written 8.6 years ago by | • modified 8.6 years ago |
Mumbai University > Electronics and Telecommunication > Sem3 > Electronic Instruments and Measurements
Marks: 10M
Year: Dec 14
written 8.6 years ago by | • modified 8.6 years ago |
Mumbai University > Electronics and Telecommunication > Sem3 > Electronic Instruments and Measurements
Marks: 10M
Year: Dec 14
written 8.6 years ago by |
In Maxwell’s inductance capacitance bridge, the value of inductance is measured by comparison with standard variable capacitance. The connection for Maxwell’s inductance capacitance bridge is shown in figure below.
Let $L_1$ =unknown inductance,
$R_1$=effective resistance of inductor $L_1$,
$R_2$ $R_3$ $R_4$ =known non-inductive resistances,
$C_{(4)}$=variable standard capacitor.
And writing the equation for balance
$(R_1+jwL_1)(\frac{R_4}{1+jwC_4R_4})=R_2R_3$
$R_1R_4+jwL_1R_4=R_2R_3+jwR_2R_3C_4R_4$
Separating the real and imaginary terms, we have
$R_1=\frac{R_2R_3}{R_4}$
and
$L_1=R_2R_3C_4$
Thus we have two variables $R_4$ and $C_4$ which appear in one of the two balance equations and hence the two equations are independent. The expression for Q factor.
$Q=\frac{wL_1}{R_1}=wC_4R_4$
Advantages –
The two balance equations are independent if we choose $R_4$ and $C_4$ as variable elements
The frequency does not appear in any of the two equations.
Disadvantages –
It requires a variable standard capacitor which may be very expensive if calibrated to the high degree of accuracy
It is limited to the measurement of low Q coils (1<q<10).< p="">