Multiscale computational analysis of Xenopus laevis morphogenesis reveals key insights of systems-level behavior
© Robertson et al; licensee BioMed Central Ltd. 2007
Received: 02 July 2007
Accepted: 22 October 2007
Published: 22 October 2007
Tissue morphogenesis is a complex process whereby tissue structures self-assemble by the aggregate behaviors of independently acting cells responding to both intracellular and extracellular cues in their environment. During embryonic development, morphogenesis is particularly important for organizing cells into tissues, and although key regulatory events of this process are well studied in isolation, a number of important systems-level questions remain unanswered. This is due, in part, to a lack of integrative tools that enable the coupling of biological phenomena across spatial and temporal scales. Here, we present a new computational framework that integrates intracellular signaling information with multi-cell behaviors in the context of a spatially heterogeneous tissue environment.
We have developed a computational simulation of mesendoderm migration in the Xenopus laevis explant model, which is a well studied biological model of tissue morphogenesis that recapitulates many features of this process during development in humans. The simulation couples, via a JAVA interface, an ordinary differential equation-based mass action kinetics model to compute intracellular Wnt/β-catenin signaling with an agent-based model of mesendoderm migration across a fibronectin extracellular matrix substrate. The emergent cell behaviors in the simulation suggest the following properties of the system: maintaining the integrity of cell-to-cell contact signals is necessary for preventing fractionation of cells as they move, contact with the Fn substrate and the existence of a Fn gradient provides an extracellular feedback loop that governs migration speed, the incorporation of polarity signals is required for cells to migrate in the same direction, and a delicate balance of integrin and cadherin interactions is needed to reproduce experimentally observed migratory behaviors.
Our computational framework couples two different spatial scales in biology: intracellular with multicellular. In our simulation, events at one scale have quantitative and dynamic impact on events at the other scale. This integration enables the testing and identification of key systems-level hypotheses regarding how signaling proteins affect overall tissue-level behavior during morphogenesis in an experimentally verifiable system. Applications of this approach extend to the study of tissue patterning processes that occur during adulthood and disease, such as tumorgenesis and atherogenesis.
Tissue morphogenesis is a complex biological process that includes the coordinated movements of multiple cells arranging and rearranging in space and time in order to give rise to biological form or structure. Morphogenic processes underpin tissue generation, degeneration, and regeneration during both embryogenesis and adulthood. Understanding the fundamental regulatory mechanisms of tissue morphogenesis has implications for a large array of biological problems, ranging from congenital heart disease  to tumorgenesis . Important information about the intracellular signaling processes and cell behaviors underlying morphogenic processes has been amassed in recent decades from reductionist experimental approaches , and many of these are currently understood in isolation [4, 5]. However, significant questions regarding how cohorts of intra- and intercellular signals orchestrate tissue-level patterning events during morphogenesis remain unanswered because we currently lack the tools needed to understand the translation of biological phenomena across different levels of spatial and temporal scales. The systems-level biology involved in directing cell and tissue rearrangements leading to changes in form has yet to be adequately coupled to mechanisms across length and time scales. This coupling requires the development of new computational approaches and the systematic pairing of these new approaches with cutting-edge experimental studies in model systems that are informative yet tractable.
This paper focuses on modeling a morphogenic process in Xenopus laevis, a process that is complex enough to warrant a systems-level approach whose outcome can be highly informative, but one that is simple enough to facilitate a range of targeted experimental manipulations, while still being computationally tractable. Understanding tissue morphogenesis in the Xenopus laevis model system is of significant value because the relevant signaling networks and cell behaviors are recapitulated in a number of mammalian developmental and growth processes, such as angiogenesis, wound healing, and tumor growth [6–8]. We have taken a multiscale computational approach for achieving a better understanding of the dynamic interplay between the spatially heterogeneous molecular signals and cellular responses that direct tissue patterning. Our simulation couples a mass action kinetics model of an intracellular signaling pathway, Wnt/β-catenin, with an agent-based model (ABM) of multicell migration and extracellular matrix assembly/degradation to study the process of mesendoderm migration in Xenopus laevis.
Multiscale computational analysis will inform the field of developmental biology by providing a framework to integrate existing data and to systematically generate and test novel hypotheses to drive experimental design. There are several key remaining challenges to multiscale, systems-level reconstruction and analysis of signaling networks, including: (1) there is a significant lack of intracellular reconstructions for networks implicated in multicellular systems; (2) there is a lack of multicellular models of vertebrate development that capture spatial and temporal heterogeneities in cell phenotype, cell behavior, and tissue environment; (3) there is a need for a computational framework that can integrate across the spatial and temporal scales critical for modeling tissue patterning processes, and determining the computational requirements for obtaining meaningful data across length and time scales is uncharted territory; and (4) rigorous methods for simplifying biological complexities need to be developed and validated, as do routines for setting appropriate boundary conditions in multiscale models. The modeling framework and results presented herein in part address each of these challenges.
