The axially symmetric laminar flow of a viscous incompressible fluid through a long straight tube of a circular cross section under a constant axial pressure gradient is known as Poiseuille flow. The axial velocity w is a function of the radial variable r only and satisfies the boundary value problem 1 w" + G w(R) = 0, w(r) bounded for 0
The axially symmetric laminar flow of a viscous incompressible fluid through a long straight tube of a circular cross section under a constant axial pressure gradient is known as Poiseuille flow. The axial velocity w is a function of the radial variable r only and satisfies the boundary value problem 1 w" + G w(R) = 0, w(r) bounded for 0
Elements Of Electromagnetics
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ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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
Transcribed Image Text:The axially symmetric laminar flow of a viscous incompressible fluid through a long
straight tube of a circular cross section under a constant axial pressure gradient is known
as Poiseuille flow. The axial velocity w is a function of the radial variable r only and
satisfies the boundary value problem
1
w" +
G
w(R) = 0, w(r) bounded for 0 <r < R,
where R is the radius of the tube, G is the pressure gradient, and u is the coefficient of
viscosity of the fluid.
(a) Find the velocity profile w(r).
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