Journal Pre-proof Bacterial biofilm formation on ion exchange membranes Moshe Herzberg, Soumya Pandit, Meagan S. Mauter, Yoram Oren PII:
S0376-7388(19)32087-3
DOI:
https://doi.org/10.1016/j.memsci.2019.117564
Reference:
MEMSCI 117564
To appear in:
Journal of Membrane Science
Received Date: 10 July 2019 Revised Date:
10 October 2019
Accepted Date: 11 October 2019
Please cite this article as: M. Herzberg, S. Pandit, M.S. Mauter, Y. Oren, Bacterial biofilm formation on ion exchange membranes, Journal of Membrane Science (2019), doi: https://doi.org/10.1016/ j.memsci.2019.117564. This is a PDF file of an article that has undergone enhancements after acceptance, such as the addition of a cover page and metadata, and formatting for readability, but it is not yet the definitive version of record. This version will undergo additional copyediting, typesetting and review before it is published in its final form, but we are providing this version to give early visibility of the article. Please note that, during the production process, errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain. © 2019 Published by Elsevier B.V.
Bacterial Biofilm Formation on Ion Exchange Membranes
Moshe Herzberg1*, Soumya Pandit1, Meagan S. Mauter2, and Yoram Oren1
Revised version submitted to Journal of Membrane Science October 10, 2019
1
Ben-Gurion University of the Negev
The Jacob Blaustein Institutes for Desert Research Zuckerberg Institute for Water Research Sede Boqer Campus, Midreshet Ben-Gurion, 84990, ISRAEL 2
Carnegie Mellon University
Department of Civil & Environmental Engineering 5000 Forbes Ave., Pittsburgh, PA, 15213, USA
*
Corresponding author:
Phone + 972 8 6563520; Fax + 972 8 6563503; E-mail:
[email protected]
1
1
Abstract
2 3
Ion exchange membranes (IEMs) often suffer from biofouling, which reduces ion exchange rates
4
and increases energy consumption in water treatment processes, such as electrodialysis, reverse
5
electrodialysis, membrane capacitive deionization, and Donnan dialysis, and in energy devices,
6
such as microbial fuel cells. In the present study, microbial biofilm formation was studied on
7
anion exchange membranes (AEMs) and a cation exchange membranes (CEMs) of the
8
homogeneous and heterogeneous types. Biofilm formation of Pseudomonas aeruginosa PAO1
9
on the IEMs was higher on the CEMs than on the AEMs, although more dead cells were found
10
on the AEMs, likely due to the presence of quaternary ammonium moieties on the AEM surface,
11
which are bactericidal. An XTT assay and NPN uptake tests confirmed the antimicrobial
12
properties of the AEM surface. The results also suggested that the surface roughness of the
13
membranes affected interactions between bacteria and the IEMs, being more pronounced on the
14
heterogeneous IEMs than on the homogeneous IEMs. Counter-ion transport properties were
15
studied under the Donnan exchange regime for both pristine and biofouled IEMs. The reduction
16
of counter-ion transport due to biofouling was more pronounced for heterogeneous CEMs and
17
AEMs than for their homogeneous counterparts, while it was more noticeable for the AEMs than
18
for the CEMs. The latter result is explained based on the preferential adsorption of the negatively
19
charged EPS components to the positively charged AEMs.
20 21 22 23 24 25 26 27 28 29 30 31 32
Keywords: ion exchange membranes; biofilm; XTT assay; specific conductivity; Donnan
33
exchange; intracellular reactive oxygen species 2
34 35 36
1. Introduction
37
treatment-related processes, such as electrodialysis and Donnan dialysis and devices such as fuel
38
cells, which have a plethora of industrial applications [1]. They have been applied widely in
39
advanced engineering tools for desalting, concentrating and modifying products in seawater
40
desalination, industrial wastewater treatment, and beverage and food engineering processes [2].
41
Recently, IEMs have been utilized in energy conversion and storage technology, including
42
reverse electrodialysis for blue energy harvesting [3], membrane capacitive deionization [4],
43
contaminant removal and wastewater treatment in ion exchange membrane bioreactors[5] and
44
microbial desalination cells [6] as examples of promising cutting-edge technologies. Biofouling
45
of IEMs poses serious concerns, when the membranes are exposed to aquatic environments.
46
Thus, reducing biofouling of IEMs is essential to achieve optimal process performance as
47
microbial biofilms and their components present a major obstacle for maintaining the IEMs’
48
long-term effectiveness [7].
Ion exchange membranes (IEMs) are important components in energy generation and water-
49
Owing to the presence of fixed ionic charges in their interior, the IEMs are utilized to separate
50
ionic species from solutions containing neutral components by applying electrical fields or
51
concentration gradients [8]. Suspended solids carrying positive or negative electrical charges and
52
colloidal matter, such as polyelectrolytes, humic acids, surfactants, biological materials and
53
multivalent salts, near the saturation level, can cause severe problems when using IEMs (e.g., in
54
electrodialysis) due to precipitation on the membrane surface or by partial penetration into the
55
membranes. When this occurs, it may be followed by a dramatic increase in the membrane
56
electrical resistance. Since most of the colloids present in natural waters are negatively charged,
57
the anion exchange membranes are mostly affected by their presence [7]. Lindstrand
58
demonstrated that negatively charged solutes, such as octanoic acid and anionic surfactants
59
(sodium octanoate and sodium dodecylbenzene sulfonate), are responsible for a higher degree of
60
fouling on anion exchange membranes (AEMs), while cation exchange membranes (CEMs) are
61
marginally affected by those foulants [9]. Bukhovets et al. studied biofouling of the
62
heterogeneous anion exchange membrane MA-41 in an electrodialysis stack in the presence of
63
amino acids and observed maximum fouling, close to the limiting current density [10].
64
Consequently, membrane electrical conductivity decreased significantly in the presence of
65
phenylalanine.
