Langmuir 2006, 22, 11255-11266
11255
Surfaces of Fluorinated Pyridinium Block Copolymers with Enhanced
Antibacterial Activity
Sitaraman Krishnan,† Rebekah J. Ward,‡ Alexander Hexemer,§ Karen E. Sohn,§
Kristen L. Lee,‡,⊥ Esther R. Angert,‡ Daniel A. Fischer,| Edward J. Kramer,*,§,£ and
Christopher K. Ober*,†
Department of Materials Science and Engineering and Department of Microbiology, Cornell UniVersity,
Ithaca, New York 14853, Department of Materials and Department of Chemical Engineering,
UniVersity of California at Santa Barbara, Santa Barbara, California 93106, and
National Institute of Standards and Technology, Gaithersburg, Maryland 20899
ReceiVed May 16, 2006. In Final Form: September 2, 2006
Polystyrene-b-poly(4-vinylpyridine) copolymers were quaternized with 1-bromohexane and 6-perfluorooctyl-1bromohexane. Surfaces prepared from these polymers were characterized by contact angle measurements, near-edge
X-ray absorption fine structure spectroscopy and X-ray photoelectron spectroscopy. The fluorinated pyridinium surfaces
showed enhanced antibacterial activity compared to their nonfluorinated counterparts. Even a polymer with a relatively
low molecular weight pyridinium block showed high antimicrobial activity. The bactericidal effect was found to be
related to the molecular composition and organization in the top 2-3 nm of the surface and increased with increasing
hydrophilicity and pyridinium concentration of the surface.
1. Introduction
Polycations with hydrophobic alkyl or benzyl side chains have
a disrupting effect on lipid bilayers in aqueous environment.1
Molecular simulations show that when such a polycation comes
in contact with a phospholipid bilayer, the cations attach to the
negatively charged phosphates of the lipid headgroups, while
the hydrophobic side chains insert themselves into the tail region
of the bilayer and result in its disorganization.2 The cytoplasmic
membrane of bacterial cells is a lipid bilayer consisting of
molecules such as phosphatidyl ethanolamine and phosphatidyl
glycerol (Figure 1). Although the bacterial cell envelope is more
complex than a simple bilayer structure, the antibacterial activity
of cationic polymers containing ammonium,3-13 pyridinium,14-20
* To whom correspondence should be addressed. E-mail: cober@
ccmr.cornell.edu (C.K.O.); edkramer@mrl.ucsb.edu (E.J.K.). Tel: 607-2558417 (C.K.O.); 805-893-4999 (E.J.K.). Fax: 607-255-2365 (C.K.O.); 805893-8486 (E.J.K.).
† Department of Materials Science and Engineering, Cornell University.
‡ Department of Microbiology, Cornell University.
§ Department of Materials, University of California at Santa Barbara.
£ Department of Chemical Engineering, University of California at Santa
Barbara.
| National Institute of Standards and Technology.
⊥ Present address: Department of Microbiology, University of Illinois at
Urbana-Champaign, Urbana, IL 61801.
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Figure 1. Phospholipid molecule; R ) -CH2CH2NH3+ in phosphatidyl ethanolamine and -CH2CH(OH)CH2OH in phosphatidyl
glycerol.
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10.1021/la061384v CCC: $33.50 © 2006 American Chemical Society
Published on Web 11/04/2006
11256 Langmuir, Vol. 22, No. 26, 2006
interaction between the polymer and the cytoplasmic membrane.1,3,4,34,35 The exact mechanism has yet to be ascertained.
Ivanov et al.2 have proposed that disruption of the cell membrane
occurs by the insertion of the hydrophobic alkyl groups, and
hence, hydrophobicity was the primary determinant of activity.
On the other hand, Kügler et al.36 have recently postulated a
mechanism based on the release of counterions from the cell
membrane and concluded that the bactericidal efficiency of
surface-tethered polycations was mainly determined by surface
charge density. Divalent cations, Mg2+ and Ca2+, neutralize and
bridge the phosphate groups of the phospholipid molecules, which
otherwise would strongly repel each other. The removal of these
cations from the outer membrane of a Gram-negative bacterium
such as Escherichia coli, in exchange for the polycation at the
surface, is said to cause destabilization of the outer membrane
leading to nonviable cells. Another mechanistic aspect of
antibacterial polycations is also noteworthy. Previously, it was
thought that a facially amphiphilic structure, in which hydrophobic
alkyl groups and hydrophilic ammonium groups segregate on
opposite sides of a low-energy, conformationally rigid backbone,
was required for antibacterial activity.37,38 It is now apparent that
even a flexible backbone could result in optimal activity.2
Although there are several studies on antibacterial activity of
nonfluorinated polymers, only a few reports on the activity of
cationic materials possessing fluoroalkyl groups can be found
in the literature. Sawada et al.39,40 have reported the antibacterial
and antiviral activity of fluorinated oligomers prepared by freeradical polymerization of an acrylamide monomer (with quaternary nitrogen) and fluoroalkanoyl peroxide initiators. These
oligomers, end-capped with fluorinated groups, were found to
inhibit replication of HIV-1 in cell culture, and also possess
antibacterial activity against Staphylococcus aureus. More recently, polynorbornene derivatives with alkylammonium (primary
amine reacted with perfluoroacetic acid) and isopropylidene
moieties as pendent groups were found to exhibit a good selectivity
against bacteria over human red blood cells.11 However, in the
absence of the isopropylidene side groups, the short perfluoromethyl group did not exhibit any antibacterial activity.
Antibacterial Activity of Surfaces. Tiller et al.17 have shown
that surface-tethered brushes of N-hexylpyridinium polymer were
effective against bacteria even in the absence of a liquid medium.
Such surfaces were found to kill, on contact, a number of airborne
Gram-positive and Gram-negative bacteria. Of the different
n-alkyl bromides used for N-alkylation of the pyridine rings,
n-hexyl bromide had the highest antibacterial activity against S.
aureus. They also found that the molecular weight of the
immobilized poly(4-vinylpyridine) (P4VP) was important for
the antibacterial properties of the surface. The reduced bactericidal
effect of surfaces with shorter P4VP chain lengths (60 kDa)
compared to high-molecular-weight P4VP (160 kDa) was
explained by the greater ability of the longer chains to penetrate
(33) Lohner, K.; Blondelle, S. E. Comb. Chem. High Throughput Screen.
2005, 8, 241-256.
(34) Lin, J.; Qiu, S.; Lewis, K.; Klibanov, A. M. Biotechnol. Bioeng. 2003,
83, 168-172.
(35) Milović, N. M.; Wang, J.; Lewis, K.; Klibanov, A. M. Biotechnol. Bioeng.
2005, 90, 715-722.
(36) Kügler, R.; Bouloussa, O.; Rondelez, F. Microbiology 2005, 151, 13411348.
(37) Tew, G. N.; Liu, D.; Chen, B.; Doerksen, R. J.; Kaplan, J.; Carroll, P.
J.; Klein, M. L.; DeGrado, W. F. Proc. Natl. Acad. Sci. U.S.A. 2002, 99, 51105114.
(38) Rennie, J.; Arnt, L.; Tang, H.; Nüsslein, K.; Tew, G. N. J. Ind. Microbiol.
Biotechnol. 2005, 32, 296-300.
(39) Sawada, H.; Wake, A.; Maekawa, T.; Kawase, T.; Hayakawa, Y.; Tomita,
T.; Baba, M. J. Fluorine Chem. 1997, 83, 125-131.
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Tomita, T.; Baba, M. J. Mater. Chem. 1998, 8, 1517-1524.
Krishnan et al.
the bacterial cell walls. The relatively thick (∼30 nm) peptidoglycan cell wall in S. aureus30 acts as a barrier between the
surface-tethered polycations and the cytoplasmic membrane.
Chemically, peptidoglycan consists of linear strands of two
alternating aminosugars, N-acetylglucosamine and N-acetylmuramic acid, that are cross-linked by short chains of amino acids
to form a three-dimensional matrix. If the loss of viability is due
to contact interaction between the polycations and the cell
membrane, the length of the polycation may seem important,
especially in the case of surface-tethered chains and Gram-positive
bacteria with thick cell walls. However, with the exception of
very low molecular weight polymers,34 surface-tethered polycations, with the polymer backbones lower in lengths than 30
nm, have been reported to exhibit antibacterial activity,17,41 which
was also observed in the present work.
