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Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin
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Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Dec 21, 2015

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Page 1: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Prolate Granular Materials

Connected Networks, Jammed States, and Force Fluctuations

By: Kenneth DesmondAdvisor: Dr. Scott Franklin

Page 2: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

What We are Studying

• We study long thin rods and their ability to jam.

• We Characterize these rods by their aspect ratio, the ratio between the rod length and the rod diameter (L/d)

Page 3: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

A Jammed State

•3” rods with an aspect ratio of 48

•An example of a jammed state without the aid of supportive walls

Page 4: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Setup

• Aspect Ratio (L/d) ranges from 8 to 48 with the diameter of the rods (d) being 1/16” or 1/8”

• The tube diameter ranges from 1.25” to 4” with a ball diameter of ¼”

•As the ball moves throw a granular medium the force sensor relays the information to the computer as voltage data

•The voltage is then converted into a force readout, based on earlier calibration

Page 5: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

How Hard Must You Pull?

Page 6: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Stick-slip Motion

• Linearly increasing force when ball is at rest followed by a very short burst of motion

• Fluctuations are due to granular rearrangement

Page 7: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Solid-body Motion

• Force fluctuations are due to stick-slip motion on the surface of the walls

Page 8: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Transition Region

• Transition region marked by small moments of solid-body like motion followed by particle rearrangements that bring the ball to stop

Page 9: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Pile Phase Space

• Transition from stick-slip to solid-body motion is gradual not sudden

Page 10: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Pile Phase Space

• We’ll focus on the closed box since it spans all the different phases

Page 11: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

FFT Spectrum

• Ordinary granular materials scale as f -2 (Albert et al.)

• Dry friction scales as f -1

Page 12: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.
Page 13: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.
Page 14: Prolate Granular Materials Connected Networks, Jammed States, and Force Fluctuations By: Kenneth Desmond Advisor: Dr. Scott Franklin.

Conclusion

• This system can exhibit three different phases

• These phases depend mostly on aspect ratio and normalized tube diameter

• Also the pile can form force chains that result in forces must greater then the pile weight with jam states being very strong and rigid