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• Navier-Stokes equations
  </td><td width="5%">(6)</td></tr> </td><td width="5%">(6)</td></tr></table>
  29 KB (4,606 words) - 18:17, 28 August 2012
• Posdat.f
  LQ(6,IC): the x direction neighbor cell; LQ(6,IC): the z direction neighbor cell;
  3 KB (540 words) - 12:13, 3 September 2011
• Reynolds stress model (RSM)
  ...theorie nichthomogener turbulenz.|rest=Zeitschrift für Physik A, Vol. 129(6), pp. 547-572}}
  8 KB (1,203 words) - 01:47, 18 April 2017
• Near-wall treatment for k-omega models
  \omega_\text{vis} = \frac{6\nu}{\beta y^2} & \omega_\text{log} = \frac{u_\tau}{C_\mu^{1/4} \kappa y}
  4 KB (581 words) - 10:40, 31 March 2021
• Best practice guidelines for turbomachinery CFD
  ...ion in a Transonic Turbine|rest=AIAA Journal of Propulsion and Power, vol. 6, no. 5}}
  41 KB (6,252 words) - 08:46, 4 March 2023
• Baldwin-Lomax model
  </math></td><td width="5%">(6)</td></tr></table> F_{KLEB}(y) = \left[1 + 5.5 \left( \frac{y \, C_{KLEB}}{y_{MAX}} \right)^6
  8 KB (1,262 words) - 09:15, 3 January 2012
• Ansys FAQ
  ...tation. Specifically section 15 ("Advice on Flow Modeling"), section 15.10.6 ("Problems with Convergence"), and any best practice guides applicable to y 6. Postprocess both the CFD and solids results in CFX-Post.
  27 KB (4,461 words) - 02:03, 18 August 2018
• Large eddy simulation (LES)
  ...for large-eddy simulation in complex geometries|rest=Physics of Fluids, 19(6): 065110, 2007}}
  6 KB (882 words) - 21:50, 24 June 2013
• Spalart-Allmaras model
  ...ac{ 1 + C_{w3}^6 }{ g^6 + C_{w3}^6 } \right]^{1/6}, \quad g = r + C_{w2}(r^6 - r), \quad r \equiv \frac{\tilde{\nu} }{ \tilde{S} \kappa^2 d^2 }
  4 KB (662 words) - 13:34, 23 April 2015
• Gauss-Seidel method
  | 6.1237E-01 | 6.2500E-01
  8 KB (1,113 words) - 09:15, 3 January 2012
• Jacobi method
  | 6.1237E-01 | 6.2500E-01
  6 KB (825 words) - 09:15, 3 January 2012
• Realisable k-epsilon model
  <math> A_0 = 4.04, \; \; A_s = \sqrt{6} \cos \phi </math> <br> <math> \phi = \frac{1}{3} \cos^{-1} (\sqrt{6} W), \; \; W = \frac{S_{ij} S_{jk} S_{ki}}{{\tilde{S}} ^3}, \; \; \tilde
  2 KB (380 words) - 19:57, 16 December 2014
• Approximation Schemes for convective term - structured grids - Summary of Discretizations Schemes and examples
  </td><td width="5%">(6)</td></tr></table> </td><td width="5%">(6)</td></tr></table>
  9 KB (1,327 words) - 05:56, 21 April 2012
• Approximation Schemes for convective term - structured grids - Common
  </td><td width="5%">(6)</td></tr></table> ... | rest=International Journal for Numerical Methods in Fluids, Vol. 8, No. 6, pp. 617-641}}
  28 KB (4,096 words) - 13:11, 24 October 2016
• LES filters
  G(x) = \left( \frac{6}{\pi \Delta^2} \right)^{1/2} e^{ \frac{-6 x^2}{\Delta^2}}
  2 KB (283 words) - 09:15, 3 January 2012
• Sand box Approximation Schemes
  \end{array}} \right . \quad \quad ( 6)</math> ... Meth. Fluids |volume=8 |page=617–641 |doi=10.1002/fld.1650080602 |issue=6|bibcode = 1988IJNMF...8..617G }}
  26 KB (3,687 words) - 20:19, 7 November 2011
• V2-f models
  ...} = 1</math>, <math>C_1 = 1.4</math>, <math>C_2 = 0.45</math>, <math>C_T = 6</math>, <math>C_L = 0.25</math> and <math>C_{\eta} = 85</math>. <math>T = \max \left[ \min \left( \frac{k}{\varepsilon},\, \frac{0.6}{\sqrt{6} C_{\mu} |S|\zeta} \right), C_T \left( \frac{\nu}{\varepsilon} \right)^{1/
  6 KB (917 words) - 05:45, 7 February 2014
• Ahmed body
  [6] M. Minguez, R. Pasquetti, E. Serre, High-order large-eddy simulation of fl
  4 KB (577 words) - 05:46, 6 October 2015
• CHAM FAQ
  :''ACP=1.6582; BCP=-8.479E-4; CCP=4.4541E-7; DCP=-2992.6'' :''(stored of SODV is EXP(-6.4406-0.3958*LOGE(TDEK)+556.835/TDEK)!ZSLSTR)''
  37 KB (5,717 words) - 12:46, 9 December 2019
• Turbulence intensity
  ...oth- and rough-wall pipe flow. Code for an example in [5] can be found in [6]. A high Reynolds number transition in the scaling has been characterized i {{reference-paper|author=[6] Basse, N.T.|year=2019|title=Python code to calculate turbulence intensity
  5 KB (661 words) - 16:24, 23 July 2022