sedimentary structures- i

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Sedimentary structures- I

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Page 1: Sedimentary structures- I

Sedimentary structures- I

Page 2: Sedimentary structures- I

Outlines

1. A bit a brainstorming…

2. Then, some classification: how and why?

3. A huge variety of sedimentary structures

Page 3: Sedimentary structures- I

Brainstorming

What kind of sedimentary structures do you know?

Page 4: Sedimentary structures- I

Definition and Classification

1. Suspension is falling in a calm or slowly moving fluid:

Stokes’ law (spheric particles < 0.2 mm)

2. « Entrainment Flow », when FF > FG

3. Gravity flow within a calm or moving fluid

Three types of sediment deposition

Page 5: Sedimentary structures- I

Definition and Classification

In entrainment flow…

Classification based on:

• The location: internal vs.

bedding

• Physical or biological

process

Page 6: Sedimentary structures- I

Definition and Classification: cross bedding

CROSS-BEDDING is a feature that occurs at various scales,Sedimentary.Rocks are

normally deposited as horizonal layers. However, you may see very layers that are at an

angle to the horizontal. These tilted layers layers are termed cross bedding.

Page 7: Sedimentary structures- I
Page 8: Sedimentary structures- I
Page 9: Sedimentary structures- I

Definition and Classification

In entrainment flow…

A series of strongly

different structures

develop, as a function

of the mean flow

velocity (laminar,

turbulent, subcritical,

supercritical), flow

depth and grain size

of transported particles

Depth: 10-22 cm; Temperature: 10°C

Page 10: Sedimentary structures- I
Page 11: Sedimentary structures- I

Current RipplesFlow (imagined as streamlines) within the sub-viscous layer

form clusters of grains that modify the flow dynamic.

A region of boundary layer separation get formed

between the flow separation point and the flow attachment

point.

Ripples are bedformscreated by the effect of

boundary layer separation on a bed of sand.

Page 12: Sedimentary structures- I

• Adsorbed layer: at margin, fluid particles attached to solid surface (a few molecules thick).

• Boundary layer: zone of bottom-ward decreasing velocity. This contains a viscous sub-layer, a reduced turbulence zone.

Layers within a flow

Page 13: Sedimentary structures- I

Current Ripples

H: 0.5 – 3 cm

L: 10 – 20 cm (max. 60 cm)

Ripple Index: 10 (sand) – 20 (silt)

Page 14: Sedimentary structures- I

How do ripples form?

Crest

1) Sand grains roll up orsaltate up to the crest on the upstream side of the

ripple.

2) Avalanching of grains occurs on the downstream side as accumulated grains become unstable at the crest, over the maximum critical slope angle (circa 30° for sand-size grains).

Stoss sideLee side

Trough

Page 15: Sedimentary structures- I
Page 16: Sedimentary structures- I

Current Ripples constrains

• Require moderate velocity within the viscous sub-layer under hydraulically smoothed conditions.

• Independent from the water-depth.

• The dominant grain size is finer than 0.6 mm; no lower grain-size limit but sediment must be non-cohesive.

• Can be up to 40 mm high and the wavelengths range up to 500 mm. Wavelength/height is usually around 10 and 40.

Page 17: Sedimentary structures- I

Current RipplesCurrent flow causes downstream migration of the ripple and all its components, creating sand layers at the angle of the slope.

These layers are called cross-laminae and form a specificsedimentary structure named cross-lamination.

3 types of ripple crest

Page 18: Sedimentary structures- I

Current Ripples

Page 19: Sedimentary structures- I

A huge variety of sedimentary structures

Current ripples

Page 20: Sedimentary structures- I

Current Ripples

First ripples (low flow velocity): parallel, long and regular crests

Increase in velocity: sinuous, then linguoid crests

Page 21: Sedimentary structures- I

Cross-laminationMainly dependent by the flow velocity/duration and the ripple shape.

Planar cross-laminationfrom straight ripples.

Trough cross-laminationfrom sinous to isolated

Ripples.

Page 22: Sedimentary structures- I

Planar cross-lamination

Page 23: Sedimentary structures- I

Trough cross-lamination

Page 24: Sedimentary structures- I

Trough to planar cross-stratification

Page 25: Sedimentary structures- I

Deep-water current ripples

Page 26: Sedimentary structures- I

Terminology for cross-stratified beds

Page 27: Sedimentary structures- I
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Climbing ripplesEach ripple migrate up the stoss side of the ripple form in front,

when the sand-addition rate ≥ migration rate.

Upward decreasing of sedimentation rate

Deposition occurs on both the stoss and the lee side.

Indicators of high sedimentation rate.

Page 29: Sedimentary structures- I

Climbing ripples

Page 30: Sedimentary structures- I

Kurt Grimm, UBC

Cojan & Renard, 2000

A huge variety of sedimentary structures

Current ripples Transport > input

Transport = input

Transport < input

current

Page 31: Sedimentary structures- I

Subaqueous Dunes• Require higher flow velocities to appear and do not form at all in

sediments < 0.1 mm.

• Range of wavelengths: 600 mm to hundreds of meters.

• Range of height: few centimeters to more than 10 meters.

• Appear in river channels, deltas and shallow-water environments with quite strong and sustained flows.

There is a relationship between flow depth and

the dimension of the dunes

Page 32: Sedimentary structures- I

• Originate in one of two ways:

– From ripples at flows ~ 50 cm/sec

– From a plane bed of sediment coarser than

~ 0.8f

A huge variety of sedimentary structures

Sand Waves: Dunes

Both dunes and ripples can occur when the grain-size ranges between 0.1-0.4

mm.

Page 33: Sedimentary structures- I

Current velocity: 40 to 150 cm/s, grain size > 0.15 mm (2.8 Φ)

H = up to several 10s meters

L = up to several 100s meters

Index = ca. 5 (fine sand) - 50

(coarse sand)

Oblique stratification, often

tangential at the base of the

structure (bottomset)

www.nasm.si.edu

A huge variety of sedimentary structures

Dunes

Page 34: Sedimentary structures- I

Ripples vs. Dunes

Clear separation (no overlap) in both wavelength and bedform height between ripples and subaqueous dunes.

The two bedforms are not the same!

Dunes seem to be more dependent by water depht because are generated by large-scale turbolence within the whole flow.

Page 35: Sedimentary structures- I
Page 36: Sedimentary structures- I

Cross-beddingMainly dependent by the flow velocity/duration and shape.

Planar cross-beddingfrom straight dunes.

Trough cross-beddingfrom sinuous to isolated

dunes.

Page 37: Sedimentary structures- I

Plane beds

• A bed with active sediment transport but no obvious topography.

• Occurs in two different physical settings

– All sediments coarser than circa 0.4 mm near the initiation of motion (lower regime) (Still not so not clear process)

– Sediments of any grain size at very high velocity (upper regime) (planar configuration is associated with the planing or flattening of the bed)

Page 38: Sedimentary structures- I

Dune

Upper plane bed

Trias, Nevada

A huge variety of sedimentary structures

Entrainment current, upper flow regime: Upper Plane Bed

Flow velocity between 60 and 180 cm/s

Upper flow regime: supercritical fluid and Fr>1

Formation of Upper Plane Beds, with motion of sediments by traction or

saltation, inducing the development of sorting lineations

Page 39: Sedimentary structures- I

Internal Structures in Plane Beds• The internal structures produced are a series of

thin, parallel and sub-horizontal laminae (parallel or planar lamination).

• Internally, the laminae can comprise alternations of slightly finer and coarser sediments.

Page 40: Sedimentary structures- I

Current velocity > 120 cm/s:

formation of antidunes,

bedform in phase with surface

waves

Occurrence: tidal current and

flooding events

A huge variety of sedimentary structures

Entrainment current, upper flow regime: Antidunes

current

Tidal channel, California

Antidunes are commonly observed in small streams that flow across beaches

into the ocean. Flume studies have shown that they can also occur in

submarine environments beneath density flows like turbidity currents.

Page 41: Sedimentary structures- I

Cojan & Renard, 2000

A huge variety of sedimentary structures

Entrainment current, upper flow regime: Antidunes

Antidunes: slow

height, length (L) up

to 5 m

Index: between 7

and > 100, usually

high

A: laminae on the

lee side (low

angle slope)

B: laminae wrapping the

entire antidune

C: slightly inclined laminae

on the stoss side: upstream

motion of the antidune

water surface

water surface

water surface

The water surface is

strongly in phase with the

bed. A train of

symmetrical surface

waves is usually

indicative of the presence

of antidunes.

Page 42: Sedimentary structures- I

A huge variety of sedimentary structures

Entrainment current, upper flow regime

Very high current velocity: Chutes and pools, mainly an erosive

feature

Chutes: high flow regime inducing upper plane beds

Pool: downstream, a thicker package of sediment corresponds to

an hydraulic threshold

Page 43: Sedimentary structures- I

Bedforms stability diagram

Very slow flow: parallel, planar beds, no mouvement,

deposition by settling of suspension: lower plane bed

Flow velocity between 5-60 cm/sec: small ripples for

sediments < 0.8 mm (0.3 ϕ)

Page 44: Sedimentary structures- I
Page 45: Sedimentary structures- I

WavesAn ocean wave is an oscillatory motion of the sea surface

caused by wind and involving transfer of energy between particles but no mass transport.

Page 46: Sedimentary structures- I

Wave Parameters– Wave crest

– Wave trough

– Wave height

– Wave length

– Wave Amplitude

– Wave period (time interval between arrival of consecutive crests at a

stationary point).

Amplitude

Page 47: Sedimentary structures- I

Motion of Water Particles beneath Waves

The oscillatory motion generates a circular pathway.

With increasing depth internal friction reduces the motion and the effect of the

surface waves dies out.

The depth to which surface waves affect a water body is

referred to as the

wave base

Page 48: Sedimentary structures- I

Interaction of waves and shoreline

Page 49: Sedimentary structures- I

Motion of Water Particles beneath Waves

Page 50: Sedimentary structures- I

A huge variety of sedimentary structures

Wave ripples and orbital velocity

Vertical decrease in velocity

from water surface to the wave

base

Wave base = L/2, where L =

wave length

Page 51: Sedimentary structures- I

Wave ripple cross-laminationIn cross-section wave ripples are generally symmetrical in profile,

laminae within each ripple dip in both directions and are overlapping.

Wave ripples can form in any non-cohesive sediment and are principally seen in coarse silts and sand. If the wave energy is high enough wave

ripples can form in granules and pebbles

Page 52: Sedimentary structures- I

Wave ripples

Several features are common in wave-ripple lamination. Foresets on

the parallel-to-flow face may dip in opposite directions, sometimes in

adjacent ripples, sometimes within a single ripple. Laminae may be

interleaved at an individual ripple crest.

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Wave ripples

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Modern wave ripples

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Current ripples vs. Wave ripples

Page 57: Sedimentary structures- I

A huge variety of sedimentary structures

Mixed ripples

Page 58: Sedimentary structures- I

Cojan & Renard, 2000

« Hummock »« Swale »

A huge variety of sedimentary structures

Hummocky cross stratifications (HCS)

HCS: undulating set of cross laminae both concave up

(swales) and convex up (hummocks)

storm- generated wave causing strong oscillatory flows and/or

combined flow. Erosion of the seabed into Hummocks and

swales.Swales and hummocks are superimposed on top of

each others

Erosive base, low angle (10-15°), rippled top

Page 59: Sedimentary structures- I

A huge variety of sedimentary structures

Hummocky cross stratifications (HCS)

Page 60: Sedimentary structures- I

Summary

1. Storms with oscillatory flows and unidirectional currents

2. Erosive base with angle usually <10°3. Laminae parallels to the base

4. Changes from concave up to convex up

5. Crests not straigth but more curved

6. Coarse silt to fine-medium sands

Page 61: Sedimentary structures- I

Ferron Sandstone, Gentile Wash, Utah

A huge variety of sedimentary structures

Hummocky cross stratifications (HCS)

Page 62: Sedimentary structures- I

Ashgill, Ordovician, Anti-Atlas, between Merzouga and Erfoud

A huge variety of sedimentary structures

Hummocky cross stratifications (HCS)

Page 63: Sedimentary structures- I

Ashgill, Ordovician, Anti-Atlas, between Merzouga and Erfoud

A huge variety of sedimentary structures

Hummocky cross stratifications (HCS)

Page 64: Sedimentary structures- I
Page 65: Sedimentary structures- I

Cojan & Renard, 2000

HCS

Upper plane bed

A huge variety of sedimentary structures

Hummocky cross stratifications (HCS)

Cross-stratifications

Mud

Bioturbation

Conglomerate

Groove, flutes

« Tempestite »

Linked to a rapid

increase of the orbital

velocity of wavesFAIR WEATHER

STORM

WEATHER

IDEAL SEQUENCE

Page 66: Sedimentary structures- I
Page 67: Sedimentary structures- I

Tempestite, Carboniferous, east of Tineghir, Anti-Atlas, Morocco

A huge variety of sedimentary structures

Hummocky cross stratifications (HCS)

Page 68: Sedimentary structures- I

Tides

Tides are formed by the gravitational attraction of teh moon and sun on teh Earth

combined with the centrifugal force caused by the movement of the Earth around

the center of mass of teh Earth-moon system

Semi diurnal or diurnal tidal cycles

Neap-spring tidal cycles

Annual tidal cycles

Page 69: Sedimentary structures- I

Tides

Page 70: Sedimentary structures- I
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Tidal sedimentation

Herringbone cross bedding

Page 72: Sedimentary structures- I

Tidal sedimentation

Page 73: Sedimentary structures- I

A huge variety of sedimentary structures

Current ripples in tidal environments

FLASER BEDDING

LENTICULAR BEDDING

WAVY BEDDING

Page 74: Sedimentary structures- I

Lenticular and wavy lamination in dark mudstone and pale sandstone

Page 75: Sedimentary structures- I

Entrainment flow - Synthesis