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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214] FREEDOM OF THE FOURTH ORDER. 223
is of course
(Pe + P<t,) cos W) - sin W) de-l> = 2Pe cos (0<f>),
or
(P4> ~ Pe) cos W) ~ sin W) de4> = °-
If then p<i, = p(i we must have sin(Ö</>) dfj,,,= 0, which requires that 0 and
<f> must intersect at either a finite or an infinite distance.
In the case where <f> is at right angles to 0 it follows from the formula
= cos (#</>) p6 that ■sr^ = 0, or that 0 and <f> are reciprocal. But two screws
which are at right angles and also reciprocal must intersect, and hence we
have the following theorem.
If 0 be a screw of stationary pitch in an n-system, then any other screw
belonging to the n-system and at right angles to 0 must intersect 0.
If <j> belongs to an n-system its co-ordinates must, on that account, satisfy
6 - n linear equations. If it be further assumed that </> has to be perpen-
dicular to 0, then the co-ordinates of have to satisfy yet one more equa-
tion, i.e.
. dll , dll ..
In this case </> is subjected to 7 - n linear equations. It follows (§ 76) that
(p will have as its locus a certain (n — l)-system, whence we have the following
general theorem.
If 0 is a screw of stationary pitch in an n-system P then among the
(n _ systems included in P there is one Q such that every screw of Q intersects
0 at right angles.
These theorems can also be proved by geometrical considerations. If a
screw 0 have stationary pitch in an n-system it follows a fortiori that 0 must
have stationary pitch on any cylindroid through 0 and belonging wholly to
the n-system. This means that 0 must be one of the two principal screws
on such a cylindroid. Choose any other screw </> of the system and draw the
cylindroid (0, <f>) then 0 is a principal screw, and if 0 and the other principal
screw on the cylindroid be two of the co-reciprocal screws of reference, then
the co-ordinate of </> with respect to 0 is cos (00) (§ 40). But that co-ordinate
must also have the general form plt whence at once we obtain
ww = cos (Ø^Pe-
Let 0 be a screw of stationary pitch in a throe-system, and let </> and
be any two other screws in that system. Then 0 is one of the principal
screws on the cylindroid (0<f); let a be the other principal screw on that