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guidance, flight mechanics and trajectory optimization

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when a = semi major axis<br />

Q = one of Herrick's universal variables<br />

A = matrix<br />

A similar relation can be written for the velocity <strong>and</strong> variation in the orbit<br />

parameters<br />

The "correctl' velocity required for rendezvous is then given by<br />

2.3 PROPORTIONAL GUIDANCE<br />

xr = 2 +si<br />

4.<br />

= ‘gi ‘&&)&A? i’<br />

Proportional <strong>guidance</strong> refers to a class of <strong>guidance</strong> laws which exhibits<br />

smooth thrust functions chosen to be proportional to some function of range<br />

<strong>and</strong> range rate. The mechanization of these laws requires throttable motors,<br />

this requirement may be undesirable when compared with the relative simplicity<br />

<strong>and</strong> reliability of constant thrust motors. Also, these methods are ex-<br />

pected to be less optimum than those using constant-thrust motors since<br />

<strong>optimization</strong> of maneuvers indicates that thrusting should occur in periods<br />

of either full or zero thrust (see Section 2.4). The computation of the<br />

thrust vector, however, is quite simple since the gravity model is not<br />

introduced into the equations.<br />

An example of proportional <strong>guidance</strong> is presented by Sears <strong>and</strong> Fellman<br />

(Reference 2.10). In this reference, the rocket thrust is determined from<br />

the equations<br />

c<br />

= s,[p- p I-s,+ St)<br />

c = s3[p-$a+s, (p (ys)<br />

where Sl, S2, S3, S4, S , <strong>and</strong> S6 are constants <strong>and</strong> LS is the angular rate<br />

of the line of sight. 'i The subscripts r, c <strong>and</strong> z refer io the radial,<br />

circumferential <strong>and</strong> out of plane direction.) If the constants Sl <strong>and</strong> S3<br />

are made equal <strong>and</strong> S2 <strong>and</strong> Sk are set to zero, the thrust direction will be<br />

along the line of sight <strong>and</strong> the thrust magnitude will be determined by the<br />

difference between the range rate <strong>and</strong> the square root of the range. For<br />

this case, the <strong>trajectory</strong> as seen by an observer on the target satellite<br />

will appear as in Figure 2.13.<br />

53

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