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.
\[ I_0 = \frac{E}{R} \quad \Rightarrow \quad I' = \frac{I_0}{2}. \]
\[ \boxed{I' = \dfrac{I_0}{2}} \]

Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}