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Biopotential AmplifiersBiopotential Amplifiers
ECGAmplifier
Basic RequirementsBasicRequirements
Essentialfunctionofabiopotential amplifieristotakeaweakelectricsignalsofbiologicaloriginandincreaseitsamplifier
Theymusthavehighinputimpedancesothattheyprovideminimalloadingtoavoiddistortionofthesignal.Typicalinputimpedancesare1M.
Inputcircuitmustprovideprotection.Nocurrentsmustappearattheinputterminals.
Outputcircuitisprimarilyusedtodrivetheamplifierloadoutputimpedanceshouldbelow.p p
Biopotential amplifiersmustbedesignedtobeoptimalinaparticularfrequencyrangeasneededbythesignaltoobtainoptimalsignaltonoiseratios.p g
ECGRecordingSystem
Thefirststageisatransducer(AgCl electrode),whichi l i l l h l i i hconvertECGintoelectricalvoltage. Thevoltageisinthe
rangeof1mV~5mV
The second stage is an instrumentation amplifier, whichThesecondstageisaninstrumentationamplifier,whichhasaveryhighCMRR(90dB)andhighgain(1000)
Optocouplertoisolatetheinputandoutputofamplifierbyconvertingtheelectricalsignaltolightandthenback
Bandpass filterof0.04Hzto150Hzfilter.Normallyimplemented by cascading a lowpass filter and a highimplementedbycascadingalow passfilterandahighpassfilter.
CardiacVector Heartgeneratesanelectricalsignal Electricalactivityoftheheartcanbemodeledasan
electricdipolelocatedinaconductingmediumwhereadipoleconsistsofpointsofequalpositiveandnegativechargeseparatedfromoneanotherandisdenotedbythedipolemoment
Thedipolemomentisavectorfromnegativechargetopositivechargehavingthemagnitudeproportionaltotheseparationofthesecharges.
Thisdipolemomentiscalledthecardiacvector,representedbyM
Itsmagnitudeanddirectionvaryduringthecardiaccycleasthedipolefieldvariesitself.
Thecardiacvectorindicatesthedirectionofthedepolarizationintime.
WewanttocapturethecardiacvectorMbylookingt t t
Va1=M.a1=|M|cosatvectorcomponents.
We can do that bya2
MWecandothatbyconnectingleadsonthesurfaceofthebodytod b l h
a1 detectbiopotentials,thenthevoltagedifferenceintroduced in the lead is the
Figure 6 2 Relationships between the two lead
a1+
introducedintheleadistheprojectionofthecardiacvector
Figure6.2Relationshipsbetweenthetwoleadvectorsa1 anda2 andthecardiacvectorM.ThecomponentofM inthedirectionofa1 isgivenbythedotproductofthesetwovectorsanddenoted
Aleadisdefinedasaconnection between 2
onthefigurebyval.Leadvectora2 isperpendiculartothecardiacvector,sonovoltagecomponentis
seeninthislead.
connectionbetween2electrodesplacedonthebody
ExampleofLeads Eindhovenstriangle
Connectionbetween2electrodesTh i l d Theprimaryleadsare LeadI:LAtoRALead II: LL to RA LeadII:LLtoRA
LeadIII:LLtoLA RL for groundRLforground
ForaleadIIsystemwhichisverycommon,LLandRAarey ,fedtotheinputsoftheinstrumentationdiff ti l lifi I+III=IIdifferentialamplifier I+III=II
ConceptofWilsonsCentralTerminal Wilsonetal.suggestedtheuse
ofthecentralterminal asareference for measuring thereferenceformeasuringtheelectrodepotentials
Thisreferencewasformedbyconnectinga5kWresistorfromthelimbelectrodetothecommon pointcommonpoint.
