A Superhydrophobic to Superhydrophilic In Situ Wettability Switch of Microstructured Polypyrrole...
Transcript of A Superhydrophobic to Superhydrophilic In Situ Wettability Switch of Microstructured Polypyrrole...
Communication
A Superhydrophobic to Superhydrophilic InSitu Wettability Switch of MicrostructuredPolypyrrole Surfacesa
Jean H. Chang,* Ian W. Hunter
We present an electrochemical layered system that allows for the fast, in situ wettabilityswitch of microstructured PPy upon the application of an electric stimulus. We have elimi-nated the need for PPy to be immersed in an electrolyte to switch between wetting states,laying the groundwork for PPy to be used as a viable material in many applications, includingmicrofluidics or smart textiles. The PPy sur-face was switched from the superhydropho-bic state (contact angle¼ 159) to thesuperhydrophilic state (contact angle¼ 0) in3 s. A wettability gradient was also created ona PPy surface using the layered system, caus-ing a 3 mL droplet to travel approximately2 mm in 0.8 s.
Introduction
Special surfaces with the ability to switch between wetting
states have recently garnered a great deal of attention due
to their potential applications in lab-on-a-chip devices,
smart-cooling systems, liquid lenses, low friction surfaces,
and water harvesting.[1–4] By controlling the surface energy
of a material, wettability gradients can be used to induce
fluid movement. There are several methods of switching
wettability currently in development, such as electrowet-
ting[5] or photo-,[6] pH-,[7] or thermo-responsive materials,[8]
each with their own set of limitations. Specifically,
electrowetting requires high voltages, photo- and
J. H. Chang, I. W. HunterBioInstrumentation Laboratory, Department of MechanicalEngineering, Massachusetts Institute of Technology, Cambridge,Massachusetts 02139, USAFax: 1 617 252 1849; E-mail: [email protected]
a : Supporting information for this article is available at the bottomof the article’s abstract page, which can be accessed from thejournal’s homepage at http://www.macros.wiley-vch.de, or fromthe author.
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thermo-responsive materials have slow reaction times,
and pH-responsive materials require contact with a
chemical solution to facilitate the wettability change.
The conducting polymer polypyrrole (PPy) (Figure 1a) is a
unique material that addresses the limitations of the
aforementioned materials due to its fast electrochemical
switch, low operating voltage, and relative ease of
fabrication.[9] Until now, PPy required immersion in a
chemical solution to switch wetting states, which limited
the potential applications for this material.[10–14]
In this communication, a fast in situ wettability switch of
a microstructured PPy surface is presented. The contact
angles of a 3 mL probe droplet (deionized water) sitting on
the surface are used to monitor the wetting state. The
relationship between contact angle and surface energy is
given by the Young-Dupre equation,
elibrary.
the
g lvcosuE ¼ gsv�gsl (1)
where glv, gsv, and gsl are the interfacial tensions between
liquid and vapor, solid and vapor, and solid and liquid,
respectively, and uE is the equilibrium contact angle of an
ideal, chemically homogeneous surface.[15] The ability to
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Figure 1. (a) Polypyrrole’s conjugated backbone allows for the delocalization of electronsand therefore its conductivity. (b) Scanning electron microscopy (SEM) image ofmicrostructured PPy grown on a glassy carbon substrate. (c) The microstructured PPyhas a roughness on two length-scales. (d) SEM image of microstructured PPy grown on amesh substrate. The microstructures grow inside the mesh openings. (e) Schematic oflayered system.
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J. H. Chang, I. W. Hunter
actively tune the surface energy of PPy without immersion
in solution makes this material suitable for use in
microfluidic devices, where a change in surface energy
may be exploited as a driving force for droplet movement.
This functionality may result in less contamination and
greater flexibility in fluid delivery as the fluid can be driven
to any point on the surface without the constraints
imposed by predefined channels. Additionally, an in situ
wettability switch of PPy provides one with the ability to
fine-tune the material’s surface energy to match specific
application requirements. Actively switchable PPy sur-
faces therefore have many potential applications in the
areas of drug, fluid, and nutrient delivery, cell and tissue
culture platforms, and high-throughput assays. We have
developed an electrochemical layered system that allows
for the in situ wettability switch of PPy, and demonstrate
that the polymer can be switched from the super-
hydrophobic state (contact angle >1508) to the super-
hydrophilic state (contact angle <58). The ability to fully
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switch between the two opposing wet-
ting states is an important feature as it
not only allows the number of possible
applications to be maximized, but it also
implies the ability to switch to inter-
mediate wetting states.
To the best of the authors’ knowledge,
to date there has been no published work
reporting a successful wettability switch
of PPy without immersion in electrolyte.
