The Absorption of Heat by Solids and Liquids — Question 8

Section 18-7 · Physics pages 2946–2947

Question 8 Two heater powers separate heat capacity from steady loss At the same temperature, a well-mixed sample heats at .200 K/s with input power 100 W and at .500 K/s with input power 160 W. Its heat capacity C is constant; the environmental loss Pℓis the same in both instantaneous measurements. Use C ˙T = Pin −Pℓ. heater sample Pin Pℓ Schematic; labels, not drawing lengths, specify the data. (a) Infer C and Pℓ. (b) If sample mass is .400 kg, find its specific heat. Predict its instantaneous cooling slope when the heater is switched offat that temperature, and the power required for a .100 K/s rise.
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Question 8 - Solution Two heater powers separate heat capacity from steady loss heater sample Pin Pℓ (a) Method and calculation .200C = 100 −Pℓ, .500C = 160 −Pℓ. C = 60 .300 = 200 J/K, Pℓ= 100 −.200(200) = 60.0 W. (b) Interpretation and further calculation c = C/m = 500 J/(kg K), ˙Toff= −60/200 = −.300 K/s. P.100 = Pℓ+ C(.100) = 80.0 W. These are local predictions at the measured temperature, since the loss can change as temperature changes. Physical check Taking the difference of the two equations removes the unknown loss without pretending it is zero.

Question 8

Two heater powers separate heat capacity from steady loss

At the same temperature, a well-mixed sample heats at .200 K/s with input power 100 W and at .500 K/s with input power 160 W. Its heat capacity CC is constant; the environmental loss PℓP_\ell is the same in both instantaneous measurements. Use CṪ=Pin−PℓC\dot T=P_{\mathrm{in}}-P_\ell.

Diagram shown in the original SVG worksheet.

  1. Infer CC and PℓP_\ell.

  2. If sample mass is .400 kg, find its specific heat. Predict its instantaneous cooling slope when the heater is switched off at that temperature, and the power required for a .100 K/s rise.

Question 8 - Solution

Two heater powers separate heat capacity from steady loss

Diagram shown in the original SVG worksheet.

(a) Method and calculation

.200C=100−Pℓ,.500C=160−Pℓ..200C=100-P_\ell,\quad .500C=160-P_\ell.C=60.300=200J/K,Pℓ=100−.200(200)=60.0W.C=\frac{60}{.300}=200\,\mathrm{J/K},\quad P_\ell=100-.200(200)=60.0\,\mathrm W.

(b) Interpretation and further calculation

c=C/m=500J/(kgK),Ṫoff=−60/200=−.300K/s.c=C/m=500\,\mathrm{J/(kg\,K)},\quad\dot T_{\mathrm{off}}=-60/200=-.300\,\mathrm{K/s}.P.100=Pℓ+C(.100)=80.0W.P_{.100}=P_\ell+C(.100)=80.0\,\mathrm W.These are local predictions at the measured temperature, since the loss can change as temperature changes.

Physical check

Taking the difference of the two equations removes the unknown loss without pretending it is zero.