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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I g the theory of screws. ly>
of p Suppose that a and ß' be varied while their ratio is preserved P
and Q will then be transferred to P" and Q" while by the property just
proved P P' P" will be collinear and so will Q, Q', Q"- It therefore follows
that as P, P', Q, Q’ are collinear so will P, Q, P", Q." be collinear. The line
PQ will therefore be displaced upon itself for every pair of values a and
ß which retain the same ratio. The position of the resultant screw is thus
not altered by any changes of a! and ß', which preserves their ratio.
Let w be the angle between a and ß. We take the case of a point P
at an infinite distance on the common perpendicular to a and ß. 1 ns
point is displaced through a distance equal to
h Va'2+/37?+ 2a'/3' cos &>,
where h stands for the infinite perpendicular distance from P to a or to ß.
This displacement of P is normal to p which itself intersects at right angles
the common perpendicular to a and ß. As the perpendicular distance from
P to p can only differ by a finite quantity from h
bp' = A Va'2 + ß'2 + 2a ß' cos &>,
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p' = Va'2 -I- ß'2 + 2a'ß’ cos w.
This determines the amplitude of the resulting twist which is, it may be
noted, independent of the pitches.
Let d> be the angle between the directions in which a point Q on p is
displaced by the twists about a and ß, then the square of the displacement
of Q will be _________
(p2 + V) a'2 + (pf + V) ß'2 + 2 V/V + V vaß' cos </>;
but this may also be written
pp2 (a'2 + ß'2 + 2a ß' cos cP),
whence we see that pp depends only on the ratio of a to ß.
The pitch and the position of p thus depend on the single numerical
parameter expressing the ratio of a' and ß'. As this parameter vanes so
will p vary, and it must in successive positions coincide with the several
generators of a certain ruled surface. Two of these generators will be the
situations of a and of ß corresponding to the extreme values of zero and
infinity respectively, which in the progress of its variation the parameter
will assume.
We shall next ascertain the laws according to which twists (and wrenches)
must be compounded together, that is to say, we shall determine the single
screw, one twist (or wrench) about which will produce the same effect on t e
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