Two specific objectives were identified as critical to this modeling effort: (1) the establishment of a computational interface between the two modeling scales (intracellular and multicellular), and (2) a modeling structure that is intuitive and compartmentalizes functionality such that a foundation is provided for future integration of additional intracellular signaling pathways and multicellular behaviors. Consequently, the computational program was organized into sub-functions so additional features could be added without substantially modifying the computer programming code. We present the continuum-based intracellular model and discrete multicellular model separately in the Materials and Methods section. The coupling interface for these two models and its validation is described in the Results section.
Results and discussion
The development of the multiscale model and associated analyses are summarized below. The intracellular and multicellular models were individually validated to ensure their functionality before combining them into the multiscale model.
Multi-cellular system model: mesendoderm migration
Modeling sub-cellular compartments as "agents"
In a traditional biological ABM, each biological cell is represented by a single agent [12–15]. However, in this ABM each biological cell was segmented into nine sub-compartments, and each sub-compartment was modeled as a square agent (Figure 2). This sub-cellular resolution enabled different portions of a single cell (e.g. leading edge vs. trailing edge) to respond to different integrin, cadherin, and Fn concentrations. The eight agents that comprise the interfacing regions of the cell (i.e. the outer edges of the cell that are in direct physical contact with neighboring cells) can respond to eight stimuli (left, right, forward, backward, or combinations thereof). The center agent can respond to stimuli without interacting with another agent as well as serve as the "summation" of the stimuli surrounding it. Moreover, the maintenance of cell polarity is important in mesendoderm morphogenesis, and the leading edge of a cell may have experienced a different environment (e.g. cell-cell contact or cell-Fn contact) than the trailing edge of a cell, and these spatial differences would impact the overall behavior of the cell.
Despite the ability to possess different attributes and experience different spatial environments, the sub-cellular agents of a single simulated cell migrated as if they were connected to one another, thus maintaining the overall physical integrity of the simulated biological cell and preventing spatial fractionation or separation of cytoplasmic components. For example, if Agent 1 of Cell 1 resided at the leading edge of a cell sheet, it would extend lamellipodia into the extracellular space, whereas Agent 9 of Cell 1, which resided at the trailing edge of the cell would be in contact with a neighboring trailing cell (e.g. Agent 1 of Cell 2). The ABM simulated 53 independently-acting mesendoderm cells (each represented by 9 "connected" agents) with initial locations in the simulated tissue prescribed according to published fate maps . This number of cells for the grid size described above represents the average density of cells observed in literature .
Both in vivo and in the ex vivo explant model, mesendodermal cells are "shingled" with one another, or spatially juxtaposed, side-by-side and slightly overlapping front-to-back (note the overlapping cells in Figure 2). Shingling is a phenomenon exhibited by mesodermal cells, which enables their collective uni-directional movement. In order to simulate cell shingling in the ABM, we endowed agents with the ability to detect sub-cells on top of them or underneath them and acknowledge their own position in the z-direction as either an overlapping sub-cell or one being overlapped by its neighbor. The extent of shingling was a free parameter that was determined empirically by measuring the extent of shingling in Xenopus laevis mesendoderm explants imaged with confocal microscopy. If a cell were entirely on top of another cell, it would have no contact with the Fn substrate rendering it unable to exhibit traction forces on the substrate and preventing migration. Visualizing shingling required that the cells be displayed from trailing end to leading end so that the upper layers stacked on the lower layers.
Modeling the fibronectin (Fn) extracellular matrix substrate
A protein matrix consisting of Fn fibers provides a substrate for mesendoderm migration, giving migrating cells a structure on which to exert traction forces (i.e., to pull against) during their movement. Mesodermal cell movement has been shown experimentally to require Fn , and Fn gradients, in part, are thought to guide the mesendodermal cells as they migrate. Accordingly, the Fn matrix was simulated in the ABM by endowing each 2-D square stationary pixel with a variable, "FnConc", that reflected the relative amount of Fn in each pixel. The amount of Fn in each pixel was represented by gray-scaling the color of each pixel, with white representing the highest concentration and black representing no Fn (note the depiction of Fn in Figure 2). As the simulation ran, sub-cells/agents had the ability to dynamically modify the Fn concentration in each pixel, as described below. Moreover, the Fn concentration in a particular pixel had the ability to impact the behavior of a sub-cell occupying that pixel. For example, cell movement in the ABM was partially dictated by the established hypothesis that cells migrate towards increasing Fn concentrations .
