http://orcid.org/0000-0002-9840-5908
Figures
Abstract
The complex morphologies observed in many biofilms play a critical role in the survival of these microbial communities. Recently, the formation of wrinkles has been the focus of many studies aimed at finding fundamental information on morphogenesis during development. While the underlying genetic mechanisms of wrinkling are not well-understood, recent discoveries have led to the counterintuitive idea that wrinkle formation is triggered by localized cell death. This work examines the hypothesis that the material properties of a biofilm both power and control wrinkle formation within biofilms in response to localized cell death. Using an agent-based model and a high-performance platform (Biocellion), we built a model that qualitatively reproduced wrinkle formation in biofilms due to cell death. Through the use of computational simulations, we determined important relationships between cellular level mechanical interactions and changes in colony morphology. These simulations were also used to identify significant cellular interactions that are required for wrinkle formation. These results are a first step towards more comprehensive models that, in combination with experimental observations, will improve our understanding of the morphological development of bacterial biofilms.
Citation: Aguilar B, Ghaffarizadeh A, Johnson CD, Podgorski GJ, Shmulevich I, Flann NS (2018) Cell death as a trigger for morphogenesis. PLoS ONE 13(3): e0191089. https://doi.org/10.1371/journal.pone.0191089
Editor: Kevin Burrage, Queensland University of Technology, AUSTRALIA
Received: October 23, 2017; Accepted: November 29, 2017; Published: March 22, 2018
Copyright: © 2018 Aguilar et al. This is an open access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
Data Availability: All relevant data are within the paper and its Supporting Information files.
Funding: This work was funded by a grant from the National Institute of Health (P50GM076547/Center for Systems Biology). The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.
Competing interests: The authors have declared that no competing interests exist.
Introduction
Bacteria live in almost every environment. While they are critical drivers of biogeochemical cycles and ecosystem dynamics, some bacteria are major threats to human health [1–3]. Bacterial cells can attach to a surface and form a multicellular aggregate, referred to as a biofilm, which increases their survival [1]. Biofilms protect bacteria from attack by the immune system and by antibiotics and are responsible for many infections caused by implanted medical devices [4]. One of the main reasons survival is improved in biofilms is due to their complex morphologies. How bacterial assemblies develop complex morphologies has been a question pursued by many scientists. Many researchers have recently focused on the formation of wrinkles in bacterial colonies because the analysis of wrinkle formation provides fundamental information on how structural patterns can develop [5–10].
Many bacterial colonies have a complex morphology characterized by an elaborate organization of connecting wrinkles (see Fig 1). It has been shown that these wrinkles participate in liquid transport within the colony by forming permeable channels connected in a radial network [11]. The liquid-filled channels can carry nutrients, waste, and signaling molecules. Importantly, in some bacterial colonies, such as those formed by Vibrio cholerae [12], the presence or absence of wrinkles distinguishes between virulent and benign states.
Figure adapted from Jers et al. [20].
Wrinkles can form in tissues through mechanical instabilities that are generated by constrained growth of tissues with specific elastic properties [13–16]. This physical mechanism has been suggested for the development of many wrinkled or undulated morphologies, such as the wrinkled morphology of the brain, tubular organs, and some biofilms [17–19]. A novel mechanism of wrinkle formation was revealed in a recent study by Asally et al. [9] which showed that localized cell death initiates wrinkle formation in Bacillus subtilis colonies. The abundant extracellular polymeric substance (EPS) produced by cells plays a critical role in wrinkle formation, underlying the formation of local regions of cell death and providing a mechanical support that resists compressive forces stemming from cell displacement driven by cell growth and cell division. Cell death disrupts the integrated network of cells and EPS within the biofilm, providing an outlet for compressive stress [9].
Complexly organized biofilms start from a single bacterium adhering to a surface. The bacterium secretes a glue-like protein that attaches it more tightly to the substratum. Upon division, the daughter cells are cemented together and to the substratum [8]. These cell-cell and cell-surface bonds, coupled with the pressure arising from population growth, push the expanding colony into a quasi-stable state in which unrelaxed forces are dampened by the rigid structure of biofilm. This rigid structure is formed by the EPS that wraps around the cells and provides the biofilm both mechanical support and resilience against environmental stresses [21–24]. Significantly, EPS production is essential for biofilm wrinkling [22, 25, 26].
A quasi-stable state is reached between 24 to 48 hours of biofilm development when the colony appears as a smooth, disk-like structure [9]. Continued growth leads to the formation of an intricate colony-wide pattern of cell death at the colony-substratum boundary in response to nutrient depletion, high cell density, and waste accumulation (see Fig 1 in Asally et al. [9]). In regions of cell death, the colony detaches from both, the substratum and surrounding cells, and the biomass converges to the areas opened by the dying cells. This leads to buckling of the colony into a complex pattern of interlocking wrinkles illustrated in Fig 1.
