Open Access Article
Adriano A.
Torrano
ab,
Rudolf
Herrmann
c,
Claudia
Strobel
d,
Markus
Rennhak
c,
Hanna
Engelke
a,
Armin
Reller
e,
Ingrid
Hilger
d,
Achim
Wixforth
bc and
Christoph
Bräuchle
*ab
aDepartment of Chemistry and Center for NanoScience (CeNS), University of Munich (LMU), 81377 Munich, Germany. E-mail: christoph.braeuchle@cup.uni-muenchen.de
bNanosystems Initiative Munich (NIM), 80799 Munich, Germany
cExperimental Physics I, Institute of Physics, University of Augsburg, 86159 Augsburg, Germany
dDepartment of Experimental Radiology, Institute of Diagnostic and Interventional Radiology, Jena University Hospital – Friedrich Schiller University Jena, 07747 Jena, Germany
eResources Strategy, Institute of Physics, University of Augsburg, 86159 Augsburg, Germany
First published on 14th June 2016
In this work we investigate the interaction between endothelial cells and nanoparticles emitted by catalytic converters. Although catalyst-derived particles are recognized as growing burden added to environmental pollution, very little is known about their health impact. We use platinum-decorated ceria nanoparticles as model compounds for the actual emitted particles and focus on their fast uptake and association with mitochondria, the cell's powerhouse. Using live-cell imaging and electron microscopy we clearly show that 46 nm platinum-decorated ceria nanoparticles can rapidly penetrate cell membranes and reach the cytosol. Moreover, if suitably targeted, these particles are able to selectively attach to mitochondria. These results are complemented by cytotoxicity assays, thus providing insights into the biological effects of these particles on cells. Interestingly, no permanent membrane disruption or any other significant adverse effects on cells were observed. The unusual uptake behavior observed for 46 nm nanoparticles was not observed for equivalent but larger 143 nm and 285 nm platinum-decorated particles. Our results demonstrate a remarkable particle size effect in which particles smaller than ∼50–100 nm escape the usual endocytic pathway and translocate directly into the cytosol, while particles larger than ∼150 nm are internalized by conventional endocytosis. Since the small particles are able to bypass endocytosis they could be explored as drug and gene delivery vehicles. Platinum-decorated nanoparticles are therefore highly interesting in the fields of nanotoxicology and nanomedicine.
In order to mitigate the emission of particles and other dangerous substances from the engine, modern vehicles are equipped with catalytic converters. Automobile catalytic converters are able to transform more than 90% of total unburned hydrocarbons, carbon monoxide, and nitrogen oxides into rather harmless compounds, such as carbon dioxide, nitrogen and water. On the whole, they consist of a porous carrier material (e.g. CeO2, or ceria) that is decorated with active noble metals (normally platinum, but also palladium and rhodium). Although playing a fundamental role in reducing the emission of pollutants from vehicles, catalytic converters decompose with time and generate new particle emissions in the nano- and micrometer ranges. Catalyst-derived particles consisting of a carrier material and decorated with noble metals are thus formed and released into the environment.10–17 As a result of the escalating traffic worldwide, the concentration of noble metals (free or bound to the carrier material) has been increasing in urban areas. Wichmann et al.17 reported that the concentration of catalyst-derived platinum in the air of Braunschweig City (Germany) jumped from 6.0 pg m−3 in 1999 to 159 pg m−3 in 2005. Nanoparticles (NPs) generated by catalytic converters are therefore a growing burden added to particle pollution.
Since very little is known about the health impact of catalyst-derived NPs, our goal in this work is to investigate the biological effect of these NPs at the cellular level. Studying the interaction of catalyst-derived NPs with biological systems directly is hardly possible due to the low concentrations in samples like road dust. For this purpose, reasonable quantities of model compounds that resemble the actual catalyst-derived NPs were synthesized.18 Our mimetic compounds consist of a ceria NP core (defined sizes between 8 and 285 nm) decorated with ultrasmall platinum NPs (2–5 nm). The interaction between platinum-decorated ceria nanoparticles (Pt-ceria NPs) and human microvascular endothelial cells (HMEC-1) was studied in detail by live-cell imaging. Inhalation, skin contact, and ingestion are the main routes for NPs to enter the human body.19 In all three cases NPs can reach the bloodstream, where they can interact with endothelial cells covering the inner surface of blood vessels.20,21 These cells play a crucial role in the process of blood flow, while changes in endothelium are often found in a number of diseases.22–25 Therefore, endothelial cell lines represent an important model system to investigate the bioactivity and cellular uptake of NPs. In addition, we investigated if the same uptake behavior would be found in other cell types, such as human cervical cancer cells (HeLa). Surprisingly, Pt-ceria NPs of specific characteristics were rapidly found inside living cells and selectively associated with mitochondria. These exciting findings focused our investigations on the biological effects related to the unusual fast NP uptake mechanism as well as the mitochondrial-targeting properties of the model compounds.
