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guidance, flight mechanics and trajectory optimization

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endezvous velocity requirements from a much wider range of initial con-<br />

ditions than any of the methods discussed previously.<br />

In order to use the two-body equations of motion to determine the<br />

required velocity a time at which rendezvous is to occur must be selected.<br />

Some criteria for selecting the rendezvous.time, r , have been given in<br />

Sections 2.2.3.2 <strong>and</strong> 2.2.3.4. For the purpose of illustrating the method,<br />

it is assumed that the time till rendezvous is determined from some range<br />

range-rate function, i.e.,<br />

.<br />

G = f’(r) (2.16)<br />

as in Section 2.2.3.4. The procedure is (1) measure the relative range;<br />

(2) determine the desired range-rate ( 6 ) from Equation (2.16), (3)<br />

calculate the time of rendezvous, r , as<br />

R<br />

r= y-<br />

rd<br />

where Pm = measured range<br />

.<br />

5 = desired range rate<br />

(4) determine the position of the target at r using two-body equations<br />

<strong>and</strong> knowledge the target orbit (5) compute the required velocity by solving<br />

Lambert's problem using the position of the.target at r , the position of<br />

the rendezvous vehicle at t = 0 <strong>and</strong> the desired <strong>flight</strong> time r .<br />

TARGET ORBIT REmEzVOUS KEKICLE<br />

ELEMENTS 1 POSITION AT t = 0 1<br />

1<br />

A<br />

1<br />

CALCULATE<br />

POSITION<br />

OF TARGET<br />

----I<br />

;T TTM-5’ =<br />

Block Diagram of Conic RendezGous Calculation<br />

Figure. 2.11<br />

REQUIRED<br />

VELOCITY<br />

If the position <strong>and</strong> velocity of the target vehicle are expressed in an<br />

inertial coordinate system whose origin is at the center of attraction, then<br />

the position at time T can be calculated from the following (sequential)<br />

set of equations<br />

r= x't<br />

f<br />

'tz<br />

2

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