Regulating cell behaviors on micropillar topographies affected by interfacial energy

Xinghua Gaoa, Yeung Yeung Chau b, Jiao Xiee, Jun Wanaf, Yanxiao Rend, Jianhua Qin*c and Weijia Wen*abde
aBiomedical Research Institute, Shenzhen Peking University – The Hong Kong University of Science and Technology Medical Center, Shenzhen, China
bDepartment of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong. E-mail: phwen@ust.hk; Tel: +852-23587979
cKey Laboratory of Separation Science for Analytical Chemistry, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian, China. E-mail: jhqin@dicp.ac.cn; Tel: +86-41184379650
dThe Hong Kong University of Science and Technology Shenzhen Research Institute, Shenzhen, China
eSoft Matter and Interdisciplinary Research Institute, College of Physics, Chongqing University, Chongqing, China
fDivision of life science, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong

Received 3rd February 2015 , Accepted 23rd February 2015

First published on 23rd February 2015


Abstract

Micro/sub-micro substrate topography plays an important role in cell morphology and function. By localizing individual hepatic stellate cells on different micropillar topographies, we found that the cell morphology was thus greatly influenced due to the cell location. As a simple physical model showed, the morphological response of cells to micropillar topography can be triggered by a minimum interfacial energy. In particular, an established topography with a spacing of 2.5 μm and pillar diameter of 5 μm was found to be able to change the expression of E-cadherin and α-smooth muscle actin. It suggested that the size of the established topography might be closely related to cell epithelial–mesenchymal transition. This study has potential significance in mimicking the size of Disse's space in pathological conditions and advanced the understanding of the physical mechanisms of liver fibrosis and cirrhosis.


1. Introduction

The complex cellular microenvironment in which cells reside and survive is a dynamic system in vivo, and plays an essential role in cell morphology and function.1 Cells can respond to various environmental signals, which are categorized into biochemical cues or biophysical cues. These cues are mainly provided by the extracellular matrix (ECM), which acts as a cellular scaffold and exists as the primary extracellular component of tissues.2 The ECM is composed of proteins and polysaccharides with structural widths and lengths at the micro and nanometer scales, providing biophysical structures of regular configuration and biochemical support to the surrounding cells.3 The ECM is especially known for its close association with the physiological and pathological conditions in vivo, such as tumors and fibrosis.4,5

While the biochemical cues, such as small molecules, surrounding cells, and proteins have long been appreciated, attention has only recently been drawn to the biophysical cues, such as the mechanical properties,6 matrix elasticity7,8 and topography of the substrates.2,9–27 Among the biophysical cues, the substrate topography generates a variety of geometrically-defined, three-dimensional (3D) physical cues of micron and sub-micron scales; it is well known to influence cellular adhesion, spreading, proliferation and other functions via the interactions between cells and the substrate. The studies on cell response to substrate topography were mainly focused on the investigation of the cell morphology and function on various types of substrate topographies, including pillars,9,10 wells, grooves,11 protrusions12,13 and other anisotropic geometries.14 In particular, cell adhesion and the formation of cell morphology on the topographic substrate are the initial and primary steps for guiding cell spreading and other functions. For instance, the sizes of micro pillars, such as the aspect ratios and pitch were shown to affect cell morphology and spreading. While the cells would adhere on the top of isotropic micro patterns, of which the size is compatible with the cells,15 cell polarity and the direction of cell migration would be restricted on the anisotropic micro patterns, such as teardrop and ratchet.16,17 Furthermore, more evidences suggest that the topographies of micro- or nanoscales could promote and facilitate self-renewal and proliferation of stem cells.18 Some specific topography could also enhance and direct stem cell differentiation, such as neuronal differentiation of neural stem cells (NSCs),19,20 mesenchymal stem cells (MSCs)21,22 and embryonic stem cells (ESCs)23 on grooves with different aspect ratios, osteogenic differentiation of MSCs on nanoscale protrusions with a specially established dimension.24,25

Overall, cell morphology, spreading and other cellular functions largely depend on the cell type, the geometry and dimension of the substrate topography. However, only a few cell types and substrate topography have been studied to date. The influence of substrate topography on cell behaviors with respect to morphology and functions calls for further exemplification. More systematic studies on other cell types apart from stem cells, such as tissue cells need to be conducted to demonstrate the cell behaviors and its biological mechanism guiding cell response to substrate topography. Analysis of the cell responses to different topographical cues, over multiple temporal and spatial scales, is central to the understanding of various main biological functions.

