Step 1: Recall the formula for current amplitude in a series LCR circuit.
The current amplitude is given by: \[ I = \frac{E}{Z}, \] where \( Z \) is the impedance of the circuit: \[ Z = \sqrt{R^2 + (X_L - X_C)^2}. \]
Step 2: At resonance condition.
At resonance, \( X_L = X_C \). Thus, impedance becomes minimum: \[ Z = R. \] Therefore, current amplitude at resonance is: \[ I_0 = \frac{E}{R}. \]
Step 3: When resistance is doubled.
If resistance becomes \( 2R \), then the new impedance at resonance is: \[ Z' = 2R. \] Hence, the new current amplitude: \[ I' = \frac{E}{Z'} = \frac{E}{2R}. \]
Step 4: Relate new current with the original.
\[ I_0 = \frac{E}{R} \quad \Rightarrow \quad I' = \frac{I_0}{2}. \]
\[ \boxed{I' = \dfrac{I_0}{2}} \]
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,

For the AC circuit shown in the figure, $ R = 100 \, \text{k}\Omega $ and $ C = 100 \, \text{pF} $, and the phase difference between $ V_{\text{in}} $ and $ (V_B - V_A) $ is 90°. The input signal frequency is $ 10^x $ rad/sec, where $ x $ is:
An alternating current is represented by the equation, $\mathrm{i}=100 \sqrt{2} \sin (100 \pi \mathrm{t})$ ampere. The RMS value of current and the frequency of the given alternating current are

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 : \(A_2 \rightleftharpoons 2A\)