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Theoria motus corporum solidorum seu rigidorum ex primis nostrae cognitionis principiis stabilita et ad omnes motus, qui in huiusmodi corpora cadere possunt, accommodata / auctore Leonh. Eulero
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562 CAPUT V. DE MOTU GLOBORUM,

— iSefgt coffl 2 $gtdt .

=2-------erit</X = crf* + -^- (e/finfi-*)

eL -f- (x/' finh — e) &

. v - i&fgtdt coffj ~ v v , . Sgtt , , r f v

et a Y =-—--—, ideoque GX = X = et -f —-—(f/finy — e)

Fig. 139, et XI = Y -

k

- Ssfgtt

cosh. Tum vero pro mota gvratorio, qui

jam fiat in fenfum ZfiTD celeritate angulari = y circa polum O exifienteZO — x, I>ZO = et DZQ = (p + ubi I Q refert diredlionem cele-ritatis radentis, quia eonfianter e(t <p + £ = fcu direrftio IQ confians,

v - x/cofh ... ef ~ e lin[p

erit tang| = - - ; -, et tang (% — S) —

2 Sfgkt

eefRnfy — ee + 2^gkt'

e coi f)

+ &) =

, unde ambo anguli £ et $ definiuntur. Vel erit tang (<p

se an cofh

eaak fin h -f 2 Sfgt (e - ef fin h)

Celeritas autem radens fecun-

saak cofh — 2 Heffgt coffjdum diredionem IQ^efl w = k — i<$g t. Tum vero ob

4 fofgt (k/--finh)

a cof/ = o, erit arcus ZO = x quadrans, et a — / —

, 4 Uffggtt

aak

tempus t =

tt ^aak

. Hic motus inaequabilis autem tantum durabit per

quo elapfo efi tangtp =

■ aaj coff)

2 <tg{na+ff)

— ena cofb Z' aaae (ef fin b — e) - a*kk

f [ee + ■-—- +

e { aa +Jf ) + a n (f/fin^-f)

L_"^

o* J'

zfsaa R n^ ' V ' ari ‘ ( aa +ff ) 2

v / (eeff + iseaaf fin h -f- sg a 4 )

s = 9o°, et »=—-.= r-XcU- 7 - i -fubfiituto pro

/ aa+ff

kk valore. Tum autem fit angulus A = 90°, et fin £ = -——.

v

C 0 R O L L. U

1199. Si initio fuerit angulus DZO = f = o, erit k = \f (ee -fi eeff)

pro angulo DZQ^ £ fit fin g— —~ j c ofg= -— tum pofi tempus

k 1 k