Keywords
Biointerface materials, nanoparticles, antibiotic recalcitrance, transport phenomena 37
38
Graphical Abstract 39
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40
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1. Introduction 41
Biological interfaces, like microbial cells and biofilms, are more complex than 42
engineered porous membranes[1] and subsequently the transport relationships are more complex. 43
For example, the liquid-surface biointerface typically contains soft-layers comprised of fats, 44
sugars, and proteins of various charges [2]. The interior of the biointerface exhibits heterogenous 45
porosity and tortuosity [3], heterogeneous mechanical compliance, heterogenous hydrophilicity, 46
and heterogeneous charge distribution due to the presence of cells and extracellular components 47
[4]. These complex structures increase the difficulty of decoupling the impacts of charge, size, 48
geometry, and chemistry on the transport of novel drug and drug delivery vehicles through these 49
biological interfaces. In microbial biointerfaces, like bacterial biofilms [5-8], this complexity is 50
increased by the dynamic response that can occur at similar time scales to the time for total 51
penetration. The dynamic response from bacteria can include extracellular matrix production of 52
polymers like alginate, nanocellulose, proteins like flagellin [9, 10], and secretion of extracellular 53
DNA. These properties contribute to enhanced virulence [11] and treatment failure [12] in 54
diseases such as cystic fibrosis. Consequently, new therapeutic strategies, including the use of 55
nanomaterials as drug delivery vehicles, have been proposed to enhance penetration and efficacy 56
within biofilms[13-15]. 57
These new therapeutic strategies will come with their eventual environmental 58
dissemination. While engineered nanomaterials cannot be studied as a uniform class[16], 59
experimental and computational platforms that account for their fate and transport must be 60
created [17-21]. Periphyton biofilms are the primary sink for nanomaterials in estuary 61
environments [22]. The primary factors which effect ENM ecotoxicological parameters such as 62
toxicity and bioaccumulation for a given ENM-biofilm-environment system can be evaluated. 63
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What emerges is a set of four pairwise factors of the biofilm-ENM system of interest which 64
shapes bioaccumulation: size (particle/pore) [23-29], charge (surface/ECM) [24, 25, 27, 30-32], 65
chemistry (surface/ECM) [25, 31, 33], and hydropathy (surface/ECM) [27, 30, 34]. 66
Previous studies on the impact of mechanical stress on biointerfaces have used alginate 67
since it is an essential component of some biofilms and has facile preparation [35-38]. However, 68
alginate has 1 -2 orders of magnitude higher storage and loss moduli than natural biofilms [37]. 69
Additionally, alginate has different chemical absorption properties, specifically it is less able to 70
absorb divalent metallic cations than natural biofilms [37]. We have previously shown the 71
nanocellulose preparation used here has mechanical and certain chemical properties in range 72
with natural biofilms [39]. Nanomaterial exclusion from biofilms has been proposed to be a 73
function of the various heterogeneous matrix components alginate, nanocellulose, proteins; the 74
matrix size; commensal phage; bacterial cells, particularly their charge, and the channels in the 75
biofilm [4, 30, 40]. As heterogeneity is difficult to achieve synthetically, this may require 76
systematic study. For example, the importance of alginate on antibody binding in P. aeruginosa 77
biofilms was discovered through adding alginate back alginate deficient mutants. Recent work 78
on diffusion in alginate showed the impact of matrix cross-linking on size-exclusion [41]. 79
We propose the biofilm matrix and cells with their respective charges can be studied with 80
synthetic systems. We synthesized microcaps from nanocellulose that are modified with divalent 81
calcium ions as the biofilm matrix. We added neutral and charged microspheres to represent cells 82
and their respective binding affinities. We tested the ability of charged and neutral nanodextran 83
of different molecular weights to accumulate into the defined nanocellulose matrix. 84
This study tested the ability of a microcap synthesis method to replicate the important 85
effects of a biofilm on species diffusion: (a) the size-effect, (b) the volume-exclusion effect, and 86
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(c) the attachment effect. These important biofilm effects were mapped on to three hypotheses. 87
We hypothesize that if the size-effect is replicated that larger diffusing species would accumulate 88
at lower concentrations in the matrix. We hypothesize that if the volume-exclusion effect is 89
replicated, that diffusing species would accumulate at a lower concentration in a microcap with 90
impermeable particles compared to one without. We hypothesize that if the attachment effect is 91
replicated that diffusing species would accumulate at a higher concentration in the microcap 92
when attachment sites are present. Biofilms have distinct porosity profiles based on 93
environmental conditions [42, 43], distinct matrix components based on nutrient conditions and 94
external threat [36, 43], and distinct cell populations based on age and nutrient conditions. This 95
study and platform may aid in understanding how each component contributes to overall 96
accumulation. 97
2. Methods 98
