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7.9 Some Typical Model Studies 365<br />

E XAMPLE 7.7<br />

Model Design Conditions and Predicted Prototype Performance<br />

GIVEN The drag on the airplane shown in Fig. E7.7 cruising<br />

at 240 mph in standard air is to be determined from tests on a 1:10<br />

scale model placed in a pressurized wind tunnel. To minimize<br />

compressibility effects, the air speed in the wind tunnel is also to<br />

be 240 mph.<br />

FIND Determine<br />

(a) the required air pressure in the tunnel (assuming the same<br />

air temperature for model and prototype) and<br />

SOLUTION<br />

(a) From Eq. 7.19 it follows that drag can be predicted from a<br />

geometrically similar model if the Reynolds numbers in model<br />

and prototype are the same. Thus,<br />

For this example, V and / m/ 1 m V<br />

10 so that<br />

and therefore<br />

r m V m / m<br />

m m<br />

r m<br />

r m m<br />

m<br />

rV/<br />

m<br />

V /<br />

V m<br />

This result shows that the same <strong>fluid</strong> with r m r and m m m<br />

cannot be used if Reynolds number similarity is to be maintained.<br />

One possibility is to pressurize the wind tunnel to increase the<br />

density of the air. We assume that an increase in pressure does not<br />

significantly change the viscosity so that the required increase in<br />

density is given by the relationship<br />

r m<br />

r 10<br />

For an ideal gas, p rRT so that<br />

p m<br />

p r m<br />

r<br />

/ m<br />

m m<br />

m 1121102<br />

r m<br />

r 10 m m<br />

m<br />

(b) the drag on the prototype corresponding to a measured force<br />

of 1 lb on the model.<br />

V = 240 mph<br />

F I G U R E E7.7<br />

for constant temperature 1T T m 2. Therefore, the wind tunnel<br />

would need to be pressurized so that<br />

Since the prototype operates at standard atmospheric pressure,<br />

the required pressure in the wind tunnel is 10 atmospheres or<br />

(Ans)<br />

COMMENT Thus, we see that a high pressure would be required<br />

and this could not be achieved easily or inexpensively. However,<br />

under these conditions, Reynolds similarity would be attained.<br />

(b) The drag could be obtained from Eq. 7.19 so that<br />

or<br />

p m 10 114.7 psia2<br />

147 psia<br />

d<br />

1<br />

2 rV 2 / d m<br />

2 1<br />

2 r mVm/ 2 2 m<br />

d r a V 2<br />

b a / 2<br />

b d<br />

r m V m / m<br />

m<br />

a 1<br />

10 b 1122 1102 2 d m<br />

10d m<br />

p m<br />

p 10<br />

Thus, for a drag of 1 lb on the model the corresponding drag on<br />

the prototype is<br />

d 10 lb<br />

(Ans)<br />

V7.16 Wind tunnel<br />

train model<br />

Fortunately, in many situations the flow characteristics are not strongly influenced by the<br />

Reynolds number over the operating range of interest. In these cases we can avoid the rather stringent<br />

similarity requirement of matching Reynolds numbers. To illustrate this point, consider the<br />

variation in the drag coefficient with the Reynolds number for a smooth sphere of diameter d placed<br />

in a uniform stream with approach velocity, V. Some typical data are shown in Fig. 7.7. We observe<br />

that for Reynolds numbers between approximately 10 3 and 2 10 5 the drag coefficient is<br />

relatively constant and does not strongly depend on the specific value of the Reynolds number.<br />

Thus, exact Reynolds number similarity is not required in this range. For other geometric shapes<br />

we would typically find that for high Reynolds numbers, inertial forces are dominant 1rather than<br />

viscous forces2, and the drag is essentially independent of the Reynolds number.

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