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Investigation of Transonic Drag Computations in Aerodynamic ...

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<strong>Investigation</strong> <strong>of</strong> <strong>Transonic</strong> <strong>Drag</strong> <strong>Computations</strong> <strong>in</strong> APAS<br />

important factor <strong>in</strong> the conceptual design <strong>of</strong> an RLV, thus the ability to accurately<br />

calculate and understand transonic drag effects becomes important.<br />

2.0 <strong>Transonic</strong> <strong>Drag</strong> and Wave <strong>Drag</strong> Theory<br />

The drag rise that occurs as a vehicle nears the speed <strong>of</strong> sound is caused by the<br />

development and presence <strong>of</strong> shock waves that result <strong>in</strong> wave drag. Figure 1 shows the<br />

development <strong>of</strong> local shock waves which lead to a Mach wave as the sound barrier is<br />

broken. Local shock waves beg<strong>in</strong> to develop on certa<strong>in</strong> parts <strong>of</strong> an aircraft as the<br />

freestream Mach number approaches 0.85-0.9.<br />

Mach Wave<br />

U <strong>in</strong>f<br />

M ~ .7 M ~ 1.1<br />

Figure 1. Shock Wave Development<br />

These shock waves and the result<strong>in</strong>g shock <strong>in</strong>duced boundary layer are the biggest<br />

contributors to transonic drag. The drag cont<strong>in</strong>ues to <strong>in</strong>crease <strong>in</strong> magnitude until the flow<br />

is fully supersonic, at which po<strong>in</strong>t it beg<strong>in</strong>s to taper <strong>of</strong>f. This behavior can be seen <strong>in</strong><br />

Figure 2, which shows a typical transonic drag rise.<br />

Jeff Miller 2

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