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Title: Ecotoxicological studies of micro- and nanosizedbarium titanate on aquatic photosynthetic microorganisms
Author: Hudson C. Polonini Humberto M. Brandao NadiaR.B. Raposo Ludovic Mouton Claude Yepremian Alain CouteRoberta Brayner
PII: S0166-445X(14)00164-7DOI: http://dx.doi.org/doi:10.1016/j.aquatox.2014.05.005Reference: AQTOX 3842
To appear in: Aquatic Toxicology
Received date: 10-3-2014Revised date: 28-4-2014Accepted date: 6-5-2014
Please cite this article as: Polonini, H.C., Brandao, H.M., Raposo, N.R.B., Mouton, L.,Yepremian, C., Coute, A., Brayner, R.,Ecotoxicological studies of micro- and nanosizedbarium titanate on aquatic photosynthetic microorganisms, Aquatic Toxicology (2014),http://dx.doi.org/10.1016/j.aquatox.2014.05.005
This is a PDF file of an unedited manuscript that has been accepted for publication.As a service to our customers we are providing this early version of the manuscript.The manuscript will undergo copyediting, typesetting, and review of the resulting proofbefore it is published in its final form. Please note that during the production processerrors may be discovered which could affect the content, and all legal disclaimers thatapply to the journal pertain.
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Ecotoxicological studies of micro- and nanosized barium titanate on aquatic
photosynthetic microorganisms
Hudson C. Polonini †
, Humberto M. Brandão‡, Nádia R. B. Raposo
†, Ludovic
Mouton§, Claude Yéprémian¥, Alain Couté¥, Roberta Brayner*
§
†Universidade Federal de Juiz de Fora, Núcleo de Pesquisa e Inovação em Ciências da
Saúde (NUPICS), Rua José Lourenço Kelmer, s/n, 36036-900, Juiz de Fora, Brasil
‡Empresa Brasileira de Pesquisa Agropecuária (Embrapa Gado de Leite), 36038-330,
Juiz de Fora, Brasil
§Université Paris Diderot, Sorbonne Paris Cité, Interfaces, Traitements, Organisation
et Dynamique des Systèmes (ITODYS), UMR 7086, CNRS, 15 rue Jean de Baïf, F-
75205 Paris Cedex 13, France
¥ Muséum National d’Histoire Naturelle, Département RDDM, USM 505, 57 rue
Cuvier, F-75005 Paris, France
Tel.: +33 1 57 27 87 64. Fax: +33 1.57.27.72.63
E-mail: [email protected]
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INTRODUCTION
The interaction between live organisms and micro- or nanosized materials has become
a current focus in toxicology – or nanotoxicology, as it’s been currently called
(Dukhin et al., 2010). This is due, to a large extent, to the fact that smaller particles
can be more toxic than bulk materials with the same composition, mostly because of
their increased specific surface area and reactivity (Panf et al., 2012). However, a
thorough understanding of the threats these materials pose to the environment is not
completely available yet (Brayner et al., 2010).
Nanosized barium titanate (BT) has gained momentum lately in several fields, being a
promising future biological nanocarrier for proteins (Ciofani et al., 2010a), as an
enhancer of the uptake of low molecular weight drugs such as doxorubin (Ciofani et
al., 2010b), as a biomarker, through the bioconjugation of its nanocrystals with
immunoglobulin G (IgG) antibodies for imaging probes (Hsieh et al., 2010), as well
as in the design of bone graft material (Ball et al., 2013). In the meantime, in vivo
long-term biocompatibility experiments and studies on its impact on the environment
have not yet been performed, to the best of the authors’ knowledge. Therefore, it is a
material with high future biomedical applications, but with scarce safety data.
For these investigations, physico-chemistry is paramount when trying to understand
the fate and behavior of the particles on the environment (Brayner et al., 2010), to the
extent that characteristics such as size, state of dispersion, surface charge, shape,
chemical composition, surface area, and surface chemistry play important roles in the
uptake and distribution of the particles within live organisms (Oberdörster et al.,
2005a, 2005b; Powers et al., 2006). Also, it is paramount that the particle
characterization is performed in relevant media (Jiang et al., 2009), i.e., those where
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the ecotoxicological experiments will take place, wherein potential physicochemical
changes (e.g., agglomeration/aggregation and surface charge variation) can occur with
the particles in different solutions – which, in turn, can have direct impact on the
toxicological responses (Powers et al., 2007). Since BT presents a perovskite
structure, it is expected to show thermodynamic instability and reactivity in aqueous
environment (Lee, 1998), one of the reasons why not only a natural culture media was
used in this study, but also a synthetic one, with a high content of nutrients. Actually,
different dispersions of BT either in aqueous or in non-aqueous media have already
been studied (Khastgir et al., 2001; Paik et al., 1998; Bergstrm et al., 1998; Lee, 1999;
Lee, 1998; Wang et al., 2000), but none of them covered all of the characterizations
listed here or were performed in biorelevant media for toxicological assays.