In this study, the hepatic stellate cells (HSCs) that lie in the Disse's space between parenchymal cells and sinusoidal endothelial cells of the hepatic lobule have been considered. These cells in vivo were related to various kinds of liver disease and showed obvious size-dependent properties in ECM. Therefore, the individual HSC behaviors in response to different sizes of micropillar topography have been demonstrated. The results showed that the established topography could influence cell morphology and expression of protein related to cell epithelial–mesenchymal transition (EMT). In addition, as a simple physical modeling showed, the morphological response of cells to micropillar topography can be triggered by a minimum interfacial energy.

2. Materials and methods

2.1 Fabrication of micropillar substrate topography

Micropillar substrate topographies were fabricated on silicon wafers by photolithographic methods, the process flow of the fabrication for the patterned surface was showed in Fig. 1A. After UV exposure by contact aligner (SUSS Microtec MA6) and developing the pattern on the wafer, we exposed bare silicon by etching the oxide layer not covered by the pattern by STS AOE Etcher, then undergone deep reactive ion etching (Surface Technology Systems, ICP DRIE) to generate vertical walls. The photoresist layer had been removed by plasma cleaning process (PS210 Photo Resist Asher), and the remnant oxide layer has been removed by oxide etcher. Thereafter, the patterned samples had undergone piranha cleaning process to remove all contaminants.
image file: c5ra02084k-f1.tif
Fig. 1 Micro pillar silicon substrate fabrication and characterization. (A) The processes flow of micro pillar fabrication; (B) top view of the micro pillar substrate and 16 different micro pillar substrate groups; (C) the SEM images of micro pillars of different diameters and spacing used in the experiments, the x-axis indicates the diameter of the micro-pillars, and y-axis shows the side-to-side spacing between the adjacent micro-pillars.

2.2 Cell culture and EMT induction

A human hepatic stellate cell line, LX-2, was used in this study. The cells were maintained in Dulbecco's Modified Eagle's Medium with 4500 mg L−1 glucose (HG-DMEM), 10% fetal bovine serum (FBS), 100 U mL−1 penicillin, 100 μg mL−1 streptomycin at 37 °C in a humidified atmosphere, containing 95% air and 5% CO2. LX-2 cells were seeded on the micropillar and flat silicon substrate at a density of 1500 cells per cm2 and incubated for various periods (1 day for cell morphology and migration or 3 days for expression of protein related to cell EMT). In particular, for the cell EMT assay, the transforming growth factor-β1 (TGF-β1) as drug inducer was added in the culture medium with 10 ng ml−1. After cell adherence in a culture dish about 24 h, cells were exposed to the inducer medium for 48 h and then detected. The HG-DMEM, FBS, penicillin and streptomycin were purchased from GIBCO, Invitrogen. The TGF-β1 was obtained from R&D Systems, Minneapolis, MN, USA.

2.3 Cell fixation and staining

Expression of E-cadherin (E-cad) and α-smooth muscle actin (α-SMA) in LX-2 cells was performed by immunofluorescent assay. After cell treatment for 48 h, LX-2 cells on the micropillar and flat substrate were washed three times in PBS and fixed in 4% paraformaldehyde for 20 min at room temperature. For only α-SMA staining, an extra step, cells treated by 0.1% Triton X-100 was needed. After being washed by PBS, cells were blocked with goat serum for 1 h to decrease nonspecific hybridization. And then cells were incubated with anti-human E-cadherin or anti-human α-SMA primary antibody at a 1[thin space (1/6-em)]:[thin space (1/6-em)]100 dilution overnight, respectively. And next, cells were washed by PBS solution, and then incubated with the secondary antibody. The cell nucleus was stained by DAPI. After washing PBS sufficiently, the fluorescent images were obtained by the fluorescent microscope. F-actin for cell morphology was stained with Alexa Fluor 488 Phalloidin according to the reagent for manual operation. The primary antibodies were obtained from R&D Systems, Minneapolis, MN, USA. The secondary antibody was purchased from Sigma. The PBS, Triton X-100, DAPI and Alexa Fluor 488 Phalloidin were purchased from Life, Invitrogen.

2.4 Cell detection and assay

Cells were visualized using an Olympus fluorescence microscopy (Olympus IX 71, Japan). For immunofluorescence analysis, quantitation was performed by analyzing the area of the fluorescence using Image-Pro Plus 6.0 software (Media Cybematics, Silver Spring, MD, USA). Statistical analysis of the data was performed by using a Student's t-test.

2.5 Simulation of cell interfacial energy

The simulation model was constructed by the program Surface Evolver (Version 2.70, Kenneth Brakke, Mathematics Department, Susquehanna University, Selinsgrove, PA, USA), an interactive program for modelling liquid surfaces under various forces and constraints. It treats cells as liquid droplets spreading on micro patterned surfaces. We modeled the evolution of the given objects governed by minimization of energy according to the method in ref. 28. In Surface Evolver methods, geometric elements consisting vertices, edges, facets and bodies were used to build the model. The surface refers to all the geometric elements of the model entity set with boundaries, constraints and forces. The total energy of a surface resulting from the surface tension and gravitational force is which the Evolver minimizes.

3. Results and discussion

3.1 Characterization of micro-pillar substrate topography

Micro pillar areas of 1 cm2 were fabricated on silicon wafers of 400 μm by photolithographic methods, regular hexagonal arrays of circular micro pillars of 20 μm with high aspect ratios of 1[thin space (1/6-em)]:[thin space (1/6-em)]8, 1[thin space (1/6-em)]:[thin space (1/6-em)]4, 1[thin space (1/6-em)]:[thin space (1/6-em)]2 and 1[thin space (1/6-em)]:[thin space (1/6-em)]1 corresponding to the micro-post diameters of 2.5 μm, 5 μm, 10 μm and 20 μm respectively. Fig. 1A shows the process flow of the fabrication for the patterned surface. For easy reference, we used P(diameter,spacing) to denote the different micro pillar groups. For instance, P(20,2.5) refers to the pillar group of which the corresponding diameter and spacing are 20 μm and 2.5 μm. Fig. 1C shows the SEM images of the micropillar substrate topography.

3.2 Effects of micropillar topography on individual cell morphology

In this study, the attachment of LX-2 cells with a low concentration to ensure individual cell assay on micropillars, with flat substrate as the control were evaluated after seeding the cells for 24 h. LX-2 cells showed a good viability on the micro patterned substrate and the flat silicon substrate. More than 95% of cells lived for more than 3 days on both substrates. To analyze the cell morphology, the cell F-actin and nucleus were stained by phalloidin and DAPI, respectively. The fluorescence images are shown in Fig. 2A.
image file: c5ra02084k-f2.tif
Fig. 2 Individual LX-2 cell on the micro pillar substrate. (A) Fluorescence images of individual cell morphology. The illustration was cell F-actin and nucleus staining on flat substrate. Red: F-actin; blue: cell nucleus; bars = 20 μm. (B) Cell area of different micropillar group and flat substrate. ***: p < 0.005; (C) the areas and mean diameters of cell nucleus of P(5,10), P(5,5), P(2.5,10), P(2.5,5) and flat substrate. *: p < 0.05; n = 11.

