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Question: Figure shows the waveform of the current passing through an inductor of resistance \(1\Omega \) and ...

Figure shows the waveform of the current passing through an inductor of resistance 1Ω1\Omega and inductance 2H2H. The energy absorbed by the inductor in the first four seconds is

A. 144J144J
B. 98J98J
C. 132J132J
D. 168J168J

Explanation

Solution

There is a waveform of current passing through an inductor of resistance and inductor, from this we have to find the energy absorbed for the first four seconds. For total energy, it is the sum of kinetic and gravitational potential energy. By using this theory we are going to find the energy observed.

Complete step by step answer:
From the given data there is an inductor of resistance 1Ω1\Omega and inductance 2H2H.By using these values only we are going to calculate the energy. Energy observed by inductor is given as,
EL=0tPdt{E_L} = \int\limits_0^t {Pdt}
Whereas power P=VI=I(LdIdt)P = VI = I\left( {L\dfrac{{dI}}{{dt}}} \right)
So the equation is, EL=0tLI(dIdt)dt{E_L} = \int\limits_0^t {LI\left( {\dfrac{{dI}}{{dt}}} \right)dt}
In the diagram already given the time of the waveform that is from, 0t4sec0 \leqslant t \leqslant 4\sec
For 0t4sec0 \leqslant t \leqslant 4\sec
EL=204I(dIdt)dt EL=202I(3)dt+224I(0)dt {E_L} = 2\int\limits_0^4 {I\left( {\dfrac{{dI}}{{dt}}} \right)dt} \\\ \Rightarrow {E_L} = 2\int\limits_0^2 {I\left( 3 \right)dt + 2\int\limits_2^4 {I\left( 0 \right)dt} } \\\
In the above equation, dIdt=3\dfrac{{dI}}{{dt}} = 3 and time is also changed, 0t20 \leqslant t \leqslant 2
Therefore for dIdt=0\dfrac{{dI}}{{dt}} = 0 for this the time is, 2<t<42 < t < 4
EL=602Idt EL=6 {E_L} = 6\int\limits_0^2 {Idt} \\\ \Rightarrow {E_L} = 6 \\\
Which is under the area of curve,
EL=6×12×2×6 EL=36J {E_L} = 6 \times \dfrac{1}{2} \times 2 \times 6 \\\ \Rightarrow {E_L} = 36J \\\
Now we are discussing about the energy observed by 1Ω1\Omega resistor is,
ER=01I2Rdt{E_R} = \int\limits_0^1 {{I^2}Rdt}
Here
I=3t,0t2 I=6A,2t4 I = 3t,0 \leqslant t \leqslant 2 \\\ \Rightarrow I = 6A,2 \leqslant t \leqslant 4 \\\
Therefore the above equation is,
ER=02(3t)2×1dt+24(6)2dt ER=9×[t33]02+36[t]42 ER=24+72 ER=96J {E_R} = \int\limits_0^2 {{{\left( {3t} \right)}^2} \times 1dt} + \int\limits_2^4 {{{\left( 6 \right)}^2}dt} \\\ \Rightarrow {E_R} = 9 \times {\left[ {\dfrac{{{t^3}}}{3}} \right]_0}^2 + 36{\left[ t \right]^4}_2 \\\ \Rightarrow {E_R} = 24 + 72 \\\ \Rightarrow {E_R} = 96J \\\
Now to calculate the total energy observed in first four seconds is,
E=EL+ERE = {E_L} + {E_R}
As already we have calculated the above values, by substituting those values we get the total energy,
E=36+96 E=132J E = 36 + 96 \\\ \therefore E = 132\,J \\\
Hence, the correct option is C.**

Note: For calculating the total energy first we have calculated the value of energy in inductance and then calculated the energy in resistance later by adding those two energies we have the total energy in the inductor for the first four seconds. Hence we have derived the problem.