Bernoulli, Daniel
,
Hydrodynamica, sive De viribus et motibus fluidorum commentarii
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234
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248
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HYDRODYNAMICÆ
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<
s
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echoid-s6899
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xml:space
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">An vero iſta vis viva aëri inhæreat proprie externo an interno, logoma@
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chia eſt; </
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<
s
xml:id
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echoid-s6900
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xml:space
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">ſufficit quod à ſublato æquilibrio inter utrumque aërem talis vis viva
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obtineri poteſt, dum reſtitutio permittitur.</
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<
s
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<
s
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echoid-s6904
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xml:space
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">pes cubicus aëris naturali duplo rarioris, cui hypotheſi
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quadrabunt poſitiones p = 2240 lib. </
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<
s
xml:id
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echoid-s6905
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xml:space
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">a = {1/2} ped. </
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<
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xml:space
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">& </
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<
s
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echoid-s6907
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xml:space
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">x = {1/2} ped. </
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<
s
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echoid-s6908
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xml:space
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">& </
s
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<
s
xml:id
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echoid-s6909
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xml:space
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">erit vis viva, de
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qua ſermo eſt, = 1120 - 1120 log. </
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<
s
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echoid-s6910
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xml:space
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">2 = 344, id eſt, ea quæ generatur lapſu li-
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bero 344 lib. </
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<
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">ab altitudine unius pedis.</
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</
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<
s
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">Si pes cubicus ſit aëre repletus, qui naturali ſit quadruplo rarior, erit
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jam vis viva quæſita (poſito nempe p = 2240, & </
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<
s
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xml:space
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">a = {1/4}, x = {3/4}) = 1680 -
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560. </
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<
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<
s
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">4 = 904, ſeu talis quæ oritur lapſu libero ponderis 904 lib. </
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<
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</
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<
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">unius pedis.</
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</
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<
s
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">Si denique habeatur pes cubicus ab aëre omnino vacuus, ponendum
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eſt p = 2240; </
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<
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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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">atque ſic erit vis viva quæſita = 2240 X
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(1 - 0 log. </
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<
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xml:space
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">{1/0}) conſtat autem eſſe 0 log. </
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">{1/0} infinite parvum præ unitate; </
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<
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">eſt igitur
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numerus iſte = 2240, qui indicat poſſe hac vi viva 2240 libras ad altitudinem
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unius pedis elevari.</
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<
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">46. </
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">Pertinet ad præſens argumentum ſtupenda vis aëris admodum
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condenſati, ſed præſertim auræ pulveris pyrii accenſi in uſu ſclopetorum pneu-
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maticorum & </
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">tormentorum bellicorum. </
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xml:space
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">De his quæ ſeorſim commentatus ſum
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huic ſectioni adjiciam.</
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">De vi aëris condenſati & auræ pulveris pyrii ac-
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cenſi ad globos projiciendos in uſu ſclopetorum
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pneumaticorum & tormentorum bellicorum.</
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<
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<
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note
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zontaliter poſito, voceturque = a: </
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<
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">denotet A C longitudinem ſpatii, quod
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aër condenſatus ſeu aura pulveris pyrii accenſi occupat ab initio exploſionis,
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ſitque A C = b: </
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<
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<
s
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">ponimus autem, globum ca-
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vitatem animæ exacte replere & </
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<
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">liberrime in illa moveri: </
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denſati in ſpatio A D ſe habeat ad denſitatem aëris naturalis ut n ad 1: </
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