The role of surface charge density on antibacterial activity has
been recognized in some studies.36,42 Bacterial death occurred
only above a threshold value of surface charge density. Our
experiments using surfaces of P4VP block copolymers showed
that, besides the length of the pyridinium block, it is the number
of pyridinium rings in the top few nanometers of the surface that
determines the bactericidal activity. P4VP with a molecular weight
of around 21 kDa was found to exhibit almost 100% bactericidal
effect against S. aureus. Moreover, a surface wherein the
pyridinium rings were densely covered by the alkyl side groups
was found to be less effective than one in which the pyridinium
rings were exposed. Near-edge X-ray absorption fine structure
(NEXAFS) spectroscopy and X-ray photoelectron spectroscopy
(XPS), which can determine the chemical composition within
the top 2-3 nm of a surface, were used in conjunction with
contact angle measurements to study the effect of surface
chemistry on bactericidal activity.
2. Experimental Methods
2.1. Materials. Styrene (CAS no. 100-42-5, FW 104.15, >99%,
Sigma-Aldrich) was stirred over dry di-n-butylmagnesium (received
from Sigma-Aldrich as a 1.0 M solution in heptane), and 4-vinylpyridine (CAS no. 100-43-6, FW 105.14, 95%, Aldrich) was stirred
over calcium hydride (CAS no. 7789-78-8, 90-95%, Aldrich), for
12 h and distilled under vacuum after three freeze-thaw-degas
cycles. Tetrahydrofuran (THF, 99.9%, Fisher) was distilled from
Na/benzophenone. sec-Butyllithium (sec-BuLi, CAS no. 598-30-1,
CH3CH2CHLiCH3, 1.4 M solution in cyclohexane, Aldrich), lithium
chloride (CAS no. 7447-41-8, LiCl, FW 42.39, 99.9%, Mallinckrodt),
(heptadecafluoro-1,1,2,2-tetrahydrodecyl)-dimethylchlorosilane (CAS
no. 74612-30-9, F(CF2)8(CH2)2Si(CH3)2Cl, FW 540.72, >95%,
Gelest), perfluorooctyl iodide (CAS no. 507-63-1, F(CF2)8I, FW
545.96, >98%, Fluka), 5-hexen-1-ol (CAS no. 821-41-0, HOCH2(CH2)3CHdCH2, FW 100.16, 99%, Aldrich), 2,2′-azobisisobutyronitrile (CAS no. 78-67-1, NtCC(CH3)2NdNC(CH3)2CtN, FW
164.21, 98%, Aldrich), tributyltin hydride (CAS no. 688-73-3, (nBu)3SnH, FW 291.06, 97%, Aldrich), carbon tetrabromide (CAS
no. 558-13-4, CBr4, FW 331.63, 99%, Aldrich), triphenylphosphine
(CAS no. 603-35-0, (C6H5)3P, FW 262.29, 99%, Aldrich), and
1-bromohexane (CAS no. 111-25-1, CH3(CH2)5Br, FW 165.07, 98%,
Aldrich) were used as received. Poly(4-vinylpyridine-ran-butyl methacrylate) with a weight-average molecular weight of 300 kDa and
10 wt % of n-butyl methacrylate (BMA), anhydrous methylene
chloride, N,N-dimethylformamide (DMF), and nitromethane were
obtained from Aldrich and used without further purification.
Polystyrene-b-poly(ethylene-ran-butylene)-b-polystyrene (SEBS)
triblock thermoplastic elastomer (Kraton G1652) was received as
a gift from KRATON Polymers. The solvents, methanol, chloroform,
(41) Isquith, A. J.; Abbott, E. A.; Walters, P. A. Appl. Microbiol. 1972, 24,
859-863.
(42) Tiller, J. C.; Lee, S. B.; Lewis, K.; Klibanov, A. M. Biotechnol. Bioeng.
2002, 79, 465-471.
Surfaces of Fluorinated Pyridinium Block Copolymers
Langmuir, Vol. 22, No. 26, 2006 11257
Scheme 1. Reaction Scheme for the Synthesis of Fluorinated Pyridinium Block Copolymers
toluene, and diethyl ether, were purchased from Fisher and used as
received. Scheme 1 shows the reactions involved in the synthesis
of fluorinated pyridinium block copolymers.
2.2. Synthesis and Characterization of Pyridinium Polymers.
2.2.1. Synthesis of Polystyrene-b-poly(4-vinylpyridine) by Anionic
Polymerization. Polystyrene-b-poly(4-vinylpyridine) was prepared
following a literature procedure.43 Polymerization was carried out
in THF at -78 °C using sec-butyllithium initiator. Styrene was
stirred with dibutylmagnesium, and 4-vinylpyridine was dried over
calcium hydride before distillation under vacuum. THF was refluxed
over sodium/benzophenone complex and collected in a reaction flask
containing lithium chloride (about 5× the molar amount of secBuLi) by distillation. The initiator (1.4 M solution in cyclohexane)
was then injected followed by the addition of styrene using a cannula.
A small amount of the polymer solution was withdrawn from the
flask after 45 min for molecular weight determination, and the aliquot
was quenched with anhydrous, oxygen-free methanol. The 4-vinylpyridine monomer was then added to the reaction flask, at which
point, the color of the solution changed from orange to yellow. After
2 h of polymerization at -78 °C, (heptadecafluoro-1,1,2,2tetrahydrodecyl)dimethylchlorosilane (10× molar excess) was
injected to terminate the polymer chains. The solution had to be
slowly warmed to about 30 °C before a loss of color, signifying
termination of the anions, could be observed. The final polymer
content of the solution was about 5% (w/v). The monomer conversion,
determined from the masses of the monomers added and the mass
of the polymer obtained, was close to 100%. Molecular weight of
the polystyrene (PS) block was determined by gel permeation
chromatography (GPC) of the polymer in THF using four Waters
Styragel HT columns operating at 40 °C, and Waters 490 ultraviolet
(λ ) 254 nm) and Waters 410 refractive index detectors. GPC
indicated a narrow distribution with the ratio of weight-average
molecular weight to the number-average molecular weight less than
1.1. The molecular weight of the 4-vinylpyridine block was obtained
from the mass of added 4-vinylpyridine and the PS molecular weight.
Two different diblock copolymers were prepared: one with PS and
P4VP block molecular weights of 11 and 21 kDa, respectively,
designated as PS11kP4VP21k, and the other with PS and P4VP block
molecular weights of 62 and 66 kDa, respectively, designated as
PS62kP4VP66k. The PS-b-P4VP copolymers were quaternized with
6-perfluorooctyl-1-bromohexane (F8H6Br) (4) and 1-bromohexane (H6Br) to obtain block copolymers with semifluorinated side
chains (6).
2.2.2. Synthesis of Semifluorinated Alcohol (3). 6-Perfluorooctyl-1-hexanol (CAS no. 129794-54-3, F(CF2)8(CH2)6OH, FW
520.23) was prepared as described by Höpken.44 Perfluorooctyl iodide
(40 g, 73 mmol) and 11 g of 5-hexen-1-ol (109.5 mmol) were heated
to 80 °C in a three-neck round-bottom flask fitted with a reflux
condenser and purged with nitrogen. About 200 mg (1.22 mmol) of
AIBN was added in four portions over a period of 6 h, and the
reaction mixture was maintained at 80 °C for a further 6 h. Excess
5-hexen-1-ol was removed by distillation (bp 56 °C at 11 mmHg).
Reduction of the iodo-adduct, 2, was performed at 80 °C for about
24 h, by adding 30 mL of anhydrous toluene, 31.9 g (109.5 mmol)
of tributyltinhydride, and 0.657 g (4 mmol) of AIBN. The product,
which solidified on cooling, was separated by filtration and washed
with toluene to remove the tin dimer, (n-Bu)3Sn-Sn(n-Bu)3. The
yield was about 60%.
2.2.3. Synthesis of Semifluorinated Alkyl Bromide (4). 6-Perfluorooctyl-1-bromohexane (CAS no. 195247-87-1, F(CF2)8(CH2)6Br, FW 583.12) was synthesized following the procedure of Wang
and Ober.45,46 6-Perfluorooctyl-1-hexanol (3 g, 5.77 mmol) and 3
g (9.05 mmol) of CBr4 were dissolved in a mixture of 6 mL of
anhydrous THF and 12 mL of anhydrous methylene chloride, and
(43) Förster, S.; Zisenis, M.; Wenz, E.; Antonietti, M. J. Chem. Phys. 1996,
104, 9956-9970.