The focus of this study is on the transition from a smooth, stiff colony under compression to a complex wrinkled morphology triggered by localized cell death. This study does not consider the development of the smooth compressed colony or model how cell death patterns emerge, but begins with the initiation of realistic patterns of cell death at the colony-substratum interface.
We developed an agent-based model that considers cells and associated EPS as single agents to study the formation of 3D cellular structures that result from the interplay of cell death and biomechanical forces, and implemented this model using the Biocellion simulation framework [27]. Agent-based modeling is becoming a popular modeling framework to investigate the influence of mechanical properties on biological systems, including biofilms [28–32]. Agent-based approaches allow the integration of inter- and intra-cellular interactions and the exploration of cellular heterogeneity [33]. Our aims were to: a) test the hypothesis that cellular mechanical approaches allow the integration of intracellular interactions, b) explore how cellular interactions can both power and control wrinkle formation in biofilms in response to localized cell death, c) to learn how changes in mechanical properties of biofilms affect the structure of wrinkles, and d) to identify the intercellular interactions needed to form wrinkles.
Model description
To study mechanical effects on wrinkle formation, we developed an agent-based three dimensional model. Each agent is a sphere that represents a bacterial cell and a small amount EPS attached to the cell surface. The radius of an agent is αRi, where Ri is the radius of a bacterial cell, and α is a scaling factor (α > 1) that accounts for the space taken up by the mass of EPS that is attached to the cell wall (Fig 2B). Agents move in an overdamped environment in which viscous forces a have stronger effect than inertial forces. We used the equations of Brownian dynamics (BD) to model the dynamics of agents [33]. The velocity of an agent is the sum of two components: a term that is proportional to the net force acting on the agent [28], and a random term. In our implementation, the BD equations are integrated with the discrete time Euler-Maruyama scheme, so that the position xi of every cell i changes at every time step Δt according to:
(1)
where ζ is the coefficient of viscous friction, Dc is the diffusion coefficient of agents, and ξ(t) is a vector with components that are random numbers sampled from a normal distribution with zero mean and unit variance.
is the sum of all mechanical forces that act upon agent i, and depends on the current positions of the agents (x). We implemented two simple mechanical forces: those between pairs of agents and the forces between agents and the agar substratum:
(2)
The sum on the right hand side considers all agents j that are bonded to i. A bond is created between two agents when the distance between their centers becomes smaller than a threshold value δc. Similarly, a bond between two agents is broken when the distance between their centers becomes larger than δd. The force between bonded agents is described by the following equations:
(3)
(4)
where d is the distance between the centers of agents i and j. The bond between two agents, with the parameter K being the spring constant of the bonds, is an attractive force when the distance is greater than α(Ri + Rj) and a repulsive force when the distance is less than α(Ri + Rj). The attractive force between a pair of agents grows with distance until the bond breaks and the agents become unassociated. The stiffness of the bond between two agents is controlled by the parameter sb. As sb increases, the forces around the equilibrium point also increase to pull or push the cells back to the equilibrium point, more strongly enforcing the distance constraint (Fig 2D). With small sb, the distance constraint is lax and the agents are allowed to separate away from the equilibrium distance even when weak forces are applied (Fig 2D). The force between agents and the agar substrate is modeled similarly. The magnitude of the force is
, where xii = αRi − d. In this case, d is the distance of the center of agent i to the agar surface (Fig 2A). The direction of the force is perpendicular to the horizontal agar surface. A bond between a cell and agar surface is created if d is smaller than a threshold value δca, and the bond is broken if d becomes greater than δca.
Cartoon representation of cell/boundary (A) and cell/cell (B) elastic forces. Ri is the radius of cell i, α is the EPS shoving factor and d is the distance between the objects. (C) A representation of the initial configuration of cells and the parameters that define the size of the simulation system and the cell death pattern (Red). (D) Forces between two cells based on their distance for different values of sb(colors). The dashed lines indicate that the mechanical force for nonbonded cells is zero.
The initial configuration of the simulations represents the stiff colony before the onset of cell death and subsequent wrinkling. It consists of a set of agents randomly located in a rectangular box (Fig 2C). The initial positions of the cells filling the box with a specific value of volumetric density (Φ) are generated by the program SmolCrowd [9, 34]. To generate initial configurations of colonies in a compressed state, the values of Φ are selected such that average distance between agents is smaller than the rest length (2αRi). A subsequent small simulation with weak forces is applied to homogenize the arrangement of cells (see S1 Text in Supporting Information).
Cell death is modeled by removing the agents with centers located in the volumetric region of the cell death pattern (CDP) at the colony-substratum interface, depicted as a red rectangle in Fig 2C. In the following sections we will refer to agents that are composed of cells and local EPS simply as cells.
