the ground myth
play

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


  1. High Frequency Return Currents Take Path of Least Inductance Driver Receiver Ground Plane October 2007 Dr. Bruce Archambeault 41

  2. Traces/nets over a Reference Plane Microstrip Transmission Line Signal Trace Reference Planes Dielectric Stripline Transmission Line October 2007 Dr. Bruce Archambeault 42

  3. Traces/nets and Reference Planes in Many Layer Board Stackup Signal Traces Reference Planes (Power, “Ground”, etc.) October 2007 Dr. Bruce Archambeault 43

  4. Microstrip Electric/Magnetic Field Lines (8mil wide trace, 8 mils above plane, 65 ohm) Electric Field Lines Vcc October 2007 Dr. Bruce Archambeault 44

  5. Microstrip Electric/Magnetic Field Lines Common Mode 8 mil wide trace, 8 mils above plane, 65/115 ohm) Electric Field Lines Vcc October 2007 Dr. Bruce Archambeault 45

  6. Microstrip Electric/Magnetic Field Lines Differential Mode 8 mil wide trace, 8 mils above plane, 65/115 ohm) Electric Field Lines Vcc October 2007 Dr. Bruce Archambeault 46

  7. Electric/Magnetic Field Lines Symmetrical Stripline GND Vcc October 2007 Dr. Bruce Archambeault 47

  8. Electric/Magnetic Field Lines Symmetrical Stripline (Differential) GND Vcc October 2007 Dr. Bruce Archambeault 48

  9. Electric/Magnetic Field Lines Asymmetrical Stripline Vcc GND October 2007 Dr. Bruce Archambeault 49

  10. Electric/Magnetic Field Lines Asymmetrical Stripline (Differential) October 2007 Dr. Bruce Archambeault 50

  11. 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 of ‘ground’) • Provides good immunity to common mode noise • Good for signal quality/integrity October 2007 Dr. Bruce Archambeault 51

  12. 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! October 2007 Dr. Bruce Archambeault 52

  13. 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! October 2007 Dr. Bruce Archambeault 53

  14. Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec rise/fall time 1.2 1 0.8 Complementary -- Line1 Complementary -- Line 2 Skew=2ps Voltage 0.6 Skew=6ps Skew = 10ps Skew = 20ps Skew = 30ps 0.4 Skew =40ps Skew =50ps Skew =60ps 0.2 0 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (nsec) October 2007 Dr. Bruce Archambeault 54

  15. Common Mode Voltage From Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec rise/fall time 0.6 Balanced 0.4 Skew=2ps Skew=6ps Skew =10ps Skew =20ps 0.2 Skew =30ps Skew =40ps Skew =50ps Voltage 0 -0.2 -0.4 -0.6 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (nsec) October 2007 Dr. Bruce Archambeault 55

  16. Common Mode Current From Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec Rise/fall Time 100 80 60 Balanced Skew=2ps 40 Skew=6ps Skew =10ps 20 Skew =20ps Level (ma) Skew =30ps 0 Skew =40ps Skew =50ps -20 Skew =60ps -40 -60 -80 -100 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (nsec) October 2007 Dr. Bruce Archambeault 56

  17. Common Mode Current From Differential Voltage Pulse with Skew 1 Gbit/sec with 95 psec Rise/fall Time 150 Skew=2ps 140 Skew=6ps Skew =10ps 130 Skew =20ps Skew =30ps 120 Skew =40ps Skew =50ps Skew =60ps 110 Level (dBuA) 100 90 80 70 60 50 1.E+08 1.E+09 1.E+10 1.E+11 Frequency (Hz) October 2007 Dr. Bruce Archambeault 57

  18. Differential Voltage Pulse with Rise/Fall Variation/Unbalance 1 Gbit/sec with 95 psec Nominal Rise/Fall Time 1.2 1 0.8 Original Pulse rise=95ps Level (volts) Complementary Pulse Rise=90ps Complementary Pulse Rise=80ps 0.6 Complementary Pulse Rise=105ps Complementary Pulse Rise=115ps 0.4 0.2 0 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) October 2007 Dr. Bruce Archambeault 58

