Galilei, Galileo
,
Discourse concerning the natation of bodies
,
1663
Text
Text Image
XML
Document information
None
Concordance
Figures
Thumbnails
List of thumbnails
<
1 - 10
11 - 20
21 - 30
31 - 40
41 - 50
51 - 60
61 - 70
71 - 77
>
11
12
13
14
15
16
17
18
19
20
<
1 - 10
11 - 20
21 - 30
31 - 40
41 - 50
51 - 60
61 - 70
71 - 77
>
page
|<
<
of 77
>
>|
<
archimedes
>
<
text
>
<
body
>
<
chap
>
<
p
type
="
main
">
<
s
>
<
pb
pagenum
="
410
"/>
<
figure
id
="
fig262
"
number
="
1
"/>
<
lb
/>
<
emph
type
="
italics
"/>
Maſſe of the Solid depreſſed, namely of
<
lb
/>
H I K, being equall to the only part E I K,
<
lb
/>
which is contained under the firſt Levell
<
lb
/>
E F G. </
s
>
<
s
>Which is manifeſt, becauſe if
<
lb
/>
the Solid H I K be taken out, the Water
<
lb
/>
I G ſhall return into the place occupied by
<
lb
/>
the Maſs E I K, where it was continuate
<
lb
/>
fore the ſubmerſion of the Priſme. </
s
>
<
s
>And
<
lb
/>
the Maſs L G being equall to the Maſs
<
lb
/>
E K: adde thereto the Maſs E N, and it
<
lb
/>
ſhall be the whole Maſs E M, compoſed of the parts of the Priſme E N,
<
lb
/>
and of the Water N F, equall to the whole Solid H I K: And,
<
lb
/>
fore, the Maſs L G ſhall have the ſame proportion to E M, as to the
<
lb
/>
Maſs H I K: But the Maſs L G hath the ſame proportion to the Maſs
<
lb
/>
E M, as the Surface L M hath to the Surface M H: Therefore it is
<
lb
/>
nifeſt, that the Maſs of Water repulſed L G, is in proportion to the Maſs
<
lb
/>
of the Solid ſubmerged H I K; as the Surface L M, namely, that of the
<
lb
/>
Water ambient about the Sollid, to the whole Surface H M, compounded
<
lb
/>
of the ſaid ambient water, and the Baſe of the Priſme H N. </
s
>
<
s
>But if we
<
lb
/>
ſuppoſe the firſt Levell of the Water the according to the Surface H M,
<
lb
/>
and the Priſme allready ſubmerged H I K; and after to be taken out and
<
lb
/>
raiſed to E A O, and the Water to be faln from the firſt Levell H L M as
<
lb
/>
low as E F G; It is manifeſt, that the Priſme E A O being the ſame with
<
lb
/>
H I K, its ſuperiour part H O, ſhall be equall to the inferiour E I K:
<
lb
/>
and remove the common part E N, and, conſequently, the Maſs of the
<
lb
/>
Water L G is equall to the Maſs H O; and, therefore, leſs than the
<
lb
/>
Solid, which is without the Water, namely, the whole Priſme E A O, to
<
lb
/>
which likewiſe, the ſaid Maſs of Water abated L G, hath the ſame
<
lb
/>
tion, that the Surface of the Waters circumfuſed L M hath to the ſame
<
lb
/>
circumfuſed Surface, together with the Baſe of the Priſme A O: which
<
lb
/>
hath the ſame demonſtration with the former caſe above.
<
emph.end
type
="
italics
"/>
</
s
>
</
p
>
<
p
type
="
main
">
<
s
>
<
emph
type
="
italics
"/>
And from hence is inferred, that the Maſs of the Water, that riſeth in
<
lb
/>
the immerſion of the Solid, or that ebbeth in elevating it, is not equall to
<
lb
/>
all the Maſs of the Solid, which is ſubmerged or elevated, but to that
<
lb
/>
part only, which in the immerſion is under the firſt Levell of the Water,
<
lb
/>
and in the elevation remaines above the firſt Levell: Which is that
<
lb
/>
which was to be demonſtrated. </
s
>
<
s
>We will now purſue the things that
<
lb
/>
remain.
<
emph.end
type
="
italics
"/>
</
s
>
</
p
>
<
p
type
="
main
">
<
s
>And firſt we will demonſtrate that,</
s
>
</
p
>
</
chap
>
</
body
>
</
text
>
</
archimedes
>