Results
Correlation of cell death and wrinkle location
To explore the hypothesis that the biomechanical forces unleashed by cell death are sufficient for forming wrinkles in biofilms, we simulated the morphogenesis of colonies that were initially configured in a compressed state that simulates cells fully encased in EPS. The mechanical support provided by the EPS is modeled by elastic bonds between adjacent cells. To model the effect of cell death, the network of bonds at the interface of the colony and the agar substratum is broken by removing cells from the system. As Fig 3 shows, the subsequent converging movements of the cells cause vertical buckling where cell death occurred. Fig 3 demonstrates our 3D simulation of this process where cell death (the green rectangle) disrupts the connection between the biofilm and the agar substratum, and perturbs the distribution of mechanical stress. The results of this simulation are in good agreement with in vivo observations that regions of cell death that occur at the interface between a bacterial colony and the agar medium presage areas where the colony later buckles (see Fig 4G of Asally et al. [9]). Spheres in Fig 3 represent cells that are colored according to pressure (red, for compression; blue, tension; see Methods for details about the computation of pressure). Cell death creates a heterogeneous distribution of compressive stress. A region of low stress appears at the top of the region of cell death and this induces convergent horizontal cell movement towards the center of the cell death region.
The figure shows a cross-sectional image of simulated wrinkle formation. Green indicates the area of cell death. Cells are colored by according to the mechanical stress they experience (red, compression; blue, tension). Please refer to Fig 4G of Asally et al. [9] for a comparison with wrinkle formation observed in a B. subtilis colony.
To track the movement of particles during wrinkle formation, we simulated the experimental setup of Asally et al. [9]. Fig 4 outlines the computational experiment. Starting with a block of cells under mechanical stress, we mapped the cell death pattern (CDP), as shown in Fig 4A, to the bottom layer of this block, then ablated the cells in the mapped area (Fig 4B). As expected, wrinkles form above the areas of cell death as shown in Fig 4C. We discretized the surface by overlaying a grid on the simulation domain and summing the trajectories of the particles in each square of the grid to compute the velocity vector for that partition (blue arrows in Fig 4E). These velocity vectors determine the convergence (negative divergence) of vector fields, demonstrating the aggregate material directional movement. The colored areas in Fig 4E show the convergence, where a more intense color corresponds to higher convergence, (see S1 Fig in Supporting Information for a larger figure). The observed convergence along with the velocity vectors confirm the idea that wrinkles can be formed by local cell death [8]. Fig 4F shows the spatial correlation between areas of cell death and wrinkles. Fig 4G demonstrates a more complex simulation that reproduces a “smiley face” that arises from a CDP similar to the one shown in Fig 4H of Asally et al. [9]. When the designed cell death pattern is incorporated in the simulations, a smiley face of wrinkles appears on top of the biofilm (bottom panel of Fig 4G).
A: Cell death pattern (CDP). B: CDP mapped to the bottom layer of a colony in which the cells are in a quasi stable state. The upper layer of the colony is not shown in this image. C: Relief of lateral mechanical stress at the CDP area gives rise to the wrinkles. D: Reconstructed surface of biofilm. E: Velocity vectors and convergence of vector fields computed from material movement. F: Spatial correlation of CDP (green) and wrinkles (red). G: “Smiley face” simulation: an artificially designed cell death pattern results in wrinkle formation in the simulation shown in the lower panel (Grey scale proportional to height).
Mechanical stiffness influences wrinkle height and width
Studies in material science have shown that geometrical features of wrinkles in thin films are greatly affected by the mechanical properties of the film [35, 36]. To investigate this effect in biofilms, we simulated three strains of Bacillus subtilis (wild type (WT), δarfB, and δsrfA) reported to form colonies with different degrees of stiffness due to the amount and composition of EPS that they produce [9]. Compared to wild type B. subtilis, δarfB generates a softer biofilm in which EPS production is repressed [37]. In contrast, δsrfA generates a stiffer biofilm in which EPS production is increased [38]. Assally et al. [9] observed that colony stiffness correlates with wrinkle size and that δsrfA strains have larger wrinkles than WT or δarfB. We tested whether our modeling approach could reproduce this observation.
In order to determine the mechanical stiffness of our simulated colonies, we performed uniaxial compression experiments, similar to the computational experiments described in Pathamatan et al. [39]. The simulation domain for these experiments was a rectangular region with Lx = 90, and Ly = Lz = 360μm. The agents were randomly located in the rectangular region with a volumetric density of 0.6. Before the compression experiments, the agents were subjected to an homogenization stage in which the system is simulated for 2000 steps to equilibrate the inter-cellular forces (see S1 Text of the Supporting Information for details of homogenization stage). The compression experiments were performed with periodic boundary conditions in the x direction, an impenetrable wall at y = 0; and no restriction on the z direction. The cells located at the border (those that overlap with the plane y = Ly) are displaced a small distance, ΔL, in the −y direction. The system is then allowed to evolve according to the equations of motion (Eq 1). During the simulation the y coordinates of the border cells are fixed. The biofilm segment is simulated until vmax < 0.01μms−1, where vmax is the maximum velocity of the cells. At the end of the simulation, the force on the compressed surface is computed as the sum of the forces in the y direction of all border cells. Stress is then estimated by dividing the average force by the number of cells located at the border. The experiment is repeated with cells located at the border subjected to an additional displacement ΔL. Fig 5A and 5B show the stress-strain curves obtained by the computational experiments for different parameters that modulate colony stiffness. Stiffness is characterized by the slope of the curve at the initial (linear) part of the stress-strain experiments; stiffness increases with the slope of the stress-strain curve.
