It has recently been shown that finite displacement screws of a partic
ular form enter into linear patterns of combination-displaying the fam
iliar structures of the screw systems-when they are used to describe i
ncompletely specified displacements. Certain kinematic situations demo
nstrate the same simple linearity if normal usage is extended to admit
dual coefficients of combination, the system then being referred to a
s a dual system. The screw triangle rule for composing the resultant d
isplacement screw of two given finite displacement screws is examined
in this paper. On regarding the lines of the given screws as fixed, an
d the displacement movements about them as variable, it is found that
all available resultant screws occupy a structure which can be various
ly described as a dual 3-system (which contains infinitely many real 3
-systems) or as the sum of two axially-orthogonal dual 2-system (each
of which contains all linear combinations, using complementary dual si
nusoidal coefficients, of two basis screws). The basis screws and noda
l lines for these systems are found to lie on the triad of mutually or
thogonal mirror-symmetry axes for the lines of the given screws. (C) 1
997 Elsevier Science Ltd.