Step 1: The steel core and the copper sheath share the same length \(L\) and the same end faces, so they carry current in parallel. Compute each resistance separately.
Step 2: The steel core has radius \(r\), so its cross-sectional area is \(A_1 = \pi r^2\).
\[R_1 = \frac{\rho_1 L}{\pi r^2}\]
Step 3: The copper sheath is an annulus of inner radius \(r\) and outer radius \(2r\) (thickness \(r\)). Its area is
\[A_2 = \pi\big((2r)^2 - r^2\big) = \pi(4r^2 - r^2) = 3\pi r^2\]
\[R_2 = \frac{\rho_2 L}{3\pi r^2}\]
Step 4: Combine in parallel:
\[R = \frac{R_1 R_2}{R_1 + R_2}\]
Numerator: \(R_1 R_2 = \dfrac{\rho_1 \rho_2 L^2}{3\pi^2 r^4}\).
Denominator: \(R_1 + R_2 = \dfrac{L}{\pi r^2}\left(\rho_1 + \dfrac{\rho_2}{3}\right) = \dfrac{L(3\rho_1 + \rho_2)}{3\pi r^2}\).
Step 5: Divide:
\[R = \frac{\rho_1 \rho_2 L^2}{3\pi^2 r^4} \times \frac{3\pi r^2}{L(3\rho_1 + \rho_2)} = \frac{\rho_1 \rho_2 L}{\pi r^2 (3\rho_1 + \rho_2)}\]
This matches option (A).
\[\boxed{R = \dfrac{\rho_1 \rho_2 L}{\pi r^2 (3\rho_1 + \rho_2)}}\]