Borelli, Giovanni Alfonso
,
De motionibus naturalibus a gravitate pendentibus
,
1670
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ſities R fluidi N motui corporis A ad
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eã
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retardatio
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nem quam ei affert craſſities S fluidi M eodem tem
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pore T, ſe habet vt ſpatium EL ad ſpatium DL, quæ
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ſunt retardationes factæ in eiſdem fluidis, igitur ve
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locitas corporis A in fluido M ad eiuſdem velocita
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tem in fluido N habebit
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minorẽ
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proportionem,
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quã
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craſſities, & reſiſtentia fluidi N ad craſſitiem alterius
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fluidi M. </
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Cap. 10. de
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æquitempo
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ranea natu
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rali veloci
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tate
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">Ponatur poſtea DL æqualis CE, habebit ED ad
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duas æquales eamdem proportionem, & componen
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do DC ad CE erit vt EL ad LD, & ideò vt craſſities R,
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ad S, ita erit velocitas corporis A in M ad
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velocitatẽ
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eiuſdem in fluido N. </
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ponatur DL maior, quam CE, ſequitur quod
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DC ad CE maiorem proportionem habet quam EL
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ad LD, & ideò velocitas ipſius A in M ad eam, quam
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habet in N maiorem proportionem habebit, quàm
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R ad S, ſcilicèt, quàm craſſities fluidi N ad
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fluidi M. </
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COROLLARIVM.
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<
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">HInc ſequitur verum non eſſe quòd velocitates
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eiuſdem corporis grauis in duobus medijs flui
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dis ſemper reciprocè proportionales ſint reſiſtentijs
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eorumdem fluidorum. </
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ſcendere in ſpatio inani ablatis omnibus
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impedimẽ-tismedij
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tis medij</
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abſoluta, & inalterata eius velocitate natu
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rali, vt nimirum tempore vnius minuti ſeeundi hora-</
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