CFD - Modelling Turbulent Flows Flashcards
Reynolds Number (Re)
A dimensionless number used to indicate whether a fluid flow is either laminar or turbulent
Critical Reynolds Number
The onset of turbulence/transition occurs at a critical value of Re = 2300.
General Definition of Re
The ratio of inertia forces to friction forces.
Common features in transition processes
- Amplification of initially small disturbances
- Development of areas with concentrated rotational structures
- Formation of intense small-scale motions
- Growth and merging of these areas into full turbulent flows
What affects the transition processes
- Pressure Gradient
- Disturbance Levels
- Wall Roughness
- Heat Transfer
Characteristics of Turbulence
- Irregularity (random and chaotic): treated statistically rather than deterministically
- Three-dimensional rotation, unsteady
- Diffusivity: enhanced mixing and increased rates of mass, momentum, and energy transports in a flow
- Dissipation of energy (Kinetic Energy to Internal Energy)
- Multi-scale vortex structures in the turbulent fields
- Energy cascades from large-scale to smaller scale structures
- Mixing: turbulence increases the mixing of momentum and heat
Energy Cascade
Large-scale structures cascade down to small-scale structures
Kolmogorov Length Scale
Structures that are small enough that molecular diffusion becomes important and viscous dissipation of energy finally takes place.
Spectral Energy E(K). Units: (m^3/s^2)
Kinetic energy per unit mass per unit wave number of fluctuations around the wave number K.
Kolmogorov Microscales
The smallest scales presented in a turbulent flow where viscosity dominates and the turbulent kinetic energy is dissipated into heat.
Reynolds Decomposition
Defines flow property phi(t) at this point as the sum of a steady mean component “phi bar” and a time-varying fluctuating component phi ‘ (t).
phi(t) = “phi bar” + phi ‘ (t)
Kinetic Energy per unit mass of the turbulence at a given location
k = 1/2 x ui’ x ui’ = 1/2 x (u’^2 + v’^2 + w’^2
ui’ - time-averaged fluctuation in velocity
Turbulence Intensity Ti
The average r.m.s velocity divided by a reference mean flow velocity
Ti = sqrt(2k/3)/Vref
Reynolds Averaged Navier-Stokes (RANS)
Average the Navier-Stokes Equations in time and use a model to predict the extra terms that appear. Models all turbulent scales.
Large Eddy Simulation (LES)
Solve the Navier-Stokes Equations only for large turbulent scales and use a model to account for the small turbulent scales