The goal of this study is to test the ability of a synthetic biomaterial to replicate the 99
important effects of a biofilm on species diffusion. We leveraged our recently developed 100
nanocellulose hydrogel that has closer mechanical stiffness to natural biofilms. We embedded 101
the biofilm with charged and non-charged microspheres to test volume-exclusion and attachment 102
and charge based exclusion. We used two sizes of nanodextrans to test size exclusion. We used 103
standard optical tools for examining biofilms to measure the effects of the tested parameters, 104
Figure 1. 105
2.1 Microcap Design and Nanodextran Information 106
To generate the microcaps, hydrogels were used as the hydrated mesh domain to achieve 107
a size-effect. Hydrogels have been used in prior studies to simulate the extracellular matrix of the 108
biofilm [41]. The hydrogel platform chosen for our system was nanocellulose hydrogels. We 109
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recently developed a nanocellulose that better matched the mechanical storage and loss moduli 110
[39], that is also easily chemically modifiable for which future studies could choose to utilize for 111
a method of generating attachment sites independent of microspheres. 112
Fluorescent polystyrene microspheres (Spherotech | Lake Forest, IL) ranging from 0.7-113
0.9 microns in diameter were used to simulate bacteria and achieve a volume-exclusion effect. 114
Three distinct microspheres, each with distinct microsphere surface chemistry, were used: no 115
surface modifications (Plain) (Prod# FP-0862-2), carboxylate-modified (Carboxyl) (Prod# FP-116
0862-2), and amine-modified (Amino) (Prod# FP-0862-2). The carboxylate and amine-modified 117
microspheres were coated with these functional groups, which are either negatively or positively 118
charged at neutral pH. These charged microsphere surfaces were designed to only act as 119
attachment sites for the diffusing species if the diffusing species was oppositely charged. The 120
microspheres were fluorescently labelled with a vendor proprietary fluorescent tag. 121
Nanodextrans conjugated to FITC (fluorescein isothiocyanate) were used as the diffusing 122
species for the system (TdB Labs, Uppsala, Sweden). Two nanodextran molecular weights used 123
were 150 kDa and 2,000 kDa, on the premise these molecules would have different sizes, to test 124
the size-exclusion effect. The fluorescently labelled nanodextrans were chemically modified to 125
have either carboxymethyl (CM) groups with negative charge (Prod# FITC-CM-dextran-150), 126
diethylaminoethyl (DEAE) groups with positive charge (Product # FITC-DEAE-dextran-150), or 127
no modification at all (Dx) (Prod# FITC-Dx-150 and Prod# FITC-Dx-2000). The use of charged 128
nanodextrans and charged microsphere surfaces was designed to produce the attachment effect. 129
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b
c
Figure 1: A. Experimental protocol for testing diffusion into hydrogel. B. Experimental Apparatus Diagram
C. Artistic representation of microcap. Hydrogels were made as described in [39]. After centrifugation,
microspheres were added. Resultant , A flow cell (b) from Biosurface Technology was seeded with hydrogel inserts
along the coupon recess/imaging window. Red circles represent microspheres. Microspheres with amine-coating
represented. Nanodextran with no modification shown.
130
2.2 Nanocellulose Solution Synthesis 131
A nanocellulose synthetic biofilm was generated as described in [39]. Briefly, 4.00 ± 0.05 132
g of dry cellulose powder (CAS#9004-34-6 | Sigma-Aldrich | Burlington, MA) and slowly 133
mixing it with an ionic liquid solution composed of 7.00 ± 0.05 g sodium hydroxide (CAS#1310-134
73-2 | Sigma-Aldrich | Burlington, MA), 12.00 ± 0.05 g urea (CAS#57-13-6 | Sigma-Aldrich | 135
Burlington, MA), and 81.00 ± 0.05 g of reverse-osmosis filtered (RO) water and adding it to a 136
125 mL Erlenmeyer flask. The resulting suspension was mixed using an inert stir bar at 500 rpm 137
until it was homogenous and consistently cloudy. The suspension was then submerged in an ice-138
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isopropyl alcohol bath with a temperature ranging between -10 and 0 OC while still being stirred. 139
After more than 1 hour of stirring and the dissolution of the cellulose, the liquid was separated 140
into two 50 mL centrifuge tubes. The tubes were centrifuged at 10,000 RPM (rcf=13,751) for 10 141
minutes while maintaining a temperature of 22 OC. After centrifugation, the supernatant was 142
decanted and saved as nanocellulose solution, with any settled solids discarded. 143
2.3 Nanocellulose-Microsphere Solutions 144
For each batch of nanocellulose solution made, four different nanocellulose-microsphere 145
solutions were made: one with Plain microspheres, one with Carboxyl microspheres, one with 146
Amino-microspheres, and one with no microspheres. These nanocellulose-microsphere solutions 147
were prepared by mixing 5.0±0.1 mL of nanocellulose solution with 50±0.1 µL of 1wt% 148
microsphere solution in the well of a 6-well culture plate. Once all four nanocellulose-149
microsphere solutions were prepared for each nanocellulose batch on the same plate, the plate 150
was covered, wrapped in aluminum foil, and mixed for 24 hours on a shaking plate at 250 RPM 151
at room temperature ranging from 22-26 ºC. After 24 hours of mixing, the resulting 152
nanocellulose-microsphere solutions were stored at 4 ºC. 153
2.4 Microcap and Flow Cell Preparation 154
With the nanocellulose-microsphere solutions prepared, a 5 mL syringe affixed with a 155
