11. (Poiseuille flow) A viscous fluid flows steadily between two large para lel plates so that its velocity is parallel to the x-axis. (See Fig. 9.) The x component of velocity of the fluid at any point (x, y) is a function of only. It can be shown that this component u(x) satisfies the differentia equation d² u dy2 8 = 0 < y < L, where is the viscosity and -g is a constant, negative pressure gradi- ent. Find u(y), subject to the "no-slip" boundary conditions, u(0) = 0, u(L) = 0. μ 1

Elements Of Electromagnetics
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Figure 9 Poiseuille flow.
11. (Poiseuille flow) A viscous fluid flows steadily between two large paral-
lel plates so that its velocity is parallel to the x-axis. (See Fig. 9.) The x-
component of velocity of the fluid at any point (x, y) is a function of y
only. It can be shown that this component u(x) satisfies the differential
equation
d² u
dy²
X
8
μ
=
0 < y < L,
where is the viscosity and -g is a constant, negative pressure gradi-
ent. Find u(y), subject to the "no-slip" boundary conditions, u(0) = 0,
u(L) = 0.
Transcribed Image Text:Figure 9 Poiseuille flow. 11. (Poiseuille flow) A viscous fluid flows steadily between two large paral- lel plates so that its velocity is parallel to the x-axis. (See Fig. 9.) The x- component of velocity of the fluid at any point (x, y) is a function of y only. It can be shown that this component u(x) satisfies the differential equation d² u dy² X 8 μ = 0 < y < L, where is the viscosity and -g is a constant, negative pressure gradi- ent. Find u(y), subject to the "no-slip" boundary conditions, u(0) = 0, u(L) = 0.
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