Wheatstone Bridge: Wheatstone bridge is an electrical arrangement which forms the basis of the instruments used to determine an unknown resistance.
Principle of Wheatstone bridge: If four resistances P, Q, R and S are arranged as shown in figure, if the galvanometer does not show any defection, then
\(\frac{P}{Q} = \frac{R}{S}\)
Derivation
Wheatstone bridge consists of four resistances P, Q, R and S arranged as shown in Fig. with a cell E between the points A and C and a galvanometer G between B and D.
Let I be the total current given out by the cell which on reaching the point A divides itself into two parts : (a) I1 flowing through P and (b) (I - I1) through R. The current I1, on reaching the point B, divides itself into two parts : (a) Ig through the galvanometer G and (b) (I1 - Ig) through Q. The current Ig through the arm BD and (I - I1) through AD combine at D to send a current (I - I1 + Ig) through S. On reaching the point C, the current (I1 - Ig) through BC and (I - I1 + Ig) through DC combine to give the total current I, thus completing the circuit. (The values of the currents at a junction can be verified by applying Kirchhoffs first law at the junction).
Applying Kirchhoffs second law to the closed mesh ABDA, we get
I1P + IgG - (I - I1) R = 0. ...................(1)
where G is the resistance of the galvanometer.
Again applying Kirchhoffs second law to the closed mesh BCDB we get,
(I - Ig) Q - (I - I1 + Ig) S - IgG = 0 ...........................(2)
The value of R is so adjusted that the points B and D are at the same potential and as such no current flows in the arm BD i.e. Ig = 0. This is indicated by zero deflection in the galvanometer G. In this position, the bridge is said to be balanced. Putting Ig = 0 in equations (1) and (2), we get
I1P - (I - I1) R = 0
or I1P = (I - I1)R .......................(3)
and I1 Q - (I - I1) S = 0
i.e. I1 Q = (I - I1) S ........................(4)
Dividing (3) by (4), we get
\(\frac{I_1P}{I_1Q} = \frac{(I-I_1)R}{(I-I_1)S}\)
or \(\frac{P}{Q} = \frac{R}{S}\)