Omega-limit sets and bounded solutions

We prove among other things that the omega-limit set of a bounded solution of a Hamilton system $$\left\{\begin{aligned} & \mathbf{\dot{p}}=\frac{\partial H}{\partial \mathbf{q}} & \mathbf{\dot{q}}=-\frac{\partial H}{\partial \mathbf{p}} \\ \end{aligned} \right.$$ is containing a full-time solution so there are the limits of $\frac 1t\int_0^t {\mathbf p}(s)ds$ and $\frac 1t\int_0^t {\mathbf q}(s)ds$ as $t\to\infty$ for any bounded solution $(\mathbf {p,q})$ of the Hamilton system. These limits are stationary points of the Hamilton system so if a Hamilton system has no stationary point then every solution of this system is unbounded.