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Granular Materials. R. Behringer Duke University Durham, NC, USA. Outline. Overview What’s a granular material? Numbers, sizes and scales Granular phases Features of granular phases Why study granular materials? Special Phenomena Open challenges—what we don’t know.
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Granular Materials R. Behringer Duke University Durham, NC, USA
Outline • Overview • What’s a granular material? • Numbers, sizes and scales • Granular phases • Features of granular phases • Why study granular materials? • Special Phenomena • Open challenges—what we don’t know
Issues/ideas for granular gases • Kinetic theory • Hydrodynamics • Clustering and collapse • Simulations • Experiments
Issues/ideas for dense granular systems • Friction and dilatancy • Force chains • Janssen model • Constant flow from a hopper • Forces under sandpiles • Texture
Models for static force transmission • Lattice models: Q-model, 3-leg, elastic • Continuum limits of LM’s • Classical continuum models • Summary of predictions
Experimental tests of force transmission • Order/disorder • Friction • Vector nature of force transmission • Textured systems • So where do we stand?
Force fluctuations in dense systems • Force chains • Fragility • Anisotropy
Transitions • Jamming • Percolation • Relation to other phenomena—e.g. glasses • Clustering (see gases) • Fluidization • Subharmonic Instabilities (shaken systems) • Stick-slip
“Classical” systems • Shaking (convection, waves…) • Avalanches • Rotating flows • Hoppers and bunkers • Shearing • Mixing and segregation
Special techniques • Discrete element models (DEM or MD) • Lattice models • Special experimental techniques • NMR • Photoelasticity • “Carbon paper”
What is a granular material? • Large number of individual solid particles • Classical interactions between particles • Inter-particle forces only during contact • Interaction forces are dissipative • Friction, restitutional losses from collisions • Interaction forces are dissipative • A-thermal—kBT << Etypical ~ mgd • Other effects from surrounding fluid, charging may occur
Numbers, Sizes and Scales • Sizes: 1m < d < 100m– powders -100m < d , 0.5cm—grains d > 0.5 cm—pebbles, rocks, boulders… • Size range of phenomena—packed powers (pills– mm to mm • A box of cereal—mm to 10 cm • Grains in a silo—mm to 10’s of m • Sahara desert—mm to many km • Rings of Saturn, intergalactic dust clouds—up to 1020m
Granular Phases and Statistical Properties • Qualitative similarity of fluid, gas and solid states for granular and molecular systems • Difficult question: how do granular phase changes occur? • Open question: what are the statistical properties of granular systems? • Caveat: No true thermodynamic temperature—far from equilibrium • Various possible granular ‘temperatures’ proposed
Distinguishing properties of phases • Solids resist shear • Fluids are viscous, i.e. shear stresses scale with the velocity gradients • Gases are also viscous, have lower densities than fluids, and have Maxwell- Boltzmann-like distributions for velocities
Properties of granular gases • Characterized by pair-wise grain collisions • Kinetic theory works reasonably well • Velocity distributions are modified M-B • Gases can only persist with continuous energy input • Subject to clustering instability • Models (may) show granular collapse
Properties of granular solids • Persistent contacts (contrast to collisional picture for gases) • Dense slow flows or static configurations • Force chains carry most of the force • Force chains lead to strong spatio-temporal fluctuations • Interlocking of grains leads to jamming, yield stress, dilation on shearing
Solids, continued • Dilation under shear (Reynolds) • Grains interact via friction (Coulomb) Note frictional indeterminacy history dependence • Persistent contacts may limit sampling of phase space • Conventionally modeled as continuum • Strong fluctuations raise questions of appropriate continuum limit
Granular ‘phase’ transistions • Clustering in gases • Elastic to plastic (semi- ‘fluid’) in dense systems—jamming • Jamming and fragility • Note: gravity typically compacts flows—many states not easily accessible on earth
Do granular materials flow like water? • Example: sand flowing from a hopper: • Mass flow, M, independent of fill height • M ~ Da a ~ 2.5 to 3.0 • Why—force chains, jamming…
Note: method of pouring matters for the final heap (History dependence)
Simple argument to predict flow rate • M = rV D2 • V ~ (gD)1/2 • M ~ D5/2.
Why study granular materials? • Fundamental statistical and dynamical challenges • Related to broader class of systems • e.g. foams, colloids, glasses • Important applications: • Coal and grain handling • Chemical processing • Pharmaceuticals • Xerography • Mixing • Avalanche phenomena • Earthquakes and mudslides
Interesting phenomena • Pattern formation • In shaken systems • Hopper flows • Mixing/segregation • Clustering—granular gases • Avalanches • Rotating flows • Granular convection • Jamming/unjamming
Applications • Significant contribution to economy (~1$ trillion per year (?) – in US) • Granular industrial facilities operate below design—large financial losses result • Large losses due to avalanches and mudslides
Friction: Granular and otherwise • Two parallel/intertwined concepts: • ‘Ordinary’ friction • Granular friction • Both referenced to Coulomb’s original work • Mohr-Coulomb friction.
C. A. Coulomb, Acad. Roy. Sci. Mem. Phys. Divers Savants7, 343 (1773)
Example of Reynolds dilation in before and after images from a shear experiment
Microscopic origin of stresses, Fabric, Anisotropy • Fabric tensor • Microscopic origin of stress tensor • Shape effects–
Aligned force chains/contacts lead to texture and anisotropy
Force chains, Spatio-temporal fluctuations • What happens when dense materials deform? • Strong spatio-temporal fluctuations • Examples: hopper, 2d shear, sound. • Length scale/correlation questions