... fsnd . fsnd + f D1 . f D1 . , M2 ( ). f rcv = M2 ( fsnd +f D1 ) +f D2 . f D2 . f med = f rcv - f h . f h . ... 3 22 ( R + hm ) R cos 22 1- R cos 2222 1 - ( R + hm ) ( R + h )2m Ri , Ri , ri ri : 2 Ri R sin 2 ri = , ri = . ...
... 1 . . . b e . (5) b 1 h1 , 1 . m b 2 e : B r : * r ,b r r ,m f m ,2 ,A , . . (6) (7) * r ,b f b ,2 ,A , B b ,m , m ,e . ... M J2000 90-2M f f J2000 f f f f f - . 3.1. L2. , A , B * : x1 rL , A A rL , B BrL , rL L2 . ...
... using formulas: E = 2arctg 1e 1+ e p p tg p +h 2M= E e p sin E , if E e p sin E M p ... 222 x1 y1 z1 (48) =M RNB y z Vx DVRNB = M RNB 2 Vx V Vz 1 V y2 2 y1 1 (49) Vz 20 ...
... true anomaly f , describing evolution of the elliptic system, to the dimensionless time t of the TBP is performed tg E tg 1 2 1 f 2 e e M E e sinE tdimensionless M p 1 e cos f dt p3 2 df 1 e cos f 2 · A periodic halo orbit approximation is built with the ...
... 2) : D1 = n1 L1 + B1 + 1 , D2 = n2 L2 + B2 + 2 (3) 1 2 - . , D1 D2 (3) . ... 3) D1min1 , D1min 2 7 mi n1min1 , n2 n1 , min 2 min 2 n1 , n2 , Dlast . ... 2 i sin i cos i cos i - sin i cos i sin i - Vi sin i = - Vi cos i cos i - V cos sin ...
... H 12 1 22 p x p y p z yp x xp y 1/ 2 1 2 x 2 y 2 z 2 x 12 y 2 z 2 m2 m1 m2 . ... 2 y 2 z 2 )1/ 2 ; m1 m2 /2 7 r2 (( x 1)2 y 2 z 2 )1/ 2 : x 12 2 H px p 2 pz ypx xp y ...