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Question: A resistor, an inductor and a capacitor are connected in series with a \[120\,{\text{V}}\], \[100\,{...

A resistor, an inductor and a capacitor are connected in series with a 120V120\,{\text{V}}, 100Hz100\,{\text{Hz}} ac source. Voltage leads the current by 3535^\circ in the circuit. If the resistance of the resistor is 10Ω10\,\Omega and the sum of the inductive and capacitive reactance is 17Ω17\,\Omega , calculate the self-inductance of the inductor.

Explanation

Solution

Use the formula for phase difference between the voltage and current in the circuit. This formula gives the relation between the phase difference, inductive reactance, capacitive reactance and resistance. Calculate the value of inductive reactance using this equation and then use the formula for self-inductance in terms of inductive reactance and frequency.

Formulae used:
The phase difference ϕ\phi between the voltage and current is given by
tanϕ=XLXCR\tan \phi = \dfrac{{{X_L} - {X_C}}}{R} …… (1)
Here, XL{X_L} is the inductive reactance, XC{X_C} is the capacitive reactance and RR is the resistance.
The inductance LL of an inductor is given by
L=XL2πfL = \dfrac{{{X_L}}}{{2\pi f}} …… (2)
Here, XL{X_L} is the inductive reactance and ff is the frequency.

Complete step by step solution:
We have given that the resistor, inductor and capacitor are connected in series in a circuit with potential difference 120V120\,{\text{V}} and frequency 100W100\,{\text{W}}.
V=120VV = 120\,{\text{V}}
f=100Hzf = 100\,{\text{Hz}}
The phase difference between the voltage and current is 3535^\circ .
ϕ=35\phi = 35^\circ
The resistance of the resistor is 10Ω10\,\Omega .
R=10ΩR = 10\,\Omega
The sum of the inductive and capacitive reactance is 17Ω17\,\Omega .
XL+XC=17Ω{X_L} + {X_C} = 17\,\Omega …… (3)
We have asked to calculate the self-inductance of the inductor. Let us first calculate the inductive reactance.Substitute 3535^\circ for ϕ\phi and 10Ω10\,\Omega for RR in equation (1).
tan35=XLXC10Ω\tan 35^\circ = \dfrac{{{X_L} - {X_C}}}{{10\,\Omega }}
XLXC=0.7×10\Rightarrow {X_L} - {X_C} = 0.7 \times 10
XLXC=7Hz\Rightarrow {X_L} - {X_C} = 7\,{\text{Hz}} …… (4)
We can solve the equations (3) and (4) by adding them.
(XL+XC)+(XLXC)=17Ω+7Hz\left( {{X_L} + {X_C}} \right) + \left( {{X_L} - {X_C}} \right) = 17\,\Omega + 7\,{\text{Hz}}
2XL=24Ω\Rightarrow 2{X_L} = 24\,\Omega
XL=12Ω\Rightarrow {X_L} = 12\,\Omega
Hence, the inductive reactance is 12Ω12\,\Omega .
Let is now calculate the self-inductance of the inductor.
Substitute 12Ω12\,\Omega for XL{X_L}, 3.143.14 for π\pi and 100Hz100\,{\text{Hz}} for ff in equation (2).
L=12Ω2(3.14)(100Hz)L = \dfrac{{12\,\Omega }}{{2\left( {3.14} \right)\left( {100\,{\text{Hz}}} \right)}}
L=0.019H\Rightarrow L = 0.019\,{\text{H}}
L=1.9×102H\therefore L = 1.9 \times {10^{ - 2}}\,{\text{H}}

Hence, the self-inductance of the inductor is 1.9×102H1.9 \times {10^{ - 2}}\,{\text{H}}.

Note: There is no need to calculate the capacitive reactance in the circuit as we are asked to calculate the self-inductance of the inductor. The formula for the self-inductance includes only inductive reactance and not capacitive reactance. So, if one tries to calculate the capacitive reactance, it is a waste of time only.