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: 
To determine the biasing of diodes in the full wave rectifier at \(t = 15\) ms, we need to calculate the input voltage at this specific time instant. Given the input voltage equation:
\[ V_{in} = 220 \sin(100 \pi t) \]
We substitute \(t = 15\) ms (which is \(t = 0.015\) seconds) into the equation:
\[ V_{in} = 220 \sin(100 \pi \times 0.015) \]
Calculating the argument of the sine function:
\[ 100 \pi \times 0.015 = 1.5 \pi \]
Since \(\sin(1.5 \pi) = -1\), the input voltage becomes:
\[ V_{in} = 220 \times (-1) = -220 \text{ volts} \]
In a full wave rectifier, during the positive half-cycle of the input AC signal, usually \(D_1\) is forward biased and \(D_2\) is reverse biased. Conversely, during the negative half-cycle, the input voltage is negative, leading to \(D_1\) being reverse biased and \(D_2\) being forward biased. At \(t = 15\) ms, since the input voltage is \(-220\) volts (negative half-cycle), \(D_1\) becomes reverse biased, and \(D_2\) becomes forward biased.
Thus, the diodes' biasing is: \(D_1\) is forward biased, \(D_2\) is reverse biased.
Consider a water tank shown in the figure. It has one wall at \(x = L\) and can be taken to be very wide in the z direction. When filled with a liquid of surface tension \(S\) and density \( \rho \), the liquid surface makes angle \( \theta_0 \) (\( \theta_0 < < 1 \)) with the x-axis at \(x = L\). If \(y(x)\) is the height of the surface then the equation for \(y(x)\) is: (take \(g\) as the acceleration due to gravity) 
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is : 