Several mechanisms for the cellular uptake via endocytosis have been discussed in the literature. The most relevant and better understood mechanisms are clathrin-mediated endocytosis, caveolin-mediated endocytosis, macropinocytosis, and phagocytosis.26–28 Interestingly, cell-penetrating peptides,29 CdSe/ZnS core/shell quantum dots (8 nm, coated with D-penicillamine),30 and ultrasmall noble metal NPs (typically smaller than ∼10 nm), such as gold,31–35 and platinum,36,37 can escape the traditional endocytosis pathway and perform a fast direct translocation across the cell membrane into the cytosol. This unconventional uptake mechanism is characterized by fast and efficient cellular uptake, no perceptible cell membrane disruption and low cytotoxic effects.31 Although often reported, the mechanism of cell membrane penetration is not fully understood. Using coarse-grained molecular dynamics simulations, Lin and Alexander-Katz31 proposed that cell membranes generate nanoscale transient holes to assist the fast and spontaneous translocation of cell-penetrating peptides as well as ultrasmall cationic NPs into the cytoplasm. According to this model, when ultrasmall cationic NPs (e.g. 2.2 nm gold particles) approach the membrane, they are attracted to negatively charged membrane proteins. Once a certain number of NPs are located in the membrane region, nanoscale holes are formed due to the alteration of the local electric field across the plasma membrane. NPs that are already in the region will then use these holes to directly translocate into the cytosol. After translocation, the transmembrane potential is strongly reduced and the membrane rapidly reseals itself. In this context, delivery of payloads by NPs that are able to rapidly enter cells and accumulate in organelles has great potential to advance the treatment of many disorders. The interaction of Pt-ceria NPs with cells is therefore highly interesting with respect to the two complementary fields of nanotoxicology and nanomedicine. On the one hand, it plays an important role in the toxicology of nanomaterials and particle pollution; on the other hand, it can help to deliver therapeutics directly to mitochondria in the field of drug delivery and nanomedicine.
The size and shape of the model compounds synthesized for our investigations were characterized by transmission electron microscopy (TEM) measurements. Fig. 1 shows the TEM images of 8 nm ceria NPs decorated with platinum and labeled with Atto 647N (Pt-Ceria-8-atto). The primary particle size was determined by image analysis of TEM micrographs. In addition, energy-dispersive X-ray (EDX) spectroscopy (Fig. 1C) was used to prove the elemental composition of the model particles, with platinum (in blue) deposited on ceria NP cores (cerium in red).
Airborne NPs, like those released by automobile catalytic converters, tend to form aggregates in the nano- and micrometer ranges. A comparable tendency towards aggregation was observed during the synthesis of our model compounds. Large and irregular aggregates of Pt-Ceria-8-atto NPs of different sizes and shapes can be easily identified in Fig. 1.
The aggregation of particles was further characterized by dynamic light scattering (DLS) measurements of NPs dispersed in ethanol, the solvent in which particles were synthesized, as well as in cell medium supplemented with 10% FBS (fetal bovine serum). DLS measurements of the Pt-Ceria-8-atto NPs revealed a mean hydrodynamic diameter of 129 nm in ethanol and 246 nm in cell medium, with relatively broad size distributions (PDIs = 0.121 and 0.258, respectively). Analogous model compounds of 8 nm Pt-ceria NPs were prepared and labeled with a perylenediimide-derived dye with a triethoxysilyl anchor group (sample Pt-Ceria-8-pery).18 The mean hydrodynamic size of the Pt-Ceria-8-pery NPs was determined to be 154 nm (PDI = 0.116) in ethanol and 229 nm in cell medium (PDI = 0.506). The results are summarized in Table 1.
