This page gives an overview of projects in the lab. For equipment and facilities, use this link.
Granular materials consist of discrete macroscopic particles. The interactions between particles are solely due to classical interactions, such as normal contact forces and frictional forces between grains. Generally, when considering a real granular system there are also interactions with the container walls and gravity to consider. We are interested in the flows of real granular systems, and we study them with both experiment and simulation.
One system we study is the gravity-driven flow of grains through a opening. We study this partially out of pure interest, but this system is analogous to traffic flowing through a bottleneck, crowds exiting through a doorway, or blood cells moving through a constricted vessel. This geometry is typically called a silo or hopper. When the opening is smaller than some critical size, the likelihood of a clog grows astronomically. When the opening is above some critical size, the material will appear to flow freely. There is even an empirical law that describes the flow rate as a function of opening size. However, it is still not clear how this law comes about from the microscopic interactions of grains, or that the law is even that good. (For one, a common scaling argument that produces this law is actually unphysical, for two, the flow is not really continuous.) Further, it is thought that perhaps the clogging transition may be something like a phase transition, and we should seek evidence to support or refute this hypothesis.
By acquiring high-speed, high resolution videos of hopper flow we are able to understand how the individual particle motions and rearrangements create the bulk flow. For some experiments, we are able to extract the forces between particles by using photoelastic particles as our granular material. (In our simulations, we always have this information.) We are especially interested in collective measurements of motion, such as plasticity (i.e. non-affine motion) and cooperativity (i.e. dynamical heterogeneities). We also are studying the topology and evolution of the contact network during flow and clogging events.
We also study flows of avalanching granular materials. When a granular material is tilted beyond its angle of repose, the system may avalanche. Alternatively, avalanches may occur intermittently when granular material is continuously added to a pile of grains. Our current experiment investigates dry granular avalanches of hollow glass spheres. Thus these spheres mimic sand in their contact interactions, but weigh less than solid spheres. This effectively reduces the force of gravity in the system, and so the material is an analog for sand on a reduced gravity planet. Indeed, some gully features on Mars that are often attributed to liquid flows may be under a false comparison to systems on Earth, which has higher gravity than Mars. It is possible that some of these features are actually due to dry granular flows.
Hopper Flow
Force Chains
Contact Network
Angle of Repose
While grains can only passively respond to forces, other objects can actively respond to forces and other stimuli. This small shift in microscopic behavior can induce flow in a system, even without some external driving force. (A classic example of such a flow can be seen in a school of fish.) We are interested in how collective system dynamics change as a function of the object's activity, the interactions between objects, and the density of the system.
One such system we are studying is Chlamydomonas reinhardtii, a single cell form of algae. The individual alga are about 10 microns in size, and swim with two flagella. We are currently studying how their dynamics change with concentration (with no imposed flow). We will eventually subject them to imposed flow in microfluidic channels to study the shear rheology of concentrated samples.
We are also studying swarms of robots to look their collective dynamics. The robots in the still image do not have active feedback mechanisms, but do have a preferred direction of motion and are anisotropic. The arrows are fixed onto their back so we can track orientation in addition to position.
Chlamy
Robots!
In addition to granular systems, we also study colloidal suspensions. These systems are quite similar to granular systems, except the grain size is smaller (typically 1-20 um for our projects), and they are suspended in fluid. Thus to even see the grains we need a microscope. To flow these suspensions we use microfluidic devices, which we generally design. For some experiments, we can make channels in our lab (possibly with help from the Makerspace), and for some experiments we outsource the silicon mold patterning on wafers (and from these can mold the actual PDMS devices in the lab).
One project of interest involves pressure-driven flows of colloid/polymer mixtures. In the absence of flow, the colloids and polymers are well-mixed. But under the right flow conditions, these flows are shown to produce chains of colloids. We are currently working to maximize this effect.
We also have a great interest in using microfluidics for rheological characterization of materials. A pressure-driven flow through a straight channel yields a stress profile that is exactly known. By taking high speed and high resolution video of the flow, the shear rate profile can be measured. This yields a stress vs shear rate curve, as would be measured in a conventional rheometer. The advantages of microfluidics over conventional rheometry include extremely low sample consumption, high attainable shear rates, and direct measurement of the microstructure.
Further, a cross-slot microfluidic channel can be used to produce strong extensional flows. We are currently using such devices to measure the deformability of emulsion droplets, and eventually will study cells. The advantages over other deformation techniques (such as micropipette aspiration and AFM) include high throughput (= good statistics), low sample consumption, noncontact/noninvasive/nonlethal probing of cell mechanics, and measurement of deformation with high time and spatial resolution.
Pressure-Driven Shear Flow
Extensional Flow Device
Real Device: 50 micron square cross section