Our ABM framework consisted of a 29 × 27 rectangular grid of 2-D square pixels (783 total pixels, where individual pixels represented 15 μ m by 15 μ m of tissue). The NetLogo user interface provides a interactive way to set up the initial conditions of the simulation (see Figure 2). A setup function is called by clicking on a "button" in the user interface. "Slider bars", or gauges, containing tick marks allowed the user to prescribe the initial width and length of the simulated embryo explant by setting the slider bars on the desired tick marks. For the simulations presented here, the mesendoderm explant length was set to 71 percent of the total length of the simulation area, or 309 microns, while the width was set to 21 percent, or 85 microns. Note that all simulations were conducted with 53 initial cells defined as squares encompassing a 3 × 3 grid of sub-cellular agents. Each simulated cell encompassed a 45 × 45 micron square area in the simulation space. The initial extent of shingling, or cell overlap could also be prescribed by setting the value of a "slider bar", termed "confluence percentage." For all simulations, the confluence percentage was set to 77%, based on the average empirically-measured value in mesendoderm explant images .
where, μ = 250 and σ = 50, with the Fn concentration within each pixel being randomly assigned a value varying according to this distribution. We also incorporated two "slider bars" that could be used to set the mean and standard deviation of the Fn concentration distribution within the matrix, if the user wished to treat these parameters as free parameters and vary them accordingly.
The migratory behaviors of the simulated cells in the ABM were dominated by three key parameters: the relative concentrations of Fn, integrin, and cadherin proteins. As already discussed, Fn is an acellular ECM protein found in the substrate upon which cells migrate. Mesodermal cells bind Fn through α5β1 integrin, which modulates cell traction forces and, in part, affects cell migration speed . Cell-cell contact forces are imposed as neighboring cells push and pull each other as they migrate on Fn, and these interactions in mesendoderm are mediated by C-cadherin (simply referred to as "cadherin" hereafter). Cadherins are cell membrane-bound proteins that bind to cadherins on neighboring cells and transmit force from one cell to its neighbor . In the ABM, cadherin binding was limited to regions where sub-cells (agents) spatially overlapped (shingled) so that force transmission from cell to cell occurred only when neighbors were in direct contact with one another. Concentrations of engaged/activated cadherins were determined much in the same way that integrin concentrations were determined: according to the percentage of total cell surface area (i.e. the proportion of the 9 sub-cellular agents comprising each cell) physically in contact with a neighboring cell.
Levels of these three parameters differed for each cell and across cells in space and time (depending on their location in the tissue and their connectivity and shingling with other cells) but they were recorded for each cell over time. Initial levels of these parameters for each cell were set by identifying the ratio of cadherins to integrins as observed in literature. Two free parameters controlled the integrin and cadherin binding strength, and these are prescribed by the user adjusting "slider-bars."
Parameter values used in the ABM multicellular simulation.
Amount of Fn per patch (relative units; prescribed as the mean and standard deviation of the normal distribution)
Mean = 250; S.D. = 50
unpublished observation in Xenopus laevis explants
Initial gradient of Fn (Fn concentration scaling factor for each pixel row that ensures a vertical gradient in the initial Fn concentration; higher values of this parameter generate a steeper gradient)
unpublished observation in Xenopus laevis explants
Total number of mesendodermal cells
Extent of cell shingling (percentage of cell surface area overlapping the neighboring cell behind it)
Width of explant (microns)
Length of explant (microns)
Cadherin activation (mN/m2)
Integrin activation (mN/m2)
Degradation of Fn
Amount of degradation (reduction in Fn as a percentage of previous amount in that pixel prior to degradation by cell)
unpublished observation in Xenopus laevis explants
Strength (percent contribution of the polarity signal to the direction or heading of the cell)
hypothesized based on 
Mean distance traveled per time step (microns)
Quantifying and visualizing simulated mesendoderm behaviors
Each cell in the ABM moved independently from one another, but its movements were impacted by the local Fn concentration of the cell and connectivity/shingling with neighboring cells. Cells were instructed to move generally towards increasing Fn concentrations; however, they were also simultaneously pushed and pulled by neighboring cells. Consequently, each movement calculation required the spatial summation of force vectors from each sub-cell into a net force vector consisting of the forces that cells exerted on Fn and the push/pull forces exerted by neighboring (shingled) cells. Note that individual forces on cells were not balanced, per se, which is a limitation of the current model; however, by using a simple relationship to correlate the net amount of force experienced by a cell with migratory behavior (Eq. 7), the ABM was able to predict realistic migratory behaviors.
The importance of cell shingling
the characteristic aggregate movement of the mesendoderm that has been observed experimentally was recovered. By adding the Fn force vector with the shingling force vectors (Eq. 6),
final Force Vector subcell = fibronectin Vector subcell + shingling Vector subcell (6)
The exponentially limited normal distribution was used because it is a smooth function, with upper and lower limits of 0 μ m and 13 μ m, respectively. The equation was an approximation to the cellular response and was justified only by qualitative data, thereby making it a potential source of error. In order to compensate for the potential inaccuracy, the mean distance traveled (set to 6.5 μ m for the initial simulation), could be set to correspond to any force value. Likewise, the standard deviation of the distance traveled is also a free parameter that can be determined empirically.
