The Molar Specific Heats of an Ideal Gas — Question 10

Section 19-7 · Physics pages 3170–3171

Question 10 A controlled cooling transient identifies heat capacity from its time scale A rigid vessel contains .500 mol of ideal gas with constant CV and negligible vessel heat capacity. Heat loss follows ˙Q = −G(T −Ta) with G = .250 W/K and room temperature Ta = 300 K. A small fan keeps the gas uniform without significant energy input. Starting at 360 K, the gas reaches 330 K after 40.0 ln 2 seconds. t T −Ta Axes and labels specify the model; the sketch is schematic. (a) Derive the temperature history and infer CV from the measurement. (b) How long after the start does temperature reach 315 K? If the gas amount doubles with unchanged G and CV , how does that time change?
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Question 10 - Solution A controlled cooling transient identifies heat capacity from its time scale t T −Ta (a) Method and calculation nCV dT dt = −G(T −Ta) ⇒T −Ta = (Ti −Ta)e−t/τ, τ = nCV G . 330 −300 360 −300 = 1 2 = e−(40 ln 2)/τ ⇒τ = 40.0 s, CV = Gτ n = 20.0 J/(mol K). (b) Interpretation and further calculation 315 −300 360 −300 = 1 4 ⇒t = τ ln 4 = 80.0 ln 2 s ≈55.4518 s. n →2n ⇒τ →2τ, t →110.904 s. The capacity is inferred from the decay curve without assigning a molecular model. Physical check The time scale determines total thermal capacity divided by conductance; a nonnegligible vessel would add to the inferred total.

Question 10

A controlled cooling transient identifies heat capacity from its time scale

A rigid vessel contains .500 mol of ideal gas with constant CVC_V and negligible vessel heat capacity. Heat loss follows Q̇=−G(T−Ta)\dot Q=-G(T-T_a) with G=.250G=.250 W/K and room temperature Ta=300T_a=300 K. A small fan keeps the gas uniform without significant energy input. Starting at 360 K, the gas reaches 330 K after 40.0ln⁡240.0\ln2 seconds.

Diagram shown in the original SVG worksheet.

  1. Derive the temperature history and infer CVC_V from the measurement.

  2. How long after the start does temperature reach 315 K? If the gas amount doubles with unchanged GG and CVC_V, how does that time change?

Question 10 - Solution

A controlled cooling transient identifies heat capacity from its time scale

Diagram shown in the original SVG worksheet.

(a) Method and calculation

nCVdTdt=−G(T−Ta)⇒T−Ta=(Ti−Ta)e−t/τ,τ=nCVG.nC_V\frac{dT}{dt}=-G(T-T_a)\ \Rightarrow\ T-T_a=(T_i-T_a)e^{-t/\tau},\quad\tau=\frac{nC_V}{G}.330−300360−300=12=e−(40ln⁡2)/τ⇒τ=40.0s,CV=Gτn=20.0J/(molK).\frac{330-300}{360-300}=\frac12=e^{-(40\ln2)/\tau}\ \Rightarrow\tau=40.0\,\mathrm s,\quad C_V=\frac{G\tau}{n} =20.0\,\mathrm{J/(mol\,K)}.

(b) Interpretation and further calculation

315−300360−300=14⇒t=τln⁡4=80.0ln⁡2s≈55.4518s.\frac{315-300}{360-300}=\frac14\ \Rightarrow\ t=\tau\ln4=80.0\ln2\,\mathrm s\approx55.4518\,\mathrm s.n→2n⇒τ→2τ,t→110.904s.n\to2n\ \Rightarrow\tau\to2\tau,\quad t\to110.904\,\mathrm s.The capacity is inferred from the decay curve without assigning a molecular model.

Physical check

The time scale determines total thermal capacity divided by conductance; a nonnegligible vessel would add to the inferred total.