Errors in Measurement

Permanent Magnet Moving Coil Instrument

Moving Iron Instrument

Electrostatic Type Instruments

Thermocouple Type Instruments

Rectifier Type Instruments

Wheatstone Bridge

Kelvin Bridge

Maxwell Bridge

Anderson’s Bridge

Hay’s Bridge

Owen’s Bridge

Schering Bridge

Heaviside Bridge

De Sauty’s Bridge

Temperature Sensors and its types

Electrodynamometer Type Wattmeter

Induction Type Meters

Energy Meter with Lag Adjustment Devices

Low Power Factor Wattmeter

Working Principle of Potentiometer

Megger

Power Factor Meters

Varmeter

Measurement of Three Phase Power

Weston Type Frequency Meter

Phase Sequence Indicator

## Wheatstone Bridge

For measuring accurately any electrical resistance **Wheatstone bridge** is widely used. There are two known resistors, one variable resistor and one unknown resistor connected in bridge form as shown below. By adjusting the variable resistor the current through the Galvanometer is made zero. When the electric current through the galvanometer becomes zero, the ratio of two known resistors is exactly equal to the ratio of adjusted value of variable resistance and the value of unknown resistance. In this way the value of unknown electrical resistance can easily be measured by using a **Wheatstone Bridge**.

## Wheatstone Bridge Theory

The general arrangement of **Wheatstone bridge circuit** is shown in the figure below. It is a four arms bridge circuit where arm AB, BC, CD and AD are consisting of electrical resistances P, Q, S and R respectively. Among these resistances P and Q are known fixed electrical resistances and these two arms are referred as ratio arms. An accurate and sensitive Galvanometer is connected between the terminals B and D through a switch S_{2}. The voltage source of this Wheatstone bridge is connected to the terminals A and C via a switch S_{1} as shown. A variable resistor S is connected between point C and D. The potential at point D can be varied by adjusting the value of variable resistor. Suppose current I_{1} and current I_{2} are flowing through the paths ABC and ADC respectively. If we vary the electrical resistance value of arm CD the value of current I_{2} will also be varied as the voltage across A and C is fixed. If we continue to adjust the variable resistance one situation may comes when voltage drop across the resistor S that is I_{2}.S is becomes exactly equal to voltage drop across resistor Q that is I_{1}.Q. Thus the potential at point B becomes equal to the potential at point D hence potential difference between these two points is zero hence current through galvanometer is nil. Then the deflection in the galvanometer is nil when the switch S_{2} is closed.

Now, from **Wheatstone bridge circuit**

and

Now potential of point B in respect of point C is nothing but the voltage drop across the resistor Q and this is

Again potential of point D in respect of point C is nothing but the voltage drop across the resistor S and this is

Equating, equations (i) and (ii) we get,

Here in the above equation, the value of S and P ⁄ Q are known, so value of R can easily be determined.

The electrical resistances P and Q of the Wheatstone bridge are made of definite ratio such as 1:1; 10:1 or 100:1 known as ratio arms and S the rheostat arm is made continuously variable from 1 to 1,000 Ω or from 1 to 10,000 Ω

The above explanation is most basic **Wheatstone bridge theory**.

### Video Presentation of Wheatstone Bridge Theory

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