classical mechanics - What are Hamilton's equations with respect to a nonstandard symplectic form?

Hamilton's equations for a Hamiltonian $H(q,p)$ w.r.t. to a standard symplectic from $\omega = dq \wedge dp$ are

$$\dot{q} = \partial H_{p}, \quad \dot{p} = - \partial H_{q}$$

How do Hamilton's equations write w.r.t. a nonstandard symplectic form $F(q,p) dq \wedge dp$, where $F(q,p)$ is some smooth function?

Answer

1. 
   

   More generally, let there be given a Poisson manifold $(M,\pi)$, where

   $$\pi ~=~ \frac{1}{2} \pi^{IJ} \frac{\partial}{\partial z^I} \wedge \frac{\partial}{\partial z^J}$$ is a Poisson bi-vector, and $$\{ f, g\}_{PB}~=~\frac{\partial f}{\partial z^J}\pi^{IJ}\frac{\partial g}{\partial z^J}$$ is the corresponding Poisson bracket. Let the Hamiltonian $H$ be a globally defined function on $M$. Then Hamilton's equations read $$\dot{z}^{I}~=~\{ z^I, H\}_{PB},$$ i.e. time-evolution is given by (minus) the Hamiltonian vector field $$X_H~=~\{H,\cdot\}_{PB}.$$
   
   


2. 
   

   If the Poisson structure is invertible, then $M$ is a symplectic manifold with symplectic 2-form

   $$\omega ~=~\frac{1}{2} \omega_{IJ}~ \mathrm{d}z^I \wedge \mathrm{d}z^J,$$ where $\omega_{IJ}$ is the inverse matrix: $$\pi^{IJ}\omega_{JK}~=~\delta^I_K.$$
   
   


3. 
   

   In canonical/Darboux coordinates

   $$(z^1, \ldots, z^{2n})~=~(q^1, \ldots, q^n,p_1,\ldots, p_n) ,$$ the above construction reduces to the standard Poisson bi-vector $$\pi~=~\frac{\partial}{\partial q^i} \wedge \frac{\partial}{\partial p_i},$$ and the standard symplectic 2-form $$\omega ~=~ \mathrm{d}p_i \wedge \mathrm{d}q^i.$$