(44) Höpken, J.; Möller, M.; Boileau, S. New Polym. Mater. 1991, 2, 339356.
11258 Langmuir, Vol. 22, No. 26, 2006
the solution was cooled to -5 °C. Triphenylphosphine (2.37 g, 9.05
mmol) was added in small portions over a period of 15 min. After
the mixture was stirred for 1 h at -5 °C and 6 h at room temperature,
the solvents were evaporated from the reaction mixture under vacuum
and about 50 mL of diethyl ether was added. An insoluble solid
(triphenylphosphine oxide byproduct) was separated by filtration
and the filtrate concentrated to obtain the crude product, which was
purified by being passed through a short silica gel column with
diethyl ether as the elution solvent. The yield was about 85%.
2.2.4. Quaternization of PS-b-P4VP Using 1-Bromohexane.
The PS-b-P4VP polymer was reacted with about 5× moles of
1-bromohexane in anhydrous DMF at 80 °C for about 24 h under
nitrogen. Thus, 1.5 g (7.36 mmol 4-VP) of the PS62kP4VP66k diblock
copolymer was dissolved in 10 mL of anhydrous DMF, and the
reaction flask was purged with dry nitrogen for about 15 min.
1-Bromohexane (5 mL, 35.6 mmol) was added, and the reaction
mixture was heated under nitrogen at 80 °C. The solution turned
dark green within about 2 h of reaction. After 24 h, the reaction
mixture was cooled to room temperature and added dropwise to 200
mL of diethyl ether at 0 °C, resulting in a brown precipitate of the
polymer. The solid was dissolved in chloroform, reprecipitated in
diethyl ether, and dried under vacuum.
2.2.5. Quaternization of PS-b-P4VP Using 6-Perfluorooctyl1-bromohexane. The PS-b-P4VP polymer was reacted with 0.3
equiv of 6-perfluorooctyl-1-bromohexane in anhydrous DMF at 80
°C for about 24 h under nitrogen. The remaining pyridine groups
were further alkylated using an excess of 1-bromohexane at 80 °C
for 24 h. The reactions were carried out sequentially without isolation
of the partially quaternized block copolymer 5 (cf. Scheme 1). Thus,
1 g (4.92 mmol 4-VP) of the PS62kP4VP66k diblock copolymer and
0.8630 g (1.48 mmol) of 6-perfluorooctyl-1-bromohexane were
dissolved in 10 mL of anhydrous DMF and heated to 80 °C under
nitrogen for 24 h, after which 5 mL (35.6 mmol) of 1-bromohexane
was added and the reaction continued for 24 h at 80 °C. After cooling
to room temperature, the polymer was precipitated in diethyl ether
at 0 °C to obtain the partially fluorinated polymer 6 shown in Scheme
1. It was further purified by reprecipitation from a 20% (w/v) solution
in chloroform into at least 20-fold volumetric excess of diethyl ether
(0 °C) to obtain a fine green precipitate.
2.2.6. Quaternization of P4VP Homopolymer and P(4VP-rBMA) Random Copolymer Using 1-Bromohexane. P4VP (2.5
g), with a molecular weight of 60 kDa, was reacted with 4.3 g of
1-bromohexane (10% molar excess) in 25 g of nitromethane at 80
°C for about 2 days. The color of the solution changed from bright
green to dark green and finally brown. After cooling to room
temperature, the viscous solution was poured into diethyl ether at
0 °C to obtain the quaternized polymer as a brown precipitate. Poly(N-hexyl-4-vinylpyridine-ran-n-butyl methacrylate) random copolymer was similarly prepared by reacting 6 g of P(4VP-r-BMA),
with an average molecular weight of 300 kDa, with 8 mL of
1-bromohexane in 60 mL of nitromethane at 80 °C for 2 days followed
by precipitation of the polymer in diethyl ether.
2.2.7. Polymer Characterization. IR spectra of the polymers
were acquired using a Mattson 2020 Galaxy Series FTIR spectrometer. Polymer films for the IR spectroscopy were prepared on
salt plates (KBr or NaCl) by drying solutions of the polymers in
chloroform. 1H and 19F NMR spectra were recorded using Varian
NMR spectrometers. CDCl3 containing 0.05% (v/v) tetramethylsilane
was used as the solvent. Differential scanning calorimetry was
performed using a TA Instruments Q1000 series differential scanning
calorimeter under nitrogen atmosphere. About 5 mg of sample was
used with heating and cooling rates of 10 °C/min.
2.3. Preparation of Surfaces for Antibacterial Tests. Surfaces
for bacterial assays were prepared on 3 in. × 1 in. glass microscope
slides. To improve adhesion of the pyridinium polymers to glass,
polystyrene-b-poly(ethylene-ran-butylene)-b-polystyrene (Kraton
SEBS G1652) was first spin-coated on the glass slides using a 10%
(w/v) solution in toluene and annealed in a vacuum oven at 120 °C
(45) Wang, J.; Ober, C. K. Liq. Cryst. 1999, 26, 637-648.
(46) Wang, J.; Ober, C, K. Macromolecules 1997, 30, 7560-7567.
Krishnan et al.
Figure 2. C K-edge and N K-edge NEXAFS spectrum of a poly(4-vinylpyridine) surface obtained at an X-ray incident angle of 55°
and entrance grid bias at the channeltron electron multiplier of -150
V. The dotted curve shows the exponential background that was
subtracted in the N K-edge region.
for 12 h. Solutions of the quaternized polymers were then sprayed
on the SEBS-coated glass slides (heated to 80 °C on a hot-plate)
using a Badger Model 250 airbrush (50 psi nitrogen gas pressure).
Samples for NEXAFS and XPS analyses were also prepared by
spin-coating polymer solutions, typically 3-5% (w/v) solutions in
chloroform, on silicon wafers using a Cee model 100CB spin coater
at 2000 rpm (acceleration of 1000 rpm/s) for 30 s.
2.4. Contact Angle and Surface Roughness. Contact angles
were measured using a NRL contact angle goniometer (Ramé-Hart
Model 100-00) at room temperature. Dynamic water contact angle
measurements were performed by addition and retraction of a drop
of water on the surface. Surface roughness was determined using
a 3-D interferometric noncontact surface profiler (ADE Phase-Shift
MicroAXM-100HR). Root-mean-square (rms) roughness values were
determined over regions of 631 µm × 849 µm size and averaged
over at least 10 measurements.
2.5. NEXAFS Spectroscopy. NEXAFS experiments were carried
out on the U7A NIST/Dow materials characterization end-station
at the National Synchrotron Light Source at Brookhaven National
Laboratory. The X-ray beam was elliptically polarized (polarization
factor ) 0.85), with the electric field vector dominantly in the plane
of the storage ring. The photon flux was about 1 × 1011 photons/s
at a typical storage ring current of 500 mA. A spherical grating
monochromator was used to obtain monochromatic soft X-rays at
an energy resolution of 0.2 eV. C and N K-shell NEXAFS spectra
were acquired for incident photon energy in the range 270-440 eV.
A computer-controlled goniometer, to which the sample holder was
attached, was used to vary the orientation of the sample with respect
to the X-ray beam. The partial-electron-yield (PEY) signal was
collected using a channeltron electron multiplier with an adjustable
entrance grid bias (EGB). All the data reported here are for a grid
bias of -150 V. The channeltron PEY detector was positioned at
an angle of 45° with respect to the incoming X-ray beam and in the
equatorial plane of the sample chamber. To eliminate the effect of
incident beam intensity fluctuations and monochromator absorption
features, the PEY signals were normalized by the incident beam
intensity obtained from the photo yield of a “clean” gold grid.47 A
linear pre-edge baseline was subtracted from the normalized spectra,
and the edge jump was arbitrarily set to unity at 320 eV, far above
the C K-edge, a procedure that enabled comparison of different
NEXAFS spectra for the same number of carbon atoms. The N 1s
Auger PEY was determined by subtracting the exponentially
decreasing background arising from C atoms in the region between
390 and 430 eV, as shown in Figure 2. Energy calibration was done
using a highly oriented pyrolytic graphite (HOPG) reference sample.
The HOPG 1s-to-π* transition was assigned an energy of 285.5 eV
according to the literature value.48 The simultaneous measurement
of a graphite-coated gold grid allowed the calibration of the photon
energy with respect to the HOPG sample. The error in the energy
calibration is expected to be within (0.5 eV. Each measurement
(47) Stöhr J. NEXAFS Spectroscopy; Springer-Verlag: New York, 1996;
Chapter 5, p 114.