We used three values of bond flexibility (sb values in color) and two values of K (K = 20.0 in panel A, and K = 2.0 in panel B). C: Top view of the colonies at the end of the simulation of colonies perturbed by cell death, for K = 2.0. Color indicates the height, red for higher values and blue for lower values. For this simulation, we used WD = 1000 and the parameter values specified in S1 Table of the Supporting information.
Within our modeling framework, there are two parameters that can potentially modulate the colony stiffness: bond flexibility (sb) and the spring constant (K). Fig 5A and 5B shows the stress-strain curves of the compression experiment for two values of K (20.0 and 2.0) and three values of sb (1.00, 0.1, and 0.01). Fig 5C shows a top view at the end of simulated wrinkle formation due to cell death for each of the three values of sb and K = 2.0. The plots show that, for a constant value of K, sb determines colony stiffness, i.e. the slope of the stress-strain curve in the linear regime. For a high value of K (Fig 5A), even though the colonies have different stiffnesses, they behave similarly. An initial linear regime is followed by a plastic region in which the stress becomes almost constant, a trend that characterizes a material that has the capacity to store energy due to compression. For a low value of K (Fig 5B), we observe two distinct material behaviors. Colonies with sb = 1.00 and sb = 0.10 behave similarly to those shown in Fig 5A. A distinct behavior is observed for sb = 0.01 in which the stress response constantly increases with strain. Notably, this is the only case in which no wrinkle is formed when there is cell death (Fig 5C). Simulations of wrinkle formation due to cell death show that colony stiffness affects the morphology of wrinkles. Stiffer colonies (with higher sb) form wider and higher wrinkles (see Fig 5C). This is in good agreement with experiments performed with mutant strains that form colonies with lower and higher stiffness than wild type.
To analyze in more detail how the colony stiffness affects the morphology of wrinkles, we performed simulations of wrinkle formation induced by cell death for sb = 0.01, 0.08, and 1.00, Φ = 0.16, and a set of cell death widths (WD = 50, 100, …, 1000). All other parameters were set according to S1 Table of the Supporting Information. For each pair of WD and sb, we performed 6 simulations corresponding to different initial distributions of cells. The relationships between cell death area (WD) and wrinkle height and area are shown in Fig 6A and 6B, respectively, for three different values of colony stiffness (sb). Wrinkles generated by sb = 1.00 are higher than those generated by sb = 0.08 and 0.01, for all values of WD except WD = 750μm. The difference in wrinkle height and area is more noticeable for larger areas of cells death (WD > 750) in which average wrinkle height and area are always larger for greater values of colony stiffness sb. These results are in good agreement with experimental observations in which colonies with higher stiffness (mutant δsrfA) generate larger wrinkles than colonies with lower stiffness (WT and δarfB strain).
A. Colony height versus the width of the cell death region (WD) for three values of colony stiffness (sb). B. Wrinkle area versus WD for three values of sb. Every point represents the average of 6 simulations with random initial positions and the bars indicate standard deviations.
In Fig 6A, we observe three local maxima of wrinkle height which are associated with different wrinkle morphologies. Higher wrinkles and different morphologies are observed for smaller heights of the cell death region (smaller values of HD), which produce smaller volumes of cell death. Fig 7 compares wrinkle heights obtained from different values of HD and colony stiffness. For HD = 27μm and sb = 1.00 there are three wrinkle height local maxima. A tall wrinkle is formed at WD = 150. This wrinkle almost disappears if HD is increased to 36 or if sb is decreased to 0.08. Wrinkle height also peaks at WD = 350 and 750. The morphology of these wrinkles is shown in Fig 8C. This pattern resembles the morphology observed in side views of wrinkles of bacterial colonies (see Fig 4G of Asally et al. [9]). Fig 7 also shows that reducing the volume of the cell death region by changing HD from 36 to 27 μm generates higher wrinkles. This non-intuitive observation may be explained by considering that a smaller volume of cell death leaves a greater biomass in the biofilm to be accommodated after cell death.
A: Ratio of central to lateral height of simulated colonies for several values of initial volumetric density (Φ) and width (WD) of the cell death pattern (CDP). The white dashed lines highlight a region in which cell death does not induce wrinkle formation. B: Representative side views at the end of simulations for different values of WD, sb and HD. The color intensities represent computed mechanical stress (see Fig 3). WD units are in micrometers.
