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Problems with using Sediment Grain Size Alone Shape can affect grain-fluid interactions, but… shape is very difficult to quantify, making it problematic to account for in a mathematical relationship. Particle density – this we can deal with – today’s lecture

Problems with using Sediment Grain Size Alone

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Problems with using Sediment Grain Size Alone. Shape can affect grain-fluid interactions, but… shape is very difficult to quantify, making it problematic to account for in a mathematical relationship. Particle density – this we can deal with – today’s lecture. - PowerPoint PPT Presentation

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Page 1: Problems with using Sediment Grain Size Alone

Problems with using Sediment Grain Size Alone

Shape can affect grain-fluid interactions, but… shape is very difficult to quantify, making it problematic to account for in a mathematical relationship.

Particle density – this we can deal with – today’s lecture

Page 2: Problems with using Sediment Grain Size Alone

Sediment Grain Size - Settling Velocity

Steps in the Derivation of Stokes’ Law (on blackboard)

1. Downward directed grav. Force

2. Balanced by upward directed drag force

3. CTSV - no acceleration, so by Newton’s 2nd - the sum of the forces must =0.

4. Equate the Forces, solve for velocity.

5. Identify relationship for drag coefficient as a fcn. of Re?

6. We’re there...

Page 3: Problems with using Sediment Grain Size Alone

CD = f(Re)

Page 4: Problems with using Sediment Grain Size Alone

Why use settling velocity?

Valuable predictor of entrainment/suspension in the surf zone

Bagnold’s concept of autosuspension - if settling velocity (ws) was less than product of swash velocity (u) and beach slope (S), then settling would never occur. (see p. 55 in Komar):

And since orbital (swash) velocity, is proportional to wave height (H) and inversely proportional to wave period (T):

Dean number, considers suspension height and wave period.

ws < uS

ws <πHS

T

ws <δh

T

Page 5: Problems with using Sediment Grain Size Alone

Example

Consider a beach with an average slope of 3˚ (S = ?), an orbital velocity of 25 cm/sec, and a wave period of 10 sec.

Bagnold’s autosuspension equation would yield: ws< 1.25cm/sec (~= to 0.15 mm diameter quartz sphere)

At a suspension level of 10 cm, Dean’s relationship would yield: ws < 1 cm/sec (~= to 0.1 mm diameter quartz sphere)

Anything finer would be remain in suspension and be (eventually) washed out to sea.

Page 6: Problems with using Sediment Grain Size Alone

Entrainment of sedimentDerivation of incipient grain motion (blackboard example):

start w/ torque balance on a grain

Page 7: Problems with using Sediment Grain Size Alone

Sediment Sorting

Page 8: Problems with using Sediment Grain Size Alone

Cross Shore Sorting - Lake Michigan

Page 9: Problems with using Sediment Grain Size Alone

Cross-shore Sorting - Duck, NC (FRF)

Page 10: Problems with using Sediment Grain Size Alone

From Komar, 1998From Komar, 1998

va- very angulara – angularsa- sub-angularsr – sub-roundedr – roundedvr – very rounded

Histograms of roundness for Augite

Page 11: Problems with using Sediment Grain Size Alone

Longshore Sorting of Beach Sediments

Page 12: Problems with using Sediment Grain Size Alone

Longshore Sorting - Willard Bascom