In this study, we used two different test organisms: a colonial cyanobacteria
(Anabaena flos-aquae) and a flagellated unicellular euglenoid (Euglena gracilis),
which are quite different morphologically and metabolically. This can be helpful to
provide a spectrum of actions of the particles, although both are representatives of the
first aquatic trophic level (producers). The use of primary producers as biological
indicators is important because they are situated at the base of the food chain and any
change in the dynamics of their communities can affect higher trophic levels of the
ecosystem. Typically, they are also quite sensitive to changes in the environment and
have relatively short life cycles, which allows the observation of toxic effects in
several generations (Cleuvers and Weyers, 2003; Costa et al., 2008). Yet, the aquatic
toxicity model was chosen because these ecosystems are the main enclosures of
contaminants, whether they are coming from direct waste into water bodies through
the discharge of effluents or released into the air or deposited in the soil (Kendall et
al., 2001).
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Thus, the aims of the present work are: (i) to assess BT toxicity and its mechanisms in
two photosynthetic organisms (A. flos-aquae and E. gracilis); (ii) to study and
correlate the physicochemical properties of BT with its toxic profile; (iii) to compare
the BT behavior and the toxic profile in synthetic (Bold’s Basal, BB, or Mineral
Medium, MM) and natural culture media (Seine River Water, SRW); and (iv) to
address whether size is an issue in toxicity of BT particles.
MATERIAL AND METHODS
The subjects of the study: BT particles and test organisms
BT characterization
Two different lots of commercial BT powders were obtained from Sigma-Aldrich,
namely BT MP (barium titanate microparticle) (CAT n. 338842, lot MKBD3182V,
<2μm) and BT NP (barium titanate nanoparticle) (CAT n. 467634, lot MKBF7837V,
<100nm and cubic crystalline phase).
The X-ray diffraction (XRD) patterns of the powders were recorded with a X’pert Pro
diffractometer (PANalytical), equipped with a multichannel X’celerator detector, and
using the Co Kα radiation (= 1.790307 Å), in the 2θ range 5°-120°, with a scan step of
0.05° for 5s. The sample holder used was a Si monocrystal. Morphological
observation of powders by scanning electron microscopy (SEM) was done using a
Zeiss Supra 40 microscope equipped with an in-lens detector. Low excitation voltage
(2.5 kV) and a small working distance (3 mm) were used, so that the charging effects
were minimal to the point that the metallization of powders was not necessary, and
then true features were not masked. Transmission electron microscopy (TEM) images
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were obtained using a JEOL 100CX-II microscope operating with an accelerating
voltage of 100 kV. The specimens were prepared by ultrasonically dispersing the
powders in ethanol prior to deposition on SEM mounts and carbon-coated TEM grids.
The specific surface area (Sg) and pore size were measured by the collection of
nitrogen (N2) adsorption–desorption isotherms on a Gemini V 2380 system (Mic
America, Inc.) at 77 K after the sample had been dried at 160 °C for 1 h. The
Brunauer–Emmett–Teller (BET) surface area was calculated from the linear part of
the BET plot. The pore size distribution was obtained from a QUANTACHROME-
Autoscan 33 mercury porosimeter.
The hydrodynamic size and the surface charge/interparticle forces (zeta potential, ζ)
of the dispersions of BT powders (100 μg mL–1, or 4.28 × 10–7 M, – in BB medium
and SRW) were characterized using a ZetaSizer Nano ZS (Malvern Instruments Inc.)
utilizing dynamic light scattering (DLS) and electrophoretic light scattering (ELS),
respectively. Effects of pH variation in the media (3, 5, 7, 9, 12, adjusted with HNO3
or NaOH in different molarities) were evaluated, as well as the degree of aggregation
as a function of time (0, 24, 48, 72 and 96h). The dispersions were sonicated (100W,
5 min) daily before analysis in order to disperse agglomerates and so that it could be
inferred that increased hydrodynamic sizes are due to aggregation. Response surfaces
were built up in order to evaluate the roles each factor plays at the aggregation state or
the surface charge of the BT dispersions. A 52 factorial experimental design (two
factors, time and pH, with 5 levels of variations each) was used according to
Montgomery (2012) and Polonini et al (2011), which provide the theoretical
background for the graphical representation used (see Supplementary Material). The
factors and their levels (codified levels in parenthesis, and real ones outside them)
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were X1: time [(–1) 0h, (–0.5) 24h, (0) 48h, (0.5) 72h, (1) 96h] and X2: pH [(–0.88) 3,
(–0.44) 5, (0) 7, (0,44) 9, (0.88) 12].
The degree of dissolution of the BT powders as a function of time (1, 2, 4, 8, 24, 48,
72 and 96h) within the media (BB medium and SRW) was evaluated following a
protocol proposed by Sivry et al. (2013). Briefly, from a stock solution (100 μg mL–1,
final volume = 100 mL) prepared at time 0, aliquots (3.5 mL) were withdrawn at the
specified time intervals and ultra-filtred using 3 kDa filters (Microsep Advance
Centrifugal Device, Pall Corporation), placed in a centrifuge (EBA 8, Hettich) for 1h,
and then added with 50 μL of saturated HNO3 (with no trace of Ba2+). All solutions
were immediately frozen until elemental analysis (Ba2+) was performed by
inductively coupled plasma optical emission spectrometry (ICP-OES) (iCAP 6200,
Thermo Scientific). Detection limit was set as 1.0 ppb. The remaining aqueous
dispersion (72 mL) was centrifuged at 20,000 × g (Sorvall Lynx 6000, Thermo
Scientific) and the media was completely evaporated in an oven at 50°C. The dry
residues were then analyzed by XRD and X-ray photoelectron spectroscopy (XPS)
(Thermo VG Escalab 250, using Al Kα of 1486.6 eV, 15 kV, 150 W) for evaluation of
the chemical/surface changes that might possibly have occurred.
