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The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Fluid Dynamics with Erosion

Brandon LloydCOMP 259May 2003

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Overview

• Sediment transport in open channels­ Bed-load transport­ Suspensed transport

• Sediment transport models• Model used for this project• Implementation issues• Future work

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Sediment Transport

• Bed-load transport: sliding, rolling, saltating

• Suspended transport: sediment moves through the fluid

Sediment

Suspension

Bed-load

Bed

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Bed-load transport

Once the forces actingon particles are strongenough to intiate motion…

… particles slide, roll, and saltate down the river bed at a steady rate.

Figure from Chanson, p. 180

Figure from Chanson, p. 200

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Suspended Transport

Suspension occurs here

• Particles entrained at the bed-load layer

• Transported by convection, diffusion, and turbulence

Figure from Chanson, p. 200

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Sediment Transport Models

• Difficult problem – most models are empirical.

• Usually make simplifying assumptions about flow.

• Many different formulas exist.

Table from Chanson, p. 198

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

My Model

• Simplified version of model used in [Haupt et al. 1999]

• Transport occurs above critical velocity.

• Fluid has a transport capacity related to velocity.

• Concentration of sediment relative to capacity determines change in terrain

height :

porosity :

ionconcentratsediment :

constants:

velocityfall:

velocitycritical :

velocityfluid :

erosion

accretion

1

,

0

0

2

2,

2

21

h

P

c

C

w

v

v

qc

qc

)P)(q(c t

h

w

vvCqwCv

s

i

s

c,s

ss

ss

ssbed

s

scssc,s

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Implementation Issues

• Semi-Lagrangian advection causes mass loss in the presence of eddies.

• What to do at boundaries?

zero concentration

backward tracing doesnot see wall mass loss.

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Implementation Issues

• Semi-Lagrangian advection causes mass loss in the presence of eddies.

• What to do at boundaries?

Recycle concentration(limits the time-step)

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Results

• Nice swirls of sediment with erosion and deposition at interactive rates (on a fast machine .)

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

Future Work

• Add bed-load transport• Add instability based on slope• Add variable material properties• Fix spikes and improve robustness• Better handling of velocities near

heightfield.• Experiment with and compare different

fluid/advection models• Add a free surface• Implement on GPU

The UNIVERSITY of NORTH CAROLINA at CHAPEL HILL

References

CHANSON, H. 1999. The Hydraulics of Open Channel Flow: An Introduction. Arnold.

HAUPT, B. J., SEIDOV, D. AND STATTEGGER, K. 1999. SEDLOB and PATLOB: Two numerical tools for modeling climatically forced sediment and water volume transport in large ocean basins. In Computerized Modeling of Sedimentary Systems. Springer-Verlag, Berlin.

WU, W., RODI, W. AND THOMAS, W. 2000. 3D numerial modeling of flow and sediment transport in open channels. Journal of Hydraulic Engineering, 4-15.


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