Gallery

The Cavitation Christmas Tree

Though it resembles a stylized Christmas tree, this dark silhouette is a momentary structure sculpted by a collapsing cavitation bubble. As the bubble implodes near a particle‑laden oil‑coated free surface, it drives a powerful free surface jet toward air. The cavitation bubble propels and stretches the thin oil film, entraining particles and pulling the interface upward into a tall, tapering column that branches into fine ligaments and droplets—forming the “branches” and “ornaments” of the tree. This image freezes an event that unfolds over only microseconds, revealing how bubble dynamics interact with complex, contaminated interfaces. By varying particle concentration, oil properties, and bubble position, my research explores how such cavitation events control interfacial deformation, erosion, and material transport in natural and engineered flows. Here, an extreme multiphase phenomenon briefly takes on a familiar holiday shape, turning high‑speed fluid mechanics into a “Cavitation Christmas Tree.”
A series of shape changes in lipid vesicle

Hollow Droplets Meet a Thin Film

Hollow droplets, comprising a liquid shell encapsulating a gas bubble, exhibit core–shell morphologies with impact dynamics fundamentally distinct from those of single-phase droplets. These droplets play pivotal roles in both natural and advanced engineering processes, including aerosol generation, 3D printing, and thermal spray coating. Using high-speed imaging, we reveal the full sequence of hollow droplet impact on a thin liquid  lm, including splashing and counter-jet formation, governed by the intricate interplay between droplet impact dynamics and internal bubbles. By introducing combinations of modi ed non-dimensional numbers, we establish a uni ed scaling for the mechanics underlying these phenomena. This previously unexplored regime o ers new insights into  uid fragmentation pathways and provides a quantitative framework for interpreting and controlling splash phenomena across disciplines.
A series of shape changes in lipid vesicle

Surprising Dynamics of Hollow Droplet Impact on Solid Surfaces

Droplet impact on solid surfaces plays a critical role in both natural and industrial contexts. Hollow droplets, composed of a gas bubble encapsulated by a liquid shell, exhibit a distinct core–shell structure that imparts unique physical and chemical properties compared to single-phase droplets. This morphology is prevalent in various practical processes, including raindrop impacts on the Earth's surface, the deposition of hollow spherical particles during thermal spray coating, and bubble-bursting aerosol transfer from the ocean. In many of these scenarios, the liquid shell can behave viscoelastically when the phase contains polymers, surfactants, or biological macromolecules commonly found in natural and industrial fluids. We are investigating this phenomenon to better understand and control the spreading and bouncing behavior of such droplets.
A series of shape changes in lipid vesicle

Beads-on-a-String Structured Jets Produced by Bursting Bubbles

Bubbles rising through marine columns can scavenge contaminants due to flow mechanics and physical chemistry, including biocontaminants such as microbial extracellular polymeric substances (highly hydrated polymers that are mainly composed of polysaccharides, proteins, and DNA). These biocontaminants introduce intricate three-dimensional polymeric networks, forming a viscoelastic layer at the bubbles’ surfaces. When such a contaminated bubble with a viscoelastic coating reaches the air-liquid interface and bursts, it produces a distinct “beads-on-a-string” pattern during the formation of the resulting Worthington jet, and ejects these biocontaminants as small drops into the atmosphere. Therefore, understanding the bursting dynamics of contaminated bubbles is crucial, as it plays a key role in the airborne transmission of biocontaminants within marine ecosystems.
A series of shape changes in lipid vesicle

Collective oil-coated bubble bursting

Collective oil-coated bubble bursting tends to generate jet drops with smaller sizes, greater overall numbers of drops and higher droplet ejection heights than bare bubble bursting at either clean or surfactant-laden aqueous surfaces, as shown in the figure. The droplet size is one key parameter in predicting its residence time and transport, as small droplets are more easily lifted by turbulent eddies. These contaminant-laden drops smaller than 10 μm in diameter could pose a higher risk of pollutant spread or infection as they can penetrate farther into the respiratory tract than larger drops. The oil-coated bubbles in our experiments could typify the ubiquitous contaminated or compound bubbles in the oceans, and bubble-bursting jet drop particles have been found to contain different compositions with stronger ice nucleating abilities than film drop particles. Our discovery may therefore improve chemical transport modelling related to bubble-driven fluxes in the context of sea spray aerosols.

