Heat Transfer Mechanisms — Question 5

Section 18-11 · Physics pages 3020–3021

Question 5 Convective cooling reveals a heat-transfer coefficient A small body remains nearly uniform in temperature and has heat capacity C = 600 J/K and exposed area .0500 m2. It cools by convection alone in air at 290 K, obeying C dT/dt = −hA(T −290) with constant h. Starting at 350 K, it reaches 320 K after 120 s. t T −T∞ Axes and labels specify the model; the sketch is schematic. (a) Infer h and the thermal time constant. (b) Find the time from the start at which the body reaches 300 K and the heat lost by that time.
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Question 5 - Solution Convective cooling reveals a heat-transfer coefficient t T −T∞ (a) Method and calculation T −290 = (350 −290)e−t/τ, τ = C hA. 320 −290 350 −290 = 1 2 = e−120/τ ⇒τ = 120/ ln 2 = 173.123 s. h = 600 ln 2 .0500(120) = 69.3147 W/(m2K). (b) Interpretation and further calculation 300 −290 60 = 1 6 = e−t/τ ⇒t = 120 ln 6 ln 2 = 310.196 s. Qout = C(350 −300) = 30000 J. The uniform-temperature assumption concerns fast internal equilibration; it is separate from the external convection law. Physical check The body approaches the ambient temperature asymptotically; the exponential model does not reach it in finite time.

Question 5

Convective cooling reveals a heat-transfer coefficient

A small body remains nearly uniform in temperature and has heat capacity C=600J/KC=600\,\mathrm{J/K} and exposed area .0500m2.0500\,\mathrm{m^2}. It cools by convection alone in air at 290 K, obeying CdT/dt=−hA(T−290)C\,dT/dt=-hA(T-290) with constant hh. Starting at 350 K, it reaches 320 K after 120 s.

Diagram shown in the original SVG worksheet.

  1. Infer hh and the thermal time constant.

  2. Find the time from the start at which the body reaches 300 K and the heat lost by that time.

Question 5 - Solution

Convective cooling reveals a heat-transfer coefficient

Diagram shown in the original SVG worksheet.

(a) Method and calculation

T−290=(350−290)e−t/τ,τ=ChA.T-290=(350-290)e^{-t/\tau},\quad\tau=\frac C{hA}.320−290350−290=12=e−120/τ⇒τ=120/ln⁡2=173.123s.\frac{320-290}{350-290}=\frac12=e^{-120/\tau}\ \Rightarrow\ \tau=120/\ln2=173.123\,\mathrm s.h=600ln⁡2.0500(120)=69.3147W/(m2K).h=\frac{600\ln2}{.0500(120)}=69.3147\,\mathrm{W/(m^2K)}.

(b) Interpretation and further calculation

300−29060=16=e−t/τ⇒t=120ln⁡6ln⁡2=310.196s.\frac{300-290}{60}=\frac16=e^{-t/\tau}\ \Rightarrow\ t=\frac{120\ln6}{\ln2}=310.196\,\mathrm s.Qout=C(350−300)=30000J.Q_{\mathrm{out}}=C(350-300)=30000\,\mathrm J.The uniform-temperature assumption concerns fast internal equilibration; it is separate from the external convection law.

Physical check

The body approaches the ambient temperature asymptotically; the exponential model does not reach it in finite time.