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
Søgning i bogen
Den bedste måde at søge i bogen er ved at downloade PDF'en og søge i den.
Derved får du fremhævet ordene visuelt direkte på billedet af siden.
Digitaliseret bog
Bogens tekst er maskinlæst, så der kan være en del fejl og mangler.
428] THE THEORY OF SCREWS IN NON-EUCLIDIAN SPACE. 475
We thus learn the remarkable fact, that if a right (left) vector be followed
by a left (right) vector, the effect produced is the same as if the order of
the two vectors had been interchanged.
This is not true for two right vectors or two left vectors.
The theorems at which we have arrived may be thus generally
enunciated:—
In the composition of vectors the order of two heteronymous vectors does
not affect the result, but that of two homonymous vectors does affect the result.
In the composition of two homonymous vectors the result is also an homony-
mous vector. In the composition of two heteronymous vectors the result is not
a vector at all.
The theorems just established constitute the first of the fundamental
principles relating to the Theory of Screws in non-Kuclidian Space referred
to in § 396. Their importance is such that it may be desirable to give a
geometrical investigation.
428. Geometrical proof that two Homonymous Vectors com-
pound into one Homonymous Vector.
Left vectors cannot disturb any
right generators of the infinite quad-
ric. Take two such generators, AB
and A'B' (Fig. 48). Let AA',
BB’, GC be three left generators
which the first vector conveys to
A-lAi, Bfff, GfJf and the second
vector further conveys to A.,A.f
B2B.f C2Cf Let X and Y be the
double points of the two homo-
graphic systems defined by A, B, G
and A*, B.2, G2. Then we have
(ABGX) = (A2BAX),
and
(ABGY) = (AMY).
As anharmonic ratios cannot be
altered by any rigid displacement, it
follows that X and Y must each
occupy the same position after the
second vector which they had before
the first, similarly, X' and Y' will
remain unchanged, and as the two
rays, AB and A'B‘ are divided homo-
Fig. 48.