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Theoria motvs corporvm coelestivm in sectionibvs conicis solem ambientivm
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20

Libr. I. Sect. I.

VI. sin i v.s/r sia i F y/-

P

(e i) cos FP

V (ei)uSimili modo addendo vtrimque i fit

. (e - 4 -1) b

an| F\/ -77

v cos F

. p . (e-\-i)b

= Hu = i(«

u

A~Il. cos \ v.sf r = cos \F\J-

(e+1) cosi*

= cos 2 F\/

= §(w+i)v/'

i- (« +1) v/'

(g1) &

COS jp'

(e1 )b

(e + 1) u w

Diuidendo VI per VII ad III reueniremus; multiplicatio producit

VIII. r sin v = pcolaxigip tangF = b tmgyj tangi 1 '

= i p cotang yj (u~) = £ b tangy* (u)

E combinatione aequatt. II, V porro facile deducitur

1 j ®

IX. rcosv~b(e ~ o&F ) =i b ( 2 e u)

X. r

22 .

Per differentiationem formulae IV prodit (spectando y/ vt quantitatem con-

stantem)

rr dv =

d u

u

~ i ('

tang i(p + yj) tang i {?

yi)j d v =z

r tangy/

d v ; hinc

pr

u tang 7,

'P

d u, siue substituendo pro r valorem ex X,

rr&v

bb tang 7^/

(

hu

-)

v)

dzj

Integrando deinde ita, vt integrale in perihelio euanescat, fit

J

frrdv bbtangyj (i e (u) logu) = ht\/p. y/(i +^) r= lttangyj\/b.\/{1

Logarithmus hic est hyperbolicus quodsi logarithmos e systemate Briggico vel ge-neraliter e systemate cuius modulus X adhibere placet, massaque p (quam procorpore in hyperbola incedente haud determinabilem esse supponere possumus) ne-giigitur, aequatio hancce formam induit:uu 1 211

XI. iXe

u

logu