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guidance, flight mechanics and trajectory optimization

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I(7)<br />

I<br />

COMPUTE<br />

c (7)<br />

=- MISS<br />

g-r -1 =P-<br />

*Block Diagram of Miss Distance Guidance<br />

Figure 2.12<br />

APPLY TRANSITION<br />

EtrCMATRIX TOP(r)<br />

TO DEEIERMINE<br />

VELOCITY C@RECTION<br />

Because of the fact that the solution to Lambert's problem, in the<br />

first method, is replaced by a repeated application of the equations de-<br />

termining the position followed by a matrix operation, this second method<br />

holds considerable computational advantage over the first. This simpli-<br />

fication is purchased, however, at the expense of generality in the method.<br />

Some of the difficulties mentioned in the first paragraph of this<br />

section can be overcome by the incorporation of direct measurement of the<br />

relative range into the equation defining the velocity. Such an incor-<br />

poration is discussec by Gedeon (Reference 2.14). In this reference, Gedeon<br />

compares the direct measurement of the relative range with that calculated<br />

by the conic equations for application to a process employing differential<br />

corrections of the transfer orbit parameters. Only an outline of this<br />

procedure is presented here, since the reference uses Herrick's universal<br />

parameters rather than the orbital elements discussed to this point. The<br />

coordinate system is such that the 2 axis is normal to the "transfer" orbit<br />

<strong>and</strong> x is along the radius r . Let the subscripts m <strong>and</strong> c denote the<br />

measured <strong>and</strong> calculated values of the relative position ( AX, AY <strong>and</strong> 4~ );<br />

then the residuals ( 6x , 8~ ) are defined by<br />

where<br />

6x = Ax, -Ax,<br />

A relation between these residuals <strong>and</strong> variations in the elements of the<br />

transfer orbit can be written as<br />

52

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