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Fighter Combat - Tactics and Maneuvering

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ONE-VERSUS-ONE MANEUVERING, DISSIMILAR AIRCRAFT 151<br />

supersonic fighter engages a bogey that is limited to subsonic speeds. Just<br />

how much excess speed is required can be estimated using an altitude-<br />

Mach (H-M) diagram or Equation 3 in the Appendix before the engagement.<br />

Assuming an engagement altitude, the bogey's maximum attainable<br />

energy level can be located on the chart. Adding the desired energy<br />

(altitude) advantage to the bogey's energy level determines the approximate<br />

energy level required of the high-T/W fighter. The speed at which<br />

this desired energy level intersects the engagement altitude represents the<br />

necessary airspeed of the energy fighter.<br />

The speed advantage necessary to provide a given zoom-altitude advantage<br />

is highly dependent on the bogey's airspeed. For example, a 2,000-ft<br />

zoom advantage over a bogey traveling at 100 knots true airspeed (KTAS)<br />

would require the energy fighter to have about 130 knots of excess airspeed<br />

(230 KTAS total). But with the bogey at 500 KTAS, the energy fighter<br />

would need about 540 KTAS (only a 40-knot advantage). Although faster<br />

bogeys require less speed advantage for the energy fighter to attain a given<br />

zoom-altitude margin, this phenomenon is offset to a large degree because<br />

faster fighters generally need more altitude margin. The figures given here<br />

are only gross estimates, since they do not consider possible energy<br />

changes during the zoom maneuver.<br />

Assuming this energy advantage can be attained at the first pass, the<br />

pilot of the high-T/W fighter may choose to zoom immediately, as shown<br />

in Figure 4-5. The major difference between this scenario <strong>and</strong> that of Figure<br />

4-4 comes from the great energy advantage of the high-T/W fighter in this<br />

case, which enables the energy fighter to remain well above its opponent,<br />

<strong>and</strong> facilitates its maneuvering in the vertical plane.<br />

In this scenario the energy fighter has a substantial speed advantage<br />

approaching the pass (time "1") as well as slightly greater altitude.<br />

Together this speed <strong>and</strong> altitude advantage form the high-T/W fighter's<br />

desired energy margin. The purpose of the height advantage in this case is<br />

not only to provide extra energy margin, but also to induce the bogey pilot<br />

into a sharply nose-high maneuver. Allowing some vertical separation<br />

(i.e., passing almost directly over the bogey) gives the bogey room for a lead<br />

turn, but the pilot must turn almost purely in the vertical to take advantage<br />

of it. Too much separation here may provide the low-wing-loaded<br />

opponent a reasonable snapshot at the pass, while too little vertical advantage<br />

offers him little incentive to zoom. An altitude advantage at the pass<br />

equal to about one-quarter of the bogey's best turn radius is usually a good<br />

compromise.<br />

In Figure 4-5 the angles fighter begins a near-vertical lead turn at time<br />

"1," while the energy fighter continues straight ahead for a few seconds.<br />

Here the pilot of the energy fighter must assess whether the bogey pilot has<br />

timed his pull-up properly to gain lead for a gun snapshot at the pass. If so, a<br />

quick out-of-plane (level) jink is in order to spoil the shot before he starts a<br />

pull-up of his own. This slight delay in the energy fighter's zoom also helps<br />

the pilot keep sight of the bogey underneath. The energy fighter should<br />

begin its pull-up, at sustained-G levels, as the bogey begins to approach<br />

effective guns range. Turning up <strong>and</strong> away from the bogey at this point

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