Step 1: Read the flow arrangement from the figure.
Fluid 2 flows along the central axis of the inner tube, entering at \(20^{\circ}\)C and leaving at \(30^{\circ}\)C, while Fluid 1 connects to the annulus around the inner tube, entering at \(60^{\circ}\)C and leaving at \(40^{\circ}\)C, so the two streams flow counter to each other.
Step 2: Assign the convective coefficients to the correct surfaces.
Fluid 2 (inside the inner tube) has \(h_i = 80\) W/(m\(^2\)K), acting on the tube's inner surface of radius \(r_i=0.010\) m. Fluid 1 (in the annulus) has \(h_o = 50\) W/(m\(^2\)K), acting on the tube's outer surface of radius \(r_o = 0.011\) m.
Step 3: Compute the three resistances in the tube wall, for length \(L=1\) m.
Inner convection: \(A_i=2\pi r_iL=0.06283\) m\(^2\), \(R_i=\dfrac{1}{h_iA_i}=\dfrac{1}{80(0.06283)}=0.1989\) K/W.
Wall conduction: \(R_{wall}=\dfrac{\ln(r_o/r_i)}{2\pi kL}=\dfrac{\ln(1.1)}{2\pi(386)}=\dfrac{0.0953}{2425.3}=0.0000393\) K/W, very small since the tube conducts well.
Outer convection: \(A_o=2\pi r_oL=0.06912\) m\(^2\), \(R_o=\dfrac{1}{h_oA_o}=\dfrac{1}{50(0.06912)}=0.2894\) K/W.
Step 4: Add the resistances and get \(UA\).
\(R_{total}=0.1989+0.00004+0.2894=0.4884\) K/W, so \(UA=1/R_{total}=2.048\) W/K.
Step 5: Find the LMTD for the counter-flow arrangement.
At one end, \(\Delta T_A = 60-30=30^{\circ}\)C; at the other end, \(\Delta T_B=40-20=20^{\circ}\)C. \(\text{LMTD}=\dfrac{\Delta T_A-\Delta T_B}{\ln(\Delta T_A/\Delta T_B)}=\dfrac{10}{\ln(1.5)}=\dfrac{10}{0.4055}=24.66^{\circ}\)C.
Step 6: Get the heat transfer rate.
\(Q=UA\times\text{LMTD}=2.048(24.66)=50.5\) W.
Final Answer:
Adding the three resistances in series to build \(UA\), then multiplying by the counter-flow LMTD, gives the total heat duty.
\[ \boxed{Q = 50.5 \ \text{W}} \]