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Theoria motvs corporvm coelestivm in sectionibvs conicis solem ambientivm
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RELATIONES INTER LOCOS PLYRES IN ORBITA.

0

a

[1] cosi-p =:} +~

/ . C ,c\ . (e+ i)aW - V~cjV - - -

[3] cos i v' = i ^ & + V "cvr) V~ ' r r~~'

[4] siniv=i^\/Cc V~(J^jV --

Hinc statim demanant sequentes:

/ 1 \ . ee 1

[5] sin.F:=:§a(C

r.

[ 6 ] sin/=|:a(c)/

rr

ee 17 1

rr

17 ] C03F = ^ ( , + i,_ ( C + ^)) - ^[8] co»/=^(C+-L)(c+^-^jr

Porro fit per aequ. X art. 21

r =^ e (v + 7 r ) 1

a

a~ =i e ( a + s)

atque liinc

t*] Jf =-=f(c£-)(«f)

[ 1 0 ] ~ = i ^ (C+ (c +~)2

Haec aequatio 10 cum 8 combinata praebet

r -\-r (c -f ) cos f. y /rr

[11] « =-f-

*(c_ T ) =

Statuendo itaque perinde vt in ellipsieosj est positiuus vel negatiuusj fit

y/ + v'-

. r v r

2 cos f

1 + 2 vel = i