| Particle | Fluorescent dye | Primary particle sizea [nm] | Aggregate sizea [nm] | Hydrodynamic sizeb [nm] | PDIe | Zeta potential [mV] | |||
|---|---|---|---|---|---|---|---|---|---|
| EtOHc | Cell mediumd | EtOHc | Cell mediumd | EtOHc | Cell mediumd | ||||
| a Particle diameter measured by transmission electron microscopy (TEM). b Mean hydrodynamic diameter determined by dynamic light scattering (DLS) measurements. c Particle dispersion in ethanol. d Particle dispersion incubated for 30–40 min in cell medium supplemented with 10% FBS. e Polydispersity index (PDI) is a width parameter describing the hydrodynamic particle size distribution. Shortly, PDI <0.1 indicates monodisperse samples with narrow size distributions, PDI between 0.1 and 0.5 characterizes a relatively broad size distribution, and PDI >0.5 points to polydisperse samples with broad size distributions. f Not determined. | |||||||||
| Pt-Ceria-8-atto | Atto 647N | 8 | n.d.f | 129 | 246 | 0.121 | 0.258 | +35.1 | −7.6 |
| Pt-Ceria-8-pery | Perylenediimide | 8 | n.d.f | 154 | 229 | 0.116 | 0.506 | +27.1 | −10.8 |
| Ceria-47-atto | Atto 647N | 8 | 47 | 110 | 158 | 0.096 | 0.486 | +36.4 | −6.5 |
| Pt-Ceria-46-atto | Atto 647N | 8 | 46 | 103 | 135 | 0.157 | 0.372 | +45.9 | −7.4 |
| Pt-Ceria-143-atto | Atto 647N | 8 | 143 | 167 | 173 | 0.020 | 0.340 | +35.3 | −10.0 |
| Pt-Ceria-285-atto | Atto 647N | 8 | 285 | 292 | 428 | 0.060 | 0.172 | +49.2 | −10.6 |
On the one hand, it is desirable to investigate the interaction of model compounds that closely resemble not only the composition but also the aggregation behavior of actual catalyst-derived NPs. On the other hand, it is of paramount importance to find out whether model compounds of different sizes would have distinct biological effects. Ideal samples to investigate particle-size dependent cellular responses should thus have very narrow size distributions. To accomplish this task we developed a strategy to synthesize Pt-ceria NP samples with reasonable monodisperse size distributions (i.e. PDI <0.1). The method is based on using polyvinylpyrrolidone (PVP), a surface-active reagent, to obtain the aggregation control of 8 nm ceria NPs during the synthesis.18 This means that NP aggregation is not avoided, but rather controlled. Fig. 2 shows representative TEM images of stable, uniform and almost spherical aggregates achieved by using this strategy. Ceria NPs of 8 nm are the building blocks to form new NPs of 47 nm (Ceria-47-atto, Fig. 2A). Nearly spherical ceria NP aggregates are the ideal starting material for mimetic catalyst-derived NPs of defined core sizes and decorated with platinum. By using this procedure, Pt-decorated ceria NPs of three different core sizes were produced: 46 nm (Pt-Ceria-46-atto), 143 nm (Pt-Ceria-143-atto), and 285 nm (Pt-Ceria-285-atto). The TEM images of these particles are shown in Fig. 2B–D, respectively.
DLS measurements revealed the hydrodynamic diameter and the PDI values of the new samples. The results presented in Table 1 show that reasonable narrow size distributions were achieved. Ceria-47-atto and Pt-Ceria-46-atto, the smaller model compounds, still presented a tendency to increase their sizes by clustering with neighboring aggregates in a process that can be termed super-aggregation (Fig. 2A and B). This is directly reflected by the mean hydrodynamic sizes/PDI of these samples dispersed in ethanol: 110 nm/0.096 for Ceria-47-atto NPs and 103 nm/0.157 for Pt-Ceria-46-atto NPs. Even more satisfactory results were obtained with the larger model compounds Pt-Ceria-143-atto and Pt-Ceria-285-atto. Very small PDI values were achieved and the mean hydrodynamic sizes were just slightly larger than those measured by TEM (as expected, due to hydration and solvation effects). The mean hydrodynamic sizes/PDI in ethanol were determined to be 167 nm/0.020 for Pt-Ceria-143-atto NPs and 292 nm/0.060 for Pt-Ceria-285-atto NPs.
