Gravesande, Willem Jacob 's
,
Physices elementa mathematica, experimentis confirmata sive introductio ad philosophiam Newtonianam; Tom. 1
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MATHEMATICA. LIB. II. CAP. I.
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<
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3.</
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<
s
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xml:space
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">Tubi vitrei A, B, D, eodem modo, ac de tubo A in
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præcedenti Experimento dictum, aquâ immerguntur, & </
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<
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.
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fig. 2.</
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aqua in omnes, ſublato digito, ad eandem altitudinem ad-
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ſcendit, quàm in tubo C; </
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<
s
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xml:space
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</
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<
s
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xml:space
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">in tubo B deorſum; </
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<
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xml:space
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">in tubo A eſt lateralis; </
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<
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xml:space
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liqua; </
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<
s
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xml:space
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">in unoquoque tamen preſſio æqualis eſt; </
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<
s
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xml:space
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fluidi quantitas vaſe infundatur, æqualiter etiam aqua in ſin-
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gulis tubis elevatur.</
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<
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<
s
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xml:space
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">Ex hiſce ſequitur fluidorum particulas ſingulas ab omni
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parte æqualiter premi, & </
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<
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">ideo quieſcere; </
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<
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tinuo inter ſe moveri, ut a multis ſtatuitur.</
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</
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<
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<
s
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xml:space
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">In tubis communicantibus, ſive æqualibus, ſive inæqua-
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">714.</
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libus, ſive rectis, ſive obliquis, fluidum eandem adipiſcitur
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altitudinem; </
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dem plano horizonti parallelo; </
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<
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citur.</
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<
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<
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">Sit vas A, tubus verticalis B, & </
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">tubus inclinatus D; </
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<
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">715.</
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municationem habeant ope tubi CE; </
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<
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xml:space
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<
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.
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fig. 3.</
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& </
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<
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xml:space
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">concipiatur ſuperficies horizonti parallela fgb; </
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<
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tudines fi & </
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nor eſt . </
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rint æquales, aqua non quieſcet; </
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<
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do l & </
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<
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ſio oriatur ex gravitate partium, quæ tendit ad terræ cen-
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trum, altitudo fluidi prementis juxta hanc directionem
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menſurari debet, id eſt, erit bm; </
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<
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mnæ bn nullam mutationem adfert; </
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funditatem ubique preſſio verſus omnes partes æqualis da-
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tur .</
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<
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4.</
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<
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<
s
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<
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nem quamcunque non quieſcit, niſi omnes ſuperficies
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fig. 4.</
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ſint in eodem plano horizonti parallelo. </
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<
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cum tubis vitreis B & </
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<
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tur.</
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