Darkfield-Confocal Microscopy detection of nanoscale particle internalization by human lung cells
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Concerns over the health effects of nanomaterials in the environment have created a need for microscopy methods capable of examining the biological interactions of nanoparticles (NP). Unfortunately, NP are beyond the diffraction limit of resolution for conventional light microscopy (~200 nm). Fluorescence and electron microscopy techniques commonly used to examine NP interactions with biological substrates have drawbacks that limit their usefulness in toxicological investigation of NP. EM is labor intensive and slow, while fluorescence carries the risk of photobleaching the sample and has size resolution limits. In addition, many relevant particles lack intrinsic fluorescence and therefore can not be detected in this manner. To surmount these limitations, we evaluated the potential of a novel combination of darkfield and confocal laser scanning microscopy (DF-CLSM) for the efficient 3D detection of NP in human lung cells. The DF-CLSM approach utilizes the contrast enhancements of darkfield microscopy to detect objects below the diffraction limit of 200 nm based on their light scattering properties and interfaces it with the power of confocal microscopy to resolve objects in the z-plane.
Validation of the DF-CLSM method using fluorescent polystyrene beads demonstrated spatial colocalization of particle fluorescence (Confocal) and scattered transmitted light (Darkfield) along the X, Y, and Z axes. DF-CLSM imaging was able to detect and provide reasonable spatial locations of 27 nm TiO2 particles in relation to the stained nuclei of exposed BEAS 2B cells. Statistical analysis of particle proximity to cellular nuclei determined a significant difference between 5 min and 2 hr particle exposures suggesting a time-dependant internalization process.
DF-CLSM microscopy is an alternative to current conventional light and electron microscopy methods that does not rely on particle fluorescence or contrast in electron density. DF-CLSM is especially well suited to the task of establishing the spatial localization of nanoparticles within cells, a critical topic in nanotoxicology. This technique has advantages to 2D darkfield microscopy as it visualizes nanoparticles in 3D using confocal microscopy. Use of this technique should aid toxicological studies related to observation of NP interactions with biological endpoints at cellular and subcellular levels.
KeywordsConfocal Laser Scanning Microscope Numerical Aperture Chromatic Aberration High Numerical Aperture Darkfield Microscopy
The recent proliferation of nanotechnology combined with concerns over the health effects of human exposure to ambient ultrafine particulate matter (UFP) have created a need for information on the toxicology of nanomaterials. Studies to date have made it apparent that the effects of nanomaterials cannot be safely extrapolated from the toxicological properties of larger-scaled materials of the same composition [1, 2].
Nano-scaled materials are generally defined as structures possessing at least one dimension that is 100 nm or less [3, 4]. The small size and correspondingly large surface to mass ratio of nanomaterials are features which may alter their interactions with cells and tissues [5, 6]. Incidental human exposure to environmental nanomaterials most often occurs through the inhalation of ambient ultrafine particulate matter that is primarily produced during the combustion of fossil fuels . Conversely, nanomaterials that are intentionally engineered are more commonly known as nanoparticles. In this manuscript, the term nanoparticle (NP) will be used to refer to nano-scaled materials without regard to their origin and are considered to be under 100 nm in size.
Relative to ingestion and dermal absorption, inhalation of NP may be the most likely route of human exposure. The small size of NPs not only allows them to become airborne easily, but promotes deposition in the deep lung as well . Indeed, inhaled UFP have been reported to be more potent in inducing adverse health effects than larger particles [1, 3, 8, 9]. Some studies have suggested that inhaled NP penetrate the respiratory epithelial barrier and are distributed systemically to various organs and tissues, including the brain [1, 5, 10, 11, 12].
Imaging is a powerful technique for the study of cellular interactions with extracellular substrates, including particles [13, 14]. Many critically important toxicological processes, such as the mechanisms through which nanomaterials penetrate into cells, are best addressed using imaging approaches. However, with the exception of fluorescently tagged synthetic particles, the small size of nanoparticles puts them beyond the limit of detection of about 200 nm using conventional bright-field light microscopy techniques. As an alternative, application of electron microscopy (EM) in NP studies has grown considerably in the past few years and remains the "gold standard" for many NP studies as this technology can easily observe particles below 100 nm in size. Unfortunately, EM is costly, labor intensive, limited to materials with sufficient electron density contrast, and primarily restricted to fixed specimens.
