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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160
THE THEORY OF SCREWS.
[162-
The line at infinity on the plane of z is of course intersected by all the real
generators of the cylindroid, inasmuch as they are parallel to z. Ihe points
at infinity on the planes x + iy = 0 are each the residence of an imaginary
screw, also belonging to the surface. The pitches of both these screws are
infinite.
We may deduce the two screws of infinite pitch on the surface in another
way. The equations of a screw are
y — x tan 0,
z = m sin 20,
while the pitch is
p„ + m cos 20.
If tan 0 be either + i, we find both z infinite and the pitch infinite. We
thus see that through the infinitely distant point I, on the nodal line of the
cylindroid, two screws belonging to the surface can be drawn, just as at any
finite point. The peculiarity of the two screws through I is, that their
pitches are equal, i.e. both infinite, and this is not the case with any other
pair of intersecting screws.
It is now obvious why the envelope just considered turned out to be
a parabola rather than any other conic section. Every plane section will
have the line at infinity for a transversal cutting two screws of equal pitch;
the envelope of such transversals must thus have the line at infinity for
a tangent, i.e. must be a parabola.
163. Chord joining Two Points.
If 0' and 0" be the angles by which two points on the cubic are defined,
then the equation to the chord joining those points is
Ax + By + <7=0;
where A = 2 m cos (#' — a) cos (0" — a) cos (0' + 0"),
B = h sin ß + m cos ß cos (0' + 0") sin (2a - 0' - 0")
— m cos ß sin (0' + 0") cos (0' — 0"),
C = — tan ß (A — m cot ß sin 2Ö') (A — m cot ß sin 20").
If in these expressions we make 0' + 0" = 0, we obtain the equation for the
chord joining screws of equal pitch, as already obtained.
We shall find that, in particular sections, these expressions become con-
siderably simplified. Suppose, for example, that the plane of section be a
tangent plane to the cylindroid. The cubic then degenerates to a straight
line and a conic. The condition for this will be obvious from the equation