Bernoulli, Daniel
,
Hydrodynamica, sive De viribus et motibus fluidorum commentarii
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HYDRODYNAMICÆ
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<
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xml:space
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">Hæc autem de oſcillationibus finitis. </
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eſſe cenſeamus, videbimus illas fieri omnes inter ſe tantochronas, manen-
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te eadem fluidi quantitate, eodemque canali, quæcunque interea ſint cana-
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lis figura & </
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">Oſcillationes minimæ fluidi in quocunque canali oſcillantis,
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quamvis inæquales inter ſe, ſunt omnes Iſochronæ.</
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<
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">Cum oſcillationes ſunt minimæ, poſſunt illæ canalis particulæ, in qui-
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bus ſuperficies fluidi agitantur, pro cylindricis haberi, igitur manentibus
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denominationibus iisdem, manebit valor, quem aſſignavimus litteræ v in
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§. </
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">ex eadem ratione ſequitur, litteras a, b, α, β & </
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">x ceu infinite parvi
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valoris negligi poſſe præ {M/g}, ſic ut in præſenti caſu cenſeri debeat
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v = {2gγaαcx - (gγαb + ggab)xx/2γaαMN}</
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<
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">Sunt igitur vi paragraphi duodecimi oſcillationes omnes, quoad mi-
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nimæ ſunt, inter ſe Iſochronæ. </
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oſcillationibus minimuis fluidi in canali quocunque agitati.</
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dt = dx√(2γaαMN/gγαb + ggab}):</
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Igitur vi Paragraphi decimi tertii erit longitudo quæſita penduli cum præ-
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dictis oſcillationibus tautochroni = {γaαMN/gγαb + ggaβ}. </
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