27G nozzle was used to fill the nozzle with nanocellulose-microsphere solutions. The 156
nanocellulose solution was then extruded through the nozzle using the syringe. Once a small 157
amount of nanocellulose solution was extruded, priming the nozzle, the nozzle would then “leak” 158
the solution semi continuously. The nozzle tip was then repeatedly (between 10-30 times) 159
pressed onto the surface of a polycarbonate coupon, with a microscopic amount of hydrogel 160
being left behind on the coupon as residue with each press. The coupon then sat at room 161
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temperature in a plastic petri dish for greater than 48 hours to dry with no plastic cover but 162
aluminum foil cover, which prevented contamination and fluorescent overexposure, but allowed 163
for air flow. This let the hydrogel residues to dry onto the coupon and form microcaps. Before an 164
experiment, the microcap covered coupon was loaded into a flow cell (Prod# FC 275-AL | 165
BioSurface Technologies | Bozeman, MT, USA), where the flow cell chamber containing the 166
coupon was filled with reverse-osmosis water first to rehydrate the microcap. Almost 167
immediately after, the chamber was then filled with a 5 µM solution of Calcofluor White (CW) 168
stain dissolved in water (Cat# 29067 | Biotium | Fremont, CA, USA). The fluorophore would 169
then slowly diffuse into the microcaps, allowing for fluorescent imaging of the hydrogel domain 170
of the microcap. 171
2.5 Nanodextran Exposure and Imaging Procedure 172
Once the flow cell was loaded with coupons covered with CW-stained microcaps, the 173
flow cell was then connected to a microfluidic apparatus with two inlets: reverse-osmosis filtered 174
(RO) water and 30 mg/L fluorescently labelled-nanodextran dissolved in Dulbecco’s phosphate 175
buffer solution (PBS) (Figure 1). The flow cell was placed on a confocal laser scanning 176
microscope, which allowed for real-time 3-D fluorescent imaging of the microcaps. 177
Each experiment involved a two-phase procedure: characterization and accumulation. To 178
perform an experiment, the flow chamber was flushed with 1 mL/min RO water during the 179
characterization phase. While the flow chamber containing the microcap-covered coupon was 180
flushed with 1 mL/min RO water, the microcaps on the coupon were checked to determine if 181
there were three microcaps less than 250 microns in diameter (all tests had at least three). A z-182
stack, or a series of microscope images taken at close, regularly spaced focal lengths to 183
reconstruct a 3-D image of a sample, was taken of three microcaps on each coupon (with the 184
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three smallest microcaps usually chosen). Field of view size was adjusted for each microcap to 185
take up the entire image. Nyquist sampling was used to select z-section thicknesses and image 186
resolution. These z-stacks were set up to image three features in each microcap: the hydrogel 187
mesh by imaging the CW stain (Laser: 405 nm/Detector Range: 410-546 nm), the impermeable 188
microspheres (Laser: 561 nm/Detector Range: 585-700 nm), and the presence of FITC (Laser: 189
488 nm/Detector Range: 410-546 nm). In addition to measuring the presence of FITC, this same 190
signal was also used to determine the location of the coupon within the image, as the coupon 191
reflected green light at its surface. This first image before any FITC was added to the system will 192
be referred to as the characterization image. 193
After the characterization image of each of the microcap of interest, the microcaps were 194
exposed to a continuous stream of nanodextran during the accumulation phase of the experiment. 195
This was done by flowing 1 mL/min of the 30 mg/L nanodextran dissolved in PBS into the flow 196
chamber continuously for 24 minutes. After this continuous exposure to a constant concentration 197
of nanodextran, the flow in the chamber was stopped, and the microcaps re-imaged using the 198
same parameters as those for the characterization image, producing an accumulation image for 199
each microcap. This was done to quantify two things: the concentration of nanodextran (via the 200
proxy measurement of FITC-signal) in the water immediately surrounding each microcap, and 201
the concentration of nanodextran within each microcap. 202
During accumulation phase of each experiment, time-lapse imaging of a single-z-plane 203
within one of the imaged microcaps was taken to monitor if the system reached equilibrium 204
during each phase (which all were confirmed to reach). 205
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2.6 Experimental Design 206
To test the functional properties of these microcaps, three predicted experimental effects 207
were tested to determine the capacity of these microcaps to replicate the biofilm features of 208
interest, Figure 2. The size-exclusion effect was tested to determine if a hydrated mesh was 209
formed. The volume-exclusion effect was tested to determine if the embedded microspheres 210
were diffusing species impermeable. The attachment effect was tested to determine if the 211
diffusing species were immobilized via opposite charge interactions with the surface of the 212
microspheres, indicating diffusing species attachment sites. 213
a
b
c
Figure 2: (a-c)Diagrams of hypothesized size-exclusion effect, charge based attachment effects,
and volume exclusion effect. d-e Hypothesized outcomes of nanodextran concentration in
hydrogels based on the given effect.
