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Theoria motvs corporvm coelestivm in sectionibvs conicis solem ambientivm
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76

I. A

II

III

Libe. I. Sect. II.

sin co cos u + cos co sin u cos isin a sin u + cos co cos u cos i

cos co sm u sm i

'(4f)=- sir

&_ / d i \

r \d«/

A^ /_d l \ _

r V dr A '

IV. (j = 1 + -g- COS {L & co) = 1 +^-cos(Z,/)

/db\ , . . . . , . . .. ,

. A f J = cos co cos u sin b sin co sin u cos i sm b + sm u sm i cos b

_ T A /d b\ . . , ...

I. 1 \ = cos (o sin u sin b sin a cos u cos i sm b -f cos u sm ? cos b

, r A /d b\ . . , .

VII. -p- i -jj- J sm co sm u sin i sm b -f- sm u cos i cos b

V.

VI

VIII.

A_

R

(1L)

\d&J

: sin b sin ( Z >Q co) sin b sin {JL T)

Formulae IV et VIII liic iam In forma ad calculum commodissima apparent; for-mulae I, III, V autem per substitutiones obuias ad formam concinniorem redigun-tur, puta

I*

HI*

(*)= ,T' ! '

m-

cos co tang bR

R

V * ("dr) ="72T cos ( L ~ l ) sin5 =7^- cos (£ /) tang/

Denique formulae reliquae quoque II, VI, VII per introductionem quorundam an-gulorum auxiliarium in formam simpliciorem abeunt: quod commodissime fit se-

. tang co

quenti modo. Determinentur anguli auxiliares M, N per formulas tang./!/ =-

cos l

tang N sin co tang i = tang M cos co sin i. Tunc simul fitcos i 2 -}- sin co 2 sin i

cos M 2cos JV 2

i 2

i -f tang A ?i -f tang M z

cos i 2 -ftang co z = cos : ^ am fi uum ambiguitatem in determinatione ipso-

rum M i N per tangentes suas remanentem ad lubitum decidere liceat, hoc ita

e x . , , cos M sin IV , . .

heri pos e patet, vt habeatur - -r- -j- cos co , ac proin: = 4- sm i. Qui-

COS iV j r gjjj jyi

bus ita factis, formulae II, VI, VII transeunt in sequentes: