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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^00 THE THEORY OF SCREWS. [200-
moves over the cylindroid and the corresponding point moves over the
straight line. Hence we obtain the following important result:__
The several screws on a cylindroid correspond to the points on a straight
line.
Ill general two cylindroids have no screw in common. If, however, the two
cylindroids be each composed of screws taken from the same three-system,
then they will have one screw in common. This is demonstrated by the
fact that the two straight lines corresponding to these cylindroids necessarily
intersect in a point which corresponds to the screw common to the two
surfaces.
Three twist velocities about three screws will neutralize and produce
rest, provided that the three corresponding points lie in a straight line, and
that the amount of each twist velocity is proportional to the sine of the
angle between the two non-corresponding screws.
rhiec wrenches will equilibrate when the throe points corresponding to
the screws are collinear, and when the intensity of each wrench is propor-
tional to the sine of the angle between the two non-corresponding screws.
201. The Screws of the Three-system.
In any three-system there are three principal screws at right angles to
each other, and intersecting in a point (§ 173). It is natural to choose these
as the screws of reference, and also as the axes for Cartesian co-ordinates.
The pitches of these screws are pu p2, p3, and we shall, as usual, denote the
screw co-ordinates by 3lt 32, 03. The displacement denoted by this triad of
co-ordinates is obtained by rotating the body through angles 3lt 02, 33 around
three axes, and then by translating it through distances p^, p..3.,, p3d3 parallel
to these axes. As these quantities are all small, we have, for the displace-
ments produced in a point x, y, z,
Sx =p131+z3.2 - y 3.
^y = p-ß-1 + x3s-z31,
& = pA + y31 - x32;
these displacements correspond to a twist about a screw of which the axis
has the equations
pA + z32-y33 = pA + «A- zA _ p333 + y3, - x3„
3, 3.2 3S
while the pitch p is thus given :
,n _ PA + pA2 + p-A2
1 fff + ØJ + ØJ ■
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