📄 Extracted Text (10,508 words)
Whitesides Group - Research Page 1 of 7
The Whitesides Research Group SIMMS
Research
Microfluidics
The Whitesides Group is very active in microfluidics. Our
previous accomplishments in the field include work on
laminar flow in microchannels (Figures 1,2), fabrication of
three-dimensional channel topologies (Figures 3) and
mixing by chaotic advection (Figure 4). We have also
applied microfluidics to fabricate monodisperse polymer,
hydrogel, and metal microparticles coated with thin, nylon-
coated membranes (Figure 5). Currently, we are working on
several projects related to microfluidics, including
exploiting the behavior of bubbles and droplets for mixing Figure 1
and other applications, manipulating samples
electrokinetically and probing the use of solder as electrodes
in microchannels.
Bubbles and Droplets in Microchannels
Our recent experiments in microfluidics include
investigations into the behavior of bubbles and droplets in
microchannels. Specifically, we are interested in four sub-
areas: (I) enhanced mixing in microfluidic systems using
bubbles; (2) the paths from monodisperse to chaotic Figure 2
bubbling in flow-focusing devices; (3) the production of
bubbles with uniquely high periodicities in modified flow-
focusing systems; (4) the path-selection process that bubbles
demonstrate as they move through a network. Mixing in
microchannels, in particular, is an important challenge in
the microfluidics subgroup of our laboratory (the other areas
introduced here are described further in the complexity
section of the website).
Mixing between streams of fluid that flow in a laminar
fashion is difficult to achieve. Previously, we have
introduced a method to enhance mixing involving multiple
lithographic steps. Our current work uses bubbles to Figure 3
facilitate the folding over of streams of fluid as they proceed
through a network of microchannels (Movie 6). The bubbles
partially block the channels in which they move, causing a
portion of a stream of bulk fluid to cross over into the
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channel in which the other stream moves. This process is
repeated several times before the streams are mixed fully,
with the final mixing device occupying an area of only a
square millimeter on the chip. -stasktA
V2 cycle
Electrokinetic Flow in Microfluidic Channels
Itaal
We are exploring electrokinetically-driven microfluidic
systems for separation of complex biological samples. Our Figure 4
ultimate goal is to provide a new sample handling method
(femtomole/nL) for proteomic analysis and high-throughput -•
biochemical assays. Currently, we are investigating - •
geometrical designs, surface coatings and concentration
techniques such as isotachophoresis. - •-• •-• ••• O'N
TWIST Valves
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We have developed a new approach for controlling the flow 7 C-47-r
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of fluids in microfluidic channels. TWIST valves consist of
small machine screws (500 um diameter) embedded in a Figure 5
layer of polyurethane cast above microfluidic channels
fabricated in poly(dimethylsiloxane) (PDMS). The
polyurethane is cured photochemically with the screws in
place; on curing, it bonds to the surrounding layer of PDMS
and forms a stiff layer that retains an impression of the
threads of the screws (Figure 7). The valves are separated
from the ceiling of microfluidic channels by a layer of
PDMS, and are integrated into channels using a simple
procedure compatible with rapid prototyping. Turning the
screws actuates the valves by collapsing the PDMS layer
between the valve and channel, controlling the flow of
fluids in the underlying channels. These valves have the
useful characteristic that they do not require power to retain Movie 6
their setting (on/off). They also allow settings between "on"
and "off', resist large back pressures (>350 kPa) without
failure, and can be integrated into portable, disposable
microfluidic devices for carrying out biological assays
Int
(Figure 8).
TWIST Pumps
We have designed a system for storing and pumping fluids
in microfluidic devices fabricated in poly(dimethylsiloxane)
(PDMS) using TWIST valves. The method uses valves to
isolate microfluidic reservoirs that are filled with solutions Figure 7
of reagents under pressure; the fluid is released, and the
flow rate controlled, by opening one of the valves. Figure 9
shows a microfluidic pump fabricated using this approach.
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References
1. Jeon, N. L. et al. "Generation of Solution and Surface
Gradients Using Microfluidic Systems", Langmuir, 2000,
16, 8311-8316.
2. Wu, H. et al. "Fabrication of Topologically Complex
Three-Dimensional Microstructures: Metallic Microknots"
J. Am. Chem. Soc., 2001, 122, 12691-12699. Figure 8
3. Stroock, A. D. et al. "Chaotic Mixer for Microchannels"
Science, 2002, 295, 647-654.
4. Xu, S. et al "Generation of Monodisperse Particles by
Using Microfluidics: Control over Size, Shape, and
Composition" Angewandte Chemie 44 (5), 2005, 724-728.
5. Weibel, D. B. et al. "Torque-Actuated Valves for
Microfluidics" Analytical Chemistry 77(15); 4726-4733,
2005.
Figure 9
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The Whitesides Research Group
Research
Fluidic Optics
c1— I 'me WO*
Photonics deals with photons as a medium for transmitting
information. Typically, photonic circuits either rely on 004 Ckiya
passive devices with pre-designed optical functions, or use 0llg•ctib.
active components where application of external fields
changes the optical properties of the materials (e.g. in Can null Wei
electro-optical devices). Our projects in fluidic optics
explore alternatives to application of external fields - in
these projects we demonstrate the generation and
reconfiguration of photonic devices in real time by
manipulating flowing liquids. Figure 1
Fluid Optical Waveguides
We take advantage of laminar flow in microscopic channels
(i.e. microfluidic systems) and of diffusion. In the simplest ,
demonstration, we sandwich a fluid of higher index of
refraction between two streams of liquid with lower index
of refraction (Figuire 1). In microchannels, the liquids 11.
flowing through the channel will not mix except by
molecular diffusion; thus, the flow is laminar and the two
liquids flowing side-by-side form an optically smooth Figure 2
interface [1,2]. This system acts as a waveguide (we call it a
"liquid-liquid" or L2 waveguide).
Fluid optical waveguides are fabricated easily and rapidly in
organic polymers using the convenient techniques for rapid
prototyping developed in our group. The L2 waveguides are
dynamic their structure and function depend on a continuous
flow of the core and cladding liquids. They can be
reconfigured, renewed (if damaged), and continuously
adapted in ways that are not possible with solid-state
waveguides. Manipulation of the rate of flow and the
composition of the liquids (thus the optical properties) tunes
the characteristics of these optical systems in real time. Figure 3
Currently, we are studying the design and operation of fluid
analogs of several common optical elements: single- and
multi-mode waveguides, optical switches, and evanescent
couplers [3].
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Generation of Light in Microchannels
We have also demonstrated that fluid waveguides can
generate light in microchannels, thus simplifying the
coupling of light from external sources to these fluidic " • t
devices [4]. When laminar streams of fluorescent organic
dyes are separated by a low index fluid and illuminated by 620 660 as MO
an incandescent light source (Figure 2), they each produce
fluorescence of specific color that can be collected and Figure 4
propagated by a fluid waveguide. One can tune the
wavelength (color), position, shape and intensity of these
microfluidic light sources by making adjustments of the rate
of flow or composition of individual streams. Such simple
fluidic light sources could be important, for example, for
microanalysis "on-chip" in integrated biophotonic
microsystems.
Microfluidic Dye Laser
We used microfluidic technology to design a miniaturized
waveguide dye laser, in which the laser cavity contained a
liquid core-liquid cladding waveguide (Figure 3). The key
feature of the laser is a long optical path length along the
waveguide axis that allows us to achieve high gain in one
pass and thus lower the threshold for lasing. By adding thin
gold coatings on the surfaces of the T-junctions, we built the
laser mirrors into flouresent L2 waveguide light source.
Rhodamine 640 perchlorate dissolved in methanol served as
the core stream, and pure methanol worked as the cladding
stream. Optical pumping of the microlaser with a 532-nm
frequency-doubled Nd:YAG laser at 50 Hz results in the
bandwidth decrease by an order of magnitude at laser
threshold (Figure 4). The fluid waveguide laser is readily
tunable by continuously varying the composition of the
mixed solvent (methanol-dimethylsulfoxide) while using the
same concentration of the dye. The ability to easily change
wavelength is critical for applications in spectroscopy and
for various types of optical detection requiring different
wavelengths.
Select Publications
I. Stroock, A. D.; Dertinger, S. K. W.; Ajdari, A.; Mezic, I.;
Stone, H. A.; Whitesides, G. M. Science 2002, 295, 647-
651.
2. Ma, H.; Jen, A. K. Y.; Dalton, L. R. Adv. Mater. 2002,
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14, 1339-1365.
3. Wolfe, D. B.; Conroy, R. S.; Garstecki, P.; Mayers, 13. T.;
Fischbach, M. A.; Paul, K. E.; Prentiss, M.; Whitesides, G.
M. Proc. Nat. Acad. Sci. USA 2004, 101, 12434-12438.
4. Vezenov, D. V.; Mayen, B. T.; Wolfe, D. B.; Whitesides,
G. M. Appl. Phys. Lett. 2005, 86, 041104.
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The Whitesides Research Group
Research
Simple Nanotechnology
"Nanofabrication" is the process of making functional
structures with arbitrary patterns having minimum
dimensions currently defined (more-or-less arbitrarily) to be
—100 nm. Microelectronic devices and information
technologies have improved, and will continue to improve,
as a result of large-scale, commercial implementation of
nanofabrication. The motivation for these improvements is
to increase the density of components, to lower their cost,
and to increase their performance per device, and per Figure 1
integrated circuit. Methods used to generate nanoscale
structures and nanostructured materials are commonly
characterized as "top-down" and "bottom-up". The
conventional top-down techniques include photolithography
and scanning beam (or maskless) lithography (e.g., electron
beam and focused ion beam lithography). The limitations of
these conventional approaches when applied to innovative
problems - high capital and operating costs, the difficulty in
accessing the facilities necessary to use them, and their
restricted applicability to many important classes of
problems - motivate our exploration and development of
new, or "unconventional" nanofabrication techniques.
Unconventional techniques have the potential to be the Figure 2
ultimate, low-cost method for certain types of
nanomanufacturing; approaches based on reel-to-reel
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processing are particularly attractive for low-cost processes.
Unconventional approaches are also operationally much POMS
simpler to use than are conventional techniques, and thus
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help to open nanoscience and nanotechnology to exploration
by a wide range of disciplines, especially those historically
only weakly connected to electrical engineering and applied SAA%
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physics.
Nanofabrication by Molding Figure 3
The Whitesides group has developed four unique methods
for fabricating nanostructures by molding (Figures 1, 2): (1)
Replica Molding (RM) consists of three steps: i) creating a
topographically patterned master (usually by conventional
techniques; see, for example, ii) transferring the pattern of
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this master into PDMS by replica molding; and iii)
fabricating a replica of the original master by solidifying a
liquid precursor against the PDMS mold. (2) Solvent-
Assisted Micromolding (SAMIM) uses an elastomeric mold
and an appropriate solvent to emboss polymer films. (3)
Micromolding In Capillaries (MIMIC) uses capillarity to fill
a series of channels in a topographically patterned PDMS •
stamp with a fluid, low-viscosity polymer or ceramic
precursor. (4) Microtransfer Molding (µTM), prepolymer
fills the recessed regions of the mold, and excess Figure 4
prepolymer is removed from the top surface using a flat
edge. After placing the mold in contact with a rigid
substrate, the prepolymer is cured by appropriate means. St0ftb
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Nanofabrication by Stamping
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We have developed two methods for patterning molecules -SO • 2/0 non
on surfaces with high resolution (Figure 3). In microcontact
printing (µCP), molecules are transfered from a patterned Substrate
PDMS stamp to a substrate by the formation of covalent
bonds. In electrical microcontact printing (e-µCP), a flexible Figure 5
electrode is used to pattern a thin film of electret-based
material (i.e., that accepts and maintains an electrostatic
potential), probably by injecting and trapping charges.
Edge Lithography
We are exploring several methods for creating
nanostructures from using the topographical changes in the
edges of patterns. One approach is to pattern nanostructures
by selective removal or deposition of material at the edges
of lithographically-defined topographic features, such as Figure 6
SAMs (Figure 4).
A second approach (Controlled Undercutting), patterns
arrays of nanostructured trenches can be fabricated by the
controlled undercutting of topographic features using
isotropic wet etching, followed by deposition of a thin film
(Figure 5).
A third approach is Phase-Shifting Photolithography (Figure
6). In this technique, the vertical edges of a transparent,
topographically patterned substrate can induce changes in
the phase of incident, collimated light to create narrow
regions of constructive and destructive interference. Phase- Figure 7
shifting photolithography uses this phenomenon to project
"dark or "bright" spots of incident light onto the surface of a
photoresist.