Once all of the cells calculated a distance and direction, the movement occurred. All nine of the sub-cells moved the same distance in the same direction, which ensured that no cell (agent) fractionated into pieces. Cells at the leading edge moved first, followed by cells behind them.
The importance of Fn
We hypothesized that the Fn gradient was one of the major driving forces behind the collective movement of the migrating cells. Because cells moved towards increasing Fn concentrations, the establishment of a gradient served as a biasing force to direct the cells in a uniform direction. Thus, the migration of cells created a Fn concentration gradient, which sustained the forward movement. This self-sustainability suggests that natural feedback mechanisms within mesendodermal cells create systematic movement from randomness . However, by implementing an initial Fn gradient at the outset of the simulation, the cells moved at a faster rate because they did not have to wait for the gradient to evolve. This result suggests a method for the multicellular system to implement a positive feedback process as the matrix serves as a signal from one cell to another.
Consistent model system behaviors
The initial testing of the multicellular model was qualitative to ensure that the characteristic motion of the migrating cells was accurate. Specifically, three key emergent phenomena were necessary to prove basic movement accuracy: forward movement, collective movement, and shingling. In the preliminary tests, however, the cells did not behave as expected. Rather than moving towards a common location as a cohesive unit, the cells scattered in multiple directions and exhibited only limited shingling. The inaccuracies suggested the model was incomplete. After reviewing the code and running multiple simulations, it was determined that the modeled cell behavior did not have a sufficient accounting of polarity.
Importance of polarity signals
Polarity was incorporated into the multicellular simulation in an attempt to address the shortcoming described above. The term "polarity signal" refers to structural and/or biochemical rearrangements of the Fn matrix by migrating cells . These changes provide directional information on past cell movements (e.g., "ruts" define the most traveled areas of a road). In the multicellular model, cells were programmed to leave a polarity signal on each pixel they occupied, which biased the migration of future cells towards that pixel. The results of multiple simulations suggested that the polarity signals were necessary for cells to move forward and towards one another, causing them to cluster and shingle in a way that is qualitatively consistent with what has been observed experimentally (Figure 3). This result suggests that polarity signals are not only relevant to mesendoderm migration, but they may be essential in this morphogenic process. There are certainly other mechanisms for cell polarity in this process such as gradients of diffusible signals that are not yet accounted for in this model but may be the subject of further improvements as discussed below. In addition, other mechanisms for collective movement will need to be explored as the model is expanded and refined.
Importance of cadherin-integrin balance
In addition to the "polarity signal," a balance between cadherin and integrin-mediated forces was necessary to ensure accurate aggregate movements. As long as the assigned integrin binding strength was on the same order of magnitude as the cadherin binding strength (~2.5 mN/m2), there was sufficient force to keep neighboring cells together. This observation emerged from running multiple simulations and is consistent with what has been observed experimentally . This balance of cell-cell and cell-matrix forces emerged from the multicellular simulation presented herein.
Factors impacting cell migration speed
This analysis determined that 0.286 simulation time steps in the ABM correlated to one minute, and the time scale of the agent-based model was calibrated so the simulated movements represented accurate cell speeds.
Emergent tissue morphogenesis
The simulated mesendoderm explant tended to narrow laterally and extend vertically in the direction of migration. The initial width of the explant was 85 μ m, and after two hours of simulated time, the tissue height doubled (Figure 5B). This thinning and lengthening behavior has been qualitatively observed in the Keller explant model. We hypothesize that the narrowing resulted from shingling forces and polarity signals, both of which encouraged cell aggregation. We hypothesize that the lengthening could be explained by the combined forward migration and narrowing of the tissue. It is important to note that this phenomenon was not programmed or "hard-wired" into the simulation, but emerged from the individual behaviors of the individual cells and sub-cells.
Integration and validation of multiscale model
There are multiple interactions between the Wnt/β-catenin signaling network and the mesodermal migration behavior described above. It has been hypothesized that the Fn concentration surrounding a cell impacts the strength of the initial Wnt signal . To simulate this interaction, we coupled the intracellular signaling model with the multicell ABM, such that each cell in the ABM was underpinned by its own intracellular signaling model. The multiscale model is, therefore, a multicellular ABM (see Additional File 1) that utilizes a JAVA extension (see Additional File 2) to run Matlab® simulations (see Additional File 3) of the intracellular signaling pathways for each cell at every time step.