66
Bacteria-mediated biofouling is caused by attachment of planktonic bacteria, followed by
67
the proliferation of sessile colonies on the membrane surface and maturation of the microbial 3
68
biofilm [11]. Previous work on bacterial attachment and biofilm formation has identified key
69
surface properties that promote biofilm growth: Hydrophobic rough surfaces, which include H-
70
bond donors and lack H-bond acceptors with low toxicity, usually promote bacterial attachment
71
and biofilm [12,13]. There is a lack of information on bacteria-mediated biofouling of various
72
categories of IEMs, as well as the effects on membrane performance, related transport
73
mechanisms, and particularly, the influence of the fixed charged groups of the IEM surface on
74
biofilm formation. In this study, commercially available homogeneous and heterogeneous IEMs
75
were investigated for their biofouling propensity using mono-culture biofilm experiments.
76
Variations of biofilm components and the related production of reactive oxygen species (ROS)
77
were analyzed in response to the membrane type. The mode of action by which biofilm
78
formation was affected was related to a comprehensive characterization of the IEM surface. The
79
effect of biofilm formation on counter-ion transport under the Donnan exchange regime was
80
tested as well.
81 82
2. Materials and Methods
83 84
2.1 Membrane conditioning.
85
The IEMs were conditioned prior to their use according to the following procedures.
86
Heterogeneous membranes were cleaned with acetone in order to remove wax/oily coatings from
87
the membranes. This step was followed by immersing the dry membrane in 50% (v/v) ethanol
88
for at least 6–8 h. Further, both homogeneous and heterogeneous IEMs were kept in a saturated
89
NaCl solution (300 g/L) for 12 h with gentle stirring. Before use, the membranes were washed
90
for 30 min with double distilled water (DDW) followed by exposing the membranes to a 10%
91
LB medium in the flow cell device.
92 93
2.2 Characterization of the anion and cation exchange membranes
94
The types of the commercial ion exchange membranes and their prime characteristics are
95
presented in Table 1. All the membranes were analyzed for surface roughness topology, surface
96
charge, and hydrophobicity [14].
97 98 99 100 101
4
102 103
Table 1: Specification of the commercially available IEMs used in the present study Type
Heterogeneous
Commercial name
Company, Country
MA40
MK40
Polyethylene Shchekinoazot, Russia
Thickness
RR'NH,
0.51
(mm)
Polyethylene
–SO3H
0.54
Polyethylene
R (CH3)3N+
0.72
Polyethylene
R - SO3-
0.64
N.A.
R- SO3-
0.34
N.A.
RR'R"N
0.37
Polyethylene
R (CH3)3N+
0.21
CMT
Polyethylene
R–SO3H
0.2
AMV
N.A.
N.A
0.14
AMH-PES
Mega,
RALEX®
Czechs
CMH-PES
Republic
Excellion I-200 Excellion I-100
SnowPure USA
LLC,
AMT Asahi Glass, Japan
CMV
Selemion, Japan
N.A.
N.A
0.16
AEX
Neosepta, Alstom, Japan
N.A.
N.A
0.18
N.A.
N.A
0.17
CMX 104
Fixed ionic group
RR'R"N
RALEX®
Homogeneous
Inert binder
N.A.: Not available
105 106
Surface hydrophobicity/hydrophilicity: Hydrophobicity of the different surfaces was determined
107
by the captive bubble contact angle method using the OCA 20 (DataPhysics, Filderstradt,
108
Germany) instrument. The IEMs were immersed in DDW overnight for conditioning at room
109
temperature prior to measurement. The analysis was carried out by placing a 10-µL air bubble
110
onto the surface; contact angles were measured using SCA-20 software (DataPhysics) by
111
drawing the surface baseline and drop profile and calculating the angle at the line of the three-
112
phase contact. At least five measurements were taken for each sample. In this case, a higher
113
contact angle indicates higher hydrophilicity. 5
114
Zeta potential: Zeta potentials of the IEM surfaces were determined at different pH values using
115
a Zeta potential analyzer (SurPass Elektrokinetic Analyzer, Anton Paar, Austria). As an
116
electrolyte, 0.1 mM KCl was used, and 0.1 N NaOH and 0.1 N HCl were used for adjusting the
117
pH.
118
Surface topography: Atomic force measurements were performed on the pristine IEM surfaces
119
for a surface roughness comparison. Imaging of the surface topography was performed using a
120
Nanoscope IIID MultiMode AFM microscope (Veeco-DI, Santa Clara, CA, USA) using an NP-S
121
cantilever with a spring constant of 0.06 N/m in tapping mode. The AFM image scanning area
122
was 25 µm2, and scans were carried out in air[14]. The temperature of the sample was monitored
123
during the scans. Roughness indices were estimated using the method of root-mean-square for
124
the Z-plane at a resolution of 5 µm2.
125
2.2 Biofilm growth on different IEM surfaces in a flow cell
126
Twelve different IEMs (Table 1) were placed in a flow cell for determination of biofilm
127
formation. For this purpose, an FC 81-PC transmission flow cell (BioSurface Technologies
128
Corporation, MT, USA) was used. The flow cell was sterilized with 70% ethanol for 30 min
129
followed by a thorough rinse with sterile DDW for 60 min [14].
130
Preparation of Pseudomonas aeruginosa PAO1 inoculum: The P. aeruginosa PAO1 strain, a
131
well-characterized Gram-negative bacterium that has become the most accepted model organism
132
for studying biofilm formation, was used in this study. Here, three independent biofilm
133
experiments were initiated from a stationary phase overnight culture of P. aeruginosa PAO1.
134
Each culture originated from one distinct bacterial colony. After 8.5 h of incubation at 30°C and
135
150 rpm stirring, the liquid culture was diluted 100 × in LB broth and incubated overnight. A
136
volume sample of 80 mL of the overnight culture was washed three times in 100 mM of NaCl
137
solution, and the optical density of the bacterial suspension was adjusted to OD600 nm of 0.1.
138
This suspension was used as the inoculum for biofilm growth in the flow cells and the Donnan
139
exchange experiments.
