Bernoulli, Daniel
,
Hydrodynamica, sive De viribus et motibus fluidorum commentarii
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SECTIO SEPTIMA.
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nam, quantum ſuper eandem elevata fuerat, provenit iſte defectus ab aſcenſu
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pot. </
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">aquæ durante deſcenſu ejectæ, cui debet eſſe proportionalis.</
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<
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">Notabile eſt, quod cum eo profundius deſcendat aqua in cylin-
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dro, quo magis ab initio deſcenſus fuerit elevata & </
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<
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">quo majori lumine perfo-
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ratum eſtfundum, nunquam tamen omnis aqua ex cylindro effluere poſſit
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quantumvis fuerit ante deſcenſum elevata & </
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<
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">pars cylindri ſubmerſa utlibet
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parva, ipſumque ſimul foramen vel totum fundum exhaurire ponatur.</
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<
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">Velocitas ſuperficiei aquæ internæ maxima eſt, cum ſumitur
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x = ({a
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/nna - nnb - a + 2b})
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<
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<
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">Si proinde n = 1, exiſtente ſcilicet orificio cylindri toto aperto, fit
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x = b, & </
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">maxima eſt velocitas, cum ambæ ſuperficies ſunt in eadem altitu-
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dine poſitæ.</
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<
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">Quia vero multa ſunt, quæ ex hiſce æquationibus dignoſci nequeunt
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in duobus caſibus, nempe nn = 1 & </
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">nn = 2, hique multa habent particula-
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ria, eoſdem ſeorſim jam attingam.</
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">erit - xdv = (x - b) dx (per §. </
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- dv = dx - {bdx/x}, quæ ſic integrata, ut ſit ſimul v = o & </
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x - a + b log. </
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xml:space
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">{a/x}, ſeu v = a - x - b log. </
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. </
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">Ut obtineatur maximus deſcenſus, faciendum eſt a - x - b log. </
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<
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= o; </
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<
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">patet autem ex iſta æquatione, nunquam negativum valorem obtinere
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litteram x, imo nequidem totam evaneſcere ſine contradictione, niſi pona-
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tur {a/b} = ∞, quod indicat fieri non poſſe, ut omnis effluat aqua durante de-
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ſcenſu in iſto caſu & </
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<
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quintum.</
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. </
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<
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">Velocitas maxima talis eſt, quæ debetur altitudini a - b - b log. </
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<
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atque ſi differentia inter a & </
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<
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">b, quam ponam = c, ſit valde parva, exiſten-
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tibus nimirum excurſionibus fluidi perexiguis ratione longitudinis, ad </
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