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Published byCharles Sparks Modified over 11 years ago
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The example of Rayleigh-Benard convection
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Pattern-forming instabilities: The example of Rayleigh-Benard convection
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Rayleigh-Benard convection. Boussinesq approximation, incompressible flow
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Rayleigh-Benard convection. Boussinesq approximation, incompressible flow
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Rayleigh-Benard convection. Boussinesq approximation, incompressible flow
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Rayleigh-Benard convection. Boussinesq approximation, incompressible flow
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Rayleigh-Benard convection: static state
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Rayleigh-Benard convection
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Rayleigh-Benard convection: static state with pure conduction Fixed temperature b.c.
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Rayleigh-Benard convection. Boussinesq approximation, incompressible flow
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Rayleigh-Benard convection: non dimensional formulation
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Rayleigh-Benard convection Important parameters: R = g D 3 T 2 -T 1 ) / = a = L D
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Rayleigh-Benard convection. If R < R crit conduction T(x,y,z,t)=T cond (z)=T 2 - z (u,v,w)=(0,0,0) If R > R crit convection T= T cond + (u,v,w) non zero
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Rayleigh-Benard convection. Linear stability analysis
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2D Rayleigh-Benard convection (non dimensional formulation)
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2D Rayleigh-Benard convection
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2D Rayleigh-Benard convection: Linearization around the static state
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2D Rayleigh-Benard convection: Linearization around the static state
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2D Rayleigh-Benard convection: Linearization around the static state
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2D Rayleigh-Benard convection: Linearization around the static state
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2D Rayleigh-Benard convection: Linearization around the static state
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Rayleigh-Benard convection. Linear stability analysis
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2D Rayleigh-Benard convection: Threshold to convection
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Rayleigh-Benard convection: above R crit, convective motion occurs. This takes the form of parallel rolls
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The convective rolls saturate the instability
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Amplitude expansion
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Amplitude expansion: first order
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Amplitude expansion: second order
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Amplitude expansion: third order
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Amplitude expansion: third order The Fredhom alternative: eliminate the secular term and get a solvability condition: The Landau equation
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Amplitude expansion: third order The Landau equation with real coefficients
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Pitchfork bifurcation at R 2 =0
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Stability of the rolls: Busse balloon
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Stability of the rolls
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