140
Biofilm formation studies: The washed bacterial suspension was injected into the flow cell at a
141
rate of 2 mL/min (shear rate of 27 s-1) for 40 min [14]. After the bacterial deposition phase, a
142
bacterial growth medium was injected for 24 h at 2 mL/min. The growth medium (10% LB
143
solution) consisted of 1.0 g/L of Bacto Tryptone (Becton, Dickinson and Company), 0.5 g/L of
144
yeast extract (Becton, Dickinson and Company), and 100 mM of NaCl (Merck), and adjusted to
6
145
pH 7.0 ± 0.1. The average biovolumes of dead cells, live cells and extracellular polymeric
146
substances (EPS) for four different types of IEMs (homogeneous CEM, homogeneous AEM,
147
heterogeneous CEM, and heterogeneous AEM) were calculated and plotted for comparison.
148
Confocal laser scanning microscopy (CLSM) and imaging: Fouled membranes were carefully
149
removed from the flow cell and cut into pieces of around 5 mm × 5 mm from a similar location
150
in the middle of the membrane coupon. A biofilm staining solution (Molecular Probes, Inc.) was
151
prepared by mixing 5 µM of SYTO 9™ (live cell stain), 3 µM of propidium iodide (PI, dead cell
152
stain), and 0.1 mg/mL of Concanavalin A conjugated to Alexa Fluor 633 (binds to alpha-linked
153
mannose residues of EPS) in a phosphate buffer saline (PBS) solution at pH 7.2 (Invitrogen).
154
Biofilms were incubated in the staining solution for 30 min in the dark. The stained biofilm
155
samples were visualized using a CLSM ZeissMeta510 (Carl ZEISS, Inc., USA) equipped with
156
Zeiss dry objective LCI Plan-Neo Fluor (20 × magnification and numerical aperture of 0.5).
157
Images were analyzed, and the specific biovolume (µm3/µm2) in the biofouling layer was
158
determined by COMSTAT, an image processing software, written as a script in Matlab 6.5 (The
159
Math Works, Inc., Natick, MA, USA) and equipped with an image-processing tool box [15]. For
160
every sample, six positions on each IEM were chosen and microscopically observed, acquired,
161
and analyzed. A three-dimensional reconstruction of the CLSM image stacks was carried out
162
using Imaris software (Imaris Bitplane, Zurich, Switzerland). Averages of the biovolumes of live
163
and dead cells and EPS for four different IEM categories (each category has three different
164
commercial IEMs; Table 1) were calculated and compared.
165
2.3 Antimetabolic activity of IEM surface on P. aeruginosa PAO1
166
In order to investigate the antimetabolic activity of the IEM surface on attached biofilm, XTT, a
167
colorimetric 2, 3-bis (2-methoxy-4-nitro-5-sulfophenyl)-5- [(phenylamino) carbonyl]-2H-
168
tetrazolium hydroxide (XTT) reduction assay was carried out [16]. The electron transport system
169
in the cellular membrane of live bacteria reduces the XTT tetrazolium salt to formazan, which
170
can be measured spectrophotometrically. N-methyl dibenzo pyrazine methyl sulfate (PMS) was
171
used as an electron mediator transferring electrons from the bacterial outer membrane to
172
XTT[17]. On the other hand, nonviable bacteria are unable to reduce tetrazolium salt. By virtue
173
of the XTT assay, the antimetabolic activity of the IEM surface on attached biofilm can be
174
determined. In the present study, the biofouled IEM was removed from the flow cell after 18 h
175
of the experiment and cut into three pieces. Each piece of 1.6 cm × 1.2 cm covered with P.
176
aeruginosa PAO1 biofilms was gently washed with PBS to remove non-adherent bacteria. Each 7
177
IEM sample was added to a 15-ml centrifuge tube (Falcon™ 15 mL Conical Centrifuge Tubes)
178
containing XTT/PMS buffered solution [16]. The XTT stock solution was prepared by dissolving
179
10 mg of XTT (Thermo Fisher Scientific) in 10 ml of 10% LB solution. Ten mM of the (N-
180
methyl dibenzo pyrazine methyl sulfate) PMS solution in phosphate-buffered saline (PBS) was
181
prepared by dissolving 3 mg PMS (AppliChem, Darmstadt, Germany) into 1 mL PBS (Sigma-
182
Aldrich). The XTT/PMS mix solution was prepared by supplementing the 10 mL of XTT
183
solution with 25 µL of the PMS solution. Each falcon tube containing one IEM piece was filled
184
with 1.5 ml of autoclaved PBS buffer and 1 mL of XTT/PMS mix solution. Falcon tubes were
185
then incubated at 30 ºC for 2 h. Then, 150 µl from each sample was taken to a 96-well
186
transparent plate (Greiner 96 Flat Bottom Transparent Polystyrol). The results of the colorimetric
187
change due to formazan production were measured at 450 nm with multimode reader device [14]
188
(Infinite 200 PRO, Tecani-control).
189
An additional set of control experiments for this test was done with a similar size of different
190
pristine IEMs (namely, in the absence of bacteria) to ensure that XTT does not adsorb on IEM
191
surfaces and that the IEM surfaces do not oxidize XTT to formazan. A calibration curve for the
192
reduction of XTT to formazan by P. aeruginosa PAO1 was provided elsewhere [14]. The
193
average absorbance values for four different categories of IEMs (homogeneous CEM,
194
homogeneous AEM, heterogeneous CEM, and heterogeneous AEM) were calculated, and a
195
graph was plotted.
196
2.4 The effect of IEM surface exposure to the bacteria on cell membrane permeation
197
P. aeruginosa PAO1 membrane permeation assays were performed by using fluorescent
198
hydrophobic probe 1-N-phenylnaphthylamine (NPN) uptake as a tool to investigate whether the
199
exposed fixed ionic groups of the IEM have any impact on the bacterial cell membrane. The
200
ability of any chemical substance to cause damage to the bacterial outer cell surface has been
201
extensively quantified by NPN uptake assay [18]. Owing to its hydrophobic nature, the NPN is
202
unable to percolate through intact bacterial membranes and therefore exhibits a weak
203
fluorescence emission. On the contrary, NPN uptake should increase with damaged (functionally
204
invalid) outer membranes. Hydrophobic chemical agents such as NPN cannot be absorbed to the
205
bacteria due to the orientation of the LPS present on the outer side of the bacterial membrane
206
[18]. Therefore, bacteria with impaired cell membranes emit high fluorescence compared to non-
207
damaged ones [19]. In the present experiments, four different IEMs from each category were
208
chosen for biofilm formation in NPN uptake assays; these were CMV for homogeneous CEMs, 8
209
AMV for homogeneous AEMs, MK40 for heterogeneous CEMs, and MA40 for heterogeneous
210
AEMs, respectively. NPN was added to the 12-h-old biofilm, on the different IEM surfaces at a
211
concentration of 10 µM. After 30 min of incubation, the excess amount of NPN was washed
212
gently with 0.85% NaCl solution. The uptake of NPN was determined by measuring the
213
fluorescence emitted at 420 nm after excitation at 350 nm using an argon laser in the CLSM
214
[19]. CLSM images were generated using the Zeiss LSM Image Browser. Colored images were
215
analyzed with COMSTAT to determine the biovolume (µm3/µm2) as described in the previous
216
section, and imaging was done with IMARIS v7.5 software (IMARIS Bitplane, Zurich,
217
Switzerland).
218
2.5 Assessment of bacterial intracellular oxidative stress
219
The bacterial intracellular oxidative stress was assessed by quantification of reactive oxygen
220
species (ROS) inside the bacterial cell. The ROS-sensitive green fluorescent dye 2′, 7′-
221
dichlorodihydrofluorescein diacetate (DCFH-DA) (Sigma-Aldrich, Israel), which is converted to
222
dichlorodihydrofluorescein in the presence of intracellular ROS [20], was used. This test was
223
conducted because it was hypothesized that the presence of a charged surface close to bacterial
224
biofilm can cause oxidative stress, which is a reason for the overproduction of intracellular free
225
radicals [21]. The amount of intracellular ROS was estimated from dichlorodihydrofluorescein
226
(DCF) production measured at 480-nm excitation/530-nm emission [22]. The four different
227
IEMs (CMV, AMV, MK40 and MA40) were considered for this test. The biofilm was allowed to
228
grow for 12 h on the surface of the IEMs. The DCFH-DA was added immediately to the IEMs
229
with biofilms at a concentration of 5.0 µg/ml (dissolved in ethanol) after which the cells were
230
incubated for 30 min. Next, the excess amount of DCFH-DA dye was carefully washed with
231
phosphate buffer (pH 7.2), followed by CLSM imaging performed on the biofilms.
232
2.6 Performance of biofouled IEMs during Donnan exchange
233
Counter-ion transport ability in terms of ion diffusion flux was determined and compared
234
between pristine and biofouled IEMs in a customized Donnan dialysis setup [23]. In the Donnan
235
exchange, the concentration gradients across the studied membrane separating two solutions with
236
different compositions are the driving force for counter-ion transport. A rectangular Plexiglas
237
cell, with feed and receiving compartments (9.1 cm long × 4.5 cm wide) and a channel height of
238
0.44 cm separating a single ion exchange membrane (IEM) with an active area of 41 cm2, was
239
used for these experiments. The solutions were delivered to each compartment from 2.5-L
240
vessels and circulated by two-headed centrifugal pumps (MRC Ltd., Israel) at flow rates of 3.2 9
241
L/h (linear velocity 1.13 cm/sec) from/to the feed/receiving compartments. All experiments were
242
performed at 26 ± 10 ºC, controlled by an aquarium heater (Aqua One, Chung Xing. Co. Ltd.).
243
The different solutions and counter-ions determined for their fluxes are listed in Table 2.
244 245
Table 2: Description of the solutions in the feed and receiving compartments for the Donnan
246
exchange experiments Studied membranes CEMs (CMV, MK40) AEMs (AMV, MA40)
Receiving compartment NaCl (1M)
Feed compartment KCl (1M)
Counter-ion measured K+
NaCl (1M)
Na2SO4 (1M)
SO4-2
247 248
A customized cylindrical flow cell (height 21 cm, radius = 8 cm) of ≈ 4-L volume was used for
249
biofilm formation on the surface of four different categories of IEMs (CMV, homogeneous
250
CEM; AMV, homogeneous AEM; MK-40, heterogeneous CEM; and MA-40, heterogeneous
251
AEM) (Figure S-1, SI). The same growth medium was used and the same inoculum preparation
252
technique was followed as mentioned earlier (biofilm growth on different IEM surfaces in a flow
253
cell). Feed solution was injected to the flow cell without recirculation using a peristaltic pump
254
(Masterflex, Cole-Parmer) at a flow rate of 2 mL/min for 6 d (144 h). After this period, IEMs
255
were collected aseptically, gently washed with the background solution, and used for the Donnan
256
exchange experiment (Figure S-2, SI).
257
Counter-ion flux was determined by tracking the change in sulfate and potassium concentrations
258
as a function of time in the receiving compartment for AEMs and CEMs, respectively [23]. For
259
the Donnan dialysis experiment with AEMs, the Standard 4500E Turbidimetric Method was
260
used for determining sulfate concentration, where sulfate is precipitated as BaSO4 by the
261
addition of barium chloride. The turbidity of the BaSO4 suspension was then measured using a
262
spectrophotometer (Lambda EZ201 Perkin Elmer). For the CEMs, potassium samples were
263
analyzed by ICP (Varian 720-ES, Australia) for determining sulfate and potassium
264
concentrations. All the samples were diluted (20 ×) prior to ICP analysis due to the high sodium
265
concentration of the samples [23]. Counter-ion transport ability in terms of ion diffusion flux was
266
determined and compared between pristine and biofouled IEMs.
267 10
268 269 270
3. Results and Discussion
271
3.1 IEM surface characterization
272
3.1.1 Evaluation of IEM surface hydrophobicity
273
Surface hydrophobicity was estimated by the contact angle of a captive air bubble under the
274
aquatic conditions applied during the biofilm formation experiments [24]. Prior to the contact
275
angle measurement experiments, IEMs were soaked overnight in 10% LB solution under aseptic
276
conditions. The captive air bubble contact angle test results, presented in the supplementary
277
information, show that the AEM and CEMs’ surfaces are relatively hydrophilic according to
278
their large captive air bubble contact angle range of 128–150º (Table S1 and Figure S-2). Note
279
that although most of the results show that AEM surfaces are more hydrophilic than the CEM
280
surfaces, the differences in contact angles, in most cases, were not significant.