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214
To test for the size-exclusion effect, the two different sized nanodextrans were used: 150 215
kDa and 2,000 kDa. The 2,000 kDa nanodextran was expected to have a larger particle size than 216
the 150 kDa case. This was tested and confirmed using Nanoparticle Tracking Analysis and 217
Dynamic Light-Scattering measurements, shown in Table 1. While the measured sizes were 218
similar sizes via NTA and DLS, we used them as it well known that while designed for specific 219
sizes, environmental nanomaterials are never pristine. These nanodextan molecular weights were 220
chosen because they have been used in biofilm penetration studies as both small and large sized 221
nanomaterials [23, 25, 44, 45]. Additional details on nanoparticle characterization are provided 222
in the Supplementary Information. 223
Table 1: Nanodextran Characterization. All nanodextrans dispersed in Dulbecco’s Phosphate Buffer
Solution (PBS). NTA error reported as standard error from measured particle size distribution (n=5). *-
Standard error not reported on instrument. FITC-Dx-2000 size measured twice on NTA, both sizes reported.
DLS/ELS error reported as standard deviation of three triplicate measurements.
Nanodextran Nanodextran Molecular
Weight [kDa]
Size via NTA
[nm]
Size via DLS
[nm]
Charge via ELS
[mV]
FITC-Dx-150 150 226 ± 14 115 ± 24 -1.2 ± 0.4
FITC-DEAE-150 150 178 ± 5 107 ± 16 -0.4 ± 0.4
FITC-CM-150 150 173* 771 ± 1000 -5.7 ± 3.2
FITC-Dx-2000 2000 297 ± 18
306 ± 24
81 ± 0.1 -2.4 ± 0.7
Since hydrated meshes such as a biofilm extracellular matrix and a hydrogel are 224
comprised of disorganized, overlapping biopolymer chains, they can allow particles to diffuse 225
through them, but only up to a certain size. As the particle reaches a characteristic “mesh size”, 226
less of the volume within the hydrated mesh network is available for it to occupy. Once the 227
particle reaches a critical size, no amount of particle can accumulate within the matrix. Thus, as 228
particle size increases, the equilibrium concentration it reaches within a hydrated matrix 229
decrease, as less volume is available for the particle to permeate into. Hence, a decrease in 230
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diffusing species concentration with particle size within the matrix at equilibrium shows the 231
presence of a size-exclusion effect in the microcap, which in our system is likely indicative of 232
the formation of a hydrogel. Microcaps prepared using identical conditions were used in size-233
exclusion experiments. 234
To test for the volume-exclusion effect, hydrogels were prepared either with 235
microspheres within them or without microspheres. The microcaps without microspheres within 236
them would be expected to reach a higher concentration of nanodextran if the volume-exclusion 237
effect was observed. The reasoning for this is similar to the reasoning for the size-exclusion 238
effect: certain portions of the microcap volume, specifically the volume occupied by the 239
microspheres, would be unavailable for the nanodextran to occupy, leading to a lower 240
concentration overall in the microcap. Identical nanodextrans were used in volume-exclusion 241
experiments. 242
To test for the attachment effect, hydrogels embedded with three different microspheres 243
were prepared and tested against three different nanodextrans. The different microspheres tested 244
were no surface functionalization (Plain, neutrally charged surface), amine-functionalization 245
(Amino, positively charged surface), and carboxyl-functionalized (Carboxyl, negatively charged 246
surface). The different nanodextrans tested were no chemical modification (None, neutrally 247
charged), carboxymethyl-modified (CM, negatively charged) and diethylaminoethyl-modified 248
(DEAE, positively charged). Since we only expect oppositely charged combinations to lead to 249
attachment between microsphere surface and nanodextran, we expect to see significant increases 250
in nanodextran concentration within the microsphere only for the combination of CM-modified 251
nanodextran accumulating in microcaps with amine-modified microspheres, and DEAE-252
modified nanodextran accumulating in microcaps with carboxyl-modified microspheres. Two 253
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different control cases are considered for each of these combinations: (a) charged nanodextran 254
and uncharged microspheres, and b) uncharged nanodextran and charged microspheres. 255
Decreases in nanodextran concentrations within the microcap would be expected in both cases 256
compared to the oppositely charged nanodextran/microspheres case. 257
2.7 Image Analysis 258
To determine nanodextran concentration for each z-stack image taken, each pixel was 259
assigned to be in one of four spatial domains in the image: (1) the water domain (liquid domain 260
Ω!), (2) the hydrogel domain (interstitial domain Ω") (3) the microsphere domain (Ω#), and (4) 261
the coupon domain (solid domain Ω$). 262
Figure 3: Labelled Microcap from Characterization Image. Red channel: fluorescent polystyrene
microspheres (carboxyl-modified). Blue channel: CW-stained nanocellulose hydrogel. Green-channel:
polycarbonate coupon-microcap interface.