We found that the cell morphology was closely related to the cell location, which was created by the diameter and spacing of micropillar. Generally, the size of the suspending mammalian cells was about 10–20 μm in diameter. So for the 20 μm spacing of micro-pillar, the individual cell could culture at the bottom of the gap between pillars [P(20,20) P(10,20) P(5,20) P(2.5,20)] or on the top of one pillar [P(20,20) P(10,20)]. For spacings of 10 μm and 5 μm, the cell location became complicated. The individual cell could either hang between the gap and adhere to several pillars [P(20,10) P(10,10) P(5,10) P(2.5,10) P(20,5) P(10,5) P(5,5) P(2.5,5)] or on the top of one single pillar [P(20,10) P(10,10) P(20,5) P(10,5)]. And with the spacing of 2.5 μm, the cell could adhere on the top of one pillar [P(20,2.5) P(10,2.5)] or several pillars [P(20,2.5) P(10,2.5) P(5,2.5) P(2.5,2.5)]. Overall, when the cell was on the top of one pillar, the cell shape adapted to the cross section of the micro pillar, i.e. circular with diameter similar to that of the pillar. On the other hand, when the cell was at the bottom of the gap between pillars, it could occupy the gap around the pillars. For larger pillars, the cell would be pushed out and the cell shape was abnormal [P(20,20) P(10,20)]. Otherwise, the cell shape was the same as that on the flat substrate [P(5,20) P(2.5,20)]. When the cell was hanging between several pillars, there were obvious changes in the cell shape. In P(5,10), P(5,5), P(2.5,10) and P(2.5,5) groups, the cell shape was thinner and straighter than others. But in P(20,10), P(20,5), P(10,10) and P(10,5) groups, there were no obvious rules to follow. For the cells that adhered to several pillars, it was shown that if the cell was on the pillars with a little subsidence [P(5,2.5) P(2.5,2.5)], the cell shrank. Otherwise, the cell shape was the same as on the flat substrate [P(20,2.5) P(10,2.5)].

In addition, the area of individual cell, area of cell nucleus and mean diameter were calculated. It was found that the area of the cells on the micro pillar substrate decreased substantially compared to the flat substrate (as shown in Fig. 2B). This result was similar to the reported responses of the human umbilical vein endothelial cells (HUVECs).29 Some of the cell morphologies also resembled 3D cell culture in gel, and this change suggested that the micro pillar substrate might generate an approximate 3D gel-free environment for the individual cell survival. Furthermore, the area and mean diameter of cell nucleus decreased only in four different micro pillar groups [P(5,10), P(5,5), P(2.5,10) and P(2.5,5)] compared to the flat substrate. The data are shown in Fig. 2C. In these micro pillar groups, the individual cell was thinner and straighter than it was on the flat substrate, and the shape of the cell nucleus also changed from round to elliptical, probably because the cell nucleus sat almost astride the narrow spacing between the pillars.

The “top cell”, refer to a cell that stays right on the top of a single pillar, these top cells are commonly found on micro-pillars of 20 μm in diameter. The number of top cells has been counted and compared to the other cells. The percentage of top cell reached 73% and reduced with the decrease of the spacing, the reason for such reduction may be due to the narrower spacing, which enabled the cell to adhere to on several pillars. More details are shown in Fig. 3. The shape of the top cell adapted to the circular micro pillar. The area of top cell was 351.0 ± 68.3 μm2 (n = 16) in P(20,20) group, this value was very close to 314.1 μm2, which was the area of the cross section of the micro pillar. The value of the area of top cell had a small standard deviation, and it showed that the cell shape was more uniform than the others, such as the cell on the flat substrate, with an area of 616.7 ± 220.2 μm2 (n = 16). This unique phenomenon suggested that the cell can modulate itself to adapt to the topography of the substrates.


image file: c5ra02084k-f3.tif
Fig. 3 Individual cell morphology on the top of one micro pillar. (A) The percentage of top cells in different micro pillar groups. (B) Fluorescence image of individual cell morphology in P(20,20) group. (C) Fluorescence image of individual cell morphology in P(20,2.5) group. Red: F-actin; blue: cell nucleus. Scale bar = 20 μm.

