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Ch-4 part-2
ANALOG OHMMETER
Analog meter can be designed to measure
resistance by allowing unknown resistance to
complete a series circuit and calibrating the
ammeter scale to read the resistance
There are two types:
Series type ohmmeter
Shunt type ohmmeter
1- Series type ohmmeter
The current in the meter is inversely
proportional to the total resistance of the circuit
Rtot= Rzero adjust+ Rmeter + R Uk
ukmz RRR
VI
Zero adjustInternal
battery
Ammeter
Unknown
resistance
RUK
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When the load is short circuit,
Ruk = 0
Ro= Rz+ Rm
Current is very high (maximum ammeter full deflection
Ifs) , so the pointer go to right , read 0
omz
fsR
V
RR
VI
When RUk= Rzero adjust+ Rmeter=Ro
The meter will read half scale deflection
22
/
2/
fso
oukoukmz
IRV
R
V
RR
V
RRR
VI
From the above scale it is clear that, the total internal
resistance is 10K
When RUnknown=
The meter will read zero
0
omz R
V
RR
VI
The scale is nonlinear and the resistance increase in the
left side
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In general :
The deflection ratio of the meter (D) is expressed as
follows:
UKo
o
ukmz
mz
RR
R
RRR
RRD
Where
D fraction of full-scale meter deflection
Ro total internal resistance of the meter (Rm+Rz)
RUK the unknown resistance
Example-7
Find the value of the unknown resistance when the
Ifs=1mA, Rm=100 and Vbattery=3V for the followingcases
D= 20%, 40%, and 50%
zmfs
RR
VI
KmA
RI
VR m
fsz 9.2100
1
3
KKRRRzmo
39.2100
Unknown
resistance
RUK
Zero adjustInternal
battery
Ammeter
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UKo
o
RR
RD
o
o
uk RD
R
R
For D=20% =.2 , so KRuk 123
2.0
3
For D=40%=.4 , so KRuk 5.43
4.0
3
For D=50%=.5 , so KRuk 33
5.0
3
The zero adjust is necessary to compensate for the
changing voltage from the internal battery due to its ages.
To make ohmmeter sensitive to small value, connected
some resistance in parallel as shown below, so the range
can change
(The shunt resistances reduces the total internal
resistance, so larger current can passes (which mean
measure a small unknown resistance).
Zero adjust
Internal
battery
Ammeter
Rs
Range
switch
Improved series ohmmeter circuit
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2-Shunt type ohmmeter
This type is used to measure small resistance
values
The unknown resistor (Zuk) is connected inparallel with each of the meter internal
resistance and the range switch resistor
When Zuk=0 (short circuit), no current flow
through the meter, and all the current passes
through S.C
When Zuk is not connected (Open Circuit), all
the current flow through the shunt resistance,
meter resistance and range switch resistance.
The scale is nonlinear, and the resistance
increase to the right side ( reverse of series
ohmmeter)
The meter must be turned off, when it is not in
use , otherwise the battery will discharge
On-off
switch
Zero adjust
Internal
batteryA
Range
switchzUK
Shunt OhmmeterSeries Ohmmeter
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Using ohmmeter
Because the ohmmeter supplies a current to the
resistance to be tested, so it must used withun-energized circuit, otherwise the meter will
need a calibration.
The measured resistor must be isolated from
other resistance or disconnect one of its end
THE MEGAOHMMETER (MEGGER)
It is an ohmmeter used to measure very high
resistances such as insulation.
The megger is equipped with hand-crank
generator to turn generator to deliver a highenough voltage to force current in the
resistance to be measured. Or use AC source.
THE VOM35 T (10-kV model)
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VOM Voltmeter-Ohmmeter Milliammeter
It is a meter replace all the previous circuits
combined together.
Can be used to measure each of the voltage, current
and resistance.
Have different ranges for volt, ohms and amperes
Measure AC, DC voltage and current and measure
Ohms
To measuring Ac, it must have an internal rectifier
bridge
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USING VOMs
The precautions for Voltmeter, ammeter and ohmmeter
are applicable for VOMs
For ohmmeter to measure a resistance, the
zero adjust should be
checked each time the
range is switch
For voltmeter/ammeter you must set the range
switch to higher than
expected reading, then
switch to lower to read
accurate reading.
To prevent arcing (damage), the switch range not
change while the DUT is connected.
How to Measure a Capacitor
step-1 (using Ohmmeter)
1-The capacitor is removed from the circuit and discharges
by connected it across resistance
2- Adjust the VOM to ohmmeter and adjust the scale tohigher resistance range
3-Take care of the capacitor polarity if it is electrolyte
4-The ohmmeter read small resistance then it increased asthe capacitor started charges
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5-If the increase of the resistance is small , due to slowlycharging, change ohmmeter to less range.