Determinants of wrinkle formation by parameter exploration
One of our goals is to use modeling to identify parameters that are critical for biofilm morphogenesis that can be later tested in experimental settings. Here, we used the model to determine the sensitivity of wrinkle formation to different parameters. Our strategy was to systematically change the value of one or two parameters in the simulation while keeping the other parameters constant. These simulations were performed in a rectangular group of cells with varying regions of cell death located at the center of the simulation domain (Fig 2C).
First we explored a range of cell death widths (WD = 50, 100, 150, …, 1000) and volumetric densities (Φ = 0.12, 0.14, 0.16, 0.18) to identify parametric regions that allow colonies to form wrinkles. For each combination of WD and Φ, a set of 3 simulations, corresponding to different initial positions of cells, was performed with stiffness parameters sb = sba = 0.08, Dc = 0 (no cellular motility), and the additional parameters specified in S1 Table of the Supporting material. Fig 8A shows a heatmap of the ratio of height at the center of a colony to the height at the border of a colony (central height to lateral height ratio in Fig 8A, rh) at the end of the simulations. The procedure used to compute the height of the colony at the border (y = 0) and the center (y = Ly/2) is described in the Methods section. A value of rh = 1 (blue) indicates that the height of the center and the border are equal, i.e., no wrinkle had formed. Values close to 2 (yellow) indicate that one or two wrinkles had formed in the center of the colony. The lower left part of the heatmap of Fig 8A shows a parametric region of WD and Φ in which no wrinkles form. These results suggest that for relatively small volumetric densities, wrinkles do not form if the region of cell death is small. We visually inspected the morphologies at the end of the simulations used to obtain the heatmap of Fig 8; representative side views are shown in Fig 8B. These snapshots suggest that the size of the cell death region determines the final morphology of the wrinkles. Specifically, the number of wrinkles that form at the top of the cell death region depends on its width. This observation is in good agreement with observations of bacterial colonies in which larger regions of cell death generate two parallel wrinkles while relatively small regions of cell death generate a single wrinkle [9].
The effect of the adhesive forces on colony morphology was investigated by individually turning off agent-agent and agent-substratum adhesion. First, we turned off only adhesive interactions between agents and the agar surface, i.e., sba = 0 when the distance between the center of a cell and the agar surface is larger than αRi. The remaining parameters were at the values specified in the first part of this section. Fig 9A shows side views of colonies at the end of the simulations for different sizes of the cell death region and Φ = 0.16; other values of Φ generate similar morphologies. These results suggest that a loss of cell agar surface adhesion does not block the formation of wrinkles. However, surface adhesion does have a great impact on colony morphology as observed in Fig 9A. A loss of adhesive bonds to the agar surface reduces stability, allowing cells to reaccommodate in ways that generate morphologies substantially different from those of actual bacterial colonies. We also turned off the adhesive interaction between cells, i.e. sb = 0 when the distance between two cells is larger than α(Ri + Rj). The remaining parameters were fixed identically to the previous experiment. Fig 9B shows a side view of the colony at the end of the simulations for WD = 600, other values of WD produced similar morphologies. In agreement with previous observations [9], these results confirm that cell-cell adhesion is essential for the formation of wrinkled morphologies.
A: Final morphologies from simulation in which only the adhesive interactions between cells and the agar surface are turned off. B: Final morphology (WD = 600) obtained from simulations in which cell-cell adhesive interactions are turned off. In all cases in panels A and B, a volumetric density of Φ = 0.16 was used.
Discussion
To form a multicellular aggregate, such as a biofilm, cells interact via a complex interplay between biochemical signaling and biomechanical forces. However, these interactions are still poorly understood. Investigating the morphogenesis of model biological systems, such as biofilms, is important for understanding and formalizing the common patterns seen in more complex systems and organisms. Recent studies showed that cell death triggered by biochemical stress combined with a relaxation phase of biomechanical stress, plays a critical role in the initiation of wrinkles in biofilms.
We developed an agent-based model to evaluate the effect of cellular level mechanical interactions on wrinkle formation due to cell death. We modeled mechanical interactions through the implementation of elastic bonds between pairs of agents and also between agents and the agar surface. In this model, an agent is a cell and the surrounding EPS. Cell death was modeled by removing agents from the system. Because instantaneous deletion of cells may be a more drastic perturbation than encountered in biological systems, we have also performed simulations in which cells are gradually removed from the system. We found that abrupt or gradual removal of cells produced the same final results (see S1 Text in Supporting Information). By implementing the cellular processes of mechanical interactions and cell death, we were able to qualitatively recapitulate the process of wrinkle formation that are observed in colonies of Bacillus subtilis [9]. Although this simple model performed well, a more complete model would include other cellular events, such as cell density change due to cell division, cell motility, the effect of waste molecules and nutrients, and heterogeneity of EPS production.
