The Navier-Stokes equations are a set of Partial Differential Equations that describe almost all fluid dynamics. They describe how the velocity, pressure, temperature, and density of a moving fluid are related.

Incompressible Navier Stokes Equations

For incompressible fluids; if one part of the fluid is displaced, the opposite side is also displaced equally and instantly. Incompressibility means constant density .

  • where is the velocity vector
  • where is time
  • where is the density of the fluid
  • where is the pressure of the fluid
  • where is the kinematic viscosity
  • where is the external force

  • The first equation is the moment equation.
    • The Advection term
      • Says that the fluid moves on its own, and moves faster in regions of higher velocity. Shocker.
    • The Pressure term
      • Says that the fluid flow is along a pressure gradient.
      • This term causes divergence, which is illegal is zero-divergence land, and can be omitted.
      • We can correct for this omission through Projection, which uses Helmholtz-Hodge Decomposition to isolate the zero-divergence component for a given point in the field. This involves solving the Poisson Equation and then subtracting the Gradient.
    • The Diffusion term
      • Says that the fluid flow tends to diffuse along the velocity gradient, and that the more the fluid diffuses, the smooth the velocity field gets.
    • The External Force term
      • Says “Hello, I am external force”
  • The second equation is the continuity equation, which enforces incompressibility.
    • At any point, the velocity flow into that point and out of that point must net to zero, i.e. the Divergence is zero.
  • These equations generally cannot be solved analytically, and instead require Numerical Methods