All reagents were analytical grade, and ultrapure water (18.2 MΩ cm resistivity at 25
°C and < 10 ppb total organic carbon) was obtained with an Elga Pure-Lab Classic
UV.
Cell cultures
Anabaena flos-aquae planktonic prokaryotic cyanobacteria, strain ALCP B24, and
Euglena gracilis eukaryotic euglenoid came from the Muséum National d’Histoire
Naturelle (MNHN) Culture Collection.
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A. flos-aquae was grown in 275 mL (= 75 cm2) Erlenmeyer flasks with air-permeable
stoppers, in (i) sterile BB medium (Table S1) with pH adjusted to 7.0 using 1 M
NaOH and buffered with 3.5 mM phosphate buffer solution or (ii) SRW (Table S2)
(measured pH = 8.01), at a controlled temperature of 20.0 ± 0.5°C and a luminosity of
30-60 μmol m–2 s–1 photosynthetic photon flux (PPF), under ambient CO2 conditions.
E. gracilis was grown in 250 mL Erlenmeyer flasks, in (i) sterile mineral medium
(MM) (Table S3) with pH adjusted to 4.0 using 1 M HCl or (ii) SRW (measured pH =
8.01), at a controlled temperature of 20.0 ± 0.5°C and a luminosity of 70-100 μmol m–
2 s–1 photosynthetic photon flux (PPF), under ambient CO2 conditions.
SRW, representative of a highly anthropized watershed, was collected near the
University of Paris 7 – Diderot, Paris, France (GPS: 48.831039°N, 2.381709°E). The
sample was immediately filtered after collection through a 0.22 μm acetate membrane
(Millipore) under vacuum to remove contaminants and microorganisms and stored in
pre-cleaned, acid-washed polyethylene bottles, at 4°C until analysis.
Toxicological assessment
Stock suspensions containing 1000 μg mL–1 by weight of BT powders were obtained
by sonicating aliquots of 10 mg of BT MP or BT NP in 10 mL SRW, BB or MM for
10 min at 200W (VWR, USA). The sonication was used to break micrometric
aggregates and stabilize the suspensions. Aliquots of these suspensions were then
added to the batch cultures (exponential growth organisms, prepared 3 days before
starting the test at a concentration of 5.0 × 105 cells mL–1) to obtain the final
concentrations of BT powders corresponding to 1, 25, 50, 75 and 100 μg mL–1 (or
4.28 × 10–8, 1.07 × 10–7, 2.14 × 10–7, 3.22 × 10–7, and 4.28 × 10–7 M, respectively).
Therefore, this study uses higher concentrations than for contamination in natural
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water, aiming to assess the acute toxicity of the materials. The experiment was also
conducted with Ba2+ at 1.5 μg mL–1 (7.28 × 10–6 M) because of the degree of
dissolution of the particles, which did not exceed 1.5%.
The toxic response was evaluated by means of cell counting at 24, 48, 72 and 96h
after the BT powders spiking, as a function of the exposure concentration in
comparison with the average growth of replicate, unexposed control cultures. The cell
counting was performed with bright field microscopy, using the Cellometer Auto X4
(Nexcelom, USA), which simultaneously calculates the percentage of cell viability
(live/dead test, conducted with the trypan blue dye, which selectively colors dead
cells blue).
The average specific growth rate (μ) was calculated as the logarithmic increase in the
cell counting from the following equation for each single flask of controls and
treatments, from days 0 to 4 (calculated section-by-section):
(1)
where is the cell count at time i and is the same parameter at time j.
The percent inhibition of growth rate for each treatment replicate was then calculated
as:
(2)
where is the percent inhibition in average specific growth rate, is the mean
value for average specific growth rate (μ) in the control group, and is the average
specific growth rate for the treatment replicate. Finally, the inhibition percentage for
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each BT powder was plotted against the logarithm of the BT concentrations, and then
the regression analysis was performed to obtain the values of the concentration of the
BT powders suspended in test medium that results in a 50% reduction in the growth
within the exposure period (ErC50).
Assessment of the factors linked to the toxicity
Microscopical observation
The interaction between the test organisms and the treatments (100 μg mL–1, after 72h
of exposure) were observed using SEM and TEM. For SEM, control and treatments
were fixed with a mixture containing 2.5% of glutaraldehyde and 1.0% of picric acid
in phosphate Sörengen Buffer (0.1 M, pH 7.4). Dehydration was then achieved in a
series of ethanol baths (from 50% to100%). The samples were dried with a BAL-TEC
CDP 030 supercritical point dryer after ethanol baths. The images were obtained in a
Zeiss Supra 40 microscope equipped with an in-lens detector. Low excitation voltage
(2.5 kV) and a small working distance (3 mm) were used, so that the charging effects
were minimal to the point that the metallization of powders was not necessary, and
then true features were not masked.
