3.1 Surface energy regulates cell responses
The physiochemical properties of ECM could have strong effects on cell-ECM interactions.33 In this study, surfaces with flat PDMS, nanopillars, silicon oxide, and titanium oxide were developed, and their influence on cell migration behaviors was investigated. X-ray photoelectron spectroscopy (XPS) was used to study the chemical compositions of the oxides. The silicon oxide was in the form of SiO1.7 and the titanium oxide was in the form of TiO1.4 based on the XPS analysis.
Surface energy of an ECM or an engineered platform is related to its physical and chemical characteristics.34 Water contact angle measurement was used to evaluate the surface energy of different surfaces on the microfabricated platforms. Figure 2 shows the water contact angle, migration trajectory, and cell morphology on different surfaces without FN coating. Surfaces with flat PDMS and nanopillars were hydrophobic (contact angle > 90°) with a larger water contact angle of 101° and 131°, corresponding to the low surface energy of 22.9 and 16.0 mN/m, respectively, as shown in Figs. 2(a-b). On the other hand, PDMS surfaces coated with 20 nm thick silicon oxide or titanium oxide were hydrophilic (contact angle < 90°). Their water contact angles were 12° and 74°, respectively, and the corresponding surface energy was 47.8 and 32.3 mN/m, as shown in Figs. 2(c-d). Surface energy of biomaterial could drive ligand topology and generate different focal adhesion signaling pathways between cells and substrates. These signals could modulate cytoskeletal tension and cause different cell responses.35
To observe the difference in cell behavior, the Supplementary movie SV1 of MC3T3-E1 cell migration on different surfaces over 16 h with 5 min/frame were given. As shown in Figs. 2(e-h), cells cultured on these surfaces had random migration trajectories. No guidance effect for cells on various platforms was found as cells had similar migration speed in the x- and y-directions, as shown in Supplementary Fig. S3(a). This is due to the lack of directional surface topography for cell migration guidance. However, cells migrated on hydrophobic flat PDMS or nanopillar surfaces had longer paths and faster movements than those cells on hydrophilic oxide surfaces. The persistence length and kymographs of cell migration on different surfaces were analyzed to characterize the total travel distance of the migration path and the pace of the cell movement, as shown in Supplementary Figs. S4 and S5. Cells migrated on PDMS surface with nanopillars had the longest total migration path and the fastest cell movement pace. These could be related to the PDMS surface with nanopillars was the most hydrophobic surface, which made it easiest for cells to detach from the surface and continue to migrate. Both the persistent lengths and the kymographs are consistent with the trajectories shown in Figs. 2(e-h). Figures 2(i-l) show the distinctive morphologies of MC3T3-E1 cells on different surfaces. Cells cultured on hydrophobic flat PDMS or nanopillar surfaces possessed polarized morphologies, and the elongated cells had leading and trailing edges, indicating strong motile behavior as shown in Figs. 2(i-j). In particular, the presence of nanotopography can promote cell elongation, contraction, and ultimately cell migration. As shown in Fig. 2(j), nanopillars formed discontinuous surface for cell adhesion. This made it easier for cells to attach to and detach from the surface during migration, leading to rapid cell movement.36 Furthermore, deformation of the nanopillars was observed, suggesting that the nanopillars may be more conducive to transmitting cytoskeletal tension to the substrate.37 On surface with nanopillars, cells extended numerous filopodia in all directions and the extensions of filopodia were more prominent around the advancing cell edge. However, cells grown on hydrophilic oxide surfaces showed less elongation and more spreading, as shown in Figs. 2(k-l). One plausible explanation for these differences is related to the surface energy modulation of the distribution and deposition of adsorbed proteins.38 These results indicate that surface energy could be a critical factor affecting cell migration behaviors and cell shapes.
