Physics%20of%20Convection - PowerPoint PPT Presentation

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Physics%20of%20Convection

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Physics of Convection Motivation: Convection is the engine that turns heat into motion. Examples from Meteorology, Oceanography and Solid Earth Geophysics – PowerPoint PPT presentation

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Title: Physics%20of%20Convection


1
Physics of Convection
  • Motivation
  • Convection is the engine that turns heat
    into
  • motion.
  • Examples from Meteorology, Oceanography and
    Solid Earth Geophysics
  • Basic Equations, stationary convection,
    time-dependence, influence of mechanical inertia,
    volumetric effects ..

2
Atmospheric phenomena - Large scale
Headly-cells gt horizontal transport -
Thermals which result in Cumulus and
Cumulo-Nimbus clouds gt vertical transport from
surface to the Tropospause - characteristic
Inertia Coriolis forces
3
Oceanographic processes - Large scale water
exchange Arctics-Tropics - El Nino - Double
Diffusive Convection (e.g. Polynoyas) -
characteristic density determined by temp.
salinity
4
Solid Earth Planets - Convection in the
Earth mantle - MHD - convection in the Earth
core generating mag. field - Magama chambers
-characteristic no inertia(mantle),
multicomponent
5
Basic scenario
6
Non dimensional equation for time-dependent
convection in a constant-property Boussinesq
fluid
with
7
scaled by
where
8
How to solve the equations
- Problem coupled system i.e v depends on T
and T
depends on v - Analytic
-linearize equation -see if
infinitesimal disturbance gets amplified gt
critical value for Ra 600, independent of Pr
- first instablities have a roll pattern -
other patterns also exist like square patter,
hexagon pattern, cross-roll pattern ... - no
extrema principal
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12
Higher Rayleigh numbers
13
Numerical Simulation
Solve the equations by a numerical method (e.g.
finite element, fd, spectral, fv...) variables
are available at any point in space high
viscosity, rotation, spherical geometry are
easily realized - long 3D timeseries are still
expensive - small-scale features can not be
resolved
14
Rayleigh
Prandtl
15
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18
Time-dependent convection
- onset of time-dependence from boundary layer
theory - At high Pr. large scale coherent
structures with superimposed boundarie layer
instabilities (BLI's) which are drifting with
the main flow - with incrasing Ra the strength
of the major up- and downwelling decreases
19
Influence of the Prandtl number
- The Prandtl number measures the ratio of
mechanical inertia - Typical values are Pr(Water)
7., Pr(Air) 0.7 Pr(EarthMantle) 1024
, Pr(OuterCore) 0.04
20
Pr 0.025
Pr0.7
Pr100.
21
Temperature - Depth profiles for different
Prandtl numbers
22
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24
Percentage of vertical vorticity
25
The influence of volumetric heating
- Decay of U, Th, and K lead to a volumetric
heating of the Earth mantle
26
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28
Volumetric heating leads to - break of symmetry
between up-and down wellings - 'passive'
upwellings with no distinct temperature
signature - cylindrical shape of down-wellings -
no large scale coherent structures - no different
scales for the downwelling
29
Temperature and Pressure dependent viscosity
  • Investigations of material properties for the
    Earth?s mantle indicate a strong dependence on
    both temperature and pressure.

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31
Thermochemical Convection
The density is not only a function of the
temperature but also of a second component
32
Examples of 'fingers'
Experiment sugar-salt system
Numerical simulation
33
Layer formation
34
Effects observed - motion can be observed in
hydrostatic stable systems - potential energy is
converted in kinematic energy - formation of
well mixed convection layers - dynamics
strongly dependent on the diffusivity difference
between the two components
35
Effects of Rotation
36
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38
What has not been talked about ... - effect of
pressure dependent thermal expansivity -
non-Newtonian rehologie - effects of
non-Cartesian geometry - effects due to
rotation -.....
39
Conclusion
  • Convection is THE important transport mechanism
    in geophysical systems
  • for moderate heat differences systems exhibit a
    stationary flow
  • depending on the magnitude of the Prandtl number
    the flows are becoming time-dependent
  • for low-Pr. flow the velocity fields have a
    strong toroidal component
  • effect like volumetric heating break the symmetry
    between up- and down-wellings
  • most geophysical flows are in a regime where the
    flows are chaotic
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