low & high resistance measurements and a.c....
TRANSCRIPT
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LOW & HIGH RESISTANCE MEASUREMENTS and A.C. BRIDGES
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SECTION D LOW & HIGH RESISTANCE MEASUREMENTS:
LIMITATIONS OF WHEATSTONE BRIDGE; KELVIN’S DOUBLE BRIDGE METHOD, DIFFICULTIES IN HIGH RESISTANCE MEASUREMENTS.
MEASUREMENT OF HIGH RESISTANCE BY DIRECT DEFLECTION, LOSS OF CHARGE METHOD, MEGOHM BRIDGE & MEGGAR.
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A.C. BRIDGES:
GENERAL BALANCE =N, CKT. DIAGRAM, PHASOR DIAGRAM, ADVANTAGES, DISADVANTAGES,
APPLICATIONS OF MAXWELL’S INDUCTANCE, INDUCANCE-CAPACITANCE, HAYS, ANDERSON, OWENS, DE-SAUTY’S,SCHERING & WEINS BRIDGES, SHIELDING & EARTHING.
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Low Resistance Measurement
D.C Bridges:D.C Bridges:
The basic D.C bridges consist of four resistive arms with a source of emf (a battery) and a null detector usually galvanometer or other sensitive current meter. D.C bridges are generally used for the measurement of resistance values.
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Low Resistance Measurement
Wheatstone Bridge:Wheatstone Bridge:
This is the best and commonest method of measuring
medium resistance values in the range of 1Ω to the low
megohm. The current through the galvanometer
depends on potential difference between point (c) and
(d). The bridge is said to be balance when potential
difference across the galvanometer is zero volts, so
there is no current through the galvanometer (Ig=0).
This condition occurs when Vca=Vda or Vcb=Vdb
hence the bridge is balance.
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Kelvin’s BridgeKelvin’s Bridge
Kelvin bridge is a modification of the Wheatstone bridge and provides greatly increased accuracy in the measurement of low value resistance, generally below (1Ω). It is eliminate errors due to contact and leads resistance. (Ry) represent the resistance of the connecting lead from R3 to R4. Two galvanometer connections are possible, to point (m) or to point (n).
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Kelvin’s BridgeKelvin’s Bridge
1. If the galvanometer connect to point (m) then
R4 = Rx + Ry therefore unknown resistance will be higher than its actual value by Ry
2. If the galvanometer connect to point (n) then
R4 = Rx+ Ry therefore unknown resistance will be lower than its actual value by Ry.
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Kelvin’s BridgeKelvin’s Bridge
1. If the galvanometer connect to point (m) then
R4 = Rx + Ry therefore unknown resistance will be higher than its actual value by Ry
2. If the galvanometer connect to point (n) then
R4 = Rx+ Ry therefore unknown resistance will be lower than its actual value by Ry.
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Kelvin BridgeKelvin Bridge
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Kelvin’s Double Bridge MethodKelvin’s Double Bridge Method
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Kelvin’s Double Bridge MethodKelvin’s Double Bridge Method
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High Resistance Measurement Commonly used High Resistance measurement methods are-
Direct Deflection Method
Megohm Bridge
MEGGAR
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Direct Deflection Method
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Megohm BridgeMegohm Bridge
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MEGGARMEGGAR
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A.C.BridgesA.C.Bridges
A.C.Bridges are those circuits which
are used to measure the unknown
resistances, capacitance, inductance,
frequency and mutual inductance.
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R 1 R 4 R 1 R 3 = R 2 R4
R 2 R 3
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Generalized Bridge configuration
Z1.Z4=Z2.Z3
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Four arms
A source of excitation
For low frequency measurement power-line acts as a source. For higher frequencies electronic oscillators are used.
Battery
Balance Detector
• Head Phone250 Hz to 3-4 kHz
• Vibration Galvanometer 5 Hz to 1000Hz. But used below 200 Hz.
• Tuneable amplifier detector 10 Hz to 100 kHz
Components of AC bridges
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Measurement of Measurement of selfself-- inductanceinductance
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In the Maxwell’s inductance bridge ,there are two
pure resistances used for balance relations but on
other side or arms the two known impedances are
used.
The known impedances and the resistances make
the unknown impedances as Z1 and Z2.Such a
network is known as Maxwell’s A.C.. Bridge. As
shown in fig.
Maxwell’s inductance BridgeMaxwell’s inductance Bridge
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In the Maxwell’s inductance bridge ,there are two
pure resistances used for balance relations but on
other side or arms the two known impedances are
used.
The known impedances and the resistances make
the unknown impedances as Z1 and Z2.Such a
network is known as Maxwell’s A.C.. Bridge. As
shown in figure below-
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Fig.
(R1 + jwL1 )R3 = (R4 + jwL4 )R2
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Phasor diagram
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Maxwell’s inductance and capacitance Maxwell’s inductance and capacitance bridgebridge
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PhasorPhasor DiagramDiagram
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In the Anderson Bridge the unknown inductance is
measured in terms of a known capacitance and
resistance.
this method is capable of precise measurements of
inductance over a wide range of values from a few
micro-henrys to several henrys and is the best
bridge method.
Anderson BridgeAnderson Bridge
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Phasor diagram
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It is particularly useful if the phase angle of the
inductive impedance is large.
In this case a comparatively smaller series
resistance R1 is used instead of a parallel
résistance.( which has to be of a very large value)
as shown in fig.
Hay’s Bridge
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Fig
L3= C1 R2 R4 R3= w C1 R1 R2 R4
1+w R1 C1 1+w R1 C1
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Measurement of Measurement of CapacitanceCapacitance
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We will consider only De Sauty bridge method of comparing two capacitances the bridge has maximum sensitivity when C2 = C3.
The simplicity of this method is offset by the impossibility of obtaining a perfect balance if both the capacitors are not free from the dielectric loss.
A perfect balance can only be obtained if air capacitors are used. as shown in fig.
Capacitance BridgeCapacitance Bridge
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Desauty Bridge
C2= C3 R1 /R2
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Phasor Diagram E3=E4=I2R4 I1R3
E1=E2=I1/WC1
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Schering bridge used for the measurement
of capacitance and dielectric loss of a
capacitor.
It is a device for comparing an imperfect
capacitor C2 in terms of a loss-free
standard capacitor C1. As shown in fig.
Schering BridgeSchering Bridge
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Schering bridge
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Phasor Diagram
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It is also a ratio bridge used mainly as the feedback network in the wide range audio-frequency R-C oscillators.
It is may be used for the measurement of the audio-frequency but it is not as accurate as the modern digital frequency meters. As shown in fig.
Wien Parallel BridgeWien Parallel Bridge
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Wien’s bridgeWien’s bridge
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Stray conductance
Mutual Inductance
Stray Capacitance
Residues in components
Sources of Errors in Bridge Circuits
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Use of High-quality Components
Bridge Lay-out
Sensitivity
Stray Conductance Effects
Eddy Current Errors
Residual Errors
Frequency and Waveform Errors
Precaution and Techniques used Precaution and Techniques used for reducing Errorsfor reducing Errors
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Wagner Wagner EEarthing Devicearthing Device