An Elementary Course in Synthetic Projective GeometryLehmer, Derrick Norman
Science
An Elementary Course in Synthetic Projective Geometry
Lehmer, Derrick Norman
Geometry, Projective
*166. Extension of the theory of poles and polars to space.* As an
illustration of his remarkable powers of generalization, we may note that
Desargues extended the notion of poles and polars to space of three
dimensions for the sphere and for certain other surfaces of the second
degree. This is a matter which has not been touched on in this book, but
the notion is not difficult to grasp. If we draw through any point _P_ in
space a line to cut a sphere in two points, _A_ and _S_, and then
construct the fourth harmonic of _P_ with respect to _A_ and _B_, the
locus of this fourth harmonic, for various lines through _P_, is a plane
called the _polar plane_ of _P_ with respect to the sphere. With this
definition and theorem one can easily find dual relations between points
and planes in space analogous to those between points and lines in a
plane. Desargues closes his discussion of this matter with the remark,
"Similar properties may be found for those other solids which are related
to the sphere in the same way that the conic section is to the circle." It
should not be inferred from this remark, however, that he was acquainted
with all the different varieties of surfaces of the second order. The
ancients were well acquainted with the surfaces obtained by revolving an
ellipse or a parabola about an axis. Even the hyperboloid of two sheets,
obtained by revolving the hyperbola about its major axis, was known to
them, but probably not the hyperboloid of one sheet, which results from
revolving a hyperbola about the other axis. All the other solids of the
second degree were probably unknown until their discovery by Euler.(7)
*167.* Desargues had no conception of the conic section of the locus of
intersection of corresponding rays of two projective pencils of rays. He
seems to have tried to describe the curve by means of a pair of compasses,
moving one leg back and forth along a straight line instead of holding it
fixed as in drawing a circle. He does not attempt to define the law of the
movement necessary to obtain a conic by this means.
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