  When we consider a differential equation $\Delta=0$ whose set of solutions is
${{\cal S}}_\Delta$, a Lie-point exact symmetry of this is a Lie-point
invertible transformation $T$ such that $T({{\cal S}}_\Delta)={{\cal
S}}_\Delta$, i.e. such that any solution to $\Delta=0$ is tranformed into a
(generally, different) solution to the same equation; here we define {\it
partial} symmetries of $\Delta=0$ as Lie-point invertible transformations $T$
such that there is a nonempty subset ${{\cal P}} \subset {{\cal S}}_\Delta$
such that $T({{\cal P}}) = {{\cal P}}$, i.e. such that there is a subset of
solutions to $\Delta=0$ which are transformed one into the other. We discuss
how to determine both partial symmetries and the invariant set ${{\cal P}}
\subset {{\cal S}}_\Delta$, and show that our procedure is effective by means
of concrete examples. We also discuss relations with conditional symmetries,
and how our discussion applies to the special case of dynamical systems. Our
discussion will focus on continuous Lie-point partial symmetries, but our
approach would also be suitable for more general classes of transformations;
the discussion is indeed extended to partial generalized (or Lie-B\"acklund)
symmetries along the same lines, and in the appendix we will discuss the case
of discrete partial symmetries.