  19. 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 Voltage 0 -0.05 Complementary Pulse Rise=90ps -0.1 Complementary Pulse Rise=80ps Complementary Pulse Rise=105ps -0.15 Complementary Pulse Rise=115ps -0.2 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) October 2007 Dr. Bruce Archambeault 59

  20. 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 Current (ma) 0 -20 Complementary Pulse Rise=90ps -40 Complementary Pulse Rise=80ps Complementary Pulse Rise=105ps Complementary Pulse Rise=115ps -60 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) October 2007 Dr. Bruce Archambeault 60

  21. Common Mode Current From Differential Voltage Pulse with Various Rise/Fall Unbalance 1 Gbit/sec with Nominal 95 psec Rise/fall Time 90 85 Complementary Pulse Rise=90ps 80 Complementary Pulse Rise=80ps Complementary Pulse Rise=105ps 75 Complementary Pulse Rise=115ps Level (dBua) 70 65 60 55 50 1.E+08 1.E+09 1.E+10 1.E+11 Frequency (Hz) October 2007 Dr. Bruce Archambeault 61

  22. 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 October 2007 Dr. Bruce Archambeault 62

  23. 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?” October 2007 Dr. Bruce Archambeault 63

  24. 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 October 2007 Dr. Bruce Archambeault 64

  25. Microstrip/Stripline Across Split in Reference Plane • 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! October 2007 Dr. Bruce Archambeault 65

  26. 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 October 2007 Dr. Bruce Archambeault 66

  27. Split Reference Plane Example PWR GND October 2007 Dr. Bruce Archambeault 67

  28. Split Reference Plane Example With Stitching Capacitors Stitching Capacitors Allow Return current to Cross Splits ??? PWR GND October 2007 Dr. Bruce Archambeault 68

  29. Capacitor Impedance Measured Impedance of .01 uf Capacitor 100.0 10.0 Impednace (ohms) 1.0 0.1 1.E+06 1.E+07 1.E+08 1.E+09 Frequency (Hz) October 2007 Dr. Bruce Archambeault 69

  30. Frequency Domain Amplitude of Intentional Current Harmonic Amplitude From Clock Net 160 140 120 level (dBuA) 100 80 60 40 0 200 400 600 800 1000 1200 1400 1600 1800 2000 freq (MHz) October 2007 Dr. Bruce Archambeault 70

  31. MoM Microstrip Model Current Distribution Example October 2007 Dr. Bruce Archambeault 71

  32. MoM Microstrip Model Current Distribution Example October 2007 Dr. Bruce Archambeault 72

  33. 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 October 2007 Dr. Bruce Archambeault 73

  34. 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 120 110 100 Maximum Radiated E-Field (dBuv/m) 90 80 70 No-Split 60 Split 50 40 30 20 10 100 1000 Frequency (MHz) October 2007 Dr. Bruce Archambeault 74

  35. 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 120 110 100 Maximum Radiated E-Field (dBuv/m) 90 80 70 60 No-Split 50 Split Split w/ one Cap 40 Split w/ Two Caps 30 20 10 100 1000 Frequency (MHz) October 2007 Dr. Bruce Archambeault 75

  36. Stitching Caps with Via Inductance Comparison of Maximum Radiated E-Field for Microstrip With and without Split Ground Reference Plane and Stiching Capacitors 120 110 100 Maximum Radiated E-Field (dBuv/m) 90 80 70 60 No-Split Split 50 Split w/ one Cap Split w/ Two Caps 40 Split w/One Real Cap Split w/Two Real Caps 30 20 10 100 1000 Frequency (MHz) October 2007 Dr. Bruce Archambeault 76

  37. Example of Common-Mode Noise Voltage Across Split Plane Vs. Stitching Capacitor Distance to Crossing Point 25 20 15 Gap Voltage 100MHz 200MHz 300MHz 10 400MHz 500MHz 600MHz 700MHz 5 800MHz 900MHz 1000MHz 0 0 200 400 600 800 1000 1200 1400 1600 1800 2000 Distance (mils) October 2007 Dr. Bruce Archambeault 77

  38. 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 October 2007 Dr. Bruce Archambeault 78

  39. Pin Field Via Keepouts?? s d Return current path Return Current must go around deviation minimal entire keep out area --- just as bad as a slot Recommend s/d > 1/3 October 2007 Dr. Bruce Archambeault 79

