Density and Pressure — Question 3

Section 14-2 · Physics pages 2076–2077

Question 3 A local density is not generally a whole-column density A vertical sample of height H has constant horizontal area A and density ρ(z) = ρ0(1 + z/H), where z runs upward from its base. This profile is prescribed at the instant of measurement; no claim of stable equilibrium is made. z 0 H Prescribed density increases with height; this is not an equilibrium assumption. (a) Find the total mass and mean density. Is the density at midheight equal to the mean? (b) Find the height of its center of mass and explain its displacement from midheight.
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Question 3 - Solution A local density is not generally a whole-column density z 0 H (a) Derivation and calculation dm = Aρ(z) dz, M = ρ0A ∫H 0 (1 + z/H) dz = 3 2ρ0AH . ¯ρ = M/(AH) = 3 2ρ0 = ρ(H/2) . The equality with the midpoint value follows specifically from the linear profile and constant area. (b) Result and interpretation Mzcm = ρ0A ∫H 0 (z + z2/H) dz = 5 6ρ0AH2. zcm = (5/6)ρ0AH2 (3/2)ρ0AH = 5H 9 . zcm −H/2 = H/18 > 0. Physical check The heavier upper slices shift the center upward; the prescribed profile is not asserted to be stable.

Question 3

A local density is not generally a whole-column density

A vertical sample of height HH has constant horizontal area AA and density ρ(z)=ρ0(1+z/H)\rho(z)=\rho_0(1+z/H), where zz runs upward from its base. This profile is prescribed at the instant of measurement; no claim of stable equilibrium is made.

Diagram shown in the original SVG worksheet.

  1. Find the total mass and mean density. Is the density at midheight equal to the mean?

  2. Find the height of its center of mass and explain its displacement from midheight.

Question 3 - Solution

A local density is not generally a whole-column density

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

dm=Aρ(z)dz,M=ρ0A∫0H(1+z/H)dz=32ρ0AH.dm=A\rho(z)\,dz,\quad M=\rho_0A\int_0^H(1+z/H)\,dz=\boxed{\tfrac32\rho_0AH}.ρ‾=M/(AH)=32ρ0=ρ(H/2).\boxed{\bar\rho=M/(AH)=\tfrac32\rho_0=\rho(H/2)}.The equality with the midpoint value follows specifically from the linear profile and constant area.

(b) Result and interpretation

Mzcm=ρ0A∫0H(z+z2/H)dz=56ρ0AH2.Mz_{\mathrm{cm}}=\rho_0A\int_0^H(z+z^2/H)\,dz=\frac56\rho_0AH^2.zcm=(5/6)ρ0AH2(3/2)ρ0AH=5H9.\boxed{z_{\mathrm{cm}}=\frac{(5/6)\rho_0AH^2}{(3/2)\rho_0AH}=\frac{5H}{9}}.zcm−H/2=H/18>0.z_{\mathrm{cm}}-H/2=H/18>0.

Physical check

The heavier upper slices shift the center upward; the prescribed profile is not asserted to be stable.