We first aimed to investigate the role of bond stiffness on wrinkle morphology. We found that bond stiffness is the major modulator of colony stiffness. By changing the bond stiffness, we simulated colonies with distinct mechanical behaviors. Colonies that generate wrinkles when perturbed by cell death have a mechanical behavior characterized by a linear elastic regime followed by plastic-like behavior. Colonies without plastic-like behavior did not form wrinkles after cell death. Moreover, colonies simulated with higher stiffness generated wider and higher wrinkles, in good agreement with observations of bacterial colonies [9]. In the simulations, the relationship between wrinkle height and stiffness is more pronounced for wider cell death regions. Furthermore, decreasing the height of the cell death region resulted in larger wrinkles, even when cell death regions are relatively small. This non-intuitive result suggests a complex interplay between the geometry and volume of the cell death region and wrinkle morphology. In actual biofilms, it is likely that the volume of cell death regions is influenced by colony stiffness, which will require a model that relates cell death to mechanical stress.
We performed simulations that correspond to different sets of parameters that characterize our model. This approach helped us identify properties beside mechanical stiffness that determine wrinkle formation. Our results suggest that small cell death regions are less likely to trigger wrinkles in colonies with low cell densities. Moreover, the size of cell death regions determines the morphology of the wrinkles; large cell death regions produce multiple wrinkles with specific wavelengths, whereas smaller cell death regions generate a single wrinkle on top of the region of cell death. Our results also show that cell-cell adhesion is essential for wrinkle formation. However, while cell adhesion to the agar substratum influences colony morphology, its suppression does not completely prevent the formation of wrinkles.
The wrinkle formation simulated in this study represents one specific morphological feature of the whole colony. Future work will include expanding the current simulation to a larger spatial scale, including other biological events such as cell division, the effects of nutrients and waste molecules, as well as intracellular gene regulatory networks that modulate the primary determinants of wrinkling, cell adhesion and cell death.
Methods
Agent based framework
We implemented the wrinkle formation model (see Model description) in Biocellion, an HPC simulation framework designed to accelerate agent-based simulations of biological systems composed of millions to billions of cells. Biocellion, which runs on clusters and has been tested in a cloud computing environment, is already capable of producing high-fidelity simulation data for living cell system models having billions of cells, such as yeast patterning, bacterial colonies on soil aggregate, and cell sorting [27, 40]. The code of our implementation of the model is freely available with a set of inputs that were used to simulate the process of wrinkle formation.
Convergence computation
In vector calculus, convergence (negative divergence) is a vector operator that represents the volume density of inward flux of a vector field around a given point. As mentioned in the main text, we partition the xy plane into a set of mesh cells using a Cartesian mesh. For each particle we track the movement and compute the displacement vector. We compute the convergence at a particular mesh cell by subtracting the number of particles that enters that mesh cell from the number of particles that left.
Vector field
In vector calculus, a vector field is an assignment of each point with a velocity vector. The velocity vector for each voxel is computed as the aggregation of all displacement vectors of particles which were initially located in that voxel.
Computation domain
In simulations of wrinkle formation, we set up periodic boundary conditions in the y and z directions and rigid walls in the x direction. x = 0 represents the agar surface that supports the colony. For the simulation shown in Fig 3 we used dimensions of Lx = 90, Ly = 1440, and Lz = 360 micrometers and a volumetric density of Φ = 0.16. In Fig 4G we used approximately 800,000 cells structured in a 90 × 4500 × 3600 micrometer block, and a 200 × 9600 × 3500 micrometer block in the experiment of Fig 4C. The generation of cells within the computation domain with each volumetric density (Φ) is described in S1 Text of the Supporting Information.
Computation of mechanical stresses
In our agent based model, individual cells are explicitly included, allowing the modeling of mechanical interactions. In particular, the mechanical forces in a given spatial configuration of cells provide important information about the spatial distribution of mechanical stresses in the interior of the colony. The local stress tensor at cell i of a colony in a given configuration is [33, 41]:
(5)
where Vi is the volume of each spherical agent, fij is the force acting on agent i due to agent j, and rij is the position of the center of cell j relative to the center of cell i. Similarly to Fenley et al. [41], we compute the hydrostatic stress for visualization of figures in the main text:
(6)
where
is a scalar value that can be visualized for each cell. In the main text,
is referred to as the mechanical stress that a cell supports due to mechanical interactions.
Colony height
To compute colony height (H), we divide the simulation domain into regular voxels of 20 × 20 × 20μm. Each voxel is determined by three indices (i, j, k), which represent its position in the x, y, and z directions, respectively. For every voxel we compute the average height of the cells located in that voxel:
(7)
where Ni,j,k is the number of cells located in voxel (i, j, k), and
is the height (x coordinate) of cell l located in the voxel. The height of the colony is then computed as:
(8)
The height of the border of the colony is computed as Hj=0 = maxi,k(H(i,0,k)), and the height of the center of the colony is Hj=72 = maxi,k(H(i,72,k)) for the system in which Lx = 1440μm. These values are used to compute the border to center height ratio (rh) used in Fig 8A.
