on the right hand side of Eq.(3) is the term about acceleration due to pressure. From the term, we can find that the acceleration due to pressure is in proportion to the pressure gradient ∇P, and is in inverse proportion to the fluid density ρ. The minus sign before ∇P is necessary because the force due to the pressure gradient works in the direction whose pressure is the lowest. The second term of ν∇^2u is the viscosity term, which is the acceleration vector due to viscosity. The viscosity term diffuses the momentum of fluid. The coefficient ν is the kinematic viscosity coefficient. The third term g is the acceleration vector due to the gravity.
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