Wilsonsterminalisnotground buttheaverageofthelimbpotentialswiththetotalcurrentatthispointtobezero
There are other leadThereareotherleadconfigurationscalledAugmentedLeads
OtherLeads AugmentedForsignalaugmentation Disconnecttheunipolarelectrodeyouaremeasuringfromthewilsonsy gterminalandthenmeasure
ChestLeads
V1V6ChestleadsV3V4bestforseptal defects
ThemostcommonlyusedclinicalECGsystem,the12leadECGsystem,consistsofthe following 12 leads whichthefollowing12leads,whichare:
I,II,III
aVR,aVL,aVF
V1,V2,V3,V4,V5,V6
ECGWaveECGNominalData
wave Lead I Lead II Lead IIIwave LeadI LeadII LeadIIIP 0.015to0.12 0.000to0.19 0.073to0.13Q 0.0to0.16 0.0to0.18 0.0to0.28R 0 02 t 1 13 0 18 t 1 68 0 03 t 1 31R 0.02to1.13 0.18to1.68 0.03to1.31S 0.0to0.36 0.0to0.49 0.0to0.55T 0.06to0.42 0.06to0.55 0.06to0.30
DesignofanECGcircuit
Rightlegelectrode
Drivenrightlegcircuit
Sensingelectrodes
Leadfaildetect ADC Memory
Amplifierprotectioncircuit
Leadselector Preamplifier
Auto Baseline Isolated
Isolationcircuit
Driveramplifier
Recorderprinter
Autocalibration
Baselinerestoration powersupply
Parallelcircuitsforsimultaneousrecordingsfromdifferentleads
Controlprogram
MicrocomputerOperatordisplay
Ke board
Figure6.7Blockdiagramofanelectrocardiograph
ECGanalysisprogram
Keyboard
MainComponentsoftheECGCircuitPreamplifier
InitialAmplification
NeedsveryhighI/Pimpedance
HighCMRR
Typically,itisa3opamp
Isolationcircuitry
BlockstheECGfrompowerlinefrequencies
differentialamplifierwithagaincontrolswitch
eque c es
Drivenrightlegcircuit
Provides a reference point on theDriverAmplifier
AmplificationoftheECGsignalforappropriate recording
Providesareferencepointonthebodyinsteadofground
appropriaterecording
PreamplifierDesignDesignSpecificationsg p
AmplificationRange:202000FrequencyRange(0.05150Hz)HighInputImpedance2.5M
Hi h CMRR (E 60dB)HighCMRR(Ex60dB)
Step1:SingleOpampDifferentialAmplifier
Forthisdifferentialamplifier
For a CMRR>60dB or CMRR>1000
VOUT =(V1 V2)R4/R3
ForaCMRR>60dBorCMRR>1000Gd/Gc>1000Gd isgovernedbyR4/R3ifwechooseR4=47K and R3=10K Gd=4 7 andR4 47KandR3 10K,Gd 4.7andGc=0.0047whichisgoodCommonModerejection.WecanreplaceR4inthiscircuitbyapotentiometertoy padjusttoincreasecommonmoderejection.
PreamplifierDesignCont. Step2:Considerthe2opampstageanddesignitforhighgain
VOUT = (V1 V2)(1+2R2/R1) VOUTGain= 1+2R2/R1 If we choose R2=22K and R1=10K thenIf we choose R2 22K and R1 10K, then gain=(1+(2*22)/10))=5.4
PreamplifierDesignCont. Step3:Cascadethe2opampstagewiththedifferential amplifierdifferentialamplifier
TotalGainoftheinstrumentationamplifier=4.7*5.4~25
VOUT = (V1 V2)(1 + 2R2/R1)(R4/R3)
PreamplifierwithFilteringSTEP5
LowPassf=1/(2*pi*RC)~106HzTruncatesTruncatesfrequencies>106Hz
NoninvertingamplifierGain=(1+150K/4.7K)~32
STEP6
( / )TotalGain=25*32=800
HighPass=RC=3.3sf=1/(2*pi*RC)~0.05Hz
STEP4
Passesfrequencies>0.05Hz
Someadditionaldesignconsiderations
Highgainstagesearlyinthesignalpath.However,theHighPassFilterstageshouldbeplacedimmediatelyafterthed ff l l f h ff hdifferentialamplifiertochopofftheDCcomponentofitsoutput.Otherwise,thisDCcomponentwillbeamplifiedbythegainstageandmaysaturatetheg g yfollowingopamps
ItsgainisdeterminedbytheresistorRg.