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We and others have discovered that exposing the edge of a
thin film can lead to the formation of nanostructure (Figure
7). This method of edge lithography takes advantage of the Owas0
Uwe
numerous methods that can grow thin films over large areas
with a thickness between 1 and 50 nm. Converting these
films - which are thin in the vertical direction - into
structures that are thin in the lateral direction is an approach
to fabricating nanostructures.
Figure 8
Approaching Zero Through Crystalline Fracture
(Cracking)
• • 1.4 am
We have demonstrated a convenient method to generate - A
steps in a planar, surface with vertical dimension ranging
from the microscale to the atomic ( less than 0.5 nm) scale
(Figure 8). The process involves introducing a crack
halfway into a wafer of single-crystal silicon. These cracks 23nn
have the following attributes: i) they are continuous steps of
smoothly decreasing height, which run in straight lines
along crystal planes; ii) the step edges of the cracks are
typically —10 µm in height at edge of the wafer (where they Figure 9
initiate) and decrease to 0 nm at the "tip" of the crack
(where they disappear into the atomically smooth surface of
the silicon wafer; hence "approaching zero"); and iii) these
steps are continuous and linear, thereby making them easy
to find and characterize. We demonstrate the use of crystal
fracture for metrology in nanosciencc, by probing the limits
of polymeric replication with 0.4 nm resolution (Figure 9).
Functional, Dispersable, Nanostructures from
Templates
Figure 10
Metallic half-shells with submicron diameters: We have
demonstrated the use of spherical silica colloids on substrate
as template on which metallic half-shells are formed.
Dissolution of the template releases hollow metallic (Au, Pt,
Pd) hemispheres with nanometric-scale dimensions (Figure
10).
Metallic rods with submicron diameters: We use the
method of Martin to perform sequential electrodeposition of
multiple components with a porous template and to generate
multi-functional nanostructures. For example, it is possible
to generate nanorods with alternating sections of gold and
nickel (Figure 1 O. The gold provides a surface that can be Figure II
functionalized with thiol chemistry, while the nickel allows
the nanorods to be manipulated with an external magnetic
field. The rods naturally self-assemble into hexagonal
bundles through magnetic interactions. The magnetic forces
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polarize the disk-like section within the individual rods,
perpendicular to the physical (long) axis of the rods and
promote lateral interactions that direct the self-assembly of
the rods.
Free-standing metallic pyramidal shells: We fabricate
metallic shells with a pyramidal structure where the tips
have a radius of curvature of —50 nm (Figure 12). The
templates are formed by anisotropic etching of Si. The metal
shells are formed by electrodeposition. The uniformity of Figure 12
the templates fabricated by photolithography or soft
lithography ensures the uniformity in shape and size of the
pyramidal shells.
Select Publications
1. Xia, Y. and Whitesides, G. M. Angew. Chem. 1998, 37,
550.
2. Xia, Y. et al. Chem. Rev. 1999, 99, 1823.
3. Gates, B. D. et al. Annu. Rev. Mater. Res. 2004, 34, 339.
4. Gates, B. D. et al. Chem. Rev. 2005, in press
5. Kim, E., Xia, Y. and Whitcsides, G. M. Nature 1995,
376, 581.
6. Zhao, X., Xia, Y. and Whitesides, G. M. Adv. Mat. 1996,
8, 837.
7. Xia, Y. et al. Science 1996, 273, 347.
8. Odom, T. W. et al. Langmuir 2002, 18, 5314.
9. Gates, B. D. and Whitesides, G. M. SACS 2003, 125,
14986.
10. Xu, Q. et al. JACS, 2005, 127, 854-855.
11. Kumar, A., Biebuyck, H. A. and Whitesides, G. M.
Langmuir 1994, 10, 1498.
12. Love, J. C. et al. JACS 2002, 124, 1576.
13. Jacobs, H. O. and Whitesides, G. M. Science 2001, 291,
1763.
14. Aizenberg, J., Black, A. J. and Whitesides, G. M. Nature
1999, 398, 495.
15. Odom, T. W. et al. JACS 2002, 124, 12112.
16. Love, J. C., Paul, K. E. and Whitesides, G. M. Adv.
Mater. 2001, 13, 604.
17. Xu, Q., Gates, B. and Whitesides, G. M. SACS 2004,
126, 1332.
