Case 1: DC Circuit When the coil is connected to a DC supply, the inductive reactance is 0, so:
\[ I = \frac{V}{R} \implies R = \frac{20}{5} = 4 \, \Omega. \]
Case 2: AC Circuit When the coil is connected to an AC supply:
\[ I = \frac{V}{Z} \implies Z = \frac{20}{4} = 5 \, \Omega, \]
where \( Z \) is the impedance of the coil, given by:
\[ Z = \sqrt{R^2 + X_L^2}. \]
Substitute \( R = 4 \, \Omega \):
\[ 5 = \sqrt{4^2 + X_L^2} \implies X_L^2 = 25 - 16 = 9 \implies X_L = 3 \, \Omega. \]
The inductive reactance \( X_L \) is related to the self-inductance \( L \) by:
\[ X_L = 2 \pi f L \implies L = \frac{X_L}{2 \pi f}. \]
Substitute \( X_L = 3 \, \Omega \), \( f = 50 \, \text{Hz} \), and \( \pi = 3 \):
\[ L = \frac{3}{2 \cdot 3 \cdot 50} = \frac{3}{300} = 0.01 \, \text{H} = 10 \, \text{mH}. \]
Final Answer: 10 mH.
Draw the plots showing the variation of magnetic flux φ linked with the loop with time t and variation of induced emf E with time t. Mark the relevant values of E, φ and t on the graphs.
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: