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Question: A virtual current of \(4A\) and \(50Hz\) flows in an AC circuit containing a coil. The power consume...

A virtual current of 4A4A and 50Hz50Hz flows in an AC circuit containing a coil. The power consumed in the coil is 250W250W. If the virtual voltage across the coil is 100V100V, the inductance in the coil will be-
(A). 15πH\dfrac{1}{5\pi }H
(B). 13πH\dfrac{1}{3\pi }H
(C). 15H15H
(D). 1πH\dfrac{1}{\pi }H

Explanation

Solution

In AC circuits different components like capacitor, inductor and resistor can be connected together. The current flowing in an AC circuit is generally taken as the root mean squared current which is the average square of values of currents. The power is dissipated across the resistor and the total impedance is the root of squares of reactance and resistor.

Formulae used:
P=Irms2RP=I_{rms}^{2}R
V=IrmsZV={{I}_{rms}}Z
Z=XL2+R2Z=\sqrt{X_{L}^{2}+{{R}^{2}}}
ωL=XL\omega L={{X}_{L}}

Complete step-by-step solution:
Inductance is the tendency to oppose the change of current in a circuit. The current can change by changing its direction or magnitude. It is directly proportional to the rate of change of current I the circuit. Its SI unit is Henry (HH). The potential developed due to change in current is given by-
e=LdIdte=-L\dfrac{dI}{dt}
Here,
ee is the potential developed
LL is the inductance
dIdt\dfrac{dI}{dt} is the rate of change of current

In an AC circuit, the value of current oscillates between mean and extreme positions. The power consumption in an AC circuit takes place over a resistor as in a resistor power is dissipated as heat.

The formula for power is-
P=Irms2RP=I_{rms}^{2}R
Here,
PP is power
Irms{{I}_{rms}} is the root mean square current
RR is the resistor

Given, Irms=4A{{I}_{rms}}=4A, P=250WP=250W. We substitute given values in the above equation to get,
240=(4)2×R R=24016 R=15Ω \begin{aligned} & 240={{(4)}^{2}}\times R \\\ & \Rightarrow R=\dfrac{240}{16} \\\ & \therefore R=15\Omega \\\ \end{aligned}
Therefore, the resistance in the circuit is 15Ω15\Omega .

The voltage in the circuit is given by-
V=IrmsZV={{I}_{rms}}Z
Here,
VV is the voltage
ZZ is the impedance
Z=VIrms Z=1004 Z=25Ω \begin{aligned} & \Rightarrow Z=\dfrac{V}{{{I}_{rms}}} \\\ & \Rightarrow Z=\dfrac{100}{4} \\\ & \therefore Z=25\Omega \\\ \end{aligned}

We know that,
Z=XL2+R2 Z2=XL2+R2 (25)2=XL2+(15)2 XL2=625225 XL2=400 XL=20Ω \begin{aligned} & Z=\sqrt{X_{L}^{2}+{{R}^{2}}} \\\ & \Rightarrow {{Z}^{2}}=X_{L}^{2}+{{R}^{2}} \\\ & \Rightarrow {{(25)}^{2}}=X_{L}^{2}+{{(15)}^{2}} \\\ & \Rightarrow X_{L}^{2}=625-225 \\\ & \Rightarrow X_{L}^{2}=400 \\\ & \therefore {{X}_{L}}=20\Omega \\\ \end{aligned}
Therefore, the inductive reactance is 20Ω20\Omega

Inductive reactance is also given by-
ωL=XL 2πfL=XL 2π×50L=20 L=15πH \begin{aligned} & \omega L={{X}_{L}} \\\ & \Rightarrow 2\pi fL={{X}_{L}} \\\ & \Rightarrow 2\pi \times 50L=20 \\\ & \therefore L=\dfrac{1}{5\pi }H \\\ \end{aligned}

Therefore, the inductance in the coil is 15πH\dfrac{1}{5\pi }H. Hence, the correct option is (A).

Note:
In an inductor potential difference is developed because the magnetic flux due to current associated with the inductor changes when current changes. The negative sign indicates that the direction of potential is opposite to the direction of change of current. If a capacitor was introduced in the circuit, the total reactance would be the difference between inductive and capacitive reactance.