Bernoulli, Daniel
,
Hydrodynamica, sive De viribus et motibus fluidorum commentarii
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HYDRODYNAMICÆ
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<
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">9. </
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">Fuerit igitur vas cylindricum verticaliter poſitum aqua ple-
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num, ſitque altitudo aquæ ab initio fluxus = a, amplitudo cylindri = m, am-
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plitudo foraminis = n, Sectio venæ ſolidæ = {n/α} effluxerit jam aqua per tempus
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t; </
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<
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">ſitque tunc altitudo aquæ reſidua ſupra foramen = x, eodemque temporis
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puncto habeat ſuperficies aquæ internæ velocitatem, quæ reſpondeat altitudini
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v: </
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<
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">erit velocitas ipſa = √ v, eſt autem elementum temporis d t proportio-
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nale elemento ſpatii - d x diviſo per velocitatem √v, unde dt = {- dx/√v}.</
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<
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">Determinatus @equidem fuit valor ipſius v in ſect. </
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<
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nationibus uſi ſumus, quibus nunc utimur. </
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">At quoniam pro recta aquarum
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erogatarum menſura requiritur, ut foramini n ſubſtituatur ſectio venæ con-
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tractæ {n/α}, ſequitur, ut in valore ipſius v eadem fiat ſubſtitutio atque ſic ſta-
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tuatur v = {nna/2nn - mmαα}(({a/x})
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- {x/a})</
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<
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">Hic vero valor ſi ſubſtituatur in æquatione
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dt = {- dx/√v}, oritur
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dt = - dx: </
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<
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">√[{nna/2nn - mmαα} (({a/x})
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- {x/a})]
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ope cujus æquationis omnia tempora deſiderata definiri poſſunt per approxi-
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mationes, ſeu ſeries, ſi modo in ſingulis punctis valor ipſius α innoteſcat:</
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Aſſumemus autem eſſe illum conſtantis valoris, quandoquidem in præſenti
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caſu nihil ſit, à quo mutari poſſit præter diverſas altitudines & </
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">velocitates
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fluidi, quæ parum vel nihil quantum ſenſibus percipi poteſt ad id negotii
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conferunt.</
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<
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">Jam ut æquatio deſiderata per ſeries exhiberi poſſit, conſiderabi-
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mus quantitatem.</
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<
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">√[{nna/2nn - mmαα} (({a/x})
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- {x/a})] fub hâc forma
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({nnx/mmαα - 2nn})
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X (1 - ({x/a})
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) -
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