NetLogo and Matlab® are not directly compatible, so an intermediary JAVA program was designed to interface the two. NetLogo has extension capabilities that allow JAVA code to be called from within NetLogo code. The JAVA code was a simple JAR file that called Matlab® and executed the intracellular simulation. This connection allowed the two scales to interact dynamically as one multiscale model.
The intracellular and multicellular model operated on identical timescales: after the cells took a step that equated to 3.5 minutes of movement, the intracellular model ran for a simulation of 3.5 minutes. This enabled seamless temporal integration between the two biological scales. The goal of this early stage model was not the precise simulation of gastrulating tissue, but rather proof that the concepts of multiscale modeling can be effectively applied to capture multiscale phenomena (intracellular signaling and multicell interactions).
A framework for multiscale modeling of biological systems is presented. A published model of an intracellular signaling network key to morphogenesis was implemented. A novel multicellular ABM of mesendoderm migration was generated. Several hypothesized regulatory mechanisms were probed, including: (1) the role of cell-to-cell contacts mediated by cadherins in regulating the cohesiveness of the mesendoderm explant during development, (2) the role of the Fn matrix in modulating cell migration speed, (3) the necessity of a haptotactic polarity signal in regulating unidirectional migration of mesendodermal cells within the explant, and (4) the relationship between cadherins and integrins in promoting mesendoderm morphogenesis.
An intracellular model of Wnt/β-catenin signaling in the Xenopus embryo was implemented. This model was verified by reproducing the results presented in Lee et al. (2003). The model was modified to include user-defined inputs and outputs, so that it could read and write to text files that could be accessed by NetLogo. On the multicellular level, literature-supported rules were added to the model to direct cell movement and the program was modified to allow communication with JAVA and (indirectly) Matlab®. Aggregate cell movement was validated qualitatively for the multicellular scale model. Communication was achieved between the two separate models, resulting in a novel multiscale modeling approach.
The multiscale model retained specific characteristic behaviors of the observed phenomenon. One of the key outcomes of this project was the repeatability of the tissue movement. Each cell was allowed to randomly move and interact with other cells, as long as it obeyed simple rules. The randomness, however, consistently resulted in patterned behaviors, suggesting that inherent system characteristics, rather than individual agents, were responsible for the complex biological events. The model effectively represented the fibronectin attachments and shingling behaviors of cells, which resulted in the emergent phenomena of unified forward movement. When combined with the intracellular scale, the model gained sensitivity to changes within individual cells, which resulted in a more complete representation of the system.
Currently, the multiscale model is functional, but has many areas for improvement. There is insufficient quantitative data in literature relating the effects of Fn levels to the Wnt/β-catenin signaling pathway, and the effects of β-catenin levels to cadherin expression levels, so the linear relationships between these factors were qualitatively assumed. Determining these relationships will require additional experimental studies or may be inferred through a detailed parameter analysis of the simulation. Chemotactic gradients may also be important features of mesendoderm migration not yet included in the current model, and they will be critical features to consider in subsequent iterations (albeit the relative importance of chemotactic signals has been questioned and is a focus of current research ). Cell proliferation and death may also be considered in future model developments, although there is a lack of evidence of the relative importance of these processes as well. Computing limitations severely reduced the speed of the multiscale model. The code was designed to be easily expandable rather than computationally efficient, so the simulations required significant computational resources. Although this was not a problem in the abbreviated simulations, this could make a complete simulation of embryogenesis very time consuming. Finally, the connection of the intracellular signaling pathway to the multiscale model assumes that there are no changes during the 3.5 minute interval that the simulation is run. In reality, the pathway is constantly adapting to new conditions, and our model has no way to predict what happens within the 3.5 minute interval.
The models described herein set the stage for future improvements that will enhance predictive capabilities and enable their application to a wider range of biological questions. The intracellular level model can be adapted to include more signaling pathways, as mentioned above, including Wnt/JNK, PDGF, FGF and activin pathways, which have demonstrated importance in mesendoderm migration [20, 24–27]. Moreover, the incorporation of a continuum-based model to approximate the actual forces experienced by cells as they migrate, exert traction forces on the Fn substrate, and push and pull neighboring cells is an important next step. The amount of mechanical force experienced by cells in this system is known to impact levels of integrin and cadherin activation, and therefore should be accounted for in this complex system. We suggest that this could be accomplished by developing a finite element model (FEM) that could also be implemented in Matlab® and called by a JAVA program to communicate with NetLogo in a way that is similar, if not identical, to the intracellular signaling model described here. The integration of a FEM with a NetLogo-based ABM has already been accomplished to study the impact of fluid forces on white blood cell adhesion in the microcirculatory system .