The transfer of ceria and Pt-ceria NPs from ethanol into cell medium, while avoiding the formation of large aggregates and super-aggregates, was a considerable challenge. In many cases, the traditional method to redisperse NPs (centrifugation followed by washing steps and a final redispersion in water) failed completely. Using this procedure, aggregates in the micrometer range were often formed and could not be broken down again to the original particle sizes. Importantly, in such cases cell membrane penetration by aggregated Pt-ceria NPs was not detected. In fact, this was the first hint that led us to explore the strong particle size-dependent effect in the uptake behavior of Pt-ceria NPs. After innumerous trials with different conditions and methods, an efficient and yet simple procedure was designed. Shortly, a small aliquot of well-dispersed NPs in ethanol is added into a microreaction tube; ethanol is left to evaporate; dried NPs are then redispersed directly in cell medium (see details in section 3.2). The final NP dispersion in cell medium, prepared as just described, maintained the particles closer to their original sizes. Importantly, NPs smaller than ∼50–100 nm were still present after redispersion, as indicated overall by the remarkable and consistent particle-size dependent uptake behavior of Pt-ceria NPs.
The surface charge, or zeta potential, of all samples dispersed in either ethanol (after synthesis) or in cell medium supplemented with 10% FBS was determined based on electrophoretic mobility measurements (Table 1). Positive surface charges with comparable magnitudes were measured in all samples dispersed in ethanol, with values ranging from +27.1 mV for Pt-Ceria-8-pery NPs to +49.2 mV for Pt-Ceria-285-atto NPs. The zeta potential values of all samples dispersed in cell medium were also found to be similar to each other, with negative values ranging from −10.8 mV for Pt-Ceria-8-pery to −6.5 eV for Ceria-47-atto. These results indicate that zeta potential values were not considerably altered by labeling, platinum decoration, or differences in the primary particle size. Therefore, all samples used in this study have a comparable net surface charge that, as expected, will mainly depend on the dispersion medium.
The very first uptake experiments in which HMEC-1 cells were incubated with Pt-Ceria-8-atto NPs revealed remarkable results: NPs were rapidly internalized by cells and were found selectively attached to mitochondria. As depicted in Fig. 3A, a substantial amount of Pt-Ceria-8-atto NPs is found associated with mitochondria after just 10 min of incubation time. Determination of Manders’ overlap coefficient38 revealed that as much as 91% of NPs overlap the mitochondria. Time-lapse confocal live-cell studies confirmed the association of NPs with mitochondria. In Fig. 3B, the typical dynamics of mitochondria inside cells can be appreciated. The translational motion and the bending of mitochondria are exactly followed by associated NPs, resulting in a perfect colocalization in space and time (see movie available as ESI “movie_mt-NPs”†).
![]() | ||
| Fig. 3 Live-cell imaging studies on the cellular uptake behavior of Pt-Ceria-8-atto NPs during a short interaction time. (A) Bright-field (left panel) and confocal images of a representative HMEC-1 cell (dashed line) incubated with Pt-Ceria-8-atto NPs for 10 min. After this short period, a considerable number of NPs (middle left panel, magenta) were internalized and accumulated in mitochondria (middle right panel, green: MitoTracker). Note the high degree of colocalization (Manders’ overlap coefficient of 91%) in the merge image (right panel, white). Inset: boxed regions of confocal images in detail. Remarkably, the mitochondrial network and the distribution of Pt-Ceria-8-atto NPs are characterized by overlapping filament-like structures. Scale bar = 10 μm. (B) Confocal image of another representative HMEC-1 cell with Pt-Ceria-8-atto NPs (magenta) associated with mitochondria (green; colocalizing pixels in white). Inset: time-lapse images of the boxed region. Note that the typical mitochondrial dynamics (e.g. translational motion, bending, stretching) is perfectly followed by associated NPs with a complete colocalization in space and time (see the ESI “movie_mt-NPs”†). Scale bar = 5 μm. Altogether, these results point to a very fast cellular uptake mechanism of Pt-Ceria-8-atto NPs, followed by a selective NP attachment to mitochondria. | ||
Interestingly, traditional endocytosis does not seem to be the uptake pathway taken by Pt-Ceria-8-atto NPs after short incubation times. In the live-cell imaging study presented in Fig. 4A, the cell plasma membrane was stained just before the addition of NPs. Thus, new endosomes formed from the cell surface (possibly enclosing NPs) were fluorescently marked. Our results consistently showed no endosomal localization of Pt-Ceria-8-atto NPs (here, only 1% of the NP signal overlaps endosomes). The particles were instead distributed along with the filament-like structures of the mitochondrial network, as elucidated in Fig. 3. After relatively long incubation times, however, the results were different. The peculiar uptake behavior of the Pt-Ceria-8-atto NPs after 18 h of incubation time is shown in Fig. 4B. Pt-ceria NPs do not only accumulate in mitochondria but also in lysosomes, the terminal vesicles that receive the cargo from endosomes.39 On the whole, a mixed uptake pathway was observed. Our findings points to the presence of two populations of particles in the sample: one population that escapes the endocytic pathway, is rapidly internalized, and accumulates in mitochondria; and another population that follows traditional endocytosis, is less efficiently internalized, and is delivered to lysosomes. Further research has demonstrated that particle size is a crucial factor determining the uptake mechanism of Pt-ceria NPs (see below).
