Bewegung vom Typus 2/3 im Dreikörperproblem. 

 2 r^3.i.oi5 



^20 — ''^97o%+ ^" ^'O.O ßl3+ :^ 4:o.O ßl6+ \^ A^Ö;!'" ^5 + 



/j — A(+U L Jl-O fi _L J_ Jl R L J -1-1 -OO ■ J_ 4-1.1. OD 



V21 — ^0.1.1 r) 3.0.0l^8^ r) o.O.O 1 9 „ '^3.1.0 rs^ ^ "^3.0.1 I2 



- Y ^6^I-'i'° ^^"*' 7 A"i:l-°ßi- f l^-i^.o.oTs + -| P-'-ls 0.0Y9 



387 



(29) 



Analog erhält man für P: 

 P =: p„+Pi COS oiv+p./f^ COS \' +/'4T| COS (3w—\') +Pf,ri cos (6>y— v) 

 +P3'ri' cos \'i+/'5''l' cos (3;i' — Vj)4-j'7-Tj' cos (ßiv~\\) 



+ /-',,rj^ cos 3jy 4-/'i4Yi^ cos (3»w— 2v) +/7j-rj'' cos (6w— 2v) +p.^,^ri^ cos (Otv — 2v) 



+;'j,iTjTj' cos (3/i' + V — VJ+^ijjTjTj' cos (3;y — V — Vi)+/',^r|7)' cos (6W — V — Vj)+/72jTjYl'c0S (9W— V — Vj)| 



+/iiiTj7]' cos (3w — v+Vj)+/'j^r/'^ cos (3w— 2Vj) +Pi.Ji'^ cos (6w— 2vj) +P22'^^ cos (9^^— 2Vj) 



(30) 



+/?j,,7)'^ cos 3^ 

 wobei: 



+;'23'ri-r|'cos(v-v,) 



Constanter Theil; 



Po = ;ßo,oj+ - Ä:°.o ßi + - P-Sa.o.oYr + - B^:l, ß? 



Ordng. 



II. Ordnung 



III. Ordng. 



(31) 



0. Grad. Coefficienten in P„ 



1 



p, = B3.0.0+ [Bll^ + -Bi-l,] ßi+3[j.ßß.o.oYi 

 I. Or'dng! 



II. Ordnung 



+ ) — B"'^ + ^ «-0 + - B'" ' ß'^ 

 ^ j r, •".■i.O.O ^ . -".3.0.0 ^ . ^9.0.0 ' l'l 



/ 4 'J-O-o 4^ -"g.o.orPi'i 



+ ['•' < -S3 0.0-4 -ßs.o.oH -Bg.o.o > Y?- 



( 4 8 8 ) 



III. Ordnung 



(32) 



