Research Article  Open Access
A. W. Lund, C. C. Bilgin, M. A. Hasan, L. M. McKeen, J. P. Stegemann, B. Yener, M. J. Zaki, G. E. Plopper, "Quantification of Spatial Parameters in 3D Cellular Constructs Using Graph Theory", BioMed Research International, vol. 2009, Article ID 928286, 16 pages, 2009. https://doi.org/10.1155/2009/928286
Quantification of Spatial Parameters in 3D Cellular Constructs Using Graph Theory
Abstract
Multispectral threedimensional (3D) imaging provides spatial information for biological structures that cannot be measured by traditional methods. This work presents a method of tracking 3D biological structures to quantify changes over time using graph theory. Cellgraphs were generated based on the pairwise distances, in 3DEuclidean space, between nuclei during collagen I gel compaction. From these graphs quantitative features are extracted that measure both the global topography and the frequently occurring local structures of the “tissue constructs.” The feature trends can be controlled by manipulating compaction through cell density and are significant when compared to random graphs. This work presents a novel methodology to track a simple 3D biological event and quantitatively analyze the underlying structural change. Further application of this method will allow for the study of complex biological problems that require the quantification of temporalspatial information in 3D and establish a new paradigm in understanding structurefunction relationships.
1. Introduction
Traditional reductionist biology has developed a wealth of knowledge concerning individual molecules and their function. This data set, however, has exceeded our capabilities for integration and analysis. Attempts to step outside these subcellular networks, into the equally complex world of three dimensional (3D) tissue development, are limited by our ability to deal with the spatial and temporal information that can be gathered in such studies [1]. Multispectral imaging has the potential to provide insight into the spatial orientation and dynamic organization of biological structures; however, we are still not equipped to quantitatively analyze and use all the data that is present in such images.
Graph theory has emerged as a method to characterize the structure of large complex networks leading to a better understanding of the dynamic interactions that exist between their components. A graph is a mathematical structure that represents the relationships between members of a given set and is depicted as discrete points (nodes) connected by interactive links (edges) [2]. These graphs define pairwise interactions which can be either directed or undirected [1]. Both local and global topographical characteristics extracted from these graphs can define the network structure (topology) and relationships that exist within the node population [3]. Nodes with similar characteristics tend to cluster together and the pattern of this clustering provides information as to the shared properties, and therefore the function, of those individual nodes [4]. The graph theory approach permits users to test hypotheses that define the characteristics of node interaction, regardless of whether the relationships between nodes are well defined or not.
Graph theory has been applied to a variety of real networks from biology to social networking the internet and literature citations. Biological networks have common designs that are governed by simple and quantifiable organizing principles [1]. These principles are not random: evolution by natural evolution has consistently repeated efficient and functional patterns of organization. We can use our understanding of these principles to extract information about the function of complex biological networks, from proteinprotein interactions, cell signaling cascades, disease networks [5], transcriptional, metabolic [6, 7], and genetic regulatory systems [8], and brain connectivity [9–11]. These studies highlight the ability of graph theory to capture the modularity of biological networks and provide important insight into the function of these networks on a global level. Researchers have recently used graph theory to extract topological features from neural networks and compare connectivity between young and old patients. They were able to extract information from these graphs that suggest that the process of aging that occurs in the brain may actually be due to changes that are occurring in the modularity of their sparse networks [11]. While significant steps have been made, the key challenge still remains to understand the structure and dynamic interactions of living cells within the context of their physical environment including matrix architecture, cellular compartmentalization, and cytoskeletal affects that may restrict these subcellular interactions [1]. If we can understand the design principles that govern biological organization, then we can use those principles to inform and accelerate studies of tissue morphogenesis, development, differentiation, and organogenesis.
Natural and engineered tissues are a collection of cells arranged within a structural scaffold of extracellular matrix (ECM) proteins that provide biochemical and mechanical cues to direct the function of those cells. Tissue function is therefore dependent upon the spatiotemporal resolution of matrix proteins, cells, and signaling molecules. Understanding the interactions of this complex set of components over time requires novel techniques of extracting data from the intact tissue. In fact, the three dimensionality of tissue itself is critical for the maintenance of normal cellular function [12, 13]. Changes in cell shape [14], ECM organization [15], tissue geometry [16], and mechanics [17] affect gene expression profiles [18], differentiation [19], and cancer progression [20]. It is therefore critical to probe cellular function within nativelike environments and treat these “tissues” as multiscale networks of interacting units.
