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MECHANICS of FLUIDS LABORATORY - Mechanical Engineering

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EXPERIMENT 10<br />

DRAG FORCE DETERMINATION<br />

An object placed in a uniform flow is acted<br />

upon by various forces. The resultant <strong>of</strong> these<br />

forces can be resolved into two force components,<br />

parallel and perpendicular to the main flow<br />

direction. The component acting parallel to the<br />

flow is known as the drag force. It is a function <strong>of</strong><br />

a skin friction effect and an adverse pressure<br />

gradient. The component perpendicular to the<br />

flow direction is the lift force and is caused by a<br />

pressure distribution which results in a lower<br />

pressure acting over the top surface <strong>of</strong> the object<br />

than at the bottom. If the object is symmetric<br />

with respect to the flow direction, then the lift<br />

force will be zero and only a drag force will exist.<br />

Measurement <strong>of</strong> the drag force acting on an object<br />

immersed in the uniform flow <strong>of</strong> a fluid is the<br />

subject <strong>of</strong> this experiment.<br />

Equipment<br />

Subsonic Wind Tunnel<br />

Objects<br />

A description <strong>of</strong> a subsonic wind tunnel is<br />

given in Experiment 9 and is shown schematically<br />

in Figure 9.3. The fan at the end <strong>of</strong> the tunnel<br />

draws in air at the inlet. An object is mounted on a<br />

stand that is pre calibrated to read lift and drag<br />

forces exerted by the fluid on the object. A<br />

schematic <strong>of</strong> the test section is shown in Figure<br />

10.1. The velocity <strong>of</strong> the flow at the test section is<br />

also pre calibrated. The air velocity past the<br />

object can be controlled by changing the angle <strong>of</strong><br />

the inlet vanes located within the fan housing.<br />

Thus air velocity, lift force and drag force are<br />

read directly from the tunnel instrumentation.<br />

There are a number <strong>of</strong> objects that are<br />

available for use in the wind tunnel. These<br />

include a disk, a smooth surfaced sphere, a rough<br />

surface sphere, a hemisphere facing upstream,<br />

and a hemisphere facing downstream. For<br />

whichever is assigned, measure drag on the object<br />

as a function <strong>of</strong> velocity.<br />

Data on drag vs velocity are usually graphed<br />

in dimensionless terms. The drag force D f is<br />

customarily expressed in terms <strong>of</strong> the drag<br />

coefficient C D (a ratio <strong>of</strong> drag force to kinetic<br />

energy):<br />

in which ρ is the fluid density, V is the free<br />

stream velocity, and A is the projected frontal<br />

area <strong>of</strong> the object. Traditionally, the drag<br />

coefficient is graphed as a function <strong>of</strong> the<br />

Reynolds number, which is defined as<br />

Re = VD<br />

ν<br />

where D is a characteristic length <strong>of</strong> the object<br />

and ν is the kinematic viscosity <strong>of</strong> the fluid. For<br />

each object assigned, graph drag coefficient vs<br />

Reynolds number and compare your results to<br />

those published in texts. Use log-log paper if<br />

appropriate.<br />

Questions<br />

1. How does the mounting piece affect the<br />

readings?<br />

2. How do you plan to correct for its effect, if<br />

necessary?<br />

uniform flow<br />

lift force<br />

measurement<br />

object<br />

mounting stand<br />

drag force<br />

measurement<br />

FIGURE 10.1. Schematic <strong>of</strong> an object mounted in<br />

the test section <strong>of</strong> the wind tunnel.<br />

D f<br />

C D<br />

=<br />

ρV 2 A/2<br />

27

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