The induced emf in a coil is given by:\[(\text{Emf})_{\text{induced}} = -L \frac{di}{dt}\]
In terms of magnitude:
\[|\text{Emf}_{\text{induced}}| = \left| L \frac{di}{dt} \right|\]
Given:
\[|\text{Emf}_{\text{induced}}| = 0.1 \, \text{V}\]
\[\frac{di}{dt} = \frac{2 - (-2)}{0.2} = \frac{4}{0.2} = 20 \, \text{A/s}\]
Now, solve for \( L \):
\[0.1 = L \times 20\]
\[L = \frac{0.1}{20} = 0.005 \, \text{H} = 5 \, \text{mH}\]


In the circuit shown, assuming the threshold voltage of the diode is negligibly small, then the voltage \( V_{AB} \) is correctly represented by:
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: