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guidance, flight mechanics and trajectory optimization

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The solution to these equations are<br />

I (2.13)<br />

From these equations, it is seen that the position <strong>and</strong> velocity will simultaneously<br />

go to zero if k < 1. However, if the acceleration is examined,<br />

it will be found that for $ 4 k < 1 infinite acceleration is required<br />

as t -c f/4 . Therefore, for practical rendezvous, k must be restricted to<br />

the range 0 4 k c 3.<br />

Flight control is accomplished by generating an error signal, V,, from<br />

the continuous monitoring of the actual <strong>and</strong> desired velocity<br />

<strong>and</strong> igniting the rocket motor whenever this value reaches a specified thres-<br />

hold. The thrust angle (i.e., the angle between the thrust vector <strong>and</strong> the<br />

x axis) is<br />

e=ay:cbo<br />

Figure 2.6<br />

In-Plane Steering Angle<br />

The relative out of plane motion (i,) is sinusoidal <strong>and</strong> uncoupled from the<br />

planar motion. Thus, the-out of plane motion could be nulled separately;<br />

alternately, the desired Z can be selected as some function of the Z error,<br />

e-&J<br />

2, = -az<br />

44

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