This paper presents a novel application of graph theory to extract and quantify the tissue structure/function relationship. We construct cellgraphs that place cell nuclei as the nodes of the graphs and link those nuclei as a function of their pairwise distance based on the assumption that cells that are in physical contact (i.e., membrane proximity) interact. Previous work demonstrates that graph theorybased analysis of the locations of cell nuclei provides important information concerning the (dys)functional states of the tissue [21–23]. Cellgraphs and their variants (Hierarchal Cellgraphs and ECMaware cellgraphs) based on pathological images of brain, breast, and bone cancer, respectively, model tissue structure to provide quantitative metrics that enhance diagnostic accuracy over that of other automated methods [24]. These results arose from graphs of 2D cell nuclei in histological images, suggesting that a wealth of knowledge has yet to be exploited in higherresolution images. Here we extend graphbased analysis of 3D fluorescent images to track biological structures in a dynamic fashion and extract data reflecting fundamental changes in tissue organization and structure.
2. Materials and Methods
2.1. Cell Culture
Cryopreserved hMSCs (Lonza) were grown according to manufacturer’s instructions. hMSCs were cultured in Dulbecco’s Modification of Eagle’s Medium 1x (DMEM) supplemented with 10% fetal bovine serum (FBS) and fungizone/penicillin/streptomycin (FPS) (10,000 units/mL). Medium was changed every three days and cultures were incubated at C in a humidified atmosphere containing 95% air and 5% CO_{2}. Cells were detached using trypsinEDTA and passaged into fresh culture flasks upon reaching confluence. hMSCs were used between passages 6 and 8. In preparation for incorporation into 3D constructs, cells were washed with PBS, detached with trypsinEDTA, collected, and counted. All reagents were purchased from Fisher Scientific unless otherwise noted.
2.2. 3D Collagen I Culture
Threedimensional collagen I gels were prepared by mixing cells with the following reagents: DMEM (14%), FBS (10%), 5 Conc. DMEM (16%), 0.1N NaOH (10%), and 4 mgmL collagen I (50%) (MP Biomedicals). The final collagen concentration is 2 mg/mL within each construct. Constructs of a volume of 1.0 mL were made in 12well plates and the cellular density was kept at 1.0 10^{6} cells per mL ECM and 3.0 10^{5} cells per mL, for their respective experimental sets. The constructs were incubated at C for 30 minutes, released from the wells, and incubated in DMEM for 24 hours. The floating gels were removed at from culture at each time point and imaged using a Nikon digital camera for compaction. Gel images were analyzed using Image J (NIH) and the percent change in volume was calculated. Triplicates of each sample were analyzed. Statistical analysis was performed using the student test; a value less that .05 was considered significant.
2.3. Fluorescence Imaging
Collagen I constructs were prepared for fluorescence staining at hours 0, 1, 2, 4, 6, 10, 16, and 24. Constructs were washed with PBS followed by a 30minute incubation at C in 3% paraformaldehyde. The constructs were then washed with PBS and incubated at C for 30 minutes in cell blocking solution (0.25% Tween20, 1% BSA in PBS). Collagen constructs were incubated for 10 minutes at room temperature in SYTOX Green Dye (Invitrogen) at a final concentration of 50 nM in cell blocking solution. The samples were stored at C in PBS until imaging. 3D confocal images were taken using a Zeiss LSM 51 and Image J (NIH) was used to convert the files into .tiff format for segmentation.
2.4. Image Segmentation Node Identification
The 3D confocal images were segmented using the Otsu Thresholding algorithm [25]. The Otsu Thresholding algorithm assumes that there are two classes of pixels in the observed image and finds a threshold value that will automatically separate the foreground pixels from the background. The algorithm searches for the threshold value that minimizes the intraclass variance. After finding this optimal threshold, the intensity values of each pixel are compared against the threshold and the pixels with intensity values higher than the threshold assigned as foreground pixels. The foreground pixels that are touching each other are connected, and the center of mass of these nuclei is calculated to identify node (vertex) set for cellgraph generation.
