A Treatise on the Theory of Screws
Forfatter: Sir Robert Stawell Ball
År: 1900
Forlag: The University Press
Sted: Cambride
Sider: 544
UDK: 531.1
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178] FREEDOM OF THE THIRD ORDER. 179
This equation denotes a form of Steiner’s surface :
where
a — 2x b — c + -2,J- + c — a 2z a — b + 1,
2x b — c c — a 2z a — b + 1,
7 = 2x b — c + _ty_ _ c — a 2z a — b + 1,
3 = 2x b — c c — a _2z_ a — b + 1.
From the form of its equation it appears that this surface has three
double lines which meet in a point, viz. the three axes OX, OY, OZ. This
being so any plane will cut the surface in a quartic curve with three double
points, being those in which the plane cuts the axes. If the plane touch the
surface, the point of contact is an additional double point on the section, that
is, the section will be a quartic curve with four double points, i.e. a pair of
conics. The projections of the origin on the generators of any cylindroid
belonging to the system lie on a plane ellipse (§ 23). This ellipse must lie
on the Steiner quartic. Hence the plane of the ellipse must cut the quartic
in two conics and must be a tangent plane. See note on p, 182.
178. Screws of the Three-System parallel to a Plane.
Up to the present we have been analysing the screw system by classifying
the screws into groups of constant pitch. Some interesting features will be
presented by adopting a new method of classification. We shall now divide
the general system into groups of screws which are parallel to the same
plane.
We shall first prove that each of these groups is in general a cylindroid.
For suppose a screw of infinite pitch normal to the plane, then all the screws
of the group parallel to the plane are reciprocal to this screw of infinite
pitch. But they are also reciprocal to any three screws of the original
reciprocal system; they, therefore, form a screw system of the second order
(§ 72)—that is, they constitute a cylindroid.
We shall prove this in another manner.
A quadric containing a line must touch every plane passing through the
line. The number of screws of the system which can lie in a given plane
is, therefore, equal to the number of the quadrics of the system which can
be drawn to touch that plane.