数字电路的噪声和布局.docx

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数字电路的噪声和布局.docx

数字电路的噪声和布局

南京师范大学电气与电子工程学院教学授课计划60

 

Chp.8DIGITALCIRCUITNOISEANDLAYOUT

 

(数字电路的噪声和布局)

 

本章学习要求:

了解如下主要概念、方法和内容。

 

1.时域与频域关系,模拟与数字电路关系等

 

2.数字逻辑器件的噪声(内部噪声源分析)

 

3.数字电路接地系统噪声(接地线电感的影响;减小电感的方法,实际数字电路

接地系统考虑等)

 

4.电源分配(电源解偶解偶电容类型与数值,电解解偶电容,解偶电容的配置)

 

5.噪声电压控制目标与测量

 

§8.1Introduction

1.Adigitalsystemisalsoaradio-frequency(RF)systemwithnoiseandinterferencepotential

2.SmallICdigitallogicgates(数字逻辑门电路),whichdrawonlyafewmAcurrent,canalsobeaseriousnoisesourcefor

(1)highswitchingspeed

(2)combinedwithinductanceoftheconductor

Thenoisesourcewhencurrentchangethroughaninductor

VLdidt

Example:

“on”state,I=5mA,

“off”state,I=1mA

Soi4mA,howevert2ns!

!

Alsoifapowersupplywiringhasaninductanceof500mH,L=500mH

南京师范大学电气与电子工程学院教学授课计划61

Thenoisevoltageacrossthepowersupplywiringwhengatechangestate

di

VNL

dt

 

500mH

 

=1V!

4mA

2ns

Realizingthepowersupplyvoltageofthissystemisonly5V,therefore

 

VN%1V%20%

V5V

 

3.Chp.8andChp.9willdiscusstechniquestominimize

(1)internalnoisegeneration

(2)radiatedemission

 

§8.2FrequencyVersusTimeDomain频(域与时域关系)

 

1.Thoughdigitalcircuitworksintimedomain,becauselegalrequirementontheemissionarespecifiedinfrequency-domain,so“f”versus“t”shouldbeknown

2.Bandwidthofadigitalsystem

Definition:

logicpulsebandwidthshouldbethepoint,wheretheenergycontentintheharmonic(consistasquarewave)isnegligiblewhenbeyondthispoint.OrthebreakpointwheretheFouriercoefficientstarttodecayat40dB/decade

 

BW

1

tr

 

tr:

pulserisetimee.g.tr=2ns,BW=159MHz

Typicalrise/falltimeandrelatedbandwidthforlogicdevice

 

§8.3AnalogVersusDigitalCircuit

1.Inananalogcircuit,smallnoisecoupledintocircuitmaycauseinterference,whichoftenoccursinlowsignallevel(mV,mA)orinhigh-gainamplifier;Incontrast,digitalcircuithavenoamplifierand

南京师范大学电气与电子工程学院教学授课计划62

operateatlargesignallevel

2.FornoisemarginLSTTL,V=400mV~600mV,CMOS,V

N

=1.5V(Vcc

N

=5V),Sodigitalcircuithaveaninherentimmunitytolow-levelnoise

 

§8.4DigitalLogicNoise

1.Inanalogcircuit,externalnoiseisusuallytheprimaryconcern,however,indigitalcircuit,internalnoisesourceisthemajorconcern

2.Reasonforinternalnoise

(1)groundbusnoise

(2)powerbusnoise

(3)transmissionlinereflection

(4)crosstalk

3.Noisemeasurementrequirement

A)groundvoltagedifferencebetweenvariouspointsinthesystem

B)Vcc-to-groundvoltageonthepowersupplypinsofallIC’s

 

§8.5InternalNoiseSource

1.Fig.8-1Noisegenerationwhenoutputofgate“1”switchesfromhightolow(P277)

2.Sincegate“1”resistanceRisverysmallindischargepath(R,L,Cinseries),high-Q

resonantmaycauseoutputtonegative

 

Q

 

1L

RC

 

Fig.8-2outputvoltagewaveform(p278)

(A)ringingduetostraycapacitanceandinductance(B)ringingdampedbyaddingoutputresistor