  40. Changing Reference Planes Six-Layer PCB Stackup Example Signal Layer Plane Signal Layer Signal Layer Plane Signal Layer October 2007 Dr. Bruce Archambeault 80

  41. Microstrip/Stripline through via (change reference planes) Via Trace October 2007 Dr. Bruce Archambeault 81

  42. How can the Return Current Flow When Signal Line Goes Through Via?? What happens to Return Current in this Region? Return Current October 2007 Dr. Bruce Archambeault 82

  43. 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 October 2007 Dr. Bruce Archambeault 83

  44. Return Current without Intentional Path GND PWR October 2007 Dr. Bruce Archambeault 84

  45. Return Current Across Reference Plane Change With Decoupling Capacitor (on Top) Decoupling Capacitor Common-Mode Current Displacement Current Reference Planes Return Current October 2007 Dr. Bruce Archambeault 85

  46. RF Current @ 700 MHz with One Capacitor 0.5” from Via October 2007 Dr. Bruce Archambeault 86

  47. RF Current @ 700 MHz with One Capacitor 0.5” from Via (expanded view) October 2007 Dr. Bruce Archambeault 87

  48. Possible Routing Options Six-Layer Board Bad Signal Layer Reference Plane Signal Layer Signal Layer Reference Plane Signal Layer Bad Signal Layer Reference Plane Signal Layer Signal Layer Reference Plane Signal Layer Good Signal Layer Reference Plane Signal Layer Signal Layer Reference Plane Signal Layer October 2007 Dr. Bruce Archambeault 88

  49. Compromise Routing Option for Many Layer Boards Good Compromise Vcc1 Gnd Reference Plane Lot’s of Decoupling caps near ASIC October 2007 Dr. Bruce Archambeault 89

  50. Typical Driver/Receiver Currents V CC switch IC IC load driver V DC C L Z 0 , v p logic 0-to-1 GND logic 1-to-0 V CC V CC IC load IC load IC IC driver charge discharge driver Z 0 , v p Z 0 , v p V CC 0 V GND GND October 2007 Dr. Bruce Archambeault 90

  51. Suppose The Trace is Routed Next to Power (not Gnd) TEM Transmission V cc1 Line Area V cc1 “Fuzzy” Return “Fuzzy” Return Path Area Path Area Return Path Options: -- Decoupling Capacitors -- Distributed Displacement Current October 2007 Dr. Bruce Archambeault 91

  52. Suppose The Trace is Routed Next to a DIFFERENT Power (not Gnd) TEM Transmission V cc1 Line Area V cc2 “Fuzzy” Return “Fuzzy” Return Path Area Path Area Return Path Options: -- Decoupling Capacitors ??? May not be any nearby !! -- Distributed Displacement Current – Increased current spread !!! October 2007 Dr. Bruce Archambeault 92

  53. 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 October 2007 Dr. Bruce Archambeault 93

  54. Mother/Daughter Board Connector Crossing • Critical Signals must be referenced to same plane on both sides of the connector October 2007 Dr. Bruce Archambeault 94

  55. Mother/Daughter Board Connector Crossing Signal Signal PWR GND Connector Signal Path Signal GND PWR Signal October 2007 Dr. Bruce Archambeault 95

  56. Return Current from Improper Referencing Across Connector Signal Signal GND PWR Displacement De-cap Current Connector Return Path Signal Path De-cap Signal GND PWR Signal October 2007 Dr. Bruce Archambeault 96

  57. Return Current from Proper Referencing Across Connector Signal Signal GND PWR Return Path Connector Signal Path Signal GND PWR Signal October 2007 Dr. Bruce Archambeault 97

  58. Board-to-Board Differential Pair Issues PCB Plane 2 C Microstrip o n n e c t o r M i c r o s t r i p V P C B Ground-to-Ground P l a n e 1 noise October 2007 Dr. Bruce Archambeault 98

  59. Example Measured Differential Individual Signal-to-GND Individual Differential 500 mV P-P (each) Signals ADDED Common Mode Noise 170 mV P-P October 2007 Dr. Bruce Archambeault 99

  60. Measured GND-to-GND Voltage 205 mV P-P October 2007 Dr. Bruce Archambeault 100

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