Coulomb’s Model

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Coulomb’s Model θ r θ max Δθ Identified two characteristic Angles: θ r , Angle of Repose θ max , Maximum Stable Angle Additional material treated as a single entity.

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Coulomb’s Model. Identified two characteristic Angles: θ r , Angle of Repose θ max , Maximum Stable Angle. Additional material treated as a single entity. Δθ. θ max. θ r. Strengths and Weaknesses of the Coulomb Model. Gives a mathematical model for avalanches. - PowerPoint PPT Presentation

Transcript of Coulomb’s Model

Page 1: Coulomb’s Model

Coulomb’s Model

θr

θmaxΔθ

Identified two characteristic Angles:

•θr, Angle of Repose•θmax, Maximum Stable Angle

Additional material treated as a single entity.

Page 2: Coulomb’s Model

Strengths and Weaknesses of the Coulomb Model

• Gives a mathematical model for avalanches.

• θmax and θr are observable in piles with many particles.

• Only applicable to large-scale observations. (Doesn’t account well for unique surface properties.)

Page 3: Coulomb’s Model

Bak-Tang-Wiesenfield Cellular Automaton Model

A highly simplified model that lends itself well to computer simulation.

Represents a pile by a grid of cells: each cell may contain a grain.

Grains are added to the pileone at a time.

Page 4: Coulomb’s Model

Bak-Tang-Wiesenfield Cellular Automaton Model

Simulates avalanches with two rules:

•The difference in height between adjacent columns must not exceed two cells.•If adding a grain would break this rule, grains are moved in pairs until an acceptable state is reached.

Page 5: Coulomb’s Model

Uses of the Bak-Tang-Wiesenfield Model

• Offers a good computational model. Easy to generalize in 3-d.

• Predicts a relation that gives the frequency of avalanches of a given size.

• Offers a way to predict how a pile will respond to certain disturbances.

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A Common Experimental Setup

Avalanches

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Tracking Individual Particles:

Individual particles behave very differently from the collective avalanche.

Used Positron-Emission Particle Tracking to follow the movements of individual particles in a rotating drum.

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Tracking Individual Particles:

Avalanches do not move particles from top to bottom in one step.

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Wet Granular Materials

• Added oil to glass beads in a rotating drum.

• Amount of oil small compared to amount of beads.

• Changes frictional forces, adds cohesive forces.

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Wet Granular Materials:Change in Maximum Angle

Percent Liquid Content

Ang

le (

Deg

rees

)

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References

• Duran, J. (2000). Sands, powders, and grains. New York: Springer.

• Lim, S. Y., Davidson, J. F., Forster, R. N., Parker, D. J., Scott, D. M., & Seville, J. K. (2003). Avalanching of granular material in a horizontal slowly rotating cylinder: PEPT studies. Powder Technology, 25‑30.

• Tegzes, P., Schiffer, P., & Vicsek, T. (2002, August). Avalanche Dynamics in Wet Granular Materials. Physical Review Letters, 89(9), 094301‑1 ‑ 094301‑4.