3.2 Cell migration and cell morphology on different surfaces
Figure 3 shows the cell migration speed, aspect ratio, and elongation of MC3T3-E1 cells on different surfaces without FN coating. Cells migrated fastest at 0.99 µm/min on surface with nanopillars, as shown in Fig. 3(a). In addition, cells on flat PDMS surface migrated faster with a speed of 0.64 µm/min than those on silicon oxide or titanium oxide surfaces. The migration speed of cells on the silicon oxide surface was 0.36 µm/min compared to 0.25 µm/min on the titanium oxide surface. These results agree with previous studies that cell migration speed was closely related to surface topography, surface energy, and surface chemistry.39 Interestingly, cells on nanopillars had the highest migration speed compared to other surfaces. This is attributed to the fact that nanopillars generated a most hydrophobic surface, making it more difficult to form focal adhesion sites, and hence weaker cell adhesion and faster cell migration speed.40 On the contrary, hydrophilic surfaces promoted stronger cell adhesion, and resulted in slower cell migration speed. However, a highly hydrophilic surface inhibited the binding of cell adhesion mediators, thus hindering cell adhesion behavior. The moderate hydrophilic surface with a contact angle between 60° to 80° has been shown to have the highest cell adhesion.23,41,42 On titanium oxide surface, the water contact angle was 74°, corresponding to the highest cell adhesion and the slowest migration speed.17
Changes in aspect ratio over 16 h are shown in Fig. 3(b). The cell aspect ratio is defined as the ratio between the major and minor axes when cells are fitted to an ellipse.10 Initially, cells on the flat PDMS surface had a more rounded shape, and the aspect ratio was small because of the unstable attachment to the hydrophobic PDMS surface.23 Once cells formed a stable attachment to the PDMS surface over time, the aspect ratio increased with time. It became larger than those on the titanium oxide surface after 9 h. For cells on the surface with nanopillars, they also were more rounded initially, and the aspect ratio increased with time. However, cells had a smaller aspect ratio but frequent cytoskeletal rearrangement compared to those on flat PDMS surface, corresponding to more rapid cell movement, as shown in Supplementary movie SV1(b).43 In addition, the aspect ratio for cells on titanium oxide surface was larger than those on silicon oxide surface.
Furthermore, cell elongation was obtained by averaging the aspect ratio over 16 h, as shown in Fig. 3(c). MC3T3-E1 cells on the surface with nanopillars showed a cell elongation of 3.65, similar to those on the flat PDMS surface with an elongation of 3.82. In comparison, cell elongation for cells seeded on silicon oxide and titanium oxide surfaces was 2.90 and 3.48, respectively. These results indicated that the polarization characteristics of cells on the hydrophobic surface were more obvious than those on the hydrophilic surface. This may be due to the different surface energy that affected the distribution of adsorbed protein, and proteins on the hydrophobic surface were more likely to form unidirectional distribution.18,38 The elongation of cells on nanopillars was similar to that on flat PDMS surface, as they had similar surface energy and fast cytoskeletal rearrangement. However, there was still significant difference compared with cells on silicon oxide surface, which had a more rounded shape. The hydrophilic silicon oxide had the highest surface energy, making it easier for cells to adhere on the surface in multiple directions, resulting in less cell elongation. These results showed that cell morphology could be controlled by changing the surface energy.
On the other hand, cell area on silicon oxide or titanium oxide surfaces was larger than on flat PDMS or nanopillar surfaces, as shown in Supplementary Fig. S3(b). These findings coincided with the previous finding that the fibroblast cells on hydrophilic surfaces exhibited larger cell area compared to those on hydrophobic surfaces.23 In particular, cells on nanopillar surface showed the smallest cell area, which was consistent with a previous report that indicated cells on nanopillars resulted in a 40–50% reduction in cell area compared to those on a flat surface.44 These results indicate that there are close relationships between cell migration speed, morphology, and surface energy on different surfaces.
