C.
Muoth
a,
M.
Rottmar
b,
A.
Schipanski
b,
C.
Gmuender
a,
K.
Maniura-Weber
b,
P.
Wick
a and
T.
Buerki-Thurnherr
*a
aParticles-Biology Interactions, Empa, Swiss Federal Laboratories for Materials Science and Technology, Lerchenfeldstrasse 5, 9014 St. Gallen, Switzerland. E-mail: tina.buerki@empa.ch
bBiointerfaces, Empa, Swiss Federal Laboratories for Materials Science and Technology, Lerchenfeldstrasse 5, 9014 St. Gallen, Switzerland
First published on 19th July 2016
To ensure the safe design and effective application of nanomedical therapies, it is of major importance to understand nanoparticle (NP) uptake mechanisms. Actin-dependent endocytosis has been proposed as a major uptake mechanism for numerous NPs in different cells. However, it is not clear which aspect of the structure and dynamics of the actin cytoskeleton is of relevance in this process. Despite the fact that the cytoskeletal organization is very much dependent on the cellular microenvironment, most mechanistic uptake studies have been performed under classic 2D cell culture conditions, which fail to represent the morphological and mechanical constraints present in biological tissues. In this study, human choriocarcinoma BeWo cells were physically constrained on micropatterns of different geometries to study the uptake of 80 nm, 240 nm and carboxylate 300 nm polystyrene particles and the dependence on different actin structures. Interestingly, major differences in the actin cytoskeletal organization of BeWo cells did not affect the intracellular distribution and amount of internalized polystyrene NPs for all investigated particle sizes and modifications. Therefore, we suggest a more central role for actin dynamics in actin-dependent NP endocytosis, rather than the overall actin organization.
The actin cytoskeleton plays a fundamental role in different cellular processes, including many types of endocytosis, such as phagocytosis, macropinocytosis, circular dorsal ruffles or clathrin-mediated endocytosis (CME).15,16 Actin assembly can create protrusions that engulf extracellular materials. Actin also supports the invagination of membrane segments into the cytoplasm, scission of new vesicles from the plasma membrane and intracellular movement of the vesicles. In CME in yeast, vesicle budding is completed by the formation of a tubular invagination that is driven by the attachment of filamentous actin (F-actin), which occurs concomitantly with nucleation of actin at the plasma membrane.17,18 Similar events have been shown for mammalian cells, where a close association between F-actin accumulation and vesicle formation was observed at a late stage of CME.19,20 In addition, there is also evidence that actin not only plays a mechanical role, but also a structural role in CME, where it guides the endocytic machinery to a specific site on the plasma membrane (reviewed in ref. 21). A central role for actin dynamics in NP uptake by different cell types has been proposed in several studies employing pharmacological inhibitors that affect actin reorganization and G/F-actin ratios, such as cytochalasin or latrunculin.22–25 Although there is some indication that actin-dependent internalization may be dependent on particle size and aspect ratio/geometry,26,27 the use of different cell types, pharmacological inhibitors or NP types makes it difficult to compare different studies and to obtain a clear mechanistic insight. As such, treatment of macrophages with cytochalasin B resulted in the reduced uptake of 1000 nm, but not that of 20 nm polystyrene (PS) NPs,25 while cytochalasin D treatment significantly diminished the internalization of small 20 nm silica NPs in A549 lung epithelial cells.24 In addition, the use of such pharmacological inhibitors has some drawbacks, including a low specificity and cytotoxicity at increased concentrations or prolonged exposure times. Furthermore, cytochalasin can also affect other biological processes unrelated to actin polymerization, such as protein synthesis28 or glucose transport.29 Besides actin dynamics, we hypothesize that the global organization of actin filaments, as well as their assembly into higher-order structures, such as contractile bundles or three-dimensional networks may be implicated in cellular NP uptake and subcellular localization.
The microcontact printing (μCP) technique presents an interesting approach to mechanically controlling the organization of the actin cytoskeleton and when creating defined patterns, a more tissue-like microenvironment can be mimicked.30 On substrates produced by μCP, single cells can be cultivated on cell-adhesive islands of defined geometry and size to manipulate and control the cell spreading area, shape, cytoskeletal organization and cell contractility, among other factors.31–34 It has been previously shown that geometric cues can guide the formation of actin stress fibers and lamellipodia.35 While cell adhesive areas with concave edges promote the formation of actin stress fibers,34 those with convex edges are strong cues for the formation of lamellipodia.36 Both actin stress fibers and lamellipodia have been shown to influence cell polarity.36,37 Micropatterns with increased substrate stiffness and shapes that promote high cytoskeletal tension enhanced the osteogenesis of mesenchymal stem cells,35,38,39 whereas unspread, round cells tend to express elevated markers of adipogenesis.35,39,40 Taken together, these reports demonstrate the potential of μCP to enable studies on basic cell responses to individual cues with shape-normalized single cells.
In this study, μCP was employed to investigate the influence of different actin cytoskeletal organizations on uptake and internalization of PS particles by BeWo cells. Therefore, BeWo cells were cultivated on four different pattern geometries, resulting in the same cell surface area but different shapes, which induced highly distinct organization of the actin cytoskeleton. Nontoxic, fluorescent and monodisperse PS particles were used as model particles for the uptake studies. BeWo cells were exposed to 80 nm, 240 nm and carboxylate 300 nm PS particles, followed by quantitative uptake analysis using confocal microscopy and a digital image analysis method. We achieved the successful normalization of BeWo cell shape and distinct actin filament arrangements, a prerequisite for subsequent studies on actin-dependent NP uptake. Intracellular distribution and the amount of internalized NPs by shape-normalized BeWo cells were independent of the cytoskeletal organization for all investigated sizes and modifications of PS particles. This model presents a novel approach to studying the role of actin structures in NP uptake, kinetics and intracellular fate over time, and its dependency on different NP properties and cell types. A detailed knowledge of these NP-cell interactions is crucial for the development of targeted drug delivery systems.
Plain | COOH | ||
---|---|---|---|
80 nm | 240 nm | 300 nm | |
a Abbreviations: DD double distilled; TEM transmission electron microscopy. b According to manufacturer's information. c Grafmueller et al.44 d Grafmueller et al.43 e Experimentally determined (mean ± SD). | |||
Diameter (nm) | 87b | 240 | 302.7d |
Diameter TEM (nm) | 78.1 ± 20.5c | 220.5 ± 5.1d | 289.4 ± 10.2d |
Hydrodynamic diameter (nm) in DD water | 97 ± 0.8c | 230 ± 65.3d | 283 ± 85.2d |
Hydrodynamic diameter (nm) in growth mediume | 162 ± 5.3 | 207 ± 10.9 | 312 ± 9.4 |
Initial no. of particles per mL in growth medium | 2.18 × 1012 | 1.70 × 109 | 7.50 × 108 |
Particle surface (nm2) per mL in growth medium | 1.31 × 1016 | 2.59 × 1014 | 1.97 × 1014 |
Zeta potential in 10 mM NaCl (mV) | −50 ± 9.7c | −20.5 ± 2.7d | −55.6 ± 6.1d |
Zeta potential in growth medium (mV)e | −10.9 ± 0.8 | −10.9 ± 0.6 | −9.3 ± 0.97 |
Fluorescent dyeb | Yellow green | Yellow | Yellow green |
Excitation/emissionb | 485/528 | 485/520 | 485/528 |
Manufacturer | Polyscience Inc | Spherotec Inc | Polyscience Inc |
TEM analysis was performed in a previous study and showed a primary particle size of 78.1 ± 20.5 nm for the plain 80 nm PS particles,44 220.5 ± 5.1 nm for the plain 240 nm PS particles43 and 289.4 ± 10.2 nm for the 300 nm COOH–PS particles.43 In suspension, hydrodynamic diameters of 80 nm, 240 nm and 300 nm COOH–PS particles increased to 97 ± 0.8 nm, 230 ± 65.3 nm and 283 ± 85.2 nm in water and to 162 ± 5.3 nm, 207 ± 10.9 nm and 312 ± 9.4 nm in growth medium, respectively (ESI Fig. 1†). The zeta potential was negative for all PS particles suspended in 10 mM sodium chloride, but for 80 nm and 300 nm COOH–PS particles, it was significantly lower than for 240 nm PS particles. Since 240 nm and 300 nm PS particles were similar in size but with different zeta potential, they were included to investigate whether NP surface charges affect their internalization by micropatterned cells.
When working with fluorescent NPs, a common problem is the release of labile dye in a biological milieu, as free fluorophores may significantly alter the in vitro and in vivo outcomes.45–48 Therefore, we assessed the stability of the fluorescent dye in growth medium at 37 °C over 72 h, and no decrease in fluorescence intensity or any leakage of free dye from the different PS particles used in this study were observed (ESI Fig. 2A and B†).
