CFD Online Logo CFD Online URL
www.cfd-online.com
[Sponsors]
Home > Forums > Software User Forums > ANSYS > FLUENT

WheelSeperation--viscous models and wall functions

Register Blogs Community New Posts Updated Threads Search

Reply
 
LinkBack Thread Tools Search this Thread Display Modes
Old   March 17, 2006, 09:26
Default WheelSeperation--viscous models and wall functions
  #1
Mark G
Guest
 
Posts: n/a
Hiya, hopefully I can get some bloody useful answers because I am stumped!

My project is to investigate endplate design and the interation with the wheel (modelled as static is this case)

As I have just self taught in a short period of time, I do not know how to create 3d boundary layers in gambit, so used size functions to create a coarse mesh in fluent and adapt both "velocity gradients" and Wall Plus values.

With speeds of 50m/s (reynolds numbers of 2e6+) I was expecting the flow to separate on the wheel (with 1,000,000 grid meshes), however it doesnt look like it does seperate from post anylsis. (coeffiecents of drag are similar to the invicid case)

What viscous model is best for high pressure gradient bluff bodies, with seperated flows. I have wall plus values to within 300 (which is recommended for resolving BL)...so it should work :S ????

ANY advice, much appreciated!!

Mark
  Reply With Quote

Reply


Posting Rules
You may not post new threads
You may not post replies
You may not post attachments
You may not edit your posts

BB code is On
Smilies are On
[IMG] code is On
HTML code is Off
Trackbacks are Off
Pingbacks are On
Refbacks are On


Similar Threads
Thread Thread Starter Forum Replies Last Post
Natural convection in a closed domain STILL NEEDING help! Yr0gErG FLUENT 4 December 2, 2019 01:04
Water subcooled boiling Attesz CFX 7 January 5, 2013 04:32
Two-Layer Models and Wall Functions sdwijeya Siemens 0 June 18, 2010 16:25
mixing length models and wall functions tiz Main CFD Forum 1 April 2, 2007 17:38
Wall functions? Pr Main CFD Forum 7 April 8, 2004 07:15


All times are GMT -4. The time now is 01:11.