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• Baldwin-Lomax model
  * {{reference-paper|author=Baldwin, B. S. and Lomax, H.|year=1978|title=Thin Layer Approximation and Algebraic Model * {{reference-paper|author=Granville, P. S.|year=1987|title=Baldwin-Lomax Factors for Turbulent Boundary Layers in Pre
  8 KB (1,262 words) - 09:15, 3 January 2012
• Turbulence modeling
  #### [[Prandtl's one-equation model]] ##### [[Wilcox's k-omega model]]
  3 KB (282 words) - 19:16, 10 April 2021
• Introduction to turbulence/Nature of turbulence
  SONNET TO TURBULENCE by S. Corrsin <ref>Stan Corrsin was a famous and much beloved turbulence researc ...visor. </ref> on the occasion of his 70th birthday, with apologies to Bill S. and Liz B.B.
  16 KB (2,597 words) - 21:12, 9 November 2016
• Ansys FAQ
  ...ulation which has converged at a condition close to the problem simulation's condition.</LI> ...tion process, I get the warning message "A wall has been placed at portion(s) of an OUTLET" ====
  27 KB (4,461 words) - 02:03, 18 August 2018
• Numerical methods
  # [[Solution of Poisson's equation]] ### [[Moore's kd-tree algorithm]]
  4 KB (399 words) - 12:42, 26 August 2012
• Incompressible flow
  \frac{\partial u_i}{\partial t} = \pi^S (-u_j \frac{\partial u_i}{\partial x_j} + \nu \Delta u_i) , which result from the Helmholtz decomposition. <math>\pi^S</math> and <math>\pi^I</math> are the solenoidal (divergence-free) and irro
  8 KB (1,427 words) - 18:57, 19 August 2013
• Siemens FAQ
  ...-CCM+ lite version available with more limited functionality and CD-adapco's own 3D CAD tool ( 3D-CAD ) has been integrated into the STAR-CCM+ client. [[Category: FAQ's]]
  8 KB (1,278 words) - 21:48, 9 December 2017
• Large eddy simulation (LES)
  ...technique for simulating turbulent flows. An implication of [[Kolmogorov]]'s (1941) theory of self similarity is that the large eddies of the flow are d *{{reference-paper|author=Kim, W and Menon, S.|year=1995|title=A new dynamic one-equation subgrid-scale model for large e
  6 KB (882 words) - 21:50, 24 June 2013
• Spalart-Allmaras model
  ...\frac{\partial \tilde{\nu}}{\partial x_j} & = & C_{b1} [1 - f_{t2}] \tilde{S} \tilde{\nu} + \frac{1}{\sigma} \{ \nabla \cdot [(\nu + \tilde{\nu}) \nabla \tilde{S} \equiv S + \frac{ \tilde{\nu} }{ \kappa^2 d^2 } f_{v2}, \quad f_{v2} = 1 - \frac{\ch
  4 KB (662 words) - 13:34, 23 April 2015
• Finite volume
  |V_r| \frac{du_r}{dt} + \sum_{s \in N(r)} \int_{V_r \cap V_s} f_i n_i ds = 0
  4 KB (643 words) - 09:15, 3 January 2012
• Standard k-epsilon model
  :<math> P_k = \mu_t S^2 </math> Where <math> S </math> is the modulus of the mean rate-of-strain tensor, defined as : <br>
  3 KB (401 words) - 20:15, 16 December 2014
• Biconjugate gradient stabilized method
  : Allocate temperary vectors p, phat, s, shat, t, v, rtilde <br> :: s = r - alpha * v <br>
  2 KB (281 words) - 17:01, 31 October 2016
• Overset grids
  ...halmesh is freely available. Unfortuately, the other two are subject to U.S. goverment export controls, and are thus not generally available (see [http
  7 KB (1,042 words) - 14:13, 17 August 2021
• Realisable k-epsilon model
  ...lon}}\right) \frac{\partial \epsilon}{\partial x_j} \right ] + \rho \, C_1 S \epsilon - \rho \, C_2 \frac{{\epsilon}^2} {k + \sqrt{\nu \epsilon}} + C_{1 ...a}{\eta + 5}\right] , \;\;\;\;\; \eta = S \frac{k}{\epsilon}, \;\;\;\;\; S =\sqrt{2 S_{ij} S_{ij}} </math> <br>
  2 KB (380 words) - 19:57, 16 December 2014
• Approximation Schemes for convective term - structured grids - Summary of Discretizations Schemes and examples
  Below it's cleary seen the numerical diffusion impact, comparing the contour fields ob ''It's just a scrap. Later I'll correct it, although it's a complete working code''
  9 KB (1,327 words) - 05:56, 21 April 2012
• Approximation Schemes for convective term - structured grids - Common
  J_{h} - J_{l} & + J_{n} - J_{s} & + J_{e}- J_{w} & + \\ + D_{h} - D_{l} & + D_{n} - D_{s} & + D_{e} - D_{s} & = S_{p}
  28 KB (4,096 words) - 13:11, 24 October 2016
• Wall-adapting local eddy-viscosity (WALE) model
  ...lta _s^2 \frac{(S_{ij}^{d} S_{ij}^{d})^{3/2}}{(\overline{S}_{ij} \overline{S}_{ij})^{5/2} + (S_{ij}^{d} S_{ij}^{d})^{5/4}} </math>
  880 B (137 words) - 08:31, 19 May 2018
• Coeff 11.f90 - calculate the coefficients
  !------------------ s face-------------------- !------------------ s face--------------------
  5 KB (957 words) - 17:58, 20 April 2012
• Sample code for solving Smith-Hutton test - Fortran 90
  ''It's just a scrap. Later I'll correct it, although it's a complete working code''
  3 KB (378 words) - 18:02, 20 April 2012
• LU decomposition
  do s = 1, n-j i = j + s
  4 KB (696 words) - 09:22, 21 November 2011