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Physics 313: Lecture 2 Wednesday, 8/27/08
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Comments to the Class Get in habit of reading Announcements link of 313 web page before each class. Lecture files change within a few days after lecture. Extra meeting this week to discuss homework, related background material? Topics: Finish canonical example of a pattern-forming nonequilibrium system, R and Rc. Discussion of examples: what are the interesting scientific questions? When are natural systems high-dimensional and so need new approaches?
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Rayleigh-Benard Convection: Canonical Pattern-Forming System
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Cloud Street: Clouds in Convecting Layer
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How Patterns Observed? Shadowgraphy
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Buoyancy Force Versus Dissipation From Viscosity and Thermal Conduction
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Dimensionless “Driving” or Bifurcation Parameter: the Rayleigh Number R
Nonequilibrium systems characterized by one or more dimensionless parameters, of which one is often a ratio of “driving” to “dissipation”. Starting from thermal equilibrium, nothing happens until driving parameter exceeds critical value Rc ~ 1708. Rayleigh number, Prandtl number, Reynolds number famous parameters in fluid dynamics. Worked example of where dimensionless parameters come from.
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Example Using the Rayleigh Number
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Worked Example: Where Dimensionless Parameters Like R Come from
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Convection Patterns Unique patterns? What sets the length scale?
Unique patterns? What sets the length scale? Unique wavelength? Rotation speed?
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Chaotic Convection Patterns
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Discussion: Are These Spatiotemporal Chaotic Patterns Different?
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Effect of Pattern Formation on Transport
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Almost Periodicity Common Feature:Defects
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Crispation Patterns (Faraday Waves)
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