In order to investigate if the mitochondrial-targeting properties observed for Pt-Ceria-8-atto NPs are an intrinsic ability of Pt-ceria NPs, regardless of the attached fluorophores, we prepared 8 nm Pt-ceria NPs labeled with perylenediimide (Pt-Ceria-8-pery), a neutral and chemically quite inert fluorescent dye.18 Missing the mitochondrial-targeting moieties, perylenediimide-labeled NPs would still be able to perform rapid cell membrane penetration, but would not accumulate selectively in mitochondria. Our hypothesis was confirmed by live-cell confocal studies. HMEC-1 cells were incubated with cell culture medium containing 50 μg mL−1 of either Pt-Ceria-8-atto or Pt-Ceria-8-pery NPs for 2 h. Cells exposed to 50 μg mL−1 of Pt-Ceria-8-pery NPs presented a blurry cytosolic distribution of NPs. In order to enhance the effect and optimize the visualization, the concentration of the Pt-Ceria-8-pery NPs was increased to 500 μg mL−1. As depicted in Fig. 5, both Pt-Ceria-8-atto and Pt-Ceria-8-pery NPs were internalized by cells, but while Atto 647N-labeled particles are mostly accumulated in mitochondria, perylenediimide-labeled particles are clearly distributed throughout the cytosol. The fraction of Pt-Ceria-8-atto NPs overlapping mitochondria for the upper cell in Fig. 5A is 86%. In contrast, the fraction of the Pt-Ceria-8-pery NPs overlapping mitochondria for the cell on the right in Fig. 5B is 46%. Nevertheless, since perylenediimide-labeled NPs cover the entire cytosolic region, 46% may be an overestimation caused by the diffraction-limited signal of NPs that are not physically associated with mitochondria, but rather diffusely surrounding them. The Atto 647N dye has therefore two functions in our model NPs: labeling and mitochondrial targeting.
This comparison study indicates that only with the assistance of a mitochondrial-targeting moiety (here, Atto 647N) the selective mitochondrial localization of cytosolic NPs is promoted. Since fluorescence microscopy relies on the use of fluorophores to label the objects of interest, eventual dye leakage or dye transfer to other objects may lead to misleading interpretations. It is therefore worth emphasizing why the findings presented in this work cannot be attributed to dye leakage from NPs. First of all, perylenediimide and Atto 647N are covalently bonded to the particle surface.18 Second, we simulated the leakage of the Atto 647N dye from NPs in the cell medium under comparable live-cell imaging conditions. The outcomes were that free Atto 647N molecules are not able to efficiently cross the plasma membrane of cells, and no accumulation of the Atto 647N dye in the mitochondria was observed (Fig. S1†). Finally, equivalent NPs lacking the decoration with platinum or larger than ∼150 nm do not display any mitochondrial localization, although labeled with Atto 647N (see below).
HMEC-1 cells were incubated with cell media containing 20 μg mL−1 of either Ceria-47-atto or Pt-Ceria-46-atto NPs, washed and imaged afterwards. The results presented in Fig. 6 show the effect of ultrasmall platinum NPs (2–5 nm) on the surface of ceria NPs. While Pt-Ceria-46-atto NPs are mostly found distributed as filament-like structures that coincide with the mitochondrial network (Fig. 6A), internalized Ceria-47-atto NPs appear as punctate fluorescence patterns that characterize the endocytosis uptake route (Fig. 6B). The same peculiar uptake behavior of Pt-Ceria-8-atto NPs after long incubation times (Fig. 4B) was observed for Pt-Ceria-46-atto NPs. Importantly, after very short incubation periods such as 20 min, Pt-Ceria-46-atto NPs were already detected in mitochondria, but Ceria-47-atto NPs were not even detected inside the cell (data not shown). It was necessary to perform longer incubation time experiments, such as 8 h, to detect reasonable amounts of intracellular Ceria-47-atto NPs. In the present case, 83% of mitochondria are overlapped by Pt-Ceria-46-atto NPs (Fig. 6A). In contrast, only 4% of mitochondria are overlapped by Ceria-47-atto NPs (Fig. 6B). In fact, a similar result (3%) was measured for the signal of lysosomes overlapping mitochondria in Fig. 4B. Such small values for the degree of colocalization (Manders’ overlap coefficient) can therefore be attributed to the proximity between vesicles and mitochondria in the cytoplasm.
