guidance, flight mechanics and trajectory optimization
guidance, flight mechanics and trajectory optimization
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 />
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