Acoustic emission of sand

Granular Flows
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Lecture 8: Geomorphology
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Comparing a sand dune to a sand pile
-- what are the effects of scale?
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Geomorpology: study of landforms
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Aeolian processes: sand dunes
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Hillslope processes: avalanches & rock slides
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Micro, meso & macroscale: from grain to dune
Singing & booming sand dunes
Quicksand & sandcastles
Erosion and deposition
Not in this lecture: fluvial, glacial, tectonic & volcanic processes
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Aeolian processes – booming sand dunes
From: National Geographic, Death Valley DVD, 2009
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Micro- versus macroscale?
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Processes:
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Micro: creep, saltation, suspension
Meso: avalanches, ripples, separation
Macro: dune building, migration
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Aeolian sand transport
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Forces due to the wind:
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Aerodynamic forces:
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drag force (due to Newton’s turbulent drag):
lift force (due to pressure difference):
ratio on Earth: c = 0.85
Gravitational forces (grain’s weight):
Momentum balance:
Shield’s number: tangential force - resisting grain movement
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fluid shear stress ta
reduced density in air ’
packing of grains  internal angle of friction: 
shape and sorting of grains 
From: Wind-blown sand, by H.J. Herrmann
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Micro processes (1)
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Saltation trajectories & speed:
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Ballistic paths for grains 0.1- 0.3 mm
Chain reaction: multiple particles
Wind speed:
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fluid threshold: initiate saltation
 lifting & splashing
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impact threshold: halt saltation
 stops saltation
Threshold wind speed:
 V ~ 1.5 m/s for 0.1 mm particles
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From: R.A. Bagnold, The Geographical Journal, 1937
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Micro processes (2)
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Suspension trajectories & speed:
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Carried high by turbulence
Suspended in air for grains < 0.06 mm
Dust storms: soil erosion, moves great distances
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Dust storms: downdraft, moves laterally as a density current
Elevations of 2500 m, speeds of 200 m/s
From: NASA SeaWIFS Project (http://www.earthds.info/pdfs/EDS_16.PDF)
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Meso processes (1) – sand flux
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Sand flux q depends on:
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Shear velocity u & threshold ut
Grain diameter d, density, etc
Scaling of sand flux q:
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Behavior in steady-state (saturated):
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far away from fluid threshold: cubic (Bagnold):
close to threshold: not well understood
Unsteady behavior: numerical simulations
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saturation flux qs, saturation length scale ls
From: Wind-blown sand, by H.J. Herrmann
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Meso processes (2) – small-scale features
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Sand ripple formation: bedform by surface roughness
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Unevenness (random or saltation-induced) perpetuates
Creation of saltation shadow  creation of ripple
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fast propagation (~ 1 cm/minute),
wavelength: ~ 10 – 20 cm
height: ~ 1 cm
Granule ripple formation: miniature barchanoid ridges
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Creation of jams of coarser grains via surface creep
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slow growth and propagation speed,
 exist for decades
wavelength: ~ 2 – 6 m
height: ~ 12.5 – 60 cm
From: R.P. Sharp, Journal of Geology, 1963 & A.J. Parsons, 1994
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Macro processes (1)
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Formation, evolution & migration of dunes:
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Coupled (iterative) set of equations between:
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shear stress: from perturbations across a hill h(x,y)
sand flux: from the shear velocity & shear stress
height of the dune: from the sand flux
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If a dune moves shape-invariantly (h(x,y) = c):
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migration velocity vd is inversely related to height h
large dunes move slowly
small dunes move fast
minimum size dune: ~ 1.5 m
 due to competition between saturation length and separation bubble
From: Wind-blown sand, by H.J. Herrmann
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Macro processes (2)
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Migration velocity and height:
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Connection between aeolian and aquaous dune formation?
Bedforms
on aeolian
barchan
dunes
Aeolian barchan dunes
Aqueous
barchan
dunes
From: Charru et al., Ann. Review of Fluid Mech., 2013
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Macro processes (3)
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Dune morphology depends on:
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Amount of available sand
Wind variability
Unidirectional winds,
increasing sand supply:
Barchan dunes
Barchanoid ridge
Transverse dunes
Star dunes
Reversing dunes
Complex wind regime,
variable sand supply:
Linear dunes
From: McKee, A study of global sand seas, 1979
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Macro processes (4)
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Entire systems of barchan dunes:
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Small barchan dune catches up with a large one:
Swallowing
Breeding
Increasing
height
small dune
Budding
Solitary
behavior
From: O. Duran et al., Phys. Rev E Stat Nonlin Soft Matter Phys, 2005
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Macro processes (5) – aeolian vs aqueous
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Comparison migration & Re-number: Re p 
Aeolian dunes:
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Migration speed:
cd ~ 25m/year = 8.10-7 m/s
Uchar = 8 m/s,  = 15.68.10-6,
D=0.002
Particle Rep ~ 1000
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UDp
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Aqueous dunes:
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Migration speed:
cd ~ 20cm/10min = 3.10-4 m/s
Uchar = 0.4 m/s,  = 1.004.10-6,
D=0.002
Particle Rep = ~ 800
2D aqueous dune
migration in a slit
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Applications – aqueous dunes
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Initial conditions:
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Observed:
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Ripple formation
Slipface creation & migration
Bifurcation: splitting and merging dunes
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Small dune catches up, or runs away
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Applications – dune migration (1)
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Ground penetrating radar:
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Antenna: electromagnetic waves
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traverse entire dune in small steps
Change in electrical conductivity
Analysis of reflected waves
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Applications– dune migration (2)
From: N.M. Vriend, M.L. Hunt, R.W. Clayton, GJI, 2012
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Applications – booming sand dunes (1)
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Music from the desert
An array of geophones:
wave propagation in
plane configuration
Microphone recording: Eureka
Dunes, Death Valley NP
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Applications – booming sand dunes (2)
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Source: shearing of grains in the avalanche
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Constructive interference in a waveguide:
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Amplification of sound
Setting the frequency
Frequency of sound:
nc1
fn 
, n  1,2,3,...
2
2 1/ 2
2 H (1  c1 / c2 )
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for c0 = c2 and critical refraction
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Applications - quicksand
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Quicksand: sand, clay & salt water
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Sensitive to small stress variations:
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low stress: viscosity slowly changes
high stress: viscosity drops magnitudes
 liquid behavior  reduces friction
first liquefies, then collapses
Sinking mechanism:
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trapping: liquefaction and sedimentation
 water and sand separates in fractions
 apparent viscosity increases
untrapping: add water to liquefy compacted sand
alternatively: low density humans prevents complete submersion!
From: Bonn et al., Nature, 2005
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Applications – sand castles
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Sandcastles: perfect composition?
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Stiffness of sand:
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dry: hardly supports own weight
wet: forms liquid bridges (ideal: 1%)
too wet: bridges form large liquid pockets
Stability of wet sand columns:
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elastic buckling under own weight
critical height:
 column of R = 20 cm  hcrit = 2.5 m
increase height: compaction or density 
 use hydrophobic sand: water  air
From: Bonn et al., Nature, 2005, Moller & Bonn, EPL, 2007
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Hillslope processes – avalanches (1)
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Snow avalanches:
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Erosion & deposition
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Grain processes:
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mass balance changes
segregation
levee formation
Velocity evolution:
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start-up
steady-state
run-out
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Hillslope processes – avalanches (2)
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Hillslope processes – avalanches (3)
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