2013 Image Gallery

Image Descriptions 2013

Compound Droplets on a Fiber

Floriane Weyer, Laurent Dreesen, Nicolas Vandewalle
GRASP
University of Liège, Belgium

Compound Droplets on a FiberThe picture shows two compound droplets on a horizontal fiber. They are made of an oil drop containing a pure (blue, on the left) or a soapy (red, on the right) water droplet.

The compound droplets are of great importance in fiber-based microfluidics since they prevent evaporation and contamination. Depending on the nature of the inner droplet, the behavior of the system is different. For pure water, the inner droplet forms a spherical cap whereas, for soapy water, the droplet spreads inside the oil drop and a quadruple contact line is formed. The position of the droplets on the fiber depends on the balance between capillary and gravity forces. When the gravity forces prevail over the capillary forces, the droplets fall off the fiber. The picture shows the form adopted by the droplets when they are close to the detachment. The nature of the inner droplet influences the shape of the compound drop which is more elongated for pure water than for soapy water.

F.Weyer is financially supported by an FNRS grant. This work is also supported by the FRFC 2.4505.12.

Abstract

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Reporters may freely use this image. Credit F.Weyer, L. Dreesen and N. Vandewalle, University of Liège.

Contact Information
N.Vandewalle
GRASP
University of Liège
Physics department B5
Allée du 6 Août, 17
University of Liège
B-4000 Liège
BELGIUM

Bubbles in Complex Microgeometries

Martin Sauzade, Thomas Cubaud
Stony Brook University

Bubbles in Complex MicrogeometriesMultiphase flows in confined geometries can exhibit a variety of intriguing morphologies. At the small scale, the unique balance of forces produces flow patterns that are typically governed by viscous and capillary effects. While surface tension tends to minimize interfacial area with bubbles having spherical shape, viscous laminar flows can also strongly deform bubbles in velocity fields set with the channel geometry. Here, the deformation of capillary surfaces is accentuated with the use of a highly viscous carrier fluid (viscosity: 1,000 cS) and the presence of circular cavities along a square microchannel (h = 250 um) for smoothly modulating flow velocity. In such viscous-dominated regime, air bubbles adopt a range of shapes depending on their size and packing. In particular, when passing through a series of extensions and constrictions, bubbles are observed to strongly elongate in accelerating flow regions and swell in decelerating flow fields. These experiments illustrate the possibility to control the flow morphology of microbubbles through the interplay between channel geometry and viscous flow.

This material is based upon work supported by the National Science Foundation under Grant no. CBET-1150389

Abstract

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This image may be freely reproduced with the accompanying credit: M. Sauzade and T. Cubaud (Stony Brook University)

Contact Information
Thomas Cubaud
Stony Brook University
http://me.eng.sunysb.edu/~microfluidics/

Blast-Born Vortices

Dell Olmstead, Tennille Bernard, Patrick Wayne, John Vigil, C. Randall Truman
Peter Vorobieff
The University of New Mexico

Blast-Born VorticesA mosaic of three images shows the evolution of a planar cross-section of a sulfur hexafluoride (SF6) gas column surrounded by air and impulsively accelerated by a shock (blast) wave. The image extent in the vertical direction is 16 mm, the Mach number of the shock is 1.7, which corresponds to shock front speed of about 560 m/s . The images were captured with a digital SLR camera and visualize laser-induced fluorescence in acetone pre-mixed with SF6 (1% by volume). Actual color of the fluorescence is shown unaltered. Flow direction is from right to left. The images were taken 50, 100, and 150 microseconds after the shock. This mechanism of shock-driven vortex formation is important for a number of practical problems, from inertial confinement fusion to supernova explosions.

This research is sponsored by the US National Nuclear Security Agency (NNSA).