263
This was done by segmenting the hydrogel using the CW signal, the microspheres using 264
the AF594 signal, and the coupon using the FITC-signal in each image, and assuming all 265
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remaining pixels were within the water domain. The total microcap domain was the union of the 266
microcap and microsphere domains. 267
The microspheres were segmented using an Otsu threshold on the AF594 signal in 268
MATLAB. The hydrogel domain was segmented in ImageJ using a Otsu threshold, followed by 269
a region-filling algorithm (CW-stain only penetrated ~10 microns into hydrogel), followed by an 270
algorithm for discarding very small filled regions. The coupon was segmented using an edge-271
detection algorithm along the z-direction. An important note on this process was that coupon 272
segmentation was not perfect. The coupon segmentation algorithm was designed to favor a pixel 273
as coupon as opposed to water or hydrogel on purpose, since the accuracy of the water and 274
hydrogel signal was more important than the coupon signal. 275
With each pixel assigned to a domain, the average value of the nanodextran/FITC signal 276
in each domain in the microcap was quantified. Rather than use average FITC-signal in the 277
microcap, [𝐹𝐼𝑇𝐶]%&'()'*+ , directly, the ratio of the FITC-signal in the microcap to the FITC-278
signal in the water, [𝐹𝐼𝑇𝐶],*-.( , or the nanodextran-microcap partition coefficient, 𝐾/, was 279
calculated for each microcap’s accumulation image, Equation 1. This ensured any variation in 280
FITC concentration and signal within the flow cell was normalized between microcaps. 281
𝐾/ = [𝐹𝐼𝑇𝐶]%&'()'*+
[𝐹𝐼𝑇𝐶],*-.(
Equation 1: Microcap Partition Coefficient
The MATLB code for image analysis is included as Supplementary Information and is 282
available via Github. 283
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2.8 Statistical Analysis 284
Figure 4: Design of Experiments and Replicates
For each nanodextran-hydrogel combination tested, two types of replicates were used, all 285
on the hydrogel side: batch replicates and microcap replicates. Three batches of each hydrogel 286
tested (no microspheres, plain microspheres, carboxyl-microspheres and amine-microspheres) 287
were generated, leading to 12 different hydrogels with three batch replicates each. For each 288
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batch, one coupon covered with microcaps was generated for each nanodextran tested, leading to 289
33 different coupons. On each coupon, three microcap replicates were tested on each. This led to 290
a total of 99 microcaps tested. 291
To compile the data for each experimental condition (nanodextran-microcap 292
combination), the nanodextran-microcap partition coefficient for each microcap tested was first 293
found (see Image Analysis for how this was calculated). This value was then averaged for the 294
three microcaps on each coupon tested, as these replicates were determined to be technical 295
replicates, which warrant averaging together for the purposes of statistical analysis. This left 296
three nanodextran-microcap partition coefficients for each experimental condition, each one 297
representing a different hydrogel batch. These three nanodextran-microcap partition coefficients 298
comprised the sample for each experimental condition. 299
For each set of experimental conditions compared for each hypothesis, the three 300
nanodextran-microcap partition coefficients for each batch were compared to each other using 301
Welch’s one-way t-tests using an alpha of 0.05. Welch’s test was used since variances were not 302
assumed to be equal. One-way tests were used since only an effect in one direction would 303
constitute evidence for each hypothesis. All samples passed the Shapiro-Wilks test for normality. 304
3. Results 305
The microcaps generated using this synthesis procedure were tested for their ability to 306
replicate the core features of a synthetic biofilm. These included size-exclusion effects, volume 307
exclusion effects and attachment effects. Different combinations of microcaps and diffusing 308
nanodextran were used to test for these effects through equilibrium nanodextran partition 309
coefficients in the microcaps. 310
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Testing for Hydrated Mesh Property via the Size Effect 311
To test for the size-exclusion effect, nanodextran-microcap partition coefficients for 312
microcaps with plain microspheres were compared between a 150 kDa nanodextran and a 2,000 313
kDa nanodextran. The results, as shown in Figure 5, show a statistically significant size-314
exclusion effect in the hydrogel mesh was observed. 315
316
Figure 5: Size-Exclusion Effect Test for Verifying the
Hydrogel Mesh Property of the Synthetic Biofilm
System. Error bars represent 95% confidence intervals
on the sample. P-value represents results from one-tailed
Welch’s t-test. Experiments used 4 wt% hydrogels loaded
with 0.01 wt% plain polystyrene microspheres with
neutrally charged nanodextrans. Partition coefficient
represents nanodextran-microcap partition coefficient.