Hence, platinum decoration has an enormous influence on the cellular uptake behavior of our model compounds for catalyst-derived NPs. The presence of ultrasmall platinum NPs on the surface of ceria NPs is a necessary condition for the unusual uptake mechanism under investigation.
Cellular uptake experiments parallel to those presented in Fig. 6 were performed. The peculiar uptake behavior of the 46 nm Pt-ceria NPs is depicted in Fig. 6A. Crucially, the same trend in the uptake mechanism was not observed for larger Pt-ceria NPs. The results in Fig. 7 show that, although decorated with platinum and labeled with Atto 647N, both Pt-Ceria-143-atto and Pt-Ceria-285-atto NPs fail to associate with mitochondria. Moreover, after short incubation times, such as 20 min, no evidence of NP internalization was found (data not shown). Intracellular NPs were only detected after longer incubation times. After 8 h, a punctuate pattern of internalized Pt-Ceria-143-atto and Pt-Ceria-285-atto NPs can be visualized (Fig. 7A and B). As described previously, such a NP pattern distribution is characteristic of particle endocytosis. The fraction of mitochondria overlapped by Pt-Ceria-143-atto and Pt-Ceria-285-atto NPs was negligible (2% and 6%, respectively), and it can be attributed to the signal overlapping of NPs inside endocytic vesicles and neighboring mitochondria.
Taken together, the unusual uptake behavior observed for 46 nm Pt-ceria NPs was not observed for 143 and 285 nm Pt-ceria NPs after short or long incubation times. These results point to a remarkable particle size effect: Pt-ceria NPs smaller than ∼50–100 nm escape the usual endocytic pathway and are transported directly to the cytosol by a fast uptake process; Pt-ceria NPs larger than ∼150 nm, by contrast, are taken up via the conventional endocytosis route.
In order to study the role of clathrin- and caveolin-dependent endocytosis in the uptake of small Pt-ceria NPs, we performed live-cell imaging in the presence of specific inhibitors. First, the clathrin-mediated pathway of HMEC-1 cells was completely inhibited with 15 μg mL−1 chlorpromazine (CP) incubated for 30 min and, after that, co-incubated transferrin was no longer internalized. In a parallel experiment, cells with the clathrin-mediated pathway completely blocked by CP were co-incubated with Pt-Ceria-46-atto NPs (100 μg mL−1). A considerable amount of NPs was detected inside the cell after a short incubation time of 20 min (Fig. S2†). Once inside the cells, Pt-ceria NPs associated with mitochondria. These results indicate that the clathrin-mediated endocytosis is not involved in this uptake process. Next, we investigate the influence of caveolin-mediated endocytosis. Caveolae vesicle formation depends on the integrity of the actin network in the cell.46 It means that actin disruption inhibits caveolin-mediated endocytosis (as well as macropinocytosis and phagocytosis).27,47–49 For caveolin-mediated endocytosis inhibition studies, cells were incubated with cytochalasin D (CyD), a fungal toxin that promotes actin depolymerization.49 CyD (5 μg mL−1) was added to HMEC-1 cells 15 min prior to addition of Pt-ceria NPs and was present in all biological media used throughout the experiments. Inhibition of caveolin-mediated mechanism was confirmed by confocal imaging showing no internalization of sphingolipid lactosylceramide molecules (LacCer). Finally, cells with the caveolin-mediated pathway inhibited by CyD were co-incubated with Pt-Ceria-46-atto NPs (100 μg mL−1). The results presented in Fig. S3† demonstrate that NPs were able to enter the cell and reach mitochondria within short incubation times, such as 20 min. These results indicate that the caveolin-mediated endocytosis as well as other actin-dependent mechanisms are not involved in the uptake process of small Pt-ceria NPs.
It is reported in the literature that cell membrane penetration by ultrasmall NPs (e.g. 6–10 nm) is an energy-independent process. Therefore, NP internalization occurs not only at 37 °C, but also with cells maintained at 4 °C.32,50 However, these studies also show that the amount of internalized NPs is typically drastically reduced at 4 °C. The reduced number of internalized NPs is probably influenced by changes in the mechanical properties of lipid bilayers at low temperatures.51,52 To investigate the uptake behavior of small Pt-ceria NPs at 4 °C we incubated HMEC-1 cells with Pt-Ceria-46-atto (100 μg mL−1) on ice for 30 min. In our results, no internalization of Pt-ceria NPs at 4 °C was detected (data not shown). Yet, upon warming of cells back to 37 °C, fast internalization of NPs occurred. The observed inhibition of Pt-ceria NP uptake at 4 °C may have been influenced by the core sizes of our particles (see Table 1), which are significantly larger than the abovementioned ultrasmall NPs. We hypothesize that Pt-ceria NPs are not able to translocate membranes at 4 °C due to changes in the elastic properties of cell membranes at low temperatures.
