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Amine Enrichment of Thin-Film Composite
Membranes via Low Pressure Plasma
Polymerization for Antimicrobial Adhesion
Article in ACS Applied Materials & Interfaces · June 2015
DOI: 10.1021/acsami.5b01603 · Source: PubMed
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Research Article
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Amine Enrichment of Thin-Film Composite Membranes via Low
Pressure Plasma Polymerization for Antimicrobial Adhesion
Rackel Reis,*,† Ludovic F. Dumée,‡ Li He,‡ Fenghua She,‡ John D. Orbell,† Bjorn Winther-Jensen,§
and Mikel C. Duke†
†
Institute for Sustainability for Innovation, College of Engineering and Science, Victoria University, Hoppers Lane, Werribee, Victoria
3030, Australia
‡
Institute for Frontier Materials, Deakin University, Pigdons Road, Waurn Ponds,Victoria 3216, Australia
§
Faculty of Engineering, Monash University, Bayview Avenue, Clayton, Victoria 3800, Australia
S Supporting Information
*
ABSTRACT: Thin-film composite membranes, primarily based on poly(amide) (PA) semipermeable materials, are nowadays
the dominant technology used in pressure driven water desalination systems. Despite offering superior water permeation and salt
selectivity, their surface properties, such as their charge and roughness, cannot be extensively tuned due to the intrinsic
fabrication process of the membranes by interfacial polymerization. The alteration of these properties would lead to a better
control of the materials surface zeta potential, which is critical to finely tune selectivity and enhance the membrane materials
stability when exposed to complex industrial waste streams. Low pressure plasma was employed to introduce amine
functionalities onto the PA surface of commercially available thin-film composite (TFC) membranes. Morphological changes
after plasma polymerization were analyzed by SEM and AFM, and average surface roughness decreased by 29%. Amine
enrichment provided isoelectric point changes from pH 3.7 to 5.2 for 5 to 15 min of plasma polymerization time. Synchrotron
FTIR mappings of the amine-modified surface indicated the addition of a discrete 60 nm film to the PA layer. Furthermore, metal
affinity was confirmed by the enhanced binding of silver to the modified surface, supported by an increased antimicrobial
functionality with demonstrable elimination of E. coli growth. Essential salt rejection was shown minimally compromised for
faster polymerization processes. Plasma polymerization is therefore a viable route to producing functional amine enriched thinfilm composite PA membrane surfaces.
KEYWORDS: plasma polymerization, antimicrobial properties, amine enrichment, functional thin-film coatings,
nanoscale surface engineering
■
range of stresses associated with water transport under high
pressure and exposure to a range of complex contaminants.3
Over the past four decades, improvements via chemical and
fabrication routes have led to RO being the global primary
desalination technology. Despite their success, TFC membranes still suffer from issues associated with scaling, fouling
(e.g., colloidal, organic, and biofouling), and attack by oxidative
INTRODUCTION
TFC membranes are nanostructured materials that are core
components in RO desalination technology. These materials
are composed of a dense 100−200 nm thick PA film coated
onto a mesoporous support layer, typically made of poly(sulfone) (PSf) membrane, supported onto a macroporous
poly(ester) backing.1 The chemistry of the active PA layer
governs water and ion transport across the membrane,
achieving removal of up to >99% of dissolved salts and organic
molecules.2 In water treatment plants or during industrial
wastewater treatment, the PA layer is constantly subjected to a
© XXXX American Chemical Society
Received: February 19, 2015
Accepted: June 17, 2015
A
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typically more stable and uniform thin-films, independently of
the deposited monomer and the reactivity of the substrate. A
few works have reported on the plasma polymerization of TFC
membranes. These studies involved the grafting of hydroxylbased monomers in order to improve hydrophilicity, a pathway
for reducing fouling or scaling by favoring wettability.36−38
Another group of compounds, such as amines, have previously
been demonstrated to act as surface primers to improve the
adhesion and stability of hydrophilic coatings (e.g., poly(ethylene) glycol (PEGs) or poly(glycerol)).21,39 Plasma
polymerization of amine functionalities such as allylamine and
acrylonitrile has previously been used for TFC fabrication via
plasma polymerization, to form active top layers.40−42 Poly(acrylonitrile) (PAN)-based TFC membranes have been
prepared via plasma polymerization, which has been
commercialized by Sumitomo Co. as Solrox.43 Amine coatings,
such as N-vinylimidazole, offer a promising functionality known
for having a strong affinity with metals such as silver, which can
potentially introduce antimicrobial properties and possible
metal selectivity properties for metal contaminated wastewater
separation.44,45
In this work, the active PA layer of a commercial TFC
membrane was directly functionalized with amine moieties by
plasma polymerization of 1-vinylimidazole (VIm) monomers.