2.5. CellGraph Generation
A graph is given by where is the vertex set of the graph and is the edge (link) set of the graph. Cellgraphs are constructed for structural modeling of tissue organization. The vertex set contains the nuclei, obtained from image segmentation as explained above. The edge set represents pairwise relationships between cells. We assume that a pair of cells interacts if they are in physical contact (e.g., cell membranes are touching or very close to each other). Thus, we define a distancebased edge function to model this hypothesis, and a link between a pair of two nodes is established when the Euclidean distance between them is defined as where , and are , , coordinates of node , respectively.
For each pair of vertices the pairwise Euclidean distance is calculated and a link is set when that distance is smaller than the linking (edge) threshold. This threshold value is determined by considering the nucleusmembrane ratio and estimating cell diameter. We have identified thresholds, corresponding to the approximate radii of spread mammalian cells, of 65, 70, and 75 microns (from a distortion free sphere representation of the cell membrane to observable distortion) and executed our algorithms for each.
2.6. CellGraph Features
Topographical properties for each cell graph were extracted and averaged over the entire graph to represent global measures of “tissue organization”; see Table 1. These computed properties or cellgraph metrics are well accepted in the internet topology generator and simulation literature (see http://cat.inist.fr/?aModele=afficheN&cpsidt=14492873 and references therein) and used to (i) characterize graph topography and (ii) verify if two graphs come from the same distribution. A rigorous explanation of these metrics and their significance is provided in our previous publications [23, 24].

2.7. Computing Randomness of Tissue Organization
The Cumulative Nearest Neighborhood Distribution (CNND) function [26] was used to generate random positions of nuclei and compared to experimental nuclei locations. The CNND function was calculated from the 3D geometry in our tissue samples defined by a 3D bounding box B that includes all the cells in a sample. For each cell we chose a uniformly random , , coordinate in B. Given B the function takes distance threshold as the input parameter, defined as follows: where is an indicator function, is the distance of cell from its nearest neighbor, and is the total number of cells segmented in the image.
This function value represents the fraction of the cell counts for which their nearest neighbor falls within the threshold distance , and as the threshold increases, more cells include their nearest neighbor within the threshold. Thus, this function value always increases from 0 to 1.
The randomness of cellcell relationships was tested by defining an edge function according to the ErdosRenyi model, calculating the same set of features on our random graphs, and comparing the random graph metrics to that of the cellgraphs: where nodes are linked by a probability of [27]. Here the edge definition is independent of node location. A variation of the model, the model, chooses a graph at random from the set of all possible graphs with nodes and links. For each time point and cell density, we generated a cellgraph, calculated the number of nodes and links in that cellgraph, and then generated a random graph using the model. We generated 10 random graphs, calculated the metrics, and then averaged them. We compared the average values of these metrics to the cellgraph metrics.
2.8. VoronoiDelaunay Graph Modeling of Samples
We compared the cellgraph technique to Voronoi diagrams and the Delaunay triangulation method [28–30]. On a sample tissue image, the Voronoi diagram partitions the image into convex polytopes (i.e., polygons in 2D and polyhedrons in 3D) such that each polytope contains exactly one cell (generating point) and every point in a given polytope is closer to its generating point than to any other generating point in the tissue (Voronoi cell). Delaunay triangulations were built by linking the generating points of neighboring Voronoi cells. We built Delaunay triangulations on cells identified in the segmentation step, then calculated the same set of metrics, and observed their changes over time.
2.9. Subgraph Pattern Mining
Classical graph mining [31] finds frequent subgraphs from a graph database, . The support of a subgraph is defined as , where if is a subgraph of and 0 otherwise. A subgraph is considered frequent if its support across the graph database is equal or higher than a userdefined support threshold.
For the cell graphs we sought subgraphs that are frequent with respect to their embedding count in one large graph. Support of a subgraph, , is equal to its embedding count in one large graph, , which is provided as input. We considered each cell graph in a separate graph mining session to find its frequent subgraphs. In each session, we used a common support threshold value [20] and used only the edgedisjoint embeddings (explained below) while counting the embedding. Frequent subgraphs for different cell graphs were processed further to find those with high support at one time point, but not in others. To do so, we modified the support count method of the graph mining algorithm in a DMTL library [32] which provides modular design and therefore simpler modification. In our support count subroutine, we used Ullman's algorithm [33] which returns the decision that a graph, , is a subgraph of and also provides all possible embeddings of in . Since subgraph mining is very costly (subgraph isomorphism test is Hard), we restricted our mining process to consider subgraphs that have at most four edges.
