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2. Non-dimensionalization and scaling of the Navier–Stokes ...

   en.wikipedia.org/wiki/Non-dimensionalization_and...

   Further, non-dimensionalized Navier–Stokes equations can be beneficial if one is posed with similar physical situations – that is problems where the only changes are those of the basic dimensions of the system. Scaling of Navier–Stokes equation refers to the process of selecting the proper spatial scales – for a certain type of flow ...

3. Pressure-correction method - Wikipedia

   en.wikipedia.org/wiki/Pressure-correction_method

   While so called global or inner iterations represent the real time-steps and are used to update the variables and , based on a linearized system, and boundary conditions; there is also an outer loop for updating the coefficients of the linearized system. The outer iterations comprise two steps:

4. Streamline upwind Petrov–Galerkin pressure-stabilizing Petrov ...

   en.wikipedia.org/wiki/Streamline_upwind_Petrov...

   The streamline upwind Petrov–Galerkin pressure-stabilizing Petrov–Galerkin formulation for incompressible Navier–Stokes equations can be used for finite element computations of high Reynolds number incompressible flow using equal order of finite element space (i.e. ) by introducing additional stabilization terms in the Navier–Stokes Galerkin formulation.

5. Navier–Stokes equations - Wikipedia

   en.wikipedia.org/wiki/Navier–Stokes_equations

   The incompressible Navier–Stokes equation is a differential algebraic equation, having the inconvenient feature that there is no explicit mechanism for advancing the pressure in time. Consequently, much effort has been expended to eliminate the pressure from all or part of the computational process.

6. Projection method (fluid dynamics) - Wikipedia

   en.wikipedia.org/wiki/Projection_method_(fluid...

   In computational fluid dynamics, the projection method, also called Chorin's projection method, is an effective means of numerically solving time-dependent incompressible fluid-flow problems. It was originally introduced by Alexandre Chorin in 1967 [1] [2] as an efficient means of solving the incompressible Navier-Stokes equations.

7. Large eddy simulation - Wikipedia

   en.wikipedia.org/wiki/Large_eddy_simulation

   Large eddy simulation of a turbulent gas velocity field.. Large eddy simulation (LES) is a mathematical model for turbulence used in computational fluid dynamics.It was initially proposed in 1963 by Joseph Smagorinsky to simulate atmospheric air currents, [1] and first explored by Deardorff (1970). [2]