Most studies have reported an ex situ
wettability switch, where the surface is
dipped in a liquid electrolyte and dried
before measuring the surface energy
change.[10–12] Others have reported an
in situ surface energy switch by using
liquid probes that were immiscible in
water, but were still required to wet the
surface with liquid electrolyte.[13,14]
Furthermore, while Isaksson et al.,[16]
demonstrated a wettability switch of
the conducting polymer polyaniline with-
out electrolyte immersion, only a limited
range of contact angle values, 9–378, was
reported. The polymer was doped with
dodecylbenzenesulfonate, and the direc-
tional spreading of a droplet on an
electrochemically induced wettability
gradient was observed.[16]
Description of Layered System
The layered system developed in this
work was an electrolytic cell that con-
sisted of a superhydrophobic film of PPy
(the working electrode) and gold-coated stainless steel foil
(the counter electrode) separated by a polymer gel
electrolyte layer (Figure 1e). A two-electrode configuration
was used since practical applications of the layered system
would only require a controlled voltage input, rather than a
potentiostat for a three-electrode configuration.[17] It has
been shown that oxidation and reduction of PPy alter its
chemical composition and thus the surface energy as ions
diffuse into and out of the material.[9,11] A wettability
switch can therefore be initiated by applying a voltage
between the working and counter electrodes of the system,
driving ions into or out of the polymer. The design was
inspired by PPy bending actuators, in which a PPy working
electrode and a counter electrode (can be metallic foil or
another PPy film) sandwich an electrolyte layer (either
liquid or gel electrolyte).[18–20] The bending actuators utilize
a volumetric change in the polymer caused by the influx
and efflux of large counterions upon application of a voltage
across the electrodes.[18–20]
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A Superhydrophobic to Superhydrophilic In Situ Wettability Switch of . . .
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Experimental Part
Reagents and Materials
Pyrrole (99%, Sigma–Aldrich) was vacuum distilled and stored
under nitrogen at �20 8C. Potassium perfluorooctanesulfonate
(KPFOS, Sigma–Aldrich), ferric chloride hexahydrate (Sigma–
Aldrich), acetonitrile (anhydrous, 99%) (Sigma–Aldrich), propylene
carbonate (anhydrous, 99.7%, Sigma–Aldrich), and poly(methyl
methacrylate) (PMMA; average molecular weight 120 000, Alfa
Aesar) were of analytical grade and used as received.
Electrochemical Deposition of Polypyrrole
PPy doped with KPFOS was synthesized via galvanostatic poly-
merization with a current density of 1.5 A m�2 at ambient
temperature for 2 h using a VMP2 Multichannel Potentiostat
(Princeton Applied Research). The deposition solution contained
pyrrole (0.1 M), ferric chloride hexahydrate (0.0008 M), and KPFOS
(0.015 M) in acetonitrile. The surface morphology of the polymer
was characterized using a JEOL JSM-6060 scanning electron
microscope and a KLA Tencor P-11 Surface Profiler with a 2 mm
probe tip. Electron dispersive spectroscopy was performed using a
JEOL 6700F scanning electron microscope.
Wettability Switch in an Electrolyte Bath
A three-electrode configuration was used for the wettability switch
in the electrolyte bath. The electrolyte bath was constructed out of
Teflon1 and the electrolyte contained KPFOS (0.015 M) in
acetonitrile. PPy grown on a glassy carbon was used as the
working electrode, gold-plated stainless steel foil was used as the
counter electrode, and a silver wire was used as the quasi-reference
electrode. A potentiostat was used to apply a constant reduction or
oxidation voltage. Contact angles of a 3 mL droplet of distilled water
were measured using a Canon EOS 50D Digital SLR camera and a
MATLAB1 script. The measurement technique error was deter-
mined to be �28.
In Situ Electrochemical Wettability Switch
A two-electrode configuration was used for the in situ wettability
switch. Nylon mesh coated with 200 nm of gold by an AJA
International Orion 5 Sputter Coater was used as the PPy deposition
substrate, and gold-plated stainless steel foil was used as the
counter electrode. The PMMA-based electrolyte consisted of KPFOS
(0.1 M) in propylene carbonate with PMMA (25 wt.-%). The aqueous
electrolyte contained KPFOS (0.015 M) in distilled water. A
potentiostat was used to apply a constant voltage. A Canon EOS
7D Digital SLR camera and a Phantom v9.0 high-speed camera
were used to record video of droplet behavior. Contact angles and
droplet volume were determined using a MATLAB1 script. The
electrolytes were characterized using electrochemical impedance
spectroscopy techniques and a TA Instruments AR-G2 stress-
controlled rheometer.
