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Fighter Combat - Tactics and Maneuvering

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408 APPENDIX<br />

turn performance (i.e., rate <strong>and</strong> radius) improves, but total aircraft drag also<br />

increases. Eventually a load factor is reached at which the entire thrust of<br />

the engines is needed just to offset this drag, leaving no excess power for a<br />

simultaneous climb or for acceleration. Equation 4 indicates that when<br />

thrust equals drag, Ps is zero. Figure A-14 shows how the zero-Ps line reacts<br />

by shrinking <strong>and</strong> deforming under increased G. This process is further<br />

illustrated by Figure A-17.<br />

This figure consists of H-M plots of the same supersonic jet fighter at<br />

load factors of 3 Gs <strong>and</strong> 5 Gs. The outer curve in each case is the 1-G Ps = 0<br />

line for reference. Within this 1-G envelope are specific-excess-power<br />

values (in ft/sec) for the two sample load factors. Note that the zero-Ps<br />

envelope shrinks considerably in the 3-G plot, <strong>and</strong> even farther under 5 Gs.<br />

Figure A-17. H-M Diagrams for 3 Gs <strong>and</strong> 5 Gs

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