‹ Théorie du mouvement de la luneChapitre 403 sur 488 · Ho · texte numérisé non relu

Ho

005 2gt> — co -H c W j — o",oo48 (6) I

= — o",oo48

ieo^ 2 gv — cy — cW j -h o",oo48 (6) |

= -H o",oo48

co5 2gi>-Hcp— cW j -H o",OOo3 (6) J

= -H o",ooo3

COS 2gi>-*-a>-HcW j — o",ooo3 (6) )

= — o",ooo3

005 lEv

H i9"ji36i (3) -h 4", 53 2 7 (4))

COS lEv — CV

cos iEv-\-cv

cos 2Ev -\rc'mv

j — 0", 1609 (4) — o",o 191(5) — o",oo45 (6) j

cos zEv — c'mv

j -H 1 ", 1 2 63 (4) -t- 0", 4oo 1 (5) -h 0", 1 1 5 5 (6) j

Cos 2 Ev — 2 CO

j -h 2",8859 (4) -h o*,5 2 89 (5) -ho", 1 442 (6) |

COS 2Ev-+-2CV

| -H o",o 2 1 6 (4) — o",oo 1 1 (5) |

COS 2Ev — 2 go »

|-ho",i552(5)-o",oi33(6)|

cos 2 Ev -H2gV>

t -h o",o388 (5) -h o",oo63 (6) |

= -h o",oo63

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