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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418] THE THEORY OF SCREWS IN NON-EUCLIDIAN SPACE.
461
Reverting, then, to a space of which the several points correspond to the
objects of a content, we find, that for every homographic transformation
which corresponds to a displacement in ordinary geometry a singly infinite
family of quadrics is to remain unchanged, and the infinite quadric itself is
to form one member of this family.
Let us now suppose a range in the content submitted to this description
of homographic transformation. Let P, Q be two objects on the range, and
let X, F be the two infinite objects thereon. This range will be transformed
to a new position, and the objects will now be P', Q', X', Y'. Since infinite
objects must remain infinite, it follows that X' and Y' must be infinite, as
well as X and Y. Also, since homographic transformation does not alter
anharmonic ratio, we have
(PQXY) = (P'Q'X'Y')-,
whence, by Axiom V., we see that the intervene from P to Q equals the
intervene from P’ to Q'; in other words, that all intervenes remain unchanged
by this homographic transformation.
Every homographic transformation which possesses these properties must
satisfy a special condition in the coefficients. This may be found from
the determinantal equation for p (p. 458), for then the following symmetric
function of the four roots p2> p3, p4 must vanish:
(piPi ~ Pspt) (piPs ~ p-2pi) (piPt ~ PzpsY
418. The Geometrical Meaning of this Symmetric Function.
We may write the family of quadrics thus :
X,X, + XZ8Z4 = 0.
All these quadrics have two common generators of each kind:
Æ = 0, X, = 0 (X4 = 0, X4 = 0
J and J and
= 0) ^4 = 0 ^-^-2 “ 0, ^3 ~ 0.
For the rays X4 = 0, X3 = 0, and X4 = 0, X4 = 0, are both contained in the
plane Xlt and therefore intersect, and, accordingly, belong to the opposed
system of generators.
The geometrical meaning of the equation
PlPz Psp4 = 0
can be also shown.
The tetrahedron formed by the intersection of the two pairs of generators
just referred to remains unaltered by the transformation. Any point on the
edge, X4 = 0, X3- = 0, of which the co-ordinates are
0, X2, 0, X4,