Elsevier

Ultramicroscopy

Volume 82, Issues 1–4, February 2000, Pages 297-305
Ultramicroscopy

Atomic force microscopy imaging of living cells: a preliminary study of the disruptive effect of the cantilever tip on cell morphology

https://doi.org/10.1016/S0304-3991(99)00139-4Get rights and content

Abstract

Recent studies have demonstrated that atomic force microscopy (AFM) is a potential tool for studying important dynamic cellular processes in real time. However, the interactions between the cantilever tip and the cell surface are not well understood, and the disruptive effect of the cantilever tip on cell morphology has not been well characterized. In this study, the disruptive effect of the scanning cantilever tip on cell morphology, in the AFM contact mode, has been investigated. The aims of this study are to identify what kinds of cell morphological changes generally occurred under normal AFM imaging conditions and to find out how long cells remain viable during scanning. Two cell lines, SK–N–SH (human neuroblastoma cells) and AV12 (Syrian hamster cells) were studied in the experiment because these are widely used in biomedical research as an expression system for studying cellular functions of neuronal receptors. The experimental results suggest that the sensitivity of cells to the cantilever disruptive effect is dependent on cell type and that there are patterns observed in the changes of cell morphology induced by the cantilever force in these two cell lines.

Keywords

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Keywords

Cell morphology
AFM cantilever
Cell adhesion
Cell death

1. Introduction

Atomic force microscopy (AFM), with the capability of operating in aqueous solution, has great potential as a tool for imaging living cells in their physiological environments and for studying biologically important dynamic cellular processes in real time, with molecular resolution [1], [2], [3]. In addition, AFM can be used to study quantitatively cell elasticity and molecular interaction forces. Currently, real-time monitoring of dynamic events of living cells, cell–cell interactions and morphological changes of the cells in response to intracellular and extracellular stimuli has been the focus of a number of AFM studies [4], [5], [6], [7], [8], [9]. However, most of the AFM studies of living cells reported so far have been conducted using the contact mode, where the tip physically contacts the cell surface during scanning and exerts certain forces onto the cell surface. The scanned cells inevitably suffer various degrees of structural deformation or damage because of their intrinsic softness, which may provoke significant biological changes inside the cell. Furthermore, when AFM is used to monitor dynamic cellular events, there are difficulties in determining whether the changes in cell morphology observed are authentic, arising from dynamic cellular movement, or are artificial, induced by the perturbing action of the AFM cantilever [5], [10]. To make matters worse, the interactions between the cantilever tip and the cell surface are so complex that there is no simple way to control the tip–cell interactions and to eliminate the disruptive effect of the scanning cantilever. This has become a significant technical hurdle in AFM imaging of living cells [1], [2], [3]. Therefore, for further exploration of AFM applications in the study of important dynamic cellular processes, the disruptive effect of the cantilever on cell morphology must be investigated, and more AFM studies are necessary to establish whether a relationship exists between cell morphology and disruptive effect of the cantilever.
In this study, we investigated the disruptive effect of the scanning cantilever tip on cell morphology. We scanned a large number of samples under identical experimental conditions in order to identify what kinds of changing patterns in cell morphology generally induced by the scanning cantilever in the contact mode and to find out how long cells remain viable under normal AFM imaging conditions. Two cell lines, AV12 (a Syrian hamster cell line) and SK–N–SH (a human neuroblastoma cell line), were used in the experiment because these cells are widely used, in biomedical research, as an expression system for studying cellular functions of neuronal receptors. We expected that the experimental results would provide some guidance for further AFM studying of dynamic cellular events of these two cell lines and for future high-resolution AFM imaging of neuronal receptors expressed in these cells.

2. Experimental methods

SK–N–SH cells were obtained from the American Type Culture Collection (Manassas, USA) and AV12 cells were kindly provided by Eli Lilly Corporation (Indianapolis, USA). Sterilized glass coverslips of 15 mm in diameter were placed in cell culture dishes containing freshly passaged SK–N–SH or AV12 cells. The cells were cultured in conventional culture media in all cases and incubated at 37°C with 5% CO2. After 2 days, the glass coverslips were mounted for AFM imaging.
AFM imaging of living cells were carried out in 25 mM HEPES-buffered cell culture media (without serum) at room temperature using a Nanoscope IIIa (Digital Instruments Inc., Santa Barbara, CA) equipped with a 120 μm (J type) scanner and an AFM fluid cell. The AFM was operated in the contact mode using a 200 μm long, V-shaped silicon nitride cantilever (Digital Instruments Inc.). The nominal force constant of the cantilever is 0.06 N/m. The image data were collected in the deflection mode with a loading force of typically 1 nN and at a scan rate of typically 0.9 Hz. During scanning, fresh culture media were injected into the AFM fluid cell to maintain the volume of solution, and the setpoint voltage was adjusted to minimize the cantilever loading force.

