Bernoulli, Daniel
,
Hydrodynamica, sive De viribus et motibus fluidorum commentarii
Text
Text Image
Image
XML
Thumbnail overview
Document information
None
Concordance
Notes
Handwritten
Figures
Content
Thumbnails
page
|<
<
(51)
of 361
>
>|
<
echo
version
="
1.0RC
">
<
text
xml:lang
="
la
"
type
="
free
">
<
div
xml:id
="
echoid-div65
"
type
="
section
"
level
="
1
"
n
="
46
">
<
p
>
<
s
xml:id
="
echoid-s1311
"
xml:space
="
preserve
">
<
pb
o
="
51
"
file
="
0065
"
n
="
65
"
rhead
="
SECTIO TERTIA.
"/>
tum acquirit, qui in expellendas aquas ſolus impenditur, hocque pacto
<
lb
/>
enormem jactum producit. </
s
>
<
s
xml:id
="
echoid-s1312
"
xml:space
="
preserve
">Hanc phænomeni cauſam mox clarius una cum
<
lb
/>
debitis menſuris explicabo, poſtquam præmiſero verba, quæ hâc de re ex-
<
lb
/>
tant, in hiſtor. </
s
>
<
s
xml:id
="
echoid-s1313
"
xml:space
="
preserve
">Acad. </
s
>
<
s
xml:id
="
echoid-s1314
"
xml:space
="
preserve
">Reg. </
s
>
<
s
xml:id
="
echoid-s1315
"
xml:space
="
preserve
">ſc. </
s
>
<
s
xml:id
="
echoid-s1316
"
xml:space
="
preserve
">Paris. </
s
>
<
s
xml:id
="
echoid-s1317
"
xml:space
="
preserve
">ad An. </
s
>
<
s
xml:id
="
echoid-s1318
"
xml:space
="
preserve
">1702. </
s
>
<
s
xml:id
="
echoid-s1319
"
xml:space
="
preserve
">On voit quelques fois, dici-
<
lb
/>
tur in loco citato, l’eau qui ſort par un ajutage ſaillir trois ou quatre fois
<
lb
/>
plus haut que ne lui permét la hauteur du réſervoir, ausſi ſe rémet - elle bien
<
lb
/>
vite à la hauteur, que lui preſcrivent les loix de l’hydroſtatique. </
s
>
<
s
xml:id
="
echoid-s1320
"
xml:space
="
preserve
">Mais com-
<
lb
/>
ment a-t-elle pu en ſortir en un inſtant. </
s
>
<
s
xml:id
="
echoid-s1321
"
xml:space
="
preserve
">Mſr. </
s
>
<
s
xml:id
="
echoid-s1322
"
xml:space
="
preserve
">De la Hire l’attribue a de
<
lb
/>
l’air enfermè dans la conduite, qui aγant été preſſé & </
s
>
<
s
xml:id
="
echoid-s1323
"
xml:space
="
preserve
">mis en reſſort par
<
lb
/>
l’eau, qui deſcendoit toujours, s’eſt debandé contre celle qui montoit & </
s
>
<
s
xml:id
="
echoid-s1324
"
xml:space
="
preserve
">lui
<
lb
/>
a donné cette viteſſe momentanée.</
s
>
<
s
xml:id
="
echoid-s1325
"
xml:space
="
preserve
"/>
</
p
>
<
p
>
<
s
xml:id
="
echoid-s1326
"
xml:space
="
preserve
">Recte itaque animadvertit Dn. </
s
>
<
s
xml:id
="
echoid-s1327
"
xml:space
="
preserve
">De la Hire aëri ſaltum deberi, dubium-
<
lb
/>
que nullum eſt quin veram rationem, quâ aër id producere poſſit, fuiſſet
<
lb
/>
eruturus, ſi phænomenon, quod obiter attigit, attentius conſideraſſet, fa-
<
lb
/>
cile utique perſperſpecturus, aërem inter medias aquas nullam ſuſtinere preſſio-
<
lb
/>
nem, niſi ſuper incumbentis aquæ (imo ne hanc quidem in aquis fluentibus,
<
lb
/>
uti inferius in ſect. </
s
>
<
s
xml:id
="
echoid-s1328
"
xml:space
="
preserve
">XII. </
s
>
<
s
xml:id
="
echoid-s1329
"
xml:space
="
preserve
">demonſtrabo) nec adeoque aërem compreſſum for-
<
lb
/>
tius expellere poſſe aquam ſibi præcedentem, quam ſi ſui loco aqua eſſet. </
s
>
<
s
xml:id
="
echoid-s1330
"
xml:space
="
preserve
">Ego
<
lb
/>
quidem prævidi (quod facillimo experimento ſæpe poſtea ſum expertus) non
<
lb
/>
eſſe aquam ante aërem poſitam ſolito altius aſſurgentem, ſed illam, quæ aërem
<
lb
/>
ſequitur, quod nunc clarius faciam.</
s
>
<
s
xml:id
="
echoid-s1331
"
xml:space
="
preserve
"/>
</
p
>
<
p
>
<
s
xml:id
="
echoid-s1332
"
xml:space
="
preserve
">Sit igitur in Figura vigeſima aquæ ductus C A D B cylindricus, ut eſſe
<
lb
/>
ſolet, isque totus aquâ plenus, præter particulam m n B aëre plenam. </
s
>
<
s
xml:id
="
echoid-s1333
"
xml:space
="
preserve
">Du-
<
lb
/>
cantur lineæ horrizontalis & </
s
>
<
s
xml:id
="
echoid-s1334
"
xml:space
="
preserve
">verticalis C H & </
s
>
<
s
xml:id
="
echoid-s1335
"
xml:space
="
preserve
">H B: </
s
>
<
s
xml:id
="
echoid-s1336
"
xml:space
="
preserve
">ponamus brevitatis ergo
<
lb
/>
aëris gravitatem præ gravitate aquæ nullam cenſeri poſſe, ita ut tranſitus aëris
<
lb
/>
per orificium B nihil reſiſtat fluxui aquæ, quamvis de cætero facile foret in-
<
lb
/>
ertiæ aëris rationem habere, niſi calculi prolixitatem evitare vellemus in re,
<
lb
/>
ubi nullam quærimus præciſionem. </
s
>
<
s
xml:id
="
echoid-s1337
"
xml:space
="
preserve
">Sit longitudo canalis C A D f vel C A D m
<
lb
/>
(ponimus enim differentiolam mf aëre repletam valde parvam) = β mf vel
<
lb
/>
ng = δ: </
s
>
<
s
xml:id
="
echoid-s1338
"
xml:space
="
preserve
">H B = a; </
s
>
<
s
xml:id
="
echoid-s1339
"
xml:space
="
preserve
">amplitudo tubi = m, amplitudo orificii B = n; </
s
>
<
s
xml:id
="
echoid-s1340
"
xml:space
="
preserve
">Denique
<
lb
/>
demus aquæ, cum ſuperficies eſt in mn, nullum eſſe motum, quæſituri </
s
>
</
p
>
</
div
>
</
text
>
</
echo
>