Although there has been some work to develop multiscale computational analyses for various biological systems/processes [28–31], the immediate goal of this work is the creation of a "digital embryo." This will serve as a new tool for answering the larger questions in developmental biology that require more than the classical reductionist approach. Such models can become a community-wide effort to integrate data and hypotheses of key development processes. These computer simulations and models provide a forum for addressing competing hypotheses. In addition, there are differences between our proposed multiscale approach compared to that taken by others in this area. For example, we propose to utilize published parameters for the key signaling pathway and cell-level interactions. Others have arrived at systems level properties, such as robustness, by being more comprehensive in the total number of genes but by exclusively relying on parameter estimation . Previous attempts at multiscale modeling in the vertebrate have not incorporated spatial and temporal systems-level heterogeneities, such as variations in the tissue environment and cell-to-cell differences in phenotype or genotype [33, 34], although some have addressed this in invertebrates, such as Drosophila [35, 36].
Since mesoderm migration depends on both intracellular and extracellular events, it was an ideal starting point for such analysis. In a recent review by  the need for a multiscale modeling framework is described in detail, as are the challenges faced by the computational physiology community. Despite the great strides made by the international "Physiome Project" in establishing computational models at each level of structural organization in a variety of organ systems, a central remaining challenge is to develop integrative frameworks that couple the single cell gene network to the multicell, heterogeneous environment. Our computational framework is a first step at modeling multiscale systems with molecular details for each cell and by incorporating spatial and temporal heterogeneities in an experimentally verifiable system.
Model system: Xenopus laevis gastrulation
Xenopus laevis, commonly known as the African clawed frog, is frequently used to study tissue morphogenesis during embryonic development because of its similarities to the same process in humans, and because its tissues can be surgically excised at different stages of embryogenesis and studied ex vivo by plating the explants on glass coverslips . The modeling effort herein is, therefore, focused on the ex vivo migration of mesendodermal cells, which closely recapitulates their morphogenic behaviors in vivo between developmental stages 10 and 12 (Figure 1) .
Wnt/β-catenin intracellular signaling network
A Xenopus-specific Wnt/β-catenin signaling pathway model was published by Lee et al. (2003) . The authors primarily modeled this pathway with mass action kinetics. We reconstructed this model in Matlab® (see Additional File 1). In addition, we created graphical user interfaces (GUIs) that enabled manipulation of the initial conditions for the system of ordinary differential equations for testing and debugging purposes. As appropriate, the default parameters (e.g., initial concentrations and rate constants) were set to the values published by Lee et al. (2003).
Our Matlab® implementation of the model by Lee et al., 2003 was first validated by comparing our Matlab® predictions to their published results. For example, steady state values were confirmed and all plots characterizing β-catenin levels over time with various perturbations to the network (e.g., gene knockout, overexpression) were reproduced. This validation process ensured that the system of ordinary differential equations was reconstructed correctly.
Agent-based modeling (ABM) for multi-cellular simulations
ABM is a discrete modeling approach that enables the simulation of the behaviors of individual agents, or in this case, cells and their sub-cellular compartments, within a heterogeneous environment over time. ABM is particularly useful for studying emergent biological tissue patterning events, such as morphogenesis [13, 14], where aggregate cell behaviors acting and interacting in space and time give rise to new tissue structures. Rules that govern agent (cell) behaviors are derived from the published literature and from independent experiments. The collection of rules, or a rule-set, dictates how an individual agent will act given different environmental stimuli, such as the presence of Fn at its discrete location or the presence of a neighboring cell in direct contact with it via cadherin coupling. The ABM, therefore, represents the collection of individual agent behaviors that emerge as they individually interact with one another and with their dynamic environment. ABM has been used to examine the morphogenic process of blastocoel roof thinning, another integral part of embryogenesis, thus substantiating the feasibility of applying ABM to the study of embryonic processes . NetLogo, a software package available for free download , was used for the ABM in this study. The relevant Matlab, NetLogo, and Java code can also be downloaded from our lab websites (see  and ).
List of abbreviations
– Agent-based model(ing)
– extracellular matrix
We thank Bryan Thorne and Erwin Gianchandani for their assistance with the development of the JAVA intermediary code. We also thank Erin Armstrong for her contributions to the initial development of the ABM. Financial support was supplied by NIH grant HD26402 (DWD).