The resulting amine enrichment presents a versatile platform
for further functional modifications including attachment of
silver nanoparticles (Ag NPs), conferring measurable antimicrobial activity. The surface and metallic attachment
properties of the novel material were comprehensively
characterized, and the impact of the modification on the
essential membrane performance was also assessed.
species. The latter may arise from upstream equipment cleaning
or water disinfection, affecting flux and rejection performance.4
Therefore, new routes to further refine their properties are still
needed.
Surface modification is one approach to alter surface
properties, such as charge and roughness, that can potentially
reduce fouling across the surface of membranes.5,6 Surface
morphology and chemical composition play key roles in the
physicochemical interactions of the membrane surface with
contaminants present in solution.7 In particular, surface
roughness was shown to have a significant impact on fouling
mechanisms by facilitating adhesion and cake layer formation
on the membrane surface.8 Evidence of the effect of posttreatment coatings, such as reduced surface roughness, was
shown to lead to lower tendencies for organic compound
fouling during desalination operation.9−11 Furthermore,
depending on the nature and polarity of such coatings, the
surface charge of the modified membranes may be finely
altered. In addition, surface charge strongly influences fouling
mechanisms and also impacts on single salt permeation and
pure water permeability.12−14 The techniques reported to date
for TFC membranes involve chemical grafting polymerization15,16 and surface coating.5,17−19 Chemical routes for
polymer grafting utilize chemical initiators to generate freeradicals, enabling polymerization of monomers onto the
membrane surface.5,20 This technique was shown to lead to
an improved flux during organic fouling tests carried out under
operating conditions, due to repulsive interfacial interactions by
grafted functionalities.21 However, the adhesive interactions
between polymer and monomer mostly depend on the choice
of a suitable monomer to react with chemical groups present on
the material.22 Surface coatings, on the other hand, may lead to
covalent immobilization of large macromolecules containing a
number of specific functionalities.5,23 Typically, surface coatings
involve several steps whereby the polycondensation of the
monomers leads to the formation of a high-density layer. The
dense surface coating may cross-polymerize within the top
surface of the bulk supporting material, which may largely
compromise the materials permeation properties.17 Therefore,
although surface modifications across TFC membranes were
shown to improve fouling resistance by altering specific
interactions with contaminants, the adverse impact of the
coatings on the membrane’s performance and chemical stability
therefore requires a controlled incorporation of functional
groups across the surface of the materials to be treated.24,25
Low pressure plasma is a rapidly developing surface
modification technique that has been used for almost four
decades across a range of different industries.26−29 In
membrane technology, plasma treatment has been intensively
studied over the last two decades in attempts to increase the
hydrophilicity and improve the low-fouling properties of ultraand microfiltration membranes.25 A challenge in applying
plasma polymerization to TFC membranes is the difficulty of
characterizing the plasma polymerized coatings, since the
functionalities of the polymerized surface can be unpredictably
rearranged.30 Furthermore, the substrate has to be subjected to
vacuum conditions during the plasma process, which can cause
capillary stresses across the pores of the membrane material and
ultimately impact liquid permeability.31−33 Polymerization of
monomers is induced by plasma-generated free-radicals formed
in a plasma chamber and on the material’s surface.34,35 Low
pressure conditions allow the control of the polymerization
conditions and thus of the introduced moieties, which leads to
■
MATERIALS AND METHODS
Reagents and materials. BW30 TFC and PSf membranes were
purchased from Dow Filmtec Corp. (IMCD limited Australia) and
Beijing Puqirui (MWCO 30,000−50,000) technology, respectively.
Prior to the plasma treatment BW30 membranes were soaked in DI
water for 5 h in order to remove preservative materials and then dried
in air. Reagents 1-vinyl imidazole (VIm) for plasma polymerization
and Luria−Bertani agar for bacterial assessment were purchased from
Sigma-Aldrich. Ag NPs (average 20 nm diameter coated with 0.3 wt %
of Poly(vinylpyrrolidone) (PVP)) were purchased from Nanostructured & Amorphous Materials, INC.
