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
Table of Notes
<
1 - 3
[out of range]
>
<
1 - 3
[out of range]
>
page
|<
<
(215)
of 361
>
>|
<
echo
version
="
1.0RC
">
<
text
xml:lang
="
la
"
type
="
free
">
<
div
xml:id
="
echoid-div234
"
type
="
section
"
level
="
1
"
n
="
184
">
<
p
>
<
s
xml:id
="
echoid-s6304
"
xml:space
="
preserve
">
<
pb
o
="
215
"
file
="
0229
"
n
="
229
"
rhead
="
SECTIO DECIMA.
"/>
hujus autem æquationis normam, ſi ponatur pro ſecunda obſervatione
<
lb
/>
x = 1542, invenitur E = 0, 9317, ipſa autem obſervatio indicat E = 0,
<
lb
/>
9364: </
s
>
<
s
xml:id
="
echoid-s6305
"
xml:space
="
preserve
">differentia inter hypotheſin & </
s
>
<
s
xml:id
="
echoid-s6306
"
xml:space
="
preserve
">obſervationem eſt plus quam ſeſquilineæ,
<
lb
/>
quæ ſane notabilis eſt reſpectu habito ad differentiam parvam altitudinum ver-
<
lb
/>
ticalium.</
s
>
<
s
xml:id
="
echoid-s6307
"
xml:space
="
preserve
"/>
</
p
>
<
p
>
<
s
xml:id
="
echoid-s6308
"
xml:space
="
preserve
">Si jam porro pro tèrtia obſervatione ponatur x = 13158, fit ex hypo-
<
lb
/>
theſi E = 0, 5469, dum experimentum indicavit E = 0, 6257: </
s
>
<
s
xml:id
="
echoid-s6309
"
xml:space
="
preserve
">quæ diffe-
<
lb
/>
rentia nimia eſt, quam ut ullo modo logarithmica ſervari poſſit: </
s
>
<
s
xml:id
="
echoid-s6310
"
xml:space
="
preserve
">valet enim
<
lb
/>
hæc differentia plus quam duos pollices cum duabus lineis.</
s
>
<
s
xml:id
="
echoid-s6311
"
xml:space
="
preserve
"/>
</
p
>
<
p
>
<
s
xml:id
="
echoid-s6312
"
xml:space
="
preserve
">§. </
s
>
<
s
xml:id
="
echoid-s6313
"
xml:space
="
preserve
">25. </
s
>
<
s
xml:id
="
echoid-s6314
"
xml:space
="
preserve
">Rejecta logarithmica conſequens eſt elaſticitates in diverſis at-
<
lb
/>
moſphæræ altitudinibus nequaquam eſſe denſitatibus proportionales, aut quod
<
lb
/>
eodem recidit, diverſum eſſe in diverſis altitudinibus medium caloris gradum.
<
lb
/>
</
s
>
<
s
xml:id
="
echoid-s6315
"
xml:space
="
preserve
">Aliæ igitur ab aliis, quibus defectus iſte probe fuit notatus, fuerunt excogita-
<
lb
/>
tæ regulæ: </
s
>
<
s
xml:id
="
echoid-s6316
"
xml:space
="
preserve
">earum tamen nulla ad experimentum III. </
s
>
<
s
xml:id
="
echoid-s6317
"
xml:space
="
preserve
">(§. </
s
>
<
s
xml:id
="
echoid-s6318
"
xml:space
="
preserve
">23.) </
s
>
<
s
xml:id
="
echoid-s6319
"
xml:space
="
preserve
">ſatis accommo-
<
lb
/>
data dici poteſt. </
s
>
<
s
xml:id
="
echoid-s6320
"
xml:space
="
preserve
">Veram, quam natura ſequatur, legem invenire, rem eſſe pu-
<
lb
/>
to vix ſperandam: </
s
>
<
s
xml:id
="
echoid-s6321
"
xml:space
="
preserve
">quis enim aliter quam levibus conjecturis aſſequetur@ ra-
<
lb
/>
tionem velocitatum mediarum in particulis aëreis: </
s
>
<
s
xml:id
="
echoid-s6322
"
xml:space
="
preserve
">Incidi tamen forte in ali-
<
lb
/>
quam hypotheſin, quæ phænomenis non male reſpondet: </
s
>
<
s
xml:id
="
echoid-s6323
"
xml:space
="
preserve
">prius autem pro
<
lb
/>
quacunque velocitatum lege curvam dabo, quam ad ſpecialem iſtam hypothe-
<
lb
/>
ſin deſcendam.</
s
>
<
s
xml:id
="
echoid-s6324
"
xml:space
="
preserve
"/>
</
p
>
<
p
>
<
s
xml:id
="
echoid-s6325
"
xml:space
="
preserve
">§. </
s
>
<
s
xml:id
="
echoid-s6326
"
xml:space
="
preserve
">26. </
s
>
<
s
xml:id
="
echoid-s6327
"
xml:space
="
preserve
">Sit linea verticalis A D (Fig. </
s
>
<
s
xml:id
="
echoid-s6328
"
xml:space
="
preserve
">59,); </
s
>
<
s
xml:id
="
echoid-s6329
"
xml:space
="
preserve
">Q F horizontalis radat ſu-
<
lb
/>
<
note
position
="
right
"
xlink:label
="
note-0229-01
"
xlink:href
="
note-0229-01a
"
xml:space
="
preserve
">Fig. 59.</
note
>
perficiem maris: </
s
>
<
s
xml:id
="
echoid-s6330
"
xml:space
="
preserve
">Denotet B F velocitatem mediam particularum aërearum in
<
lb
/>
ſuperficie maris: </
s
>
<
s
xml:id
="
echoid-s6331
"
xml:space
="
preserve
">B M denſitatem mediam & </
s
>
<
s
xml:id
="
echoid-s6332
"
xml:space
="
preserve
">B Q elaſticitatem, quæ in omni
<
lb
/>
loco æque alto eadem eſt. </
s
>
<
s
xml:id
="
echoid-s6333
"
xml:space
="
preserve
">Deinde per puncta F, M, Q ductæ concipiantur
<
lb
/>
curvæ E F H, L M O, P Q S ceu ſcalæ, quæ in omnibus altitudinibus, veluti
<
lb
/>
B C, applicatis C G, C N, C R denotent velocitates medias particularum aë-
<
lb
/>
rearum, denſitates medias & </
s
>
<
s
xml:id
="
echoid-s6334
"
xml:space
="
preserve
">elaſticitates medias. </
s
>
<
s
xml:id
="
echoid-s6335
"
xml:space
="
preserve
">Datis nunc duabus curvis ter-
<
lb
/>
tiam licet determinare ex eo, quod elaſticitates (ceu experientia docuit & </
s
>
<
s
xml:id
="
echoid-s6336
"
xml:space
="
preserve
">
<
lb
/>
§. </
s
>
<
s
xml:id
="
echoid-s6337
"
xml:space
="
preserve
">§. </
s
>
<
s
xml:id
="
echoid-s6338
"
xml:space
="
preserve
">3. </
s
>
<
s
xml:id
="
echoid-s6339
"
xml:space
="
preserve
">4 5. </
s
>
<
s
xml:id
="
echoid-s6340
"
xml:space
="
preserve
">& </
s
>
<
s
xml:id
="
echoid-s6341
"
xml:space
="
preserve
">6. </
s
>
<
s
xml:id
="
echoid-s6342
"
xml:space
="
preserve
">explicatum fuit) ſint proxime in ratione compoſita ex qua-
<
lb
/>
drato velocitatum modo dictarum & </
s
>
<
s
xml:id
="
echoid-s6343
"
xml:space
="
preserve
">ſimplici denſitatum.</
s
>
<
s
xml:id
="
echoid-s6344
"
xml:space
="
preserve
"/>
</
p
>
<
p
>
<
s
xml:id
="
echoid-s6345
"
xml:space
="
preserve
">Ipſe quidem monui prædicto loco hanc proportionem non poſſe exa-
<
lb
/>
cte eſſe veram, quia aër quidem elaterem poteſt habere infinitum ſeu vi in-
<
lb
/>
finita comprimi, non poteſt autem in ſpatium plane infinite parvum </
s
>
</
p
>
</
div
>
</
text
>
</
echo
>