Encyclopaedia Index
TITLE : A whirlpool in a pond
BY : CHAM User Support Team - Dr S V Zhubrin  
FOR : Demonstration case 
DATE : November, 2000
PHOENICS Version : 3.3.1 
PHYSICAL SITUATION :
  - Steady free surface turbulent flow of water recirculating
      under influence of bottom stresses and internal blockage
      in an open pond.
  
 - The task is to simulate the velocity distribution along with
      free water surface elevation.
 
ASSUMPTIONS :
  - Hydrostatic pressure
  
 - Incompressible, homogeneous fluid
  
 - Non-varying bed topography
  
 - Shallow flow: small vertical scale relative to horizontal
  
 - Well-mixed-in-depth flow: uniform vertical distributions
 
SHALLOW-WATER MODELLING:
     - Two-dimensional treatment of three-dimensional flows with
         the local depth calculated as part of solution.
     
 - Depth-averaged version of Navier-Stokes equations;
     
 - Equations solved by analogy to isentropic, compressible gas flow:
         
             - Density, RHO1= Water density*Depth
             
 - Pressure, P1= g*RHO1**2/(2*water density), i.e.
             
 - RHO1=sqrt(2*water density*P1/g)
             
 - U1, V1 = depth-averaged velocity components.
         
 
 
NUMERICAL DETAILS :
  - Cartesian computational grid.
  
 - Effective-viscosity turbulence model
  
 - Boundary conditions:
      
          -  Fixed fluxes for inlet mass/momentum and
          
 -  Fixed-pressure outlet (equivalent to fixed depth).
          
 -  Bottom stresses are calculated by relating them
               to the velocities via Chezy's coefficient.
     
 
 
RESULTS :
    The plots show the distribution of velocity and water depth (free
    surface elevation) within the pond.
Pictures are as follows :
THE IMPLEMENTATION
   All model settings have been made in VR-Editor of PHOENICS 3.3.1.
   The relationships for bottom stresses are introduced via  PLANT menu.
   The relevant Q1 file  can be inspectedby clicking
   here.
   svz