I was given a definition.
A symmetry of a plane figure $F$ is an isometry that maps $F$ to itself, that is, an isometry $f:R^2 \to R^2$ such that $f(F)=F$.
I don't really understand this because is $F$ not a collection of points and the domain of the function consists of single points in $R^2$?
Can someone help me out? Thanks.