Density and Pressure — Question 5

Section 14-2 · Physics pages 2080–2081

Question 5 A spatially varying pressure shifts the resultant A rectangular panel has width b and length L. A prescribed net normal pressure varies along the coordinate x as q(x) = q0(1 + x/L), 0 ≤x ≤L. It is uniform across the width. The same normal direction applies everywhere; the pressure profile is given, not derived from depth. x q q0 L 2q0 Linear prescribed net-pressure profile. (a) Find the resultant force and its point of application xR. (b) Evaluate for q0 = 2.0 kPa, b = 0.40 m, L = 0.60 m. Why does using the midpoint pressure find the force but not its moment?
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Question 5 - Solution A spatially varying pressure shifts the resultant x q q0 L 2q0 (a) Derivation and calculation dF = bq0(1 + x/L) dx. F = bq0 ∫L 0 (1 + x/L) dx = 3 2bq0L . FxR = bq0 ∫L 0 (x + x2/L) dx = 5 6bq0L2. xR = 5L/9 . (b) Result and interpretation F = 3 2(.40)(2000)(.60) = 720 N , xR = .33333 m . M0 = FxR = 240 N m, F(L/2) = 216 N m. Midpoint pressure equals the mean for a linear profile, but placing the resultant at the midpoint loses the correct moment. Physical check The resultant lies toward the higher-pressure end: 5L/9 > L/2.

Question 5

A spatially varying pressure shifts the resultant

A rectangular panel has width bb and length LL. A prescribed net normal pressure varies along the coordinate xx as q(x)=q0(1+x/L)q(x)=q_0(1+x/L), 0≤x≤L0\le x\le L. It is uniform across the width. The same normal direction applies everywhere; the pressure profile is given, not derived from depth.

Diagram shown in the original SVG worksheet.

  1. Find the resultant force and its point of application xRx_R.

  2. Evaluate for q0=2.0kPaq_0=2.0\,\mathrm{kPa}, b=0.40mb=0.40\,\mathrm{m}, L=0.60mL=0.60\,\mathrm{m}. Why does using the midpoint pressure find the force but not its moment?

Question 5 - Solution

A spatially varying pressure shifts the resultant

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

dF=bq0(1+x/L)dx.dF=bq_0(1+x/L)\,dx.F=bq0∫0L(1+x/L)dx=32bq0L.F=bq_0\int_0^L(1+x/L)\,dx=\boxed{\tfrac32bq_0L}.FxR=bq0∫0L(x+x2/L)dx=56bq0L2.Fx_R=bq_0\int_0^L(x+x^2/L)\,dx=\tfrac56bq_0L^2.xR=5L/9.\boxed{x_R=5L/9}.

(b) Result and interpretation

F=32(.40)(2000)(.60)=720N,xR=.33333m.\boxed{F=\tfrac32(.40)(2000)(.60)=720\,\mathrm N},\quad\boxed{x_R=.33333\,\mathrm m}.M0=FxR=240Nm,F(L/2)=216Nm.M_0=Fx_R=240\,\mathrm{N\,m},\quad F(L/2)=216\,\mathrm{N\,m}.Midpoint pressure equals the mean for a linear profile, but placing the resultant at the midpoint loses the correct moment.

Physical check

The resultant lies toward the higher-pressure end: 5L/9>L/25L/9>L/2.