Geometrical Solutions Derived from Mechanics; a Treatise of ArchimedesArchimedes
History
Geometrical Solutions Derived from Mechanics; a Treatise of Archimedes
Archimedes
Geometry -- Early works to 1800
From the points $\alpha$ and $\gamma$ draw $\alpha\zeta \|
\delta\beta\epsilon$, and the tangent $\gamma\zeta$; produce
[$\gamma\beta$ to $\kappa$, and make $\kappa\theta = \gamma\kappa$].
Think of $\gamma\theta$ as a scale-beam with the center at $\kappa$
and let $\mu\xi$ be any straight line whatever $\|
\epsilon\delta$. Now since $\gamma\beta\alpha$ is a parabola,
$\gamma\zeta$ a tangent and $\gamma\delta$ an ordinate, then
$\epsilon\beta = \beta\delta$; for this indeed has been proved in the
Elements [i.e., of conic sections, cf. \emph{Quadr. parab.} 2]. For
this reason and because $\zeta\alpha$ and $\mu\xi \| \epsilon\delta$,
$\mu\nu = \nu\xi$, and $\zeta\kappa = \kappa\alpha$. And because
$\gamma\alpha : \alpha\xi = \mu\xi : \xi o$ (for this is shown in a
corollary, [cf. \emph{Quadr. parab.} 5]), $\gamma\alpha : \alpha\xi =
\gamma\kappa : \kappa\nu$; and $\gamma\kappa = \kappa\theta$,
therefore $\theta\kappa : \kappa\nu = \mu\xi : \xi o$. And because
$\nu$ is the center of gravity of the straight line $\mu\xi$, since
$\mu\nu = \nu\xi$, then if we make $\tau\eta = \xi o$ and $\theta$ as
its center of gravity so that $\tau\theta = \theta\eta$, the straight
line $\tau\theta\eta$ will be in equilibrium with $\mu\xi$ in its
present position because $\theta\nu$ is divided in inverse proportion
to the weights $\tau\eta$ and $\mu\xi$, and $\theta\kappa : \kappa\nu
= \mu\xi : \eta\tau$; therefore $\kappa$ is the center of gravity of
the combined weight of the two. In the
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{\small Fig.~1.}
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same way all straight lines drawn in the triangle $\zeta\alpha\gamma
\| \epsilon\delta$ are in their present positions in equilibrium with
their parts cut off by the parabola, when these are transferred to
$\theta$, so that $\kappa$ is the center of gravity of the combined
weight of the two. And because the triangle $\gamma\zeta\alpha$
consists of the straight lines in the triangle $\gamma\zeta\alpha$ and
the segment $\alpha\beta\gamma$ consists of those straight lines
within the segment of the parabola corresponding to the straight line
$\xi o$, therefore the triangle $\zeta\alpha\gamma$ in its present
position will be in equilibrium at the point $\kappa$ with the
parabola-segment when this is transferred to $\theta$ as its center of
gravity, so that $\kappa$ is the center of gravity of the combined
weights of the two. Now let $\gamma\kappa$ be so divided at $\chi$
that $\gamma\kappa = 3\kappa\chi$; then $\chi$ will be the center of
gravity of the triangle $\alpha\zeta\gamma$, for this has been shown
in the Statics [cf. \emph{De plan. aequil.} I, 15, p. 186, 3 with
Eutokios, S. 320, 5ff.]. Now the triangle $\zeta\alpha\gamma$ in its
present position is in equilibrium at the point $\kappa$ with the
segment $\beta\alpha\gamma$ when this is transferred to $\theta$ as
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