(48) Rosenberg, R. A.; Love, P. J.; Rehn, V. Phys. ReV. B 1986, 33, 40344037.
Surfaces of Fluorinated Pyridinium Block Copolymers
was taken on a fresh spot of the sample in order to minimize possible
beam damage effects. Charge compensation was carried out by
directing low-energy electrons from an electron gun onto the sample
surface.
2.6. X-ray Photoelectron Spectroscopy. XPS measurements were
performed using a Kratos Axis Ultra Spectrometer (Kratos Analytical,
Manchester, UK) with a monochromatic Al KR X-ray source (1486.6
eV) operating at 225 W under 1.0 × 10-8 Torr. Charge compensation
was carried out by injection of low-energy electrons into the magnetic
lens of the electron spectrometer. The pass energy of the analyzer
was set at 40 eV for high-resolution spectra and 80 eV for survey
scans, with energy resolutions of 0.05 and 1 eV, respectively. The
spectra were analyzed using CasaXPS v. 2.3.12Dev4 software. The
C-C peak at 285 eV was used as the reference for binding energy
calibration.
2.7. Antibacterial tests. 2.7.1. Viable Counts. Trypticase Soy
Broth (TSB, 5 mL; per liter: 17 g of casein peptone, 3 g of soy meal
peptone, 2.5 g of D-(+)glucose, 5 g of NaCl, and 2.5 g of dipotassium
hydrogen phosphate) was inoculated with 100 µL of an overnight
culture of S. aureus and incubated at 37 °C for 4 h. The cells were
centrifuged at 5000 rpm (room temperature) for 1 min using an
Eppendorf model 5415C microcentrifuge, and the pellet was
resuspended in 1 mL of sterile filtered water. The suspension of S.
aureus (∼106 cells/mL) was sprayed on test surfaces. Initially, the
application of bacteria to test surfaces was performed as described
by Tiller et al.,17 but this procedure was subsequently modified to
improve safety as follows. To control aerosols, spraying was
performed in a class II type A biological safety cabinet (SterilGARD
Hood, Baker Company) with a HEPA filter. Sprayed surfaces were
dried in air for about 2 min and then placed in a sterile Petri dish.
Molten agar-containing TSB (1.5% w/v of agar) was poured on the
slides and allowed to solidify.
2.7.2. LIVE/DEAD BacLight Bacterial Viability Assay. LIVE/
DEAD Bacterial Viability Kit (BacLight) was obtained from
Molecular Probes, Inc. Equal volumes of SYTO 9 and propidium
iodide (PI, received as a solution in anhydrous dimethyl sulfoxide)
were mixed thoroughly in a microcentrifuge tube. A suspension of
S. aureus (∼105 cells/mL) was prepared as described above. The
BacLight dye mixture (30 µL) was added to 1 mL of the cell
suspension, which was then sprayed on the test surfaces. Immediately
after the spraying, the test surfaces were covered with glass coverslips
and incubated in the dark for 15 min. Phase-contrast and fluorescence
microscopy were performed, within 30 min after spraying, using an
Olympus BX61 epifluorescence microscope with a 100× UPlanApo
(N.A. 1.35) objective. The microscope was equipped with filter
cubes for viewing SYTO 9 and PI fluorescence. Images were acquired
using a Cooke SensiCam with a Sony Interline chip and Slidebook
software (Intelligent Imaging Inc.). Glass microscope slides were
used as controls.
3. Results and Discussion
3.1. Polymer Synthesis and Characterization. The PS-bP4VP polymers were easily soluble in DMF. The use of DMF
as a solvent resulted in higher degrees of quaternization within
shorter reaction times compared to chloroform, possibly due to
higher reaction temperatures that could be used under nonpressurized conditions. Moreover, the PS11kP4VP21k formed a cloudy
solution in chloroform, suggesting micelle formation.
The pyridinium block copolymer, prepared by reacting 0.3
equiv of 6-perfluorooctyl-1-bromohexane with the PS62kP4VP66k
block copolymer, is denoted by PS62kP4VP66k(F8H60.3H6)Br.
The polymer PS11kP4VP21k(F8H60.3H6)Br was similarly prepared
by reacting PS11kP4VP21k with 0.3 equiv of F8H6Br followed
by an excess of H6Br. The PS11kP4VP21k and PS62kP4VP66k block
copolymers quaternized with 1-bromohexane alone are denoted
by PS11kP4VP21kH6Br and PS62kP4VP66kH6Br, respectively.
These were readily soluble in chloroform or chloroform/methanol
mixtures to form clear solutions or cloudy micellar dispersions.
Although all the block copolymers were end-capped with
Langmuir, Vol. 22, No. 26, 2006 11259
Figure 3. IR spectra of (a) PS62kP4VP66k; (b) PS62kP4VP66k
quaternized with 1-bromohexane; and (c) PS62kP4VP66k reacted with
0.3 equiv of F8H6Br followed by an excess of H6Br. 1640 cm-1
CdN+ stretching vibrations; 1200-1300 cm-1 C-F stretching
vibrations; 700 cm-1 styrene C-H bending vibrations.
perfluorooctyl groups, the PS62kP4VP66k(F8H60.3H6)Br and PS11kP4VP21k(F8H60.3H6)Br polymers containing the F8H6Br side
chains will be called “fluorinated”, whereas the PS62kP4VP66kH6Br and PS11kP4VP21kH6Br polymers without the semifluorinated side chains will be referred to as “nonfluorinated”.
To interpret the NEXAFS spectra of the block copolymer
surfaces a quaternized homopolymer of 4-vinylpyridine was
prepared and used as a reference. P4VP with a molecular weight
of 60 kDa was alkylated using 1-bromohexane. Unlike the block
copolymers that were not soluble in nitromethane, the quaternization reaction of the P4VP homopolymer could also be
performed in this solvent. The resulting polymer is denoted by
P4VP60kH6Br. A random copolymer of 4-vinylpyridine and
BMA with 10 wt % BMA and a total weight-average molecular
weight of 300 kDa was alkylated with 1-bromohexane. The
resulting high-molecular-weight copolymer, denoted by P(4VPr-BMA)300kH6Br, was compared with the quaternized PS-bP4VP diblock copolymers for antibacterial activity. Surfaces
prepared using P(4VP-r-BMA)300kH6Br were found to retain
clarity when immersed under water, whereas the P4VP60kH6Br
polymer clouded upon water immersion.
Figure 3 shows the IR spectra of the PS62kP4VP66k diblock
copolymers. The peak at 700 cm-1, arising due to C-H bending
vibrations of the styrene phenyl ring, is unique to the PS block
and is absent in P4VP homopolymers (cf. Supporting Information). The quaternization reaction resulted in an almost complete
shift of the peak at about 1600 cm-1, corresponding to the CdN
stretching vibration of the pyridine ring, to about 1640 cm-1.
The PS11kP4VP21k polymers showed a similar shift of the peak
at 1600 to 1640 cm-1. Thus, the nonfluorinated, as well as the
fluorinated, pyridinium diblock copolymers showed a high degree
of quaternization, which was also evident from the XPS spectra
of these polymers, as discussed in Section 3.5. The extent of
alkylation of P4VP is usually determined using the relative
intensities of the peaks at 1600 and 1640 cm-1.49 However, in
the case of the quaternized diblock copolymers, the PS block is
also expected to show an aromatic CdC stretching resonance at
1600 cm-1. Interestingly, as seen in Figure 3, the 1600 cm-1
peak expected for PS is highly suppressed in the quaternized
block copolymer, while the aromatic C-H bending resonance
of PS at 700 cm-1 is quite pronounced.
The expected polymer composition was further confirmed by
1H and 19F NMR spectroscopy. Figure 4 shows the 1H NMR
spectra of the PS62kP4VP66k block copolymer precursor and the
(49) Panov, V. P.; Vorontsov, E. D.; Evdakov, V. P. J. Appl. Spectrosc. 1975,
23, 958-962.
11260 Langmuir, Vol. 22, No. 26, 2006
Krishnan et al.
Figure 4. 300 MHz 1H NMR spectra of (a) PS62kP4VP66k and (b) PS62kP4VP66k(F8H60.3H6)Br in CDCl3.