For each subgraph we detected the frequency of its occurrence at each time point and for each cell density using edgedisjoint embeddings. Subgraph pattern size was restricted to an upper limit of four edges, and each vertex is labeled by an integer number corresponding to the proportional degree of that vertex to capture local network information. The labeling scheme is shown in Table 2. If every vertex in a graph has a unique label, the embedding count of a graph, , in a larger graph, , can be at most one. However, in our samples, multiple vertices may have the same label (Table 2); so the embedding count for a subgraph may be greater than one. To avoid unfairly elevated embedding counts caused by a subgraph where many of its vertices share the same labels we only considered edgedisjoint embeddings while counting the support of a pattern. Because finding the maximum value for the edgedisjoint embedding count from the total embedding count is Hard, we used simple smallest degree heuristics to find an independent set [25] to obtain the edgedisjoint embedding support of a subgraph pattern. All the subgraphs that have an edgedisjoint embedding count more than the threshold value of 20 were returned by the algorithm.

3. Results
3.1. Macro and Microscale Compaction Occurs in the First 24 Hours of Collagen I Culture
To provide proof of concept for our cellgraph method we encapsulated hMSC in 3D collagen I hydrogels at a concentration of cells/mL of collagen I. A hallmark of hMSC hydrogel culture is the cell dependent compaction event that begins immediately following encapsulation. Triplicate samples were fixed at hours: 0, 1, 2, 4, 6, 10, 16, and 24 postencapsulation. We imaged the entire collagen I gel after fixing, as shown in Figure 1(a). The collagen I hydrogels compacted to approximately 15% of their original volume over the 24hour time course, with the largest change in volume occurring within the first six hours. At each time point the nuclei were imaged by confocal microscopy (10) to reflect cellular organization within the 3D space of each hydrogel; see Figure 1(b). The number of nuclei captured within the 10 field of vision increased over time as the hydrogels compacted.
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3.2. Graph Theory Applied to 3D Confocal Images Generates DistanceDependent CellGraphs
Cellgraphs, Figure 2(b), were generated from the 3D reconstruction of the fluorescent image zstacks; see Figure 2(a). The 3D images were segmented, nodes identified, and links formed based upon their Euclidean distance as described in the methods. This method was able to successfully segment the 3D nuclear images and form cellgraphs that demonstrate the relationships between nodes over time. The number of edges, links, between cell nuclei increased throughout the time course; see Figure 2(b). This is consistent with the increased nuclear density observed in the fluorescent images.
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3.3. Quantitative Metrics Can Be Extracted from CellGraphs That Characterize 3D Organization Over Time
The utility of these cellgraphs comes from the ability to extract meaningful and quantitative metrics to describe the relationships between nodes. The metrics (Table 1) were computed for the generated cellgraph of each zstack over the time course. These metrics quantitatively provide information as to the 3D orientation and potential interactions of cells in culture; see Table 3. The metrics were dependent on the location of the cells relative to one another. The number of nodes increased with time which represents the number of nuclei and is again consistent with the visual data. The number of edges increased as the hydrogels underwent compaction and the distance between cells decreased. The giant connected ratio reached one by 16 hours in our collagen I hydrogel time course. The percent of isolated points and end point metrics both reached a value of zero by 16 hours. The average degree increased over the 24hour period while the clustering coefficient had a sharp increase between 1 to 2 hours and leveled off by 10 hours. The diameter peaked at 10 hours and the number of connected components decreased to zero by 16 hours into the time course. Our results are stable for link thresholds between 65 to 75 microns as shown in Table 4.


3.4. An Increased Cellular Density Increases the Rate of Hydrogel Compaction during the First 24 Hours
To demonstrate the metrics’ sensitivity to perturbations in the biological system we repeated the experiment using a higher cell concentration ( cell/mL of ECM). The cells/mL gels compacted to less than 10% of their original volume by hour 16; see Figure 3(a). These observations are reflected in the fluorescent images of nuclei over time; see Figure 3(b).
