The Absorption of Heat by Solids and Liquids — Question 2

Section 18-7 · Physics pages 2934–2935

Question 2 Variable specific heat changes the calorimetric inversion A .500 kg solid has c(T) = 400 + 2(T −300) J/(kg K) for 300 ≤T ≤400 K. It starts at 300 K and receives 12.0 kJ without losses, phase change or mechanical work. T −300 c 400 Axes and labels specify the model; the sketch is schematic. (a) Integrate Q = m ∫c(T) dT to find its final temperature. (b) Find the error caused by treating c as its initial value. Determine the mean specific heat over the actual temperature interval.
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Question 2 - Solution Variable specific heat changes the calorimetric inversion T −300 c 400 (a) Method and calculation Let x = Tf −300. 12000 = .500 ∫x 0 (400 + 2u)du = .500(400x + x2). x = −400 + √ 4002 + 96000 2 ≈52.9822 K, Tf ≈352.982 K. The other quadratic root lies outside the specified domain. (b) Interpretation and further calculation xc0 = 12000 .500(400) = 60.0 K. xc0 −x ≈7.0178 K, c = Q mx = 400 + x ≈452.982 J/(kg K). Using the smaller initial capacity overpredicts the rise. Physical check The recovered final temperature lies within the coefficient law's stated range.

Question 2

Variable specific heat changes the calorimetric inversion

A .500 kg solid has c(T)=400+2(T−300)c(T)=400+2(T-300) J/(kg K) for 300≤T≤400300\le T\le400 K. It starts at 300 K and receives 12.0 kJ without losses, phase change or mechanical work.

Diagram shown in the original SVG worksheet.

  1. Integrate Q=m∫c(T)dTQ=m\int c(T)\,dT to find its final temperature.

  2. Find the error caused by treating cc as its initial value. Determine the mean specific heat over the actual temperature interval.

Question 2 - Solution

Variable specific heat changes the calorimetric inversion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Let x=Tf−300x=T_f-300.12000=.500∫0x(400+2u)du=.500(400x+x2).12000=.500\int_0^x(400+2u)du=.500(400x+x^2).x=−400+4002+960002≈52.9822K,Tf≈352.982K.x=\frac{-400+\sqrt{400^2+96000}}2\approx52.9822\,\mathrm K,\quad T_f\approx352.982\,\mathrm K.The other quadratic root lies outside the specified domain.

(b) Interpretation and further calculation

xc0=12000.500(400)=60.0K.x_{c_0}=\frac{12000}{.500(400)}=60.0\,\mathrm K.xc0−x≈7.0178K,c¯=Qmx=400+x≈452.982J/(kgK).x_{c_0}-x\approx7.0178\,\mathrm K,\quad\overline c=\frac{Q}{mx}=400+x\approx452.982\,\mathrm{J/(kg\,K)}.Using the smaller initial capacity overpredicts the rise.

Physical check

The recovered final temperature lies within the coefficient law's stated range.