2nd orderfilterSalleyKeyhighpassfilter
Power line 120 V
InterferencefromElectricDevices Powerlineinterference
ProblemswithECG.Powerline 120V
C3C1C2
Thereiselectricfieldcouplingbetweenthepowerlineandtheleadwires and/or ECG amplifier. This
interference
A
B
Z1
Z2
Id1
Id2
wiresand/orECGamplifier.Thiscouplingismodeledasacapacitor.Itcausesacurrenttoflowfromthepowerlinethroughtheskinelectrode
Electrocardiograph
G
impedancethroughthebodytoground.Bodyimpedanceislow~500.HencethevoltageVA VB =
ZG Id1+Id2
Id1*Z1Id2*Z2.Iftheelectrodesareplacedclosetogetherthecurrentsareapproximatelythesame.VA VB =Id *(Z Z ) ~120V if Id is in nA and Figure6.10 Amechanismofelectric
fieldpickupofanelectrocardiographresultingfromthepowerline.Couplingcapacitancebetweenthehotsideof
Id1*(Z1Z2)~120VifId1isinnA anddifferenceofZ1Z2isinK.Thisisquitehigh.This can be minimized by shielding thepowerlineandleadwirescauses
currenttoflowthroughskinelectrodeimpedancesonitswaytoground.
ThiscanbeminimizedbyshieldingtheleadsandgroundingeachshieldattheECGunit.Alsoloweringskinelectrodeimpedancesmayhelp.
Powerline 120V Thereisalsoapossibilityofcurrentfromthepowerline
ProblemswithECG.Cbidb
toflowthroughthebodyasshowncausingacommonmodelvoltagetoappearinthesignal.
The magnitude of this signal is V =i *Z Typical valuesElectrocardiograph
A
Zin
Z1cm
B
cm
ThemagnitudeofthissignalisVcm=idb ZG.Typicalvaluesare10mVforidb=0.2AandZG=50K.
ForaperfectamplifierthisisnoproblemastheZ2 B
G
Zin
cm
differentialamplifierwithrejectthecommonmodesignal.Butforrealamplifierswithfiniteinputimpedance,thereissomeVcm thatappearsintheoutput
ZGidb
output.
VAVB=Vcm ((Z2Z1)/Zin)ifZ1 andZ2 are
ProblemswithECGCont. Othersourcesofinterference interference
Magneticfieldpickup
EMG i t fEMGinterference
Figure6.12Magneticfieldpickupbytheelctrocardiograph (a)LeadwiresforleadImakeaclosedloop(shadedarea)whenpatientandelectrocardiograph
Figure6.9 (a)60Hzpowerlineinterference (b) Electrom ographic
areconsideredinthecircuit.Thechangeinmagneticfieldpassing
throughthisareainducesacurrentintheloop.(b)Thiseffectcanbe
interference.(b)ElectromyographicinterferenceontheECG.
minimizedbytwistingtheleadwirestogetherandkeepingthemclosetothe
bodyinordertosubtendamuchsmallerarea.
ProblemswithTransients ToprotecttheECGcircuitagainsthighvoltagesweneedvoltage
limitingcircuitry.
These occur for example in the operating room when the ECG isTheseoccurforexampleintheoperatingroomwhentheECGiscombinedwiththeuseofanelectrosurgicalunitthatwillinducehightransientvoltagesintothepatient.
Voltage limiting devices such as diodes are used for protecting the VoltagelimitingdevicessuchasdiodesareusedforprotectingtheECGcircuitryandareconnectedbetweentheleadandRLground.
