Borelli, Giovanni Alfonso
,
De motionibus naturalibus a gravitate pendentibus
,
1670
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31 - 60
61 - 90
91 - 120
121 - 150
151 - 180
181 - 210
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391 - 420
421 - 450
451 - 480
481 - 510
511 - 540
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da erit. </
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<
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">Et quia fluidum catenùs motum, quem fluxio
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nem vocamus, elicere poteſt, ſcilicèt catenus fluidum
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eſt quatenùs eius aliquæ partes mouentur cæteris
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quieſcentibus, vel diuerſis, & inæqualibus motibus
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agitantur ab ijs, qui competunt duris, & continuis
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corporibus; ergò ad hoc, vt nulla particula corporis
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fluidi care at hac paſſione fluiditatis; oportet vt ſem
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per ei conueniat fluiditatis definitio, ſcilicèt ſemper
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quælib et eius pars moueri poſſit cæteris quieſcenti
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bus, vel inæqualibus motibus agitentur, quàm ſint il
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li, qui duris, & continuis corporibus competunt. </
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<
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partes contiguæ eiuſdem maſſæ non poſſunt partim
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moueri, partim quieſcere, vel inæqualibus motibus
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agitari diuerſo modo, ac continuis corporibus
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cõ-
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petit, niſi inter ſe ſint diuiſæ, & diſcretæ; igitur nul
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la particula fluidi corporis quantumuis exigua aſſi
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gnari poteſt, quæ actu diſſecta, & ſubdiuiſa non ſit in
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plures alias particulas; qua propter nunquam perue
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niri poterit ad finem enumerationis multitudinis par
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tium eius, & ideò talis multitudo maior erit
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quocũ-que
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que</
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numero, ſcilicèt maior quacumque quantitatę
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finita, ergo infinita erit; at infinitæ partes actu diui
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ſæ ſi eſſent quantæ ſiue inter ſe æquales, ſiue non, effi
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cerent
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extẽſionem
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in finitam, ergò ſphęra fluida pal
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maris eſſet infinitæ magnitudinis, quod eſt falſum̨,
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igitur non quantæ, ſed indiuiſibilia puncta erunt; hoc
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verò eſt quoque impoſſibile, cùm infinita puncta ex
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tenſionem quantam nequeant componere: ergò fal
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ſum eſt, quòd minimæ particulæ ex quibus fluidum̨ </
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