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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