Table 1. Solutions Used to Prepared Surfaces for Antibacterial Tests
polymer
PS11kP4VP21kH6Bra
PS62kP4VP66kH6Bra
PS11kP4VP21k(F8H60.3H6)Brb
PS62kP4VP66k(F8H60.3H6)Brb
P(4VP-r-BMA)300kH6Bra
formulation
solution appearance
1.5% (w/v)c in 1:1 (v/v)
chloroform-methanol blend
1.5% (w/v) in chloroform
1.5% (w/v) in 1:1 (v/v)
chloroform-methanol blend
1.5% (w/v) in chloroform
1.5% (w/v) in chloroform
clear, pale yellow
cloudy
clear, dark green
clear, dark green
clear, pale yellow
a
P4VP precursors quaternized using a molar excess of 1-bromohexane alone. b P4VP precursors reacted with 0.3 equiv of 6-perfluorooctyl-1bromohexane followed by reactions with an excess of 1-bromohexane. c 1.5% (w/v) ≡ 0.015 g/mL.
PS62kP4VP66k(F8H60.3H6)Br fluorinated pyridinium polymer. The
peak near 8.3 ppm in the spectrum of the unquaternized polymer
(Figure 4a) corresponds to the protons of the pyridine ring ortho
to the nitrogen atom. The peaks near 6.4 and 7.1 ppm result from
the meta protons and the protons of the styrene phenyl rings. The
effect of quaternization is clearly evident in the 1H NMR spectrum
of Figure 4b, where the protons of the pyridine ring now appear
at 8.2 and 9.1 ppm. These 1H nuclei are less shielded due to the
positive charge on the carbon atoms of the ring, and thus appear
at higher resonance frequencies (or chemical shifts, δ). The
positions of the phenyl ring protons remain unchanged. Also
seen are the protons of the alkyl side chains, near 0.88 and 2.7
ppm, the former attached to carbon atoms away from the
pyridinium ring while the latter attached to carbon atoms closer
to the pyridinium ring. The peak near 2.1 ppm is probably from
the -CF2CH2- protons of the semifluorinated alkyl side chains.45
The 376.13 MHz 19F NMR spectrum of PS62kP4VP66k(F8H60.3H6)Br showed peaks at -81.4 (-CF3), -114.9 (-CF2CH2-),
-122.5, -123.4, -124.1, and -126.7 ppm (-CF2CF3) (cf.
Supporting Information).
IR spectroscopy of the pyridinium homopolymer, P4VP60kH6Br, showed a nearly complete shift in the position of the CdN
stretching resonance from 1600 to 1640 cm-1, indicating a high
degree of alkylation of the P4VP polymer. The IR spectra of the
unquaternized and quaternized P4VP and P(4VP-r-BMA)
polymers are shown in the Supporting Information. Using the
peak at 1720 cm-1 corresponding to CdO stretching vibrations
of n-butyl methacrylate as an internal standard, the degree of
quaternization in P(4VP-r-BMA)300kH6Br was determined by
the percent decrease in the absorbance of the CdN stretching
peak at 1600 cm-1 and was found to be about 94%.
Unlike the semifluorinated alkyl side-chain ionenes (polymers
with quaternary nitrogen atoms in the main chains) studied by
Table 2. Advancing and Receding Water Contact Angles on
Spray-Coated Surfaces
water CA
surface
θw,adv
θw,rec
PS11kP4VP21kH6Br
PS11kP4VP21k(F8H60.3H6)Br
PS62kP4VP66kH6Br
PS62kP4VP66k(F8H60.3H6)Br
P(4VP-r-BMA)300kH6Br
73°
63°
55°
56°
99°
16°
8°
16°
7°
10°
Wang and Ober46 or the 4-vinylpyridine polymers quaternized
with ω-alkylphenylbenzoate derivatives studied by Masson et
al.,50 the pyridinium block copolymers did not show strong thermal
transitions in DSC, possibly because of the relatively low density
of the semifluorinated alkyl groups along the polymer backbone.
3.2. Preparation of Test Surfaces. The coating formulations
are given in Table 1. Glass microscope slides, which were spincoated with a layer of SEBS, were used as substrates. The SEBS
film results in an elastomeric surface in which the cylindrical
domains formed by the PS end-blocks (∼7.5 kDa MW) act as
physical cross-links in a matrix of the poly(ethylene-ran-butylene)
central block (∼35 kDa MW). About 3 mg of the pyridinium
polymer was used per square centimeter of the surface. The
spray-coated surfaces were dried in a vacuum oven at 60 °C for
24 h. The properties of the surfaces, characterized by contact
angle measurements and NEXAFS spectroscopy, were found to
be fairly sensitive to the coating formulation and processing.
3.3. Water Contact Angle Measurements. Table 2 lists the
advancing and receding water contact angles (CA), denoted by
θw,adv and θw,rec, respectively, on the spray-coated surfaces used
in the antibacterial tests. The variation in the measured values
(50) Masson, P.; Gramain, P.; Guillon, D. Macromol. Chem. Phys. 1999, 200,
616-620.
Surfaces of Fluorinated Pyridinium Block Copolymers
Langmuir, Vol. 22, No. 26, 2006 11261
Figure 5. C 1s (a) and N 1s (b) NEXAFS spectra of surfaces prepared by spin-coating poly(4-vinylpyridine) and poly(N-hexyl pyridinium
bromide) from chloroform solutions on silicon wafers; P4VP molecular weight was 60 kDa. The surfaces were annealed for 12 h in a vacuum
oven at 120 °C. The spectra were obtained at an X-ray incident angle of 55° and the channeltron entrance grid bias of -150 V.
was within (2°, and the values reported are averages of at least
five measurements. The rms roughness values, determined by
optical interferometry, were close to 1 µmsabout 0.6 µm for
PS11kP4VP21k(F8H60.3H6)Br, 0.9 µm for PS62kP4VP66k(F8H60.3H6)Br, and 1.1 µm for P(4VP-r-BMA)300kH6Br. An unquaternized PS-b-P4VP copolymer, spin-coated on a silicon wafer and
annealed in a vacuum at 150 °C for 15 h had θw,adv and θw,rec
values of 95° and 69°, respectively, similar to those for a PS
surface. Thus, it can be inferred that the surface at equilibrium
is covered by the lower-surface-energy PS block at equilibrium,
as expected.51,52 However, the quaternized block copolymer
surfaces had lower contact angles (cf. Table 2), indicating the
presence of the pyridinium block at the surface. Interestingly,
the receding contact angles were lower for the PS11kP4VP21k(F8H60.3H6)Br and PS62kP4VP66k(F8H60.3H6)Br surfaces with
hydrophobic semifluorinated side groups than the nonfluorinated PS11kP4VP21kH6Br and PS62kP4VP66kH6Br surfaces. One
may infer that, in contact with water, the surface concentration
of the hydrophilic pyridinium rings is higher in surfaces with a
mixture of F8H6 and H6 alkyl groups. Moreover, the large contact
angle hysteresis indicates that these mixed surfaces are mobile,
that is, the surfaces can reconstruct to become hydrophilic in the
presence of water.
Quaternization of the 4-vinylpyridine polymer did not always
result in lowering of the contact angles. A spray-coated surface
of poly(4-vinylpyridine-ran-n-butyl methacrylate), annealed at
60 °C for 24 h, had advancing and receding water contact angles
of 72° and 20°, respectively. However, the corresponding
quaternized polymer, P(4VP-r-BMA)300kH6Br, had θw,adv and
θw,rec values of 99° and 10°, respectively (cf. Table 2). The higher
advancing water contact angle is attributed to a layer of
hydrophobic n-hexyl chains covering the pyridinium rings. The
lower-surface-energy53 -CH3 (∼24 mJ/m2) and -CH2- (∼31
mJ/m2) groups of the alkyl side chains will be preferentially
present at the air-polymer interface, covering the higher energy
pyridinium groups.
3.4. NEXAFS Spectroscopy. NEXAFS spectroscopy allows
the determination of the relative numbers of carbon and nitrogen
atoms and also the orientation of bonds in the surface region.
The size of the edge jump54 is proportional to the number of
absorbing atoms (C or N) and thus varies with surface
(51) Surface energy of PS is about 39.3 mJ/m2, and that of P4VP is 68.2 mJ/m2
(ref 52).
(52) Jiang, X.; Tanaka, K.; Takahara, A.; Kajiyama, T. Polymer 1998, 39,
2615-2620.
(53) Pittman, A. G. In Fluropolymers; High Polymers Series XXV; Wall, L.
A., Ed.; Wiley-Interscience: New York, 1972; p 419-449.
