Step 1: Finding Resistance (\(R\))
We use the formula for resistance when the rated voltage (\(V\)) and rated power (\(P\)) are given:
\(R = \frac{V^2}{P}\)
Given:
\(V = 200 \, \text{volts}, \quad P = 50 \, \text{watts}\)
Substituting the values:
\(R = \frac{200^2}{50} = \frac{40000}{50} = 800 \, \Omega\)
Thus, the resistance is:
\(R = 800 \, \Omega\)
Step 2: Finding Power (\(P\)) for a Different Voltage
To calculate the power consumed for an applied voltage (\(V_{\text{applied}}\)) of 100 volts, we use the formula:
\(P = \frac{V_{\text{applied}}^2}{R}\)
Given:
\(V_{\text{applied}} = 100 \, \text{volts}, \quad R = 800 \, \Omega\)
Substituting the values:
\(P = \frac{100^2}{800} = \frac{10000}{800} = 12.5 \, \text{watts}\)
Thus, the power consumed is:
\(P = 12.5 \, \text{watts}\)
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: