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
|<
<
(294)
of 361
>
>|
<
echo
version
="
1.0RC
">
<
text
xml:lang
="
la
"
type
="
free
">
<
div
xml:id
="
echoid-div292
"
type
="
section
"
level
="
1
"
n
="
221
">
<
p
>
<
s
xml:id
="
echoid-s8762
"
xml:space
="
preserve
">
<
pb
o
="
294
"
file
="
0308
"
n
="
308
"
rhead
="
HYDRODYNAMICÆ
"/>
titudinis aquarum in vaſe ſupra foramen poſitarum: </
s
>
<
s
xml:id
="
echoid-s8763
"
xml:space
="
preserve
">fuerit enim quantitas
<
lb
/>
aquarum dato tempore effluentium = Q; </
s
>
<
s
xml:id
="
echoid-s8764
"
xml:space
="
preserve
">altitudo earum = A, erit ma-
<
lb
/>
gnitudo foraminis aquas eructantis proportionalis cenſenda quantitati {Q/√ A}
<
lb
/>
pro eodem tempore: </
s
>
<
s
xml:id
="
echoid-s8765
"
xml:space
="
preserve
">at vero vis repellens, quæ hic navem promovet, æqualis
<
lb
/>
eſt magnitudini foraminis ductæ in duplam altitudinem aquarum (per §. </
s
>
<
s
xml:id
="
echoid-s8766
"
xml:space
="
preserve
">4.)
<
lb
/>
</
s
>
<
s
xml:id
="
echoid-s8767
"
xml:space
="
preserve
">id eſt, æqualis quantitati {Q/√ A} X
<
emph
style
="
bf
">2</
emph
>
A ſeu 2 Q √ A. </
s
>
<
s
xml:id
="
echoid-s8768
"
xml:space
="
preserve
">Ex comparatione utrius-
<
lb
/>
que propoſitionis ſequitur laborem hominum in elevandis aquis exantlatum
<
lb
/>
eſſe ad vim naves propellentem inde obtinendam, ut Q A ad 2 Q √ A ſive ut
<
lb
/>
√ A ad quantitatem aliquam conſtantem: </
s
>
<
s
xml:id
="
echoid-s8769
"
xml:space
="
preserve
">igitur quo minor eſt altitudo ad
<
lb
/>
quam aquæ elevantur, eò major vis naves promovens ab eodem labore obti-
<
lb
/>
netur, ita ut labore hominum quantumvis parvo vis naves propellens utcun-
<
lb
/>
que magna obtineri poßit. </
s
>
<
s
xml:id
="
echoid-s8770
"
xml:space
="
preserve
">Verum etiam inertia aquarum, quæ hauriuntur,
<
lb
/>
(de qua ab initio hujus paragraphi diximus) naves retardans eo majorem
<
lb
/>
obtinet rationem ad vim naves propellentem, quo minor aſſumitur altitudo
<
lb
/>
A, ad quod animus hic probe eſt advertendus.</
s
>
<
s
xml:id
="
echoid-s8771
"
xml:space
="
preserve
"/>
</
p
>
<
p
>
<
s
xml:id
="
echoid-s8772
"
xml:space
="
preserve
">§. </
s
>
<
s
xml:id
="
echoid-s8773
"
xml:space
="
preserve
">22. </
s
>
<
s
xml:id
="
echoid-s8774
"
xml:space
="
preserve
">Perſpicuum eſt ex præcedente paragrapho, altitudinem ad quam
<
lb
/>
aquæ ſunt elevandæ eſſe ex earum claſſe, quæ alicubi maximæ ſunt. </
s
>
<
s
xml:id
="
echoid-s8775
"
xml:space
="
preserve
">Ut ve-
<
lb
/>
ro altitudo maxime ad propoſitum proficua determinetur, aliæ nobis ſe of-
<
lb
/>
ferunt quæſtiones prius examinandæ.</
s
>
<
s
xml:id
="
echoid-s8776
"
xml:space
="
preserve
"/>
</
p
>
</
div
>
<
div
xml:id
="
echoid-div298
"
type
="
section
"
level
="
1
"
n
="
222
">
<
head
xml:id
="
echoid-head284
"
xml:space
="
preserve
">Problema.</
head
>
<
p
>
<
s
xml:id
="
echoid-s8777
"
xml:space
="
preserve
">Ponatur navis uniformi progredi velocitate, quæ generatur lapſu li-
<
lb
/>
bero per altitudinem B, fingaturque aquas continue affluere in navem, ve-
<
lb
/>
luti ſub forma pluviarum, & </
s
>
<
s
xml:id
="
echoid-s8778
"
xml:space
="
preserve
">quidem tanta quantitate, quantam remotis om-
<
lb
/>
nibus impedimentis alienis ſuppeditaret cylindrus conſtanter plenus ad alti-
<
lb
/>
tudinem A per orificium magnitudinis M. </
s
>
<
s
xml:id
="
echoid-s8779
"
xml:space
="
preserve
">Quæritur quantam reſiſtentiam
<
lb
/>
navis ab iſto perpetuo & </
s
>
<
s
xml:id
="
echoid-s8780
"
xml:space
="
preserve
">uniformi aquarum affluxu earundemque inertia pa-
<
lb
/>
tiatur.</
s
>
<
s
xml:id
="
echoid-s8781
"
xml:space
="
preserve
"/>
</
p
>
</
div
>
<
div
xml:id
="
echoid-div299
"
type
="
section
"
level
="
1
"
n
="
223
">
<
head
xml:id
="
echoid-head285
"
xml:space
="
preserve
">Solutio.</
head
>
<
p
>
<
s
xml:id
="
echoid-s8782
"
xml:space
="
preserve
">Aſſumatur tempus quodcunque t, quod ſi æſtimetur ex ſpatio, quod
<
lb
/>
fluidum affluens ſua velocitate percurrit, diviſo per eandem velocitatem, </
s
>
</
p
>
</
div
>
</
text
>
</
echo
>