3. Results

3.1. AV12 cells

The growth of AV12 cells to the glass coverslips requires cell-to-cell interactions or cell-to-extracellular matrix interactions, and the cells usually form patches of various sizes on the substrate. Fig. 1 shows a typical series of sequential AFM images taken from a patch containing several AV12 cells. As shown in Fig. 1a, the living cells on the surface were initially held together by an extensive and dense fibrillar structure that is believed to be the extracellular matrix (ECM) possibly interconnected with the cytoskeleton. Soon after the completion of the second scanning (Fig. 1b), the fine fibrillar features were disrupted, reflecting from a decrease in the density of the fibrillar structure. Once the contact with the ECM was degraded, the cells underwent remarkable changes in morphology with further scanning, i.e., the cells collapsed and their large nuclei became apparent (Fig. 1c). The flat areas surrounding the nuclei are the cell membranes, showing the predominant structures frequently observed in the AFM imaging of living cells, i.e., the cytoskeleton. The cell adhesion to the substrate was weakened by the disruption of the cell-ECM or cell-to-cell interactions and the potential for cellular displacement by the scanning cantilever was increased. As noted, a single cell seen in the previous scan was removed, leaving a void in the upper right corner of the surface (Fig. 1d). The loss of this cell appeared to affect the integration among its neighbors, and the rest of the neighboring cells were swept away in the subsequent scanning (Fig. 1e and f).
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Fig. 1. A typical sequence of deflection-mode AFM images (60×60 μm) obtained from a patch containing several AV12 cells over a period of ∼42 min, showing dramatic changes in the cell morphology. Image acquisition time: ∼6 min/frame.

Fig. 2 shows another typical series of sequential AFM images obtained from a patch with a higher density of AV12 cells. The fibrillar structure was still discernible from the healthy cells (Fig. 2a), but its density was less than that shown in Fig. 1a. However, in this case, the disruption of the cell-to-ECM contact did not bring about abrupt morphological changes in the cells. Here, we believe that, as compared to the cells in Fig. 1, the cells in a patch of greater density have little room to move or spread themselves around. Instead, the cells gradually rounded up, reflected by the more bright areas appearing in the AFM images (Figs. 2b and c). The rounded cells, owing to their weakened adhesion to the neighboring cells or to the substrate, appeared to be more susceptible of being removed by the scanning cantilever. It appeared that cells in a compact layer were more resistant to the cantilever disruptive force, for instance, only one rounded cell was removed after continuously scanned over ∼40 min (Fig. 2c). The rest of the cells were held firmly in their place by the remaining cell-to-ECM interactions (Fig. 2d) and were gradually removed by the scanning cantilever. As noted, the fibrillar structure connecting two cells at the left up-right quadrant of Fig. 2c and d remained intact, and these two cells were the last that were removed (Figs. 2e and f).
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Fig. 2. Another typical sequence of deflection-mode AFM images (80×80 μm) from a patch of a higher density of AV12 cells, showing that the cells in a more compact layer are less susceptive to the cantilever disruptive force. Image acquisition time: ∼8 min/frame.

3.2. SK–N–SH cells

SK–N–SH cell lines are comprised of two distinct cell types [11]. One cell type, termed `N', is neuroblastic in appearance, with a small, rounded, loosely adherent cell body. The other cell type, termed `S', is large and flattened, resembling epithelial or fibroblast cells, and is highly substrate-adherent. A typical sequence of AFM images of two SK–N–SH cells (i.e., the S type) acquired in situ over a period of ∼100 min is shown in Fig. 3. The distinctive cytoskeleton network was frequently observed in living SK–N–SH cells and was the dominant topographic feature in the AFM images (Fig. 3a). The S-type cells appeared stable under the imaging conditions used and did not show any significant changes in morphology over a scanning period of ∼43 min (Figs. 3b and c). However, substantial changes in the cell morphology were observed after ∼62 min scanning and occurred at the edges of the cells (Fig. 3d). It appeared that the cells began to shrink in size as if the edge of the cell was being scraped away by the scanning cantilever, but the “footprint” of the lost edge part was left at the surface (Fig. 3d). As scan continued, an apparent boundary (indicated by an arrow in Fig. 3e) emerged between the two cells (Figs. 3e and f). Because of tip contamination or cell degradation, the cytoskeleton was less discernable in Figs. 3e and f. The small and round-shaped cell, i.e., the N-type (upper half of Figs. 3a–c) disappeared by approximately 57 min, because this kind of the cell does not have strong adhesion to the substrate surface. Finally, it was noted that the cytoskeleton structure remained intact with respect to its organization and orientation over the 100-min time course shown.
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Fig. 3. A typical time-lapse series of deflection-mode AFM images (80×80 μm) of SK–N–SH cells, showing that the cytoskeleton structure remains intact over a scanning period of ∼100 min. Image acquisition time: ∼5 min/frame.