281 282
3.1.2 Roughness estimation with AFM
283
AFM contact mode scans were carried out on the various IEMs. Roughness indices were
284
estimated at a resolution of 5 µm2, using the method of root-mean-square for the Z-plane. The
285
3D and 2D visualization of the AFM scans are provided in Figure 1 and Figure S-4
286
(supplementary information), respectively. Previous studies showed that larger surface roughness
287
facilitates more biofilm formation: Nano- and micro-scale surface roughness commonly
288
enhances the adhesion of bacteria to substrates during the initial steps of colonization as it
289
provides more surface area for cell attachment [25]. Accordingly, the higher average roughness
290
values of the heterogeneous IEMs likely play a role in their biofouling propensity (Figure 1).
291 292 293
11
294 295 296 297 298 299 300 301 302 303 304 305 306 307 308 309 310 311 312 313 314 315 316 317 318 319 320 321 322 323 324
Figure 1: Roughness of different IEMs: Top panel- Average roughness values of different
325
categories of IEMs; Bottom panel- 3D visualization of the commercial IEMs: (A) Heterogeneous
326
AEM (MA-40); (B) Heterogeneous CEM (MK-40); (C) Homogeneous AEM (AMV); (D)
327
Homogeneous CEM (CMV) at a resolution of 5 µm2.
328 329 330
3.1.3 Evaluation of zeta potential of IEM surface
331
In order to determine the possible impact of electrostatic interactions between the IEM surface
332
and the bacterial cell membrane, the surface zeta potential of the IEMs was analyzed, while the
333
zeta potential of the cells under similar aquatic conditions was studied elsewhere [26]. Zeta
334
potential values of the different IEMs used in this study are depicted in Figure 2 for a pH range 12
335
of 4 to 10. Larger negative zeta potential values were detected for both the homogeneous and
336
heterogeneous CEM surfaces than for the AEM surfaces, indicating that a relatively stronger
337
electrostatic repulsion is expected between the bacterial cells and the CEM surface. Owing to the
338
presence of carboxylate groups in the lipopolysaccharides (LPS) of the outer cell membrane of
339
P. aeruginosa PAO1, these cells possess a negative surface charge (as expressed by negative
340
zeta potential values) between a pH of 2.2 and 11 [27]. On the contrary, zeta potential values of
341
both homogeneous and heterogeneous AEMs were at a positive magnitude (approximately
342
within the range of +5 mV to +35 mV), indicating the presence of positively charged fixed
343
groups on the surface of the AEM. Owing to the presence of the positive charge, a higher degree
344
of bacterial and EPS attachment is expected to take place due to electrostatic attraction [28]. The
345
CEM displayed a slightly negative charge (approximately within the range of -10 mV to -85
346
mV), in 0. 1 mM KCl, correlating to the charge of the sulfonate functional groups, which may
347
result in the repulsion of the negatively charged bacterial cell surfaces and EPS.
348 349 350 351 352 353 354 355 356 357
Figure 2: Zeta potentials of different commercial IEMs as a function of pH: CEMs (left panel)
358
include homogeneous (CMV and CMT) and heterogeneous (MK-40 and CMX) surfaces. AEMs
359
(right panel) include homogeneous (AMV and AMT) and heterogeneous (MA-40 and AEX)
360
surfaces. All samples were measured in 1 mM of KCl solution and titrated with 100 mM of HCl
361
or 100 mM of NaOH.
362 363 364
3.2 Quantification of biofilm formation
365
In this part of the study, we evaluated the effect of IEM surface on the magnitude of biofilm
366
formation, while the hydrodynamic conditions in the flow cell were maintained as constant.
367
Figure 3 shows representative CLSM images of biofilm formed on different IEM types. A 13
368
quantitative analysis of the dead and live cells is presented in Figure 4. The IMARIS 3D images
369
in Figure 3 show a presence of predominantly dead cells on the AEMs (Figures 3 A and C),
370
while EPS and live cells were more visible on the heterogeneous CEM (Figure 3 D). Further, it
371
can be inferred that none of the IEMs were capable of inhibiting biofilm development. Likely,
372
once bacterial cells and EPS overrode the charged functional group of the underlying IEMs,
373
biofilm could grow [29,30].
374
375 376 377
Figure 3: P. aeruginosa PAO1 biofilms formed on different types of IEMs as observed with
378
CLSM: (A) Homogeneous AEM (AMV); (B) Homogeneous CEM (CMV); (C) Heterogeneous
379
AEM (MA-40); and (D) Heterogeneous CEM (MK-40) after 24 h of biofilm formation. The red,
380
green, and blue clusters indicate dead cells, live cells, and EPS, respectively. Orange clusters
381
indicate an overlapping zone of dead cells and live cells. Each image (A–D) is a perspective of a
382
600 µm × 600 µm image.
383 384 385 386 387
14
388
389 390
Figure 4: Biofilm formation on IEMs: Left panel – Average biovolumes of dead and live cells
391
on the different commercial IEMs after 24 h. Right panel – Ratio of biovolumes of dead/live
392
cells in biofilms formed on the different commercial IEMs after 24 h. X-axis legend: (A)
393
Homogeneous AEMs include AMV, Neosepta AEX and AMT; (B) Heterogeneous AEMs
394
include Ralex AEM, MA-40 and Excellion I-200; (C) Homogeneous CEMs include CMV,
395
Neosepta CMX and CMT; (D) Heterogeneous CEMs include Ralex CEM, MK-40 and Excellion
396
I-100. Each error bar represents one standard error.
