A) Impedance is independent of frequency
B) Impedance is dependent of frequency
C) Impedance is the resistance only
D) None of the above
Correct Answer: C
Solution :
[c]Here |
(i) Rand L is series wire in wire AB so reactance \[{{\Zeta }_{1}}=R+\operatorname{j}\omega L\] |
(ii) C and R is series wire. So, \[{{\Zeta }_{2}}=R+\frac{1}{\operatorname{j}\omega L}\] |
The equivalent circuit is shown as, |
Hence, impedance Z is given as \[\frac{1}{Z}=\frac{1}{{{Z}_{1}}}+\frac{1}{{{Z}_{2}}}\] |
\[=\frac{1}{R+j\omega L}+(R+j\omega C)\]\[=\frac{1+(R+j\omega C)(R+j\omega L)}{R+j\omega L}\]\[=\frac{(1+R-{{\omega }^{2}}CL)+j(\omega CR+\omega LR)}{R+j\omega L}\] |
\[\Rightarrow \]\[Z=\frac{R+j\omega L}{(1+{{R}^{2}}-{{\omega }^{2}}CL)+j\omega L(C+L)}\]\[=\frac{[R+j\omega L][1+{{R}^{2}}-{{\omega }^{2}}CL-j\left( \omega R \right)\left( C+L \right)]}{(1+{{R}^{2}}-{{\omega }^{2}}CL)+{{\omega }^{2}}{{R}^{2}}{{(C+L)}^{2}}}\] |
Hence, the imaginary part of the impedance is gives as \[=\omega L(1+{{R}^{2}}-{{\omega }^{2}}CL)-{{\omega }^{2}}{{R}^{2}}(C+L)\] |
Putting \[{{R}^{2}}=\frac{L}{C}\]we get it zero. |
You need to login to perform this action.
You will be redirected in
3 sec