Demonstrative Video
Problem-1
- \[\begin{aligned} V(t) & = 30t^2, \quad t>0 \\ & 0, \quad t<0 \end{aligned}\]\(t=5\)Find the current through a 5-H inductor if the voltage across it is given by:
Solution-1
- \[i=\frac{1}{5} \int_{0}^{t} 30 t^{2} d t+0=6 \times \frac{t^{3}}{3}=2 t^{3} \mathrm{~A}\], and Since
- \[w=\int p d t=\int_{0}^{5} 60 t^{5} d t=\left.60 \frac{t^{6}}{6}\right|_{0} ^{5}=156.25 \mathrm{~kJ}\], and the energy stored is then The power
- \[\left.w\right|_{0} ^{5}=\frac{1}{2} L i^{2}(5)-\frac{1}{2} L i(0)=\frac{1}{2}(5)\left(2 \times 5^{3}\right)^{2}-0=156.25 \mathrm{~kJ}\]Alternatively, we can obtain the energy stored
Problem-2
The current through 0.1 H inductor is \(i(t)=10t\cdot e^{-5t}\) A. Find the voltage across inductor and energy stored in it.
Solution-2
- \[v=0.1 \frac{d}{d t}\left(10 t e^{-5 t}\right)=e^{-5 t}+t(-5) e^{-5 t}=e^{-5 t}(1-5 t) \mathrm{V}\], and Since
- \[w=\frac{1}{2} L i^{2}=\frac{1}{2}(0.1) 100 t^{2} e^{-10 t}=5 t^{2} e^{-10 t} \mathrm{~J}\]The energy stored is
Problem-3
The voltage across a 2 H inductor is known to be \(6cos5t\) V. Determine the resulting inductor current if \(i(t =-\pi/2)=1\) A.
Solution-3
- \[i(t)=\frac{1}{2} \int_{t_{0}}^{t} 6 \cos 5 t d t+i\left(t_{0}\right)\]\[\begin{aligned} i(t) &=\frac{1}{2}\left(\frac{6}{5}\right) \sin 5 t-\frac{1}{2}\left(\frac{6}{5}\right) \sin 5 t_{0}+i\left(t_{0}\right) \\ &=0.6 \sin 5 t-0.6 \sin 5 t_{0}+i\left(t_{0}\right) \end{aligned}\]Current through inductor
The first term indicates that the inductor current varies sinusoidally; the second and third terms together represent a constant which becomes known when the current is numerically specified at some instant of time.
- \[\begin{aligned} i(t)&=0.6 \sin 5 t-0.6 \sin (-2.5 \pi)+1\\ & = 0.6 \sin 5t + 1.6 \end{aligned}\], and find that with as , we identify at Using the fact that the current is
Problem-4
The terminal voltage of a 2 H inductor is \(v=10(1-t)\) V. Find the current flowing through it at \(t=4\) s and the energy stored in it at \(t=4\) s. Assume \(i(0) = 2\) A.
Solution-4
- \[\begin{aligned} L & = 2~\mathrm{A} \quad v(t) = 10(1-t)~\mathrm{V} \quad i(0) = 2~\mathrm{A} \end{aligned}\]Given data:
- \[\begin{aligned} i(t) & = i(0) + \dfrac{1}{L} \int_{0}^{t} v(t)dt \\ & = 2+\dfrac{1}{2} \int_{0}^{t} (10-10t)dt \\ & = 2+5t-2.5t^2 \end{aligned}\]Current expression:
- \[\begin{aligned} i(t)|_{t=4~\text{sec}} & = 2+20-40 = -18~\mathrm{A} \end{aligned}\]Value of current at 4 sec
- \[\begin{aligned} W|_{0}^{4~\text{sec}} & = \dfrac{1}{2} (L)\left[i^2(4)-i^2(0)\right]\\ & = 320~J \end{aligned}\]Energy:
Problem-5
If the voltage waveform in the figure is applied to 10 mH inductor, find the inductor current \(i(t)\). Assume \(i(0)=0\) A.