(54) The edge jump is given by the difference of the electron yield about 30
eV above the ionization threshold (320 eV in C 1s NEXAFS spectra and 430 eV
in N 1s spectra) and the electron yield just below the first resonance (cf. ref 55).
As discussed in Section 2.5, the latter is ∼0 for both C 1s and N 1s spectra, and
the C 1s edge jump has been set to unity.
concentration.55 The NEXAFS spectra reported here were
normalized such that the carbon edge jump was the same ()1)
for all the surfaces. Hence, the magnitude of the nitrogen edge
jump is proportional to the surface concentration of nitrogen
atoms relative to carbon. Moreover, a comparison of the intensity
of the C 1s f π* peak (near 285.7 eV for P4VP) is another
indication of the presence or absence of pyridinium groups at
the surface. Using NEXAFS spectroscopy, a comparison of the
surface pyridinium concentrations can be made in a dry state,
which the bacterial cells are likely to encounter when they initially
contact the surface. Spectrophotometric titration of surface
pyridinium groups, involving immersion of the surfaces in
aqueous solution of fluorescein dye, has been described by Tiller
et al.17
3.4.1. N-Hexylpyridinium Surfaces. Figure 5 shows the C
1s and N 1s NEXAFS spectra of surfaces prepared using P4VP60kH6Br polymer, as well as the P4VP60k precursor. The asymmetry
in the shape of the C 1s f π* peak is attributed to a 1s core level
shift arising from differences in the partial charges on the carbon
atoms at ortho and meta positions. The ortho atoms that are
bonded directly to the nitrogen are more positive than the meta
atoms which are further away from the nitrogen.56 Similarly, the
partial charge on the nitrogen atom will be higher than those on
the carbon atoms of the ring. Hence, the difference in the resonance
energies for the 1s f π* transition before and after quaternization
is much more pronounced in the N 1s spectra (Figure 5b) than
in the C 1s spectra.57 Quaternization had a strong effect on the
position of the N 1s f π* resonance, which shifted to a higher
energy by about 2 eV (from 400.7 eV for the unquaternized
P4VP60k polymer to 402.7 eV for the quaternized P4VP60kH6Br
polymer). Similar shifts were observed in the XPS nitrogen signals
of the quaternized polymers (Section 3.5) and have been reported
for P4VP and protonated P4VP by Fujii et al.58
In Figure 5, it is seen that the intensity of C 1s f π*CdC, CdN
peak is notably lower for the quaternized surface. The N 1s f
π* resonance for this surface (Figure 5b) is also lower in intensity
compared to the P4VP60k surface. The observed decrease is, in
most part, due to the decrease in the transition probability (the
number of electrons excited per unit time from the 1s shell) after
quaternization and also, in the case of the N 1s resonances, due
to the fact that the nitrogen to carbon atomic ratio in the polymer
decreases from 1/7 to 1/13 after quaternization.
(55) Stöhr J. NEXAFS Spectroscopy; Springer-Verlag: New York, 1996;
Chapter 7, p 211.
(56) Kolczewski, C.; Püttner, R.; Plashkevych, O.; Ågren, H.; Staemmler, V.;
Martins, M.; Snell, G.; Schlachter, A. S.; Sant’Anna, M.; Kaindl, G.; Pettersson,
L. G. M. J. Chem. Phys. 2001, 115, 6426-6437.
(57) Ito, E.; Oji, H.; Araki, T.; Oichi, K.; Ishii, H.; Ouchi, Y.; Ohta, T.; Kosugi,
N.; Maruyama, Y.; Naito, T.; Inabe, T.; Seki, K. J. Am. Chem. Soc. 1997, 119,
6336-6344.
(58) Fujii, S.; Armes, S. P.; Araki, T.; Ade, H. J. Am. Chem. Soc. 2005, 127,
16808-16809.
11262 Langmuir, Vol. 22, No. 26, 2006
Krishnan et al.
Figure 6. C 1s (left) and N 1s (right) NEXAFS spectra of PS-b-P4VP copolymers before (a and b) and after (c and d) quaternization with
1-bromohexane. The surfaces were prepared by spin-coating 5% (w/v) solutions of the block copolymers in chloroform on silicon wafers
and annealing at 150 °C, above the glass transition temperature (Tg) of the two blocks, for 12 h in a vacuum. Tg of PS and P4VP are about
100 and 142 °C, respectively.52 The NEXAFS spectra were obtained at an X-ray incident angle of 55°.
If the surface composition is uniform (same as that in the
bulk), the relative intensities of the N 1s f π* peaks at 400.7
eV in the NEXAFS spectra of the unquaternized and quaternized
polymers is an indication of the degree of quaternization. The
nitrogen edge jumps of the spectra in Figure 5b were normalized
to the same value so that the comparison was made for the same
number of nitrogen atoms in both the surfaces (cf. Supporting
Information). From the decrease in the intensity of the π*
resonance at 400.7 eV in the normalized spectra, it was inferred
that more than 90% of the pyridine groups have undergone the
quaternization reaction.59
Rather different results were obtained from the polystyreneb-poly(4-vinylpyridine) surfaces. Quaternization of the PS-bP4VP polymer resulted in an increase in the intensity of the N
1s resonances in the NEXAFS spectra. The C 1s NEXAFS spectra
of the PS11kP4VP21k and PS62kP4VP66k surfaces in Figure 6a are
indistinguishable from the spectrum of PS homopolymer. Thus,
the unquaternized block copolymer surfaces are almost completely
covered by the lower surface-energy PS block, which fully
supports the interpretation of the contact angle results. Using
PS-b-P4VP block copolymers in which the P4VP block was
end-functionalized with 3,3,3-trifluoropropyldimethylchlorosilane, Jiang et al. found that the P4VP block segregated to the
surface because of the low surface-energy -CF3 group at its
end.52 However, the PS11kP4VP21k and PS62kP4VP66k block
copolymers used in our study did not show surface segregation
of the higher-surface-energy block, even though the P4VP blocks
were terminated with perfluorooctyl groups. The reason for the
difference probably lies in the fact that the block copolymer
studied by Jiang and co-workers had a relatively low molecular
weight (14 kDa total) compared to those used in the present
(59) The degree of quaternization estimated using this procedure will differ
from that obtained by more conventional methods (such as IR or elemental analysis)
if the low-surface-energy alkyl groups in the quaternized polymer form a thin
layer at the surface covering the higher-surface-energy pyridinium rings. The
maximum thickness of this layer can be estimated to be ∼7.7 Å, corresponding
to a fully stretched n-hexyl chain attached to the pyridinium nitrogen. In such a
case, the degree of quaternization obtained from the NEXAFS spectra will be a
slight overestimate.
study. A single perfluorooctyl group at the end of our longer
P4VP blocks was unable to bring these to the surface.60
While the PS62kP4VP66k block copolymer surface did not show
any N 1s signal, the 4-vinylpyridine block could be detected in
the N 1s NEXAFS spectrum of the PS11kP4VP21k polymer.
However, these resonances were much weaker in intensity
compared to the P4VP homopolymer (cf. Figure 5b). The radius
of gyration of PS with a molecular weight of 62 kDa can be
estimated to be about 7 nm.61 The thickness of the PS layer
covering the 4VP block is expected to be at least 7 nm, which
is large compared to the escape depth of the N 1s Auger electrons.
Hence, if the P4VP block is buried below a layer of PS chains,
it would not be detectedsas observed experimentally for the
PS62kP4VP66k surface. The radius of gyration of PS with a
molecular weight of 11 kDa is about 2.9 nm, comparable to the
escape depth of the N 1s Auger electrons. Therefore, some
detection of the Auger electrons resulting from N 1s transitions
would be expected for the PS11kP4VP21k surface, as seen
experimentally.
When the PS-b-P4VP polymer is quaternized with 1-bromohexane, the lower-surface-energy -CH3 and -CH2- groups of
the alkyl side chains would be thermodynamically favored at the
air-polymer interface over the phenyl rings of the PS block. In
contrast to the unquaternized polymers, the presence of the
pyridinium block at the surface is evident from the NEXAFS
spectra of Figure 6 (c and d). The N 1s resonances are higher
in intensity, compared to the spectra in Figure 6b, especially in
the case of the PS62kP4VP66kH6Br surface. The spectra of the
block copolymers with different molecular weights, PS11kP4VP21k(60) To displace the PS block from the surface, the decrease in P4VP block
surface energy contributed by the perfluorooctyl groups must compensate for the
increased energy of the exposed P4VP surface. This compensation will require
a high areal density of perfluorooctyl groups, resulting in the necessity of the
P4VP chains to stretch away from the surface. The free energy penalty for the
required P4VP stretching increases as the P4VP block length increases and, thus,
above some block length, the perfluorooctyl end group will be ineffective in
bringing the P4VP block to the surface.
