A bridge in its simplest form consists of a network of 4 resistance arms forming a loop , with a dc source of current applied to 2 opposite junctions and a current detector connected to the opposite two junctions.
Bridge circuits are extensively used for measuring components values like R, L
and C. Since the bridge merely compares the worth of an unknown component
thereupon of an accurately known component (a standard), its measurement
accuracy are often very high. This is because the readout of this comparison is
predicated on the null indication at bridge balance, and is actually
independent of the characteristics of the null detector. The measurement
accuracy is therefore directly related to the null indicator used. The basic dc
bridge is used for accuracy measurement of resistance and is called whetstone’s
bridge.
Whetstone’s bridge is the most accurate method available for measuring
resistances, ranging from approximately one ohm to several mega ohms.
Figure shows the circuit diagram of a whetstones bridge.
Wheatstone's Bridge |
The source of emf and switch is connected to points A and B.
A sensitive current indicating meter, the galvanometer, is connected to points C and D.
The galvanometer is a sensitive micro ammeter, with a zero centre scale when there is no current through the meter, the galvanometer pointer resets at O. i.e mid scale
Current in one direction causes the pointer to deflect on one side and current within the other way to the opposite side.
When SW1 is closed, current flows and divides into the two arms, at the pointer A, i.e I1 and I2.
The bridge is balanced when there is no current through the galvanometer, (or) when the electrical potential at point C and D is equal i.e the potential across the galvanometer is zero.
To obtain the bridge balance equation, we have form the figure.
I1R1
= I2R2
........................ (1)
For the
galvanometer current to be zero, the following conditions should be satisfied.
I1 = I3
= E / R1 + R3
........................ (2)
I2 = I4
= E / R2 + R4
........................ (3)
Combing equations
(1),(2) and (3) and simplifying, we obtain
E / R1 +
R3 = E / R2 + R4
R1 *( R2
+ R4) = (R1
+ R3) * R2
R1R2
+ R1R4 = R1R2 + R3R2
R4 = R2R3
/ R1 ( or) R1R4
= R2R4 ............. (4)
This is the
equation for the bridge to be balanced. If three of the resistances have known
values, the fourth may be determined form eq(4). Hence , if R4 is
the unknown resistor , its resistance Rx can be expressed in terms of the remaining
resistor, as follows.
Rx = R3 . R3 / R1
Resistor R3 is named the “Standard arm” of the bridge, and resistor
R2 and R1 are called the “Ratio arms”.
The measurement of unknown resistance Rx is independent of the
characteristics or the calibration of the null detaching galvanometer, provided
that the null detector has sufficient sensitivity to indicate the position of
the bridge with the specified degree of precision.
APPLICATIONS:
A wheatstone bridge may be used to measure the dc resistance of various of wire
either for the purpose of quantity control of the wire itself, or f some
assembly in which it is used. For example, the resistance of motor windings,
transformers, solenoids, and relay coils are often measured.
It is also used extensively by telephone companies and others to locate cable
faults. The fault could also be two lines shorted together, or one line shorted
to ground.
LIMITATIONS:
For low resistance measurement, the resistance of the leads and contacts
becomes significant and introduces a error. This can be eliminated by Kelvin’s
double bridge.
For high resistance measurements, the resistance presented by the bridge
becomes so large that the galvanometer is insensitive to imbalance. Hence a
power supply has to replace the battery and a dc VTVM replaces the
galvanometer.
In the case of high resistance measurements in mega ohms. The wheatstones
bridge cannot be used.
The rise in temperature causes a change within the value of the resistance, and
excessive current may cause a permanent change in value.
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