6- If the resistance not increase, the capacitor is bad
Step-2 (using Voltmeter)
1-Change the VOM to voltage measuring
2-The capacitor is connected in series with voltmeter, seefigure
3-When the voltage is applied , it will divide betweeninternal voltmeter resistance and the capacitor
4- As the capacitor start to charges , the voltage across thevoltmeter is decease.
5-If the voltage not increase, the capacitor is bad
For large electrolyte capacitors may it have leakage current,
so they can appear bad especially with high impedance
meter, to check, compare with similar and good capacitor
Disadvantages of PMMC voltmeter
Low input impedance: Loading effect
Insufficient sensitivity to detect lowlevel signal
Supply
Cap
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Approach
Utilized electronic devices such as
Op-amp ,BJT or FET to solve the above problems
Operational Amplifier (op-amp)
Inverting Amplifier
f
oin
R
V
R
v
00
1
1R
R
v
v f
in
o
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Non-inverting Amplifier
inA vv
f
outinin
R
Vv
R
v
1
0
1
1R
R
v
v f
in
out
1-Using Op-amp to Measure voltage and current
This circuit can be used as ammeter or
Voltmeter
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Ammeter
When function switch at A, current passes through
Rs, so voltage appear on V+
and current can bereading through the meter
Voltmeter
When function switch at V, based on the selected
range, a voltage appears on V
+
Vo=A*V+
Where A is the op-amp gain
Example-8
For the circuit shown, if Ifs=50A, Rm=1K and the Op-
Amp gain is 101, calculate the value of RS
Vo= A*Vin= 101*0.1=10.1 V
Vo = Ifs*( Rs+Rm)
10.1 = 50*10-3
mA*(Rs+ 1K)
Rs= 201 K
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Transistor
The output voltage is related to input current, so it
is called :
Trans-Resistor Transistor
IE= IC+IB IC= IB Ic = IE
1
1 =(100-200)
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It is clear that the common collector (Emitter
follower) have the largest input impedance, so it
can be used as VOA
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Electronic meter
1-Transistor Emitter Follower Voltmeter
Example-9
The simple emitter-follower
circuit has VCC= 20 V,Rs+Rm=
9.3 k, Im= 1mA at full scale,and transistor hFE= 100
(a) Calculate the meter current
when Vin= 10 V
(b) Determine the voltmeter
input resistance with and
without the transistor.
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Solution
When Vin=10V
(a) Im= (10-0.7)/9.3 =1 mA
Disadvantages of this cir cui ts
1-Can't measure voltage less than 0.5V, because
the junction between B, E will be off
2- When the input voltage is 5v(half the input),the meter reading must be 0.5mA, but in fact
I =(5-0.7)/9.3 =0.4624 mA
(b) The input impedance with transistor
KRRI
V
I
VR ms
E
in
B
inin 930)3.9(*100)(
(b) The input impedance without transistor
KRRI
VR ms
fs
inin )3.9()(
Based on this example, the above circuit has some
drawback
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2- Emitter Follower Bridge Configuration
Voltmeter
Vm refer to the voltage o the meter
Vm=VE1-VE2
VE1=Vin-VBE1
VE2=Vp-VBE2
When Q1 and Q2 are identical , then VBE1=VBE2
Vm=VE1-VE2=(Vin-VBE1)-(Vp-VBE2) =Vin-Vp
When Vin=0, R5is adjusted such that Vp=0
Consequently, if Vp is set properly, Vm will be the
same as Vin
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Junction Field Effect Transistor
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FET VOMs and Electronic Meters
With using FET amplifier, the sensitivity can
increase from 20K/V to 10M /V
The resistance loading effect will nearly have no
effect.
The capacitive loading still needs to be considered
at high frequencies
The FET amplifier is sensitive to noise than thepassive VOM
3- FET Voltmeter
Vm = VE1-VE2
EG= VGS+VBE1+VE1So VE1 =EG- VGS-VBE1
VE2 =Vp-VBE2,
Vm = VE1-VE2= EG- VGS-VBE1-Vp+VBE2
= EG- VGS-Vp
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The JEFT added a very high input resistance which
is need for voltmeter to minimize the loading effect
and make sensitivity is good
4- Electronic Ohmmeter (series connection)
1RR
REE
x
xB
1
1
E
E
RR
Bx
Example-10For the electronic ohmmeter shown in the Figure,
determine the resistance scale marking at 1/3 and 2/3 of
full scale
1
1
E
E
RR
B
x
At (1/3) full scale deflection E=EB/3
21
3/1
111 R
E
E
R
E
E
RR
B
BB
x
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At (2/3) full scale deflection E=2EB/3
1
112
13/2
1
R
E
E
R
E
E
RR
B
BB
x
At (1/2) full scale deflection E=EB/2
1
11
12/
1
R
E
E
R
E
E
RR
B
BB
x
5-Electronic Ohmmeter (parallel connection)
When Rx= or open circuit
21
2
RR
REE B
which is the full scale deflection
When Rx//R2=R1
2//
//
11
1
21
2 BB
x
xB
E
RR
RE
RRR
RREE
which is the half- scale deflection
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When Rx= 0 or short circuit
E =0
When Rx= any value
x
xB
RRR
RREE
//
//
21
2
AC Electronic Voltmeter
The scale on ac voltmeters are ordinarily calibrated in
rms volts
It should be noted that the rms value is calculated from
Vin, while the average value is calculated from the output
of ac-dc converter
Form factor is the ratio of the rms value to the average
value of the wave form
Crest factor is the ratio of peak value to the rms value
of the wave form
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Average-Responding Voltmeter
=================================
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Peak-Responding Voltmeter
The primary difference between the peak-
responding voltmeter and the average responding
voltmeter is the use of a detector (storage capacitor
with the rectifying diode)
In the first positive cycle: VC tracks Vin with the
difference of VD, until Vinreaches its peak value.
