Fluids at Rest — Question 3

Section 14-3 · Physics pages 2096–2097

Question 3 Bottom force and liquid weight need not be equal An open vessel of height H widens upward. Its horizontal area at height z above the base is A(z) = A0(1 + z/H). It contains liquid of density ρ up to z = H. Use gauge pressure so the common atmospheric contribution is removed. liquid H A0 Widening vessel schematic; the specified area law defines its geometry. (a) Find the downward force exerted by the liquid on the horizontal base and the liquid weight. (b) Find the net vertical gauge force exerted by the sidewalls on the liquid. Explain how this resolves the apparent mismatch.
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Question 3 - Solution Bottom force and liquid weight need not be equal liquid H A0 (a) Derivation and calculation pB = ρgH, FB = pBA0 = ρgHA0 . V = ∫H 0 A0(1 + z/H) dz = 3 2A0H. W = ρgV = 3 2ρgA0H , FB/W = 2/3. (b) Result and interpretation For the liquid as the system, the base force is upward: FB + Fw,z −W = 0. Fw,z = W −FB = 1 2ρgA0H upward . The sloping walls support the remaining one-third of the weight through their normal forces. Physical check The force on the base is opposite to the base force on the liquid; keeping this action-reaction distinction resolves the sign.

Question 3

Bottom force and liquid weight need not be equal

An open vessel of height HH widens upward. Its horizontal area at height zz above the base is A(z)=A0(1+z/H)A(z)=A_0(1+z/H). It contains liquid of density ρ\rho up to z=Hz=H. Use gauge pressure so the common atmospheric contribution is removed.

Diagram shown in the original SVG worksheet.

  1. Find the downward force exerted by the liquid on the horizontal base and the liquid weight.

  2. Find the net vertical gauge force exerted by the sidewalls on the liquid. Explain how this resolves the apparent mismatch.

Question 3 - Solution

Bottom force and liquid weight need not be equal

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

pB=ρgH,FB=pBA0=ρgHA0.p_B=\rho gH,\qquad\boxed{F_B=p_BA_0=\rho gHA_0}.V=∫0HA0(1+z/H)dz=32A0H.V=\int_0^H A_0(1+z/H)\,dz=\tfrac32A_0H.W=ρgV=32ρgA0H,FB/W=2/3.\boxed{W=\rho gV=\tfrac32\rho gA_0H},\qquad F_B/W=2/3.

(b) Result and interpretation

For the liquid as the system, the base force is upward:FB+Fw,z−W=0.F_B+F_{w,z}-W=0.Fw,z=W−FB=12ρgA0Hupward.\boxed{F_{w,z}=W-F_B=\tfrac12\rho gA_0H\ \text{upward}}.The sloping walls support the remaining one-third of the weight through their normal forces.

Physical check

The force on the base is opposite to the base force on the liquid; keeping this action-reaction distinction resolves the sign.