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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209] PLANE REPRESENTATION OF THE THIRD ORDER. 209
By changing the sign of a, and then changing the signs of ß and of y, we
shall obtain the four points iu which the pencil 0(Pn P2, Pt, Pß cuts the
axis </>3 = 0. If four values of be represented by k, I, m, n, the required
<Pa
anharmonic ratio is, of course,
(n — l)(m — k)
(n — m) (I — k) ’
and after a few reductions we find that this becomes
But we have
et^p^p^
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a^yW^-ßW.^)'
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Eliminating fp2, we find that 022 and 0<? disappear also when we make
a2 = p2-p3, ß2=ps~Pi, 72 = Pi~P-2,
and we obtain the following result:
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3 (P^PffP^ = P'-: p' x ,
Pt-Pt Pi-p
which gives the following theorem:—
Measure off distances plt p2, p3, p, from an arbitrary point on a straight
line, then the anharmonic ratio of the four points thus obtained is equal to the
anharmonic ratio subtended by any point of the p-pitch conic at the four points
of indeterminate pitch.
It is possible without any sacrifice of generality to make the zero-pitch
conic a circle. For take three angles A, B, G whose sum is 180° and such
that the equations
sin 2/1 _ sin 2B _ sin 2G
Pi Pt Pt
are satisfied where plt p2, p3 are the three principal pitches of the three-
system. If the fundamental triangle has A, B, G for its angles then the
equation
a/ sin 2J + a22 sin 2B + «32 sin 2G = 0,
is the equation of the zero-pitch conic. It is however a well-known theorem
in conics that this equation represents a circle with its centre at the ortho-
centre, that is, the intersection of the perpendiculars from the vertices of the
triangle on its opposite sides.
We thus have as the system of pitch conics
a,2 sin 2 A + a22 sin 2B + «32 sin 2G — p (a2 + a22 + a32) = 0.
B.
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