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Cellgraphs, Figure 4(b), generated based upon the new 3D images, Figure 4(a), showed an increased connectivity, expressed as visible links at earlier time points. The transition to high connectivity occurred at six hours in the high cell density gels, while the low cell density samples transitioned at ten hours. Quantitative metrics from the high cell density gels are listed in Table 5. In the cell/mL gels the number of edges between the nodes increased over time, with the largest increase occurring between 10 and 16 hours. The giant connected ratio approached one beginning at 10 hours. The percent of isolated points and percent of end points reached zero at 10 hours. The average degree underwent the largest increase from 10 to 16 hours and peaked at 16 hours followed by a decrease of approximately 20% by 24 hours. The diameter peaked at 2 hours and decreased by hour 10. The number of connected components also reached one by hour 16.

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3.5. Increasing Cellular Density Leads to a Shift in the Metrics Transition over Time
The sensitivity of our metrics to gross changes in biological function is a prerequisite to the extension of this method into more complex problems. Quantification of gel compaction revealed a relationship between collagen I compaction and cell density; see Figure 5. The cell/mL gels showed significant compaction within the first hour while the cell/mL samples did not significantly compact until the second hour (). After 24 hours of culture the cell/mL gels reached a final volume of 5.27% of the original while the cell/mL gels reached 11.92% .
Figure 6 graphically represents the relationship between some of graph features in the two experimental sets. The average degree reached its maximum at an earlier time (16 hours) in the cell density gels than in the cell density gels (24 hours); see Figure 6(a). The clustering coefficient also differed; see Figure 6(b). The diameter or maximum eccentricity had a large shift in its peak to an earlier time point (2 hours) in high density gels compared to lowdensity gels (10 hours); see Figure 6(c). The cell/mL graphs had a continuous increase in the number of edges during the 24 hours. The cell/mL graphs peak at an earlier time point of 16 hours with a large increase occurring between 10 and 16 hours; see Figure 6(d). The giant connected ratio reached a value of one at an earlier time point when the cell density was increased to cell/mL from cell/mL; see Figure 6(e). The number of connected components decreased at a faster rate when the cell density was increased to cell/mL; see Figure 6(f).
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3.6. CellGraph Features Significantly Diverge from Those Extracted from Random Graphs
To show that tissue has a structure which is different from the random organization of the same number of cells, we established two properties: (i) cells are not randomly scattered in 3D space, and (ii) cells interact in a nonrandom fashion. For the first property, we randomly distributed points representing the cells within 3D space with the same density and geometry seen in the images. The CNND function was implemented explained for both random scattering and for actual cell locations obtained from image segmentation. The results, Figure 7, indicate that cells in the compacting gels were not randomly scattered in the gels. Note that parameter t is a measure of distance and defines the neighborhood size such that as farther nodes are included to the neighborhood, the difference from random scattering diminishes. Similarly, small values of are not informative since neighborhoods become sparse. However, Figure 8 demonstrates that for a wide range of values the difference is significant and more importantly such difference is observed for smaller values as time progresses and the gels compact.
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To show that cellcell interactions cannot be modeled by randomly picking pairwise interactions between cells, we defined an edge function according to ErdosRenyi (ER) model and generated random graphs to distinguish their features from those extracted from our cellgraphs. Consider three cases for generating random graphs: (i) cell locations are chosen randomly and the ER edge function is used, (ii) cell locations, obtained from image segmentation, are taken as node locations and ER edge function is used, and (iii) node locations are randomly chosen but the cellgraph edge function is used. Since case (ii) is subsumed in (i) (recall that ER model takes number of nodes and edge probability as its only parameters), we only analyzed case (i) and case (iii).
For case (i) random graphs were generated with equal numbers of nodes and edges as found in the cellgraphs at each given time point. We extracted the same features calculated for our cellgraphs from these random graphs. Some of the metrics are defined by the number of nodes and links present in the tissue (i.e., average degree) and therefore must be consistent between the cell and random graphs. The remaining values in our cellgraphs were significantly different from those found in the random graphs, indicating that the cellgraph metrics and random metrics did not come from the same distribution; see Figure 8. For example, the clustering coefficient of the random graphs for 3.0 10^{5 }cell/mL samples fluctuated between 0.02 and 0.03, but gradually increased from 0.35 to 0.62 for the cellgraphs over the 24hour time period. This difference captures the compaction of the tissue samples as the value gradually increases. Also, the giant connected component of the high density random graphs maintained a value of 1 throughout the 24 hour period, whereas the values for the cellgraphs steadily increased to 1, matching the compaction of the tissue samples. The average eccentricity increased throughout compaction in cellgraphs whereas in random graphs this metric was almost constant.