- Srivastava D, Olson EN: A genetic blueprint for cardiac development. Nature. 2000, 407: 221-6. 10.1038/35025190PubMedView ArticleGoogle Scholar
- Folkman J, Hahnfeldt P, Hlatky L: Cancer: looking outsidethe genome. Nat Rev Mol Cell Biol. 2000, 1: 76-9. 10.1038/35036100PubMedView ArticleGoogle Scholar
- Davidson LA, Marsden M, Keller R, Desimone DW: Integrin alpha5beta1 and fibronectin regulate polarized cell protrusions required for Xenopus convergence and extension. Curr Biol. 2006, 16: 833-44. 10.1016/j.cub.2006.03.038PubMedView ArticleGoogle Scholar
- Davidson LA, Keller R, DeSimone D: Patterning and tissue movements in a novel explant preparation of the marginal zone of Xenopus laevis. Gene Expr Patterns. 2004, 4: 457-66. 10.1016/j.modgep.2004.01.001PubMedView ArticleGoogle Scholar
- DeSimone DW, Davidson L, Marsden M, Alfandari D: The Xenopus embryo as a model system for studies of cell migration. Methods Mol Biol. 2005, 294: 235-45.PubMedGoogle Scholar
- Peirce SM, Skalak TC: Microvascular remodeling: a complex continuum spanning angiogenesis to arteriogenesis. Microcirculation. 2003, 10: 99-111.PubMedView ArticleGoogle Scholar
- Lin X, Feng XH: Abrogation of transforming growth factor-beta signaling in pancreatic cancer. World Journal of Surgery. 2005, 29: 312-316. 10.1007/s00268-004-7824-3PubMedView ArticleGoogle Scholar
- Grazul-Bilska AT, Johnson ML, Bilski JJ, Redmer DA, Reynolds LP, Abdullah A, Abdullah KM: Wound healing: the role of growth factors. Drugs of Today. 2003, 39: 787-800. 10.1358/dot.2003.39.10.799472PubMedView ArticleGoogle Scholar
- Davidson LA, Hoffstrom BG, Keller RE, DeSimone DW: Mesendoderm extension and mantle closure in Xenopus laevis gastrulation: combined roles for integrin alpha-5-beta1, fibronectin, and tissue geometry. Dev Biol. 2002, 242: 109-129. 10.1006/dbio.2002.0537PubMedView ArticleGoogle Scholar
- Kumar S, Maxwell IZ, Heisterkamp A, Polte TR, Lele TP, Salanga M, Mazur E, Ingber DE: Viscoelastic retraction of single living stress fibers and its impact on cell shape, cytoskeletal organization, and extracellular matrix mechanics. Biophys J. 2006, 90: 3762-73. 10.1529/biophysj.105.071506PubMed CentralPubMedView ArticleGoogle Scholar
- Wang JH, Lin JS: Cell traction force and measurement methods. Biomech Model Mechanobiol. 2007Google Scholar
- Bailey AM, Thorne BC, Peirce SM: Multi-cell Agent-based Simulation of the Microvasculature to Study the Dynamics of Circulating Inflammatory Cell Trafficking. Annals of Biomedical Engineering. 2007, 35: 916-936. 10.1007/s10439-007-9266-1PubMedView ArticleGoogle Scholar
- Longo D, Peirce SM, Skalak TC, Davidson L, Marsden M, Dzamba B, DeSimone DW: Multicellular computer simulation of morphogenesis: blastocoel roof thinning and matrix assembly in Xenopus laevis. Dev Biol. 2004, 271: 210-22. 10.1016/j.ydbio.2004.03.021PubMedView ArticleGoogle Scholar
- Thorne BC, Bailey AM, Peirce SM: Combining Experiments with Multi-Cell Agent-Based Modeling to Study Biological Tissue Patterning. Briefings in Bioinformatics. 2007, 245-257.Google Scholar
- Peirce SM, Van Gieson EJ, Skalak TC: Multicellular simulation predicts microvascular patterning and in silico tissue assembly. Faseb J. 2004, 18: 731-3.PubMedGoogle Scholar
- Marsden M, DeSimone DW: Regulation of cell polarity, radial intercalation and epiboly in Xenopus: novel roles for integrin and fibronectin. Development. 2001, 128: 3635-47.PubMedGoogle Scholar
- Carsons SE: Fibronectin in Health and Disease. CRC Press, Boca Raton, FL
- Lauffenburger DA, Horwitz AF: Cell migration: a physically integrated molecular process. Cell. 1996, 84: 359-69. 10.1016/S0092-8674(00)81280-5PubMedView ArticleGoogle Scholar
- Kuhl M, Wedlich D: Xenopus cadherins: sorting out types and functions in embryogenesis. Dev Dyn. 1996, 207: 121-34. 10.1002/(SICI)1097-0177(199610)207:2<121::AID-AJA1>3.0.CO;2-JPubMedView ArticleGoogle Scholar
- Nagel M, Tahinci E, Symes K, Winklbauer R: Guidance of mesoderm cell migration in the Xenopus gastrula requires PDGF signaling. Development. 2004, 131: 2727-2736. 10.1242/dev.01141PubMedView ArticleGoogle Scholar
