Galilei, Galileo
,
Discourse concerning the natation of bodies
,
1663
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the
Gravity
of
the
water
,
yet
the
caſe
ſtands
ſo
,
that
the
Rampart
doth
alſo
contract
it
ſelf
,
and
the
Cylinder
contained
in
it
doth
de
miniſh.
Nevertheleſs
it
ſhall
be
demonſtrated
,
how
that
the
Cone
A
B
D
being
of
any
ſuppoſed
bigneſſe,
and
made
at
the
firſt
of
a
Matter
exactly
equall
in
Gravity
to
the
Water
,
if
there
may
be
affixed
to
it
ſome
Weight
,
by
means
of
which
it
may
deſcend
to
the
bottom
,
when
ſubmerged
under
water
,
it
may
alſo
by
vertue
of
the
Rampart
ſtay
above
without
ſinking
.
Let
,
therefore
,
the
Cone
A
B
D
be
of
any
ſuppoſed
greatneſſe,
and
alike
in
ſpecificall
Gravity
to
the
water
.
It
is
manifeſt
,
that
being
put
lightly
into
the
water
,
it
ſhall
reſt
without
deſcending
;
and
it
ſhall
advance
above
water
,
the
Point
[Figure 18]
AS
T
, tripple
in
height
to
the
height
of
the
Rampart
E
S
:
Now
,
ſuppoſe
the
Cone
A
B
D
more
depreſſed
,
ſo
that
it
advance
above
wa
ter,
only
the
Point
A
I
R
,
higher
by
half
than
the
Point
A
S
T
,
with
the
Rampart
about
it
C
I
R
N
.
And
,
becauſe
,
the
Cone
A
B
D
is
to
the
Cone
A
I
R
,
as
the
cube
of
the
Line
S
T
is
to
the
cube
of
the
Line
I
R
,
but
the
Cylin
der
E
S
T
O
,
is
to
the
Cylinder
C
I
R
N
,
as
the
Square
of
S
T
to
the
Square
of
I
R
,
the
Cone
A
S
T
ſhall
be
Octuple
to
the
Cone
A
I
R
,
and
the
Cylinder
E
S
T
O
,
quadruple
to
the
Cylinder
C
I
R
N
:
But
the
Cone
A
S
T
,
is
equall
to
the
Cylinder
E
S
T
O
:
Therefore
,
the
Cylinder
C
I
R
N
,
ſhall
be
double
to
the
Cone
A
I
R
:
and
the
water
which
might
be
contained
in
the
Rampart
C
I
R
N
,
would
be
double
in
Maſs
and
in
Weight
to
the
Cone
A
I
R
,
and
,
therefore
,
would
be
able
to
ſuſtain
the
double
of
the
Weight
of
the
Cone
AIR
:
Therefore
,
if
to
the
whole
Cone
A
B
D
,
there
be
added
as
much
Weight
as
the
Gravity
of
the
Cone
A
I
R
,
that
is
to
ſay
,
the
eighth
part
of
the
weight
of
the
Cone
A
S
T
,
it
alſo
ſhall
be
ſuſtained
by
the
Rampart
C
I
R
N
,
but
without
that
it
ſhall
go
to
the
bottome:
the
Cone
A
B
D
,
being
,
by
the
addition
of
the
eighth
part
of
the
weight
of
the
Cone
A
S
T
,
made
ſpecifically
more
grave
than
the
water
.
But
if
the
Altitude
of
the
Cone
A
I
R
,
were
two
thirds
of
the
Altitude
of
the
Cone
A
S
T
,
the
Cone
A
S
T
would
be
to
the
Cone
A
I
R
,
as
twenty
ſeven
to
eight
;
and
the
Cylinder
E
S
T
O
,
to
the
Cylinder
C
I
R
N
,
as
nine
to
four
,
that
is
,
as
twenty
ſeven
to
twelve
;
and
,
therefore
,
the
Cylinder
C
I
R
N
,
to
the
Cone
A
I
R
,
as
twelve
to
eight
;
and
the
exceſs
of
the
Cylinder
C
I
R
N
,
above
the
Cone
A
I
R
,
to
the
Cone
A
S
T
,
as
four
to
twenty
ſeven
: there
fore
if
to
the
Cone
A
B
D
be
added
ſo
much
weight
as
is
the
four
twenty
ſevenths
of
the
weight
of
the
Cone
A
S
T
,
which
is
a
little
more
then
its
ſeventh
part
,
it
alſo
ſhall
continue
to
ſwimme,
and
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