SAND DYNAMICS AND RIPPLE DYNAMICS
SAND DYNAMICS
Here we focus on the description and quantification of the dynamics of a
single particle moving in a turbulent, wall-bounded, oscillatory
flow. In simple words, this is a single sand grain moving in water which
is being forced back and forth over a plane and rigid surface by the
passage, say, of waves.
Our tool is a spectral-element Navier Stokes solver, with which we
perform numerical simulations of the three dimensional situation. This
requires the use of computers such as my beowulf cluster and others
similar to these which are housed at the MCS division of Argonne
National Laboratory.
Two types of experiments are being performed:
1) Fixed particle. In this case the particle is constrained to stay at
one location while the fluid moves around it.
2) Moving particle. The particle is allowed to move in response to the
flow around it. The particles two degrees of freedom are translation
and rotation.
What we are interested in doing is in characterizing in great detail the
lift and drag of the particle as a function of the Reynolds number, the
gap between the particle and the wall, and a parameter that is related
to the frequency of the flow. We do this numerically because this
experiment has been mostly inaccessible to wet-lab experimental means
in the range of parameters that we are interested in.
Some Animations
This is a collaborative effort with Dr. Paul Fischer and
Dr. Gary Leaf, from the MCS Division at Argonne National
Laboratory
Sand Ripples:
We are using an annular sediment dynamics tank to experimentally probe
the generation and stability of sand ripples that are generated by the
action of a steady shearing force on a bed of loose sediment. The
tank is about 1 meter in diameter and has a width of about 2.5 cm.
The shear is provided by a powerful motor, which drives a rotor over the water/sediment-filled tank.
The topography along the ring is captured by a sequence of video
cameras , which are capable of seeing the whole 360 degrees of the
tank at once. The system is driven as well as captured by a
computer/controller combination , using
labview and pcrunner.
The sediment will form patterns under
steady or oscillatory shearing.
Movies that show the sediment in motion will be posted here shortly. For
now, you'll have to settle for
a low-tech
short animation. The rotor is the
object moving above, the ripples are entirely made up of sand. The whole
thing is in water. The bars precess in the direction of the rotor shear.
What is striking, as is evident from the space-time plots is that there are
bursts of activity in the bars where the bar locally accelerates in the
process losing sediment.
This is a collaborative effort with Profs. Raymond Goldstein and
Adriana Pesci, from the Physics department, University of Arizona.
Last modified: 9 March 2001