Viscosity
Example 1 (continued)
The figure below shows an
enlarged view of the gap, b, with the
linear velocity distribution. The velocity distribution
is V(y) = Vo (1 – y/b) where b is the gap width and Vo is the constant velocity of the shaft. For a Newtonian fluid, τ =
μ dV/dy. Thus τ =
μ ( - Vo /b )
Note: The shear stress in the
fluid is constant across gap. Recall μ
= ν ρ
where ν is the kinematic viscosity and
ρ is the fluid density specific gravity for lubricant = 0.91,
ρ for water is 1000 kg/m3
The shear force, FS , is just the shear stress time the area it
acts on which is ((2π)(D/2)L). FS =
μ ( - Vo /b )
(2π)(D/2)L where L is
the length of the shaft
Now for equilibrium, →
Σ F = 0
μ ( - Vo /b )
(2π)(D/2)L + P
= 0 P =
μ ( Vo /b ) π D L ,
From the data: μ
= 8.0 x 10-4 (m2/sec)
(1000 kg/m3)(0.91), Vo
= 3 m/sec, b = 0.3 mm = 0.0003 m,
D = 25 mm = 0.025 m, L = 0.5 m P = 286
N (result) |
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