Abstract

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This image may be freely reproduced with the accompanying credit: P. Vorobieff/UNM

References
€ C. Randall Truman, M. Anderson, P. Vorobieff, P. Wayne, C. Corbin, T. Bernard & G. Kuehner, "Spike and vortex formation in an impulsively-accelerated multiphase medium", in Computational Methods in Multiphase Flow VII, eds. Brebbia, Vorobieff, pp. 127-134, 2013, URL: http://library.witpress.com/pages/PaperInfo.asp?PaperID=2489

Contact Information
Peter Vorobieff
The University of New Mexico
Albuquerque, NM 87131

Washing Wedges

Etienne Reyssat
PMMH, ESPCI,
Université Paris 6,
Université Paris 7

Sequence of top views of a sharp wedge

The images represent a sequence of top views of a sharp wedge (angle 1°) formed by two almost horizontal glass plates. The apex of the wedge is located along the bottom boundary of the pictures and the width of an image is about 10 cm. The apex of the wedge is initially filled with a small volume of silicone oil (clear liquid).

A surfactant solution introduced in the wedge

A surfactant solution (dyed red liquid) is then introduced in the wedge. As it preferentially wets the glass plates, a complex exchange process occurs that leads to the extraction of the oil from the wedge. The oil/water interface destabilizes, oil drops are released and, driven by the confinement gradient, migrate away from the tip of the wedge through the water phase.

different stages of the exchange process of oil and soap solution

The sequence shows different stages of the exchange process of the oil and soap solution. In the present case, the oil viscosity is 5 cSt and the exchange is complete after typically one hour.

Abstract

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To use this image, please contact: Etienne Reyssat

Contact Information
Etienne Reyssat
PMMH, UMR 7636 du CNRS, ESPCI, Université Paris 6,
Université Paris 7
ESPCI, 10 rue Vauquelin, 75005 Paris, France, EU

Condensation of Droplets Inside Bubbles

Mahshid Mohammadi
Kendra V. Sharp
Oregon State University

Condensation of Droplets Inside bubblesDry bubbles moving in the microchannels may become immobile due to the presence of pinning and capillary forces. Upon stagnation, small droplets begin to condense on the polycarbonate channel walls inside the saturated bubbles. The droplet nucleation points become visible within a few seconds. As the size of the droplets gradually increases they coalesce and become larger. This phenomenon is similar to the condensation of droplets on the inside of a half-full closed bottle of water; however, in that large scale case, it takes much longer for the air to become saturated. The microchannels shown in the images are 250 µm wide and 100 µm deep. The bubbles in the microchannels are so small that the air within saturates very quickly; the bubbles may already be saturated before stagnation. The length of the bubbles increases over time due to the formation and growth of droplets inside them. At higher water flow rates, the pressure of the surrounding water as well as the pressure inside the bubbles is larger. Therefore, there is an increase in the rates of evaporation, condensation, and droplet growth.

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These images can be freely reproduced with the accompanying credit: Mahshid Mohammadi/Oregon State.

Contact Information
Kendra V. Sharp
School of Mechanical, Industrial, and Manufacturing Engineering
Oregon State University
Corvallis, OR, USA

3D Cylinder Wake

Eric Deem, François Nicolas, Louis Cattafesta, Farrukh Alvi
Florida State University

3D Cylinder WakeVolumetric velocity data are acquired in the wake of a cylinder of diameter D=20 mm and aspect ratio AR[=L/D]=3 immersed in a boundary layer. The Reynolds number based on diameter is Re=38,000. The relative boundary layer height is δ/H=0.45.

This plot is mean 3D streamlines of the wake behind the cylinder measured by tomographic PIV. The wake of the cylinder was chosen for this experiment due to the rich 3D flow features that can be observed. For example, two distinct counter-rotating regions are apparent in this plot. The mean was computed from 500 samples.

The funding for this research is provided by the AFOSR Grant [FA2386-12-1-3015], under the Defense University Research Instrumentation Program (DURIP), monitored by Dr. Doug Smith. Further support is provided by the NSF-PIRE grant [OISE-0968313] and the Florida Center for Advanced Aero-Propulsion (FCAAP).

