electrical & electronics measurement ee302 · 2012-06-27 · loading effects ii.. underunder...
TRANSCRIPT
Measurements For Nation’s Progress Is Imperative: Measurements For Nation’s Progress Is Imperative: Why?Why?
TheThe advancementadvancement ofof ScienceScience andand TechnologyTechnology isis dependentdependent uponupon
aa parallelparallel progressprogress inin measurementsmeasurements techniquestechniques.. TheThe reasonreason isis
thatthat thethe progressprogress inin sciencescience andand technologytechnology leadsleads toto discoveringdiscovering
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newnew phenomenaphenomena andand relationships,relationships, whichwhich requiresrequires newnew typestypes ofof
quantitativequantitative measurementsmeasurements..
Field Of Field Of Engineering ApplicationsEngineering Applications Of Measurement SystemsOf Measurement Systems
1.1. DesignDesign ofof equipmentequipment andand processesprocesses..
2.2. ProperProper operationoperation andand maintenancemaintenance ofof equipmentequipment andand processesprocesses..
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3.3. QualityQuality controlcontrol assuranceassurance programsprograms forfor industrialindustrial processesprocesses..
Methods of MeasurementsMethods of Measurements
1.1. DirectDirect MethodsMethods:: TheThe unknownunknown quantityquantity isis directlydirectly comparedcompared againstagainst
aa standard,standard, whichwhich areare commoncommon forfor thethe measurementsmeasurements ofof physicalphysical
quantitiesquantities likelike length,length, massmass andand timetime..
DisadvantagesDisadvantages areare::
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DisadvantagesDisadvantages areare::
i.i. LimitedLimited accuracyaccuracy duedue toto humanhuman factorsfactors..
ii.ii. LessLess sensitivesensitive..
Methods of MeasurementsMethods of Measurements, , contcont
2.2. IndirectIndirect MethodsMethods:: TheThe unknownunknown quantityquantity underunder measurementmeasurement isis
determineddetermined viavia thethe useuse ofof measurementmeasurement systemssystems asas followsfollows::
AdvantagesAdvantages areare::
to be to be measuredmeasured
QuantityQuantity
TransducerTransducer
For converting For converting
physical quantity physical quantity
into electric into electric
signalsignal
Signal Signal
ProcessingProcessing
For noise For noise
reduction, reduction,
amplification, etcamplification, etc
Measuring Measuring
DeviceDevice
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AdvantagesAdvantages areare::
i.i. HighHigh accuracyaccuracy andand sensitivitysensitivity cancan bebe obtainedobtained byby usingusing electronicelectronic
andand digitaldigital typetype instrumentsinstruments..
ii.ii. AvailabilityAvailability toto useuse commercialcommercial instrumentinstrument--typestypes atat lowerlower costscosts withwith
acceptedaccepted accuracyaccuracy andand sensitivitysensitivity..
iii.iii. MeasurementsMeasurements ofof nonnon--physicalphysical quantitiesquantities..
Classification of InstrumentsClassification of Instruments
Broadly, instruments are classified into two categories:Broadly, instruments are classified into two categories:
1.1. AbsoluteAbsolute instrumentsinstruments:: TheseThese instrumentsinstruments givegive thethe magnitudemagnitude ofof thethe
quantityquantity toto bebe measuredmeasured inin termsterms ofof physicalphysical constantsconstants ofof thethe
instrumentsinstruments.. ForFor example,example, TangentTangent GalvanometerGalvanometer.. ItIt isis usedused onlyonly inin
standardstandard institutionsinstitutions forfor calibrationcalibration..
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standardstandard institutionsinstitutions forfor calibrationcalibration..
2.2. SecondarySecondary instrumentsinstruments:: InIn thesethese instrumentsinstruments thethe magnitudemagnitude ofof thethe
quantityquantity toto bebe measuredmeasured isis indicatedindicated onon gradedgraded scalescale (e(e..gg.. analoganalog
instruments)instruments) oror displayeddisplayed numericallynumerically onon screenscreen (e(e..gg.. digitaldigital
instruments)instruments)..