397 398
A significantly higher biomass of cells was observed on the heterogeneous CEM than on
399
all the other IEMs. The lowest and highest biovolumes of the cell layers (live and dead) of 16.49
400
µm3/µm2 (± 0.84) and 25.44 µm (±2.5) were measured for the homogeneous AEM and the
401
heterogeneous CEM, respectively. No significant difference in the cell biovolumes was found
402
between the heterogeneous AEM and the homogeneous CEM (≈18.7 µm3/ µm2). Interestingly,
403
the biovolume ratio of dead to live cells was significantly higher for AEMs (≈0.6) than for CEMs
404
(0.27) (Figure 4B). The larger dead cell biomass detected on the AEMs suggested that the AEM
405
surface provides a higher surface toxicity towards the attached bacteria. In addition, the contact
406
angle analysis showed that the AEM surface is slightly more hydrophilic than that of the CEM,
407
which may result in reduced biofilm formation. At the stationary growth phase of P. aeruginosa
408
PAO1, the bacterial membrane surface was observed to increase its hydrophobicity [26].
409
Therefore, hydrophobic interaction should be important for biofilm formation, especially on the
15
410
CEM surface [29]. This higher surface roughness of the heterogeneous membranes also
411
contributes to elevation in biofilm formation for both CEM and AEM types.
412
A higher amount of EPS was detected on the CEMs than on the AEMs as shown in
413
Figures 3 and 5A. The significantly low EPS amount observed on the homogeneous AEM could
414
be the result of a low percentage of viable cells in the biofilms and a relatively low surface
415
roughness (Figures 4 and 1). Both homogeneous and heterogeneous CEMs provided a better
416
surface for EPS formation with ~ 1.1–1.2 µm3/ µm2 specific biovolume. On the contrary, the
417
lowest amount of EPS (< 0.2 µm3/µm2) was present on the homogeneous AEM with a higher
418
amount of EPS on the heterogeneous AEM of ~ 0.5 µm3/µm2. Interestingly, a higher ratio of
419
EPS biovolume (EPS on CEM/EPS on AEM) was observed for the homogeneous IEMs than for
420
the heterogeneous ones (Figure 5B). While the lower cell viability observed for the AEMs
421
compared to the CEMs, which will be further analyzed in this study, could explain the lower
422
EPS amounts, surface roughness provides a secondary effect of retaining the EPS matrix under
423
shear. The combination of low surface roughness for the homogeneous IEM surface and
424
cytotoxic effects owing to quaternary ammonium moieties on the AEM surface is likely the
425
reason for the lowest amount of EPS and the highest ratio of its EPS amount to the EPS amount
426
on its CEM counterpart (Figure 5 B). It should be mentioned that the CEMs in this study provide
427
a better surface for biofilm colonization despite the repulsive interactions that are expected
428
between negatively charged bacteria/biopolymers and the surface (negatively charged by
429
sulfonate groups) [31]. Reduced bacterial attachment to negatively charged surfaces usually
430
reduces biofilm formation only in the short term [15], and commonly, adsorption of dissolved
431
organic matter and EPS , via hydrophobic interactions, provides a conditioning film, which
432
enables sessile microbial growth on the surface and biofilm formation [30,32]. In addition,
433
elevated biofilm growth and EPS production on the CEM surface was also attributed to the
434
higher viability of the attached cells compared to the AEM surface.
435 436 437 438 439 440 441 442 443 444
16
445 446 447
Figure 5: EPS accumulated on the different commercial IEMs after 24 h of biofilm growth: Left
448
panel – Biovolume of EPS on the IEMs (µm3/µm2): X-axis legend (A) Homogeneous AEMs
449
include AMV, Neosepta AEX and AMT; (B) Heterogeneous AEMs include Ralex AEM, MA40
450
and Excellion I-200; (C) Homogeneous CEMs include CMV, Neosepta CMX and CMT; (D)
451
Heterogeneous CEMs include Ralex CEM, MK40 and Excellion I-100; Right panel – The
452
average ratio of EPS amounts generated on different CEMs to AEMs for both homogeneous and
453
heterogeneous membrane types. Error bars represent one standard error.
454 455 456
3.3 Antimetabolic activity of IEM surface on P. aeruginosa
457
The measurement of the metabolic activity of sessile P. aeruginosa cells by the XTT assay
458
provided a clear indication of the possible antimicrobial activity of the membrane surface [33].
459
The viable cells on the surface will convert XTT to soluble formazan salt, and therefore, the
460
absorbance of formazan at 450 nm is indicative for the viability of the sessile bacteria. The
461
results of the XTT tests are summarized in Figure 6. The higher absorbance of formazan
462
originated from the biofouled CEMs indicates that the metabolic activity of the bacteria attached
463
to the CEM was not hampered by the exposed -SO3- ionic group of the CEM. On the contrary,
464
the magnitude of absorbance was lower for the case of both homogeneous and heterogeneous
465
AEMs, suggesting that the viability of the sessile bacteria was reduced while growing on these
466
surfaces. The quaternary ammonium ion in the AEM likely inhibits proliferation and reduced the
467
viability of the attached bacteria. Interestingly, a higher absorbance was observed for the
468
heterogeneous than for the homogeneous AEM. In the heterogeneous AEM, the ion exchange
469
groups are clustered and unevenly distributed in the membrane matrix unlike in the
470
homogeneous AEM where the charged groups are distributed uniformly over the membrane
17
471
polymer matrix [34]. Hence, the lower magnitude of absorbance value for the homogeneous
472
AEM indicates greater antimicrobial activity on the surface owing to the more uniform
473
distribution of charged quaternary ammonium resin. The lower absorbance value with the blank
474
sample suggested that none of the charged groups (quaternary ammonium or sulfonate) in the
475
IEMs interacted with XTT, and they were also unable to reduce it to formazan. The XTT assay
476
was thus useful for measuring the effect of the charged groups in the IEM on the viability of P.
477
aeruginosa PAO1 biofilms.
478
Possible effects of EPS or dead cells covering the quaternary ammonium groups should
479
be considered for longer term, more realistic biofouling scenarios. In this study, well developed
480
biofilm was formed providing opportunity to the EPS/dead cells to cover the quaternary
481
ammonium groups. However, these effects, which may alter the antimicrobial effectiveness of
482
the surface, should be further considered. Indeed, the time range as well as the aquatic conditions
483
promoting adsorption of foulants, which may consequently affect the antimicrobial activity of
484
the surface, is a subject for a continuing study.
