Fluids at Rest — Question 2

Section 14-3 · Physics pages 2094–2095

Question 2 A density gradient changes the meaning of a depth estimate Depth h is measured downward from the surface of a stratified liquid. Its density is ρ(h) = ρ0(1 + h/H) for 0 ≤h ≤H. Surface pressure is p0 and gravity is constant. h p −p0 The hydrostatic pressure slope increases with depth because the prescribed density increases. (a) Derive p(h) by balancing a thin horizontal slice. Evaluate the bottom excess pressure. (b) At what depth is the pressure excess half its bottom value? Compare with H/2.
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Question 2 - Solution A density gradient changes the meaning of a depth estimate h p −p0 (a) Derivation and calculation For a thin slice of area A, p(h)A + ρ(h)gA dh −p(h + dh)A = 0. dp dh = ρ0g(1 + h/H). p(h) = p0 + ρ0g ( h + h2 2H ) , p(H) −p0 = 3 2ρ0gH . (b) Result and interpretation Let u = h/H. Half the bottom pressure excess requires u + 1 2u2 = 3 4 ⇒u2 + 2u −3 2 = 0. h/H = −1 + √ 5/2 = .581139 . The negative root is outside the fluid. More than half the depth is required because the upper liquid contributes less pressure rise per unit depth. Physical check At h = H/2, the pressure fraction is (.5 + .125)/1.5 = 5/12 < 1/2.

Question 2

A density gradient changes the meaning of a depth estimate

Depth hh is measured downward from the surface of a stratified liquid. Its density is ρ(h)=ρ0(1+h/H)\rho(h)=\rho_0(1+h/H) for 0≤h≤H0\le h\le H. Surface pressure is p0p_0 and gravity is constant.

Diagram shown in the original SVG worksheet.

  1. Derive p(h)p(h) by balancing a thin horizontal slice. Evaluate the bottom excess pressure.

  2. At what depth is the pressure excess half its bottom value? Compare with H/2H/2.

Question 2 - Solution

A density gradient changes the meaning of a depth estimate

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For a thin slice of area AA,p(h)A+ρ(h)gAdh−p(h+dh)A=0.p(h)A+\rho(h)gA\,dh-p(h+dh)A=0.dpdh=ρ0g(1+h/H).\frac{dp}{dh}=\rho_0g(1+h/H).p(h)=p0+ρ0g(h+h22H),p(H)−p0=32ρ0gH.\boxed{p(h)=p_0+\rho_0g\left(h+\frac{h^2}{2H}\right)},\quad\boxed{p(H)-p_0=\tfrac32\rho_0gH}.

(b) Result and interpretation

Let u=h/Hu=h/H. Half the bottom pressure excess requiresu+12u2=34⇒u2+2u−32=0.u+\tfrac12u^2=\tfrac34\Rightarrow u^2+2u-\tfrac32=0.h/H=−1+5/2=.581139.\boxed{h/H=-1+\sqrt{5/2}=.581139}.The negative root is outside the fluid. More than half the depth is required because the upper liquid contributes less pressure rise per unit depth.

Physical check

At h=H/2h=H/2, the pressure fraction is (.5+.125)/1.5=5/12<1/2(.5+.125)/1.5=5/12<1/2.