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This image may be freely reproduced with the accompanying credit: E. Deem/FSU

Contact Information
Eric Deem
Florida State University
2003 Levy Ave
Tallahassee, Florida 32310

Vortex Knots in Experiment

Dustin Kleckner, Martin Scheeler, William T. M. Irvine
University of Chicago

It was nearly 150 years ago that Lord Kelvin first proposed his atomic theory in which knots in the Ether acted as the fundamental building blocks for matter. While the Ether was soon ushered out of style, knots have remained a fruitful mathematical and scientific interest for over a century, appearing in a wide range of topics, from quantum field theories to electromagnetism to plasmas and fluid flows [1-3]. Although knots in the vorticity field of a fluid have long been studied in theory [4], success in generating and observing these topological vortex loops in a real fluid has only recently been achieved [5].

Figure 1

Figure 1 shows one such topological vortex loop tied into a trefoil knot evolving in water. The knot is generated in the presence of tiny micro-bubbles, which are pulled into the low-pressure region at the vortex core where they scatter light, illuminating the structure of the vortex loop. In experiment, high-speed laser scanning tomography is used to capture the three-dimensional structure of the trefoil knot as it evolves, revealing its dynamics as it stretches and deforms itself until it ultimately undergoes a series of reconnection events that untie the knot into two unlinked rings. Interestingly, we observe that a pair of linked vortex rings follows this same general framework over its evolution: an initial rapid stretching of the rings as they approach a series of reconnection events that ultimately unlink them.

Figure 2

In order to create these topological vortex loops, a novel method was developed in which the vortex loops are shed from an accelerated hydrofoil, a collection of which are shown in Figure 2. With a wing profile cross-section, the hydrofoils have a trailing edge that traces out the desired path of the vortex loop, such that upon impulsive acceleration, they shed a starting vortex with the same geometry and topology as the hydrofoil itself. Advances in rapid prototyping and 3D printing have allowed us to quickly fabricate a zoo of hydrofoils of different shapes and topologies, which let us explore a wide variety of vortex dynamics from a geometric and topological perspective.

This work is supported by the National Science Foundation (NSF) Materials Research and engineering Centers (MRSEC) at the University of Chicago, and by the A. P. Sloan Foundation and the Packard Foundation.

Meeting Abstract (Event: 203835)

Meeting Abstract (Event: 203612)

Usage Information
Reporters may freely use this image. Credit Dustin Kleckner and William T.M. Irvine /U.Chicago.

Resources
[1] Witten, E., “Quantum-field theory and the Jones polynomial”, Commun. Math Phys., 121, 351-399 (1989). URL: http://link.springer.com/article/10.1007%2FBF01217730

[2] Kedia et al., “Tying knots in light fields”, PRL 111, 150404, (2013). URL: http://prl.aps.org/abstract/PRL/v111/i15/e150404

[3] Berger, M.A., “Introduction to magnetic helicity”, Plasma Phys. Control Fusion 41, B167-B175 (1999). URL: http://iopscience.iop.org/0741-3335/41/12B/312

[4] Moffat, H.K., “Degree of knottedness of tangled vortex lines” J. Fluid Mech. 35, 117-129 (1969). URL: http://journals.cambridge.org/action/displayAbstract?fromPage=online&aid=382055&fulltextType=RA&fileId=S0022112069000991

[5] Kleckner, D. and Irvine, W.T.M. “Creation and dynamics of knotted vortices”, Nature Physics 9, 253-258 (2013). URL: http://www.nature.com/nphys/journal/v9/n4/full/nphys2560.html

Galaxy in a Kitchen Sink

Hamid Ait Abderrahmane, Aslan Kasimov
King Abdullah University of Science and Technology,
Thuwal, Saudi Arabia

flow structure of a spinning pentagonal hydraulic jumpThe photograph shows the flow structure of a spinning pentagonal hydraulic jump and logarithmic spiral waves of fluid elevation downstream of the jump which are produced when a jet of water-glycerol mixture hits a horizontal glass plate and starts spreading radially out. The picture is taken from below the plate. The spiral waves in this experiment bear striking resemblance to the spiral density waves in galaxies. We found that the structure of the flow in the hydraulic jump exhibits counterparts of such additional salient morphological features of galactic flows as the outflow from the center, the jets, circum-nuclear rings, gas inflows toward the galactic center, and vortices. The hydrodynamic instability that is responsible for the formation of these features in the hydraulic jump may have a counterpart that plays an important role in the formation and persistence of the galactic spiral arms.

