To determine the average power dissipated by the circuit, we first calculate the total impedance \( Z \) of the series circuit. The inductor's reactance \( X_L \) is \( 100 \, \Omega \), the capacitor's reactance \( X_C \) is \( 50 \, \Omega \), and the resistor's resistance \( R \) is \( 50 \, \Omega \). The formula for total impedance in a series circuit is:
\( Z = \sqrt{R^2 + (X_L - X_C)^2} \)
Substituting the values, we compute:
\( Z = \sqrt{50^2 + (100 - 50)^2} = \sqrt{50^2 + 50^2} = \sqrt{2500 + 2500} = \sqrt{5000} \)
\( Z = 50\sqrt{2} \, \Omega \)
The voltage \( V \) supplied by the AC source is \( 10 \, V \). The root mean square (RMS) current \( I \) is given by \( I = \frac{V}{Z} \):
\( I = \frac{10}{50\sqrt{2}} = \frac{1}{5\sqrt{2}} \, \text{A} \)
The average power dissipated by a resistive element in an AC circuit is determined by the formula:
\( P = I^2 \cdot R \)
Plugging in the RMS current and resistance values, we calculate:
\( P = \left(\frac{1}{5\sqrt{2}}\right)^2 \cdot 50 = \frac{1}{50} \cdot 50 = 1 \, \text{W} \)
The computed average power dissipated, \( 1 \, \text{W} \), falls within the expected range of \( 1,1 \). Hence, the average power dissipated by the circuit is 1 W.
Step 1: Identify the given parameters.
Inductive reactance, \( X_L = 100 \, \Omega \)
Capacitive reactance, \( X_C = 50 \, \Omega \)
Resistance, \( R = 50 \, \Omega \)
RMS voltage of the AC source, \( V_{rms} = 10 \, V \)
Frequency of the AC source, \( f = 50 \, Hz \)
Step 2: Calculate the impedance \( Z \) of the series LCR circuit.
The impedance of a series LCR circuit is given by: \[ Z = \sqrt{R^2 + (X_L - X_C)^2} \] Substitute the given values: \[ Z = \sqrt{(50 \, \Omega)^2 + (100 \, \Omega - 50 \, \Omega)^2} \] \[ Z = \sqrt{(50)^2 + (50)^2} = \sqrt{2500 + 2500} = \sqrt{5000} \, \Omega \] \[ Z = 50\sqrt{2} \, \Omega \]
Step 3: Calculate the RMS current \( I_{rms} \) in the circuit.
Using Ohm's law for AC circuits: \[ I_{rms} = \frac{V_{rms}}{Z} \] Substitute the values of \( V_{rms} \) and \( Z \): \[ I_{rms} = \frac{10 \, V}{50\sqrt{2} \, \Omega} = \frac{1}{5\sqrt{2}} \, A = \frac{\sqrt{2}}{10} \, A \]
Step 4: Calculate the average power \( P_{avg} \) dissipated by the circuit.
The average power dissipated in an AC circuit is only through the resistor and is given by: \[ P_{avg} = I_{rms}^2 R \] Substitute the values of \( I_{rms} \) and \( R \): \[ P_{avg} = \left(\frac{\sqrt{2}}{10} \, A\right)^2 \times 50 \, \Omega \] \[ P_{avg} = \left(\frac{2}{100}\right) \times 50 \, W \] \[ P_{avg} = \frac{1}{50} \times 50 \, W \] \[ P_{avg} = 1 \, W \] The average power dissipated by the circuit is 1 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 : \(A_2 \rightleftharpoons 2A\)