Title: Sediment transport by coherent structures in a horizontal open channel flow experiment
1Sediment transport by coherent structures in a
horizontal open channel flow experiment
- Lorentz Workshop 2006
- Leiden
W.A. Breugem and W.S.J. Uijttewaal
Environmental Fluid Mechanics
2Overview
- Introduction
- Sediment transport in open channel flow
- Experimental setup
- Results
- Concentration profile development
- Drift velocity histogram
- Spatial drift velocity structure
- Conclusions
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
3Sediment transport in open channel flow
- Focus
- Suspended sediment, hence outer region
- Dilute flow (for now)
g
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
4Flume setup
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
5Particle requirements
- Comparison with DNS
- Be suspended at Re 10,000 (i.e. u/ws 5)
- dp/lk lt 1 (assumption in Maxey Riley eq.)
- Rep lt 1 (assumption in Maxey Riley eq.)
- Experimental procedure
- Phase discrimination dp gt3 dtracer
- Materials
- Tracer hollow glass (dtracer 15 mm)
- Sediment polystyrene (dp 375 mm, rp/rf1.035)
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
6Instantaneous result
- Re 500
- Polystyrene particles
- Flow from left to right
- 0.8 ucl subtracted
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
7Concentration profiles
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
8Drift velocity
- Drift from average Stokes drag force (Simonin et
al., 1993) - I.e. The drift velocity is the deviation of the
average fluid velocity seen by a particle. - Vertical momentum equation
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
9Drift velocity profiles
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
10Drift velocity PDF (Predominantly settling, x16h)
y/h 0.55
vT0.2u
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
11Drift velocity, deviation from random sampling
(predominantly settling, x 16 h)
- More particles in Q4, less in Q2
- Downgoing particles in Q4
- Upgoing particles in Q1 and Q2
vT0.2u
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
12Drift velocity histogram (fully developed, x 75
h)
y/h 0.55
vT0.2u
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
13Drift velocity, deviation from random sampling
(fully developed, x 75h)
vT0.2u
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
14Conceptual picture of particle transport
Fully developed situation
Settling situation
Velocity Quadrants
u
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
15Spatial structure
- The spatial structure is studied with conditional
averages - Conditional averages are determined with Linear
Stochastic Estimation (LSE). - With LSE, conditional averages can be calculated
from two-point correlations. - A vortex head (rotating with the mean shear) at
three different reference heights is used as
condition. - Vortex identification is done with swirling
strength.
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
16Fluid flow structure (vortex near the wall)
Q3
Q2
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
17Drift velocity structure (vortex near the wall)
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
18Fluid flow structure (vortex at 0.5 h)
Q2
Q3
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
19Drift velocity structure (vortex at 0.5 h)
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
20Conceptual model (hairpin vortex)
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
21Settling situation
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
22Conceptual picture fully developed situation
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
23Spatial relation between Q2 Q3
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
24Spatial relation between Q2 Q4
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion
25Conclusion
- The increased concentration in either fast
(settling situation) or slow (fully developed
situation) flow structures, cause the mean
particle velocity to differ from the mean fluid
velocity. - Downward transport occurs in sweeps (Q4) and
inward interactions (Q3), upward transport in
ejections. - In predominantly settling, particles are found
less in ejections (Q2) and more often in sweeps
(Q4). - In fully developed situation, particles are found
less sweeps, and more often in both ejections and
inward interactions. This is due to the alignment
of several hairpin vortices.
Introduction - Experimental setup Drift
velocity - Flow structures - Conclusion