guidance, flight mechanics and trajectory optimization
guidance, flight mechanics and trajectory optimization
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 />
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