Abstract

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This image may be freely reproduced with the accompanying credit: H. Ait Abderrahmane, A.
Kasimov/KAUST

Contact Information
Prof. Aslan Kasimov
Physical Mathematics Laboratory
Applied Mathematics and Computational Sciences
Room 4-2226, KAUST, Thuwal 23955--‐6900, KSA
http://web.kaust.edu.sa/faculty/aslankasimov

Streamwise Vortices Generated by Rolling Up Shear Layers

Christoph Strangfeld, Karsten Düwel, Christian N. Nayeri, Christian O. Paschereit
Technische Universität Berlin

Streamwise Vortices Generated by Rolling Up Shear LayersStreamwise vortices produce strong low pressure regions and are generated on delta-wings, on the leeward side of trains, and at slanted rear ends of road vehicles and helicopters. In the presented experimental flow visualization (smoke in air), the flow separates downstream of a generic model: a swept, semi-span backward facing step. The separated flow rolls up into the vortex along the entire edge. The shear layer between the vortex core and the free stream is subjected to Kelvin-Helmholtz instabilities and continuously produces vorticity. Finally downstream, the shear layer vorticity convects into the vortex core and increases its circulation.

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This image may be freely reproduced with the accompanying credit: C. Strangfeld and K. Düwel/ TU-Berlin

Contact Information
Christoph Strangfeld
Institute of Fluid Dynamics and Technical Acoustics
-Hermann-Föttinger Institut-
Chair of Fluid Dynamics
Technische Universität Berlin

Technische Universität Berlin
Gebäude HF
Müller-Breslau-Str. 8
10623 Germany

Charged Jumping Droplets

Nenad Miljkovic
Daniel Preston
Massachusetts Institute of Technology

Ryan Enright
Bell Labs Ireland

Alexander Limia
Evelyn Wang
Massachusetts Institute of Technology

droplets on a superhydrophobic surface

When droplets on a superhydrophobic surface (shown at the top of NMiljkovic1) coalesce during water vapor condensation, the excess surface energy causes the merged droplet to leap off the surface. We observe that upon leaving the surface, the jumping droplets’ trajectory (pictured using long exposure photography) can be bent by an electric field, demonstrating that this ejection process causes them to become charged. The surface shown is nanostructured copper oxide coated with a thin hydrophobic monolayer of tri-chloro silane, rendering it superhydrophobic.

droplets merging during water vapor

Here we show a long-exposure-time image of droplets merging during water vapor condensation on a cooled superhydrophobic nanostructured copper oxide tube (outer diameter is 6.35mm, cooling water flow on the inside). Droplets that leap off also repel each other, because they gain a small positive charge during the merging and leaping process. This suggest the electrostatic effect could be exploited to produce surfaces that can be easily cleaned, enhance heat transfer, and anti-icing by the application of an electric field, to aid the droplet removal process.

We gratefully acknowledge funding support from the MIT S3TEC Center, an Energy Frontier Research Center funded by the Department of Energy, Office of Science, Basic Energy Sciences under Award no. DE-FG02-09ER46577.

