Vorticity Equation
For an incompressible fluid with const viscosity, show that
∇.[( ∇→. ∇)V→] = 1/2 ∇2(V→.V→) - V→.(∇2V→) - ω→.ω→
Using Navier-Stokes equation and the above result, show that the pressure distribution can be related to the velocity and vorticity by
∇2(P/δ) ω→.ω→ + V→.(∇2V→) - 1/2∇2(v→.v→)