485 486 487
Figure 6: The effect of the different IEM types on cell viability analyzed with XTT: Average
488
absorbance value at 450 nm attributed to the production of soluble formazan salts by biofilms
489
developed after 18 h on the different membranes. X-axis legend (A) Heterogeneous AEMs:
490
Ralex AEM, MA40 and Excellion I-200; (B) Heterogeneous CEMs: Ralex CEM, MK40 and
491
Excellion I-100; (C) Homogeneous AEMs: AMV, Neosepta AEX and AMT; (D) Homogeneous
492
CEMs: CMV, Neosepta CMX and CMT. Blank samples denote the average absorbance value
493
obtained using pristine IEMs. Error bars represent one standard error. 18
494 495
3.4 Cell membrane integrity assays upon cell exposure to different IEM surfaces
496
The effect of exposing P. aeruginosa PAO1 sessile cells to different IEM surfaces on the cell
497
membrane integrity was analyzed by NPN permeation tests. Enhanced uptake of NPN occurs in
498
a bacterial population containing cells whose outer membrane is damaged and functionally
499
inactive [35]. In the present study, an increased fluorescence was detected in cells on the AMV
500
(homogeneous AEM) and the MA-40 (heterogeneous AEM), which indicated the detrimental
501
effect of quaternary ammonium groups present on these membranes' surfaces (Figure 7). The
502
NPN uptake was found to be much less for the CEMs. Average contents of cells stained with
503
NPN as determined by specific biovolumes of 1.006 µm3/ µm2 (± 1.03), 9.32 µm3/µm2 (± 1.004),
504
2.93 µm3/µm2 (± 0.92) and 28.3 µm3/µm2 (± 1.65) were measured for the homogeneous CEM
505
(CMV), homogeneous AEM (AMV), heterogeneous CEM (MK40) and heterogeneous AEM
506
(MA40), respectively. A possible cell-surface electrostatic interaction could be promoted by the
507
positive charge of quaternary ammonium and the negatively charged LPS of the P. aeruginosa
508
PAO1 cell surface. The quaternary ammonium groups are known to display an electrostatic
509
interaction with anionic LPS, which leads to alteration of the cell membrane architecture, thus
510
enhancing membrane permeability, leakage of cell components, and subsequent cell death[28].
511
These results corroborate the biofilm formation results observed in Section 3.2 and delineate the
512
antimetabolic activities of the AEMs observed in Section 3.3.
513
19
514
515 516
Figure 7: Analysis of bacterial outer membrane permeability according to the uptake assay of 1-
517
N-phenylnaphthylamine (NPN): Cells tagged with NPN, after 12 h of biofilm growth, were
518
observed in the CLSM (blue clusters) and reconstructed images were made with IMARIS
519
software (A-D); The images present the following: (A) Homogeneous AEM (AMV); (B)
520
Homogeneous CEM (CMV); (C) Heterogeneous AEM (MA40); and (D) Heterogeneous CEM
521
(MK40). Each image (A-D) is a perspective of 600 µm × 600 µm image. (E) A quantitative
20
522
analysis of the specific biovolume attributed to the NPN-tagged cells. Performed with
523
COMSTAT Matlab script. Error bars represent one standard error.
524 525
The results presented so far are in accordance with earlier reports where two different
526
antibacterial modes of actions were deduced for positively charged surfaces by quaternary
527
amines[36]. One of the mechanisms is involved in the displacement of divalent cations (e.g. Ca2+
528
and Mg2+) present on the bacterial outer surface by polymer chains with positively charged
529
surfaces[37]. Displacement of these divalent ions, which hold together the negatively charged
530
surface of the lipopolysaccharide network of Gram-negative bacteria, leads to disruption of the
531
outer membrane of these bacteria. The second mechanism deals with the penetration of
532
positively charged polymer chains into the inner bacterial membrane, which leads to cell leakage
533
and eventually inactivation[38]. In our case, the first suggested mechanism is possible, while the
534
second one is less likely, as it requires penetration of positively charged polymers, which in this
535
case, are affixed to the IEM matrix and not accessible to the bacterial cell membranes.
536 537
3.5 Effect of IEM surface charge on bacterial intracellular ROS generation
538
An excessive liberation of bacterial intracellular ROS in response to a harsh surrounding
539
environment (for example, the presence of nanoparticles [29], antibacterial agents, and positively
540
charged compounds) was previously shown by Terada et al [28]. In the present study, we
541
hypothesized that exposure of bacterial cells to the charged IEM surface may affect the redox
542
potential across the cell membrane and accelerate ROS production in the sessile bacteria.
543
Overproduction of intracellular/endogenous ROS can commence due to exposure to exogenous
544
stimulation (both physically and chemically), and consequently, cellular damages occur that may
545
become irreversible and cause cell death [39]. For the above mentioned purpose, the oxidation of
546
DCFH-DA was carried out to detect and quantify the intracellular ROS when bacterial cells were
547
exposed to differently charged IEM surfaces [27]. It was evident from the CLSM results that
548
AEMs, irrespective of their types, induce production of more intracellular/endogenous ROS than
549
CEMs (Figure 8), and that the presence of quaternary ionic groups on AEMs likely accelerate
550
ROS overproduction.
551
21
552 553
Figure 8: IMARIS 3-D images of 2′, 7′-dichlorodihydrofluorescein (DCFH) stained bacterial
554
cells (for ROS generation) on the surface of different categories of IEM after 12 h of biofilm
555
growth; (A) Homogeneous AEM (AMV); (B) Homogeneous CEM (CMV); (C) Heterogeneous
556
AEM (MA-40); (D) Heterogeneous CEM (MK-40); each image (A-D) is a perspective 600 µm ×
557
600 µm.
558 559 560
3.6 Effects of biofouling on transport properties of IEMs during the Donnan exchange
561
In the Donnan dialysis process, counter-ions carrying the same electrical charge are exchanged
562
between two solutions through an ion exchange membrane. The driving force for the transport of
563
ions through the membranes is their concentration gradients across the membrane. It is expected
564
that the transport of ions will be hampered when the membrane is biofouled due to mass
565
transport limitations. In the present study, sulphate and potassium passage through AEMs and
566
CEMs, respectively, was investigated in a customized Donnan dialysis cell. The results for
567
sulphate and potassium accumulation in the receiving compartment as a function of time are
568
shown in Figure 9. Fluxes are expressed by the slopes of the respective curves and summarized
569
in Table 3. The percentage of flux decline shown in the rightmost column of Table 3 was
570
calculated as 100 × [flux(pristine membrane)-flux(fouled membrane)]/flux (pristine membrane). 22
571
From the data presented in Table 3, it is evident that the extent of flux decline is larger for
572
the heterogeneous IEMs than for the homogeneous IEMs and for the AEMs than for the CEMs.
