The Equation of Continuity — Question 4

Section 14-8 · Physics pages 2198–2199

Question 4 A centerline speed is not an area-average speed A steady axial flow in a circular pipe of radius R has the prescribed profile v(r) = vmax(1 −r2/R2). Density is uniform. This profile may describe a viscous flow; continuity does not require an inviscid model. r v vmax R Prescribed parabolic speed profile from the axis to the wall. (a) Integrate over circular rings to find Q and the mean speed. (b) What fraction of the volume flow passes through the inner half-radius disk? Compare it with that disk's area fraction.
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Question 4 - Solution A centerline speed is not an area-average speed r v vmax R (a) Derivation and calculation dA = 2πr dr, Q = 2πvmax ∫R 0 ( r −r3 R2 ) dr. Q = 1 2πR2vmax , ¯v = Q/(πR2) = vmax/2 . Using centerline speed as mean speed doubles the flow estimate. (b) Result and interpretation Q(a) = 2πvmax ∫a 0 ( r −r3 R2 ) dr = πvmax ( a2 −a4 2R2 ) . Q(R/2) Q(R) = 2 (1 4 −1 32 ) = 7 16 = 43.75% . A(R/2)/A(R) = 1/4 = 25%. The central region carries disproportionate flow because it moves faster. Physical check The flux integral works for the prescribed viscous profile; incompressible continuity does not require inviscid flow.

Question 4

A centerline speed is not an area-average speed

A steady axial flow in a circular pipe of radius RR has the prescribed profile v(r)=vmax(1−r2/R2)v(r)=v_{\max}(1-r^2/R^2). Density is uniform. This profile may describe a viscous flow; continuity does not require an inviscid model.

Diagram shown in the original SVG worksheet.

  1. Integrate over circular rings to find QQ and the mean speed.

  2. What fraction of the volume flow passes through the inner half-radius disk? Compare it with that disk's area fraction.

Question 4 - Solution

A centerline speed is not an area-average speed

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

dA=2πrdr,Q=2πvmax∫0R(r−r3R2)dr.dA=2\pi r\,dr,\quad Q=2\pi v_{\max}\int_0^R\left(r-\frac{r^3}{R^2}\right)dr.Q=12πR2vmax,v‾=Q/(πR2)=vmax/2.\boxed{Q=\frac12\pi R^2v_{\max}},\qquad\boxed{\bar v=Q/(\pi R^2)=v_{\max}/2}.Using centerline speed as mean speed doubles the flow estimate.

(b) Result and interpretation

Q(a)=2πvmax∫0a(r−r3R2)dr=πvmax(a2−a42R2).Q(a)=2\pi v_{\max}\int_0^a\left(r-\frac{r^3}{R^2}\right)dr=\pi v_{\max}\left(a^2-\frac{a^4}{2R^2}\right).Q(R/2)Q(R)=2(14−132)=716=43.75%.\boxed{\frac{Q(R/2)}{Q(R)}=2\left(\frac14-\frac1{32}\right)=\frac7{16}=43.75\%}.A(R/2)/A(R)=1/4=25%.A(R/2)/A(R)=1/4=25\%.The central region carries disproportionate flow because it moves faster.

Physical check

The flux integral works for the prescribed viscous profile; incompressible continuity does not require inviscid flow.