An important prerequisite to study the dependency of NP uptake on cytoskeletal organization is the absence of cytotoxic effects. Using the MTS assay, we confirmed that none of the PS particles decreased the viability of BeWo cells within 24 h of exposure (ESI Fig. 3A and B†).
In this study, BeWo cells were grown on adhesive micropatterns of different geometries (disc, H, crossbow (CB) and Y) (Fig. 1A) in order to achieve differences in cytoskeletal organization without changing the cell surface area. The optimal pattern size, which best supported the spreading of BeWo cells was 1600 μm2. On smaller micropatterns (1100 and 700 μm2), cells displayed a roundish morphology while on larger patterns (>2000 μm2), they were not able to span over the entire adhesive area (data not shown). Major differences in the actin cytoskeleton occurred between Y patterns with three non-adhesive areas, CB and H patterns with two non-adhesive areas and disc patterns lacking non-adhesive areas. On Y patterns, filamentous actin (F-actin) stress fibers were concentrated along the whole outline of the cell, whereas on CB and H patterns, they only formed along two borders of the cell. In contrast, BeWo cells spread on the disc patterns displayed a strong actin network in the center of the cell where the cytoskeleton spanned over the nucleus (Fig. 1B). Furthermore, the formation of lamellipodial extensions and filopodial protrusions were detectable on adhesive areas in BeWo cells grown on disc, H and CB patterns (Fig. 2). To confirm that the cytoskeletal organization was reproducible, actin heatmaps of 20 individual cells per pattern were made (Fig. 1C). Actin heatmaps showed a highly reproducible and distinct arrangement of the actin cytoskeleton within each pattern demonstrating the successful normalization of BeWo cells.
Heatmaps were made to show the average distribution of internalized PS particles. After an exposure time of 14 h, uptake was observed for all shape-normalized BeWo cells exposed either to 80 nm (Fig. 3D), 240 nm (Fig. 3E) or 300 nm COOH–PS particles (Fig. 3F). As expected, for single cell analysis,61 the amount of internalized NPs was highly variable between different cells, even if cultivated on the same pattern. Independent of the different pattern geometries, all NPs were located predominantly in the perinuclear region, probably in the form of NP-filled vesicles. Although it may appear from several individual images in Fig. 3 that actin is also very much localized around the nuclei, heatmaps from 20 individual cells clearly showed that a consistent perinuclear localization of actin is only true for cells spread on the disc patterns (Fig. 2). Therefore, perinuclear actin structures are most likely not responsible for the observed nuclear localization of the NPs. Most importantly, NP heatmaps did not show any obvious differences in the amount or intracellular distribution of internalized NPs, despite the presence of highly distinct actin organization on the four pattern geometries.
In addition to the qualitative observations, the quantity of internalized NPs was analyzed by applying a macro specifically designed to reliably measure NP uptake by single cells (“Particle_in_Cell-3D”61 for ImageJ). This macro requires the use of fluorescently labelled NPs, as well as a staining procedure to visualize the cell border or cell membrane. However, direct labelling of the cell membrane (e.g. with cell tracker dyes, DiI, DiO or DiD) led to the partial detachment of the cells from the patterns after fixation (data not shown). Therefore, labelling of the actin cytoskeleton was used as an indirect approach to identify the cell border. Integrated pixel intensities of internalized NPs were calculated for 20 cells per pattern geometry, using the same z-stack images as for the heatmaps (Fig. 4). Comparison of PS particle uptake by BeWo cells grown on disc, H, CB and Y patterns revealed no differences for either the 80 nm (Fig. 4A) or 240 nm PS particles (Fig. 4B). A slightly increased uptake was observed only for 300 nm COOH–PS particles by cells grown on Y patterns, compared to CB and H patterns (Fig. 4C), but this trend was not observed for 80 nm or 240 nm PS particles. As this increase was very modest and not consistent for all NP types, it is unlikely that cells with high levels of peripheral stress fibers incorporate more NPs than cells with a more central F-actin meshwork.