573
The differences between the heterogeneous and the homogeneous membranes correlate well with
574
the results described in Section 3.2 that show the difference in the amount of biomass
575
accumulated on the two classes of membranes. The larger biovolumes collected on the surfaces
576
of the heterogeneous membranes is attributed to the larger diffusion limitations at the solution-
577
membrane interface, which emerge from the enhanced concentration polarization in this
578
region[40].
579
Based on the differences between the behavior of the CEMs and AEMs as a substratum
580
for biofilm development discussed in the previous sections, the differences in the mass transfer
581
properties for these types of membranes are, in a way, counterintuitive. While the AEMs support
582
biofilm formation to a lower extent than the CEMs, the ion flux decline was more pronounced
583
for the biofouled AEM membrane (Table 3). It should be noted that most types of EPS are
584
negatively charged at pH values exceeding 4, mostly due to deprotonation of carboxylic,
585
hydroxyl, or sulfonic functional groups [41–43]. As a result, depending on the pH and the other
586
aquatic conditions, EPSs are adsorbed to positively charged surfaces, such as those of the AEMs,
587
or are prone to bind to positively charged organic molecules and multi-valent cations [42–46]. In
588
this respect, also other studies confirm the fouling propensity of AEMs towards organic fouling
589
[47–49].
590
Based on the above properties, we hypothesize that under the current experimental
591
conditions for biofilm growth followed by the Donnan exchange studies, the negatively charged
592
EPS components are preferentially bound, mainly via electrostatic interactions, to the positively
593
charged fixed ionic groups of the AEMs at the membrane-solution interface. This interaction will
594
likely form an electrostatically neutral layer on the membrane surface, which will become
595
partially blocked, and thus, interfere with the ion exchange process. Such an adsorbed EPS layer
596
is minute and does not have to exceed the density of the fixed ionic groups on the membrane
597
surface that can be estimated to be as low as 1.5–2.5 × 10-9 equivalents/cm2 (supplementary
598
information).
599 600 601
23
602 603 604 605 606 607 608 609 610 611 612 613
24
614
Figure 9: Sulphate (A) and potassium (B) diffusion to the receiving compartments per unit
615
membrane area as a function of time, for pristine and biofouled membranes. Linear lines
616
represent the slope of the ions' passage versus time, from which ion flux was calculated.
617 618 619
Table 3: Summary of ion fluxes for pristine and fouled membranes. Conditions, flux Membrane
Membrane Type
Analyzed
Pristine
Fouled
ion
(eq.m-2.h-1)
(eq.m-2.h-1)
Flux Decline (%)
MA-40
Heterogeneous
MK-40 AMV CMV
Homogeneous
SO42-
0.123
0.032
74
K+
0.232
0.0975
58
SO42-
0.48
0.284
40.8
K+
0.35
0.252
28
620 621 622
4. Conclusions
623
The present study investigates the formation of mono-culture bacterial biofilm on different
624
commercially available IEM surfaces. It should be mentioned that mono-culture biofouling
625
studies commonly provide reproducible and robust approach, in which involved mechanisms are
626
more easily elucidated as concluded in this paper, while under more realistic conditions of mixed
627
environmental consortia, interactions between microbial species and environmental conditions
628
effects on the different microbes would make it hard to draw conclusive mechanisms. The results
629
suggest that IEM type affects the electrostatic interactions with bacteria; however, the CEM
630
surface provides a better carrier for biofilm formation despite the possible repulsion from
631
bacteria and most negatively charged EPS components. The specific biovolumes of cells and
632
EPS, used for quantifying biofilm growth, were larger on the CEM than on the AEM surface.
633
The antimicrobial characteristics of the AEM were demonstrated, in which the lower cell
634
viability on the AEM surfaces was due to quaternary amine groups on the surface facilitating the
635
disruption of bacterial cell membranes, while the CEM surface did not facilitate such an effect. 25
636
Hence, the CEM provides a better platform for sessile microbial growth. The Donnan exchange
637
studies also confirmed the impact of bacterial biofilm growth on the IEMs, in which a
638
consequent sharp decline in counter-ion passage was documented for all types of membranes,
639
with heterogeneous IEMs and AEMs dominating. The overall study revealed that the charged
640
groups and the surface roughness determine the biofouling propensity of IEMs.
641 642
Acknowledgments
643
This research was supported by the United States-Israel Binational Science Foundation
644
under award number 2012142 and the Planning and Budgeting Committee (PBC) of the
645
Council for Higher Education for the Postdoctoral Fellowship Award provided to Dr. Soumya
646
Pandit.
647 648
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31
Highlights •
Mechanisms of biofilm formation ion exchange membranes (CEM and AEM) were tested.
•
Anti-metabolic activity of AEM surface affecting membrane integrity was confirmed.
•
Biofilms reduced the counter-ion transport mainly for heterogeneous AEMs.
Ben-Gurion University of the Negev Blaustein Institutes for Desert Research Zuckerberg Institute for Water Research Dept. of Desalination and Water Treatment Assoc. Prof. Moshe Herzberg Phone: 972-8-6563520, 972-50-2029608 Fax: 972-8-6563503 E-mail:
[email protected]
Journal of Membrane Science Editorial Office
Dear Editor: In our revised manuscript “Bacterial Biofilm Formation on Ion Exchange Membranes”, which is submitted for possible publication in Journal of Membrane Science, there are no declarations of interest.
"Declarations of interest: none'. We thank you very much for your consideration, Sincerely, Moshe Herzberg
Sede Boqer Campus, Tel: 086563520` Fax: 086563503
,קמפוס שדה בוקר 8086563503 : ; פקס086563520:'טל