Plasma polymerization technique. The monomer VIm was
plasma polymerized using a low-power plasma system reported in
detail elsewhere.46 In this work, plasma polymerization was performed
initially on a PSf membrane to assess chemical changes before treating
the TFC membranes. Membranes were placed separately in the
vacuum chamber (2 L) and firmly attached using sticky tape onto a
support, exposing the active side only. The plasma polymerization
process was divided into three stages inside the chamber, i.e. (i)
vacuum conditioning stage: the system was pumped down from an
initial Ar gas environment to 5 Pa; (ii) polymerization stage: VIm
monomer was injected into the system together with Ar gas to a
pressure of 7 Pa. The flow rate was 1.60 mL/min and energy delivered
was 1 W/L. At this stage the time exposure could be controlled, being
a crucial parameter for generation of free-radicals on the membrane
surface and for the control of the etching effect; (iii) reaction stage: the
Ar plasma is switched off allowing completion of the reaction involving
the monomer.
Silver attachment on TFC membranes. Amine rich and pristine
TFC membranes were immersed separately into an Ag NP solution
(0.1 mM, 50 mL) for 12 h, rinsed with DI water and dried in 35°.
Membranes were then subjected to microbial adherence assessment
and silver evaluation with XPS and EDS analysis. Three plasma
polymerization times of 5, 9, and 15 min were used on both PSf and
B
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Figure 1. SEM morphology analysis with progressive smoother surface images for TFC membranes: a) TFC-pristine, b) TFC-VIm-5, c) TFC-VIm-9
and d) TFC-VIm-15 with film rupture effect.
TFC membranes. To ensure correct assessment of the plasma effect, a
control sample was produced, which was a pristine membrane which
was inserted into the plasma vacuum chamber with only the vacuum
conditioning stage performed.
Characterization of amine rich TFC membranes. Amine rich
surfaces were first characterized with synchrotron Attenuated Total
Reflection-Fourier Transform Infrared Spectroscopy ATR-FTIR at the
Australian Synchrotron (AS) and then in our laboratory. For the
samples analyzed at the AS, single spectra and mapping analysis were
performed using a Bruker Hyperion 2000 coupled to laser V80v, MCT
narrow band 50 μm detector and spectrometer equipped with an ATR
element (45° multireflection germanium and BaF2 as background).
Mapping analysis investigated the distribution of cross-linking
functional groups across the surface and estimated amine rich coating
thickness. The thickness was evaluated using eq 1 where absorbance
intensity from new functionalities observed after plasma was correlated
according to the IR depth from the given frequency.
⎡A ⎤
2t
ln⎢ t ⎥ =
dp
⎣ A0 ⎦
potential was calculated based on four repeat measurements obtained
from both directions of flow in the cell.
Scanning electron micrograph (SEM) images were obtained with a
Quanta dual beam Gallium (Ga) Focus Ion Beam (FIB) from FEI and
samples were coated with carbon prior to image analysis. The images
for SEM mapping were collected under 20 keV with working distance
of 10 mm.
Atomic Force Microscopy (AFM) analysis was performed in
tapping mode using a Bruker equipped with Nanoscope V multimode
scan coupled with a microscope camera 10xA Nikon series 110422.
The resonance frequency and force constant for the probe was 300
kHz (±100 kHz) and 40 N/m. Data were collected using Nanoscope
8.4 software, a scan size of 7 μm and images were evaluated using
Gwyddion.36 data analysis software.
X-ray photoelectron spectroscopy (XPS) was performed using XPS
Spectrometer Kratos AXIS Nova (Kratos Analytical Ltd, Manchester,
UK) with aluminium Kα radiation as the X-ray source (1486 eV) at La
Trobe University, Victoria Australia University, Victoria Australia. XPS
Spectrometer with aluminum Kα radiation as the X-ray source (1486
eV). A quantitative elemental composition of the modified PA was
provided for a surface depth of 1−5 nm. The technique was able to
detect PA elements and silver concentration with detection limits of
0.1% of the bulk material.
Membrane performance test. Salt rejection and water
permeation performance were tested with a laboratory-scale crossflow filtration system (CF042, Sterlitech Corp., WA, USA). The
concentrated feed stream containing sodium chloride (2000 ppm at 25
°C) was pumped to the system with an effective membrane area of 42
cm2 and flowing tangentially across the membrane surface under 15
bar and trans-membrane pressures were monitored and maintained at
the target working pressure within a ± 2% accuracy. The outlet
permeate flow was collected after 180 min and salt rejection
conductivity measured immediately after the test. Salt concentration
was determined using an electrical conductivity meter (Hach HQ40d)
and mass of permeate was measured with a balance (EJ-410) and a
webcam was used to record at specific interval of 1 min the
corresponding mass.
