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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266] EMANANTS AND PITCH INVARIANTS. 279
This can be verified in the following manner. We have
K=pX'3,
d\j d Xj d \ 2
and, therefore, if X be reciprocal to the first screw of reference, the formula
to be proved is
d Xj d X;
A few words will be necessary on the geometrical signification of the
differentiation involved. Suppose a Dyname X be. referred to six co-ordinate
screws of absolute generality, and let us suppose that one of these co-
ordinates, for instance X1( be permitted to vary, the corresponding situation
of X also changes, and considering each one of the co-ordinates in succession;
we thus have six routes established along which X will travel in correspond-
ence with the growth of the. appropriate co-ordinate. Each route is, of
course, a ruled surface; but the conception of a surface is not alone adequate
to express the route. We must also associate a linear magnitude with each
generator of the surface, which is to denote the pitch of the corresponding
screw. Taking X and another screw on one of the routes, we can draw a
cylindroid through these two screws. It will now be proved that this
cylindroid is itself the locus in which X moves, when the co-ordinate cor-
related thereto changes its value. Let 0 be the screw arising from an
increase in the co-ordinate Xjj a wrench on 0 of intensity 0' has components
of intensities 0/,)... 0,'' ■ A wrench on X has components X/,... X8 . But
from the nature of the case,
V V” V
If therefore 0" be suitably chosen, we can make each of these ratios — 1,
so that when 0" and X" are each resolved along the six screws of reference,
all the components except 0”, — X/' shall neutralize. But this can only be
possible if the first reference screw lie on the cylindroid containing 0 and X.
Hence we deduce the result that each of the six cylindroids must pass
through the corresponding screw of reference; and thus we have a complete
view of the route travelled by a screw in correspondence with the variation,
of one of its co-ordinates.
Let the six screws of reference be 1, 2, 3, 4, 5, 6. Form the cylindroid
(X, 1), and find that one screw on this cylindroid which has with 2, 3,4, 5, 6,
a common reciprocal (§ 26). From a point 0 draw a pencil of four rays parallel
to four screws on the cylindroid. Let OA be parallel to one of the principal
screws; OX be parallel to X, Oq to y, and Oh to the first screw of reference.