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.
\[ I_0 = \frac{E}{R} \quad \Rightarrow \quad I' = \frac{I_0}{2}. \]
\[ \boxed{I' = \dfrac{I_0}{2}} \]
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
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:
Consider the sound wave travelling in ideal gases of $\mathrm{He}, \mathrm{CH}_{4}$, and $\mathrm{CO}_{2}$. All the gases have the same ratio $\frac{\mathrm{P}}{\rho}$, where P is the pressure and $\rho$ is the density. The ratio of the speed of sound through the gases $\mathrm{v}_{\mathrm{He}}: \mathrm{v}_{\mathrm{CH}_{4}}: \mathrm{v}_{\mathrm{CO}_{2}}$ is given by