Measurement of Self Inductance by Maxwell Bridge            

Introduction

To determine the self-inductance of an unknown coil.

Theory

This bridge circuit measures an inductance by comparison with variable standard self inductance. The connections for balance condition is shown in Fig. 1.

Rm501 Figure

Fig 1: Circuit Diagram for Measurement of Self Inductance by Maxwell Bridge

Let, L1= Unknown self Inductance of resistance R1,

L2= variable inductance of fixed resistance r2,

R2= variable resistance connected in series with inductor L2,

R3,R4= known non inductive resistances,

At balance condition,

$$ (R_1 +j \omega L_1)*R_4 = (R_2 + r_2 + j \omega L_2)*R_3 ...(1) $$

Equating both the real and imaginary parts in eq.(1) and seperating them,

$$ L_1 =(\frac{R_3}{R_4})L_2 ...(2) $$

$$ R_1 = (\frac{R_3}{R_4})*(R_2+r_2) ...(3) $$

Resistors R3 and R4 are normally a selection of values from 10, 100, 1000 and 10,000Ω. r2 is a decade resistance box.