Consider a nonconstant \(T\)-periodic orbit \(\gamma (t)\) of the smooth autonomous differential equation \[ \dot {x}=f(x),\qquad x\in \mathbb {R}^n. \]
- Describe the Poincaré Return Map associated to \(\gamma \).
- A \(2\pi \)-periodic solution of the planar system \[ \begin {aligned} \dot {x} &= x-(x+y)\sqrt {x^2+y^2},\\ \dot {y} &= y+(x-y)\sqrt {x^2+y^2} \end {aligned} \] is given by \(\gamma (t)=(\cos t,\sin t)\). Find a Poincaré Return Map associated to \(\gamma \).
- Find the derivative of the Poincaré Return Map from part (b) at \(\gamma \).
- Using (c), determine whether the solution (b) is stable and define the sense of stability you mean.