Fig. 4 shows another typical sequence of AFM images of SK–N–SH cells over a period of ∼130 min. The cytoskeleton network was discernable on the surface of the larger and flattened SK–N–SH cell (i.e., the S-type) in Fig. 4a, which was attached with a small and rounded cell, i.e., the N-type (Figs. 4b and c). The N-type cell was loosely adhesive to the substrate and was removed at which time the larger cell appeared injured and its size was reduced (Fig. 4d). The injured cell gradually had its central part rise up (Fig. 4e) and became more swollen after about 130 min of scanning (Fig. 4f). This cell totally disappeared from the surface in the next scan. As can be seen in Fig. 4, the cytoskeleton network is visible over a scanning period of ∼80 min. In addition, the lamellipodia of the healthy cells appeared smooth and flattened (Fig. 4a), but after the cell sustained scanning over ∼30 min, the edge of the cell exhibited filopodia (Fig. 4b). The filopodia were changing their patterns from scan to scan and remained visible until the cell was removed (Figs. 4c–f).
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Fig. 4. Another typical time-lapse series of deflection-mode AFM images (60×60 μm) of a SK–N–SH cell, showing an another example of the cantilever disruptive effect on cell morphology. Image acquisition time: ∼5 min/frame.

4. Discussion

As it is known, in the contact mode, the cantilever is physically in contact with the cell surface during scanning, and the cantilever exerts both vertical compression and lateral shear forces on the cell surface. The force applied by the cantilever is typically in the range of 1 nN, which is destructive for living cells. Therefore, under normal AFM imaging conditions, cells are inevitably injured to some degree, which will eventually lead to cell death.
Our preliminary experimental results suggest that there is a relationship between sensitivity to the cantilever disruptive effect and cell type and that there are some patterns existing in the change of cell morphology in the two cell lines studied. The AV12 cells were more susceptive to damage caused by the cantilever disruptive force than the SK–N–SH cells. Once the AV 12 cells were injured, significant changes in the cell morphology were immediately observed. Moreover, by examining survival of each AV12 cells in the AFM images with time, we found that the cells were not equally susceptible to be removed by the cantilever when deprived of cell-to-cell or cell-to-substrate adhesion. Instead, the degree of sensitivity varies from cell to cell. We believe that cell adhesion is one of the major physiological factors that control cell susceptibility to the cantilever disruptive effect. The survival of the AV12 cell requires cell adhesion to extracellular matrix (ECM) and cell-to-cell interactions; by contrast, the survival of the SK–N–SH cells requires mainly cell adhesion to the substrate, provided by the stress fibers developed within the cells. When appropriate ECM contacts are absent and cell adhesion to the substrate is degraded, cells suffer injury and undergo cell death processes [12]. The injured cells gradually lose their normal shape, become rounded up and shrink in size, and are removable from the substrate surface.
It should be mentioned that our experiments, like most of AFM studies reported so far [1], [2], [3], have been conducted in a balanced salt buffer and at room temperature that is not equivalent to the environment of cell culture. Together with the cantilever disruptive force, this factor may significantly accelerate the process of cell death and reduce the time window of cell viability. However, these are the conditions commonly used in AFM studies of living cells. Furthermore, we found that the rather strong interactions between the cantilever and the cell surface are often present during scanning, and the damaging effects of the scanning cantilever on the cell surface may start right from the beginning of scan. The observation of the disruptive effect of the scanning cantilever in AFM images depends on the viability of the cell type and the experimental conditions used (e.g., scanning time, loading force, imaging mode, etc.).
Finally, our study has shown that the susceptibility of cells to the AFM cantilever disruption is strongly adhesion-dependent. It is known that the adhesion of a cell to others or to a substrate is mediated by specific receptor–receptor or receptor–ligand bonds or ECM elements. Thus, it may be possible to use biochemical methods to enhance cell adhesion, to investigate further, using AFM, adhesion-mediated cell resistance to the cantilever disruption, and to seek a new sample preparation to improve cell survival.

5. Conclusions

We studied the disruptive effect of the AFM scanning cantilever on cell morphology. Our experimental results show that the disruptive effect on the cell morphology induced by the AFM cantilever often exists in the contact mode under normal imaging conditions. The cells being scanned suffer injuries to various degrees, depending on the cell type and viability, and the injured cells may undergo remarkable changes in morphology. In general, with prolonged scanning, the cells gradually change their normal shape (e.g., becoming more rounded and shrinking in size), lose their adhesion to the substrate or to the neighboring cells, and detach or are removed from the substrate surface. Our study indicates that the improvement of cell adhesion is a way to promote cell resistance to the cantilever disruptive effect.

Acknowledgements

We would like to thank the NIH for financial support and Dr. J. Strong for critical review of the manuscript. JML is supported by F31 DA05834.

References

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