Errors in MeasurementsErrors in Measurements
1.1. True Value:True Value:
i.i. ItIt isis notnot possiblepossible toto determinedetermine thethe “true“true value”value” ofof aa quantityquantity byby
experimentalexperimental meansmeans.. TheThe reasonreason forfor thisthis isis thatthat thethe positivepositive
deviationsdeviations fromfrom thethe truetrue valuevalue dodo notnot equalequal thethe negativenegative deviationsdeviations
andand hencehence dodo notnot cancelcancel eacheach otherother..
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ii.ii. InIn practicepractice thethe “true“true value”value” isis measuredmeasured byby aa ““standardstandard unitunit””.
2.2. Static (or Absolute) ErrorStatic (or Absolute) Error ( )Aδ
ItIt isis defineddefined asas thethe deviationdeviation ofof thethe measuredmeasured valuevalue (A(Amm)) fromfrom itsits truetrue
oneone (A(Att),), oror tm AAA −=δ
Errors in MeasurementsErrors in Measurements
3.3. Static CorrectionStatic Correction ( )Cδ
i.i. ItIt isis defineddefined asas thethe correctioncorrection toto bebe addedadded toto thethe measuredmeasured valuevalue soso
asas toto obtainobtain itsits truetrue value,value, oror
ii.ii. TheThe truetrue valuevalue ofof anan instrumentinstrument
mt AAC −=δ
CAA mt δ+=
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ii.ii. TheThe truetrue valuevalue ofof anan instrumentinstrument
iii.iii. Generally,Generally,
CAA mt δ+=
AC δ−=δ
Errors in MeasurementsErrors in Measurements
4.4. Relative Static ErrorRelative Static Error ( )Aδ
i.i. TheThe percentagepercentage staticstatic errorerror ((%% εεεεεεεεrr)) ofof anan instrumentinstrument ==
ii.ii. WhenWhen AAtt isis unknown,unknown, thethe percentagepercentage staticstatic errorerror ((%%εεεεεεεεrr)) ofof anan
instrumentinstrument cancan bebe expressedexpressed asas aa fractionfraction ofof thethe fullfull scalescale deflectiondeflection
100A
A
t
×δ
10
instrumentinstrument cancan bebe expressedexpressed asas aa fractionfraction ofof thethe fullfull scalescale deflectiondeflection
((ff..ss..dd)) asas::
iii.iii. TheThe truetrue valuevalue AAtt ==r
m
1
A
ε+
100d.s.f
A% r ×
δ=ε
Example Example 11::
AA voltagevoltage hashas aa truetrue valuevalue ofof 11..55 VV.. AnAn analoganalog indicatingindicating instrumentinstrument withwith
aa scalescale rangerange ofof 00--22..55 VV showsshows aa voltagevoltage ofof 11..4646 VV.. WhatWhat areare thethe valuesvalues
ofof absoluteabsolute errorerror andand correctioncorrection.. ExpressExpress thethe errorerror asas aa fractionfraction ofof thethe
truetrue valuevalue andand thethe ff..ss..dd..
Solution Solution 11::
V04.05.146.1AAAerrorAbsolute −−−−====−−−−====−−−−====δδδδ
11
%6.11005.2
04.0)d.s.fofpercentageaasressed(experrorlativeRe
%66.21005.1
04.0
A
A)(%errorlativeRe%
V04.0ACcorrectionAbsolute
V04.05.146.1AAAerrorAbsolute
tr
tm
−−−−====××××−−−−
====
−−−−====××××−−−−
====δδδδ
====εεεε
++++====δδδδ−−−−====δδδδ
−−−−====−−−−====−−−−====δδδδ
Errors in MeasurementsErrors in Measurements
5.5. Limiting ErrorLimiting Error
TheThe manufacturersmanufacturers havehave toto specifyspecify thethe deviationdeviation fromfrom thethe specifiedspecified valuevalue
ofof aa particularparticular quantityquantity inin orderorder toto enableenable thethe purchaserpurchaser toto makemake properproper
selectionselection accordingaccording toto hishis requirementsrequirements.. TheThe limitslimits ofof thesethese deviationsdeviations
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fromfrom thethe specifiedspecified valuevalue areare defineddefined asas limitinglimiting errorserrors..
