Layer Signal Layer Signal Layer Reference Plane Reference Plane

Good

Signal Layer Signal Layer Signal Layer Signal Layer Reference Plane Reference Plane

Possible Routing Options

Six-Layer Board

slide-89
SLIDE 89

October 2007

  • Dr. Bruce Archambeault

89

Compromise Routing Option for Many Layer Boards

Good Compromise

Reference Plane Gnd Vcc1

Lot’s of Decoupling caps near ASIC

slide-90
SLIDE 90

October 2007

  • Dr. Bruce Archambeault

90

Typical Driver/Receiver Currents

switch IC load IC driver VDC GND CL VCC Z0, vp GND IC load IC driver VCC VCC charge

logic 0-to-1

Z0, vp IC load IC driver GND VCC 0 V discharge

logic 1-to-0

Z0, vp

slide-91
SLIDE 91

October 2007

  • Dr. Bruce Archambeault

91

Suppose The Trace is Routed Next to Power (not Gnd)

Vcc1 Vcc1 “Fuzzy” Return Path Area “Fuzzy” Return Path Area Return Path Options:

  • - Decoupling Capacitors
  • - Distributed Displacement Current

TEM Transmission Line Area

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October 2007

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92

Suppose The Trace is Routed Next to a DIFFERENT Power (not Gnd)

Return Path Options:

  • - Decoupling Capacitors ??? May not be any nearby!!
  • - Distributed Displacement Current – Increased current spread!!!

Vcc1 Vcc2 “Fuzzy” Return Path Area “Fuzzy” Return Path Area TEM Transmission Line Area

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SLIDE 93

October 2007

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93

Via Summary

Route critical signals on either side of ONE reference plane Drop critical signal net to selected layer close to driver/receiver

Many decoupling capacitors to help return currents

Do NOT change reference planes on critical nets unless ABSOLUTELY NECESSARY!! Make sure at least 2 decoupling capacitors within 0.2” of via with critical signals

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SLIDE 94

October 2007

  • Dr. Bruce Archambeault

94

Mother/Daughter Board Connector Crossing

  • Critical Signals must be referenced to

same plane on both sides of the connector

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SLIDE 95

October 2007

  • Dr. Bruce Archambeault

95

Mother/Daughter Board Connector Crossing

Connector

Signal Path

GND PWR Signal Signal PWR GND Signal Signal

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  • Dr. Bruce Archambeault

96

Return Current from Improper Referencing Across Connector

Connector

De-cap Signal Path

GND PWR Signal Signal PWR GND Signal Signal

Return Path De-cap Displacement Current

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October 2007

  • Dr. Bruce Archambeault

97

Return Current from Proper Referencing Across Connector

PWR GND Signal Signal

Connector

Signal Path

GND PWR Signal Signal

Return Path

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October 2007

  • Dr. Bruce Archambeault

98

Board-to-Board Differential Pair Issues

C

  • n

n e c t

  • r

P C B P l a n e 1 PCB Plane 2 M i c r

  • s

t r i p Microstrip V Ground-to-Ground noise

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SLIDE 99

October 2007

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99

Example Measured Differential Individual Signal-to-GND

Individual Differential Signals ADDED Common Mode Noise 170 mV P-P 500 mV P-P (each)

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SLIDE 100

October 2007

  • Dr. Bruce Archambeault

100

Measured GND-to-GND Voltage

205 mV P-P

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SLIDE 101

October 2007

  • Dr. Bruce Archambeault

101

Antenna Structures

Dipole antenna PCB GND planes Non-Dipole antenna

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SLIDE 102

October 2007

  • Dr. Bruce Archambeault

102

Pin Assignment Controls Inductance for CM signals

Signal Pin Related Ground Pins 37.17 nH 25.21 nH 16.85 nH 20.97 nH (a) (b) (c) (d)

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SLIDE 103

October 2007

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103

How Many “Ground” Pins Across Connector ???

  • Nothing MAGICAL about “ground”
  • Return current flow!
  • Choose the number of power and “ground”

pins based on the number of signal lines referenced to power or “ground” planes

  • Insure signals are referenced against

same planes on either side of connector

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SLIDE 104

October 2007

  • Dr. Bruce Archambeault

104

Ground Myth Summary

  • THERE IS NO SUCH THING AS

“GROUND”

  • Define which reference type is needed
  • Plan the return current path

– Avoid split reference planes & changing reference planes

  • Differential signals have significant common

mode, and must follow normal EMC rules

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SLIDE 105

October 2007

  • Dr. Bruce Archambeault

105

IEEE IEEE