For TEM, control and treatments were fixed with a mixture containing 2.5% of
glutaraldehyde and 1.0% of picric acid in phosphate Sörengen Buffer (0.1 M, pH 7.4).
Post-fixation using osmium tetroxide (OsO4) was conducted and the dehydration was
achieved in a series of ethanol baths (from 50% to 100%). The samples were
processed for flat embedding in a Spurr resin, and then ultrathin sections were made
using a Reicherd-Young Ultracut microtome (Leica). Sections were contrasted with a
4% aqueous uranyl acetate solution and Reynold’s lead citrate before visualization,
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which was performed in a Tecnai 12 operating at 80kV equipped with a 1Kx1K Keen
Viewcamera.
Effect of particles on aggregation and surface charge of test organisms
The hydrodynamic size and the zeta potential of the test organism cultures with added
BT MP or BT NP in BB, MM or SWR (100 μg mL–1, at 0, 24, 48, 72 and 96h of
exposure) were characterized using a ZetaSizer Nano ZS (Malvern Instruments Inc.).
Effect of particles on oxidative stress in test organisms
The activity of superoxide dismutase (SOD), which catalyzes the dismutation of the
superoxide anion (O2.-) into hydrogen peroxide and molecular oxygen, was quantified
in the controls and treatments (1, 50 and 100 μg mL–1, at 24, 48, 72 and 96h of
exposure) using a SOD Assay Kit-WST 19160 (Sigma-Aldrich, Germany). This
allows very convenient SOD assaying by utilizing Dojindo’s highly water-soluble
tetrazolium salt, WST-1 (2-(4-Iodophenyl)- 3-(4-nitrophenyl)-5-(2,4-disulfophenyl)-
2H-tetrazolium, monosodium salt) that produces a water-soluble formazan dye upon
reduction with a superoxide anion. The reduction rate with O2 is linearly related to the
xanthine oxidase (XO) activity, and it is inhibited by SOD. Therefore, the IC50 (50%
inhibition activity of SOD or SOD-like materials) can be colorimetrically determined.
The controls and treatments were incubated at 37°C for 20 min, and then read at 450
nm using an Envision Multilabel Plate Reader (Perkin-Elmer, USA).
Effect of particles on the photosynthetic activity of test organisms
The photosynthetic activities of the controls and treatments (1, 50 and 100 μg mL–1, at
24, 48, 72 and 96h of exposure) were determined by the Pulsed Amplitude
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Modulation (PAM) method, using a Handy PEA (Hansatech, UK) fluorometer. This
method uses the saturation pulse principle, in which a sample is subjected to a short
pulse of light, which saturates the photosystem II (PSII) reaction centers of the active
chlorophyll molecules. This process suppresses photochemical quenching, which
might otherwise reduce the maximum fluorescence yield. A ratio of variable over
maximal fluorescence (Fv/Fm) can then be calculated, which approximates the
potential quantum yield of PSII.
Effect of particles on the test organisms’ mitochondria
Intracellular levels of adenosine-5-triphosphate (ATP) in controls and treatments (1,
50 and 100 μg mL–1, at 24, 48, 72 and 96h of exposure) were quantified using an ATP
Bioluminescent Assay (Sigma-Aldrich). Cell lysis of test organisms was mechanically
achieved in a vortex using glass beads followed by centrifugation (15 min at 2000 ×
g), in order to obtain the free ATP in the supernatant. The assay can determine the
ATP in samples containing 2 × 10–12 to 8 × 10–5 M by quantitative bioluminescence.
ATP is consumed and light is emitted when firefly luciferase catalyzes the oxidation
of D-luciferin. When ATP is the limiting reagent, the light emitted is proportional to
the ATP present into the cells. The relative luminescent units were detected with an
Envision Multilabel Plate Reader equipped with a luminescent optical filter.
Statistical analysis
Statistical analyses were performed using SPSS v.14.0. For comparisons among
control and treatments, ANOVA followed by Tukey’s post-hoc test was conducted for
the variables meeting the criteria of normality (Shapiro-Wilk test, p > 0.05),
homoscedasticity (variance homogeneity, Levene test, p > 0.05) and independence
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(Durbin Watson test, p ~ 2.0). For the variables which violated the assumptions for
ANOVA validity, the non-parametric Kruskal-Wallis test was conducted. Differences
between groups were considered statistically significant when p ≤ 0.05 and
marginally significant when 0.05 < p ≤ 0.1.
RESULTS AND DISCUSSION
Description and characterization of the materials
The two materials used in this study were previously characterized (Supplementary
Material). Briefly, they were identified by XRD as tetragonal BaTiO3 (BT MP) and
cubic BaTiO3 (BT NP), with average crystallite sizes of 172.0 ± 102.4 Å (with 0.19 ±
0.06% of micro strain) and 60.0 ± 16.7 Å (0.10 ± 0.05%), respectively. Using SEM
and TEM, the diameter of the particles could be estimated as 150 nm (BT MP) and 60
nm (BT NP), and the BT MP presented some degree of polydispersion. The BET
surface area was calculated as 3.24 m2 g−1 for BT MP and 16.60 m2 g−1 for BT NP,
the total pore volumes were 0.006 and 0.07 cm3 g−1, respectively, and the mean pore
diameters were 7.34 and 17.46 nm, respectively.