Conventional darkfield (DF) microscopy is an illumination technique used in light microscopy to optimize differences in contrast by selectively capturing light scattered by the specimen. In brief, this is accomplished with the attachment of a specialized light condenser that uses a light stop comprised of an annulus with a narrow aperture to obliquely illuminate the specimen via a hollow cone of light [15, 16, 17]. Using a confocal microscope, the light illuminating the specimen is focused by the objective, and collected by a darkfield condenser. Essentially, these instruments use a reverse light path from normal DF applications for DF detection in confocal mode. Consistent with normal DF illumination, the blockage of centralized light in DF-CLSM reveals only structures of the specimen that are capable of scattering light. DF detects light that is refracted, diffracted or reflected. This light scattering allows DF to detect extremely small structures, offering a potential light microscopy tool for the study of nanoparticles associated with cells. If a DF oil condenser with a 1.2-1.4 numerical aperture is used, it allows lenses with a higher numerical aperture to also be used which diminishes resolution losses in the microscope. However, the numerical aperture of the lens must be slightly below that of the numerical aperture of the condenser for DF to work. Previous studies have used DF imaging to observe NP [18, 19, 20, 21, 22, 23]. Largely, these studies have been limited by visualizing NP in only a single 2D plane instead of producing a 3D image as presented in this communication.
In the present study, we show that the capability of DF to detect nanoparticles that can be effectively interfaced with a confocal laser scanning microscope (CLSM) to spatially localize nanoparticles along the z-axis of the cell, thereby permitting a determination as to whether nanoparticles are associated with the cell surface or within the cell. This communication reports the novel integration of DF and CLSM microscopy and its utilization in the measurement of nano-particle uptake and localization relative to intracellular organelles and the nucleus in cultured human lung cells.
Materials and Reagents
Green fluorescent 6.5 μm, 2.0 μm, 0.5 μm, 140 nm, 100 nm, and 50 nm polystyrene spheres (beads) were acquired from Polysciences Inc. (Warrington, PA) and Bangs Laboratories Inc. (Fishers, IN). Titanium dioxide nanoparticles with an average diameter of 27 nm were obtained from Degussa (Aeroxide TiO2, Parsippany, NJ). HCS Cell Mask Blue (H32720) and Prolong Gold Antifade Reagent with and without DAPI (P36934 and P36935) were purchased from Invitrogen (Molecular Probes, Eugene, OR). First Contact cleaning polymer was obtained from Photonic Cleaning Technologies (Platteville, WI).
A slide cleaning protocol was devised to minimize the presence of unwanted background debris detectable by darkfield microscopy [24, 25]. New "pre-cleaned" microscope slides (Fisher Scientific, Pittsburgh, PA) were subjected to additional cleaning by wiping them using ammonia based glass cleaner and lens paper. As the slides were wiped, they were placed into a slide rack taking care to provide even spacing between each slide. Next, the slide rack was placed into a lidded vessel large enough to fully submerge the slides and washed successively in the following solutions: 1) 1:5 dilution of ammonia based glass cleaner in deionized water (dH20), 2) deionized water, and 3) 70% ethanol. Importantly, for each wash step, the lidded vessel containing the slides was placed in a bath sonicator and the entire apparatus was sonicated for 30 minutes in each wash solution. Washed slides were stored in 70% ethanol until needed. Just prior to coverslip mounting, a slide was removed from the 70% ethanol, briefly rinsed in 100% ethanol and allowed to air dry for approximately five minutes. Lastly, to further aid in the removal of slide debris, the specimen area of the slide was painted with a commercially available cleaning polymer (First Contact), allowed to cure for a minimum of 15 minutes, and peeled off immediately before mounting coverslips. All reagents used to wash slides were filtered using 0.22 μm filters. All steps in which the slides were exposed to air (i.e. removal from the various wash solutions) were carried out in a biological hood to minimize contamination with airborne debris. Use of this slide cleaning procedure produced slides that were relatively free of debris detectable by DF-CLSM.
Fluorescent Polystyrene Beads
Suspensions of 50 nm, 100 nm, 140 nm, 500 nm, 2 μm and 6.5 μm Fluorescent polystyrene beads (Polysciences, Warrington, PA) were prepared in dH2O and directly applied to freshly cleaned glass slides. Following a drying time of 15 to 20 minutes, #1.5 coverslips were mounted onto the slides using Prolong Gold Antifade Reagent.
