The notion of the family boundary curves (FBC) is introduced for that
version of the inverse problem of Lagrangian dynamics which deals with
the determination of the potential V(u, v) under which a given monopa
rametric family of curves f(u, v) = c, on the configuration manifold (
M(2), g) of a conservative holonomic system with n = 2 degrees of free
dom, can be described as dynamical trajectories (orbits) of the repres
entative point. It is shown that, in general, curves of the family f(u
, v) = c generated by a class of potentials V(u,v) are actual orbits o
nly in a subregion of the region where they are defined as geometrical
entities. (In general, the FBC are distinct from the well known zero
velocity curves (ZVC), the later referring to orbits of the same const
ant energy). If, however, the holonomic system is subject to non-conse
rvative generalized forces, it is shown that we can always find many p
airs of such forces {Q(1), Q(2)} giving rise to any family of trajecto
ries lying in any pre-assigned (open or closed) region of the configur
ation space. Three examples are presented to account both for conserva
tive and non-conservative forces.