18. Gates, B. D. et al. Angew. Chem. Int. Ed. 2004, 43,
2780.
19. Xu, Q. et al. JACS, 2005, 127, 854-855.
20. Love, J. C. et al. Nano.Lett. 2002, 2, 891.
21. Love, J. C. et al. JACS. 2003, 125, 12696.
22. Qiaobing, X. et al. Nano.Lett. 2004, 4, 2509.
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The Whitesides Research Group
Research
Science for Developing Economies
An important problem is to use first-world science to benefit
the welfare of people in developing economies. The
Whitesides group is using its competencies in materials
science, engineering and biology to attack this type of
global problem, with a focus on health diagnostics and local
energy production. (Other problems include nutrition,
sanitation, information technology, education, ecosystem
management, and wealth creation.)
Figure I
Our approach - what we call "simple solutions" - relies on a
re-thinking to basic issues of design assumptions, from the
ground up, to fit the technology to the socioeconomic
constraints present in the developing world. Simple
solutions are inexpensive to produce, easy to maintain or
replace, simple to use, adaptable to local conditions,
scalable for mass consumptions, and easily stored and
transported. To the greatest degree possible, they are
independent of first-world infrastructure (such as electricity
and trained personnel).
Health Diagnostics Figure 2
A top priority for improving health in developing countries
is technology for simple, affordable diagnosis of infectious
diseases. We have developed new approaches that provide
low-cost, simple, and reliable solutions for (1) signal
amplification and detection in microfluidic devices, (2)
reagent handling in microfluidics, (3) fabrication of
microfluidic systems, and (4) valving. The work
demonstrates the potential of simplifying high-performing
devices (such as lab-on-a-chip devices) for use as diagnostic
tools in developing economies.
Figure 3
POCKET Immunoassay: The POCKET immunoassay
"POCKET" is short for portable and cost-effective) is an
integrated approach to a miniaturized immunoassay. It is
inexpensive and operable with minimal equipment and
technical skills, and shows an analytical performance
approaching that of enzyme-linked immunosorbent assays
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(ELISA).
The immunoassay (Figure 1) is performed in an
inexpensive, miniaturized platform (made by soft
lithography), in which the amplification chemistry is
compatible with microfluidics and simple optics. The
immunoassay functions with a portable and reusable
detector was built from components costing less than S45
US and consists of an InGaAIP red semiconductor laser
diode (654 nm) as the light source and an optical integrated Figure 4
circuit as the photodetector (Figure 2). The detector is
powered using a single 9V battery and can be used outdoors
1.10 1100
in daylight without changes in background signal. Instead of dilution dilution
enzyme-conjugated secondary antibodies in conventional Is
ELISA, the system uses antibodies conjugated to 10 nm serum
gold colloids; amplification of detection events is I
accomplished by electroless deposition of a silver film, Ilt
control
whose opacity is a function of the concentration of the t_ serum
analyte (Figure 3). In sensitivity, limit of detection, and
reproducibility, the POCKET immunoassay performs I men
comparably to conventional ELISA, and within a factor of
10 of the most sensitive ELISA format - chemiluminescence Figure 5
(Figure 4). The POCKET immunoassay can also reliably
distinguish the sera of HIV- I -infected patients from those of
noninfected patients (Figure 5).
Reagent-Loaded Cartridges: Current techniques for
automating fluid delivery in microfluidic devices, which
include valves and electroosmosis, require sophisticated
microfabrication of the chip, bulky instrumentation, or both.
Reagent-loaded cartridges are a simple and reliable
technique for storing and delivering a sequence of reagents
to a microfluidic device (Figure 6). The technique is low-
cost, requires minimal user intervention, and can be
performed in resource-poor settings (e.g., outside of a Figure 6
laboratory) in the absence of electricity and computer-
controlled equipment. In this method, cartridges made of
commercially available tubing are filled by sequentially
injecting plugs of reagents separated by air spacers (Figure
7). The air spacers prevent the reagents from mixing with
each other during cartridge preparation, storage, and usage.
As an example, we used this technology to complete an
immunoassay with low-nanomolar sensitivity in a
microchannel in 2 min; we demonstrated the diagnosis of
HIV in 13 min.
Figure 7
Novel Energy Concepts
Coal is a hugely abundant fuel source. We are exploring
approaches to fuel cells in which powdered coal is the fuel.