- Sivasankar S, Brieher W, Lavrik N, Gumbiner B, Leckband D: Direct molecular force measurements of multiple adhesive interactions between cadherin ectodomains. Proc Natl Acad Sci USA. 1999, 96: 11820-4. 10.1073/pnas.96.21.11820PubMed CentralPubMedView ArticleGoogle Scholar
- Gradl D, Kuhl M, Wedlich D: The Wnt/Wg signal transducer beta-catenin controls fibronectin expression. Mol Cell Biol. 1999, 19: 5576-87.PubMed CentralPubMedView ArticleGoogle Scholar
- Kuhl M, Geis K, Sheldahl LC, Pukrop T, Moon RT, Wedlich D: Antagonistic regulation of convergent extension movements in Xenopus by Wnt/beta-catenin and Wnt/Ca2+ signaling. Mech Dev. 2001, 106: 61-76. 10.1016/S0925-4773(01)00416-6PubMedView ArticleGoogle Scholar
- Winklbauer R, Keller RE: Fibronectin, mesoderm migration, and gastrulation in Xenopus. 1996, 177: 413-426.Google Scholar
- Nagel M, Winklbauer R: Establishment of substratum polarity in the blastocoel roof of the Xenopus embryo. Development. 1999, 126: 1975-84.PubMedGoogle Scholar
- Winklbauer R, Selchow A: Motile behavior and protrusive activity of migratory mesoderm cells from the Xenopus gastrula. 1992, 150: 335-351.Google Scholar
- Wardle FC, Smith JC: Refinement of gene expression patterns in the early Xenopus embryo. Development. 2004, 131: 4687-96. 10.1242/dev.01340PubMedView ArticleGoogle Scholar
- Winslow RL, Cortassa S, Greenstein JL: Using models of the myocyte for functional interpretation of cardiac proteomic data. Journal of Physiology. 2001, 563: 73-81. 10.1113/jphysiol.2004.080457.View ArticleGoogle Scholar
- McCulloch AD: Functionally and structurally integrated computational modeling of ventricular physiology. Japanese Journal of Physiology. 2004, 54: 531-539. 10.2170/jjphysiol.54.531PubMedView ArticleGoogle Scholar
- Izaguirre JA, Chaturvedi R, Huang C, Cickovski T, Coffland J, Thomas G, Forgacs G, Alber M, Hentschel G, Newman SA, Glazier JA: CompuCell, a multi-model framework for simulation of morphogenesis. Bioinformatics. 2004, 20: 1129-1137. 10.1093/bioinformatics/bth050PubMedView ArticleGoogle Scholar
- Jonsson H, Heisler M, Reddy GV, Agrawal V, Gor V, Shapiro BE, Mjolsness E, Meyerowitz EM: Modeling the organization of the WUSCHEL expression domain in the shoot apical meristem. Bioinformatics. 2005, 21 (Suppl 1): i232-40. 10.1093/bioinformatics/bti1036PubMedView ArticleGoogle Scholar
- von Dassow G, Meir E, Munro EM, Odell GM: The segment polarity network is a robust developmental module. Nature. 2000, 406: 188-182. 10.1038/35018085PubMedView ArticleGoogle Scholar
- Woolf PJ, Prudhomme W, Daheron L, Daley GQ, Lauffenburger DA: Bayesian analysis of signaling networks governing embryonic stem cell fate decisions. Bioinformatics. 2005, 21: 741-753. 10.1093/bioinformatics/bti056PubMedView ArticleGoogle Scholar
- Prudhomme W, Daley GQ, Zandstra P, Lauffenburger DA: Multivariate proteomic analysis of murine embryonic stem cell self-renewal versus differentiation signaling. Proc Natl Acad Sci USA. 2004, 101: 2900-2905. 10.1073/pnas.0308768101PubMed CentralPubMedView ArticleGoogle Scholar
- Reeves GT, Kalifa R, Klein DE, Lemmon MA, Shvartsman SY: Computational analysis of EGFR inhibition by Argos. Dev Biol. 2005, 284: 523-35.PubMedView ArticleGoogle Scholar
- Mizutani CM, Nie Q, Wan FY, Zhang YT, Vilmos P, Sousa-Neves R, Bier E, Marsh JL, Lander AD: Formation of the BMP activity gradient in the Drosophila embryo. Developmental Cell. 2005, 8: 915-924. 10.1016/j.devcel.2005.04.009PubMed CentralPubMedView ArticleGoogle Scholar
- Hunter P, Nielsen J: A strategy for integrative computational physiology. Physiology. 2005, 20: 316-325. 10.1152/physiol.00022.2005PubMedView ArticleGoogle Scholar
- Lee E, Salic A, Krüger R, Heinrich R, Kirschner MW: The roles of APC and axin derived from experimental and theoretical analysis of the Wnt pathway. PLoS Biol. 2003, 1: 116-132.Google Scholar
- Wilensky U: NetLogo. 1999, http://ccl.northwestern.edu/netlogoGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.