**A potentiometer or a rheostat is an instrument used to measure and compare potentials without drawing any current from the circuit.**

**Potentiometer Principle**

The potential difference across any length of wire of uniform cross-section area is directly proportional to its length where a constant current flows through it.

A potentiometer consists of a resistance R in the form of a wire on which a terminal C can slide as shown in Fig.

The resistance between A and C can be varied from 0 to R as the sliding contact is moved from A to B. Let a battery of emf E be connected across R as shown in Fig.

The current flowing through it is given by

$I=\frac{E}{R}~~~~~\cdots \text{ }~~~~\left( 1 \right)$

If we represent the resistance between A and C by r, then the potential drop between these points will be,

$V=Ir~~~~\text{ }\cdots \text{ }~~~~\left( 2 \right)$

Putting the value of I from eq (1) into (2) we obtain,

$V=\frac{E}{R}*r$

Where C is moved from A to B, r varies from 0 to R and potential drop between A and C changes from 0 to E. Such an arrangement is known as a potential divider. A potential divider can be used to determine the unknown emf of a source by using the circuit given below.

The figure shows that R is in the form of a straight wire of uniform area of cross-section. A source of potential, whose E_{x} emf is to be measured is connected between A and sliding contact C through a galvanometer G. The positive terminal of E_{x} and that of the potential divider are connected to the same point A.

“If the point C and negative terminal of E_{x} are at the same potential then the two terminals of galvanometer will be at the same potential and no current will flow through the galvanometer.”

Therefore, in order to measure the potential E_{x}, the position of C is so adjusted that the galvanometer shows no deflection. Under this condition, the emf E_{x} is equal to the potential difference between A and C whose value ($\frac{E}{R}*r$) is known.

In the case of wire of uniform area of cross-section, the resistance is proportional to the length of a wire. Therefore unknown is given by;

${{E}_{x}}=\frac{r}{R}*E$

Or

${{E}_{x}}=\frac{l}{L}*E$

Where L is the length of wire AB and l is a length of wire from A to C. The unknown emf E_{x} should not exceed E-value, otherwise, the null condition will not be obtained.

**Uses of Potentiometer**

- It can be used to determine the emf of a cell.
- It can be used to compare the emf of two cells.
- It can be used as a continuously potential divider.

- You May Also Read: Impedance Measurement Theory