Wrinkle area
To estimate the wrinkle area at the end of a simulation (Fig 6B), we divide the simulation domain into regular 20 × 20 × 20μm voxels, and compute the maximum height in the x direction, hx(j, k) = maxi H(j, k). The matrix hx(j, k) is then mapped into a binary image using a threshold value of 1.3Hj=0, where Hj=0 is the height of the border of the colony. Other threshold values generated a similar trend than the one shown in Fig 6B. Finally, the wrinkle area is computed as the maximum area of the connected components of the binary image.
Supporting information
S1 Fig. Vector field and convergence for biofilm surface, demonstrating the aggregate material directional movement.
https://doi.org/10.1371/journal.pone.0191089.s001
(TIFF)
S1 Table. Parameters, constants, and expressions used in the simulations.
https://doi.org/10.1371/journal.pone.0191089.s002
(PDF)
S1 Text. Supplementary information for “Cell death as a trigger for morphogenesis”.
https://doi.org/10.1371/journal.pone.0191089.s003
(PDF)
References
- 1. Donlan RM, Costerton JW. Biofilms: survival mechanisms of clinically relevant microorganisms. Clinical Microbiology Reviews. 2002;15(2):167–193. pmid:11932229
- 2. Hunter P. The mob response. EMBO Reports. 2008;9(4):314–317. pmid:18379581
- 3. Edlund A, Yang Y, Hall AP, Guo L, Lux R, He X, et al. An in vitrobiofilm model system maintaining a highly reproducible species and metabolic diversity approaching that of the human oral microbiome. Microbiome. 2013;1(1):25. pmid:24451062
- 4. Costerton J, Montanaro L, Arciola C. Biofilm in implant infections: its production and regulation. The International Journal of Artificial Organs. 2005;28(11):1062–1068. pmid:16353112
- 5. Haussler S, Fuqua C. Biofilms 2012: new discoveries and significant wrinkles in a dynamic field. Journal of Bacteriology. 2013;195(13):2947–2958. pmid:23625847
- 6. Dietrich LEP, Okegbe C, Price-Whelan A, Sakhtah H, Hunter RC, Newman DK. Bacterial community morphogenesis is intimately linked to the intracellular redox state. Journal of Bacteriology. 2013;195(7):1371–1380. pmid:23292774
- 7. Payne S, Li B, Cao Y, Schaeffer D, Ryser MD, You L. Temporal control of self-organized pattern formation without morphogen gradients in bacteria. Molecular Systems Biology. 2013;9(1).
- 8. Schultz D, Onuchic JN, Ben-Jacob E. Turning death into creative force during biofilm engineering. Proceedings of the National Academy of Sciences. 2012;109(46):18633–18634.
- 9. Asally M, Kittisopikul M, Rué P, Du Y, Hu Z, Çağatay T, et al. Localized cell death focuses mechanical forces during 3D patterning in a biofilm. Proceedings of the National Academy of Sciences. 2012;109(46):18891–18896.
- 10. DePas WH, Hufnagel DA, Lee JS, Blanco LP, Bernstein HC, Fisher ST, et al. Iron induces bimodal population development by Escherichia coli. Proceedings of the National Academy of Sciences. 2013;110(7):2629–2634.
- 11. Wilking JN, Zaburdaev V, De Volder M, Losick R, Brenner MP, Weitz DA. Liquid transport facilitated by channels in Bacillus subtilis biofilms. Proceedings of the National Academy of Sciences. 2013;110(3):848–852.
- 12. Teschler JK, Zamorano-Sánchez D, Utada AS, Warner CJ, Wong GC, Linington RG, et al. Living in the matrix: assembly and control of Vibrio cholerae biofilms. Nature Reviews Microbiology. 2015;13(5):255. pmid:25895940
- 13. Li B, Cao YP, Feng XQ, Gao H. Mechanics of morphological instabilities and surface wrinkling in soft materials: a review. Soft Matter. 2012;8(21):5728–5745.
- 14. Rodriguez EK, Hoger A, McCulloch AD. Stress-dependent finite growth in soft elastic tissues. Journal of Biomechanics. 1994;27(4):455–467. pmid:8188726
- 15. Dervaux J, Ben Amar M. Morphogenesis of growing soft tissues. Phys Rev Lett. 2008;101:068101. pmid:18764507
- 16. Dervaux J, Ciarletta P, Amar MB. Morphogenesis of thin hyperelastic plates: A constitutive theory of biological growth in the Föppl–von Kármán limit. Journal of the Mechanics and Physics of Solids. 2009;57(3):458–471.
- 17. Tallinen T, Chung JY, Rousseau F, Girard N, Lefèvre J, Mahadevan L. On the growth and form of cortical convolutions. Nature Physics. 2016;12(6):588–593.
- 18. Li B, Cao YP, Feng XQ, Gao H. Surface wrinkling of mucosa induced by volumetric growth: theory, simulation and experiment. Journal of the Mechanics and Physics of Solids. 2011;59(4):758–774.
