Let GG act on MM by a .

For x∈Mx\in M, the orbit map at xx is the

Φx:G⟶M,Φx(g)=g⋅x.\Phi^x: G \longrightarrow M,\qquad \Phi^x(g)=g\cdot x.
Image and stabilizer

Its image is the G⋅xG\cdot x.

The fiber (Φx)−1(x)(\Phi^x)^{-1}(x) is the GxG_x. The orbit map is constant on cosets gGxgG_x, because Φx(gh)=g⋅x\Phi^x(gh)=g\cdot x for h∈Gxh\in G_x, and hence factors through G/GxG/G_x.

Examples
  1. Left translation on GG. For the action of GG on itself by left multiplication and a fixed h∈Gh\in G, the orbit map is g↦ghg\mapsto gh.
  2. Rotations of a vector. For SO(2)↷R2SO(2)\curvearrowright \mathbb{R}^2 and x≠0x\neq 0, the orbit map parametrizes the circle of radius ∥x∥\|x\|.
  3. Conjugation. For the conjugation action of GG on itself, the orbit map at hh is g↦ghg−1g\mapsto ghg^{-1}, whose image is the conjugacy class of hh.