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guidance, flight mechanics and trajectory optimization

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Manipulation of the equations involving d' results in<br />

From this equation, it is seen that the condition<br />

K2 + K -1 =. 0<br />

must be met if $ is to remain finite as p approaches zero.<br />

2.4 OPTIMIZATION OF THE RENDEZVOUS MANEUVER<br />

The cost of transporting fuel to space is so great that it is essential<br />

in the design of the maneuvers to determine those which require the least<br />

fuel <strong>and</strong> to choose the <strong>guidance</strong> mechanizations which approximate the optimum.<br />

Eventhough the considerations of this monograph deal with small orbital<br />

changes, the problem can be studied from the point of view of orbital<br />

transfers. Thus, it is known from the work of several authors (Reference 3.1<br />

through 3.5) that impulsive transfer of either one or two impulses will be the<br />

optimal transfer (minimum A V requirement) between orbits such as are<br />

involved here. Further, a phasing technique similar to that discussed by<br />

Strahly (3.6) which involves splitting one of the two impulses into two<br />

portions which are used as an integral number of revolutions apart can yield<br />

rendezvous with the impulse of optimum two-impulse transfer. Some<br />

possibilities of this technique were demonstrated by Bender (3.7). Con-<br />

sequently, there exists a determinable lower bound to the velocity increment<br />

to rendezvous for any given case. This bound can be used to evaluate the<br />

effectiveness of any chosen scheme for its nearness to being optimal.<br />

There is a feature of optimal two-impulse orbital transfer which<br />

partially removes the need to optimize. This is the fact that for orbit<br />

pairs which do not intersect deeply <strong>and</strong> which are fairly near to one another<br />

all the way around, the effect of varying the departure point around the<br />

first orbit is not very significant (see Figures 5 <strong>and</strong> 6 of Reference 3.8).<br />

In addition to this feature of this class of optimum, impulsive transfers is<br />

the well known result due to Lawden (3.1) which states that optimal space<br />

maneuvers employing a rocket motor are constructed of zero <strong>and</strong> maximum thrust<br />

segments. Thus, rendezvous schemes universally utilize this principle in<br />

their design.<br />

56

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