A series of shape changes in lipid vesicle

Bubble cap rupture

Film drops produced from bursting bubble on the sea surface microlayer can be enriched with micro-organisms or bacteria and transported to the atmosphere. Once a bubble is created in a bulk solution, the bubble rises with small particulates to the surface and forms a spherical cap at the surface. The shape of the cap remains constant before the bubble spontaneously ruptures, often fragmenting into film droplets as shown in the picture. Investigating bubble bursting behavior paves the way to predict the transmission of small particulates, such as microplastics, bacteria, or even viruses from sea surface and other forms of water sources.
A series of shape changes in lipid vesicle

Bubble bursting jets at an oil-covered aqueous surface

When a bubble bursts and produces a jet at an oil-covered aqueous interface, the oil layer greatly influences the hydrodynamic process and modify the drop size and velocity. After the bubble bursts, the oil layer spreads to the bottom and damps the capillary waves simultaneously. As a result, a faster and thinner jet emerges with a more viscous and thicker oil layer. This study advances our understanding of the interplay between bubbles and contaminated surfaces.

Multi-vesicular Vesicles

This video highlights different sealing behavior when a multivesicular vesicle (a vesicle containing many smaller vesicles) bursts. These two vesicles were placed in the same hypotonic solution. Both vesicles swell due to the osmotic imbalance, eventually bursting under the increasing strain. Once the strain is released, each vesicle will spontaneously reseal. In one case the sealing occurs cleanly, while in the second, there is a tangle of lipid protrusions on the surface. Understanding what drives clean and tangled resealing could add insight into physiologically relevant membrane behavior as well as pointing the way to more precise artificial drug delivery systems.

Transformations

A sequence of spontaneous shape transformations of a giant unilaminar vesicle. It is nearly 5 microns across, about the size of a single red blood cell. Thermal oscillations of the membrane drives the changes seen in this image. This models the shape energetics of red blood cells, a feature crucial for transporting oxygen throughout the body.
A series of shape changes in lipid vesicle

Nanoparticle Galaxy 

When an aqueous suspension of nanoparticles consisted of polymers is exposed to air, the adsorption and aggregation of those nanoparticles form a glaxy-like structure at the air-water interface. This top-view image was captured by a confocal microscope. The light came from the fluorescent emission of dye molecules encapsulated in the nanoparticles. The area shown in the image is approximately 2.5 by 2.0 mm
A series of shape changes in lipid vesicle

Blooming Flowers

When a small quantity of oil (a linear alkane) is deposited on the surface of an aqueous solution of detergent molecules, the oil spreads into a thin film and then ruptures. Multiple holes appear in the film, and the oil ridges around the growing holes transform into intricate petal-like patterns in a process that is similar to the breakup of a liquid filament into droplets. These films with growing holes are like gardens of blooming interfacial flowers. This top-view image was captured with a standard digital SLR camera and macro lens. The rainbow colored patterns are created by the interference of light from an LED panel and they reveal the structure of the oil film. The area shown in the image is approximately 1.7 by 1.3 cm.
A series of shape changes in lipid vesicle

Dancing Fringes

When you look at a small bubble at the interface, you will see dancing interference fringes induced by marginal regeneration. The dance of the interference fringes, which represents iso-thickness lines of the bubble film, results from the convection motion developed over the bubble cap. This motion consists of the periodic emission of spaced plumes from the edge of the cap. Once they have left the pinching zone, the thinner plumes rise because of their positive buoyancy with respect to the surrounding thicker portions of the film. The area shown in the image is approximately 2.0 by 0.5 cm.