317
Testing for Impermeable Sub-volume via the Volume-Exclusion Effect 318
To test for the volume-exclusion effect, nanodextran-microcap partition coefficient for 4 319
wt% hydrogel microcaps embedded with either no microspheres or 0.01 wt% plain microspheres 320
were compared using a neutrally charged, 150 kDa nanodextran. The results, as shown in Figure 321
6, show no volume-exclusion effect due to the presence of the microspheres was observed. 322
323
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Figure 6: Volume-Exclusion Effect Test for
Verifying the Impermeable Subdomain Property of
the Synthetic Biofilm System. Error bars represent
95% confidence intervals on the sample. P-value
represents results from one-tailed Welch’s t-test.
Experiments used 4 wt% hydrogels loaded with
variable wt% plain polystyrene microspheres and
neutrally charged, 150 kDa nanodextran. Partition
coefficient represents nanodextran-microcap partition
coefficient.
324
Testing for Attachment Sites via the Attachment Effect 325
To test for the attachment effect, 4 wt% hydrogels embedded with 0.01 wt% neutrally, 326
negatively, and positively charged microspheres were tested against neutrally, negatively, and 327
positively charged 150 kDa nanodextrans, shown in Figure 7. Opposite charge combinations 328
were tested for increases in nanodextran-microcap partition coefficients compared to both the 329
same charged nanodextran and uncharged microspheres and the uncharged nanodextran and 330
same charged microspheres. No statistically significant attachment effect was observed across all 331
comparisons. A non-statistically significant attachment effect was observed for the microcaps 332
embedded with amine-modified microspheres with a carboxymethyl-modified nanodextran for 333
comparisons to both control cases. 334
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Figure 7: Attachment Effect Test for Verifying Presence of Attachment Sites in the Synthetic Biofilm
System. Error bars represent 95% confidence intervals on the sample. P-values represent results from one-tailed
Welch’s t-test. Experiments used 4 wt% hydrogels loaded with variable 0.01 wt% plain-, carboxyl- and amine-
modified polystyrene microspheres and neutrally, positively or negatively charged, 150 kDa nanodextrans.
Partition coefficient represents nanodextran-microcap partition coefficient.
4. Discussion 335
This research sought to create a synthetic biofilm system for use studying species 336
transport in biofilms. To accomplish this, nanocellulose hydrogel microcaps loaded with 337
polystyrene microspheres were developed to proxy bacterial biofilms in the features of a 338
hydrated mesh, an impermeable subdomain, and presence of attachment sites. The replication of 339
these features in the generated microcaps were tested for by quantifying an important 340
experimental effect for each feature: the size-exclusion effect for verifying the hydrogel mesh, 341
the volume-exclusion effect for verifying the impermeable subdomain, the attachment effect for 342
verifying presence of attachment sites. 343
Experimental results indicated that the size-exclusion effect was verified, and therefore 344
the hydrogel mesh feature of the microcaps. However, the attachment effect and the volume 345
exclusion effect were not observed. This indicates that the microcaps as currently designed are 346
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21
unable to replicate the key biofilm properties needed to perform transport studies of an 347
impermeable subdomain and presence of attachment sites. 348
Size-effect agrees with prior literature on chemical species diffusion in single bacterial 349
species biofilms [23, 46]. However, evidence of this effect is limited in multispecies biofilm 350
literature on nanoparticles [47]. This is most likely due to effects of agglomeration, dissolution 351
and changes to the nanoparticle biopolymer corona in multispecies biofilms studies having 352
strong effects on effective nanoparticle size during diffusion [48, 49]. This shows the need for 353
studies with more controls over nanoparticle stability in multispecies biofilm transport studies. 354
A few distinct hypotheses could explain why the presence of microspheres and the use of 355
chemically modified microsphere surfaces and nanodextrans did not elicit the effects of volume-356
exclusion and attachment. One is the use of a 0.01 wt% microsphere percentage within the 357
hydrogels was too low to observe the anticipated effects. If little volume is made impermeable 358
due to low concentration of microspheres, then the volume-exclusion effect would be anticipated 359
to be small and below any statistically significant threshold. In addition, too low of a 360
concentration of microspheres would mean there are very few sites for nanodextran attachment, 361
which would also predict a small attachment effect again below any statistically significant 362
threshold. Another possibility is that nanodextran can penetrate and diffuse into the polystyrene 363
microspheres. While there is evidence for adsorption onto the surface of polystyrene [50], there 364
is less evidence for penetration and diffusion into polystyrene microsphere. However, no 365
