Astrodynamics 102 - DerAstrodynamics.com
Astrodynamics 102 - DerAstrodynamics.com
Astrodynamics 102 - DerAstrodynamics.com
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2-Body Lambert Algorithm<br />
Lambert's Equation for multi-revolutions (Sun)<br />
F ( x) = (x ) y) N 0<br />
Iterative Equation (Laguerre)<br />
Multi-revolution Lambert Algorithm<br />
n F (x i )<br />
i+1 i <br />
for i 1,<br />
2,..<br />
F (x i ) 2 2<br />
F (x i ) (n 1) F (x i ) n (n 1)<br />
F (x i )F (x i )<br />
F (x i )<br />
x x<br />
References:<br />
Sun, F.T., “On The Minimum Time Traj . . ”, AAS 79-164<br />
Der, G. J., “The Superior Lambert Algorithm”, AMOS,2011<br />
v (t )<br />
Lambert Problem<br />
Given: r (t ) , r (t ) , t , t , inc_to<br />
Find: v (t ) , v (t )<br />
object at t 2<br />
2<br />
Transfer<br />
Orbit 2<br />
1<br />
r (t )<br />
2<br />
1<br />
v (t )<br />
2<br />
2<br />
2<br />
Transfer<br />
Orbit 1<br />
<br />
Sphere<br />
1 2<br />
Transfer orbit 1: inc_to = 1, i < 90 o<br />
Transfer orbit 2: inc_to = 1, i > 90 o<br />
Multi- revolutions (N)<br />
may have ( 2N + 1 ) solutions<br />
for each inc_to and a given <br />
v (t )<br />
1<br />
r (t )<br />
1<br />
object at t 1<br />
v (t )<br />
1