Salt rejection R (%) was calculated according to
(1)
where t = the thickness of the coated film; A = the IR absorbance; and
dp = the depth of the IR beam.
All spectra for mapping analysis were collected with a 20 μm knifeedge aperture, corresponding to a 5 × 5 μm spot through the crystal
across a wavenumber range of 4000−850 cm−1. For each measurement
point, 64 spectra were averaged at resolution of 4 cm−1, background
was collected every 5 spectra and analyzed with OPUS 7.2 software
from Bruker Corporation.
The surface charge of the amine rich TFC membranes was
evaluated with a Surpass Anton Paar Electro Kinetic Analyzer (EKA)
utilizing Visiolab software (version 2.2). In the EKA analyzer,
membranes were placed onto a 20 mm × 10 mm adjustable gap cell
of thickness <2 mm. The streaming channel dimension was
approximately 0.1 mm. The pH electrodes (Schott Instruments)
were used for measuring of zeta potential at pressure increments from
20 mbar to 500 mbar. A KCl 1 mM solution was used, and 0.1 M HCl
and NaOH were used for pH adjustment. An average value of the zeta
C
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Figure 2. AFM morphology analysis and roughness values: (a) TFC-pristine (rms 31 ± 0.4; Ra 24 ± 0.2), (b) TFC-Vim-5 (rms 27 ± 0.7; Ra 22 ±
0.3), (c) TFC-Vim-9 (rms 29 ± 0.1; Ra 23 ± 0.5), and (d) TFC-Vim-15 (rms 24 ± 0.6; Ra 17 ± 0.4).
⎛ Cpermeate ⎞
⎟⎟ × 100%
R = 1 − ⎜⎜
⎝ Cfeed ⎠
significant smoothing effect was found. Figure 1d shows
superficial amine film rupture for 15 min membrane exposure,
suggesting, i.e., (i) mechanical rupture caused by volume
change when moved between ambient pressure and vacuum
from plasma or SEM; (ii) chemical etching from reactions with
the carrier gas causing ablation on a PA surface; or (iii) internal
stress in the PA structure due to longer polymerization and
thicker coating film. The first possibility may not significantly
contribute to the rupture effect once all membranes, including
pristine, were exposed to vacuum conditions for both plasma
and SEM. The second possibility relates to chemical etching,
commonly attributed in sputtering process or sputter coating. In
sputtering processes, electrons have high mobility; however,
ionic species in cold plasma have a low kinetic energy which
allows polymerization with preservation of functional groups,
without causing surface ablation.46,48−50 In the third possibility,
the internal stress effect is more conclusive, where significant
rupture was only found with the thicker film for 15 min of
polymerization. This effect was previously observed during
studies of the transport characteristic of radicals during plasma
polymerization, and the final deposited film thickness was
shown to be largely correlated to the deposition duration.50
The smoothing effect was also observed from AFM, as shown
in Figure 2. A decrease in surface roughness occurred with
longer plasma polymerization times. The average roughness
(Ra) and roughness mean square (Rms) were calculated from
three different locations on the membrane surface. For the
pristine TFC membrane, Ra was 24 ± 0.2 nm and Rms was 31 ±
0.4 nm. A slight decrease was found for TFC-VIm-5 (Ra 22 ±
0.3 nm; Rms 27 ± 0.7 nm) and TFC-VIm-9 (Ra 23 ± 0.5 nm;
Rms 29 ± 0.1 nm). For TFC-VIm-15 (Ra 17 ± 0.4 nm; Rms 24 ±
0.1 nm) the smoothing effect was more significant, suggesting a
potential thicker polymerized layer on the surface. The effect of
increasing thickness will be explored in the FTIR analysis.
Given that plasma polymerization allows deposition of thinfilms without penetrating the bulk material, the internal stress
(2)
where Cpermeate and Cfeed are the conductivity of salt concentration in
the permeate and feed, respectively, in μS/cm. Permeate flux F (L/m2·
h−1) was calculated by
F=
V
A×t
(3)
where V is permeate volume (L), A is effective membrane area (m2),
and t is the time over which the volume V was collected (h).
Bacterial adherence assessment. The antimicrobial property on
the membrane surface was assessed by exposing the active side of the
membrane to Escherichia coli (E. coli strain Nissle 1917). First, E. coli
was prepared following the same protocol as previously reported.47
Functionalized membranes were exposed to E. coli, and a 100 μL
aliquot of the E. coli suspension was pipetted onto an agar plate and
then spread over the surface. The membranes (7 mm diameter disk)
were placed onto the bacteria-agar surface with the silver-embedded
side facing the agar and incubated for 24 h at 37 °C. An optical
microscope, coupled with an Olympus DP70 Digital Microscope
Camera, was used to image the Petri dishes and quantify antimicrobial
inhibition zones around functionalized membranes (at 20 and 50 times
magnification). The inhibition zone distances were averaged from five
perpendicular points and measured according to the image size of 300
pixels/cm.
RESULTS AND DISCUSSION
Characterization of physical surface properties after
plasma polymerization of TFC membranes. Topographical analysis by SEM was performed on amine rich TFC
membranes in and membranes exposed to argon plasma alone
in order to visually observe the surface characteristics caused by
the polymerization. SEM images in Figure 1 show a consistent
trend for a smoothing effect after polymerization with increased
plasma exposure time. Smoother surfaces became more evident
between 9 and 15 min membrane exposure times in contrast to
membranes exposed to only argon (Figure S1), where no
■
D
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and Table S1). Increased S content suggests that the PSf
underlayer became more apparent to XPS due to small ruptures
during plasma polymerization which may adversely affect the
selectivity of the TFC membranes. In this respect, the duration
of the plasma polymerization process controlled the film
thickness, as posteriorly discussed in the IR mapping analysis
and shown in Table 1. The duration of the polymerization
contributed to increasing film thickness and potential decrease
of the stability of the deposited film. Therefore, the alterations
in the selectivity can relate to the morphology of the ruptures
(depth) and the density of the ruptures, with a certain amount
that may interfere with the selectivity.
The performance test is an essential parameter to verify the
feasibility of the plasma technique on TFC membranes. In
order to detect the impact of plasma conditions, including the
plasma etching effect, on the modified membrane’s performance, plasma polymerized membranes were compared to a
series of control membranes, as shown in Figure 3a: i.e. (i)
pristine membrane tested under “as supplied” conditions; (ii)
dried pristine that had only been dried in air for 12 h; (iii)
pristine membrane that had been subjected to vacuum
conditions from the plasma chamber; and (iv) membranes
exposed to argon plasma, used as the carrier gas in the plasma
polymerization process.
In terms of salt rejection, the fixed argon plasma conditions
did not affect the membrane’s selectivity, given that rejections
were maintained in the range of 98 to 99% for all plasma
durations (Figure 3a). However, in the plasma polymerization
process, selectivity declined similarly for the time range
between 5 and 9 min (95.5% and 95.7%). For 15 min of
treatment, the rejection was found to decline to 93.8%,
approximately 4% lower than that of the pristine membrane:
97.8% ± 0.5. The drop in salt rejection suggests an association
of factors that influenced the PA selectivity, such as film rupture
(as mentioned in SEM analysis) and surface charge, as
demonstrated in the next section.
The film rupture potentially introduced larger pores on the
PA layer, allowing larger salt molecules to diffuse across the
exposed nonselective PSf layerconfirmed with increased S/C
ratio as correlated in Table 2. For the 5 and 9 min membranes,
the thin amine film delivered nanosized ruptures near the PA
effect as found in SEM analysis (Figure 1d) may suggest that
the PA layer was also ruptured with a resultant exposed PSf
underlayer. This effect was mostly evident for the 15 min
polymerization. However, ruptures may have also occurred for
the shorter time plasma polymerized samples.
Quantitative elemental analysis performed with XPS in order
to evaluate chemical bonds rupture is shown in Table 1. The
Table 1. Correlation of Membrane Flux with Chemical/
Physical Properties after Plasma Polymerization
membranes
TFC-VIma
N/C ratio (at %)
TFC-VIm film
thickness (nm)
TFC-VIm avg
roughness Ra (nm)
TFC-dried
TFC-VIm-5
TFC-VIm-9
TFC-VIm-15
0.03
0.2
0.2
0.2
0
<21
21
60
24
22
23
17
a
Results for XPS analysis were only performed in plasma polymerization of VIm on TFC membranes.
