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# Title: Leibniz-Handschriften zur Mathematik LH 35, 10, 13
# Folio 4v, page id 00068166:0008
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farelon ita jam re omni ad volos motus notabiles reducta, omnique spictione, aute nemat
privatum resecta calculum iterum assumamus, paulo aute peractum, sed ad hibitis praeter globum
alobit E et (E) in contraria  inter se aiqualibus in contraria tendentibus, supposite angulo NCG acutissmo,c
vel DC(G) aculissimo, ita ut DH sit = bis DC + C(G) seu DC+ C DC, et DH)  DC - DC, posi nempe  punc
Get H existentibus pro E et (G) et (H) pro (E). ita ut motus ipsius E copositus sit duplus motus navis, at motus ipsiuse
sit nullus. Hinc ca balis A initio vis erat eterandi globum i, ad altitudinem 1K, et glubo E ad altitu–
dinem et globos E et (E) ad allo tudrum M N. ictu facto navis, cum globis Ee+(E) sumta aequalis glovo quiescente globo
hanc vim recipit, velocilatamque accipit  et directionem Cd; liberentur jam globi, ii descensu usque ad horczontem per
ostillationem facta hobvi viassugeri in navi habebunt vim es sssurgendi ad MN et vel velocitatem et directio
nem CG et (G), posito autem CG C() (aequadis inte e) aequari ipsi Cd patet etim ma et ik aequari et vim
cujusque exprimi posse per quad ralam velocitatem ) in corpus ductam. Sed si traduntur in grovi in oscillatiisnem extra
navem, ibi velocitas ipsius globi E erit CH,  quae est dupla CG; g (seu CG+ CG) globi vero (E) est nulla (nempe
(G- CG) navis autem suam celeritatem relinebit, n est autem navis moles, = 1- 26. Nunc ergo calculus
sic habetur: initio vis erat, 1. in C9quadr. Nanc vero, est 1 - 2E in CGqu. + E in q4. CGqu = C in 0. CG qu
Taced. Quae vires deberent aequari inter se, fieretque: I = )  2E +4E. seu 2l=b quod est abs.
itaque  cum omnia jam accidentia resecuerimus tali hypothesi pro deminstrato habendum est, rem compositionum procedere
non posse. Globas igitur in aere malum trahere intelligendi sunt modis diversis, quia mt licet contrria licet per se eo
idem modo habeant ad navem, unus tmmen motus est motui navis conloarius, alter consporans. Idem sine transditione obtiner
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motur
vroro ronise
potest, si  durante oscillatio
navi occurrat aliud aequale
corpus, I- E a quo sistatur
nam E et (E) globi non ideo sister
tur. Erit ita operae petium
judagare quid tandem piepi
debeat in talibus casibus. um dupli
isto E. et E). Quin et quid Cumisim
plici illo solo E, quod videtur conti–
une tardare debere motum nanis
retrahendo. Sed quid tum, semperitamm
aiquid motus oscillatorii refinebit
et quicquid agumus non apparet
a in fine liberationis eadem quaestio
manebit. Nec video proinde quod
copositiones motumu palvari possint
Interim tamen nec aliter exitum vide
quem enim quaeso motam accipiet E
an solam suam vim propriam susti–
nebit vi communi in navi relicta
An considera. Recurrendum ergo erit
ad experimenta in ve lam perplexa
ngens et Neu F0
Angenio et Neutont
L8V5