| In this paper we study Buttke's velicity reformulation of the incompressible Euler equation, and the symplectic integration of the Hamiltonian system obtained by discretizing the velicity equation.;We show that the linearized velicity equation is hyperbolic only in the weak sense and we analyze the characteristics of the linearized velicity equation for the variable coefficient case.;We will briefly describe the symplectic schemes; one is the implicit midpoint scheme, and the other one is a fourth-order implicit scheme. We apply the implicit midpoint scheme (IM) to our Hamiltonian system for large time, with the fixed time step (;Our work builds on recent progress of the Hamiltonian formulation of the incompressible Euler equation and the Lagrangian numerical methods for incompressible Euler's equation, particularly the work of Buttke. |