experimental evidence is offered in this research proving or disproving this hypothesis. 366
For the attachment effect, another possibility is that the charged microsphere surfaces do 367
not act as attachment and immobilization sites for its oppositely charged nanodextran. This could 368
be due to a variety of reasons including the charge-charge interactions not being strong enough 369
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22
to immobilize the nanodextran, the microsphere or the nanodextran not being charged species as 370
anticipated, or even that the immobilization of the nanodextran does not lead to higher levels of 371
nanodextran to accumulate into the hydrogel to balance the chemical potential gradient. While it 372
is possible attachment does occur in these systems but too slowly to observe in this experiment, 373
direct charge-charge interactions are the strongest intermolecular forces in chemistry, which 374
would make for quick attachment, making this possibility seem unlikely. This lack of a clear 375
effect of charge is common in the scientific literature on diffusion of chemical species in 376
hydrogel matrices such as biofilms [41, 44, 45, 51, 52]. Future experiments on this system could 377
include testing the accumulation and desorption of ions instead of nanomaterials as these have 378
been shown to matter in the biofilm matrix [53]. 379
Assuming the hypothesis that the non-observed effects were primarily due to a low 380
concentration of microspheres within the microcaps, further experimental work could replicate 381
these experiments with higher concentrations of microspheres and look for the same effects on 382
attachment and volume-exclusion. Further evidence for the size-exclusion effect could be found 383
by comparing current results to higher weight percentage nanocellulose hydrogels, which 384
theoretically lead to smaller critical mesh size, which would be anticipated to cause lower 385
nanodextran concentrations in these higher weight percentage microcaps [23, 54]. 386
The data presented here does not lend itself to diffusivity calculations common in the 387
literature. However, Bryers and Frummond showed lumped parameter diffusivity calculations 388
are inaccurate for describing transport in biofilm [55]. The data can be compared to 389
bioconcentration factors (BCFs) which have been widely reported in ecotoxicological studies of 390
engineered nanoparticles effects on environmental biofilms. Since estimates for BCFs in 391
ecotoxicological studies are usually only order of magnitude estimates, logarithmic BCF values 392
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(pBCF) will be used here to compare BCFs between different experiments [56-58]. pBCFs will 393
be calculated from dimensionless BCFs on a mass-by-mass basis (µg ENM/g biofilm divided by 394
µg ENM/g water) using the wet weight of the periphytic biofilms when possible. Since 395
periphytic biofilms are hydrated in the environment, wet weights are used to give a more 396
intuitive sense of the extent of the increase in concentration of ENM that would be seen in an 397
environmental system. If only dry-weight/AFDM BCFs are reported, wet-weight BCFs will be 398
estimated by assuming a 100:1 ratio of biofilm wet mass to biofilm dry mass. Finally, many 399
studies for the bioaccumulation of ENM quantify total metal uptake, not ENM specific uptake. 400
Unless controls for dissolution or specific quantification of ENM is stated, all BCFs reported 401
here will reflect this, limiting their representation of "true" ENM BCFs. Since most studies do 402
not report detailed kinetic analysis of ENM bioaccumulation, characteristic times, 𝑡0, of 403
bioaccumulation will be estimated when possible. Estimations of these are mostly qualitative, 404
representing approximately the time necessary to reach concentrations 50% of equilibrium 405
concentrations. 406
The data in this study are 2 – 10 times less than the pBCF reported in literature, Table 2. 407
While this hydrogel matches mechanical properties better than alginate, many biofilms contain 408
both alginate and nanocellulose polymers. Lastly, biofilms are much more than cells or beads 409
distributed in a hydrogel mesh, they also contain channels filled with pore water [55]. Equation 2 410
shows that if the amount of nanoparticles in the pore water is in equilibrium with the surrounding 411
water, the BCF in a porous biofilm will be less than an equivalent amount of nanomaterials being 412
added to a fixed amount of biofilm mass without. Equivalently, the pBCF of a biofilm with pores 413
will be greater than one without for the same amount of substance added to the biofilm, by a 414
factor of log2 for biofilm of equal weight to water. 415
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24
𝑚!"#,% + 𝑚!"#
𝑚% + 𝑚&
𝑚!"#/𝑚&
=
𝑚!"#,% + 𝑚!"#
𝑚% + 𝑚&
𝑚!"#/𝑚&
=
(𝑚!"#,% + 𝑚!"#)/𝑚%
1 + 𝑚&/𝑚%
𝑚!"#/𝑚&
<
𝑚!"#,% + 𝑚!"#
𝑚%
𝑚!"#/𝑚&
Equation 2
416
417
Table 2: Summary of literature on bioaccumulation and bioconcentration kinetic parameters of ENMs in
periphytic biofilms. n.d. no data reported. *Some hydropathies are inferred. Titanium dioxide hydropathy
depends on crystal phase which also modifies its toxicity [59].
