The Equation of Continuity — Question 5

Section 14-8 · Physics pages 2200–2201

Question 5 Radial flow spreads over a growing circumference An incompressible liquid flows steadily outward between two parallel horizontal disks separated by uniform gap b = 2.0 mm. Beyond the central inlet the flow is axisymmetric. The volume rate is Q = 6.0 × 10−5 m3/s. Use the gap-averaged radial speed. Top view of outward radial flow; the disk gap is perpendicular to the page. (a) Find the mean radial speed at r = 0.020 m and r = 0.060 m. (b) If the gap instead varies as b(r) = b0r0/r, what is the radial dependence of the mean speed? Explain why the singular limit near r = 0 is excluded.
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Question 5 - Solution Radial flow spreads over a growing circumference (a) Derivation and calculation The radial flux crosses a cylindrical surface: Ar = 2πrb, Q = Ar¯vr ⇒¯vr = Q 2πrb . ¯vr(.0200) = 6.0 × 10−5 2π(.0200)(.00200) = .238732 m/s . ¯vr(.0600) = .0795775 m/s . (b) Result and interpretation If b(r) = b0r0/r, Ar = 2πr(b0r0/r) = 2πb0r0, ¯vr = Q 2πb0r0 = constant . The finite inlet region cannot be modeled by extending radial-only motion to the axis. Fixed gap would imply ¯vr →∞; the alternate gap law itself diverges there. Physical check Tripling radius at fixed gap triples flow area and divides mean speed by three.

Question 5

Radial flow spreads over a growing circumference

An incompressible liquid flows steadily outward between two parallel horizontal disks separated by uniform gap b=2.0mmb=2.0\,\mathrm{mm}. Beyond the central inlet the flow is axisymmetric. The volume rate is Q=6.0×10−5m3/sQ=6.0\times10^{-5}\,\mathrm{m^3/s}. Use the gap-averaged radial speed.

Diagram shown in the original SVG worksheet.

  1. Find the mean radial speed at r=0.020mr=0.020\,\mathrm{m} and r=0.060mr=0.060\,\mathrm{m}.

  2. If the gap instead varies as b(r)=b0r0/rb(r)=b_0r_0/r, what is the radial dependence of the mean speed? Explain why the singular limit near r=0r=0 is excluded.

Question 5 - Solution

Radial flow spreads over a growing circumference

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The radial flux crosses a cylindrical surface:Ar=2πrb,Q=Arv‾r⇒v‾r=Q2πrb.A_r=2\pi rb,\quad Q=A_r\bar v_r\Rightarrow\boxed{\bar v_r=\frac Q{2\pi rb}}.v‾r(.0200)=6.0×10−52π(.0200)(.00200)=.238732m/s.\boxed{\bar v_r(.0200)=\frac{6.0\times10^{-5}}{2\pi(.0200)(.00200)}=.238732\,\mathrm{m/s}}.v‾r(.0600)=.0795775m/s.\boxed{\bar v_r(.0600)=.0795775\,\mathrm{m/s}}.

(b) Result and interpretation

If b(r)=b0r0/rb(r)=b_0r_0/r,Ar=2πr(b0r0/r)=2πb0r0,v‾r=Q2πb0r0=constant.A_r=2\pi r(b_0r_0/r)=2\pi b_0r_0,\quad\boxed{\bar v_r=\frac Q{2\pi b_0r_0}=\text{constant}}.The finite inlet region cannot be modeled by extending radial-only motion to the axis. Fixed gap would imply v‾r→∞\bar v_r\to\infty; the alternate gap law itself diverges there.

Physical check

Tripling radius at fixed gap triples flow area and divides mean speed by three.