First, we tested if the direct translocation of Pt-ceria NPs through the membrane was accompanied by the leakage in (or penetration) of co-incubated calcein. The fluorescent dye calcein cannot penetrate an intact cell membrane directly, but is normally internalized by endocytosis and remains enclosed by intracellular vesicles. However, if the membrane is disrupted, calcein can penetrate the cell and a diffuse pattern is observed throughout the cytosol. Scoring the percentage of cells without the cytosolic calcein distribution is a convenient way to access the viability of cells after exposure to external agents. Cell membrane damage caused by external agents is typically characterized by the majority of cells exhibiting cytosolic calcein. For example, Verma et al.32 showed that cationic gold NPs (coated with 11-mercaptoundecane-tetramethylammonium chloride) which are able to disrupt membranes, led to cytosolic calcein distribution in ∼50% of the dendritic cells, while in the control samples not treated with gold NPs, 95% of the cells were found without calcein cytosolic distribution.
We co-incubated HMEC-1 cells with cell medium containing 0.1 mg mL−1 calcein and 100 μg mL−1 Pt-Ceria-46-atto NPs for 3 h. After this, cells were washed and imaged live. The percentage of cells without calcein distribution was above 97%. Besides, no significant difference in the viability of untreated and NP treated cells was found (Fig. S5†).
Next, we performed complementary studies on the particle-induced leakage out (or release) of previously internalized cytosolic calcein. The cell-permeant and nonfluorescent calcein-AM dye can access the cytosolic compartment of living cells and, once there, it is converted to the fluorescent calcein by intracellular esterases and remains trapped in the cytosol. In our experiments, HMEC-1 cells were preincubated with 5 μM calcein-AM for 45 min. Calcein-loaded cells were washed with cell medium and incubated with 100 μg mL−1 Pt-Ceria-46-atto NPs for 0.5 and 3 h. After the respective incubation periods, cells were washed again and imaged live. The mean fluorescence intensity of cytosolic calcein was measured in untreated cells and in cells treated with Pt-ceria NPs (Fig. S6†). The data show that no leakage out of pre-loaded cytosolic calcein was induced by the uptake of NPs. Moreover, no significant difference between untreated and NP treated cells was detected. These results are in line with the previous findings on the leakage in of calcein (Fig. S5†). Altogether, calcein leakage in and out assays offer supporting evidence that small Pt-ceria NPs can access the cytosol without causing noticeable membrane disruption.
So as to test the generality of our results, we prepared 8 nm ceria NPs decorated with other noble metals; namely, rhodium and palladium. In addition, we synthesized platinum-decorated 50–80 nm mesoporous silica NPs. Preliminary results indicate that in all cases the same trend, with cell membrane penetration and mitochondrial targeting by Atto 647N-labeled NPs was achieved (data not shown). Moreover, we investigated if the uptake trend observed for small Pt-ceria NPs is cell-type dependent. Human cervical cancer cells (HeLa) were incubated with Pt-Ceria-8-atto NPs, and the same unusual uptake behavior observed before was observed for HeLa cells (Fig. S7†).
In order to gain more information regarding the cell membrane penetration and mitochondrial association of Pt-ceria NPs we performed transmission electron microscopy (TEM) of cells. First, HeLa cells were incubated with non-labeled (Pt-Ceria-46) as well as Atto 647N-labeled particles (Pt-Ceria-46-atto) for 2 h. Subsequently, specimens were fixed, dehydrated, infiltrated, embedded, cured, cut in thin sections of 80–90 nm, mounted, stained, and finally examined by TEM (for details see section 3.4). Remarkably, the results presented in Fig. 9A are in line with the hypothesis of cell membrane penetration of small, individual Pt-ceria NPs as well as conventional endocytosis of particle aggregates. In addition, the micrograph shown in Fig. 9B suggests the accumulation of targeted NPs (Pt-Ceria-46-atto) on the outer membrane of mitochondria. Yet, the production of the TEM micrographs of cells relies on standard but quite elaborated fixation, staining, embedding and ultrathin sectioning protocols that may create artifacts. These TEM images should therefore be interpreted with care and regarded as an indication of the presence of Pt-ceria NPs in the respective cellular compartments, as thoroughly shown by the live-cell imaging results presented in this work.