Meeting Abstract (Event: 204483)

Meeting Abstract (Event: 204359)

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Reporters may freely use this image. Credit N.Miljkovic/D.Preston/MIT

References
N. Miljkovic, D.J. Preston, R. Enright, E.N. Wang, "Electrostatic charging of jumping droplets," Nature Communications, Vol. 4, 2517, 2013. URL: http://www.nature.com/ncomms/2013/130927/ncomms3517/full/ncomms3517.html

N. Miljkovic, R. Enright, Y. Nam, K. Lopez, N. Dou, J. Sack, E.N. Wang, "Jumping-Droplet-Enhanced Condensation on Scalable Superhydrophobic Nanostructured Surfaces," Nano Letters, Vol. 13, pp. 179-187, 2013. URL: http://pubs.acs.org/doi/abs/10.1021/nl303835d

Contact Information
Nenad Miljkovic
Postdoctoral Associate, NanoEngineering Group
Department of Mechanical Engineering
Massachusetts Institute of Technology
77 Massachusetts Avenue
Cambridge, MA, 02139
Tel: 617 981 9247
http://mit.edu/nmiljkov/www/

Merging Soap Films

Beng Hau Tan, Silvestre Roberto Gonzalez Avila, Claus-Dieter Ohl
Nanyang Technological University

Merging Soap FilmsHigh speed video recordings reveal complex fluid mechanics in the region where two soap bubbles merge. Here, surface tension is driving a very rapid flow into artistic patterns. Although the geometry of the problem is circularly symmetric, we observe intricate instabilities giving rise to petals, fractal-like structures and streaks that emerge within 100 microseconds after merging.

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This image may be freely reproduced with the accompanying credit: Cavitation Lab @ NTU

Contact Information
Claus-Dieter Ohl
Nanyang Technological University
School of Physical and Mathematical Sciences
Division of Physics and Applied Physics
SPMS-04-01, 21 Nanyang Link
Singapore 637731

Exploding Shocks and Bubbles

Pedro A. Quinto-Su
Universidad Nacional Autonoma de Mexico

Exploding Shocks and BubblesA laser pulse is simultaneously focused at the vertices of a square creating four microscopic plasmas, each one results in the emission of a shock wave and a rapidly expanding bubble. The first photograph shows the four luminescent plasmas (bright spots), the laser induced shocks and the bubbles at 4 nanoseconds after the arrival of the laser pulse. This image also shows the overlap of the shock waves at the center (straight lines).

Later the shocks reach the bubbles and reflect as tensions, breaking the liquid nucleating a bubble cloud with a square shape (second image, 29 nanoseconds after the arrival of the laser pulse). The width of the images is 144 micrometers.

The research is partially supported by CONACYT and PAPIIT-UNAM.

Abstract

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This image may be freely reproduced with the accompanying credit: P.A. Quinto-Su/ICN-UNAM

References
P.A. Quinto-Su and K. Ando, "Nucleating bubble clouds with a pair of laser-induced shocks and bubbles", JFM, 733, R3, (2013). URL:(http://dx.doi.org/10.1017/jfm.2013.456)

Contact Information
Pedro A. Quinto-Su
Instituto de Ciencias Nucleares
Universidad Nacional Autonoma de Mexico Circuito Exterior s/n, Ciudad
Universitaria, Delegacion Coyoacán, C.P. 04510, México D.F.

Sparkling Fireworks

Chihiro INOUE
The University of Tokyo
Tokyo, Japan

Fireworks

For over 300 years since the Edo period, a sparkling fireworks called Senkou-hanabi has been popular in Japan. This firework is made by simply wrapping a black powder (a mixture of potassium nitrate, carbon and sulfur) in a twisted paper. When we enjoy these fireworks in summer night, we hold the top end of the paper string and ignite the lower end. Then, a small fireball is produced at the lower end of the paper string, and beautiful streaks of light scatter from the fireball as shown in Figure 1 with soothing sounds. The formation of these streaks is attributed to sequential atomization and luminescence of droplets ejected from the fireball driven by a series of chemical reactions. A lucid scenario, however, has not been provided for the origination process of the streaks of light. While the fireworks has been so much popular in Japan, the physics behind its beauty was remained unexplained. In our study, by using a high-speed video camera, the origination of streaks of light from the fireball is clarified.