3.3 Simulation of individual cell on different substrates

The changes of individual cell topography on the micro pillar substrate might be related to the surface energy of cell. So in this study, the program Surface Evolver (Version 2.70) has been used to construct a simple cell model. The Surface Evolver can be applied to create surfaces and volumes, set energy boundary conditions and model the evolution of the given objects governed by minimization of surface energy. Cell models started as cuboids on substrate in this work. The cube was chosen as the starting configuration for simplicity and ease of simulation. The volume of the cuboid was 8000 μm3, equal to volume of a sphere with a diameter of 24.8 μm. This diameter was approximated to the diameter of normal suspending mammalian cells. In order to enhance the similarity between the cuboid and the cell, one solid sphere of 10 μm diameter was inserted into cuboid as a non-spreading cell nucleus. This solid sphere as a fixed constraint prevents the infinite extensive spreading of the droplet on the flat substrate, but has no relevance on the bulged droplet since it does not touch its surface on the substrates with different pillars.

By considering small area on or just next to one micro pillar, we apply the Young's equation:

 
γsl = γsvγlv(cos[thin space (1/6-em)]θ) (1)
where γsl is the solid–liquid interfacial energy, γsv is the solid–gas interfacial energy, γlv is the liquid–gas interfacial energy, θ is the Young's contact angle. In this simulation, the contact angle between the substrate and cuboid was set at 7°, and the contact angle between cuboid and the surrounding area was set at 180°. The air–solid tension was considered to be negligible compared to liquid–solid tension and liquid–air tension. The liquid–air tension was set to be 1 in the following work. After adding contact angle boundary conditions, the actual contact angle on the contact line was between 7° and 180°. These boundary conditions of the contact angle were the same as that in ref. 28. Then the water–solid and interfacial energy could be calculated and reached minimum when the system was at equilibrium.

Four different initial conditions have been simulated: individual cell on the flat substrate, individual cell on the top of one micro pillar, individual cell beside one pillar and individual cell between two micro pillars. All micropillars' diameters were 20 μm. Cells were simulated similarly to water droplets, being defined with an initial condition, incompressible volume, surface tension, contact angles between the different interfaces and an impenetrable solid sphere mimicking the nucleus. In our simulation, the size of nucleus and cell volume were considered as constants during cell spreading on the substrates. Different wet side constraints were added in the four models respectively.

Each iteration was considered to be an evolution step in this work. We initially refined the cubic with triangular mesh, and obtained these initial states in Fig. 4(A1–D1). Then underwent iterations until reaching its minimum energy state. Each iteration contains the three following steps: 1, calculation of the force of vertex as a function of position by the gradient of the surface energy, which directed the vertex motion. 2, moving the vertices by the force as consraints into the proper areas, where the constrains allowed. 3, realization of the actual motion by using a global interaction scale factor (Surface Evolver Manual Version 2.70: http://www.susqu.edu/brakke/evolver/downloads/manual270.pdf). The model was then refined the second time and underwent iterations until its final equilibrium configuration. At last, we got the equilibrium configuration we need as the cell morphology.


image file: c5ra02084k-f4.tif
Fig. 4 Simulation of individual cell on different substrates. (A1) Initial state of cell on the flat surface; (A2) the minimum surface energy state of cell on the flat surface; (B1) initial state of cell beside one pillar; (B2) the minimum surface energy state of cell beside one pillar; (C1) initial state of cell between two pillars; (C2) the minimum surface energy state of cell between two pillars; (D1) initial state of cell on top of one pillar; (D2) the minimum surface energy state of cell on top of one pillar.

By minimizing the energy, the cell model evolved until it was stable. The results are shown in Fig. 4(A2–D2). According to the simulation results, when the cell was on the flat substrate without wet side constraints, it flattened and adhered with a maximum area of adhesion at the minimum surface energy state. But when the micro pillar was introduced, the spreading of individual cell would be resisted and restricted, and the simulated surface area of cell was decreased. The simulated area of cell beside one pillar or cell between two micro pillars was reduced to 88% and 85%, respectively. This trend was similar to the experimental data. Notably, the top cell was also simulated by the same method of minimum surface energy. This simulation result matches well with the experimental data. The cell morphology was like a spherical crown with basal diameter similar to that of the pillar. The simulation demonstrated that the change of cell morphology was associated with the cell surface energy. The steady or equilibrium state of cell morphology was the minimum surface energy of the cell.