3.3 Cell migration behaviors influenced by fibronectin coating
The migration behavior and cell morphology for cells on different surfaces coated with FN were further investigated, as FN coating on top of the microposts was needed for traction force study. All the work on cell migration characterization from this point on was carried out on surfaces coated with FN. With FN coated on the surfaces, the water contact angles of flat PDMS, nanopillars, silicon oxide, and titanium oxide were 64°, 82°, 22°, and 38°, respectively, as shown in Supplementary Fig. S6. The contact angles of these surfaces decreased, which corresponded to the increases in surface energy. The cell migration speed decreased on all surfaces coated with FN, but the trend remained unchanged, as shown in Fig. 4(a). A migration speed of 0.78 µm/min was obtained for cells on nanopillars with FN coating, which is significantly higher than other FN coated surfaces. In addition, the cell migration speed on flat PDMS was 0.43 µm/min, and it is higher than on silicon oxide and titanium oxide, which had migration speed of 0.37 and 0.33 µm/min, respectively. On the other hand, cell aspect ratio and elongation had little dependence on surface conditions, as shown in Figs. 4(b-c). With FN coating, cell morphology was similar on all surfaces, except for cells on nanopillars which showed a slightly larger aspect ratio.
After the FN coating, all surfaces became more hydrophilic and cell adhesion was enhanced, resulting in reduced cell migration speed. Furthermore, the addition of the protein layer facilitated cell spreading in multiple directions, leading to more rounded cell shape. These results may be related to the surface energy-driven ligand assembly.35 Cell migration behavior changed due to variations in protein adsorption.45,46 Additionally, FN is a major component of ECM that mediates various cellular behaviors. When cells attach to the ECM surface, focal adhesions are formed by binding of the integrin receptors to FN adsorbed on the surface, constituting a mechanotransduction link between the cytoskeleton and the ECM.9 The actin cytoskeleton mediates tension to adapt its shape and exhibits complex mechanocoupling responses to achieve cell migration. The formation of focal adhesions is the prerequisite for the generation of cell traction force. Cell adhesion area, protein adsorption, and fibrilar adhesion are changed and thus influence the complex cell force that acts on the ECM surface. Surface energy-driven mechanotransduction may cause cells to migrate faster on surface with nanopillars coated with FN.
3.4 Cell traction force exerted on microposts with nanopillars or oxide coatings
In this study, micropost sensing arrays were used to measure the cell traction force on platforms with various surface conditions. All the micropost arrays were coated with FN on top and Pluronic on the sidewalls of microposts, as these coatings were necessary to keep the cells on top of the microposts for cell traction force study. Supplementary Fig. S7 shows that the cell migration speed on flat PDMS surface and on microposts without nanopillars had no significant difference. Since cell migration on flat PDMS surface and on microposts without nanopillars was similar, the micropost arrays could be applied to sense the cell traction force.
Figure 5. Traction force development for MC3T3-E1 cell migration on PDMS microposts (a) without and (b) with nanopillars. (c) Normalized traction force in leading, middle, and trailing regions of cells on microposts with various surface conditions. Microposts were coated with FN on top and Pluronic on sidewalls. The yellow dashed line indicates cell contour. The starting and ending positions are indicated by asterisks and dots in the micrographs, respectively. The white arrows indicate the traction force on microposts. The length of the white arrow represents the magnitude of the traction force. Cell migration direction is marked by a blue arrow, representing the movement of the cell centroid during a single migration cycle. One-way ANOVA and Tukey’s post hoc test, ***p < 0.001.
As shown in Fig. 5(a), the measured traction force was directed towards the cell center with higher force acted around the cell periphery and lower force at the cell center. During migration, the cell elongated by protruding the leading and trailing regions. The corresponding traction force increased gradually, and higher force was found near the leading region compared to the trailing region of the cell. The cell barely moved forward when it was elongated. Then, the trailing region detached from the microposts, and the traction force dropped in both the leading and trailing regions. As the trailing region retracted, the cell moved forward and started the migration cycle again. This cyclic behavior repeated itself during cell migration and is consistent with previous findings.28,29 As shown in Fig. 5(b), cells migrated on microposts with nanopillars had the similar cyclic behavior but showed greater amplitudes of traction force in all three cell regions and shorter cycle time. Meanwhile, microposts with silicon oxide or titanium oxide also had the similar cyclic behavior. However, cells migrated with lower amplitudes of traction force and longer cycle time. These results indicate that cell migration was cyclic, and shorter cycle time and higher migration speed corresponded to cell migration on surface with larger traction force. In addition, cells generated larger traction force when they were elongated compared to contracted cells, which may be due to the greater actin cytoskeleton tension during cell elongation. Being able to realize the traction force distribution for cells during migration will provide a better understanding of the cell migration mechanisms.