(61) Cotton, J. P.; Decker, D.; Benoit, H.; Farnoux, B.; Higgins, J.; Jannink,
G.; Ober, R.; Picot, C.; des Cloizeaux, J. Macromolecules 1974, 7, 863-872.
Surfaces of Fluorinated Pyridinium Block Copolymers
Langmuir, Vol. 22, No. 26, 2006 11263
Figure 7. C 1s (left) and N 1s (right) NEXAFS spectra of spray-coated PS62kP4VP66k(F8H60.3H6)Br (s) and PS62kP4VP66kH6Br (- - -)
quaternized diblock copolymer surfaces. Spectra were obtained at 55° X-ray incident angle.
Figure 8. C 1s (left) and N 1s (right) NEXAFS spectra of poly(4-vinylpyridine-ran-n-butyl methacrylate) surfaces.
H6Br and PS62kP4VP66kH6Br, now become almost identical.
The N 1s resonances in the NEXAFS spectra of the quaternized
diblock copolymers were, however, lower in intensity than those
for the homopolymer P4VP60kH6Br due to the presence of some
phenyl rings at the surface (cf. Figure 5b and Figure 6d). The
effect of PS block at the surface is also evident in the higher
intensity of the C 1s f π* resonance compared to the P4VP60kH6Br homopolymer (cf. Figure 5a and Figure 6c).
3.4.2. NEXAFS Analysis of the Surfaces Used for Bacterial
Tests. The C 1s and N 1s NEXAFS spectra of the surfaces used
in the bacterial assays are shown in Figures 7 and 8. These surfaces were prepared by spray-coating the quaternized polymers
on SEBS-covered glass microscope slides, as previously discussed. Figure 7 compares the NEXAFS spectra of the fluorinated and nonfluorinated pyridinium diblock copolymers,
PS62kP4VP66k(F8H60.3H6)Br and PS62kP4VP66kH6Br, respectively.62 The 1s f σ*C-F resonance in the C 1s spectrum of
PS62kP4VP66k(F8H60.3H6)Br, near 293 eV in Figure 7a, showed
the presence of the semifluorinated alkyl group, and hence the
pyridinium block, at the surface. The intensity of the σ*C-F
resonance was independent of the X-ray incident angle. Hence,
the semifluorinated side groups were not oriented the surface.
The N 1s resonances and also the edge jump were higher in
intensity for the fluorinated pyridinium block copolymer surface
than the corresponding nonfluorinated polymer (cf. Figure 7b),
indicating a higher surface concentration of pyridinium rings in
the former surface.
To investigate the effect of molecular weights of the PS and
P4VP blocks on the surface composition of the quaternized
polymers, the intensities of the carbon and nitrogen K-edge
resonances were compared. For both the nonfluorinated and
fluorinated PS11kP4VP21k and PS62kP4VP66k pyridinium block
copolymers, (i) the intensity of the C 1s f π* transition was
(62) The differences in the NEXAFS spectra of the PS62kP4VP66kH6Br surfaces
prepared by the spin-coating (Figure 6) and the spray-coating (Figure 7) techniques
are attributed to the different processing conditions used for the two surfaces. The
spin-coated samples were annealed at 150 °C, which is above the glass transition
temperature of the PS block, while the spray-coated samples were dried at 60 °C.
higher in the case of the higher-molecular-weight polymers and
(ii) the edge jump and the N edge resonances were lower in
intensity for the higher-molecular-weight polymers. These
observations indicate that the surface concentration of PS units
was higher in the case of the PS62kP4VP66k polymers than the
PS11kP4VP21k polymers. An overlay of the NEXAFS spectra of
the higher- and lower-molecular-weight polymers is shown in
the Supporting Information.
Figure 8 compares the NEXAFS spectra of the P(4VP-rBMA)300k and P(4VP-r-BMA)300kH6Br surfaces. The absence
of the π* peak corresponding to unquaternized pyridine rings in
the N 1s spectrum reflects the almost complete quaternization
of the precursor polymer, which is in accord with the results
from IR spectroscopy.
3.5. XPS of Surfaces Used for Antibacterial Tests. The
relative numbers of carbon and nitrogen atoms at the surfaces
of the pyridinium polymers used in the antibacterial assays were
also compared using XPS. Bilayer coatings were prepared by
spray-coating the polymers on SEBS-covered glass slides
followed by drying at 60 °C in a vacuum to remove solvent. All
XPS data were collected with a 0° electron emission angle (along
the surface normal). Figure 9 shows the N 1s XPS spectra for
the P4VP homopolymer before and after quaternization with
1-bromohexane. Upon quaternization, the nitrogen peak shifted
to a higher binding energy. The small peak at 399 eV is due to
the nitrogen atoms that had not undergone the quaternization
reaction. By comparing the areas under the two peaks, the
percentage of nitrogen atoms that were quaternized could be
calculated. As seen in Table 3, all the pyridinium polymers showed
a high degree of quaternization.
The C 1s XPS spectra of the fluorinated pyridinium block
copolymers (Figure 10a) showed distinct -CF2- and -CF3 peaks
at binding energies of 292 and 294 eV, respectively. Although
a small number of C-F carbon atoms from the perfluorooctyl
end groups of the PS-b-P4VP precursors (cf. 1 in Scheme 1) are
expected to be present in the otherwise nonfluorinated PS11kP4VP21kH6Br and PS62kP4VP66kH6Br surfaces, the low intensity
peaks seen near 292 eV in Figure 10b are most likely the shake-
11264 Langmuir, Vol. 22, No. 26, 2006
Krishnan et al.
Figure 9. N 1s XPS peaks from P4VP60k and P4VP60kH6Br surfaces.
The peaks are normalized such that areas under the corresponding
C 1s peaks (not shown) equal unity.
Table 3. Percentage of Quaternized 4-Vinylpyridine
polymer
% quaternization
P4VP60k
P4VP60kH6Br
PS11kP4VP21kH6Br
PS62kP4VP66kH6Br
PS11kP4VP21k(F8H60.3H6)Br
PS62kP4VP66k(F8H60.3H6)Br
0
95.2
95.5
90.9
93.1
94.3
up peaks. The shoulder at 286 eV is characteristic of carbon
atoms bonded to nitrogen atoms.19 The areas under the C-N
peaks were lower for the nonfluorinated block copolymers than
the fluorinated polymers, suggesting a higher concentration of
quaternary nitrogen in the fluorinated surfaces. Moreover, the
areas of the N 1s peaks near 402 eV (Figure 10c and d) were
correspondingly lower for the nonfluorinated polymers. Thus,
the lower-molecular-weight polymers had more N+ atoms at the
surface than their higher-molecular-weight counterparts, and the
fluorinated polymers had more quaternized nitrogen at the surface
than the nonfluorinated pyridinium block copolymers.
The results of NEXAFS spectroscopy and XPS may be
summarized as follows. Quaternization of PS-b-P4VP with
1-bromohexane resulted in the presence of the higher-surfaceenergy P4VP block at the surface, which was otherwise buried
below the PS block. The relative number of N+ atoms at the
surface was further enhanced when 6-perfluorooctyl-1-bromohexane was used. Partial quaternization of PS-b-P4VP with
F8H6Br resulted in a higher surface concentration of N+ compared
to block copolymers alkylated using H6Br alone. The PS62kP4VP66k block copolymers with higher weight fractions of PS
showed higher surface concentrations of PS.
3.6. Antibacterial Assay. The antibacterial activity of the
pyridinium surfaces were evaluated by performing a viable count
on S. aureus cells sprayed onto the surfaces. As seen in Figure 11A, a large number of bacterial colonies formed on the
untreated glass slide, which is not expected to have any
bactericidal activity.
Assuming that the same number of S. aureus cells were sprayed
onto the glass control and test surfaces, the relative number of
colonies on the glass and test surfaces represents the fraction of
the sprayed cells that remained viable on the test surfaces. The
viable counts were 15-30% lower on the PS11kP4VP21kH6Br
(Figure 11B) and PS62kP4VP66kH6Br (Figure 11C) surfaces
compared to the glass control. While the nonfluorinated diblock
copolymers had a large number of bacterial colonies, only
somewhat lower than that on uncoated glass, the fluorinated
pyridinium polymers (Figure 11E and F) showed an almost 100%
decrease in the viable count. The lengths of the pyridinium blocks
in both sets of polymers were the same, but quaternization with
F8H6Br caused a significant increase in bactericidal activity of
the surfaces.