For case (iii) we also randomly distributed cells in a 3D space with the same density and geometry of the corresponding samples and used the cellgraph edge function to construct the cellgraphs. We compared the graph metrics on these randomcellgraphs with graphs from the 3D image segmentation. The cellgraphs defined a relationship (edge) between the nearest random nodes and the graph features correlated with many of the tissue cellgraph features. However, certain graph metrics such as the graph radius were different. In Figure 9, we plotted the KolmogorovSmirnov test for “radius” which indicates the distance of nodes to the central points. The red curve represents tissue cellgraphs while theblue curve corresponds to the randomcellgraphs.
3.7. CellGraphs Outperform Voronoi Graphs in Modeling Gel Compaction
In order to determine the relevance of our approach we assessed the performance of our cell graph method to the more traditional Delaunay triangulation model. The tissue was partitioned into Voronoi cells and the corresponding Delaunay graph was generated for each set of images. Graph features were extracted from these Delaunay graphs as shown in Table 6. These results suggested that Delaunay graphs did not exhibit the patterns that we observed with the cellgraph technique. For example, the average degree of the Delaunay graphs over time deviated between 13.17 and 14.33 and average clustering coefficient varied between 0.45 and 0.49. The giant connected component ratio was 1 at all times and the diameter of the network stayed almost constant, deviating between 5.2 and 7.

3.8. Significant Subgraphs Extracted from CellGraphs Determine Local Structural Motifs
The features extracted from the tissue cellgraphs were representative of the global (average) structure of our “tissues.” To extract meaningful local structures and motifs we used subgraph mining techniques that identify patterns of node interaction and measure their frequency of occurrence over time. Thousands of subgraph patterns were generated that represent repeated local motifs. The frequency of common subgraphs was also measured in random graphs, to eliminate the possibility that the local structures extracted were simply structures present in any random organization of nodes and links. Distinguishable patterns were extracted that existed only in the cellgraphs, Figure 10(a), or existed only in the random graphs, Figure 10(b), indicating a significant difference in the underlying topography of the cellgraphs from that of the random graphs. The distribution of the differences between the frequencies at which the patterns were found in the random and cellgraphs is shown in Figure 10(c). The distribution of the histogram to the extremes indicated a significant divergence from the patterns extracted from random graphs.
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3.9. Subgraph Mining Reveals Temporal Changes in Graph Patterning
The appearance of specific subgraphs was observed at distinct time points and cellular densities. To reveal the time evolution of the significant subgraphs we calculated the number of patterns that first appeared in the 3.0 10^{5} cell/mL graphs at each time point as a function of their frequency at a given time point in the 1.0 10^{6} cell/mL graphs; see Table 7. Consistently, the first appearance of certain patterns at late time points in the 3.0 10^{5} cell/mL time series correlated with patterns frequently found at early time points in the 1.0 10^{6} cell/mL series. Some time points showed a very strong correlation, with a high number of similar patterns, specifically time 10 hours in the 1.0 10^{6} series and time 16 hours in the 3.0 10^{5} series (bold value in Table 7). Additionally, a transition was observed after this time point, indicated by the presence of 3.0 10^{5} subgraphs that appeared before, after and during respective 1.0 10^{6} subgraphs.

4. Discussion
The extraction of nonrandom repeating motifs in biological structures presents a significant opportunity to define organizing design principles and use those principles to inform and accelerate natural and synthetic processes of tissue development. Here we present the spatial and temporal analysis of a simple biological observation, the compaction of collagen I hydrogels by hMSC. The progression of this event over time was dependent upon the cellular density of the starting material and represents a direct, cellmediated organizational event that can be observed through time and space. We observed that an increase in cell density caused an accelerated compaction event that resulted in a decrease in the final volume as compared to the original samples. We tracked this organization event using confocal microscopy and employed graph theory as a method to extract the 3D topography of our “tissue constructs” over the time course of the compaction event. As the hMSCs interact with and organize the naïve collagen matrix, we hypothesized that structural motifs would appear frequently and be evident at earlier time points in the dense samples. This predicts that cells interact with one another and their extracellular environment in nonrandom, defined patterns that we can quantify, and that these patterns are consistent in terms of their temporal organization.