Figure 5(c) shows the normalized net traction force in the leading, middle, and trailing regions when cells were elongated. For cells seeded on microposts without nanopillars, the traction force exerted in the leading region was 9.9 ± 0.7 nN, higher than 5.8 ± 0.6 nN in the trailing region and 3.44 ± 0.6 nN in the middle region. The trend of traction force generally agrees with previous reports.28,29 In comparison, the traction force of the leading, middle, and trailing regions for cells seeded on microposts with nanopillars was larger than that on microposts without nanopillars. The traction force in the leading region was 17.1 ± 1.0 nN, 10.2 ± 0.9 nN in the trailing region, and 6.8 ± 0.5 nN in the middle region. On the other hand, the traction force of cells on silicon oxide surface was smaller in the leading (8.4 ± 0.4 nN), middle (2.8 ± 0.3 nN), and trailing (5.7 ± 0.4 nN) regions when compared with cells on the flat PDMS surface. For cells on titanium oxide surface, the traction force in the leading, middle, and trailing regions was 7.2 ± 0.4, 2.4 ± 0.3, and 5.1 ± 0.4 nN, respectively, and they were smaller than cells on the silicon oxide surface.
In general, cells on all surfaces had a large force imbalance from the leading to trailing regions. Traction force of the leading region was the largest, and the middle region was the smallest. Furthermore, the force in the leading region was greater than that in the trailing region when cells were moving forward. This may be due to the fact that more filopodia were in the leading region compared to the trailing region, which was related to the ligand adhesion that formed a larger fibrilar adhesion force. On the other hand, cells on various surfaces had traction forces with different magnitude, which corresponded to the related cell migration speed. Cells on the nanopillars had the largest traction force, which corresponded to the fastest migration speed. With the introduction of nanotopography, nanopillars could absorb protein easily, which facilitated the transmission of traction force to the substrate.47 Also, nanopillars could promote the formation and extension of filopodia and long protrusions, therefore the fibrillar adhesion force between the cells and the substrate could be enhanced. Hence, it can be inferred that strong fibrillar adhesion force as well as good transmission of traction force could result in large cell traction force and high migration speed on surface with nanopillars.48
3.5 Cells migrated on microposts with nanopillars have more filopodia and long protrusions
Figure 6 shows the distinctive morphologies of MC3T3-E1 cells on different platforms and the quantitative analysis of filopodia and long protrusions. Cells attached to the top of microposts due to the selectively coated proteins on top and Pluronic F-127 on the sidewall of microposts.31 As cells migrated, microposts bent under cell traction force, and the displacement of microposts served to quantify the traction force exerted by the cells. As shown in Fig. 6(a), cells on microposts without nanopillars bent the microposts towards the cell center due to cell traction force, similar to cells migrated on top of microposts with nanopillars, as shown in Fig. 6(b). In addition, microposts with silicon oxide or titanium oxide bent in similar manners as shown in Figs. 6(a-b). However, cells on microposts with nanopillars had more filopodia and long protrusions, which was consistent with our previous findings that nanostructures promote the generation of filopodia and long protrusions.19
High-resolution SEM was utilized to quantify the number and length of filopodia and long protrusions on different platforms, as shown in Figs. 6(c-d) and Supplementary Figs. S8(a-b). The MC3T3-E1 cells on microposts without nanopillars typically had 6 filopodia/cell and 4 long protrusions/cell. For cells on microposts with silicon oxide and titanium oxide, the numbers of long protrusions were 3 and 4, respectively, and the same number of 5 filopodia/cell. For cells on microposts with nanopillars, the numbers of filopodia/cell and long protrusions/cell were 13 and 6, respectively. More filopodia and long protrusions were formed on microposts with nanopillars on top, which resulted in the larger cell traction force. However, there is no significant difference in the length of filopodia or long protrusions, as shown in Supplementary Figs. S8(a-b). Since the microposts were separated from one another, the discontinuous gaps between the microposts may limit the extensions of filopodia and long protrusions. Having more filopodia and long protrusions extended from the cell membrane resulted in a larger traction force, and thus gave rise to the higher migration speed of MC3T3-E1 cells on nanopillars.19 These results agreed with previous observations that more actin-rich protrusions from cell edges generated larger contractile forces during cell migration.49
3.6 Dynamic traction force monitored on various surfaces
During directional migration, cells will undergo cyclic dynamic changes during which the distribution of cell traction force from the leading front to the trailing edge can affect the cell migration.50 Thus, the measurement of cell traction force development over time from the leading to the trailing regions during cell migration is essential to provide insights into cell migration dynamics. Using the force vectors measured by the microposts and normalizing the force by the number of microposts covered by a cell, the cell traction force in the three regions and cell migration speed were analyzed as a function of time, as shown in Figs. 7(a-d).