Our quantitative analysis indicates that actin cytoskeletal organization is not a key determinant of NP internalization. Specifically, PS NP uptake was independent of the presence of wide, peripheral stress fibers, filopodia or lamellipodial structures (Fig. 1C and 2). In addition, a more peripheral or central localization of most F-actin structures did not have any influence on the amount or intracellular distribution of PS NPs either (Fig. 1C). However, due to cell type-specific differences in NP uptake, it will be important to confirm these findings for other cell types. Moreover, it appears that cell contractility is not implicated in PS NP uptake, since previous work suggested that the level of contractile forces was altered in cells grown on different micropatterns.34,36 According to these studies, cell contractility in micropatterned BeWo cells is expected to be highest on Y patterns forming three convex edges, intermediate on CB and H patterns forming two convex edges and lowest on disc patterns forming no such edges. However, to unambiguously prove that NP internalization is independent of cell contractility, contractile forces of cells on different micropatterns have to be accurately determined by appropriate force measurement methods. Finally, we suggest that the dynamic reorganization of the actin filaments, which was not significantly affected in our μCP study, is of key relevance for the active endocytic NP uptake as observed in previous studies.22–25 This is supported by the fact that the presence of pharmacological inhibitors interfering with polymerization, depolymerization or rearrangement of the actin cytoskeleton resulted in the decreased uptake of several NPs.22–25
The current knowledge on NP uptake mechanisms by different cell types ranges from actin-dependent endocytosis to non-endocytic pathways with no clear correlation to the physico-chemical properties of the particles. For example, dos Santos et al. described an energy dependent uptake process for 40 nm and 200 nm COOH–PS NPs in HeLa and glial astrocytoma 1321N1 cells.22 In contrast, a nonendocytic uptake pathway was suggested for 78 nm and 200 nm PS NPs in pulmonary macrophages.62 A more recent study in primary macrophages and a monocytic cell line has identified endocytosis, macropinocytosis or phagocytosis as the involved uptake mechanisms for 100 nm COOH– and NH2–PS NPs.41 These contradictory results clearly demonstrate the need for more detailed studies on NP uptake mechanisms, including, but not limited to the role of endocytosis and the actin cytoskeleton.
As nanotechnology is becoming a vital player in medicine, with various biomedical applications, such as drug delivery, therapeutics, diagnosis or imaging, it is necessary to understand the mechanisms by which NPs are internalized by cells. A comprehensive knowledge of NP internalization pathways in relation to distinct physico-chemical NP properties may enable the development of novel strategies to enhance or reduce NP uptake at specific sites.
The zeta potential of the particles in growth medium was determined with a Zetasizer NanoZS (Malvern Instruments, Malvern, UK).
Particle size distribution in growth medium and double distilled (DD) water was determined by nanoparticle tracking analysis (Nanosight LM 20 System, Amesbury, UK). Prior to analysis, growth medium and DD water were filtered using a 0.02 μm Anotop® 25 syringe filter (Whatman GmbH, Dassel, Germany). Results were normalized to the area under the NP concentration/size curve.
The stability of the fluorescence was assessed by analyzing the loss of fluorescence after incubation of 25 μg mL−1 PS particles diluted in growth medium at 37 °C for 3, 6, 24, 48 and 72 h using a microplate reader (Biotek Synergy, Winooski, USA) with excitation and emission wavelengths of 485 nm and 528 nm. The loss of fluorescence was measured before and after filtration through a 0.1 μm syringe filter at the end of each incubation time.
Z-stack images were acquired with a 63× magnification oil immersion objective on a confocal laser scanning microscope (LSM 780, Zeiss, Feldbach, Switzerland) using the identical color intensity threshold for each type of NP. For each of the different experimental conditions 20 individual cells were imaged, which is a similar cell number to that used in other NP uptake studies.63–65 After image processing (ZEN 2011, Zeiss, Feldbach, Switzerland; Photoshop CS6), heatmaps were determined from the 20 overlaid z-stacks/pattern for each pattern geometry, in order to visualize the average distribution of actin and internalized PS particles. Quantification of internalized 80 nm, 240 nm and 300 nm COOH–PS particles by single cells was performed from heatmap z-stack images using the ImageJ macro “Particle_in_Cell-3D”.61 Briefly, images of the actin cytoskeleton were used to recalculate the cell volume in which the particles were quantified. The total fluorescence of the internalized NPs was digitally assessed by the sum of all NP pixel intensities within each cell volume, which is assumed to be proportional to the amount of uptaken NPs.
Footnote |
† Electronic supplementary information (ESI) available: Nanoparticle size distribution measurements, fluorescence intensity measurements, cell viability experiments. See DOI: 10.1039/c6ra13782b |
This journal is © The Royal Society of Chemistry 2016 |