Since BT presents a perovskite structure, it is expected to have some thermodynamic
instability and reactivity in aqueous environment (Lee, 1998), which is evidenced by
the DLS measurements performed (Figure 1). Zeta potential results showed that in
general both particles are negatively charged. BT MP was more stable in BB and M
media, as one can observe a greater number of flat response surfaces, and as the
charge in SRW approached 0 after longer periods in suspension. The same behavior
was observed for BT NP, except in M medium in which the charge surpassed -30 mV
at the beginning of the experiments with lower pHs, but then it tended to approach 0
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over time. Apart from this case, none of the materials showed values high enough to
ensure colloidal stability, which must be at minimum 25 mV (Verwey and Oberveek,
1948; Planchon et al., 2013). This instability can actually be observed as
sedimentation in the suspension after some hours. As for the media, SRW shows a
more pronounced particle instability than the other ones. As surface charge affects the
uptake and the translocation of the particles by live organisms (Hoshino et al., 2004),
it can be expected that the particles will show distinct effects on the microorganisms,
either because of their very nature or due to their different behavior in each medium.
INSERT FIGURE 1 NEAR HERE
Another physicochemical parameter of the particles which is directly related to their
interaction with living systems is their size, since it is related to the degree of
absorption, distribution, metabolism and excretion by live organisms (Jiang et al.,
2009). The hydrodynamic size of the particles was evaluated as a function of pH and
time (Figure 2), in the same manner as performed to zeta potential measurements. The
solutions were sonicated before each measurement, in order to make clear that the
results found were due to aggregation, and not agglomeration (weak van der Waals
bonds). This is important because the aggregation of the particles can influence on the
toxicity profiles for microorganisms, since large aggregates held by strong chemical
bonds do not penetrate cells, and in these cases the effects can be more attributable to
dissolved ions rather than a direct contact (Wang et al., 2010). In BB medium, it
seems that the pH does not influence the aggregate size, unlike the time, which played
a notable role on this parameter, as the aggregate formation seems to increase largely
throughout the days in both particles. The same phenomenon happened in MM and
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SRW, but in this case a decrease in pH also led to an increase of aggregate sizes. For
MM, the BT NP aggregates were bigger than for the BT MP.
INSERT FIGURE 2 NEAR HERE
Finally, the degree of dissolution of the particles was also evaluated, as the release of
ions into the media can account for a different degree and mechanism of toxicity to
the microorganisms. This was assessed by ultrafiltration, followed by the
quantification of Ba2+ leached out from the particles into the media at the pH in which
the toxicological assessment was conducted (7.0 for BB, 4.0 for MM and 8.01 for
SRW) (Figure 3).
INSERT FIGURE 3 NEAR HERE
BT NP released more Ba2+ in the media than BT MP – 1,132 ppb after 96h in BB
medium, 6.5 times more than BT MP in the same medium; 1,258 ppb after 96h in
MM against 345 ppb from BT MP, 3.6 times more; and 1,368 ppb in SRW after the
same period, 3.4 times greater than BT MP. SRW had a more pronounced effect in
the phenomenon, once it dissolved BT MP 2.9 times more than the BB medium and
1.15 more than MM; and BT NP 1.2 times greater in BB and 1.08 in MM. Thus, such
differences can be attributed to the compositional differences between the two media
(see Supplementary Material) rather than to their pH, since SRW has only a slightly
higher pH than BB medium – although the difference is big between MM and the
others. Yet, the dissolution rates of the powders in BB medium or SRW were not
greater than 1.5%. This is the reason why this was the concentration of free Ba2+ ions
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chosen (1.5 μg mL–1, or 7.28 × 10–6 M) to perform the toxicological assessment,
where it was evaluated whether the released (and consequently penetrated) ions could
be a potential reason for the toxicity.
After the 96-h experiments, the XRD patterns of the remaining powders were
assessed (Figure S1), and no significant difference was observed between media. XPS
analyses of the residues were also performed, and the results can be seen in Table S4.
The Ba/Ti/O ratio is in good agreement with the low solubility verified by ICP-OES.
Carbon (C) is a common impurity in ultrahigh vacuum (UHV), and the signals around
285 eV (hydrocarbon) are ordinarily used as internal standard to reference other
elements when charging occurs (López et al., 1999). However, its presence in more
than one state is an indicative of the formation of BaCO3 (also observed by Ba
binding energy at ~780 eV). The deconvolution of the C 1s peak gave a peak of
carbonate in a BaCO3 surface at 288-289 eV. BaCO3 may be a byproduct of the
BaTiO3 synthesis, whichever route is used, or derived from the tendency of CO2 to
adsorb on perovskite surfaces, due to dipole-dipole interaction between the
ferroelectric BaTiO3 crystal and the polar CO2 molecule (López et al., 1999). As this
component is absent in the traces, one can expect that the carbonate may be formed as
a discrete second phase (~2%) rather than as a surface film.
INSERT TABLE 1 NEAR HERE
Thus, the main conclusions from the characterization studies are that BT NP presents
a higher reactivity than BT MP, and that SRW is a more instable than the other media,
thereby contributing to such behavior, according to the zeta potential and the results
of the dissolution experiments. Yet, the time the particles remain in suspension led to
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an increment in aggregate formation. Once again, these different behaviors can be
expected to lead to different effects on the growth of model organisms.