SoRQ

南京师范大学电气与电子工程学院教学授课计划63

§8.6DigitalCircuitGroundNoise

Groundnoiseismoreofaproblemthanpowersupplynoise

1.Reasonforgroundnoise:

transientpowersupplycurrent+signal-returncurrent

Usuallypowersupplytransientcurrentcanbecontrolledbydecouplingcapacitor,butsignal-returncurrentcan’t

2.Impedanceofground

UsuallyaPCBconductor(0.02inwide):

12m/in2pF/in15mH/in

Impedanceofa1-inchPWB(15mH)versusfrequencyisrelatedtorise/falltime

Conclusion:

inductanceisthemostconcernwhenlayingoutadigitalPCB

3.Minimizinginductance

(1)lengthofconductor

(2)diameterorwidthofaconductor

4h

L0.005ln()roundconductoraboveacurrent-returnpathd

 

L0.005ln(2h)flatconductoraboveacurrent-returnpathw

(3)providealternativepathforcurrentflow

4.Mutualinductance

5.Practicaldigitalcircuitgroundsystem

Apracticaldigitalcircuitgroundsystemmustprovidealow-impedance(lowinductance)connection

(1)Themostpracticalwayistoprovideasmanyalternative(parallel)pathaspossible,thereforeinfinitenumberofparallelpathresultinagroundplane

(2)Sincegroundplaneneedlargeareaandnotcost-effective,using

groundgridisbetterFig.8-3Agrid-typegroundsystem(p284)

6.Looparea

Iftwoconductorwithcurrentinoppositedirection(e.g.asignalloadanditsground-returnlead)

南京师范大学电气与电子工程学院教学授课计划64

LtL1L22M

 

IfL1=L2,Lt=2(L-M)Therefore,MLt

 

Conclusion:

Placingforwardandreturncurrentpathclosetogetherisaaneffectivewayofreducinginductance.Sotwistedpairorcoaxialcableispreferable,thenLt<1mH/in

 

§8.7PowerDistribution

1.Power-supplydecoupling

Fig.8-4transientpower-supplycurrent(p287)

(A)withoutdecouplingcapacitor(B)withdecouplingcapacitor

2.Decouplingcapacitortypeandvalue

(1)diskceramiccapacitorormultiplayerceramiccapacitor

high-frequency15~150MHz;Lowinductance

(2)TheminimumvalueofcapacitorrequiredbyICwhenitswitchesis

dIdt

C

dV

Example:

anICrequiresatransientcurrentof50mAfor2nSandonewishtolimitpower-supplyvoltagetransientlessthen0.1V,then

50mA2nS

C

0.1V

=0.001uF

(3)Capacitancevaluesislimited

 

A)“C”valuecan’tbetoolarge,otherwiseathigh-F,inductanceL

 

Analysis:

acapacitorhasinductanceinseries,resonantfrequencyis

1

sowhenLisdefiniteand“C”

ff

effectofL

fr

2

LC

 

(becausewhenffrXL>Xc)

南京师范大学电气与电子工程学院教学授课计划65

B)“C”valuecan’tbetoosmall,otherwisenotsufficientchargestoragetosupplythetransientcurrent

Experiment:

“C”valuecanbedeterminedbymeasuringnoisevoltageacrossICchip.Usually470-1000pF

3.Decouplingcapacitorplacement

BeingplacedascloseastotheICispossible

Fig.8-5poorandbetterplacementofdecouplingcapacitor(p290)

Rule:

keeptheloopareabetweenICanddecouplingcapacitorassmallaspossibletodecreasetheinductance

EquivalentcircuitfordecouplingcapacitorconnectedtoICInductanceconsistofthreecomponents:

①inductanceofcapacitoritself

②inductanceofPWBtrace

③inductanceofleadframewithinIC

 

§8.8NoiseVoltageObjective

1.Followingmeasurementshouldbemade

Groundnoisevoltage;power-supplynoisevoltage

2.Thebestmethodistomeasurepeak-differentialgroundnoisevoltagebetweenvariouspointsontheboard,andalsotheVcctogroundvoltageoneachIC

 