Cell Culture and Exposure
Transformed human airway epithelial cells (BEAS-2B, subclone S6;  were cultured as described previously  and maintained in serum-free KGM (Lonza, Walkersville, MD). The cells were incubated in a humidified incubator at 37°C in 5% CO2. For fixed cell studies, cells were sparsely plated (≤ 1.5 × 106 cells/well) on 12 mm, #1.5 coverslips located in 6-well culture dishes and allowed to grow for one day prior to exposure. At the time of exposure, media was removed from the cell cultures and 2 ml of a freshly prepared homogeneous suspension of 27 nm TiO2 was applied immediately. Cells were typically exposed for either 5 minutes or 2 hours (120 minutes) prior to washing and fixation. Pulsed exposures involved continuous exposure for 5 minutes followed by removal of exposure media, a brief wash using KGM, and incubation in fresh, particle free, media for an additional 115 min. After exposure, cells were washed twice in 1X Dulbecco's Phosphate Buffered Saline (PBS, Gibco, Grand Island, NY) and then fixed in 4% paraformaldehyde (PF) made up in PBS and stained.
Titanium dioxide Preparation
For each cell exposure experiment, a fresh stock solution of 27 nm TiO2 was prepared by resuspending 1 mg of dry particles in 1 ml of sterile dH2O. This solution was then sonicated for 30 seconds using a temperature-controlled cup-horn sonicator (Fisher Scientific, Pittsburgh, PA). The TiO2 particles were further diluted to their final concentration of 0.5 or 2.5 μg/ml using Keratinocyte Growth Medium (KGM). Just prior to cell exposure, these particle suspensions were sonicated again for 30 seconds and then immediately applied to 6-well dishes that contained 12 mm cover slips.
Cell Fixation, Staining, and Mounting
Following NP exposure, cells were thoroughly washed in PBS, and fixed for approximately 30-60 minutes using 1 ml of 4% paraformaldehyde per well. After fixation, cells were stained using HCS Cell Mask Blue (CMB) as a cytoplasmic stain or 4',6-diamidino-2-phenylindole (DAPI) for nuclear staining. Staining using CMB was done as an adaptation of the procedure provided by the manufacturer. Briefly, 1 ml of 0.1 μg/ml CMB in 1× PBS was added to each well and allowed to incubate overnight at room temperature. The next morning, cells were washed in 1× PBS followed by a final rinse in dH2O. Lastly, the coverslips from each well were mounted on newly cleaned slides using Prolong Gold Antifade Reagent. In experiments where DAPI staining was performed, cells were mounted using Prolong Gold Antifade Reagent with DAPI in lieu of overnight staining.
Confocal Microscopy Quality Assurance (QA)
The confocal microscope, lenses, and optical components utilized in this study were evaluated for QA using the procedures described by Zucker and Zucker et al. [28, 29, 30, 31, 32]. Briefly, colocalization was examined using PSF beads, and field illumination and laser powers were monitored. In the Nikon confocal system, laser fluorescence colocalization was present between the 488 and 561 lines, while the 404 showed a z axis spectral shift with the other 2 visible wavelengths (488 nm and 561 nm) and was not colocalized. This lack of colocalization of UV and visible laser light with the Nikon C1Si is quite typical of confocal microscopes from all manufacturers.
Simultaneous DF and CLSM
Imaging was carried out on two different configurations of confocal microscopes from Nikon and Leica. 1) A Nikon Eclipse C1si Spectral Confocal imaging system (Nikon Instruments Corporation, Melville, NY) equipped with an oil immersion Darkfield condenser (numerical aperture = 1.2 - 1.43) and 404 nm, 488 nm, 561 nm, and 633 nm lasers served as the primary means for experimental analysis. Specimens were observed via an Eclipse Ti microscope using either a 60X or 100X Plan Fluor oil immersion objective lens with adjustable iris permitting an numerical aperture ranging from 0.5 to 1.25. DF images were acquired via a transmission detector (TD). For fluorescence excitation, a conventional confocal optical path is maintained in which laser light originating from the objective lens is focused onto the specimen and then collected through the objective lens, Fluorescent light is then passed through an aperture (pinhole), and focused onto a detector consisting of a photomultiplier tube (PMT) tuned to detect specific wavelengths of light. Transmitted light detection of darkfield images begins with illumination by the same laser light originating from the objective lens. An occluding disc built into the darkfield condenser above the specimen blocks incoming light travelling on a direct path from the source but collects light scattered by the specimen and allows it to reach a transmission detector coupled to a PMT capable of monitoring multiple wavelengths of light. It is essential to have the numerical aperture of the condenser to be greater than the numerical aperture of the objective lens. 2) The 2nd configuration was used to show the methodology is applicable on instrument from different manufacturers. A Leica DIRBE microscope with a dark field condenser, 1 mm condenser lens and Plan Apo 63x with an adjustable iris diaphragm that was variable between 1.32 numerical aperture and 0.6 numerical aperture was employed. This system used a dry condenser, compared with the oil condenser from the Nikon system. The Leica system used a Plan Apo lens with an air condenser while the Nikon system used a Plan Fluor lens with an oil condenser. A higher numerical aperture with better resolution was achievable with the Nikon system due to the oil condenser. However this oil condenser is not applicable on all manufacturers' inverted microscopes.
