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guidance, flight mechanics and trajectory optimization

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The first area of work to be discussed concerns the <strong>optimization</strong> of<br />

rendezvous using stepwise thrusting either as a series of impulsive thrusts<br />

or as a series of finite burns separated by coasting arcs. This technique<br />

actually results from a development of switching functions from the<br />

Pontryagin maximum principle. In this second <strong>and</strong> third portions of the<br />

section, rendezvous studies involving continuous thrust are described. These<br />

sections deal (for the most part) with the final phase of the rendezvous<br />

maneuver; that is to say, the two objects are on the verge of a very near<br />

collision <strong>and</strong> the engine is to be used with a single burn to alter this<br />

situation <strong>and</strong> produce rendezvous. In this area of study, field free<br />

equations are, in general, satisfactory <strong>and</strong> most work deals with such motion.<br />

There is an area of 1 ow thrust rendezvolls studies in which power !.imited<br />

engines are considered. me cost functions for the fuel for such engines is<br />

quadratic, thus the linear differential. eqllations of motion yield a set of<br />

equations for the optimllm sitllat!on which is 1 inear <strong>and</strong> conseqllentlp so3vabl.e.<br />

Applications of this apnroach have been largely for interp!..anetary studies<br />

which antjci.pate e1.ectrj.c proculsinn systems. Wowever, c!.osed form solutions<br />

obtainab1.e for thi.s type of system have been suggested by Goldstein et. al.,<br />

(3.9) <strong>and</strong> Rrysnn (3.1-O) as useful. aids in studying the rendezvnlls maneuver.<br />

The method of Bryson wi1.3. be described ri.n Section 2.3.2 <strong>and</strong> finally the<br />

continuous low thrust studies (ti.tF linear cnst function) till be presented<br />

in Section 2.3.3.<br />

57

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