For the dynamical treatment of polyatomic molecules or clusters as n-body s
ystems, coordinates are conveniently broken up into external (or spatial) r
otations, kinematic invariants, and internal (or kinematic) rotations. The
kinematic invariants are related to the three principal moments of inertia
of the system. At a fixed value of the hyperradius (a measure of the total
moment of inertia), the space of kinematic invariants is a certain spherica
l triangle, depending on the number of bodies, upon which angular coordinat
es can be imposed. It is shown that this triangle provides the 24-element (
group O) octahedral tesselation of the sphere for n = 4 and the 48-element
(group O-h) octahedral tesselation for n greater than or equal to 5. Eigenf
unctions describing the kinematics of systems with vanishing internal and e
xternal angular momentum can be obtained in closed form in terms of Bessel
functions of the hyperradius and surface spherical harmonics. They can be u
seful as orthonormal expansion basis sets for the hyperspherical treatment
of the n-body particle dynamics.