Step 1: Fix which fluid touches which surface.
The figure shows Fluid 2 running straight through the inner tube's core between $20^{\circ}$C and $30^{\circ}$C, and Fluid 1 connecting to the annulus around it, between $60^{\circ}$C and $40^{\circ}$C, so heat moves from Fluid 1 in the annulus into Fluid 2 in the core, in a counter-flow pattern.
Step 2: Build the overall coefficient from the individual resistances.
With $r_i=0.010$ m, $r_o=0.011$ m, $L=1$ m, $h_i=80$ W/(m$^2$K) for Fluid 2 and $h_o=50$ W/(m$^2$K) for Fluid 1: $\dfrac{1}{UA} = \dfrac{1}{h_iA_i} + \dfrac{\ln(r_o/r_i)}{2\pi k L} + \dfrac{1}{h_oA_o}$.
Step 3: Compute each term.
$A_i = 2\pi(0.010)(1) = 0.06283$ m$^2$, so $1/(h_iA_i) = 1/(80\times0.06283) = 0.1989$ K/W.
$\ln(r_o/r_i)/(2\pi kL) = \ln(1.1)/(2\pi\times386) = 0.0000393$ K/W, negligible next to the convective terms.
$A_o = 2\pi(0.011)(1) = 0.06912$ m$^2$, so $1/(h_oA_o) = 1/(50\times0.06912) = 0.2894$ K/W.
Step 4: Sum and invert.
Total $= 0.1989+0.0000393+0.2894 = 0.4884$ K/W, so $UA = 2.048$ W/K.
Step 5: Bring in the LMTD for the counter-flow ends.
End differences are $60-30=30$ K and $40-20=20$ K, so LMTD $= (30-20)/\ln(30/20) = 10/0.4055 = 24.66$ K.
Step 6: Multiply to get the duty.
$Q = UA \times \text{LMTD} = 2.048 \times 24.66 = 50.5$ W.
Final Answer:
Whether the resistance is tracked from the inside out or folded straight into $UA$, the exchanged heat comes out the same.
\[ \boxed{Q = 50.5 \ \text{W}} \]