Figure 6 14 Voltagelimiting devices (a) CurrentFigure6.14Voltage limitingdevices(a)Currentvoltagecharacteristicsofavoltagelimiting
device.(b)Parallelsilicondiodevoltagelimitingcircuit.(c)BacktobacksiliconZenerdiode
Figure6.13Avoltageprotectionschemeattheinputofanelectrocardiograph
OtherProblemsfrequentlyencountered with the ECGencounteredwiththeECG
FrequencyDistortion:Highfrequencydistortion RoundingofftheQRSwaveform and diminishing itswaveformanddiminishingitsamplitude.Lowfrequencydistortionbaselineisnolongerhorizontalafteranevent.
Saturationorcutoffdistortion HighoffsetvoltagesandimproperlyadjustedamplifierscanproducesaturatedECGs.Peaks of the QRS are cutoff
Figure6.8EffectofavoltagetransientonanECGrecordedonanelectrocardiographinwhichthetransientcausestheamplifierto
saturate,andafiniteperiodoftimeisPeaksoftheQRSarecutoff GroundLoops If1groundof1device
ishigherthantheECGground,acurrentwillflowthroughthepatient
requiredforthechargetobleedoffenoughtobringtheECGbackintotheamplifiers
activeregionofoperation.Thisisfollowedbyafirstorderrecoveryofthesystem.
g ppresentingasafetyproblemaswellaselevatingthepatientsbodypotentialprojectingerroneousvoltagesintheECG
ArtifactsfromLargeTransientsCausealargeabruptdeflectionintheECG,takelongtimeforrecoverydue
ECG tothelargechargebuiltupinthecapacitors.
Commonmodereductioncircuits Commonmodesignalfromthebodyor
powerlineisaproblem.Eventhoughtheamplifierwillhelpineliminating
id
R+
3
thesebecauseofthehighCMRR,wecantrytoeliminatethecommonmodelsignalatthesource.Forinstancel d f ld k
Ra
Ra
+
ElectricandMagneticfieldpickupcanbeminimizedbyelectrostaticshieldingandtwistingofleadwires.
h l i i h i i h R
Rf
RoAuxiliaryopamp +
+
RL
4cm
AnothersolutionistheDrivenRightLegSystemwheretheRLelectrodeisconnectedtotheO/Pofanauxiliaryopamp The common mode signal
RRLp p
opamp.Thecommonmodesignalsensedbythevoltagefollowersisamplifiedandfedbacktothebodyraising the RL potential This negativeraisingtheRLpotential.Thisnegativefeedbackcausestheoutputcommonmodesignaltobelow.
Designconsiderations withotheramplifiersp
Figure6.16Voltageandfrequencyrangesofsomecommonbiopotentialsignals;dcpotentialsincludeintracellularvoltagesaswellasvoltagesmeasuredfromseveral
pointsonthebody.EOGistheelectrooculogram,EEGistheelctroencephalogram,ECGistheelectrocardiogram,EMGistheelectromyogram,andAAPistheaxonaction
potential.
EMGAmplifier BasicsandDesign EMG stands for electromyogramEMGstandsforelectromyogram Itismeasurementofelectricalpotentialscreatedbythecontractionof
muscles. Musclesgeneratevoltagesaround100mVwhentheycontract.These
lt tl tt t d b i t l ti d th ki d thvoltagesaregreatlyattenuatedbyinternaltissueandtheskin,andtheyareweakbutmeasurableatthesurfaceoftheskin.
TypicalsurfaceEMGsignalsforlargemuscles,suchasthebicep,arearound12mVinamplitude.
EMGsignalscontainfrequenciesrangingfrom10Hzorlowerupto1kHzorhigher.
ToobserveanEMGsignal,weneedtobuildadifferentialamplifierwithhigh commonmode rejectionhighcommonmoderejection
Thedominantcommonmodevoltagesignalsonourbodiesisusuallya60Hzsinewavethatiscapacitively coupledtousfromthe120VACwiringinthewalls.
Werejectthissignalbylookingatthedifferenceinvoltagebetweentwonearbypointsontheskinoverthemuscleofinterest.
Wewillalsowanttouseacircuitthedrawsnearlyzerocurrentfromtheinputleads,sincedccurrentpassedthroughEMGelectrodescanleadtop , p glargedcoffsetsanddegradethelongtermusefulnessoftheelectrodes.