3.4 Effects of micropillar topography on cell protein expression

HSCs are the key mediator in progressive liver fibrosis and cirrhosis.30 The HSCs are dormant under normal conditions, but when the liver is injured, they become active and will generate EMT with decreasing expression of E-cadherin (E-cad) and increasing expression of α-smooth muscle actin (α-SMA). For EMT study, while the diameter and spacing of the micropillars were 5 μm and 2.5 μm [P(5,2.5)], the micropillar topography could induce significant changes in the expressions of E-cad and α-SMA compared with the flat substrate. In addition, TGF-β, a kind of chemical inducer for inducing EMT, was also used in the study as the positive control. The fluorescence images are shown in Fig. 5.
image file: c5ra02084k-f5.tif
Fig. 5 Fluorescence images of the expression of EMT-related proteins with different conditions. E-cad: E-cadherin (green); α-SMA: α-smooth muscle actin (green); cell nucleus was stained by DAPI (blue). Scale bar = 20 μm.

In physiological conditions, HSCs are located within the micro or sub-micro scale Disse's space, between the parenchymal cells and the sinusoidal endothelial cells of the hepatic lobule.31 The Disse's space, also called perisinusoidal space, contains the blood plasma and ECM. Some researchers considered that this space to be obliterated in liver disease, especially in liver fibrosis.5 Hepatic fibrosis was associated with an inflammatory response and deposition of ECM. Following liver injury, HSCs, the main ECM-producing cells, become active and generate EMT with change of cell phenotype and secretion of ECM. A large secretion of ECM would reduce the size of the Disse's space and would most likely further activate the other HSCs, so to aggravate fibrotic liver diseases and may even develop into cirrhosis. We can say that the size of the Disse's space plays an important role in HSCs activation. Notably, it was possible to change the physiological state of the HSCs, so to induce EMT. In our experiment, we found that the expressions of E-cad and α-SMA were changed by a particular size [P(5,2.5)] of the micro pillar, which might be compatible with the size of Disse's space in pathological conditions. In addition, we also found that the cell area of P(5,2.5) group was the smallest among all groups, because the cell was strictly restricted in the space with highest surface energy. This situation was probably similar to the cells in the Disse's space full of ECM. The study indicated that the size of established topography might be able to mimic the size of Disse's space in pathological conditions. However, the experimental data like EMT-related gene expression and western blotting is not readily available because of limited cell number in this study. The change of cell behaviors under this condition calls for further investigation.

4. Conclusions

By localizing the individual hepatic stellate cells in response to the different micropillar topographies, we demonstrated that the morphology of human hepatic stellate cells were greatly associated with the micro pillar topography. As the physical modeling showed, the morphological response of cells to micro pillar topography can be triggered by a minimum interfacial energy. Notably, the established topography with 2.5 μm spacing and 5 μm pillar diameter could affect the expression of E-cadherin and α-smooth muscle actin, and these proteins were closely related to EMT. This unique size might be compatible with the size of Disse's space in real pathological condition. The findings of this study are significant in understanding the mechanisms of liver fibrosis and have potential applications in tissue engineering and therapy.

Acknowledgements

This research was supported by the Special Fund for Agro-scientific Research in the Public Interest, Ministry of Agriculture of the People's Republic of China (no. 201303045), Joint Research Fund of NSFC-RGC (11161160552, N_HKUST601/11), the PhD Start-up Fund of Natural Science Foundation of Guangdong Province and Key Laboratory of Separation Science for Analytical Chemistry, Dalian Institute of Chemical Physics, Chinese Academy of Sciences.

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Footnote

This author contributed equally to this work and should be considered as co-first author.

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