Gravesande, Willem Jacob 's
,
Physices elementa mathematica, experimentis confirmata sive introductio ad philosophiam Newtonianam; Tom. 1
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MATHEMATICA. LIB. II. CAP. XII.
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terminatur velocitas, quæ corpori quieſcenti a fluido com-
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municatur, quàm retardatio quam corpus patitur; </
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<
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ergo velocitatem hanc conſiderare, quæ ab ipſa retardatione,
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corporis agitati per fluidum quieſcens, non differt .</
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<
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</
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<
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<
s
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xml:space
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mediate corpus poteſt transferre, ſequitur igitur velocitatem
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infinite exiguam, momento infinite exiguo conſtanti, com-
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municari, proportionalem ipſi ſpatio, per quod corpus hoc
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quieſcens actione fluidi immediate transfertur, quod ſpa-
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tium ipſi preſſioni proportionale eſt , quæ ipſa
<
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ſequitur quadrati velocitatis .</
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<
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</
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<
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xml:space
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">Diminutiones idcirco velocitatis, quas corpus in fluido mo-
<
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">954.</
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tum, momentis infinite exiguis, æqualibus, ex reſiſtentiâ
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ex ſecundâ cauſâ, patitur, ſunt ut quadrata velocitatum
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ipſius corporis.</
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<
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xml:space
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reſiſtentiâ ex ſecundâ cauſâ integram poſſe amittere veloci-
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tatem.</
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<
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tia, eandem cum ipſa rationem ſequi, quamdiu corpus mo-
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tum eandem materiæ quantitatem continet, ubi autem hæc
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eſt diverſa, retardatio eſt cæteris paribus, inverſe ut hæc
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materiæ quantitas . </
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<
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xml:space
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">Ex quibus facile videmus,
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poſitis demonſtratis in capite præcedenti retardationes pro
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variis corporibus, & </
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<
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ſint.</
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<
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">Si de ſphæris, cylindris, aut conis ſimilibus, Ex. </
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gatur, poſitis cylindris, & </
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<
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">conis, juxta axium directiones
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motis, erunt retardationes ex ſecunda cauſa directè ut qua-
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drata diametrorum , ut quadrata velocitatum , ut
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tates fluidorum ; </
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bi diametrorum . </
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ſa cuborum diametrorum, ad inverſam ipſarum diametro-
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rum reducitur; </
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ſunt retardationes inverſe ut diametri.</
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<
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