The enhanced activity is attributed to the differences in surface
compositions and molecular organizations. Both NEXAFS and
XPS showed that the surface concentration of the pyridinium
rings, and hence the surface charge density, was higher in the
case of the fluorinated polymers, which is also consistent with
the lower water contact angles observed for these surfaces. A
higher charge density is expected to result in stronger electrostatic
interactions between the cells and the surface, which in turn
would lead to cell death by the mechanism discussed in Section
1. However, the concentration of pyridinium rings cannot be the
only factor affecting antibacterial activity. The surface concentration of the quaternary nitrogen was higher for PS11kP4VP21kH6Br than PS62kP4VP66k(F8H60.3H6)Br. However, the bactericidal effect of the nonfluorinated surface was significantly lower.
We do not conclusively know whether the rigid and highly
hydrophobic perfluoroalkyl helices have a greater ability to disrupt
the bacterial cell membrane. Nevertheless, the nonpolar nature
and a rodlike conformation of the fluoroalkyl helices could be
responsible for the higher antibacterial activity of the fluorinated
surfaces.
The viable count for the relatively high molecular weight
P(4VP-r-BMA)300kH6Br polymer (Figure 11D) was 60 ( 12%
lower than that on glass. Despite its high molecular weight, its
bactericidal efficiency was inferior to those of the PS11kP4VP21k(F8H60.3H6)Br and PS62kP4VP66k(F8H60.3H6)Br surfaces. This suggests that, in addition to molecular weight, the
molecular organization at the surface played a crucial role in
antibacterial activity. The reason for the reduced activity was
partially evident from the contact angle measurements. The
advancing water contact angle on the spray-coated surface of the
P(4VP-r-BMA)300kH6Br polymer was about 99°. Such a high
angle is indicative of a very dense layer of alkyl groups covering
the pyridinium rings, which we believe is unfavorable for
bactericidal activity.
The S. aureus cells used in the antibacterial assays were in the
exponential phase of growth and capable of cell division. The
lower number of bacterial colonies on the pyridinium surfaces
could be either through interference with cell division or by
causing major disorganization of the cell membrane resulting in
cell death. The BacLight staining method confirmed that the test
surfaces caused disruption of the cell membrane within 15 min
of contact. BacLight employs two nucleic acid stains: the greenfluorescent SYTO 9, which has excitation and emission maxima
at 480 and 500 nm, respectively, and the red-fluorescent PI,
which has excitation and emission maxima at 537 and 620 nm,
respectively.63,64 Besides their spectral characteristics, SYTO 9
and PI have different abilities to penetrate bacterial cell
membranes and different binding affinities toward nucleic acids.
SYTO 9 can freely permeate intact cell membranes. It is essentially
nonfluorescent in the free state, but its fluorescence quantum
yield increases by 1000-fold or more upon binding to nucleic
acids. In contrast, PI penetrates only cells with damaged
membranes. PI has a higher affinity toward nucleic acids, displaces
the less strongly bound SYTO 9 thereby reducing the intensity
of the green fluorescence, and itself fluoresces red. The
fluorescence quantum yield of PI increases 20-30-fold upon
binding to nucleic acids. Thus, by the suppression of the intensity
of green fluorescence and an enhancement in the red fluorescence,
(63) Biggerstaff, J. P.; Le Puil, M.; Weidow, B. L.; Prater, J.; Glass, K.;
Radosevich, M.; White, D. C. Mol. Cell. Probes 2006, 20, 141-146.
(64) Boulos, L.; Prévost, M.; Barbeau, B.; Coallier, J.; Desjardins, R. J.
Microbiol. Methods 1999, 37, 77-86.
Surfaces of Fluorinated Pyridinium Block Copolymers
Langmuir, Vol. 22, No. 26, 2006 11265
Figure 10. C 1s XPS spectra of spray-coated surfaces of (a) fluorinated pyridinium block copolymers and (b) nonfluorinated pyridinium
block copolymers. The corresponding N 1s spectra are shown in (c) and (d). The carbon peaks were normalized such that the total area under
the carbon peaks was equal to unity. The nitrogen peaks were normalized so that their areas were proportional to the number of nitrogen
atoms relative to the number of carbon atoms at the surfaces.
Figure 11. Photographs of S. aureus colonies on 1 in. × 1 in. regions of test surfaces.
bacteria with damaged membranes appear red while those with
intact membranes appear green.
Almost all of the cells on the glass control were stained green,
indicating intact and possibly viable cells (Figure 12a). Most of
the cells on the surface of the quaternized polymer were stained
red, suggesting disruption of the cell membrane (Figure 12b).
Thus, the antibacterial activity of pyridinium surfaces seems to
be through the loss of membrane integrity, rather than inhibition
of cell division.
4. Conclusions
Pyridinium block copolymers with fluorinated side chains were
synthesized by quaternization reaction of a semifluorinated alkyl
bromide with polystyrene-b-poly(4-vinylpyridine). Surfaces of
11266 Langmuir, Vol. 22, No. 26, 2006
Krishnan et al.
relatively low P4VP block molecular weight of 21 kDa (degree
of polymerization ∼ 200), showed almost 100% bactericidal
effect. The pyridinium surfaces were also found to inhibit the
growth of spores of the marine alga UlVa linza when immersed
in seawater.65
Figure 12. S. aureus cells on (a) uncoated glass slide and (b) glass
slide coated with the P(4VP-r-BMA)300kH6Br polymer. Cells with
intact cell membranes are stained green, and those with damaged
membranes are stained red.
the fluorinated block copolymers were found to be more effective
in decreasing the viability of airborne S. aureus than Nhexylpyridinium surfaces. NEXAFS and CA measurements
showed that fluorination resulted in an increase in the number
of pyridinium rings at the surface which, in general, correlated
with a higher antibacterial activity. In addition, the fluoroalkyl
side chains may be intrinsically favorable for disruption of the
bacterial cell membrane due to their rigidity and hydrophobicity.
Surfaces with a dense layer of alkyl side chains covering the
pyridinium groups showed higher water contact angles, lower
N 1s signals in NEXAFS spectroscopy, and were found to exhibit
lower antibacterial activity. In contrast, when the alkyl (or
fluoroalkyl) side groups were not densely packed and the surface
concentration of the pyridinium nitrogen was sufficiently high,
a greater antibacterial activity was observed. Molecular weight
does not seem to be a limiting factor in determining antibacterial
activity. The fluorinated pyridinium block copolymer with a
Acknowledgment. This research was supported by the Office
of Naval Research Grant No. N00014-02-1-0170 to C.K.O. and
E.J.K. which is gratefully acknowledged. NSF Grant No. MCB02-37025 to E.R.A. is also greatly appreciated. Additional funding
came from the National Science Foundation Division of Materials
Research (Grant Nos. DMR-0307233 and DMR-0208825). K.E.S
acknowledges support by an NSF Graduate Research Fellowship.
The research made use of the Hudson Mesoscale Processing,
Polymer Characterization and Surface Imaging facilities of the
Cornell Center for Materials Research (CCMR) and the
Microscopy and Microanalysis Central Facility of the Materials
Research Laboratory at UCSB, both with support from the
National Science Foundation Materials Research Science and
Engineering Centers (MRSEC) program (DMR-0079992 and
DMR-0520415, respectively). Use of the National Synchrotron
Light Source, Brookhaven National Laboratory, was supported
by the U. S. Department of Energy, Office of Science, Office
of Basic Energy Sciences, under Contract No. DE-AC0298CH10886. We thank Professor Lewis J. Fetters and Dr.
Ramakrishnan Ayothi for valuable discussions related to the
synthesis and characterization of the 4-vinylpyridine block
copolymers.
Supporting Information Available: IR, NMR, and NEXAFS
spectra. This material is available free of charge via the Internet at
http://pubs.acs.org.
LA061384V
(65) Krishnan, S.; Finlay, J. A.; Hexemer, A.; Wang, N.; Ober, C. K.; Kramer,
E. J.; Callow, M. E.; Callow, J. A.; Fischer, D. A. Polym. Prepr. (Am. Chem. Soc.,
DiV. Polym. Chem.) 2005, 46, 1248-1249.