- 19. Trejo M, Douarche C, Bailleux V, Poulard C, Mariot S, Regeard C, et al. Elasticity and wrinkled morphology of Bacillus subtilis pellicles. Proceedings of the National Academy of Sciences. 2013;110(6):2011–2016.
- 20. Jers C, Kobir A, Søndergaard EO, Jensen PR, Mijakovic I. Bacillus subtilis two-component system sensory kinase DegS is regulated by serine phosphorylation in its input domain. PLoS One. 2011;6(2):e14653. pmid:21304896
- 21. Webb JS, Givskov M, Kjelleberg S. Bacterial biofilms: prokaryotic adventures in multicellularity. Current Opinion in Microbiology. 2003;6(6):578–585. pmid:14662353
- 22. Kearns DB, Chu F, Branda SS, Kolter R, Losick R. A master regulator for biofilm formation by Bacillus subtilis. Molecular Microbiology. 2005;55(3):739–749. pmid:15661000
- 23. Flemming Hans-Curt WJ. The biofilm matrix. Nature Reviews Microbiology. 2010;8(9):623–633. pmid:20676145
- 24. Marvasi M, Visscher PT, Casillas Martinez L. Exopolymeric substances (EPS) from Bacillus subtilis: polymers and genes encoding their synthesis. FEMS Microbiology Letters. 2010;313(1):1–9. pmid:20735481
- 25. Branda SS, González-Pastor JE, Ben-Yehuda S, Losick R, Kolter R. Fruiting body formation by Bacillus subtilis. Proceedings of the National Academy of Sciences. 2001;98(20):11621–11626.
- 26. Romero D, Aguilar C, Losick R, Kolter R. Amyloid fibers provide structural integrity to Bacillus subtilis biofilms. Proceedings of the National Academy of Sciences. 2010;107(5):2230–2234.
- 27. Kang S, Kahan S, McDermott J, Flann N, Shmulevich I. Biocellion: accelerating computer simulation of multicellular biological system models. Bioinformatics. 2014;30(21):3101–3108. pmid:25064572
- 28. Ghosh P, Mondal J, Ben-Jacob E, Levine H. Mechanically-driven phase separation in a growing bacterial colony. Proceedings of the National Academy of Sciences. 2015;112(17):E2166–E2173.
- 29. Yan J, Sharo AG, Stone HA, Wingreen NS, Bassler BL. Vibrio cholerae biofilm growth program and architecture revealed by single-cell live imaging. Proceedings of the National Academy of Sciences. 2016;113(36):E5337–E5343.
- 30. Smith WP, Davit Y, Osborne JM, Kim W, Foster KR, Pitt-Francis JM. Cell morphology drives spatial patterning in microbial communities. Proceedings of the National Academy of Sciences. 2017;114(3):E280–E286.
- 31. Zachreson C, Wolff C, Whitchurch CB, Toth M. Emergent pattern formation in an interstitial biofilm. Physical Review E. 2017;95(1):012408. pmid:28208370
- 32. Gelimson A, Zhao K, Lee CK, Kranz WT, Wong GC, Golestanian R. Multicellular self-organization of P. aeruginosa due to interactions with secreted trails. Physical Review Letters. 2016;117(17):178102. pmid:27824438
- 33. Van Liedekerke P, Palm MM, Jagiella N, Drasdo D. Simulating tissue mechanics with agent-based models: concepts, perspectives and some novel results. Computational Particle Mechanics. 2015;2(4):401–444.
- 34. Andrews SS, Addy NJ, Brent R, Arkin AP. Detailed simulations of cell biology with Smoldyn 2.1. PLOS Computational Biology. 2010;6(3):1–10.
- 35. Huang R, Im SH. Dynamics of wrinkle growth and coarsening in stressed thin films. Physical Review E. 2006;74:026214.
- 36. Cerda E, Mahadevan L. Geometry and physics of wrinkling. Physical Review Letters. 2003;90:074302. pmid:12633231
- 37. Hamon MA, Stanley NR, Britton RA, Grossman AD, Lazazzera BA. Identification of AbrB-regulated genes involved in biofilm formation by Bacillus subtilis. Molecular Microbiology. 2004;52(3):847–860. pmid:15101989
- 38. Camp AH, Losick R. A feeding tube model for activation of a cell-specific transcription factor during sporulation in Bacillus subtilis. Genes & Development. 2009;23(8):1014–1024.
- 39. Pathmanathan P, Cooper J, Fletcher A, Mirams G, Murray P, Osborne J, et al. A computational study of discrete mechanical tissue models. Physical Biology. 2009;6(3):036001. pmid:19369704
- 40.
Kang S, Kahan S, Momeni B. In: Sun L, Shou W, editors. Simulating Microbial Community Patterning Using Biocellion. New York, NY: Springer New York; 2014. p. 233–253.
- 41. Fenley AT, Muddana HS, Gilson MK. Calculation and visualization of atomistic mechanical stresses in nanomaterials and biomolecules. PLOS ONE. 2014;9(12):1–18.