In the negative half cycle: diode is reversed bias
and the circuit keeps VCat VpVD.
The effect of discharging through R will be
minimized if its value is large enough to yield that
RC >> T.
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RMS-Responding Voltmeter
1-RMS value definition: Mathematics
2-RMS value definition: Physical
rms voltage is equivalent to a dc voltage which generatesthe same amount of heat power in a resistive load that the
ac voltage does.
Digital Multimeter
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Digital Voltmeter (DV)
DVM is essentially an Analog to digital
converter (A/D) with a digital display
Comparison between Digital and Analog Meters
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Digital Multimeter Specification
1-Resolution
The number of digits shown for a
digital multimeter is generally
expressed as a mixed number such as
31/2, 33/4 or 5
1/2 .
31/2or 33/4 mean total # of digit is 4
5 1/2 mean total # of digit is 6
1/2 mean that the most significant digit (MSD)
may be 0 or 1
31/2 can display number from 0000-1999
So, the resolution is 1 part from 2000 or .05%
3/4 mean that MSD can be either 0,1,2,3
43/4 can display number from 00000-39999
So, the resolution is 1 part from 40000 or .0025%
Example-11
For 31/2 meter , calculate the resolution for 20V,
10V, 2V, 1V ranges
Resolution = Vrange*Resolution of 31/2
For 20 v R= 20*.05/100 = 10mV
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For 10v R=10*.05/100 = 5 mV
For 2V R=2*.05/100 =1 mV
For 1V R= 1*.05/100 =0.5 mV
As voltage range decrease as the resolution increase
2-Accuracy
The accuracy of digital meter is specified in variousways.
(a) As a percentage of the reading plus or minus a
number of contents
Manufactures specify the accuracy as a
percentage of the reading plus a percentage of the
full-scale-reading
(b) Parts per million (ppm)
Example-12
Two meter reading are given as follows:
Meter-1 accuracy : 0.05% rdg. +1 digit at 250
Meter -2 accuracy 0.05% rdg.0.03% (full-scale at 250)
Compute the possible error for a 31/2 digit meter operating at
250with an input of 100V.
Due to 31/2 digit, both meter will read four digit
The optimum reading will be 100.0V
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For meter-1
0.05% rdg+1 digit ==0.05%*100+0.1=0.15
For meter-2
The meter is specified for both percentage of reading
and a full-scale. Since the full-scale reading for this
range will by 199.9V
0.05% rgd+0.03% FS 0.05%*100+0.03*199.9=0.109=0.11V
So the second meter have better accuracy than
meter-1
3-Sensitivity
Is the ratio of output response to the input causeunder static conditions
For meter , the sensitivity is related to the lowest range
available for a given function
ElectrometerIs a specialized multimeter with the capability of
measuring voltage, current, resistance, or charge
Has extremely high input impedance, above
100T
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Designed with low input offset current, low drift
and low current noise
Picometer measure small current 10-12
A
Nanovoltmeter measure small voltage10-9V
Power Measurements
1-Low frequency power measurements
There are three types of power
a-True power I2R
b-Reactive power I(VL-VC)
c-Apparent power IVs
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P =VI*Cos()
I current in Ampere (A)
V voltage in Volt (V)
P power in Watt (W)
phase between voltage and current
Cos() power factor (varies between 0 and 1)
For Single Phase
Measure V, I and the phase angle in between will
described later
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Dynamometer wattmeter
It is device used to measure V and I simultaneously
This instrument is of the electrodynamics type.
It consists of:
1- pair of fixed coils, known as current coils
2- movable coil known as the potential coil.
The fixed coils are made up of a few turns of acomparatively large conductor.
The potential coil consists of many turns of
fine wire. It is mounted on a shaft, carried in
jeweled bearings, so that it may turn inside the
stationary coils.
The movable coil carries a needle which
moves over a suitably marked scale. Spiral coil
springs hold the needle to a zero position.
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Power factor measurement
Use the previous dynamometer with adding anextra moving coil, The moving coils are
connected together at right angle to each others
One of the coils is connected in series to
inductor to respond to current that is out of
phase with the line current
The other is connected is series with a resistor
and respond to current that in phase with the
line current