Ecotoxicological assessments
The two test organisms used in this study are quite different morphologically and
metabolically, which can be helpful to provide a spectrum of actions of the particles.
The cyanobacteria A. flos-aquae is composed of one linear series of vegetative cells,
and generally possesses a lot of thick-wall heterocysts dispersed all along the
trichome (Brayner et al., 2010, 2011). E. gracilis, in turn, shows a remarkable
metabolic plasticity: it can behave as either autotrophic and photosynthetic (when
grown in the presence of light, and it is green) or as heterotrophic (when grown in the
dark, and it is colorless) (Einicker-Lamas et al., 2002). In our case, it is expected that
they show an autotrophic behavior. Yet, they can perform endocytosis and they have
the ability to move by using a flagellum, a long whiplike structure (Brayner et al.,
2010, 2011).
In the first stage, the direct effects of growth on these two organisms were assessed, i.
e., their growth after addition of BT MP and BT NP (Figure 4). A decrease on growth
was observed in both organisms, but this effect was more pronounced in E. gracilis,
for which both BT MP and BT NP led to significant growth inhibition (p<0.05) in all
concentrations tested, in both media, and since the first cell counting, after 24h of
contact. However, BT MP showed a more toxic effect than BT NP, especially in
SRW. For A. flos-aquae, the toxic effects were significant only after 72h of exposure,
and for the largest concentrations of the materials (after 96h: ≥ 75 μg mL–1 for BT NP
and =100 μg mL–1 for BT MP, in BB; and ≥ 75 μg mL–1 for both materials in SRW).
On the other hand, Ba2+ did not cause a significant reduction of growth (none for A.
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flos-aquae and only after 96 h for E. gracilis), an observation contrary to other studies
that show that the toxicity of agglomerated nanoparticles to microorganisms can be
explained by dissolved metal species (Wu et al., 2010). Although barium is known to
be reactive with air and water (Fromm, 2013), its toxicity is lower than that of most
heavy metals (López-Róldan et al., 2013), and previous studies confirm that this
alkaline earth metal is toxic only at very high concentrations (Lamb et al., 2013;
Monteiro et al., 2011; Kopittke et al., 2011). Yet, it can also be observed that the
inhibition of growth was slightly more pronounced within the SRW than within the
artificial media, BB or MM.
INSERT FIGURE 4 NEAR HERE
However, the test performed to assess the viability of the organisms showed
discrepant results, at least for A. flos-aquae (Figure 5). While no significant growth
inhibition was observed in this organism, the viability of its membrane has been
observed to be damaged in all tested concentrations for both substances from the first
day of observation, in BB medium or SRW – although the differences were more
pronounced within the latter, as one can see in Figure 4. The same was observed with
E. gracilis, an expected result, departing from the growth inhibition observed.
INSERT FIGURE 5 NEAR HERE
The assessment of cell membrane integrity was performed using the dye exclusion
method with trypan blue. It is based on the principle that intact membranes exclude
certain dyes, such as trypan blue (Strober, 2001). Normally, the viability results can
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be correlated to the mortality of cells – dead cells would not exclude the dye, and then
they appear blue in photonic microscope. In our case, however, this can be true to E.
gracilis, but not A. flos-aquae. For the latter, we can suppose that the cells have lost
some of its membrane functionality, which does not necessarily represent a fatal
event. The cell probably developed some unknown mechanism to survive in this
adverse situation.
Calculating the ErC50, was limited by the concentrations used. Using the results, some
theoretical values were above the concentrations used. For A. flos-aquae: 1271.5 μg
mL–1 for BT MP and 1208.5 μg mL–1 for BT NP, in BB; and 1047.3 μg mL–1 for BT
MP and 1117.4 μg mL–1 for BT NP, in SRW. For E. gracilis: 878.1 μg mL–1 for BT
MP and 627.8 μg mL–1 for BT NP, in MM; and 63.9 μg mL–1 for BT MP and 414.5
μg mL–1 for BT NP, in SRW. This is in accordance with a higher sensitivity of E.
gracilis, especially for BT MP. For a more realistic result, new assessments with
higher concentrations should be performed. However, the highest concentration used
in this study is already higher than what is expected to be found in nature during an
acute exposure, i.e., nanoparticle concentration around 10– 9 M (Planchon et al, 2013).
Despite the ErC50 being greater than the concentrations used (except for BT MP in E.
gracilis), toxic effects on growth and viability did occur, and this fact may have
different origins, based on what is already known from the literature. Here we
consider that the two main possible mechanisms of the observed toxicity are: (i) a
direct contact of BT particles with the cell wall (Gogniat et al., 2006), linked to a
theoretical penetration of the smallest particles and/or released ions (Planchon et al.,
2013); and/or (ii) an indirect effect through the generation of reactive oxygen species
(ROS) (Brayner et al., 2006; Chae et al., 2011). Thus, we performed different assays
to assess which is the possible one involved in BT toxicity to the model organisms.
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Assessment of the factors linked to the toxicity
SEM and TEM analysis of the microorganisms (Figures 6 and 7) allow a direct
visualization of the morphological changes they suffer upon contact with the particles.
