For DC voltage:
\[ R = \frac{V}{I} = \frac{100}{5} = 20 \, \Omega \]
For AC voltage:
\[ X_L = 20\sqrt{3} \, \Omega \]
\[ Z = \sqrt{X_L^2 + R^2} = \sqrt{(20\sqrt{3})^2 + 20^2} = \sqrt{1200 + 400} = 40 \, \Omega \]
Power dissipated in the circuit:
\[ P = I_\text{rms}^2 R = \left( \frac{V_\text{rms}}{Z} \right)^2 \times R \]
\[ P = \left( \frac{200}{\sqrt{2} \times 40} \right)^2 \times 20 \]
\[ P = \left( \frac{200}{40\sqrt{2}} \right)^2 \times 20 = 250 \, \text{W} \]
Let's solve the problem step-by-step to find the power dissipated in the circuit.
First, we have a DC voltage of 100 V causing a DC current of 5 A to flow through the inductor. Since the current flows, the resistance \( R \) of the inductor can be determined using Ohm's law \( V = IR \). Thus:
\( R = \frac{V}{I} = \frac{100\,\text{V}}{5\,\text{A}} = 20\,\Omega \).
Now, consider the AC voltage scenario. Given the AC peak voltage \( V_0 = 200\,\text{V} \), the inductive reactance \( X_L = 20\sqrt{3}\,\Omega \) is provided. The impedance \( Z \) of the inductor in the AC circuit is therefore:
\( Z = \sqrt{R^2 + X_L^2} = \sqrt{20^2 + (20\sqrt{3})^2} \).
Calculating each term:
\( 20^2 = 400 \).
\((20\sqrt{3})^2 = 400 \times 3 = 1200 \).
Thus:
\( Z = \sqrt{400 + 1200} = \sqrt{1600} = 40\,\Omega \).
Next, calculate the RMS value of the AC voltage \( V_{\text{rms}} \):
\( V_{\text{rms}} = \frac{V_0}{\sqrt{2}} = \frac{200}{\sqrt{2}} = 100\sqrt{2}\,\text{V} \).
The RMS current \( I_{\text{rms}} \) through the inductor can be calculated as:
\( I_{\text{rms}} = \frac{V_{\text{rms}}}{Z} = \frac{100\sqrt{2}}{40} = \frac{5\sqrt{2}}{2}\,\text{A} \).
The power dissipated in the circuit, primarily due to the resistor, is given by \( P = I_{\text{rms}}^2 \times R \):
\( P = \left(\frac{5\sqrt{2}}{2}\right)^2 \times 20 \).
Calculating further:
\( \left(\frac{5\sqrt{2}}{2}\right)^2 = \frac{25 \times 2}{4} = 12.5 \).
Therefore,
\( P = 12.5 \times 20 = 250\,\text{W} \).
Hence, the power dissipated in the circuit is 250 W, which is within the given range of 250,250 W.
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)