Heat Transfer Mechanisms — Question 3

Section 18-11 · Physics pages 3016–3017

Question 3 Temperature-dependent conductivity creates a curved profile A plane slab has length L = .200 m, area .0100 m2, and conductivity k(T) = k0[1 + b(T −300)], with k0 = 10.0 W/(m K), b = .0100 K−1. Its faces at x = 0, L are held at 400 K and 300 K. Use steady P = −Ak(T)dT/dx, with no generation or lateral loss. x T −300 The nonlinear profile lies above the straight endpoint chord. (a) Integrate the conduction law to find the heat rate. (b) Find the temperature at x = L/2 and explain why it is not the arithmetic mean of the face temperatures.
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Question 3 - Solution Temperature-dependent conductivity creates a curved profile x T −300 (a) Method and calculation PL A = ∫400 300 k(T)dT = k0 [ ∆T + b 2(∆T)2 ] = 1500 W/m. P = .0100 .200 (1500) = 75.0 W. (b) Interpretation and further calculation Let θ = T −300. Integrating from position x to the cold face gives θ + .005θ2 = 150(1 −x/L). x = L/2 : .005θ2 + θ −75 = 0 ⇒θ = −100 + √ 25000 = 58.1139 K. T(L/2) = 358.114 K. The hot region has larger conductivity and hence a smaller magnitude of temperature gradient for the same heat rate. Physical check The endpoint-averaged conductivity gives the exact total rate here because k is linear in temperature, but it does not make T(x) linear.

Question 3

Temperature-dependent conductivity creates a curved profile

A plane slab has length L=.200L=.200 m, area .0100m2.0100\,\mathrm{m^2}, and conductivity k(T)=k0[1+b(T−300)]k(T)=k_0[1+b(T-300)], with k0=10.0k_0=10.0 W/(m K), b=.0100K−1b=.0100\,\mathrm{K^{-1}}. Its faces at x=0,Lx=0,L are held at 400 K and 300 K. Use steady P=−Ak(T)dT/dxP=-Ak(T)dT/dx, with no generation or lateral loss.

Diagram shown in the original SVG worksheet.

  1. Integrate the conduction law to find the heat rate.

  2. Find the temperature at x=L/2x=L/2 and explain why it is not the arithmetic mean of the face temperatures.

Question 3 - Solution

Temperature-dependent conductivity creates a curved profile

Diagram shown in the original SVG worksheet.

(a) Method and calculation

PLA=∫300400k(T)dT=k0[ΔT+b2(ΔT)2]=1500W/m.\frac{PL}{A}=\int_{300}^{400}k(T)dT=k_0\left[\Delta T+\frac b2(\Delta T)^2\right]=1500\,\mathrm{W/m}.P=.0100.200(1500)=75.0W.P=\frac{.0100}{.200}(1500)=75.0\,\mathrm W.

(b) Interpretation and further calculation

Let θ=T−300\theta=T-300. Integrating from position xx to the cold face givesθ+.005θ2=150(1−x/L).\theta+.005\theta^2=150(1-x/L).x=L/2:.005θ2+θ−75=0⇒θ=−100+25000=58.1139K.x=L/2:\quad .005\theta^2+\theta-75=0\ \Rightarrow\ \theta=-100+\sqrt{25000}=58.1139\,\mathrm K.T(L/2)=358.114K.T(L/2)=358.114\,\mathrm K.The hot region has larger conductivity and hence a smaller magnitude of temperature gradient for the same heat rate.

Physical check

The endpoint-averaged conductivity gives the exact total rate here because kk is linear in temperature, but it does not make T(x)T(x) linear.