On the basis of our findings and the literature, we propose the following uptake mechanism for small Pt-ceria NPs: as one NP diffuses and approaches a cell, the ultrasmall platinum NPs on its surface generate multiple transient nanoscale holes. These holes combine and allow the membrane penetration of the NP up to a core size of ∼50–100 nm. After the passage of the particle, the membrane rapidly reseals itself. Once inside the cells, the diffusing NP will come into contact with cell organelles and, in the case of Pt-ceria NPs labeled with Atto 647N, will attach to mitochondria owing to the lipophilic cationic moieties of this dye. Fig. 10 illustrates graphically the cell membrane penetration and mitochondrial targeting by a 50 nm Pt-ceria NP.
000 (Sigma-Aldrich), dissolved in a mixture of water and ethanol. The vial was tightly closed and stirred at an appropriate oil bath temperature for the time indicated. After cooling to room temperature the nanoparticles were isolated by centrifugation and washed with water (3 times, 2 mL) and ethanol (3 times, 2 mL) as described before. The amounts of the starting material and the reaction conditions are given in Table 2 (compare Table 1).
| Sample | Ce(NO3)3·6H2O [mg] | PVP [mg] | Ethanol [mL] | Water [mL] | Temperature [°C] | Time [h] |
|---|---|---|---|---|---|---|
| Ceria-47 | 56 | 216 | 1.5 | 0.5 | 140 | 6 |
| Ceria-143 | 108 | 56 | 1.5 | 0.5 | 130 | 20 |
| Ceria-285 | 108 | 56 | 0.67 | 1.34 | 140 | 13 |
:
1) showed complete conversion (NHS ester: retardation factor Rf 0.81, Atto 647N-APS: Rf 0.87). The solution was stored at 5 °C in the dark and used without further purification for nanoparticle labeling. To the nanoparticle dispersion (20 mg) in ethanol (1.5 mL) was added 100 μL of the Atto 647N-APS solution, or 50 μL of MPD-APS (15 μmol mL−1 in chloroform), respectively, and the mixture was stirred in a closed screw cap vial (Wheaton) for 5 h at 120 °C (oil bath temperature); for MPD-APS, 140 °C was applied. Stirring was continued for 20 h at room temperature. The labeled particles were isolated by centrifugation and purified by redispersion in ethanol and centrifugation (4 times, 2 mL) as described before. The particles were stored in ethanol in the dark.
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0, 15 min; then 2
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1, 1
:
1 and 0
:
1, 1 h each). Infiltration was performed under slight agitation (300 rpm, Thermomixer Comfort; Eppendorf). The membranes were transferred from the tubes (containing 100% embedding medium) to embedding molds (Plano GmbH, cat. no. G369N). Molds containing the membranes were filled with embedding medium and cured at 60 °C for 30 h. Afterwards, ultrathin sections of 80–90 nm thickness were cut using a ultramicrotome (Leica-Reichert Ultracut E), mounted onto copper grids (Formvar-carbon 300 mesh; Ted Pella, Inc.) and stained with uranyl acetate (8% for 10 min) and Reynold's lead citrate solution (2.2% for 3 min). Finally, specimen sections were examined on a transmission electron microscope (JEM 1011, JEOL).
The results presented in this work make distinguished contributions to the fields of nanotoxicology and nanomedicine. As regards nanotoxicology, although the uptake mechanism proposed involves the fast translocation of Pt-ceria NPs into the cytosol, our findings suggest that the short-term nanotoxicology of high doses of Pt-ceria NPs (within 72 h, 100 μg mL−1) is rather low. However, long-term effects of continuous exposure to much lower doses, as in human exposure to air pollution, remain to be investigated. With respect to nanomedicine, Pt-ceria NPs (and conceivably other noble-metal decorated NPs) are fascinating materials that can rapidly and efficiently enter cells and reach intracellular organelles, such as mitochondria. In this way they represent an interesting particle type with high potential to become important platforms for intracellular-targeted drug and gene delivery.
Footnote |
| † Electronic supplementary information (ESI) available: Further information on the characterization of nanoparticles and additional live-cell imaging studies. See DOI: 10.1039/c5nr08419a |
| This journal is © The Royal Society of Chemistry 2016 |