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464 Chapter 9 ■ Flow over Immersed Bodies<br />

y<br />

pdA<br />

θ<br />

τ w dA<br />

U<br />

dA<br />

θ<br />

x<br />

F I G U R E 9.4 Pressure and shear<br />

forces on a small element of the surface of a<br />

body.<br />

integrated or resultant effects of these distributions are needed. The resultant force in the direction<br />

of the upstream velocity is termed the drag, d, and the resultant force normal to the upstream velocity<br />

is termed the lift, l, as is indicated in Fig. 9.3c. For some three-dimensional bodies there<br />

may also be a side force that is perpendicular to the plane containing d and l.<br />

The resultant of the shear stress and pressure distributions can be obtained by integrating the<br />

effect of these two quantities on the body surface as is indicated in Fig. 9.4. The x and y components<br />

of the <strong>fluid</strong> force on the small area element dA are<br />

and<br />

dF x 1 p dA2 cos u 1t w dA2 sin u<br />

dF y 1 p dA2 sin u 1t w dA2 cos u<br />

Thus, the net x and y components of the force on the object are<br />

d dF x p cos u dA t w sin u dA<br />

(9.1)<br />

and<br />

l dF y p sin u dA t w cos u dA<br />

(9.2)<br />

Lift and drag on a<br />

section of a body<br />

depend on the orientation<br />

of the surface.<br />

Of course, to carry out the integrations and determine the lift and drag, we must know the body<br />

shape 1i.e., u as a function of location along the body2 and the distribution of t w and p along the<br />

surface. These distributions are often extremely difficult to obtain, either experimentally or theoretically.<br />

The pressure distribution can be obtained experimentally by use of a series of static pressure<br />

taps along the body surface. On the other hand, it is usually quite difficult to measure the wall<br />

shear stress distribution.<br />

F l u i d s i n t h e N e w s<br />

Pressure-sensitive paint For many years, the conventional<br />

method for measuring surface pressure has been to use static<br />

pressure taps consisting of small holes on the surface connected<br />

by hoses from the holes to a pressure measuring device. Pressuresensitive<br />

paint (PSP) is now gaining acceptance as an alternative<br />

to the static surface pressure ports. The PSP material is typically<br />

a luminescent compound that is sensitive to the pressure on it and<br />

can be excited by an appropriate light which is captured by special<br />

video imaging equipment. Thus, it provides a quantitative<br />

measure of the surface pressure. One of the biggest advantages of<br />

PSP is that it is a global measurement technique, measuring pressure<br />

over the entire surface, as opposed to discrete points. PSP<br />

also has the advantage of being nonintrusive to the flow field. Although<br />

static pressure port holes are small, they do alter the surface<br />

and can slightly alter the flow, thus affecting downstream<br />

ports. In addition, the use of PSP eliminates the need for a large<br />

number of pressure taps and connecting tubes. This allows pressure<br />

measurements to be made in less time and at a lower cost.<br />

It is seen that both the shear stress and pressure force contribute to the lift and drag, since<br />

for an arbitrary body u is neither zero nor 90° along the entire body. The exception is a flat plate<br />

aligned either parallel to the upstream flow 1u 90°2 or normal to the upstream flow 1u 02 as<br />

is discussed in Example 9.1.

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