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We have developed a prototype coal fuel cell using a
solution of sub-bituminous coal (SBC) partially oxidized by
Fe-III (Figure 8). The rate of oxidation depended on the
concentration of the kon and the surface area of the coal. At
NO;
100 deg C, the maximum current density in the cell was 5 ~hode
A/L and the power density was 0.6 W/L. The cell operated Melon Mo
without loss of performance for 1000 hours.
Select Publications Figure 8
1. Sia, S.K. et al. "An Integrated Approach to Portable and
Low-Cost Immunoassay for Resource-Poor Settings."
Angew. Chem. Int. Ed. 43, 498-502 (2004).
2. Linder, V., Sia, S.K. and Whitesides, G.M. "Reagent-
Loaded Cartridges for Valveless and Automated Fluid
Delivery in Microfluidic Dcvices." Anal. Chem. 77, 64-71
(2005).
3. Weibel, D. B. et al "Modeling the Anodic Half-Cell of a
Low-Temperature Coal Fuel Cell" Angew. Chem. 44 (35),
2005, 5682-5686.
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The Whitesides Research Group SINEW
Research
Complexity and Emergence
We are exploring complex and emergent phenomena in
several dynamically self-assembling systems. Systems that
we have studied include disks spinning at liquid/liquid and
liquid/air interfaces, metal beads rolling on polymer ta-in. 00
surfaces, and components moving autonomously on the
surface of a hydrogen peroxide solution using bubble-based
propulsion. Our recent work in this area focuses on systems
in which bubbles and droplets in microfluidic networks are
the primary components.
Figure I
Periodic and Chaotic Formation of Bubbles
We are exploring the formation of bubbles in a microfluidic
flow-focusing device (Figure I) in which the rate of flow of
liquid and the pressure of gas are externally controllable. 11111111111111141111
Over much of the flow rate/pressure phase space, the system 11111111111111111111
produces monodisperse bubbles. We have shown that these
bubbles can be used to generate flowing lattices and
dynamically assembled foams (Figure 2). As one of the s•ke•kv•kil•k V
i V•
parameters is varied, however, the sizes of the bubbles e• so••• • GNI
lealfafrallIafrafti
produced become bi-disperse (Figure 3). Further variation
of the parameter leads to periodic production of bubbles of
four different sizes. The flow-focusing device can also be Figure 2
tuned to produce bubbles with a random size distribution.
The system shows similar behavior to a dripping faucet,
which also displays period-doubling bifurcations.
Stable, Periodic Behavior in a Bubble-Making System
We have extended the flow-focusing device to include five
inlets for liquid on either side of the gaseous thread. In a
simple flow-focusing device, the gaseous thread advances
into the orifice region where it is squeezed closed by the
buildup of pressure in the liquid around it. In the five-inlet
system, as the gaseous thread advances through the orifice Figure 3
region, it blocks the orifices sequentially, thereby increasing
the rate of flow of liquid through the unblocked orifices.
The advancing gaseous thread thus creates a mechanism of
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feedback in the system. Bubbles are squeezed off by the
downstream orifices as the thread is slowly squeezed at the
most upstream orifice, leading to the production of bursts of
bubbles (Movie 4). By varying the pressure of gas in the
system, for a constant rate of flow of liquid, we can tune the
number of bubbles produced by the device in each burst
from one up to 40 and back down to -10. We observe
highly stable periodic behavior over a range of pressures in
which 29 bubbles are produced per period (Figure 5).
Movie 4
Solving Mazes Using Bubbles in Microchannels
Previously, we have shown that an advancing front of ink in
a microfluidic network can elucidate the paths through the
network. We are extending this research to incorporate
bubbles that move in a continuous flow into the
microchannels. The use of bubbles increases the potential
utility of these systems as models for complicated networks,
such as traffic patterns in a busy city.
Select Publications:
Figure 5
1. Grzybowski, B. A., Stone, H. A. and Whitesides, G. M.
Dynamics of self assembly of magnetized disks rotating at
the liquid-air interface. Proceedings of the National
Academy of Sciences of the United States of America 99,
4147-4151 (2002).
2. Garstecki, P., Gitlin, I., DiLuzio, W., Whitesides, G. M.,
Kumacheva E. and Stone, H. A. Formation of monodisperse
bubbles in a microfluidic flow-focusing device. Applied
Physics Letters 85, 2649-2651 (2004).
