To determine the period of revolution if the Sun expands to twice its present radius, we will use the concept of conservation of angular momentum. The angular momentum \( L \) of a rotating object is given by:
\( L = I \omega \)
where \( I \) is the moment of inertia and \( \omega \) is the angular velocity. For a sphere of uniform density, the moment of inertia \( I \) is:
\( I = \frac{2}{5}MR^2 \)
where \( M \) is the mass and \( R \) is the radius. Since there is no external torque, the angular momentum before and after expansion remains constant:
\( I_1 \omega_1 = I_2 \omega_2 \)
Initially, we have:
\( I_1 = \frac{2}{5}MR_1^2 \)
After expansion, the new radius is \( 2R_1 \), so:
\( I_2 = \frac{2}{5}M(2R_1)^2 = \frac{8}{5}MR_1^2 \)
Given that the initial period of rotation \( T_1 \) is 27 days, we know:
\( \omega_1 = \frac{2\pi}{T_1} \)
The new angular velocity \( \omega_2 \) is:
\( \omega_2 = \frac{2\pi}{T_2} \)
From conservation of angular momentum:
\( \frac{2}{5}MR_1^2 \cdot \frac{2\pi}{27} = \frac{8}{5}MR_1^2 \cdot \frac{2\pi}{T_2} \)
Canceling out the common terms \( \frac{2\pi}{5}MR_1^2 \), we get:
\( \frac{1}{27} = \frac{4}{T_2} \)
Solving for \( T_2 \):
\( T_2 = 4 \times 27 = 108 \text{ days} \)
Thus, if the Sun's radius doubles, the period of revolution will be \( 108 \text{ days} \).
A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec: 