Example Example 22::
TheThe inductanceinductance ofof anan inductorinductor isis specifiedspecified byby aa manufacturermanufacturer asas 2020 HH ±±±±±±±± 55%%..
DetermineDetermine thethe limitslimits ofof inductanceinductance betweenbetween whichwhich itit isis guaranteedguaranteed..
Solution Solution 22::
05.05
)(errorlativeRe r ========εεεε
13
(((( ))))(((( )))) Henery12005.0120
1AAA
AA)A(cetaninducofvalueLimiting
05.0100
)(errorlativeRe
rmmrm
m
r
±±±±====±±±±====
εεεε±±±±====εεεε±±±±====
δδδδ±±±±====
========εεεε
Example Example 33::
AA 00--2525 AA ammeterammeter hashas aa guaranteedguaranteed accuracyaccuracy ofof 11 percentpercent ofof fullfull
scalescale readingreading.. TheThe currentcurrent measuredmeasured byby thisthis instrumentinstrument isis 1010AA..
DetermineDetermine thethe limitinglimiting errorerror inin percentagepercentage..
Solution Solution 33::
amperes25.02501.0d.s.fA
,instrumenttheoferroritinglimofmagnitudeThe
r =×=×ε=δ
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025.010
25.0
A
A)valuemeasuredof(
amperes25.02501.0d.s.fA
m
r
r
==δ
=ε
=×=×ε=δ
Therefore, the current being measured is between the limits of
(((( )))) (((( ))))
%5.210010
25.0errorLimiting%
amperes25.010025.01101AA rm
====××××====∴∴∴∴
±±±±====±±±±====εεεε±±±±====
Errors in Measurements: Errors in Measurements: Random errorsRandom errors
i.i. TheseThese errorserrors areare ofof variablevariable magnitudemagnitude andand signsign andand dodo notnot obeyobey anyany
rulerule..
ii.ii. TheThe presencepresence ofof randomrandom errorserrors becomesbecomes evidentevident whenwhen differentdifferent resultsresults
areare obtainedobtained onon repeatedrepeated measurementsmeasurements ofof oneone andand thethe samesame quantityquantity..
iii.iii. TheThe effecteffect ofof randomrandom errorserrors isis minimizedminimized byby measuringmeasuring thethe givengiven
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quantityquantity manymany timestimes underunder thethe samesame conditionsconditions andand calculatingcalculating thethe
arithmeticarithmetic meanmean ofof thethe valuesvalues obtainedobtained..
iv.iv. TheThe problemproblem ofof randomrandom errorserrors isis treatedtreated mathematicallymathematically asas oneone ofof thethe
probabilityprobability andand statisticsstatistics..
be the number of nbe the number of n--repeated measurements, repeated measurements,
then the arithmetic mean equalsthen the arithmetic mean equals
Standard deviation is Standard deviation is
Errors in Measurements: Errors in Measurements: Random errorsRandom errors
n21 x,,x,xLet L
n
x
x
n
1i
i∑∑∑∑========
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Probable error =Probable error =
1n
xn
1i
2i
−=σ∑=
n
6745.0 σσσσ××××
Static Characteristics of InstrumentsStatic Characteristics of Instruments
1.1. AccuracyAccuracy
ItIt isis thethe closenesscloseness withwith whichwhich anan instrumentinstrument readingreading approachesapproaches thethe
truetrue valuevalue ofof thethe quantityquantity beingbeing measuredmeasured..
AccuracyAccuracy (in(in percent)percent) == r%100 εεεε−−−−
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r
Static Characteristics of InstrumentsStatic Characteristics of Instruments
2.2. SensitivitySensitivity
i.i. TheThe staticstatic sensitivitysensitivity ofof anan instrumentinstrument isis thethe ratioratio ofof thethe magnitudemagnitude
ofof thethe outputoutput signalsignal toto thethe magnitudemagnitude ofof thethe inputinput signalsignal oror thethe
quantityquantity toto bebe measuredmeasured..
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ii.ii. ItsIts unitsunits areare millimetermillimeter perper micromicro--ampereampere,, countscounts perper voltvolt,, etcetc..
dependingdepending uponupon thethe typetype ofof inputinput andand outputoutput signalssignals..
iii.iii. DeflectionDeflection factorfactor (or(or InverseInverse sensitivity)sensitivity) ofof anan instrumentinstrument isis thethe
reciprocalreciprocal ofof thethe sensitivitysensitivity ofof thatthat instrumentinstrument..
Example Example 44::
AA WheatstoneWheatstone bridgebridge requiresrequires aa changechange ofof 77 ΩΩΩΩΩΩΩΩ inin thethe unknownunknown armarm
ofof thethe bridgebridge toto produceproduce aa changechange inin deflectiondeflection ofof 33 mmmm ofof thethe
galvanometergalvanometer.. DetermineDetermine thethe sensitivitysensitivity.. AlsoAlso determinedetermine thethe
deflectiondeflection factorfactor..
Solution Solution 44::
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Solution Solution 44::
mm/33.2429.0
1
ySensitivit
1factorDeflection
/mm429.07
mm3ySensitivit
ΩΩΩΩ============
ΩΩΩΩ====ΩΩΩΩ
====
3.3. ResolutionResolution
ItIt isis thethe smallestsmallest incrementincrement inin inputinput (quantity(quantity beingbeing measured)measured) whichwhich cancan bebe
detecteddetected withwith certaintycertainty byby anan instrumentinstrument..
Static Characteristics of InstrumentsStatic Characteristics of Instruments
Example Example 55::
AA movingmoving coilcoil voltmetervoltmeter hashas aa uniformuniform scalescale withwith 100100 divisions,divisions, thethe fullfull--scalescale
readingreading isis 200200 VV andand 11//1010 ofof aa scalescale divisiondivision cancan bebe estimatedestimated withwith aa fairfair
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readingreading isis 200200 VV andand 11//1010 ofof aa scalescale divisiondivision cancan bebe estimatedestimated withwith aa fairfair
degreedegree ofof certaintycertainty.. DetermineDetermine thethe resolutionresolution ofof thethe instrumentinstrument inin voltsvolts..
Solution Solution 55::
V2.0210
1divisionscale
10
1solutionRe
V2100
200divisionscale1
====××××========
========
Example Example 66::
AA digitaldigital voltmetervoltmeter hashas aa readread--outout rangerange fromfrom 00 toto 99999999 countscounts..
DetermineDetermine thethe resolutionresolution ofof thethe instrumentinstrument inin voltsvolts whenwhen thethe fullfull
scalescale readingreading isis 99..999999 VV..
Solution Solution 66::
21
mV1V10volt999.99999
1count
9999
1solutionRe
9999incount1isinstrumentthisofresolutionThe
3 ==×== −
Accuracy Accuracy versusversus PrecisionPrecision
i.i. TheThe termterm “Precise”“Precise” meansmeans clearlyclearly oror sharplysharply defineddefined..
ii.ii. PrecisionPrecision isis aa measuremeasure ofof thethe reproducibilityreproducibility (( oror consistency)consistency) ofof thethe
measurements,measurements, ii..ee.. givengiven aa fixedfixed valuevalue ofof aa quantity,quantity, precisionprecision isis aa
measuremeasure ofof thethe degreedegree ofof agreementagreement withinwithin aa groupgroup ofof measurementsmeasurements..
iii.iii. ConsiderConsider thethe measurementmeasurement ofof aa knownknown voltagevoltage ofof 100100 VV withwith aa metermeter..
FiveFive readingsreadings areare taken,taken, andand thethe indicatedindicated valuesvalues areare 104104,, 103103,, 105105,, 103103
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andand 105105 VV.. FromFrom thesethese valuesvalues itit isis seenseen thatthat
TheThe instrumentinstrument cannotcannot bebe dependeddepended onon forfor anan accuracyaccuracy betterbetter thanthan 55%%,,
WhileWhile aa precisionprecision ofof ±±±±±±±±11%% isis indicatedindicated sincesince thethe maximummaximum deviationdeviation
fromfrom thethe meanmean readingreading ofof 104104 VV isis onlyonly 11 VV..
%5100V100
V5errorLimiting% ====××××
++++====
WhenWhen aa numbernumber ofof independentindependent measurementsmeasurements areare takentaken inin orderorder toto
obtainobtain thethe bestbest measuredmeasured valuevalue,, thethe resultresult isis usuallyusually expressedexpressed asas
arithmeticarithmetic meanmean ofof allall readingsreadings.. TheThe rangerange ofof doubtdoubt oror possiblepossible errorerror isis
thethe largestlargest deviationdeviation fromfrom thethe meanmean ..
Range of Possible ErrorsRange of Possible Errors
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Example Example 77::
AA setset ofof independentindependent currentcurrent measurementsmeasurements werewere recordedrecorded asas 1010..0303,,
1010..1010,, 1010..1111 andand 1010..0808 AA.. CalculateCalculate thethe rangerange ofof possiblepossible errorserrors..
Solution Solution 77::
A11.10IcurrentofvalueMaximum
A08.104
08.1011.1010.1003.10
4
IIIIIcurrentAverage
max
4321av
====
====++++++++++++
====++++++++++++
====
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A04.02
05.003.0errorsofrangeAverage
A05.0IIRange
A03.10IcurrentofvalueMinimum
A03.0IIRange
A11.10IcurrentofvalueMaximum
minav
min
avmax
max
±±±±====++++
====∴∴∴∴
====−−−−====
====
====−−−−====
====
Loading EffectsLoading Effects
i.i. UnderUnder practicalpractical conditionsconditions thethe introductionintroduction ofof anyany measuringmeasuring
instrumentinstrument inin aa systemsystem results,results, invariably,invariably, inin extractionextraction ofof energyenergy
fromfrom thethe systemsystem therebythereby distortingdistorting thethe originaloriginal signalsignal underunder
measurementmeasurement..
ii.ii. ThisThis distortiondistortion maymay taketake thethe formform ofof attenuationattenuation (reduction(reduction inin
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magnitude),magnitude), waveformwaveform distortion,distortion, phasephase shiftshift andand manymany aa timetime allall
thesethese undesirableundesirable featuresfeatures putput togethertogether..
iii.iii. TheThe incapabilityincapability ofof thethe systemsystem toto faithfullyfaithfully measure,measure, record,record, oror
controlcontrol thethe inputinput signalsignal ((measurandmeasurand)) inin undistortedundistorted formform isis calledcalled
loadingloading effecteffect..
Loading EffectsLoading Effects
1.1. Loading Effects due to Loading Effects due to Shunt ConnectedShunt Connected InstrumentsInstruments
Thevinin
voltage
source oE
oZ
Output
impedance
LZ
Load
(instrument)
OnOn connectingconnecting shuntshunt connectedconnected
instrument,instrument, whosewhose impedanceimpedance isis ,,
thethe actualactual voltagevoltage decreasesdecreases toto
asas followsfollows::o
L
EI
+=
oE LE
LZ
26
AndAnd thethe %%loadingloading errorerror inin measurementmeasurement
ofof equalsequals
LooL
Lo
oL
IZEE
ZZI
×−=
+=
oE
100E
EEerrorLoading%
o
oL ×−
=
Example Example 88::
AnAn oscilloscopeoscilloscope (CRO)(CRO) havinghaving anan outputoutput resistanceresistance ofof 11 MMΩΩΩΩΩΩΩΩ shuntedshunted
byby 5050pFpF capacitancecapacitance isis connectedconnected acrossacross aa circuitcircuit havinghaving anan outputoutput
resistanceresistance ofof 1010 kk ΩΩΩΩΩΩΩΩ.. IfIf thethe openopen circuitcircuit voltagevoltage hashas 11..00 VV--peakpeak forfor aa
sinusoidalsinusoidal ACAC--source,source, calculatecalculate %%loadingloading effecteffect errorerror ofof thethe voltagevoltage
measuredmeasured whenwhen frequencyfrequency isis:: ((ii)) 100100kHzkHz ,, (ii)(ii)11MHzMHz
Solution Solution 88::
1032jjX//RZ3ΩΩΩΩ××××−−−−≅≅≅≅−−−−====
27
%6.41000.1
0.1954.0errorLoading%
peakV4.17954.0
1032j10101
00.1
Z
Z1
EE
1032jjX//RZ
kHz100at
o
3
3
o
L
o
oL
3ckHz100atL
−−−−====××××−−−−
====
−−−−−−−−∠∠∠∠====
××××−−−−××××++++
∠∠∠∠====
++++====
ΩΩΩΩ××××−−−−≅≅≅≅−−−−====
Continue Solution Continue Solution 88::
%701000.1
0.1303.0errorLoading%
peakV72303.0
3183j10101
00.1
Z
Z1
EE
3183jjX//RZ
kHz100at
o
3
o
L
o
oL
cMHz1atL
−−−−====××××−−−−
====
−−−−−−−−∠∠∠∠====
−−−−××××++++
∠∠∠∠====
++++====
ΩΩΩΩ−−−−≅≅≅≅−−−−====
28
%701000.1
errorLoading%kHz100at
−−−−====××××====
Loading EffectsLoading Effects
2.2. Loading Effects due to Loading Effects due to Series ConnectedSeries Connected InstrumentsInstruments
Thevinin
voltage
source oI
oZ
Output
impedance
OnOn connectingconnecting seriesseries connectedconnected
instrument,instrument, whosewhose impedanceimpedance isis ,,
thethe actualactual currentcurrent changeschanges toto
asas followsfollows::
oo ZE
oI LI
LZ
29
AndAnd thethe %%loadingloading errorerror inin measurementmeasurement
ofof equalsequals
oLo
o
Lo
oL I
ZZ
Z
ZZ
EI ××××
++++====
++++====
oI
100I
IIerrorLoading%
o
oL ×−
=
Thevinin
voltage
source
LI
oZ
Output
impedance
LZ
Load
(instrument)
Uncertainty Analysis and Propagation of ErrorsUncertainty Analysis and Propagation of Errors
1.1. Errors Errors vs.vs. Uncertainty Uncertainty
i.i. UncertaintyUncertainty isis thethe rangerange thatthat isis likelylikely toto containcontain thethe deviationdeviation ofof thethe
measuredmeasured valuevalue fromfrom thethe truetrue valuevalue basedbased onon randomrandom--typetype errorserrors..
ii.ii. UncertaintyUncertainty cancan bebe expressedexpressed inin absoluteabsolute termsterms oror relativerelative terms,terms, justjust
asas errorerror cancan..
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For example, consider a meter stick that indicate centimeter and
millimeter divisions. Thus
1)1) TheThe smallestsmallest valuevalue youyou cancan readread onon thisthis metermeter stickstick isis 11 mmmm..
2)2) AnyAny measurementmeasurement youyou makemake willwill bebe quotedquoted toto thethe nearestnearest millimetermillimeter..
3)3) SoSo youryour answeranswer willwill taketake thethe formform 5555 mmmm ±±±±±±±± 11 mmmm ((5555 mmmm isis thethe
measuredmeasured valuevalue && 11 mmmm isis thethe rangerange ofof uncertainty)uncertainty)..
Uncertainty Analysis and Propagation of ErrorsUncertainty Analysis and Propagation of Errors
2.2. PropagationPropagation of Uncertainties of Uncertainties
i.i. AnyAny calculationscalculations donedone usingusing aa measurementmeasurement willwill havehave aa degreedegree ofof
uncertaintyuncertainty.. ThisThis uncertaintyuncertainty isis aa measuremeasure ofof howhow confidentconfident youyou areare inin
thethe resultresult ofof youryour calculationcalculation..
ii.ii. TheThe propagationpropagation ofof thethe uncertaintiesuncertainties throughthrough variousvarious calculationscalculations hashas
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toto bebe carefullycarefully consideredconsidered..
Uncertainty Analysis and Propagation of ErrorsUncertainty Analysis and Propagation of Errors
3.3. Propagation of UncertaintiesPropagation of Uncertainties: : Sum of Two or More QuantitiesSum of Two or More Quantities
yyxxwor
yxw
yxw
∆∆∆∆××××++++
∆∆∆∆××××====
∆∆∆∆
∆∆∆∆++++∆∆∆∆====∆∆∆∆∴∴∴∴
++++====
Let the final result w be the sum of the measured quantities (x ±±±± εεεεx) & (y ±±±± εεεεy)
32
y
y
w
y
x
x
w
x
w
wor
∆∆∆∆××××++++
∆∆∆∆××××====
∆∆∆∆
Finally, the maximum calculation of w is
(((( ))))yw
yxw
xw εεεε××××++++εεεε××××±±±±====εεεε
Uncertainty Analysis and Propagation of ErrorsUncertainty Analysis and Propagation of Errors
4.4. Propagation of UncertaintiesPropagation of Uncertainties: : Difference of Two QuantitiesDifference of Two Quantities
yxw
yxw
∆∆∆∆∆∆∆∆∆∆∆∆
∆∆∆∆−−−−∆∆∆∆====∆∆∆∆∴∴∴∴
−−−−====
Let the final result w be the difference of the measured quantities
(x ±±±± εεεεx) & (y ±±±± εεεεy)
33
y
y
w
y
x
x
w
x
w
wor
∆∆∆∆××××−−−−
∆∆∆∆××××====
∆∆∆∆
Finally, the maximum calculation of w is
(((( ))))yw
yxw
xw εεεε××××++++εεεε××××±±±±====εεεε
Uncertainty Analysis and Propagation of ErrorsUncertainty Analysis and Propagation of Errors
5.5. Propagation of UncertaintiesPropagation of Uncertainties: : Product of Two or More QuantitiesProduct of Two or More Quantities
yieldswt.r.watingDifferenti
ylnxlnwln
yxw
++++====
××××====
Let the final result w be the product of the measured quantities
(x ±±±± εεεεx) & (y ±±±± εεεεy)
34
y
y
x
x
w
w
w
y
y
1
w
x
x
1
w
1
∂∂∂∂++++
∂∂∂∂====
∂∂∂∂
∂∂∂∂∂∂∂∂
××××++++∂∂∂∂∂∂∂∂
××××====
Finally, the maximum calculation of w is
(((( ))))yxw εεεε++++εεεε±±±±====εεεε
Uncertainty Analysis and Propagation of ErrorsUncertainty Analysis and Propagation of Errors
6.6. Propagation of UncertaintiesPropagation of Uncertainties: : Division of Two QuantitiesDivision of Two Quantities
yieldswt.r.watingDifferenti
ylnxlnwln
y
xw
−−−−====
====
Let the final result w be the division of the measured quantities
(x ±±±± εεεεx) & (y ±±±± εεεεy)
35
y
y
x
x
w
w
w
y
y
1
w
x
x
1
w
1
yieldswt.r.watingDifferenti
∂∂∂∂−−−−
∂∂∂∂====
∂∂∂∂
∂∂∂∂∂∂∂∂
××××−−−−∂∂∂∂∂∂∂∂
××××====
Finally, the maximum calculation of w is
(((( ))))yxw εεεε++++εεεε±±±±====εεεε
Uncertainty Analysis and Propagation of ErrorsUncertainty Analysis and Propagation of Errors
7.7. Propagation of UncertaintiesPropagation of Uncertainties: : w = f (x , y)w = f (x , y)
Using Root Sum Square (RSS) method, the error in w is defined by
(((( ))))22
2
y
wy
x
wxw
∂∂∂∂∂∂∂∂
××××∆∆∆∆++++
∂∂∂∂∂∂∂∂
××××∆∆∆∆====∆∆∆∆
36
(((( ))))2
21
22
21
yxyyxw
yxy
w&y
x
w
y
xwLet
23
21
23
21
−−−−××××∆∆∆∆++++
××××∆∆∆∆====∆∆∆∆
−−−−====∂∂∂∂∂∂∂∂
====∂∂∂∂∂∂∂∂
====
−−−−−−−−
−−−−−−−−
Example 9::
37
(((( ))))
(((( ))))2y212
x2w
2
21
22
21
22
2
21
y
y
x
x
yx
yxy
yx
yx
w
w
yieldswbysidesbothdividing
yxyyxw
21
23
21
21
22
εεεε××××++++εεεε====εεεε∴∴∴∴
∆∆∆∆++++
∆∆∆∆====
××××
−−−−××××∆∆∆∆++++
××××
××××∆∆∆∆====
∆∆∆∆
−−−−××××∆∆∆∆++++
××××∆∆∆∆====∆∆∆∆
−−−−
−−−−
−−−−
−−−−