§8.9MeasuringNoiseVoltage

1.Considerationofmeasuringnoisevoltage

1)bandwidthofmeasuringinstrument(minimum100MHz,better200MHz)

2)athigh-F,CMMRoftheinstrument

3)leadsfromtheinstrumenttothecircuitundertestCUT

 

2.Equalleadlengthofinstrument,andperpendiculartothecircuitboard

南京师范大学电气与电子工程学院教学授课计划66

Fig.8-6(p294)A)incorrectsetupB)correctone

 

SUMMARY(小结)

 

Chp.9DIGITALCIRCUITRADIATION(数字电路辐射)

 

本章学习要求:

 

了解如下主要概念、方法和内容。

1.差模辐射(辐射计算公式,环路面积,环路电流,

Fourier

级数,差模辐射包

络等)

 

2.控制差模辐射

 

3.共模辐射

 

4.控制共模辐射(共模电压控制,电缆解偶与屏蔽,共模扼流圈,共模电流测量等)

 

Introduction

1.Emissioncontrolshouldbetreatedasadesignproblem,andthroughoutthedesignprocess

南京师范大学电气与电子工程学院教学授课计划67

2.Radiationparameterandmethodsforpracticalradiatedemissionareintroducedinthischp.

 

Radiationtypeindigitalelectronics:

3differential-mode(DM)radiation:

resultofcurrentflowingaroundloopformedbyconductor

 

Fig.9-1differential-moderadiationformPCB(p299)

smallloopantennaradiatingmagneticfield

mon-mode(CM)radiation:

resultofundesiredvoltagedropthatcausepartofcircuittobeatacommon-modepotentialabove“true”ground.Whenexternalcableconnectedtothis,it’sdrivenbythisCMpotentialandradiateelectricfield

Fig.9-2common-moderadiationfromsystemcable(p299)

smallcurrentsegment(straightwire)radiatingEfield

 

§9.1Differential-Mode(DM)Radiation

1.EfieldcalculationforDMradiation

Forlooparea“A”,carryingcurrent“I”,freespacedistance“r”

 

E131.610

 

16(f

2AI)

(1)sin

 

V/m

r

Note:

forsmallloop,thisisaccurate;forlargeloop,thisisapproximate

Ifacircuitonagroundplaneismeasured,reflectioneffectshouldbe

1621

considered.SoE26310(fAI)()sin

 

andEf2,A,I

 

Conclusion:

differential-moderadiationcanbecontrolledby

1)reducingthemagnitudeofcurrent

2)reducingthefrequencyofharmoniccontentofcurrent

3)reducingthelooparea

南京师范大学电气与电子工程学院教学授课计划68

 

2.Looparea

 

Fordigitalcircuitdesign,Aplacingsignalleadsandtheirassociated

ground-returnleadsclosetogether.Especiallyforclockleads,backplanewireing,andinterconnectingcable.

Example:

byFCCClassBLimitmeasuredatdistance3m

IfI=25mA,f=30MHz,looparea“A”=100cm2,r=3mthen

1621

E131.610(fAI)()

 

=197uV/m(aboutthetwicetheallowableemissionofFCCLimit)

 

Butwhenlooparea“A”5cm2

 

E=100uV/m(meetFCCrequirement)

3.Loopcurrent

Measuring“I“byusingaccurateprobetoclipthecircuitwire

Loopantennaconfiguration(p302)

(A)ashortloopantenna(B)acapacitor-terminalloop

Usuallyacapacitor-loadedloopwithzero-impedanceisfrequentlyassumed4.FourierSeries

Sincedigitalcircuitusesquarewave,theFourierseriesofthecurrentshouldbeknownas

In

2Idsin(n

d)sin(n

tr/T)

nd

n

tr/T

 

I:

peak-to-peakamplitudeofthewaved:

dutycycle

tr:

risetime

Fig.9-3exampleofFourierspectrumfroma50%dutycycle(d=0.5)

trapezoidwave(p303)

南京师范大学电气与电子工程学院教学授课计划69

Sodifferential-moderadiatedemissioniscalculatedbyStep1:

calculatethecurrentcontainedineachharmonic

Step2:

substitutethiscurrentandtherespec

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