For A. flos-aquae exposed to BT particles for 72h in a concentration of 100 μg mL–1,
the morphology of the cells when observing them by SEM did not change with the
treatments, although they are a little more elongated when grown in BB medium than
when in SRW. Aggregates of cells and particles were observed (Figure 6I). The main
aspect to be pointed out is that the particles were found around the cell wall composed
by the polysaccharides, and the TEM images confirm that they did not penetrate the
cells.
INSERT FIGURES 6 AND 7 NEAR HERE
In the case of E. gracilis, the behavior of the cells under the same conditions was
completely different. The SEM images of E. gracilis controls, in both media, show
well-defined elongated cells possessing whip-like flagella. The images of cells from
treatments, however, differ greatly from these images. One can see that in both
treatments, BT MP and BT NP, cells are smaller, with a whipping-top shape, and with
no visible flagellum. This probably happens because of the endocytosis of the BT
particles and also of other substances contained into the media. The cell performed
endocytosis to such a degree that the membrane could not resist and actually ruptured,
as evidenced in Figure 7I. Thin sections of the microorganism in TEM show two main
features: nanoparticles internalized by endocytosis (Figure 7I) and a highly increased
production of bodies of paramylon, a carbohydrate similar to starch (Figures 7H, K
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and L). The chlorophyll found in E. gracilis chloroplasts can be of both a and b-types,
and they participate in the synthesis of carbohydrates, which are stored in euglenoids
cells in an unusual form known as paramylon, a B-1,3 polymer of glucose. These
paramylon bodies can be visualized as colorless or white rigid rods, and when they
achieve a concentration, which is too high for the cell to handle, the cell wall explodes
(Brayner et al., 2011). In this sense, SEM and TEM were complimentary to each
other, and both confirm that the high endocytosis of the particles led to an
overproduction of paramylon, which caused the explosion, and, consequently, the
death of the cells. This is an explanation to the fact that the cell count and the viability
in E. gracilis are low, but in A. flos-aquae only the viability is low – due to the fact
that the cells either died or lost their function, but they were still in their usual form
when the counting was performed.
Some correlation can be found between these observations and the results of surface
charge. For A. flos-aquae, the zeta potential of the cells is negative (Figure 8), as well
as that of the particles themselves (Figure 1). This is in agreement with an
electrostatic repulsion between microorganisms-particles, which hampers sorption. As
for E. gracilis, its surface charge is also negative, but very close to 0, and so this
repulsive force would not be strong enough to prevent the endocytosis. Regarding the
hydrodynamic size of the cell suspensions in absence or presence of particles, no
significant difference could be observed, but the remarkable growth of the size in A.
flos-aquae cultures – which is expected since it is a filamentary microorganism.
INSERT FIGURE 8 NEAR HERE
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The effect the particles in causing oxidative stress was also assessed (Figure 9). The
SOD activity was increased in A. flos-aquae growth in BB medium when exposed to
BT MP at 100 μg mL–1 and to BT NP in all concentrations tested, after 72h. When
grown in SRW, BT NP at 100 μg mL–1 significantly increased the SOD activity
already from the first day of assay, followed by the lower concentrations being
effective in the following days. BT MP at 100 μg mL–1 altered SOD activity after 48h
of exposure. For E. gracilis, both particles in all concentrations except for BT MP at 1
μg mL–1 exerted some effect on SOD activity. SOD activity plays a very important
role for the cell viability, since it protects them from the action of reactive oxygen
species (ROS), and so a higher SOD activity can be a reflection of a higher
exposure/production of ROS, which is associated with the activation of cell apoptosis
via the mitochondria (Cheng et al., 2011).
INSERT FIGURE 9 NEAR HERE
The increased ROS production is also known to affect photosynthesis (Figure 10)
(Rodea-Palomares et al., 2012). Indeed, the photosynthetic activity was found to be
reduced in the cells exposed to the particles. In A. flos-aquae, it differed from the
control in BB medium from the first hour assessed, for both particles; and in SRW,
the activity decreased after 48h of exposure. For E. gracilis, the effect was noticed
from the first hour for both media.
INSERT FIGURE 10 NEAR HERE
Together with the SOD activity, another measurement of the mitochondrial activity of
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the cells is the intracellular ATP content (Figure 11). The mitochondria are directly
related to the cell viability, since they are responsible not only for the ATP
production, but also for the ROS production and for the release of proteins, which
control the apoptosis (Pereira et al., 2014). In A. flos-aquae, the content of ATP
started to decline after 48h of exposure – for BB medium, it happened initially for the
higher concentrations, but after 72h all concentrations it exerted some effect, as it was
observed in SRW. For E. gracilis, the effects were seen from the first day. The
decline in ATP content may reflect a decrease in the mitochondrial activity, and so the
BT particles led to disturbances in the energy metabolism of the organisms. For the
eukaryotic Euglena cells, the strong endocytotic activity also plays a role in the
decline of ATPs, once the endocytosis process takes energy from ATP, synthesis
which is strongly associated with the transmembrane potential (Dukhin et al., 2001).
