The Absorption of Heat by Solids and Liquids — Question 4

Section 18-7 · Physics pages 2938–2939

Question 4 Partial ice melting requires a phase check before solving for temperature An insulated cup of negligible heat capacity contains .200 kg water at 20.0◦C. Add .100 kg ice at −10.0◦C. Use cw = 4200, ci = 2100 J/(kg K) and Lf = 334000 J/kg. Equilibrium melting occurs at 0◦C. water + ice Schematic; labels, not drawing lengths, specify the data. (a) Determine final temperature and the masses of remaining ice and liquid. (b) Find the minimum initial water temperature that would just melt all the ice, with final temperature 0◦C.
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Question 4 - Solution Partial ice melting requires a phase check before solving for temperature water + ice (a) Method and calculation Qw→0 = .200(4200)(20) = 16800 J, Qi→0 = .100(2100)(10) = 2100 J. mmelt = 16800 −2100 334000 = .0440120 kg < .100 kg. Both phases remain at 0◦C: mi = .0559880 kg and mw = .2440120 kg. (b) Interpretation and further calculation .200(4200)Tw,min = 2100 + .100(334000). Tw,min = 35500 840 = 42.2619◦C. A single-phase mixing equation would be invalid for the original run because the available heat cannot finish melting. Physical check Check the phase-energy budget first; a negative temperature from an all-liquid assumption would signal the wrong branch.

Question 4

Partial ice melting requires a phase check before solving for temperature

An insulated cup of negligible heat capacity contains .200 kg water at 20.0∘20.0^\circC. Add .100 kg ice at −10.0∘-10.0^\circC. Use cw=4200c_w=4200, ci=2100c_i=2100 J/(kg K) and Lf=334000L_f=334000 J/kg. Equilibrium melting occurs at 0∘0^\circC.

Diagram shown in the original SVG worksheet.

  1. Determine final temperature and the masses of remaining ice and liquid.

  2. Find the minimum initial water temperature that would just melt all the ice, with final temperature 0∘0^\circC.

Question 4 - Solution

Partial ice melting requires a phase check before solving for temperature

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qw→0=.200(4200)(20)=16800J,Qi→0=.100(2100)(10)=2100J.Q_{w\to0}=.200(4200)(20)=16800\,\mathrm J,\quad Q_{i\to0}=.100(2100)(10)=2100\,\mathrm J.mmelt=16800−2100334000=.0440120kg<.100kg.m_{\mathrm{melt}}=\frac{16800-2100}{334000}=.0440120\,\mathrm{kg}<.100\,\mathrm{kg}.Both phases remain at 0∘0^\circC: mi=.0559880m_i=.0559880 kg and mw=.2440120m_w=.2440120 kg.

(b) Interpretation and further calculation

.200(4200)Tw,min=2100+.100(334000)..200(4200)T_{w,\min}=2100+.100(334000).Tw,min=35500840=42.2619∘C.T_{w,\min}=\frac{35500}{840}=42.2619^\circ\mathrm C.A single-phase mixing equation would be invalid for the original run because the available heat cannot finish melting.

Physical check

Check the phase-energy budget first; a negative temperature from an all-liquid assumption would signal the wrong branch.