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Question: An inductor \[\left( {L = \dfrac{1}{{100\pi }}{\rm{H}}} \right)\], a capacitor \[\left( {C = \dfrac{...

An inductor (L=1100πH)\left( {L = \dfrac{1}{{100\pi }}{\rm{H}}} \right), a capacitor (C=1500πF)\left( {C = \dfrac{1}{{500\pi }}{\rm{F}}} \right) and a resistance(3Ω)\left( {3\Omega } \right) is connected in series with an AC voltage source as shown in the figure. The voltage of the AC source is given as V=10cos(100πt)VoltV = 10\cos \left( {100\pi t} \right){\rm{ Volt}}. What will be the potential difference between A and B?

(A) 8cos(100πt127)Volt8\cos \left( {100\pi t - 127^\circ } \right){\rm{ Volt}}
(B) 8cos(100πt53.13)Volt8\cos \left( {100\pi t - 53.13^\circ } \right){\rm{ Volt}}
(C) 8cos(100πt37)Volt8\cos \left( {100\pi t - 37^\circ } \right){\rm{ Volt}}
(D) 8cos(100πt+37)Volt8\cos \left( {100\pi t + 37^\circ } \right){\rm{ Volt}}

Explanation

Solution

We will write the expression for impedance of a given R-L-C circuit which gives us the relation between capacitive reactance, inductive reactance and resistance of the circuit. We will use the concept of voltage derived from Ohm’s law to write the final expression for the potential difference between A and B.

Complete step by step answer:
Given:
The inductance of the inductor is L=1100πHL = \dfrac{1}{{100\pi }}{\rm{H}}.
The capacitance of the capacitor is C=1500πFC = \dfrac{1}{{500\pi }}{\rm{F}}.
The resistance of the resistor is R=3ΩR = 3\Omega .
The voltage of the AC source is V=10cos(100πt)VoltV = 10\cos \left( {100\pi t} \right){\rm{ Volt}}.
We know that the general form of the AC voltage is V=100cos(ωt)VoltV = 100\cos \left( {\omega t} \right){\rm{ Volt}}. On comparing the given voltage of AC source with its general expression, we will get the value of frequency as below:
ω=100πHz\omega = 100\pi {\rm{ Hz}}
Let us write the expression for impedance of the given L-C-R circuit.
Z=(XCXL)2+R2Z = \sqrt {{{\left( {{X_C} - {X_L}} \right)}^2} + {R^2}} …...(1)
Here XC{X_C} is the capacitive reactance and XL{X_L} is the inductive reactive and R is the resistance of the given R-L-C circuit.
We can write the expression for capacitive reactance as below:
XC=1ωC{X_C} = \dfrac{1}{{\omega C}}
On substituting 1500πF\dfrac{1}{{500\pi }}{\rm{F}} for C and 100πHz100\pi {\rm{ Hz}} for ω\omega in the above expression, we get:

XC=1(100πHz)(1500πF) =5Ω{X_C} = \dfrac{1}{{\left( {100\pi {\rm{ Hz}}} \right)\left( {\dfrac{1}{{500\pi }}{\rm{F}}} \right)}}\\\ = 5\Omega

We can also write the expression for inductive reactance as below:
XL=ωL{X_L} = \omega L
On substituting 1100πH\dfrac{1}{{100\pi }}{\rm{H}} for L and 100πHz100\pi {\rm{ Hz}} for ω\omega in the above expression, we get:

XL=(100πHz)(1100πH) =1Ω{X_L} = \left( {100\pi {\rm{ Hz}}} \right)\left( {\dfrac{1}{{100\pi }}{\rm{H}}} \right)\\\ = 1\Omega

On substituting 5Ω5\Omega for XC{X_C}, 1Ω1\Omega for XL{X_L} and 3Ω3\Omega for R in equation (1), we get:

Z=(5Ω1Ω)2+3Ω2 =5ΩZ = \sqrt {{{\left( {5\Omega - 1\Omega } \right)}^2} + 3{\Omega ^2}} \\\ = 5\Omega

We can write the expression for phase difference as below:
ϕ=tan1(XCXLR)\phi = {\tan ^{ - 1}}\left( {\dfrac{{{X_C} - {X_L}}}{R}} \right)
On substituting 5Ω5\Omega for XC{X_C}, 1Ω1\Omega for XL{X_L} and 3Ω3\Omega for R in the above expression, we get:

ϕ=tan1(5Ω1Ω3Ω) =53.13\phi = {\tan ^{ - 1}}\left( {\dfrac{{5\Omega - 1\Omega }}{{3\Omega }}} \right)\\\ = 53.13^\circ

We can write the expression for the current of the given circuit as the ratio of voltage and impedance of the circuit.
I=VZI = \dfrac{V}{Z}
We know that the phase difference is the lag of current with a potential difference so that we can substitute 10cos(100πtϕ)Volt10\cos \left( {100\pi t - \phi } \right){\rm{ Volt}} for V and 5Ω5\Omega for Z in the above expression.

I=10cos(100πtϕ)Volt5Ω =2cos(100πtϕ)AI = \dfrac{{10\cos \left( {100\pi t - \phi } \right){\rm{ Volt}}}}{{5\Omega }}\\\ = 2\cos \left( {100\pi t - \phi } \right){\rm{ A}}

Now we will substitute 53.1353.13^\circ for ϕ\phi in the above expression.
I=2cos(100πt53.13)AI = 2\cos \left( {100\pi t - 53.13^\circ } \right){\rm{ A}}
We can write the impedance between point A and point B as the difference between capacitive and inductive reactance.
R=XCXLR' = {X_C} - {X_L}
On substituting 5Ω5\Omega for XC{X_C} and 1Ω1\Omega for XL{X_L} in the above expression, we get:

R=5Ω1Ω =4ΩR' = 5\Omega - 1\Omega \\\ = 4\Omega

The potential difference between point A and point B is given by:
V=IRV' = IR'
On substituting 4Ω4\Omega for R’ and 2cos(100πt53.13)A2\cos \left( {100\pi t - 53.13^\circ } \right){\rm{ A}} for I in the above expression, we get:

V=[2cos(100πt53.13)A][4Ω] =8cos(100πt53.13)VoltV' = \left[ {2\cos \left( {100\pi t - 53.13^\circ } \right){\rm{ A}}} \right]\left[ {4\Omega } \right]\\\ = 8\cos \left( {100\pi t - 53.13^\circ } \right){\rm{ Volt}}

Therefore, the potential difference between A and B is 8cos(100πt53.13)Volt8\cos \left( {100\pi t - 53.13^\circ } \right){\rm{ Volt}}, and option (B) is correct.

Note: Do not forget to subtract the phase difference from potential difference while writing the expression for current through the given circuit. The unit of inductive reactance, capacitive reactance is the same as the unit of resistance, so do not confuse with that.