INSERT FIGURE 11 NEAR HERE
Thus, comparing the viability tests with SEM/TEM images and with SOD, ATP and
photosynthetic activity analysis, we may see that the BT particles, but not the released
Ba2+ ions, were toxic for both microorganisms at the prevailing exposure
concentrations. The cells of the first one died after endocytosing the particles in such
a quantity that the membrane was ruptured. The cells of the latter experienced toxic
effects caused by indirect contact with the particles. In this case, aggregates of
particles surrounding the cells were observed, and one can expect that this has caused
a decrease in the availability of the necessary nutrients for the gtowth of
microorganisms because of their predicted transport by the cell membrane was
disturbed – and even the light availability could be threatened by these large metallic
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aggregates – which to some degree could have subjected the cells to stress, causing
the increase in ROS production (Rogers et al., 2010; Xin et al., 2010).
Conclusion
Taking all the data together, the main conclusions are: (i) both BT MP (~170nm,
tetragonal) abd BT NP (~ 60nm, face-centered cubic) were negative and easily
aggregatable (unstable) in all aqueous media studied, with a release rate of Ba2+ ions
not exceeding 1.5%; (ii) BT has a low toxic effect on the growth of A. flos-aquae, but
both particles affect cell viability from the lowest concentration tested, which is
caused by indirect effect on oxidative stress in cells; (iii) BT has a statistically
significant toxic effect on cell growth and viability of E. gracilis from the lowest
concentration tested (1 μg mL–1), related to the effect of endocytosed particles in such
an amount that led to a rupture of their membranes – the effect was more pronounced
for BT MP; (iv) BT was able to stress all test organisms, which was evidenced by the
increase in SOD activity, and decrease in photosynthetic efficiency and in the
intracellular ATP levels; (v) the behavior of BT in synthetic and natural media culture
was different, with the most pronounced toxic effects when growth is given in ARS -
in this case a worse physiological state of microorganisms in ARS can occur in
organisms already stressed by the particles and cause a lower cell resistance\,
probably linked to a shortage of nutrients or even a synergistic effect with a
contaminant of the river; (vi) the size of BT does not influence the effects produced
on the growth of micro-organisms, with 95% confidence.
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FIGURES CAPTIONS
Figure 1. Zeta potential of (A) BT MP in BB medium, (B) BT MP in MM, (C) BT
MP in SRW, (D) BT NP in BB medium, (E) BT NP in MM, and (F) BT NP in SRW.
X1: time [(–1) 0h, (–0.5) 24h, (0) 48h, (0.5) 72h, (1) 96h] and X2: pH [(–0.88) 3, (–
0.44) 5, (0) 7, (0,44) 9, (0.88) 12].
Figure 2. Hydrodynamic size of (A) BT MP in BB medium, (B) BT MP in MM, (C)
BT MP in SRW, (D) BT NP in BB medium, (E) BT NP in MM, and (F) BT NP in
SRW.
X1: time [(–1) 0h, (–0.5) 24h, (0) 48h, (0.5) 72h, (1) 96h] and X2: pH [(–0.88) 3, (–
0.44) 5, (0) 7, (0,44) 9, (0.88) 12].
Figure 3. Dissolution rate of BT powders in terms of Ba2+ leached out as a function of
time.
Figure 4. Cell count of A. flos-aquae and E. gracilis as a function of concentration
and time of exposure to barium titanate particles.
Figure 5. A. flos-aquae and E. gracilis viability as a function of concentration and
time of exposure to barium titanate particles.
Figure 6. SEM micrographs of A. flos-aquae in BB medium [(A) control, (B)
exposed to BT MP, (C) exposed to BT NP] and in SRW [(D) control, (E) exposed to
BT MP, (F) exposed to BT NP]. TEM micrographs of C. vulgaris thin sections in BB
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medium [(G) control, (H) exposed to BT MP, (I) exposed to BT NP] and in SRW [(J)
control, (K) exposed to BT MP, (L) exposed to BT NP].
Figure 7. SEM micrographs of E. gracilis in BB medium [(A) control, (B) exposed to
BT MP, (C) exposed to BT NP] and in SRW [(D) control, (E) exposed to BT MP, (F)
exposed to BT NP]. TEM micrographs of C. vulgaris thin sections in BB medium
[(G) control, (H) exposed to BT MP, (I) exposed to BT NP] and in SRW [(J) control,
(K) exposed to BT MP, (L) exposed to BT NP].
Figure 8. Effect of barium titanate particles on aggregation (hydrodynamic size) and
surface charge (zeta potential) of A. flos-aquae and E. gracilis as a function of time of
exposure.
Figure 9. Superoxide dismutase (SOD) activity of A. flos-aquae and E. gracilis as a
function of concentration and time of exposure to barium titanate particles.
Figure 10. Photosynthetic activity of A. flos-aquae and E. gracilis as a function of
concentration and time of exposure to barium titanate particles.
Figure 11. Adenosine-5-triphosphate (ATP) content of A. flos-aquae and E. gracilis.
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Highlights Barium titanate has toxic effects on A.flos‐aquaeand E.gracilis. Barium titanate particles affected cell growth and viability. Barium titanate particles increased SOD activity and decreased ATP levels and photosynthesis. Effects were more pronounced in Seine River water than in artificial growth medium. Size does not seem to be an issue in BT particle toxicity.
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Figure1
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Figure11b