Galilei, Galileo
,
Discourse concerning the natation of bodies
,
1663
Text
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
>
>|
though
the
Concluſions
are
true
,
yet
are
the
Cauſes
thus
aſſigned
deficient
,
nor
is
it
true
,
that
the
Solid
in
ſubmerging
, raiſeth
and
repulſeth
Maſſes
of
Water
, equall
to
the
parts
of
it
ſelf
ſubmerged
;
but
the
Water
repulſed
,
is
alwayes
leſs
than
the
parts
of
the
Solid
ſubmerged
:
and
ſo
much
the
more
by
how
much
the
Veſſell
in
which
the
Water
is
contained
is
narrower
:
in
ſuch
manner
that
it
hinders
not
,
but
that
a
Solid
may
ſubmerge
all
under
Water
, with
out
raiſing
ſo
much
Water
in
Maſs
,
as
would
equall
the
tenth
or
twentieth
part
of
its
own
Bulk
:
like
as
on
the
contrary
,
a
very
ſmall
quantity
of
Water
,
may
raiſe
a
very
great
Solid
Maſs
,
though
ſuch
Solid
ſhould
weigh
abſolutely
a
hundred
times
as
much
,
or
more
,
than
the
ſaid
Water
,
if
ſo
be
that
the
Matter
of
that
ſame
Solid
be
in
ſpecie
leſs
grave
than
the
Water
.
And
thus
a
great
Beam
,
as
ſuppoſe
of
a
1000
weight
,
may
be
raiſed
and
born
afloat
by
Water
,
which
weighs
not
50:
and
this
happens
when
the
Mo
ment
of
the
Water
is
compenſated
by
the
Velocity
of
its
Motion
.
How
the
ſub
merſion
of
So
lids
in
the
Wa
ter,
is
effected
.
What
Solids
ſhall
float
on
the
Water
.
What
Solids
ſhall
ſinke
to
the
botome.
What
Solids
ſhall
reſt
in
all
places
of
the
Wa
ter.
The
Gravitie
of
the
Water
and
S
olid
muſt
be
compared
in
all
Problems
,
of
Na
tation
of
Bodies
.
The
water
re
pulſed
is
ever
leſs
than
the
parts
of
the
Sollid ſub
merged.
A
ſmall
quantity
of
water
,
may
float
a
very
great
Solid
Maſs
.
But
becauſe
ſuch
things
,
propounded
thus
in
abſtract
,
are
ſome
what
difficult
to
be
comprehended
,
it
would
be
good
to
demonſtrate
them
by
particular
examples
;
and
for
facility
of
demonſtration
,
we
will
ſuppoſe
the
Veſſels
in
which
we
are
to
put
the
Water
,
and
place
the
Solids
,
to
be
inviron'
d
and
included
with
ſides
erected
perpendi
cular
to
the
Plane
of
the
Horizon
,
and
the
Solid
that
is
to
be
put
into
ſuch
veſſell
to
be
either
a
ſtreight
Cylinder
,
or
elſe
an
upright
Priſme
The
which
propoſed
and
declared
,
I
proceed
to
demonstrate
the
truth
of
what
hath
been
hinted
,
forming
the
enſuing
Theoreme.
THEOREME
I
.
The
Maſs
of
the
Water
whichaſcends
in
the
ſub
merging
of
a
Solid
, Priſme
or
Cylinder
,
or
that
abaſeth
in
taking
it
out
,
is
leſs
than
the
Maſs
of
the
ſaid
Solid
,
ſo
depreſſed
or
advanced
:
and
hath
to
it
the
ſame
proportion
,
that
the
Surface
of
the
Water
circumfuſing
the
Solid
,
hath
to
the
ſame
circumfuſed
Surface
,
together
with
the
Baſe
of
the
Solid
.
T
he
Proportion
of
the
water
rai
ſed
to
the
S
olid
ſubmerged
.
Let
the
Veſſell
be
A
B
C
D
,
and
in
it
the
Water
raiſed
up
to
the
Levell
E
F
G
,
before
the
Solid
Priſme
H
I
K
be
therein
immerged
;
but
after
that
it
is
depreſſed
under
Water
,
let
the
Water
be
raiſed
as
high
as
the
Levell
L
M
,
the
Solid
H
I
K
ſhall
then
be
all
under
Water
,
and
the
Maſs
of
the
elevated
Water
ſhall
be
L
G
,
which
is
leſs
than
the
Text layer
Dictionary
Text normalization
Original
Regularized
Normalized
Search
Exact
All forms
Fulltext index
Morphological index