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Results and Discussion
Development of Fast-Switching SuperhydrophobicPolypyrrole
PPy is grown electrochemically, and its surface can be made
hydrophobic by chemically doping the surface with a low
surface-energy sulfonic acid, such as a solution containing
perfluorooctanesulfonate (PFOS) ions. It is well known that
surface roughness can amplify the inherent hydrophobicity
or hydrophilicity of a surface,[21,22] a strategy that is
commonly employed to obtain superhydrophobic and
superhydrophilic surfaces.[23] To fabricate the superhydro-
phobic PPy working electrode layer for the switching
system, a soft-template polymerization that utilized ferric
chloride to create rough, microstructured PPy doped with
potassium perfluorooctanesulfonate (KPFOS) was modified
from the procedure first reported by Xu et al.,[11] and
optimized to provide a fast switch (see Supporting Informa-
tion). The surface of the fabricated film was porous (average
pore diameter 10 mm) and had a roughness on two length-
scales (Figure 1b,c), mimicking the Lotus Leaf effect[24] and
resulting in a superhydrophobic surface with a contact
angle of up to 164� 28. The average surface roughness, Sa,
was measured to be 4.13 mm, and the thickness of the
microstructures ranged between 15 and 30 mm.
During the optimization experiments, the polymers’
wetting states were switched in an electrolyte bath so that a
recipe for a robust, fast-switching polymer could be
developed before incorporation into the layered system.
The mechanism for the wettability switch is based
primarily on the change in chemical composition rather
than a change in the surface morphology upon reduction or
oxidation. No significant change in the surface roughness of
the polymer in the oxidized or reduced state was observed.
On the other hand, energy dispersive spectroscopy con-
firmed the presence of fluorine in the oxidized hydrophobic
polymer and no fluorine in the reduced hydrophilic
polymer, indicating the movement of PFOS ions upon
oxidation/reduction. In its initial state, the polymer is
oxidized and superhydrophobic. When the polymer is
placed in an electrolyte bath and a reduction voltage is
applied, PFOS ions migrate out of the polymer resulting in a
hydrophilic surface. The microstructures enhance the
hydrophilicity of the material, rendering the surface
superhydrophilic with a contact angle of 08. The process
is reversed by applying an oxidation voltage.
The polymer was grown on a glassy carbon substrate and
reduced in an electrolyte bath by application of a voltage of
�0.6 V (vs. a silver wire quasi-reference electrode). We have
previously reported that the initial state of the polymer is
over-doped, and a threshold of charge (�1 072� 225 C m�2)
that migrated out of the film needed to be reached before
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J. H. Chang, I. W. Hunter
the material could quickly switch between wetting
states.[25] Thus, the first reduction cycle (2 min) was much
longer than subsequent reduction cycles. Our polymers had
much faster switching times than polymers grown by Xu
et al.,[11] which had 20 min switching times with the same
applied voltages (�0.6 V). After the first reduction cycle,
which allowed for the threshold of charge to be reached the
polymer switched from the superhydrophobic to super-
hydrophilic state in 30 s, a 40-fold decrease in the switching
time when compared to the polymers grown by Xu et al.[11]
The polymer was oxidized by applying a voltage of þ0.6 V
(vs. Ag wire quasi-reference electrode), and switched back
to the superhydrophobic state after 5 min, a four-fold
decrease in the oxidation time. The fast electrochemical
switch may be due to a higher surface area of the PPy film,
increasing the effective electrode area. The difference in the
oxidation and reduction times can be attributed to the
reduced polymer being less conductive than the oxidized
polymer. The process was reversible for at least 100 cycles.
Figure 2. The layered system was used to change the wettabilityof PPy while a droplet was sitting on the surface of the material.Contact angles on the left and right side of the droplet are shownas a function of time. (The error bars represent a �28 measure-ment technique error.)
In Situ Wettability Switch
The optimized deposition recipe was then used to fabricate
PPy for the layered system. The polymer was grown on an
Au-coated nylon mesh, and the PPy microstructures grew
within the mesh pores while smooth PPy grew on the mesh
wires (Figure 1d). By growing the polymer on a mesh
substrate, the polymer could make contact with the
electrolyte on one side, while the surface remained dry.
This allowed for water droplets to be placed on the surface
of the polymer without mixing with the electrolyte, a
significant challenge of such electrochemical devices.
Additionally, the PPy mesh was more mechanically robust
than a free-standing film.
The mechanism for the wettability switch with the
layered system is similar to a switch in an electrolyte bath.
When a reduction voltage is applied between the working
electrode and counter electrode, PFOS ions diffuse through
the polymer bulk into the electrolyte layer, switching the
wetting state. The movement of PFOS ions out of the
polymer in conjunction with the microstructured surface is
how we were able to achieve a full range of wetting states.
