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184        Process Modelling and Simulation with Finite Element Methods

                      Surface: temperature (T)  Arrow:  velocity [u,v]   103






                      06


                      04
                      03
                      02
                      01
                       -2
                  Figure 5.1  Temperature and velocity fields for the first mode with Ra=-l .

          zero.  As Ra increases in magnitude, dissipative effects become relatively weaker
          than  the buoyancy,  so the internal  gravity waves become  long-lived  structures.
          Haarlemmer  and  Zimmerman  [6] used  wave  tank  studies  to  characterize  the
          mixing  properties  of  large  amplitude  internal  gravity  waves  that  are  initially
          seeded  in  a  concentration  stratified  fluid.   They  review  the  geophysical
          importance of this transport mechanism.


          5.2.2  Heating from below
          Heating from below changes the nature of the dynamical problem.  As we found
          when  heating  from  above,  complex  eigenvalues,  equivalent  to  damped
          propagating  waves were found.  This is because  vertical convection  is opposed
          by the stable stratification of light fluid over heavy fluid, but gravity waves can
          propagate  horizontally.  If  a patch  of  fluid  is  displaced  vertically,  it oscillates
          around its equilibrium position and can propagate right or left without loss of the
          original energy in an inviscid fluid.  Lord Rayleigh [7] showed that when heating
          from below,  the  state  of  the  fluid  at rest  is unconditionally  stable.  The same
          argument  works  in reverse  to  show that  when  heating  from below,  an inviscid
          fluid  cannot remain  at rest.  But  the  state of  rest  can persist  to high  Rayleigh
          number  in  a  viscous  fluid  with  heat  conduction  - the  dissipative  mechanisms
          oppose the  overturning  motion  until  the  heating  differential  is  strong  enough.
          The theory  of  Reid  and  Harris  [8] describes  the  critical  Rayleigh  number  for
          cells  with  upper  and  lower  rigid  boundaries  occurs  at  Ra,=1708  with  a
          wavenumber of 3.117.  The motion that is most unstable above Ra,  is supposed
          to be the onset of stationary cells in 3-D, and convection rolls in 2-D.  Since the
          linear operator,  and thus its FEM approximation  as in (5.3), is self-adjoint, then
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