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Question: An inductance of \( 1mH \) , a condenser of \( 10\mu F \) and resistance of \( 50\Omega \) are conne...

An inductance of 1mH1mH , a condenser of 10μF10\mu F and resistance of 50Ω50\Omega are connected in series. The reactance of inductors and condensers are the same. The reactance of either of them will be
(A) 100Ω100\Omega
(B) 30Ω30\Omega
(C) 3.2Ω3.2\Omega
(D) 10Ω10\Omega

Explanation

Solution

The inductive reactance and the capacitive (condenser is another name for capacitor) reactance can be equated. Since they are in the same circuit, then the frequency of the current flowing through them is the same.

Formula used: In this solution we will be using the following formula;
XL=ωL{X_L} = \omega L where XL{X_L} is the inductive reactance of the inductor, ω\omega is the angular frequency, and LL is the inductance value.
XC=1ωC{X_C} = \dfrac{1}{{\omega C}} where XC{X_C} is the capacitive reactance, and CC is the capacitance value of the capacitor or condenser.

Complete step by step solution:
An inductor and condenser are said to be connected to the same circuit in series, and then, it was said that the reactance of the condenser and the inductor are same. This implies that
XC=XL{X_C} = {X_L}
But XC=1ωC{X_C} = \dfrac{1}{{\omega C}} where CC is the capacitance value of the capacitor or condenser, and ω\omega is the angular frequency of the current flowing in the circuit and
XL=ωL{X_L} = \omega L , where LL is the inductance value.
Hence,
1ωC=ωL\dfrac{1}{{\omega C}} = \omega L
Hence, by multiplying both sides by ω\omega and dividing by LL , we get
ω2=1LC{\omega ^2} = \dfrac{1}{{LC}}
ω=1LC\Rightarrow \omega = \dfrac{1}{{\sqrt {LC} }}
By inserting known values, we have
ω=1103×(10×106)\omega = \dfrac{1}{{\sqrt {{{10}^{ - 3}} \times \left( {10 \times {{10}^{ - 6}}} \right)} }} (since 1H=103mH1H = {10^{ - 3}}mH and 1F=106μF1F = {10^{ - 6}}\mu F )
Hence, by computation, we get that
ω=1108=1104=104\omega = \dfrac{1}{{\sqrt {{{10}^{ - 8}}} }} = \dfrac{1}{{{{10}^{ - 4}}}} = {10^4}
Then, to calculate the inductive reactance, we have
XL=ωL=104×103{X_L} = \omega L = {10^4} \times {10^{ - 3}}
By computation it gives us,
XL=10Ω{X_L} = 10\Omega
Hence, the correct option is D.

Note:
Alternatively, since the inductive reactance and capacitive reactance are equal we can decide to calculate the capacitive reactance as follows
XC=1ωC=1104×(10×106){X_C} = \dfrac{1}{{\omega C}} = \dfrac{1}{{{{10}^4} \times \left( {10 \times {{10}^{ - 6}}} \right)}}
Hence, by computation, we have that
XC=1ωC=1101{X_C} = \dfrac{1}{{\omega C}} = \dfrac{1}{{{{10}^{ - 1}}}}
Hence,
XC=10Ω{X_C} = 10\Omega
Also, the angular frequency calculated above ω2=1LC{\omega ^2} = \dfrac{1}{{\sqrt {LC} }} is also called the natural frequency or resonant frequency. This is the frequency of oscillation between the inductor and the capacitor. If a current of this frequency flows through the circuit, the oscillation will be set in resonance.