List-I | List-II | ||
P | The value of \(I1\) in Ampere is | I | \(0\) |
Q | The value of I2 in Ampere is | II | \(2\) |
R | The value of \(\omega_0\) in kilo-radians/s is | III | \(4\) |
S | The value of \(V_0\) in Volt is | IV | \(20\) |
200 |
P → 2; Q → 5; R → 3; S → 4
When K1 is closed, the capacitor is uncharged, so the inductor opposes any sudden change in current. Hence, the current through \( R_0 \) is:
\[ I_1 = 0 \text{ Ampere}. \]
After a long time, the capacitor is fully charged, and the inductor acts as a short circuit. The circuit becomes resistive:
\[ I_2 = \frac{E}{R_0} = \frac{20}{5} = 4 \text{ Ampere}. \]
When K1 is opened and K2 is closed, the circuit becomes an LC-oscillator. The angular frequency is given by:
\[ \omega = \sqrt{\frac{1}{LC_0}}. \]
Substituting \( L = 25 \) mH and \( C_0 = 10 \) μF:
\[ \omega = \sqrt{\frac{1}{(25 \times 10^{-3}) \cdot (10 \times 10^{-6})}} \]
\[ = \sqrt{4 \times 10^6} = 2000 \text{ radians/s}. \]
In kiloradians:
\[ \omega = 2 \text{ kilo-radians/s}. \]
Using the energy conservation principle in the LC-oscillator:
\[ \frac{1}{2} L I_2^2 = \frac{1}{2} C_0 V_0^2. \]
Solving for \( V_0 \):
\[ V_0 = \sqrt{\frac{L}{C_0}} \cdot I_2. \]
Substituting values:
\[ V_0 = \sqrt{\frac{25 \times 10^{-3}}{10 \times 10^{-6}}} \times 4 = 200 \text{ Volts}. \]
Based on the calculations:
The correct option is (A).
In the given cycle ABCDA, the heat required for an ideal monoatomic gas will be:
Three identical rods are joined as shown in the figure. The left and right ends are kept at \( 0^\circ C \) and \( 90^\circ C \) as shown in the figure. The temperature \( \theta \) at the junction of the rods is: