Archimedes, Natation of bodies, 1662

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1that of the firſt Pyramid is preſſed by the Solid R, and by the Liquid
which that containeth, that is, that which is in the place of the Py­
ramid according to A B O X: but that part which, in the other Py­
ramid, is preſſed by the Solid H, ſuppoſed to be of the ſame Li­
quid, and by the Liquid which that containeth, that is, that which
is in the place of the ſaid Pyramid according to P O B G: and the
Gravity of the Solid R is leſs than the Gravity of the Liquid
H, for that theſe two Magnitudes were ſuppoſed to be equal in
Maſs, and the Solid R was ſuppoſed to be lighter than the Liquid:
and the Maſſes of the two Pyramids of Liquor that containeth theſe

two Solids R and H are equal ^{*} by what was preſuppoſed: There­
fore the part of the Liquid that is under the Superficies that pro­
ceeds according to the Circumference O P is more preſſed; and,
therefore, by the Suppoſition, it ſhall repulſe that part which is leſs
preſſed, whereby the ſaid Liquid will not be ſetled: But it was be­
fore ſuppoſed that it was ſetled: Therefore that Solid R ſhall not
totally ſubmerge, but ſome part thereof will remain without the
Liquid, that is, above its Surface, Which was the Propoſition.
* That is a Maſs of
the Liquid.
* For that the Py­
ramids were ſuppo­
ſed equal.
RIC. I have very well underſtood you, therefore let us come to the fifth Pro­
poſition, which, as you know, doth thus ſpeak.
PROP. V. THEOR. V.
Solid Magnitudes that are lighter than the Liquid,
being demitted in the (ſetled) Liquid, will ſo far
ſubmerge, till that a Maſs of Liquor, equal to the
Part ſubmerged, doth in Gravity equalize the
whole Magnitude.
NIC. It having, in the precedent, been demonſtrared that Solids lighter than
the Liquid, being demitted in the Liquid, alwaies a part of them remains
without the Liquid, that is above its Surface; In this fifth Propoſition it is
aſſerted, that ſo much of ſuch a Solid ſhall ſubmerge, as that a Maſs of the
Liquid equal to the part ſubmerged, ſhall have equal Gravity with the whole
Solid.
And to demonſtrate this, let us aſſume all the ſame Schemes
as before, in Propoſition 3. and likewiſe let the Liquid be ſet­
led, and let the Solid E Z H T be lighter than the Liquid.
Now if the ſaid Liquid be ſetled, the parts of it that are equija­
cent are equally preſſed: Therefore the Liquid that is beneath

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