We observed a transition from the superhydrophobic state
(contact angle in excess of 159� 28) to the superhydrophilic
state (contact angle of 08) with the layered system. There
was no observable reduction in the volume of the droplet
until the polymer reached a wetted state (specifically, when
the contact angle was less than approximately 158). In this
state, the increased surface to volume ratio as well as higher
contact area with the polymer led to some fluid loss due to
evaporation and absorption into the polymer.
While a rigorous analysis on the cycle life of the layered
system has not yet been performed, it is believed that since
the polymer has been shown to be electrochemically
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reversible when switched in an electrolyte bath, the redox
process using the layered system should also be reversible.
Additionally, when the polymer was oxidized in the layered
system, although the polymer was hydrophobic, the droplet
remained pinned due to the high capillary forces acting on
the droplet. A new droplet placed on the oxidized film was
once again in the hydrophobic state. To unpin droplets,
extra energy must be introduced into the system to
overcome the energy barrier between the pinned and
unpinned state.[26] The unpinning of droplets remains a
formidable task for researchers in this field.
The time constant of the switch was dependent on the
type of electrolyte used. When a reduction voltage of�4.0 V
(with respect to the counter electrode) was applied, a
PMMA-based gel electrolyte exhibited a full surface energy
switch in 3 s (Figure 2), while the fastest switch observed
was with an aqueous electrolyte, which switched the
polymer in 23 ms (see Supporting Information). The PMMA-
based gel electrolyte had a conductivity of 14.6� 0.003
mS m�1 and was very viscous, with a low shear rate
viscosity of 1 000 Pa s�1. The aqueous electrolyte had a
higher conductivity of 45.6� 0.022 mS m�1, however this
electrolyte also had a short shelf life due to evaporation. We
propose that the type of electrolyte can be selected and
optimized based on requirements for speed, controllability,
and shelf life, which are application dependent. Addition-
ally, the input voltage can be tuned for the desired
switching speed, as higher voltages will result in faster
ion diffusion.[20] Thus, PPy is a versatile material for
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Figure 3. (a) Schematic of modified layered system used to induce fluid movement. PFOS ions diffuse out of the polymer only in regions incontact with electrolyte. (b) Droplet movement induced by a wettability gradient created across the surface of PPy.
A Superhydrophobic to Superhydrophilic In Situ Wettability Switch of . . .
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applications requiring switchable wettability since the
switching speed can be tuned for the specific application.
Fluid Movement Induced by a Wettability Gradient
The layered system was used to demonstrate the use of
tunable PPy for applications requiring induced fluid
movement or unidirectional spreading. A wettability
gradient can be created by a voltage gradient caused by
the electrical resistance of the polymer. However, since the
resistance of the polymer changes with the doping level,[27]
a more controllable method of creating a wettability
gradient is to modify the electrolyte layer such that only
part of the polymer is in contact with the electrolyte. Thus,
any portion of PPy in contact with the electrolyte will be
switched to the hydrophilic state while PPy that is isolated
from the electrolyte will remain in the superhydrophobic
state. In the configuration shown in Figure 3a, the right half
of the polymer is in contact with the PMMA-based
electrolyte, while the left half is isolated from the
electrolyte. When a voltage was applied between the PPy
layer and the counter electrode, a droplet moved towards
the newly switched hydrophilic side. The center of mass of a
3 mL droplet traveled approximately 2 mm in 0.8 s
(Figure 3b). A future configuration of the system may
contain separators in the electrolyte layer to isolate regions
containing electrolyte. Polymer regions may also need to be
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electrically isolated to allow for the independent wett-
ability switch of such regions.
Conclusion
In summary, a layered system was developed that
electrically induces a change in the surface energy of the
conducting polymer PPy. It was demonstrated that the
layered system may be used to achieve a full range of
wetting states, switching from the superhydrophobic to
superhydrophilic states. Furthermore, we have eliminated
the need to immerse the polymer in electrolyte to facilitate
this switch, laying the groundwork for PPy to be used as a
material in applications requiring a surface energy change.
Acknowledgements: This work was funded by the Institute ofSoldier Nanotechnologies supported by the US Army ResearchOffice under grant contract number W911NF-07-D-0004, T.O.4. Theauthors would also like to thank the members of the BioInstru-mentation Laboratory at the Massachusetts Institute of Technologyfor their advice and support with this project.
Received: November 11, 2010; Revised: December 12, 2010;Published online: DOI: 10.1002/marc.201000716
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Keywords: polypyrroles; stimuli-sensitive polymers; superhydro-philic; superhydrophobic; surfaces
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