Archimedes' Principle — Question 5

Section 14-6 · Physics pages 2160–2161

Question 5 Melting floating ice depends on the receiving liquid A 2.0 kg piece of pure ice floats in a uniform liquid of density 1200 kg/m3. On melting it becomes water of density 1000 kg/m3. Assume volume additivity on mixing, no evaporation or thermal expansion, and negligible air buoyancy. The container has constant horizontal area 0.10 m2. ice Floating ice initially displaces the receiving liquid; after melting, the added water volume is set by water density. (a) Find the level change after melting. (b) Explain why the familiar no-change result for ice floating in fresh water does not apply here, and recover it as a limiting case.
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Question 5 - Solution Melting floating ice depends on the receiving liquid ice (a) Derivation and calculation Vi = m/ρℓ= 2.0/1200 = .00166667 m3. Vf = m/ρw = 2.0/1000 = .00200000 m3. ∆h = Vf −Vi A = .000333333 .100 = .00333333 m upward . (b) Result and interpretation In general, ∆h = m A ( 1 ρw −1 ρℓ ) . ρℓ= ρw ⇒∆h = 0. Here the denser receiving liquid requires less displacement than the final meltwater volume. Mixing contraction and thermal volume changes are excluded. Physical check The no-change result depends on equality of receiving-liquid and meltwater densities, not on ice density.

Question 5

Melting floating ice depends on the receiving liquid

A 2.0kg2.0\,\mathrm{kg} piece of pure ice floats in a uniform liquid of density 1200kg/m31200\,\mathrm{kg/m^3}. On melting it becomes water of density 1000kg/m31000\,\mathrm{kg/m^3}. Assume volume additivity on mixing, no evaporation or thermal expansion, and negligible air buoyancy. The container has constant horizontal area 0.10m20.10\,\mathrm{m^2}.

Diagram shown in the original SVG worksheet.

  1. Find the level change after melting.

  2. Explain why the familiar no-change result for ice floating in fresh water does not apply here, and recover it as a limiting case.

Question 5 - Solution

Melting floating ice depends on the receiving liquid

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Vi=m/ρℓ=2.0/1200=.00166667m3.V_i=m/\rho_\ell=2.0/1200=.00166667\,\mathrm{m^3}.Vf=m/ρw=2.0/1000=.00200000m3.V_f=m/\rho_w=2.0/1000=.00200000\,\mathrm{m^3}.Δh=Vf−ViA=.000333333.100=.00333333mupward.\boxed{\Delta h=\frac{V_f-V_i}{A}=\frac{.000333333}{.100}=.00333333\,\mathrm m\ \text{upward}}.

(b) Result and interpretation

In general,Δh=mA(1ρw−1ρℓ).\boxed{\Delta h=\frac mA\left(\frac1{\rho_w}-\frac1{\rho_\ell}\right)}.ρℓ=ρw⇒Δh=0.\rho_\ell=\rho_w\Rightarrow\Delta h=0.Here the denser receiving liquid requires less displacement than the final meltwater volume. Mixing contraction and thermal volume changes are excluded.

Physical check

The no-change result depends on equality of receiving-liquid and meltwater densities, not on ice density.