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Electronic Measurements & Instrumentation.
Prof S.Lakshminarayana,M.Tech.,Ph.D.,
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FACT!S I" MA#I"$ MEAS%!EME"TS
The 'oo(ness of measurements in)ol)es
se)eral im*ortant conce*ts. Some of the moresi'ni+cant of these are
• Error,
• -ali(ity,
• !eliaility,
• !e*eataility,
• Accuracy,
• Precision,• !esolution.
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FIGURE 2-5: The accuracy of a
measurement is indicated by the size of ∆!
1. Error In all measurements there is a certain degree of error present.
The word error in this context refers to normal random variation
and in no way means "mistakes" or "blunders.”
o is the true value.
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The measured value may deviate from the true value
!o by a certain amount !# $
If measurements are made repeatedly on the same parameter !which is truly unchanging$
or if different instruments or instrument operators are
used to make successive measurements.
∆X = Absolute error.
X i = Measured Value
X o = True steady state value.
∆X = X i –X o If ∆X → 0, X i →X o
Relative Error
Percentage Error Percentage Error = E r X00
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Errors in Measurement
Systems
Error is the difference between measured value and the truevalue of a physical %uantity. The accuracy of measuring
system is measured in terms of error.
Errors may be positive !&eading higher value or negative
!reading lower value.
TYPES OF ERRORS.
1. Errors due to calibration
'. (uman Errors.
). *oading Error.
+. Environmental Error. !Temperature,. &andom Error.
-. Instrument Error.
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1. Accuracy: The maximum expecteddiference in ma'nitu(e et/een measure( an(
true )alues 0often e1*resse( as a *ercenta'e ofthe full2scale )alue3.2. Precision: The ability o the instrument tore*eat the measurement of a constantmeasuran(. More *recise measurements ha)e
less ran(om error.3. Resolution: The smallest possible increment(iscernile et/een measure( )alues. As the term isuse(, hi'her resolution means smaller increments.
Thus, an instrument /ith a +)e2(i'it (is*lay 0say,4.4444 to 5.55553 is sai( to ha)e hi'her resolutionthan an other/ise i(entical instrument /ith a three2(i'it (is*lay 0say, 4.44 to 5.553. 0Su6ect to thecon(ition that the source has the re7uire(resolution3
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Accurate but not precise.
The average is close
to the center but the
individual values are
not similar.
Precise but not accurate Accurate and Precise
Precision vs. Accuracy
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WHAT IS THE DIFFERENCE BETWEEN
ACCURACY AND PRECISION?
Accuracy is de!ined as "The ability o! a measurement to match theactual value o! the #uantity being measured". $! in reality it is %&.' F
outside and a temperature sensor reads %&.' F then than sensor is
accurate.
Precision is de!ined as "()* The ability o! a measurement to beconsistently reproduced" and "(+* The number o! signi!icant digits to
,hich a value has been reliably measured". $! on several tests the
temperature sensor matches the actual temperature ,hile the actual
temperature is held constant then the temperature sensor is precise. -y
the second de!inition the number %.)&) is more precise than the
number %.)&
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• An e/ample o! a sensor ,ith -A0 accuracy and -A0 precision1 Suppose
a lab re!rigerator holds a constant temperature o! %2.' F. A temperaturesensor is tested )' times in the re!rigerator. The temperatures !rom the
test yield the temperatures o!1 %3.& %2.) %3.% %4. %2.% %3.) %4.) %4.2
%2.2 %3.'. This distribution sho,s no tendency to,ard a particular
value (lac5 o! precision* and does not acceptably match the actual
temperature (lac5 o! accuracy*.
• An e/ample o! a sensor ,ith 6OO0 accuracy and -A0 precision1
Suppose a lab re!rigerator holds a constant temperature o! %2.' F. A
temperature sensor is tested )' times in the re!rigerator. Thetemperatures !rom the test yield the temperatures o!1 %4.2 %2.% %2.)
%2.' %4.7 %2.+ %2.' %2.' %4.& %2.%. This distribution sho,s no
impressive tendency to,ard a particular value (lac5 o! precision* but
each value does come close to the actual temperature (high accuracy*.
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• An e/ample o! a sensor ,ith -A0 accuracy and 6OO0 precision1
Suppose a lab re!rigerator holds a constant temperature o! %2.' F. A temperature
sensor is tested )' times in the re!rigerator. The temperatures !rom the test yield the
temperatures o! 1 %3.+ %3.% %3.) %3.' %3.) %3.% %3.+ %3.) %3.+ %3.+. This
distribution does sho, a tendency to,ard a particular value (high precision* but everymeasurement is ,ell o!! !rom the actual temperature (lo, accuracy*.
• An e/ample o! a sensor ,ith 6OO0 accuracy and 6OO0 precision1
Suppose a lab re!rigerator holds a constant temperature o! %2.' F. A temperature
sensor is tested )' times in the re!rigerator. The temperatures !rom the test yield thetemperatures o!1 %2.' %2.' %4.2 %2.) %2.' %4.3 %2.' %2.+ %2.' %4.3. This
distribution does sho, a tendency to,ard a particular value (high precision* and is
very near the actual temperature each time (high accuracy*.