3. Wiles, J. A., Grzybowski, B. A., Winkleman, A. and
Whitesides, G. M. A tool for studying contact electrification
in systems comprising metals and insulating polymers.
Analytical Chemistry 75, 4859-4867 (2003).
4. Fuerstman, M. J., Deschatelets, P., Kane, R., Schwartz,
A., Kenis, P. J. A., Deutch, J. M. and Whitesides, G. M.
Solving mazes using microfluidic networks. Langmuir 19,
4714-4722 (2003).
5. Grzybowski, B. A., Wiles, J. A., and Whitesides, G. M.
Dynamic self assembly of rings of charged metallic spheres.
Physical Review Letters 90, (2003).
6. Grzybowski, B. A. and Whitesides, G. M. Directed
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dynamic self-assembly of objects rotating on two parallel
fluid interfaces. Journal of Chemical Physics 116, 8571-
8577 (2002).
7. Grzybowski, B. A. and Whitesides, G. M. Dynamic
aggregation of chiral spinners. Science 296, 718-721
(2002).
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The Whitesides Research Group OMNI'S
Research
Magnetics
The Whitesides group is pursuing several projects involving
magnetism. In general we use magnetism as a handle for
physical manipulation of objects that are too small to be
easily manipulated directly (e.g. with tweezers or
micromanipulators). Much of this work is in collaboration
with Professors Donald Ingber (HMS) and Mara Prentiss
(Physics).
Figure I
Multifunctional Micro- and Nano-Rods
This project involves the fabrication of multifunctional
anisotropic structures through electrodeposition inside
porous templates. For example, we have demonstrated the
synthesis of metallic rods with submicron diameters that
contain disk-like ferromagnetic sections (Figure 1) [1]. The
metallic sections of these nanorods can be easily
functionalized using thiol chemistry, while the magnetic
portions provide a handle for manipulation with external
magnetic fields. These rods also self-assemble into highly
stable, hexagonally close-packed arrays (Figure 2). This
configuration minimizes the energy of the bundle and does Figure 2
not generate a net dipole for the structure. This work
provides a simple demonstration that magnetic interactions
between ferromagnetic objects can direct and stabilize the
formation of ordered, 3D structures by self-assembly.
••••••••
Magnetic Spheres
We are currently developing methodologies for generating
was .••• •••.• •
homogeneous ferromagnetic nanoparticles coated with a
uniform thin layer of gold. Similar to the multifunctional
rods, these core-shell structures could be easily modified
with functional bio-molecules (e.g. proteins, DNAs, etc) and Figure 3
then manipulated with external magnetic fields. We are also
exploring the synthesis and use of functionalizable
metallic/magnetic spheres in the form of half-shells (Figure
3) [2]. We have demonstrated that it is possible to use
spherical colloids (e.g. silica or polystyrene) as templates
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for vapor-phase metal deposition. In this case, we deposit
colloids in a monolayer on a flat substrate and evaporate
first a magnetic layer, then a metallic layer. The colloids can
be either resuspended in solution to give half-coated
spheres, or dissolved to give half-shells.
Magnetic Separations
We are actively examining the potential for using functional
magnetic micro- and nano-structures in microfluidics [3,4].
One potential use for such structures is in microfluidic
separations. We can use functional magnetic particles to
bind to certain components of a mixture selectively. We can
flow this mixture down a microfluidc channel with multiple
outlets. Application of a magnetic field gradient across the
channel can be used to direct the magnetic labeled
components in the mixture into a specific outlet. The factors
that determine the efficiency of this system include: strength
of the magnetic field, magnetic susceptibility of the
particles, viscosity of the liquid, and flow rate.
Magnetic Traps
This project involves the fabrication of three-dimensional
magnetic traps for diamagnetic objects in an aqueous
solution of paramagnetic ions [5]. We have demonstrated
trapping of polystyrene spheres, and of various types of
living cells: mouse fibroblast (NIH-313), yeast
(Saccharomyces cerevisae), and algae (Chlamydomonas
reinhardtii). The trapped particle and location of the
magnetic trap can be translated in three dimensions by
independent manipulation of the magnets that contribute to
the overall magnetic field.
Magnetic Tweezers
We have
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