Oceanography 540--Marine Geological Processes--Autumn Quarter 2002

Settling of Particles; Threshold of Motion

Stokes Settling

Stokes developed a analysis of the settling of spherical particles involving the balance between the net gravity force acting on the particle and the viscous drag exerted by the fluid.

The viscous drag force acting on a particle will depend on its size, rand velocity, w, and the viscosity, m, of the fluid medium:

Eq 1: terms of viscous drag

Analyzing dimensionally:

Eq 2: dimensional analysis

By inspection a=b=c=1. Without developing the hydrodynamics, the viscous drag force acting on a particle is:

Eq 3: viscous drag eqn

The net gravitational force (gravity less buoyancy) will be depend on the volume, density, r , and the acceleration of gravity, g:

Eq 4: grav force eqn

At terminal velocity, these two forces are balanced:

Eq 5: equating forces

Solving for w:

Eq 6: settling velocity

Typically Deltarho is 1500 kg m^-3 and for seawater µ is .01 kg m^-1s^-1 so:

D

w

1 meter descent

1000 meter descent

1 mm

87 cm s-1

1.15 x 100 s ~ 1 second

1.15 x 103 s ~ 19 minutes

0.1 mm

0.87 cm s-1

1.15 x 102 s ~ 2 minutes

1.15 x 105 s ~ 31 hours

0.01 mm

0.0087 cm s-1

1.15 x 104 s ~ 3 hours

1.15 x 107 s ~ 1/3 year

0.001 mm = 1 m m

0.000087 cm s-1

1.15 x 106 s ~ 12 days

1.15 x 109 s ~ 35 years

The Critical Stress

Grains forming the boundary between a fluid and a sediment bed possess a finite weight and finite coefficient of friction. When the applied shear stress is low they are not brought into motion. As applied shear stress is increased, a critical shear stress is reached at which grains will begin to move. The value of the critical stress depends primarily on the size and density of the particles and secondarily on their shape, their packing, and the cohesive forces acting between particles.

One the critical stress is just exceeded, particles will advance in the direction of flow due to irregular jumps or less commonly rolls. This mode of tranport is termed the bedload and conceptually can be thought of as being deterministic, that is the behavior of a particle once in motion is dominanted by the gravity force. As the stress is further increased, particles will also begin to be suspended in solution and subject to turbulent forces. This mode of transport is called the suspended load. Due to these two modes of transport there will be a flux of material across a plane perpendicular to the flow. Our ultimate goal is to determine this mass flux by integrating the product of the velocity profile and concentration profile.

The motion of sediment can be parameterized in a number of ways. The oldest of these is due to Hjulstrom who summarized observational data in terms of fluid velocity and grain size:

Hjulstrom

Figure 1

There is a envelope of values for small particles, contrasting unconsolidated and consolidated/cohesive sediment. This reflects the importance of interparticle forces because of the higher ratio of surface area to volume.

There are a number of variants of the Hjulstrom diagram, using grain diameter as one parameter and some measure of the stress as the other (via the quadratic stress law: u, u100 or stress itself: u*):

Modified

Figure 2

Shields first suggested a more general scaling, based on an analysis of the forces acting on particles. His analysis suggested an organization of the data based on two factors.

For non-cohesive sediments, under a wide range of experimental conditions, a boundary is found in this parameter space (entrainment factor, Reynolds number) between no motion of the sediment and active erosion of the sediment:

-----

Shields

Figure 3

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As an example consider the situation for Re=10 where (reading from Figure 3) the critical Theta is 3 x 10^-2:

Eq 9: eq 23-4

Solving each of the two equations for D:

Eq 10: eq 23-5

Equating these expressions for D:

Eq 11: eq 23-6

and solving for u*, we find:

Eq 12: eq 23-7

For grains of density 2700 g/cm^3 in water of viscosity 10-3 kg m^-1s^-1:

Eq 13: eq 23-8

That is 1.6 cm/s is the scale of the rms velocity fluctuations necessary to just begin to transport a 0.6 mm grain.


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