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    3.2 Sub-group 1.2 in which one differential equation is used
  
3.2.1 Prandtl energy with prescribed length scale
    
    (a) The effective viscosity
    
    Prandtl, in 1945, generalised his hypothesis regarding the effective
    viscosity of a turbulent fluid, giving it the form:
        EV = const1 * LM * SQRT (KE)
    where: LM is a prescribed length scale, which may vary from place to
                                                             place; and
           KE is the kinetic energy of the turbulent motion, deducible
              from the velocity fluctuations in the three directions
              u', v' and w'
    Thus:
           KE = 0.5 * ( u'**2 + v'**2 + w'**2 )
    (b) The source of information about KE
    Prandtl postulated that the turbulence energy obeyed a transport
    equation of the form:
       term                        representing
      D(KE)/Dt                    time-dependence & convective transport
    = div( const2*EV* grad(KE))   turbulent diffusion
    + EV*(vel_grad)**2            kinetic-energy generation by shear
    - const3*k**1.5/LM            kinetic-energy disipation
    Thus:
-  The turbulent-viscosity concept was still used.
 -  Comparison of the formula for EV in Prandtl's mixing-length and
   energy models (see section 3.1.3 above) shows the connexion:
       KE =LM* vel_grad * LM
 - Whereas the PMLM requires only one empirical constant, the
       Prandtl energy model (PEM) requires two more.
 
    (c) Advantages and disadvantages
-  The PEM does allow for convection and diffusion of turbulence
       into regions where there is zero local generation. It is
       therefore inherently capable of simulating some phenomena
       more realistically than can the PML model.
 -  On the other hand it is no more capable than is the PMLM of
       determining for itself what the value of LM should be; and
       knowledge is almost totally absent for re-circulating and 3D
       flows.
 -  Consequently it has been little used, and is considered useful
       only close to walls, where the length scale is fairly well
       known.
 
    (d) Activation in PHOENICS
   
    In order to activate the PEM in PHOENICS, the PIL command TURMOD
    needs to be inserted in the Q1 file with the argument KLMODL.
    TURMOD(KLMODL) is equivalent to the following PIL commands:
      SOLVE(KE)
      ENUT=GRND3;KELIN=0
      PATCH(KESOURCE,PHASEM,1,NX,1,NY,1,NZ,1,LSTEP)
      COVAL(KESOURCE,KE,GRND4,GRND4);GENK=T
    Then the choice of LM formula is made by the setting of further
    parameters such as EL1, EL1A, etc (see the 
Encyclopaedia entry EL1).
wbs