The voltage across the inductor is given by:
\[ V_L = I X_L, \]
where:
- \( I \) is the current in the circuit,
- \( X_L \) is the inductive reactance given by:
\[ X_L = \omega L = 2\pi f L. \]
Given:
- \( V_L = 31.4 \, \text{V} \),
- \( L = 10 \, \text{mH} = 10 \times 10^{-3} \, \text{H} \),
- Frequency \( f = 50 \, \text{Hz} \).
Step 1: Calculate the Inductive Reactance
\[ X_L = 2\pi f L = 2 \times 3.14 \times 50 \times 10 \times 10^{-3} = 3.14 \, \Omega. \]
Step 2: Calculate the Current Using the formula \( V_L = I X_L \):
\[ 31.4 = I \times 3.14. \]
Solving for \( I \):
\[ I = \frac{31.4}{3.14} = 10 \, \text{A}. \]
Therefore, the current in the circuit is \( 10 \, \text{A} \).
Find output voltage in the given circuit.
A bead of mass \( m \) slides without friction on the wall of a vertical circular hoop of radius \( R \) as shown in figure. The bead moves under the combined action of gravity and a massless spring \( k \) attached to the bottom of the hoop. The equilibrium length of the spring is \( R \). If the bead is released from the top of the hoop with (negligible) zero initial speed, the velocity of the bead, when the length of spring becomes \( R \), would be (spring constant is \( k \), \( g \) is acceleration due to gravity):
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: