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
$\lambda\epsilon$, and one-half the spheroid is twice as great as the
same cone.
In the parallelogram $\lambda\zeta$ draw the straight lines $\phi\chi$
and $\psi\omega \| \alpha\gamma$ through the points $\beta$ and
$\delta$ and imagine a cylinder whose bases are the circles on the
diameters $\phi\psi$ and $\chi\omega$, and whose axis is
$\alpha\gamma$. Now since the cylinder whose axes form the
parallelogram $\phi\omega$ is twice as great as the cylinder whose
axes form the parallelogram $\phi\delta$ because their bases are equal
but the axis of the first is twice as great as the axis of the second,
and since the cylinder whose axes form the parallelogram $\phi\delta$
is three times as great as the cone whose vertex is at $\alpha$ and
whose base is the circle on the diameter $\beta\delta$ perpendicular
to $\alpha\gamma$, then the cylinder whose axes form the parallelogram
$\phi\omega$ is six times as great as the aforesaid cone. But it has
been shown that the spheroid is four times as great as the same cone,
hence the cylinder is one and one half times as great as the
spheroid. Q. E. D.
\section*{Proposition IV}
That a segment of a right conoid cut by a plane perpendicular to its
axis is one and one half times as great as the cone having the same
base and axis as the segment, can be proved by the same method in the
following way:
Let a right conoid be cut through its axis by a plane intersecting the
surface in a parabola $\alpha\beta\gamma$ [Fig.~4]; let it be also cut
by another plane perpendicular to the axis, and let their common line
of intersection be $\beta\gamma$. Let the axis of the segment be
$\delta\alpha$ and let it be produced to $\theta$ so that
$\theta\alpha = \alpha\delta$. Now imagine $\delta\theta$ to be a
scale-beam with its center at $\alpha$; let the base of the segment be
the circle on the diameter $\beta\gamma$ perpendicular to
$\alpha\delta$; imagine a cone whose base is the circle on the
diameter $\beta\gamma$, and whose vertex is at $\alpha$. Imagine also
a cylinder whose base is the circle on the diameter $\beta\gamma$ and
its axis $\alpha\delta$, and in the parallelogram let a straight line
$\mu\nu$ be drawn $\| \beta\gamma$ and on $\mu\nu$ construct a plane
perpendicular to $\alpha\delta$; it will intersect the cylinder in a
circle whose diameter is $\mu\nu$, and the segment of the right conoid
in a circle whose diameter is $\xi o$. Now since $\beta\alpha\gamma$
is a parabola, $\alpha\delta$ its diameter and $\xi\sigma$ and
$\beta\delta$ its ordinates, then [\emph{Quadr. parab.} 3]
$\delta\alpha : \alpha\sigma = \beta\delta^2 : \xi\sigma^2$. But
$\delta\alpha = \alpha\theta$, therefore $\theta\alpha : \alpha\sigma
= \mu\sigma^2 : \sigma\xi^2$. But $\mu\sigma^2 : \sigma\xi^2$ = the
circle in the cylinder whose diameter is $\mu\nu$ : the circle in the
segment of the right conoid whose diameter is $\xi o$, hence
$\theta\alpha : \alpha\sigma$ = the circle with the diameter $\mu\nu$
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