XPS elemental analysis can detect up to 5 nm in depth the 200
nm PA layer. Previous XPS performed on the pristine BW30
membrane was shown to lead to the detection of only carbon
(C), nitrogen (N), oxygen (O), and very low (S) contents from
the PSf supporting layer underneath.51 The spectra obtained for
the plasma polymerized samples showed 10% increase in the
N/C elemental ratio expected from the polymerization of the
VIm monomer. However, uniquely for plasma polymerized
membranes, the S/C ratio also increased by 2 to 9% (Table 2
Table 2. Correlation of Selectivity with Chemical Properties
after Plasma Polymerization
membranes
TFC-VIma
S/C ratio (at %)
TFC-control
TFC-VIm-5
TFC-VIm-9
TFC-VIm-15
0.01
0.03
0.06
0.08
TFC-VIm salt
rejection (%)
97.8
95.5
95.8
93.8
±
±
±
±
0.5
0.7
0.4
0.4
TFC-Argon salt
rejection (%)
97.8
97.9
98.8
98.1
±
±
±
±
0.5
0.1
0.3
0.1
a
Results for XPS analysis were only performed in plasma polymerization of VIm on TFC membranes.
Figure 3. Permeation test for controls and modified membranes under 15 bar inlet pressure and 2000 ppm of NaCl solution: 27 °C at pH 6.5. (a)
series of control membranes and argon plasma; (b) amine rich modified membranes.
E
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Figure 4. ATR-FTIR peak profile for absorption bands noted after plasma polymerization: (a) peaks at 1724 to 1666 cm−1 for PSf and (b) at 1716
cm−1 to 1666 cm−1 for TFC. (c) SIR-Map homogeneity analysis with integration of peak 1666 cm−1.
amide I (C−N) stretching vibration at 1666 cm−1, and an
aromatic amide (N−H) deformation vibration or CC ring
stretching vibration 1609 cm−1.54,55 The carbonyl band was
formed after plasma polymerization from the reaction of freeradicals generated by the plasma via atmospheric O2, a common
reaction found in any polymer after plasma polymerization.50 In
the amide I band, possible cross-linking related to rearranged
and ruptured imidazole rings present within the monomer was
detected on the surface. As an example, amide I stretching
vibrations were previously reported at the frequencies of 1663
and 1668 cm−1. The band 1666 cm−1 was reported for
pyrimidine, an aromatic heterocyclic organic compound similar
to the imidazole ring present within the monomer.56 The same
bands corresponding to cross-linked bonds were also found for
amine rich TFC membranes, as shown in Figure 4b. However,
no significant alterations were found for membranes exposed to
argon plasma alone, which confirms that the enhanced bands
are correlated to polymerization on the surface. The duration of
the plasma polymerization was varied for both the PSf and TFC
membranes in an attempt to alter the amine coverage. The area
of peak 1666 cm−1 was plotted in contour color maps to
evaluate the homogeneity of the chemical distributions on the
surface of the materials. Thus, synchrotron ATR-FTIR
mapping, Figure 4c, shows the amine group content for both
of these membranes after different treatment times, with
respect to the absorption at 1666 cm−1. This peak was found to
proportionally increase with longer plasma treatment times for
both PSf and TFC membrane materials. Equation 1 was used to
estimate the thickness of the plasma coating by evaluating the
penetration depth of the infrared beam across this particular
layer and lowered both salt rejections by 2%. For 15 min, the
film deposition appeared to have more penetrating ruptures but
only enough to lower salt rejection by 4%. The selectivity drops
from the 5 and 9 min membranes were still very close to the
variations of the RO membrane under a variety of system
conditions and configurations.52
The pristine membranes under air- and vacuum-dried
conditions showed flux decline by 78%. The membranes
exposed to argon plasma did not show superior decline than
the dried pristine with flux drops around 60 to 64% (Figure 3a),
which led to the conclusion that flux was not altered by plasma.
Furthermore, the flux of the plasma polymerized membranes
presented in Figure 3b showed a similar average flux decline
trend to that of dried control membranes. Therefore, the
impact on the flux was more associated with the degree of
dryness of the material than with the low pressure plasma
polymerization process.32 The drying step prior to the plasma
process suggests an effect of membrane voids collapse that led
to flux loss.31 Therefore, cleaning procedures, including solvent
exchange and atmospheric pressure conditions for plasma
polymerization of TFC membranes, may lead to less impact on
membrane permeation once no drying step is required.37,33,53
Characterization of amine moiety distribution and
chemical properties after plasma polymerization. The
amine thin-film chemical profile was investigated with ATRFTIR analysis of modified PSf as a reference material (Figure
4a), TFC membrane (Figure 4b), and TFC membrane exposed
to only argon plasma (Figure S2). Cross-linking bonds were
identified with the formation of a broad band corresponding to
a carbonyl (CO) stretching vibration around 1723 cm−1, an
F
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Figure 5. (a) Streaming potential for TFC-pristine with isoelectric point for amine rich membranes between pH 3.7 and 5.2. (b) Correlation
between increased amine groups detected by streaming potential and increased N/C ratio detected by XPS after plasma polymerization.
wavelength range.57 The degree of amine enrichment for the
PSf membrane was estimated to be between 250 nm, 290 nm,
and 345 nm for 5, 9, and 15 min plasma polymerization times,
respectively.
