Let a finite set of interacting particles be given, together with a symmetry
Lie group G. Here we describe all possible dynamics that are jointly
equivariant with respect to the action of G. This is relevant e.g., when one
aims to describe collective dynamics that are independent of any coordinate
change or external influence. We particularize the results to some key
examples, i.e. for the most basic low dimensional symmetries that appear in
collective dynamics on manifolds