Granular Flows 1 Lecture 8: Geomorphology Comparing a sand dune to a sand pile -- what are the effects of scale? Geomorpology: study of landforms Aeolian processes: sand dunes Hillslope processes: avalanches & rock slides 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 2 Aeolian processes – booming sand dunes From: National Geographic, Death Valley DVD, 2009 3 Micro- versus macroscale? Processes: Micro: creep, saltation, suspension Meso: avalanches, ripples, separation Macro: dune building, migration 4 Aeolian sand transport Forces due to the wind: Aerodynamic forces: 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 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 5 Micro processes (1) Saltation trajectories & speed: Ballistic paths for grains 0.1- 0.3 mm Chain reaction: multiple particles Wind speed: fluid threshold: initiate saltation lifting & splashing impact threshold: halt saltation stops saltation Threshold wind speed: V ~ 1.5 m/s for 0.1 mm particles From: R.A. Bagnold, The Geographical Journal, 1937 6 Micro processes (2) Suspension trajectories & speed: Carried high by turbulence Suspended in air for grains < 0.06 mm Dust storms: soil erosion, moves great distances 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) 7 Meso processes (1) – sand flux Sand flux q depends on: Shear velocity u & threshold ut Grain diameter d, density, etc Scaling of sand flux q: Behavior in steady-state (saturated): far away from fluid threshold: cubic (Bagnold): close to threshold: not well understood Unsteady behavior: numerical simulations saturation flux qs, saturation length scale ls From: Wind-blown sand, by H.J. Herrmann 8 Meso processes (2) – small-scale features Sand ripple formation: bedform by surface roughness Unevenness (random or saltation-induced) perpetuates Creation of saltation shadow creation of ripple fast propagation (~ 1 cm/minute), wavelength: ~ 10 – 20 cm height: ~ 1 cm Granule ripple formation: miniature barchanoid ridges Creation of jams of coarser grains via surface creep 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 9 Macro processes (1) Formation, evolution & migration of dunes: Coupled (iterative) set of equations between: 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 If a dune moves shape-invariantly (h(x,y) = c): 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 10 Macro processes (2) Migration velocity and height: 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 11 Macro processes (3) Dune morphology depends on: 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 12 Macro processes (4) Entire systems of barchan dunes: 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 13 Macro processes (5) – aeolian vs aqueous Comparison migration & Re-number: Re p Aeolian dunes: Migration speed: cd ~ 25m/year = 8.10-7 m/s Uchar = 8 m/s, = 15.68.10-6, D=0.002 Particle Rep ~ 1000 UDp Aqueous dunes: 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 14 Applications – aqueous dunes Initial conditions: Observed: Ripple formation Slipface creation & migration Bifurcation: splitting and merging dunes Small dune catches up, or runs away 15 Applications – dune migration (1) Ground penetrating radar: Antenna: electromagnetic waves traverse entire dune in small steps Change in electrical conductivity Analysis of reflected waves 16 Applications– dune migration (2) From: N.M. Vriend, M.L. Hunt, R.W. Clayton, GJI, 2012 17 Applications – booming sand dunes (1) Music from the desert An array of geophones: wave propagation in plane configuration Microphone recording: Eureka Dunes, Death Valley NP 18 Applications – booming sand dunes (2) Source: shearing of grains in the avalanche Constructive interference in a waveguide: Amplification of sound Setting the frequency Frequency of sound: nc1 fn , n 1,2,3,... 2 2 1/ 2 2 H (1 c1 / c2 ) for c0 = c2 and critical refraction 19 Applications - quicksand Quicksand: sand, clay & salt water Sensitive to small stress variations: low stress: viscosity slowly changes high stress: viscosity drops magnitudes liquid behavior reduces friction first liquefies, then collapses Sinking mechanism: 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 20 Applications – sand castles Sandcastles: perfect composition? Stiffness of sand: dry: hardly supports own weight wet: forms liquid bridges (ideal: 1%) too wet: bridges form large liquid pockets Stability of wet sand columns: 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 21 Hillslope processes – avalanches (1) Snow avalanches: Erosion & deposition Grain processes: mass balance changes segregation levee formation Velocity evolution: start-up steady-state run-out 22 Hillslope processes – avalanches (2) 23 Hillslope processes – avalanches (3) 24
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