Oil of viscosity μ and density ρ drains steadily down the side of a tall, wide vertical plate, as shown in Fig, C1.4 In the region shown, fully developed conditions exist', that is, the velocity profile shape and the film thickness δ are independent of distance z along the plate. The vertical velocity w becomes a function only of x, and the shear resistance from the atmosphere is negligible. (a) Sketch the approximate shape of the velocity profile w(x), considering the boundary conditions at the wall and at the film surface. (b) Suppose film thickness δ , and the slope of the velocity profile at the wall, (dw/dx) w a l l , are measured by a laser Doppler anemometer (to be discussed in Chap. 6). Find an expression for the viscosity of the oil as a function of ρ , δ (dw/dx) w a l l , and the gravitational acceleration g. Note that, for the coordinate system given, both w and (dw/dx) w a l l are negative.
Oil of viscosity μ and density ρ drains steadily down the side of a tall, wide vertical plate, as shown in Fig, C1.4 In the region shown, fully developed conditions exist', that is, the velocity profile shape and the film thickness δ are independent of distance z along the plate. The vertical velocity w becomes a function only of x, and the shear resistance from the atmosphere is negligible. (a) Sketch the approximate shape of the velocity profile w(x), considering the boundary conditions at the wall and at the film surface. (b) Suppose film thickness δ , and the slope of the velocity profile at the wall, (dw/dx) w a l l , are measured by a laser Doppler anemometer (to be discussed in Chap. 6). Find an expression for the viscosity of the oil as a function of ρ , δ (dw/dx) w a l l , and the gravitational acceleration g. Note that, for the coordinate system given, both w and (dw/dx) w a l l are negative.
Oil of viscosity
μ
and density
ρ
drains steadily down the side of a tall, wide vertical plate, as shown in Fig, C1.4 In the region shown, fully developed conditions exist', that is, the velocity profile shape and the film thickness
δ
are independent of distance z along the plate. The vertical velocity w becomes a function only of x, and the shear resistance from the atmosphere is negligible.
(a) Sketch the approximate shape of the velocity profile w(x), considering the boundary conditions at the wall and at the film surface.
(b) Suppose film thickness
δ
, and the slope of the velocity profile at the wall, (dw/dx)wall, are measured by a laser Doppler anemometer (to be discussed in Chap. 6). Find an expression for the viscosity of the oil as a function of
ρ
,
δ
(dw/dx)wall, and the gravitational acceleration g. Note that, for the coordinate system given, both w and (dw/dx)wallare negative.
Find the equivalent mass of the rocker arm assembly with respect to the x coordinate.
k₁
mi
m2
k₁
2. Figure below shows a U-tube manometer open at both ends and containing a column of liquid
mercury of length l and specific weight y. Considering a small displacement x of the manometer
meniscus from its equilibrium position (or datum), determine the equivalent spring constant associated
with the restoring force.
Datum
Area, A
1. The consequences of a head-on collision of two automobiles can be studied by considering the
impact of the automobile on a barrier, as shown in figure below. Construct a mathematical model (i.e.,
draw the diagram) by considering the masses of the automobile body, engine, transmission, and
suspension and the elasticity of the bumpers, radiator, sheet metal body, driveline, and engine
mounts.
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