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7/29/2019 G433 (2010) review of sed structures_v2.pdf
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G433Review of sedimentary structures
September 1 and 8, 2010
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Fluid Parameters
The three main parameters that determinethe stable bedformin unidirectional flowconditions are:
grain sizeflow velocityflow depth
Several other parameters are equallyimportant, though for most pure fluid flows onEarth, these parameters can be assumed tobe constant. They include:
m = fluid viscosityrf = fluid densityrs = grain density
g = gravitational constant
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Cohesive vs. non-cohesive sediments
Hjulstrom Diagram
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Bedformphase diagram and hysteresis
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2-D vs. 3-D structures
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Secondary flow created by bed roughness
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Aggradation
vs. migration ofbedforms
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Examples of
climbing bedforms(unidirectional
ripples)
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DunesDunes are similar to ripples, but dynamically distinct.
Dune wavelengths commonly range from 0.6 m tohundreds of meters; heights range from 0.05 -10.0 m.
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Upper plane bed flow: intensive sediment transport over a flat bed
Parting Lineation
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flow migration
Antidunes occur in flows with sufficiently high Froude numbers. AntidunesTypically migrates upstream and shows little asymmetry. The water surface is
strongly in phase with the bed. Commonly seen as train of symmetrical surface waves.
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Shoot and pool structures:Trains ofcyclic steps occur in verysteep flows with supercritical Froude numbers. The steps are delineated
by hydraulic jumps (immediately downstream of which the flow issubcritical).
flowhydraulic jump
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Bedforms in cohesive sediments
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Subaqueous bedforms in cohesive sediments: flutes and toolmarks, including bounce, skip, groove, and chevron marks
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Gutter castssubaqueous, usually associated with storms
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Shrinkage cracks
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Incomplete, non-orthogonal, Ordovician Eureka Quartzite, W. Utah
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Shrinkage cracks
subaerial desiccation
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Bedforms generated by surface waves Surface waves transfer little mass but considerable energy
Surface waves define orbitals in fluid that have decreasingdiameter with depth
Depth below which orbital diameters = 0 is termed wavebase
Deep water waves do not reach bottom
Shallow water waves do reach bottom; orbitals reachingbottom create a shear stress that oscillates back and forth aswaves pass overhead
With sufficient shear stress, sediment grains will move,creating bedforms
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Wave orbitalsdeep water wavesshallow water waves
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Movement of sediment by wave orbitals
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Unidirectional, combined flow, and
oscillatory bedforms
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Wave ripples
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Hummocky cross-stratification (HCS)
Occurs in fine- to medium-grained sand
Produced by combined flow
Typically occurs below fair weather wavebase by larger
waves produced during storms
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Physical features characteristic of HCS
hummocks (concave up features) and swales (concave downfeatures)
psuedo-parallel laminations within hummocks and swales
(although laminae may thicken into swales and thin overhummocks)
low angle (
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HCS
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Eolian Dunes
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Sediment dynamics
on dunes
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Grain flow depositsGrain fall depositsWind ripple deposits
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Sediment
gravity flows
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Turbidity currents:
particles are kept aloft in the body of the flow by turbulent suspension
density of flow greater than that of ambient fluidboth high density and low density turbidity currents exist
Turbidite in flume
Flume turbidite 2
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Turbidites
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Liquified flows:
very concentrated dispersions of grains in fluidusually result from shock of granular sediment (e.g. seismic shock)grains kept in suspension by fluid pore pressure and from upward movement ofexpelled fluid
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Grain flows:
characterized by grain-grain collisions.
Little reduction of friction occurs in such flows, so they can only occur onsteep slopes where the angle of initial yield has been exceeded.
Debris flows:
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Debris flows:
slurry like flows in which large particles (up to boulders) are set in a fine-grained matrix
matrix has yield strength which helps support grains during flowmatrix serves to lubricate grain irregularities so debris flows may occur onvery gentle slopes
Debris flo deposits
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Debris flow deposits