• The goal o! any instrument is to have high accuracy (sensor matching reality as close
as possible* and to also have a high precision (being able to consistently replicateresults and to measure ,ith as many signi!icant digits as appropriately possible*.
$nstruments including radar need to be calibrated in order that they sustain high
accuracy and high precision.
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). Arithmetic mean 1
The arithmetic mean$ the average of number of readings taken. The best
approximation will be made when the number of readings of the same%uantity is very large. Theoretically an infinite number of readings
would give the best result$ although in practice only a finite number of
measurements can be made. The arithmetic mean is given by
Statistical Analysis1
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+. Mean 0eviation
eviation is the departure at given reading
from the arithmetic mean of the group of
readings. If the deviation of the first reading x1 is d1$ and that of the second reading x
' is called
d' and so on then the deviation from the mean
can be expressed as
The deviation from the mean may have a
positive or a negative value and the algebric
sum of all deviation must be /ero.
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%. Average 0eviation 0
0verage deviation is an indication of the precision of
the instrument used in making the measurements.
(ighly precise instrument will yield a low average
deviation between readings.
o average deviation is the sum of the absolute values
of the deviation divided by the number of readings. Theabsolute value of the deviation is the value without
respect to sign. 0verage deviation may be expressed as
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&. Standard 0eviation
The standard deviation of an infinite number of data is the %uare
root of the sum of all the individual deviations s%uared$ divided by
the number of readings.It is represented by and it is also known as root mean s%uare
deviation. 2athematically it is given by
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8ariance
3ariance or mean s%uare deviation is same as thestandard deviation except that the s%uare root is
not obtained.
Therefore3ariance !v 4 mean s%uare deviation 4 5'
variance are used in many computations because
variances are additive.
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PRO-A-$9$TY OF ERRORS
8O9TA6E MEAS:REME;TS
2ains voltage is measured with a digital voltmeter to the nearest to 6.1 V at short
time intervals. The data are presented in table 1.'. The nominal value of the
measured voltage is ++' V. The data are presented in the histogram of 7ig. 1.+.The ordinate represents the number of observed readings !fre%uency of
occurrence of a particular value. It is also called the fre%uency distribution curve.
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8O9TA6E MEAS:REME;TS
An e/amination o! the. histogram reveals the !ollo,ing points 1
!i The largest number of readings !'6 have their values at the central value of
''6.6 3. 8ther readings are situated symmetrically. mall errors are more
probable than large errors.
!ii The tendency of the curve indicates that if more readings were taken at smaller
interval$ the curve remains symmetrical. 8nly the contour of the histogramwould become smooth. There is an e%ual probability of positive and negative
errors.
!iii The bell shaped curve is called the 9aussian distribution curve.
!iv 0 sharp and narrow distribution curve enables the observer to state that the
most probable value of the true value is the central value.
T0:*E 1.'
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PRO-A-$E ERROR
The 9aussian distribution curve as a function of standard deviation is shown in
7ig. 1.,. ;hen a large number of readings are taken$ the relation is given by
;here x 4 2agnitude of deviation from the mean.
4 <umber of readings at any given deviation x,
!the probability of deviation.
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The error distribution curve sho,s symmetrical distribution o! errors. $t can be
treated as the limiting !orm o! the histogram o! Fig. ).&. The area under the error
distribution curve bet,een the limits < =and > = represents the entire number o!
observations. The area under the curve < and > represents the case that di!!er!rom the mean by no more than the standard deviation (a*. The area under the
curve bet,een the limits < = and > = a gives the total number o! measurements ,ith
in these limits. About 72 percent o! all the cases lie bet,een the limits < and >
!rom the mean. ?ence the more !robable error is ta"en as '.74& .
Fig. ). ERROR 0$STR$-:T$O; @:R8E
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To illustrate the meaning of the probable error$ consider
measurement of nominally 166 pf capacitors. ;hen a large no. of
measurements are taken$ the mean value is found to be 166.66 pF.This means that ≈ -= percent of capacitors have values which lie
between limits of > 6.'6 pf of the mean. This indicates that if a
capacitor is selected from a lot of capacitors at random$ there is
then approximated two to one chance that the value of the capacitor
selected lies between the limits of ? 6.'6pf .@robable error r ? 6.-A+,
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@E&78&20<BE @?ARA@TER$ST$@S 87 I<T&C2E<T
Stability D The ability of a measurement system to maintain its
performance over prolonged periods of time is called stability. If a
system is highly stable$ it need not be calibrated fre%uently.7re%uent calibration is re%uired for less stable instruments.
ero Stability D It indicates the ability of an instrument to restore to
/ero reading after the input is made /ero$ while other conditions
remain the same.Resolution D It is the smallest change of input to which the
measuring system responds. If a digital instrument has a read out of
$ its resolution is 1 in .
0ccuracy and resolution are not the same.
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PRO-9EMS
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