Recall that the transverse velocity for Poiseuille flow is Др -p² + C1 4µL In r + c2 , u(r) = 0

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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Recall that the transverse velocity for Poiseuille flow is
Др
p² + cj In r + c2,
4µL
и(г) —
0 <r < R,
where Ap/L is the (constant) pressure gradient, µ is the dynamic viscosity, and L is the length of the tube. Since the solution can't blow
up at r = 0, c = 0, and c2 is determined by the no-slip condition u(R) = 0. Integrating the resulting solution over the cross-section of
the tube gives the flux
AR* Ap
Qo
8µ L
1
Now imagine that the tube has a central catheter so that -R <r < R. Use the solution for u above and apply no-slip conditions at
3
1
R and r = R to compute the flux Q for the catheterized tube.
3
r =
Qo
Transcribed Image Text:Recall that the transverse velocity for Poiseuille flow is Др p² + cj In r + c2, 4µL и(г) — 0 <r < R, where Ap/L is the (constant) pressure gradient, µ is the dynamic viscosity, and L is the length of the tube. Since the solution can't blow up at r = 0, c = 0, and c2 is determined by the no-slip condition u(R) = 0. Integrating the resulting solution over the cross-section of the tube gives the flux AR* Ap Qo 8µ L 1 Now imagine that the tube has a central catheter so that -R <r < R. Use the solution for u above and apply no-slip conditions at 3 1 R and r = R to compute the flux Q for the catheterized tube. 3 r = Qo
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