Solution-5
- \[\begin{aligned} i(0) & = 0~\mathrm{A} \quad L = 10~\mathrm{mH} \end{aligned}\]Given data:
Voltage distribution:
\[v(t) = \left\{\begin{array}{lr} 5t, & \text{for } 0<t<1\\ 5t-10, & \text{for } 1<t<2\\ 0, & \text{for } \text{elsewhere} \end{array}\right\}\]- \[i(t) = \left\{\begin{array}{lr} 250t^2, & \text{for } 0<t<1\\ 1000(1-t+0.25t^2), & \text{for } 1<t<2\\ 0, & \text{for } \text{elsewhere} \end{array}\right\}\]Current:
Problem-6
The current through 5 mH inductor is shown in fig. Determine the voltage across inductor at \(t=1,3,~ \text{and},~ 5\) ms.
Solution-6
Problem-7
Given the waveform of the current in a 3H inductor as shown in fig, determine the inductor voltage and sketch it.
Solution-7

For \(t<-1 \mathrm{~s}\) current is zero, the voltage is zero in this interval.
The current then begins to increase at the linear rate of \(1 \mathrm{~A} / \mathrm{s}\), and thus a constant voltage of \(L d i / d t=3 \mathrm{~V}\) is produced.
During the following \(2 \mathrm{~s}\) interval, the current is constant and the voltage is therefore zero.
The final decrease of the current results in \(d i / d t=-1 \mathrm{~A} / \mathrm{s}\), yielding \(v=-3 \mathrm{~V}\). For \(t>3 \mathrm{~s}, i(t)\) is a constant (zero), so that \(v(t)=0\) for that interval.
Problem-8
- \[V_L=4.3t, \quad 0 \leq t \leq50~ms\]The voltage across 2 H is given by
With the knowledge that \(i_L(-0.1)=100~\mu A\). Calculate the current (assuming it is defined consistent with the passive sign convention) at t equal to
0 ms
1.5 ms
45 ms
Solution-8
- \[\begin{aligned} i(t) &=\frac{1}{L} \int_{t_{0}}^{t} v(t) d t^{\prime}+i_{L}\left(t_{0}\right) \\ &=\frac{1}{2} \int_{-0.1}^{t} 4.3 t d t^{\prime}+100 \times 10^{-6} \\ &=\frac{4.3}{4}\left(t^{2}-0.01\right)++100 \times 10^{-6} \mathrm{~A} \quad 0 \leq t \leq 50 \mathrm{~ms} \end{aligned}\]Recall that the current flowing through an inductor is given by,
- \[\begin{aligned} i(0) &=\frac{4.3}{4}\left(0^{2}-0.01\right)+100 \times 10^{-6} \\ &=-10.75 \times 10^{-3}+100 \times 10^{-6} \end{aligned}\]Thus, \(t=0\)
- \[\begin{aligned} i(0.0015) &=\frac{4.3}{4}\left(0.0015^{2}-0.01\right)+100 \times 10^{-6} \\ &=-10.748 \times 10^{-3}+100 \times 10^{-6} \end{aligned}\]\[i(0.0015) = -10.648~\mathrm{mA}\], For
- \[\begin{aligned} i(0.045) &=\frac{4.3}{4}\left(0.045^{2}-0.01\right)+100 \times 10^{-6} \\ &=-8.573 \times 10^{-3}+100 \times 10^{-6} \end{aligned}\]\[i(0.045) = -8.473~\mathrm{mA}\], For
Problem-9
Determine the current flowing through a 6mH inductor if the voltage (defined such that it is consistent with the passive sign convention) is given by
5V;
\(100 \sin(120 \pi t), \quad t \geq 0 ~\text{and}~ 0, ~t < 0\)
Solution-9
Problem-10
A square waveform is applied across 1mH inductor. The current is a ……….wave of……..peak amplitude
Solution-10
- \[i_L = \dfrac{1}{L} \int V dt\]\[I_p = 0.5~\mathrm{A}\]\[\begin{aligned} v(t) &=u(t)-2 u(t-0.5)+2 u(t-1)+\ldots \\ i_{L}(t) &=r(t)-2 r(t-0.5)+2 r(t-1)+\ldots \end{aligned}\]Current: