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 Advection term
- 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