Presentation is loading. Please wait.

Presentation is loading. Please wait.

Physics 313: Lecture 2 Wednesday, 8/27/08

Similar presentations


Presentation on theme: "Physics 313: Lecture 2 Wednesday, 8/27/08"— Presentation transcript:

1 Physics 313: Lecture 2 Wednesday, 8/27/08

2 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?

3 Rayleigh-Benard Convection: Canonical Pattern-Forming System

4 Cloud Street: Clouds in Convecting Layer

5 How Patterns Observed? Shadowgraphy

6 Buoyancy Force Versus Dissipation From Viscosity and Thermal Conduction

7 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.

8 Example Using the Rayleigh Number

9 Worked Example: Where Dimensionless Parameters Like R Come from

10 Convection Patterns Unique patterns? What sets the length scale?
Unique patterns? What sets the length scale? Unique wavelength? Rotation speed?

11 Chaotic Convection Patterns

12 Discussion: Are These Spatiotemporal Chaotic Patterns Different?

13 Effect of Pattern Formation on Transport

14 Almost Periodicity Common Feature:Defects

15 Crispation Patterns (Faraday Waves)


Download ppt "Physics 313: Lecture 2 Wednesday, 8/27/08"

Similar presentations


Ads by Google