DF-CLSM images of fluorescent polystyrene beads observed in the absence of cells were acquired under 404 nm and 488 nm laser illumination/excitation while images of TiO2 exposed cells were obtained primarily using 404 nm laser light for better resolution. Cellular and organelle-specific fluorescent stains were used to image the space in which the NP were localized. Simultaneous fluorescent (Confocal) and transmission (Darkfield) imaging were performed for all two- and three-dimensional images acquired using this technique. All images were collected using Nikon EZ-C1 software, and post-acquisitional processing was performed using the Nikon NIS-Elements AR software package. The confocal slice number corresponding to maximal light scatter intensity was taken as the location of the nanoparticle. Similarly, the slice at which maximal fluorescence intensity was observed was used to identify the location of the nucleus. For statistical comparison, normalization of particle position relative to the nuclei of multiple cells was accomplished by subtracting the nuclear slice number from the particle slice number, dividing by the total number of slices, and multiplying by a factor of 100 to obtain the closest whole-number.
Pairwise comparisons were analyzed by the Wilcoxon's signed rank test using GraphPad Prism statistical software (San Diego, CA); p < 0.05 was considered significant.
DF-CLSM detection of nanoscale particles
Examination of in vitro particle internalization using DF-CLSM
While the use of NP in consumer products, industrial processes, and pharmaceutical applications continues to grow, knowledge of the impact of nanomaterials on human health remains limited . Compounding the challenge presented by the paucity of toxicological information on nanomaterials, investigators studying the biological effects of nanomaterials are faced with a number of unique challenges. Fundamental questions pertinent to the interaction between nanoparticles and the cell, are best addressed with imaging studies. However, NP are usually not detectable by conventional light microscopy methods. In some instances, fluorescent nano materials (i.e., Q-dots) can be used with fluorescent microscopy. Darkfield microscopy can detect the presence of nanoparticles, but their location within the cell or on the surface of the cell can not be determined with accuracy using a wide field microscope. The combination of darkfield and confocal microscopy described in this manuscript was developed in an effort to address some of these imaging challenges by bringing the strengths of two distinct light microscopy techniques (DF and CLSM) to study the interactions of cells with environmentally relevant NP.
While confocal and wide-field fluorescence microscopy are commonly used to image synthetic nanoparticles tagged with fluorophores (e.g., Q-dots) evidence that particle surface chemistry plays a critical role in toxicity raises questions about the relevance of these materials as surrogates for "real world" nanoparticles [34, 35]. Electron microscopy (EM) is usually thought of as the "gold standard" for investigation of the biological impacts of nanomaterials. Unfortunately, EM can be quite laborious and costly to employ. Darkfield microscopy is essentially an illumination-based imaging technique used to enhance the contrast of specimens for increased visibility [15, 16, 17, 36]. Confocal microscopy is a multifaceted light microscopy technique that contributes increased resolution and optical sectioning of specimens for three dimensional analyses, as well as the precise application of excitation wavelengths [37, 38, 39]. The utility of DF-CLSM in detecting NP was established by experiments in which we show that the DF scatter signal colocalizes with the fluorescence of polystyrene particles with sizes as low as 50 nm in diameter. In fact, the DF signal appeared to provide superior discrimination of monomeric units relative to fluorescence for 50 nm particles. In this study, the location of maximal scatter intensity in the z-axis was presumed to be the physical center of the particle. Using this approach, it was possible to determine the depth of penetration of the particle within the cell relative to an organelle or the nucleus. In separate experiments, similar measurements of particle penetration were made using DF-CLSM with the cell membrane as a reference (Gibbs, unpublished). Thus, the combination of DF optics with the power of a confocal microscope yields an image in which NP can be visualized within a narrow and precise focal plane for the spatial determination of NP within the cell in the z-axis. With the application of currently available and novel deconvolution processing algorithms, it may be possible to better localize the NP within the volume of the cell in three dimensions. Importantly, the DF-CLSM technique allows the visualization of non-fluorescent particles, making it suitable to the study of environmentally relevant NP. An additional advantage of DF-CLSM is its potential to be used in experiments involving live-cell imaging, which is impossible with conventional EM.