Figure 7(a) shows that cells migrating on microposts without nanopillars contracted initially at 0 min with a relatively smaller traction force for all regions. Over time, the cells became elongated with increased traction force. Traction force of the leading region was larger than that of the trailing region, and traction force of the middle region was the lowest. The trailing region started to release at 69 min as the traction force dropped in both the leading and trailing regions. After the trailing region was completely disconnected from the microposts at 81 min, cells contracted, and the next migration cycle began. The cyclic changes in the traction force and cell morphology agree with our previous findings.28 When cell shape changed from contraction to elongation, lamellipodia protruded over time and formed leading, middle, and trailing regions. Traction force increased gradually when the cell was elongated, but the cell barely moved. Cell speed increased significantly after the adhesive sites in the trailing region released, and the cell moved forward. Then the next cell migration cycle started, and the change of speed repeated.
For cells migrating on microposts with nanopillars, silicon oxide, and titanium oxide, the time dependent traction force had similar cyclic changes as cells on microposts without nanopillars, as shown in Figs. 7(b-d). The traction force for cells on microposts with nanopillars increased gradually with the protrusion of the leading region, and the cell shape changed from contracted to elongated. Traction force increased significantly when the cell changed from contraction to elongation. Later, traction force dropped rapidly as the trailing region was released, and the cell moved forward, completing the cytoskeleton reorganization. Compared with the other three surfaces, surface with nanopillars generated larger traction force, probably related to the rapid skeletal reorganization of the cells on nanostructures as mentioned above. With the release of the trailing region, cell speed increased as the cell moved ahead. A skeleton reorganization cycle was defined as the time needed between two consecutive maximum instantaneous speeds. This cycle time of the cells on the microposts with nanopillars was 42 min, and 54, 63, and 66 min for microposts without nanopillars, with silicon oxide, and with titanium oxide, respectively. These results showed that cells had the shortest cycle time on the microposts with nanopillars.
Furthermore, as shown in Fig. 7, the maximum instantaneous speed was 1.75, 1.66, 1.05, and 0.87 µm/min for microposts without nanopillars, microposts with nanopillars, microposts with silicon oxide, and microposts with titanium oxide, respectively. The corresponding traction force was 12.08, 11.62, 7.15, and 6.98 nN for these four types of micropost surfaces, respectively. To a certain extent, the maximum instantaneous speed was higher for larger traction force. In addition, the dynamic cell traction force on microposts with nanopillars was the largest throughout the cell migration cycle compared to the other three surfaces. The larger dynamic traction force also correlated to a higher migration speed. It is evident that dynamic traction force is a function of surface topography and coating that can strongly influence cell migration. Using micropost arrays to monitor cell traction force, cells on various surfaces showed similar time dependent traction force changes during migration. However, the magnitude of the cell traction force depended on the surface topography and coating on the micropost surface. These results had potential implications for designing biomimetic ECM in bone tissue engineering.