From: LordBeotian on
I think that the only 1-periodic, C^infty and uniformly bounded vector
field on the plane is the zero vector field. By 1-periodic I mean that
all the orbit returns to the starting point after time 1.

While trying to prove this statement I'm not really satisfied of my
argumets, so I hope something more linear can be found as a proof. My
Idea is the following: suppose there is a point with nonzero vector
field, then there is a closed orbit C starting from it. Take a
reference point p inside the orbit, I want to prove that any external
point x has an orbit which has a winding number wrt p which is the
same as C (this wuould prove the statement since imply the existence
of arbitrary long orbit which is impossible for a 1-periodic and
bounded vector field). To prove that the winding number is the same as
C I take a segment which connects C with x parametrized with f(t), t
in [0,1]. The winding number of the orbit starting from f(t) must be
constant unless there is a first point f(t*) where the vector field
vanishes. If the vector field vanishes on f(p) then I take a
neighbourhood B of f(t*) and I consider the time T(y) needed to exit
the neighbourhood for the orbit which starts from y in B. T is well
defined for f(t) and t<t*. The function T(f(t*)) have to diverge for t-
>t* (actually I need an argument for this but it seems reasonable) but
this is impossible because the vector field is 1-periodic.

Is there a more strightforward way to prove the statement?