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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 />

Area build-up graphs were also generated for the wave drag analyses <strong>of</strong> the 3<br />

RLV configurations. These configurations were not run <strong>in</strong> WAVDRAG, so no<br />

comparison was made with the APAS results. The APAS build-ups can be found <strong>in</strong><br />

Appendix B <strong>of</strong> this report.<br />

5.2 Wave <strong>Drag</strong> Comparisons<br />

The second and more conclusive comparison between APAS and WAVDRAG is<br />

that <strong>of</strong> the actual wave drag coefficients <strong>of</strong> each trial configuration generated by the two<br />

programs. Figure 45 shows the wave drag calculated by the wave subprogram <strong>of</strong> APAS<br />

and the results <strong>of</strong> the WAVDRAG analysis <strong>of</strong> the trial 1 configuration. Unlike APAS,<br />

WAVDRAG will generate results at Mach 1, but no lower.<br />

Trial 1<br />

C dw<br />

0.45<br />

0.4<br />

0.35<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

APAS Wavedrag<br />

WAVDRAG<br />

1 1.1 1.2 1.3 1.4 1.5 1.6<br />

Mach #<br />

Figure 45. Trial 1 Wave <strong>Drag</strong> Comparison<br />

WAVDRAG predicts a wave drag coefficient forty percent lower than APAS at<br />

Mach 1.01 due to the difference <strong>in</strong> the ways the programs calculate wave drag, one as<br />

zero-lift wave drag and the other as wave drag that <strong>in</strong>cludes that due to lift. The plots<br />

Jeff Miller 36

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