Figure 2

Figure 2 shows self-luminous images of the fireball. At t=0.0ms, the fireball expands by the combustion gas produced inside. Suddenly, at t=0.8ms, the surface of the fireball bursts. Due to the surface tension, the rim of the hole is pulled into the fireball. Then at t=2.4ms, the flow induced inside the fireball simultaneously concentrates and produces a small convex shape. At t=3.2ms, the convex portion grows rapidly to become the thin liquid thread. Finally, after t=4.0ms, the thread splits into droplets, which are recognized as streaks of light. It was revealed that the beautiful streaks of light originate from the interior of the fireball, and not from its surface.

This research was kindly supported by Dr. Joji KUWABARA and Mr. Keiji JO (Photron Ltd), and by Mr. and Mrs. Tsutsui (Tsutsui Tokimasa toy fireworks factory).

Abstract

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This image may be freely reproduced with the accompanying credit: Chihiro INOUE (The University of Tokyo, Japan)

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Dr. Chihiro INOUE
The University of Tokyo, Japan
Youtube Video

Hydrodynamic instabilities and art

Elsa de la Calleja, Sandra Zetina, Roberto Zenit
Universidad Nacional Autonoma de Mexico

Hydrodynamic Instabilities and artThis image shows the result of a density difference hydrodynamic instability. White paint is poured over a layer of black paint. Because of the density difference, the fluids mix. The process is inspired by a painting technique invented by D.A. Siqueiros.

DFD 2013 Meeting Abstract

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This image may be used for educational purposes only. Please credit: R. Zenit /UNAM

A Convention of UFOs

Sushant Anand, Adam Paxson, Kripa Kiran Varanasi
Massachusetts Institute of Technology
Cambridge, MA, USA

A Convention of UFOsOn superhydrophobic surfaces, droplets rest atop surface textures in a Cassie state and can be shed easily due to reduced pinning. However during condensation, condensing drops grow in Wenzel pinned state. By impregnating the solid surface with a lubricant this limitation can be overcome. Condensing surfaces were fabricated using standard photolithography with well-defined cubical microposts of silicon(a= 10μm,b= 10μm, and h= 10μm) and these were etched further to produce nanograss features. Subsequently they were silanized using a low-energy silane to render them hydrophobic. The textured surface was impregnated with an ionic liquid ([BMIm+][Tf2N-]) by using a controlled dip coating procedure. Experiments for observing microscale condensation growth were performed in an Environmental SEM. The surfaces were titled by 15º to the vertical and the ESEM experiments were conducted under identical conditions (pressure 1000 Pa, substrate temperature 4.5 ºC, beam voltage 25 kV, and beam current 1.7 nA). Drops condense on impregnated surfaces in Cassie state and microscale drops even with low contact angle zip across the surface giving an appearance of hovering UFOs (such as shown in image). A wetting ridge is formed around a water droplet due to interfacial force balance. The remarkable shedding behavior seen on these surfaces make them promising for enhanced condensation heat transfer.

Usage Information
This image may be freely reproduced with the accompanying credit: S. Anand/MIT

References
Anand, S.; Paxson A. T.; Dhiman R.; Smith J. D.; Varanasi K. K. Enhanced Condensation on Lubricant-Impregnated Nanotextured Surfaces. ACS Nano 2012 6 11 10122-10129. URL: (http://pubs.acs.org/doi/abs/10.1021/nn303867y)

Smith, J. D.; Dhiman, R.; Anand, S.; Reza-Garduno, E.; Cohen, R. E.; McKinley, G. H.; Varanasi, K. K., Droplet mobility on lubricant-impregnated surfaces. Soft Matter 2013, 9, (6), 1772-1780. URL: (http://pubs.rsc.org/en/content/articlehtml/2013/sm/c2sm27032c)

Contact Information
Sushant Anand
MIT
77 Massachusetts Avenue, Cambridge, MA, USA 02145

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Image & Video Galleries

Every year, the APS Division of Fluid Dynamics hosts posters and videos that show stunning images, graphics, and videos from either computational or experimental studies of flow phenomena. A panel of referees selects the most outstanding entries based on artistic content, originality, and their ability to convey information. The 66th Annual Meeting Image Gallery archives a subset of these images and videos on the APS DFD website.