guidance, flight mechanics and trajectory optimization
guidance, flight mechanics and trajectory optimization
guidance, flight mechanics and trajectory optimization
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The boundary condition to be satisfied by R(x,yj will in all cases<br />
take the form<br />
R(X/, Q-0 (2.4.62A)<br />
whether<br />
the Ix,<br />
the point<br />
) space.<br />
(%+-,g ) is fixed or allowed to vary on some surface in<br />
In tile latter case, however, Eq. (2.4.62A) has several<br />
alterna f e representations similar to those developed for the l-dimensional<br />
problem "e.g. Eqs. (2.4.46) to (2.4.52) . For example, if the terminal<br />
Point<br />
straint<br />
(xr 9gf 1 is required<br />
equations<br />
to lie in the surface specified by the icon-<br />
(2.4.62~)<br />
the boundary condition ofp as given in (2.4.62A) can also be mitten as<br />
R(z,@=O OA/ G(z,yI=03jg,.(~,y)=~ ; i=l,mj (2.4.6yi)<br />
or analogous to Eq. (2.4.52), as<br />
where// is the m dimensional vector<br />
(2.4.63~)<br />
(2.4.64)<br />
Thus, by combining (2.4.63B) with (2.4.60) <strong>and</strong> using the <strong>optimization</strong> con-<br />
dition inherent in (2.4.60), that<br />
-+- af JR = 0<br />
a$( afi<br />
i L’= 1, n<br />
(2.4.65)<br />
the transversality conditions of the Calculus of Variations, corresponding<br />
to the terminal constraints of Eq. (2.4.62B), can be developed. These<br />
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