Maxwell bridge can be used to measure
inductance by comparison either with a variable standard self-inductance or
with a standard variable capacitance. These two measurement methods can be done
by using two different Maxwell bridge forms.
In this bridge arrangement the value of unknown inductance is measured by comparison with a variable standard self-inductance. Figure 2.12 shows the circuit arrangement and phasor diagram for Maxwell’s inductance bridge under balance condition. Two branches bc and cd consist of non-inductive resistance R3 and R4. One of the arms ad consists of variable inductance L2 of fixed internal resistance r2 connected in series with variable resistance R2. The remaining arm ab consists of unknown inductance Lx of resistance Rx. A source of current is applied to two opposite junctions across ac and a null detector is connected to the other two junctions b and d.
Hence, the
impedances of four arms are
Z1 = Rx + jwLx
Z2 = R2 + r2 + jwL2
Z3 = R3
Z4 = R4
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