Higher amine densities could be measured for the TFC
membranes as a result of plasma polymerization, particularly
between 9 and 15 min. This corresponded to thicknesses of 21
and 60 nm, respectively. The 5 min of plasma polymerization
duration offered the least amine enrichment coverage, and the
thickness of the layer could not be satisfactory evaluated. The
density of the C−N stretching vibration as seen on the contour
plot map before plasma polymerization showed irregular
distribution across the surface of pristine TFC membranes.
However, after plasma polymerization, the density of these
functionalities increased with longer plasma polymerization
times, leading to a more homogeneous distributionthis was
especially evident after 15 min.
The surface charge was also investigated as a function of pH
(Figure 5) in order to set the best conditions for selectivity of
modified membranes. This analysis highlights the protonation
and deprotonation of amine groups and nascent carboxylic
groups on the surface. Polymeric membrane materials are
charged when in contact with an aqueous medium.58
Electrostatic interactions between the solution and the
membrane result in an electric double layer, and the resultant
charge on the surface can be evaluated as the zeta potential.
The zeta potential is dependent on the compositions of the
membrane surface and the ambient solution. For this reason,
this analysis was also performed for pristine and TFC
membranes exposed to argon plasma alone (Figure S3) in
order to investigate chemical reactions promoted by the
polymerization process. The curve profile for a pristine
membrane shows a flat negatively charged surface (∼30 mV)
over the pH range of 3 to 9.59 For amine rich surfaces, at low
pH, the magnitude of positive charge increased with increasing
plasma time compared to the control, most notably between 5
and 9 min (15 min yielded a similar surface property to 9 min).
This can be attributed to the protonation of the added
functional amine groups due to plasma polymerization.
Furthermore, the isoelectric points were found at pH 3.7 for
5 min, and for 9 and 15 min exposures, they increased to 4.7
and 5.2, respectively, consistent with an increase of basic amine
mieties on the surface. On the other hand, as pH increased
from 6, all amine rich samples showed proportional surface
charges increasing in magnitude of negative charge between
−40 and −50 mV at pH 8. This effect is more reflective of the
deprotonation of amine groups and nascent carboxylates
groups.60 Another potential contribution is associated with
formed carboxylates upon reaction with air after removal from
the plasma chamber, which is supported by the increased
carboxylic bands shown in Figure 4b. The membranes exposed
to argon plasma alone showed a similar curve profile to that of
the pristine, with slightly increased magnitude of negative
charge (∼ −40 mV at pH 8), while the influence of negative
charge was more attributed to available nascent carboxylic
groups. The increased amine presence on the surface is also
consistent with the increase in the N/C ratio, as measured by
XPS (Figure 5b). Furthermore, selectivity was affected for the
denser amine coverage of the 9 and 15 min membranes in
different intensities. As the feed solution was ∼6, the 15 min
membrane operated under the influence of the IEP at pH 5.2.
Minimum rejections can occur with feed solution either at or
above one or two pH units higher than the IEP.61,62 Therefore,
results led to agreement that 9 min is the optimum time with
potential pH operation conditions in the alkaline range.
Characterization of attached silver nanoparticles on
the amine rich TFC membranes. The membranes
confirmed to have increased amine functionalities were then
exposed to silver nanoparticles to explore the novel metal
binding mechanism. The enhanced binding of silver was shown
in a wide scan XPS spectrum, Figure S4b, as compared to the
pristine membrane (Figure S4a). As a further confirmation of
the silver presence, a closer analysis of the silver peak (Figure
S4c) shows the Ag3d core level spectrum split into two peaks at
372 and 366 eV, indicating Ag 3d 5/2 and Ag 3d3/2 ,
respectively.63 The percentage of silver was 6% by wt (or 1
at % equivalent) (Table S1) measured by EDS (Figure S5) at 3
keV.
