Bernoulli, Daniel
,
Hydrodynamica, sive De viribus et motibus fluidorum commentarii
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SECTIO NONA.
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<
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">Ut jam determinetur inclinatio plani ad fluidum ſub his circumſtantiis
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maxime favorabilis ut motus plani in directione B b promoveatur: </
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A B = 1, D E ſeu A C = x, B C = √1 - xx; </
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<
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">lineam E B, quæ repræ-
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ſentat motum fluidi, = v, & </
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<
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">B b ceu menſuram motus plani = V; </
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<
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ſic inſtituto calculo invenitur
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ef = xv √ (1 - xx) - (1 - xx) V, atque BN = [xv - V √ (1 - xx]:
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</
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">√ (vv + VV); </
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<
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">unde e f X B N = [xv - V √ (1 - xx)]
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X {√ (1 - xx)/√ (vv + VV)}, quæ
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quantitas maxima erit, cum fit
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(9v
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+ 18vvVV + 9V
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)x
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- (12v
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+ 30vvVV + 18V
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) x
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+ (4v
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+ 16vvVV + 9V
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) xx - 4vvVV = o.</
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<
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">Calculus ratione inclinationis alarum in moletrinis alius eſt,
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quia velocitates in diverſis alarum locis variæ ſunt; </
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<
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">ſunt enim proportiona-
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les diſtantiis à centro, facile autem nunc cuivis erit computum pro mole-
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trinis inſtituere, huic caſui non ulterius inſiſtam, ſufficiat id notaſſe, quod
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non ſatis accurate ſtatuatur ab auctoribus x x = {2/3}, & </
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ſius x ſemper minor ſit quam √ {2/3}. </
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">omnia alæ
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puncta ſimili velocitate moveri cenſeantur, fiet x = √ {1/2}, quod indicat in-
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clinandam eſſe alam ad directionem venti ſub angulo ſemirecto. </
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alarum conſtructio foret, ſi incurvarentur, ita, ut ſub angulo minori ventus
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in illas impingat ſuperius quam inferius, aut ſi fiat ut alæ ubique ventum
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ſub angulo medio quinquaginta præterpropter graduum excipiant.</
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<
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<
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que id inclinatum ſit, excipi ponitur. </
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particularum dato tempore impellentium ſemper idem eſt, nullam eſſe at-
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tentionem faciendam ad linem B N, atque ſic niſum quem aquæ faciunt ad
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movendum planum A B in directione B b ſimpliciter repræſentari per e f ſeu
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xv√1 - xx - (1 - xx) V. </
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">Igitur niſus iſte maximus obtinebitur ſumendo
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xx = {1/2} + {V/2√(vv + VV)}, atque erit ipſe niſus tunc = {1/2}√(vv + VV)
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- {1/2} V, ſi per v intelligatur preſſio directa, quam vena exerit in planum cui
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perpendiculariter occurrit.</
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