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MECHANICS of FLUIDS LABORATORY - Mechanical Engineering

MECHANICS of FLUIDS LABORATORY - Mechanical Engineering

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Experiment II<br />

For a number <strong>of</strong> wings, lift and drag data<br />

vary only slightly with Reynolds number and<br />

therefore if lift and drag coefficients are graphed<br />

as a function <strong>of</strong> Reynolds number, the results are<br />

not that meaningful. A more significant<br />

representation <strong>of</strong> the results is given in what is<br />

known as a polar diagram for the wing. A polar<br />

diagram is a graph on a linear grid <strong>of</strong> lift<br />

coefficient (vertical axis) as a function <strong>of</strong> drag<br />

coefficient. Each data point on the graph<br />

corresponds to a different angle <strong>of</strong> attack, all<br />

measured at one velocity (Reynolds number).<br />

Referring to Figure 11.2 (which is the<br />

experimental setup here), the angle <strong>of</strong> attack α is<br />

measured from a line parallel to the chord c to a<br />

line that is parallel to the free stream velocity.<br />

If so instructed, obtain lift force, drag force and<br />

angle <strong>of</strong> attack data using a pre selected velocity.<br />

Allow the angle <strong>of</strong> attack to vary from a negative<br />

angle to the stall point and beyond. Obtain data<br />

at no less than 9 angles <strong>of</strong> attack. Use the data to<br />

produce a polar diagram.<br />

Analysis<br />

Lift and drag data are usually expressed in<br />

dimensionless terms using lift coefficient and drag<br />

coefficient. The lift coefficient is defined as<br />

L f<br />

C L<br />

=<br />

ρV 2 A/2<br />

where L f is the lift force, ρ is the fluid density, V<br />

is the free stream velocity far upstream <strong>of</strong> the<br />

wing, and A is the area <strong>of</strong> the wing when seen<br />

from a top view perpendicular to the chord<br />

length c. The drag coefficient is defined as<br />

D f<br />

C D<br />

=<br />

ρV 2 A/2<br />

in which D f<br />

is the drag force.<br />

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