Detection of NP using DF-CLSM relies heavily on the intrinsic light scattering properties of the material being observed. In the validation of this technique, DF-CLSM proved to be sufficiently robust to detect several types of NP comprised of different materials ranging from polymers to nanodiamonds and metal oxides (Gibbs et al, unpublished). Interestingly, even materials with relatively smooth surfaces, like the polymers of polystyrene beads, have sufficient light scattering properties to be detected by this technique. The associated signal from larger polystyrene beads is less than that produced by smaller TiO2 nanoparticles.
The DF-CLSM imaging approach holds considerable promise for future applications in the study of the biological interactions of NP. While in the present study we chose to use a simple nuclear stain in the assessment of particle internalization, other biological processes and interactions could be examined by DF-CLSM using the numerous biosensors and staining reagents available. For laboratories with existing CLSM imaging equipment, implementation of DF-CLSM requires only the acquisition of a relatively inexpensive darkfield condenser and objective lenses with a suitable variable iris to adjust the numerical aperture, or objectives lenses with low fixed numerical aperture values. We have been able to successfully adapt both Leica and Nikon inverted confocal microscopes with condensers costing between $70 and $700, respectively.
As with any technique, DF-CLSM has limitations. In this regard, it is important to bear in mind that this application of DF is a detection method, not a technique that permits direct observation or exact size of the NP. Thus, this method does not produce an accurate size representation of nanoparticles. Likewise, agglomerates of nanoparticles may be represented as a single point with a larger size and increased light scatter. Therefore, inferences regarding size, shape, and number (i.e., agglomeration) of the structures being examined are limited, as other factors such as surface irregularity and reflectivity contribute significantly to the signal strength in DF detection. Furthermore, although they are less expensive than their high numerical aperture counterparts, it should also be noted that low numerical aperture objectives required for DF present disadvantages as well. Low numerical aperture objectives impose limits on optical resolution and may introduce chromatic aberration into the image. In our characterization of this technique, we have found that choosing a single excitation wavelength is the best way to avoid chromatic aberration and colocalization errors. Similarly, the DF and confocal fluorescence signals should ideally be acquired using the same excitation wavelength in order to avoid possible colocalization errors between different wavelengths of lights, as shown in Figure 2C. In cases where multiple excitation wavelengths are needed, they should be used sequentially rather than simultaneously and the 404 nm line should not be used with the visible wavelenghts. By default the shortest wavelength should be used for the acquisition of the DF signals, but it is important to use a wavelength in which the NP is being localized with the fluorescence structure. Notably, appropriate use of the excitation wavelengths used during image acquisition must be taken into account because data acquired with sequential excitation of multiple wavelengths may introduce chromatic aberration errors in the sample between the nanoparticles derived from one wavelength and the fluorescent signals derived from the other laser lines. This is not necessarily a limitation unique to this application, but more likely a limitation resulting from the UV and visible colocalization issues in CLSM and the quality and alignment of the optical components used in the CLSM equipment. It appears that the nanoparticles accentuate these colocalization problems relative to submicron and micron particles. It is recommended that characterization of issues regarding chromatic aberration and colocalization of various wavelengths should be made for each imaging system and each lens used.
Even with the acknowledged limitations, the DF-CLSM methodology represents a novel and workable option for many investigators searching for a light microscopy technique that can be used to study the interactions between cells and NP in the environment. By interfacing the ability of darkfield microscopy to use light scatter to detect very small structures with the power of confocal microscopy to render specimens in three dimensions, DF-CSLM provides a solution to the unique challenges of conducting toxicological studies in the nano-scale. The DF-CLSM technique is superior to widefield DF as it uses the power of the confocal microscope to produce 3D images of nanoparticles within cells.
The authors gratefully acknowledge the assistance of Mrs. Wan-Yun Cheng and Mr. Robert Silbajoris as well as the helpful discussions with Mr. Cory W. Quammen and Dr. Russel M. Taylor, II.
Disclaimer: The research described in this article has been reviewed by the National Health and Environmental Effects Research Laboratory, U.S. EPA, and approved for publication. The contents of this article should not be construed to represent Agency policy nor does mention of trade names or commercial products constitute endorsement or recommendation for use.
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