Type Biofilm Size (nm) Hydropathy Charge tC pBCF Study
Latex
carboxylate
Wetland 100 Hydrophilic (-) < 24 h ~2 [60]
Gold Estuary 65 Hydrophobic (+) < 12 d 2.18 [61]
Gold polystyrene
sulfonate
Estuary 50 Hydrophobic* -53 mV ~12 h 3.46 [22]
Citrate capped
silver
Estuary 30, 115 Hydrophobic (-) ~12 h 1.4 – 1.5 [62]
Citrate capped
silver
Marine 100 – 700 Hydrophobic -18 mV 10 min , < 4 d 4.6 [63]
Titanium dioxide Algal 150 n.d.* -17 mV < 28 d 4 - 5.6 [64]
Copper oxide Periphyton 100 – 800 Hydrophilic* -35 – +15 mV ~50 min 3.6 – 4.25 [65]
Citrate capped
silver
Aquabacteri
um
citratiphilum
30, 70 Hydrophobic -60 mV < 20 h 0.8 [66]
FITC-Dx-150 Hydrogel 92 – 240 Hydrophilic -1.2 ± 0.4 mV 24 min 0.153
FTIC-Dx-2000 Hydrogel +
neutral
spheres
81 – 330 Hydrophilic -2.4 ± 0.7 mV 24 min 0.319
FITC-Dx-150 Hydrogel +
neutral
spheres
92 – 240 Hydrophilic -1.2 ± 0.4 mV 24 min 0.164
FITC-DEAE-150 Hydrogel +
neutral
spheres
91 – 183 Hydrophilic -0.4 ± 0.4 mV 24 min 0.132
FITC-CM-150 Hydrogel +
neutral
spheres
173 – 1000 Hydrophilic -5.7 ± 3.2 mV 24 min 0.160
FITC-Dx-150 Hydrogel +
carboxyl (-)
spheres
92 – 240 Hydrophilic -1.2 ± 0.4 mV 24 min 0.145
FITC-DEAE-150 Hydrogel +
carboxyl (-)
spheres
91 – 183 Hydrophilic -0.4 ± 0.4 mV 24 min 0.179
FITC-CM-150 Hydrogel +
carboxyl (-)
spheres
173 – 1000 Hydrophilic -5.7 ± 3.2 mV 24 min 0.135
FITC-Dx-150 Hydrogel +
amino (+)
spheres
92 – 240 Hydrophilic -1.2 ± 0.4 mV 24 min 0.125
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FITC-DEAE-150 Hydrogel +
amino (+)
spheres
91 – 183 Hydrophilic -0.4 ± 0.4 mV 24 min 0.158
FITC-CM-150 Hydrogel +
amino (+)
spheres
173 – 1000 Hydrophilic -5.7 ± 3.2 mV 24 min 0.068
418
In summary, a systematic analysis through a synthetic biofilm model adds to the toolkit 419
of biointerface studies. Size exclusion has been replicated in alginate [41] and now in 420
nanocellulose. While attachment and volume-exclusion were not replicated, future work using 421
similar matrices should also consider concentration of microspheres within the nanocellulose 422
matrix. For example, there may be a critical concentration of microspheres or bacterial cells 423
necessary for some of the absorption effects. While these can be studied with non-toxic 424
nanomaterials, these affects are often very difficult to uncouple in living systems [67]. 425
5. Conclusion 426
This study aimed to emulate key physicochemical barriers to diffusion found in natural 427
biofilms using tunable synthetic microcap biofilm matrix system. Through the controlled 428
exposure of nanodextrans with varying size and surface charge, we evaluated the system’s ability 429
to emulate three core physicochemical features often implicated in biofilm-associated transport 430
resistance: size exclusion, charge interactions, and volume exclusion. The results demonstrated a 431
statistically significant size-exclusion effect, confirming the ability of the nanocellulose-based 432
microcaps to mimic the selective permeability of hydrated biofilm matrices. However, the 433
designed system did not display statistically significant volume-exclusion or attachment effects, 434
suggesting that the current microsphere concentration and charge configurations were 435
insufficient to replicate these additional features. 436
These findings reflect patterns observed in natural biofilms studies, where size-based 437
diffusion hinderance is commonly reported, but charge-based interaction and volume exclusion 438
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are more context-dependent. The absence of strong attachment or volume exclusion effects may 439
be due to insufficient microsphere loading, incomplete charge immobilization, or the dynamic 440
behavior of the nanodextrans in the hydrated mesh. 441
Future studies should explore increased microsphere loading, use of covalently bound 442
attachment sites or incorporation of more biologically relevant surface chemistries to better 443
recapitulate these additional transport-limiting features. Ultimately, refining this synthetic 444
biofilm platform will enhance its utility in advancing the ecotoxicology of engineered 445
nanomaterials. 446
447
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