Step 1: Set up the two heat loss paths.
Wire radius \( r_1 = 1\,mm = 0.001\,m \). Insulation adds 2 mm, so outer radius \( r_2 = 3\,mm = 0.003\,m \).
Surface temperature stays fixed at \( T_s = 420\,K \), and air is at \( T_\infty = 320\,K \), so \( \Delta T = 100\,K \) in both cases.
Step 2: Heat loss without insulation (pure convection).
\( Q_1 = h(2\pi r_1)\Delta T = 25 \times 2 \times 3.14 \times 0.001 \times 100 = 15.7\ W/m \).
Step 3: Heat loss with insulation (conduction plus convection in series).
Conduction resistance of the plastic layer: \( R_{cond} = \dfrac{\ln(r_2/r_1)}{2\pi k} = \dfrac{\ln 3}{2 \times 3.14 \times 0.5} = \dfrac{1.099}{3.14} = 0.350\ m.K/W \).
Convection resistance at the outer surface: \( R_{conv} = \dfrac{1}{h(2\pi r_2)} = \dfrac{1}{25 \times 2 \times 3.14 \times 0.003} = 2.123\ m.K/W \).
Total resistance \( R = 0.350 + 2.123 = 2.473\ m.K/W \), so \( Q_2 = \Delta T / R = 100/2.473 = 40.4\ W/m \).
Step 4: Take the ratio asked in the question.
\( \dfrac{Q_2}{Q_1} = \dfrac{40.4}{15.7} = 2.58 \).
Final Answer:
The insulated wire actually loses more heat per metre because the outer radius sits well below the critical radius of insulation, giving ratio 2.58, option (A).
\[ \boxed{Q_{ins}/Q_{bare} \approx 2.58} \]