The silver functionalized membranes were tested for
antimicrobial properties by exposure to E. coli. A number of
studies have correlated the silver ions release with the bacteria
elimination mechanism and, as well, the biocidal lifespan.45 The
release rates are mainly influenced by the particle size and pH
conditions, although some limitations on the methodology for
separation of nanoparticles and ions prior to detection
potentially can led to experimental artifacts.64 The particle
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Figure 6. Bacteria assessment with increased inhibition zone distance associated with amine rich and Ag NPs attached on membrane surfaces: (a)
TFC-pristine, (b) TFC-VIm-5Ag, (c) TFC-VIm-9Ag, and (d) TFC-VIm-15Ag.
etching is time dependent over a 6−24 h observation period.65
For particles around 20 nm under neutral aqueous medium as
used in this study, fast biocidal activity (∼2−4 nm/h) enabled
elimination of bacteria in the first 5 h and elimination
maintained within 24 h.66,67 Inhibition zones indicating
antimicrobial activity are shown in Figure 6. The inhibition
zone showed different distance ranges which could be
potentially caused by the aggregation/agglomeration of the
Ag NPs, and therefore, the average was measured from five
points. The pristine membrane, Figure 6a, shows a dense
bacterial area with no inhibition zone. For the 5 min plasma
exposure membrane treated with silver, inhibition zones started
to appear, in contrast to the bacteria-free valleys that are clearly
identified as dispersed “bubbles”, and the average was 304 μm
with minimum distance of 77 μm. For 9 and 15 min (Figure 6c
and 6d), inhibition zones were more defined with an average of
342 and 330 μm and minimum distances of 266 and 115 μm,
respectively. The amine enrichment was therefore found to be
directly correlated to the diameter of the inhibition zones and
also showed minimum distances were less likely for longer
polymerization times. This suggests that longer plasma
polymerization durations lead to more coordination sites
being available for silver attachment.
While the silver attachment and associated antimicrobial
functionality have been demonstrated, the effect of leaching
over time is an important issue. Silver leaching from chemically
modified silver nanoparticles bonded to the surface of TFC
membranes showed Ag+ release lasting months during
operational cross-flow filtration.68 This indicates that silver
modified membranes may require reloading of silver nanoparticles, possibly during routine cleaning of the operating
membrane plant. Therefore, further research is needed to
investigate the long-term stability of the attached amine groups,
as well as the attached silver nanoparticles, during operation
conditions to confirm the viability of plasma polymerization for
improved performance of TFC membranes.
CONCLUSIONS
Plasma polymerization demonstrated feasibility for adherence
of amine functionality onto PA layer in thin-film composite
membrane. The coating thickness was readily controlled by
exposure time, which influences film density and homogeneity.
An increasing value for the surface isoelectric point with
increasing polymerization time was consistent with increasing
amine enrichment which it benchmarked optimum pH
conditions suitable for amine rich membranes. Enhanced
metal binding to the added amine groups was demonstrated
with silver nanoparticles, where antimicrobial property was
confirmed.
■
■
ASSOCIATED CONTENT
S Supporting Information
*
Figure S1: SEM topographical analysis of TFC membranes
exposed to argon plasma Figure S2: ATR-FTIR analysis of TFC
membranes exposed to argon plasma Figure S3: Streaming
potential analysis for membranes exposed to argon plasma
Figure S4: XPS analysis of silver peak and Ag 3d core level
Figure S5: EDS spectra of silver peak Table S1: XPS contents
from plasma polymerized membranes and Ag NPs attachment
″This material is available free of charge via the Internet at
http://pubs.acs.org/.″The Supporting Information is available
free of charge on the ACS Publications website at DOI:
10.1021/acsami.5b01603.
■
AUTHOR INFORMATION
Corresponding Author
*E-mail: rackel.reis@live.vu.edu.au; Tel: +61406903950.
Notes
The authors declare no competing financial interest.
ACKNOWLEDGMENTS
The authors would like to acknowledge Ph.D. stipend and
project funding from the Collaborative Research Network
initiative of the Australian Department of Industry. R.R.
■
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acknowledges the postgraduate top up scholarship from the
National Centre of Excellence in Desalination Australia, funded
by the Australian Government through the National Urban
Water and Desalination Plan. The authors also acknowledge
Mark Tobin, Lilijana Puskar, and Danielle Martin from the
Australian Synchrotron (Melbourne), Robert Jones from
Centre for Materials and Surface Science, Department of
Physics in La Trobe University, Bao Lin for AFM contribution,
Maëlle Lemoing from Deakin University for bacteria assessment, and Jianhua Zhang from Victoria University for access to
the filtration system.
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