Temperature — Question 7

Section 18-1 · Physics pages 2824–2825

Question 7 Equal temperature can coexist with different phase energy At a fixed pressure, liquid and solid forms of an ideal substance coexist at Tm = 300 K. For a 2.0 kg sample, the supplied phase-energy model at Tm is U = Us + fmℓ, where f is liquid mass fraction and ℓ= 100 kJ/kg. Two equilibrium preparations have fA = .20 and fB = .80. solid + liquid T = Tm Schematic; labels, not drawing lengths, specify the data. (a) Find UB −UA. Does a temperature measurement distinguish the two liquid fractions? (b) Preparation A gains 40 kJ solely by melting while remaining at coexistence. Find its new fraction and temperature.
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Question 7 - Solution Equal temperature can coexist with different phase energy solid + liquid T = Tm (a) Method and calculation UB −UA = (fB −fA)mℓ= .60(2)(100) = 120 kJ. TA = TB = Tm = 300 K. A single temperature does not fix the fraction of coexisting phases or the energy. (b) Interpretation and further calculation ∆f = ∆U mℓ= 40 2(100) = .20, ff = .40. Tf = 300 K. Because 0 < ff < 1, the specified coexistence model still applies; the energy changes phase fraction rather than temperature. Physical check This exercise supplies its phase-energy relation; quantitative calorimetry and latent heat are developed later in the chapter.

Question 7

Equal temperature can coexist with different phase energy

At a fixed pressure, liquid and solid forms of an ideal substance coexist at Tm=300KT_m=300\,\mathrm K. For a 2.0kg2.0\,\mathrm{kg} sample, the supplied phase-energy model at TmT_m is U=Us+fmℓU=U_s+fm\ell, where ff is liquid mass fraction and ℓ=100kJ/kg\ell=100\,\mathrm{kJ/kg}. Two equilibrium preparations have fA=.20f_A=.20 and fB=.80f_B=.80.

Diagram shown in the original SVG worksheet.

  1. Find UB−UAU_B-U_A. Does a temperature measurement distinguish the two liquid fractions?

  2. Preparation A gains 40kJ40\,\mathrm{kJ} solely by melting while remaining at coexistence. Find its new fraction and temperature.

Question 7 - Solution

Equal temperature can coexist with different phase energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

UB−UA=(fB−fA)mℓ=.60(2)(100)=120kJ.U_B-U_A=(f_B-f_A)m\ell=.60(2)(100)=120\,\mathrm{kJ}.TA=TB=Tm=300K.T_A=T_B=T_m=300\,\mathrm K.A single temperature does not fix the fraction of coexisting phases or the energy.

(b) Interpretation and further calculation

Δf=ΔUmℓ=402(100)=.20,ff=.40.\Delta f=\frac{\Delta U}{m\ell}=\frac{40}{2(100)}=.20,\qquad f_f=.40.Tf=300K.T_f=300\,\mathrm K.Because 0<ff<10<f_f<1, the specified coexistence model still applies; the energy changes phase fraction rather than temperature.

Physical check

This exercise supplies its phase-energy relation; quantitative calorimetry and latent heat are developed later in the chapter.