Archimedes' Principle — Question 2

Section 14-6 · Physics pages 2154–2155

Question 2 An object can float at an interface while fully submerged A rigid object of volume V and density 900 kg/m3 lies wholly below the free surface across an oil–water interface. Oil density is 800 and water density 1000 kg/m3. Ignore surface tension and assume sufficiently deep layers. oil water The object straddles the liquid interface and remains fully submerged. (a) Find the fraction of object volume in water at vertical equilibrium. (b) Explain the vertical response to a small upward displacement that transfers a positive volume δV from water into oil. Is that equilibrium restoring?
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Question 2 - Solution An object can float at an interface while fully submerged oil water (a) Derivation and calculation Let fV be in water and (1 −f)V in oil. Then B = gV [ρwf + ρo(1 −f)], W = ρbgV. ρb = ρo + (ρw −ρo)f ⇒f = 900 −800 1000 −800 = 1 2 . (b) Result and interpretation An upward displacement transfers δV > 0 from water to oil: δB = ρogδV −ρwgδV = −(ρw −ρo)gδV < 0 . δW = 0 ⇒net force becomes downward. The equilibrium is vertically restoring while the body still crosses the interface; rotational stability is a separate question. Physical check A physical fraction 0 < f < 1 requires the object density to lie between the two liquid densities.

Question 2

An object can float at an interface while fully submerged

A rigid object of volume VV and density 900kg/m3900\,\mathrm{kg/m^3} lies wholly below the free surface across an oil–water interface. Oil density is 800800 and water density 1000kg/m31000\,\mathrm{kg/m^3}. Ignore surface tension and assume sufficiently deep layers.

Diagram shown in the original SVG worksheet.

  1. Find the fraction of object volume in water at vertical equilibrium.

  2. Explain the vertical response to a small upward displacement that transfers a positive volume δV\delta V from water into oil. Is that equilibrium restoring?

Question 2 - Solution

An object can float at an interface while fully submerged

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Let fVfV be in water and (1−f)V(1-f)V in oil. ThenB=gV[ρwf+ρo(1−f)],W=ρbgV.B=gV[\rho_wf+\rho_o(1-f)],\quad W=\rho_bgV.ρb=ρo+(ρw−ρo)f⇒f=900−8001000−800=12.\rho_b=\rho_o+(\rho_w-\rho_o)f\Rightarrow\boxed{f=\frac{900-800}{1000-800}=\frac12}.

(b) Result and interpretation

An upward displacement transfers δV>0\delta V>0 from water to oil:δB=ρogδV−ρwgδV=−(ρw−ρo)gδV<0.\delta B=\rho_og\delta V-\rho_wg\delta V=\boxed{-(\rho_w-\rho_o)g\delta V<0}.δW=0⇒net force becomes downward.\delta W=0\Rightarrow\text{net force becomes downward}.The equilibrium is vertically restoring while the body still crosses the interface; rotational stability is a separate question.

Physical check

A physical fraction 0<f<10<f<1 requires the object density to lie between the two liquid densities.