To address this hypothesis we constructed cellgraphs from our 3D micrographs and extracted topographical features that assess the global 3D structure of the “tissue constructs” as they organize over time. Such techniques have previously been reported to extract meaningful information concerning the (dys)functional state of 2D tissue and can play a significant role in diagnosis of cancer pathologies [21–24]. In addition, past and current work on the nature of complex biological networks has consistently benefited from the use of graph theory as a means of extracted underlying relationships between system components [1, 2, 5, 6, 8–11, 34, 35]. We employed this technique here to define distancebased 3D graphs of cell nuclei and found that significant trends do exist in the extracted features over time and that these features represent the connectivity, modularity, and relationships that exist within our tissue. We conclude that the cells within our tissue exist in dense communities that steadily converge over time and that each cell has a high interaction with an increasing number of neighbors as the tissues organize and compact. In addition, a decrease in cellular density resulted in a delay or shift in these feature trends that is consistent with visual observation of construct compaction over time.
The use of random graphs as a negative control was critical to ensure the extraction of meaningful and nonrandom metrics. The divergence of features extracted from our cellgraphs from those found in random graphs indicates that there exists structure within our “tissue” that is different from a random organization of the same number of cells and links. This is consistent with the theory that random networks do not accurately describe real networks, that networks are highly ordered structures, and that keys to their function lie within that inherent structure [36]. In fact, as the density of the experimental samples increases over time, the difference between the random graphs and cellgraphs becomes more and more remarkable. In a random graph at a density of 1.0 10^{6} cell/mL the graph is connected, and as the density increases, the diameter decreases as more links are added to the graph. Within our cellgraphs, however, at this same cell density, we see a steadily increasing diameter. This increase in diameter is due to the fact that the connectivity at time zero is sufficiently low to observe increases as the gels condense over time, unlike randomly generated graphs, and therefore the diameter of the entire graph responds by growing as the giant connected component size grows as well. The random graph is connected as a function of the number of nodes and links incorporated into its generation, but there is no true structural relationship evident, as there is no change observed in eccentricity or clustering coefficient. Instead what we see in our cellgraphs is a steadily emerging structural relationship between nodes that is quantified by changes in eccentricity and the clustering of the nodes.
We also used subgraph mining to extract a finer picture of the local structure present within our cellgraphs. Through a multilevel analysis of the cellgraphs we can project a quantitative, sensitive, and rigorous fine structure on the global features extracted above. Searching the micro level space of the graph we find local structures that are not represented equally over the whole of the graph. In this way, functional components of the tissue, or modules, are identified. For example, a sample in which only a portion represents cancerous tissue might be averaged out and classified as inflamed or normal. However, through the use of subgraph mining, and local feature analysis, an area of densely connected cells would be identified as a specific tissue compartment with unique properties and lead to reclassification as cancer [23, 24, 37]. We identified subgraphs or motifs from the cellgraphs that were significantly different from those that were frequently extracted from random graphs. Again, this indicates that there is an inherent structure that is specific to our cellgraphs and is not characterized by a random distribution of nodes in space.
Over time these subgraphs became increasingly complex and incorporated nodes with higher degrees and therefore more interaction with neighboring cells, consistent with the conclusion from the global features. In addition, the frequent subgraphs appeared at specific points in time, and not all subgraphs were present at all time points for all densities examined in this study. We hypothesize that the formation of distinct local structures occurs in a specific temporal order. The time evolution of our subgraphs indicates that there is a “route” that a population of cells takes while interacting with and organizing a naïve matrix, and if we change a fundamental property of that population, then we change the rate at which the “tissue” is able to complete that “route.” This hypothesis was confirmed by quantifying the frequency of subgraph occurrence as a function of time. When compared across the two densities, we observed that the appearance of new subgraphs in the less dense sample at late time points consistently correlated with high frequencies of those same patterns at earlier time points in the dense sample. We conclude that a population of cells follows a consistent organizing pattern over time, and while the rate of that organization can be altered by changes in the cell population, the route or order in which that organization takes place remains constant.
Point pattern analysis and its variants [31, 38] focus on spatial analysis of points (cells in our case), whereas to define the “tissue structure” one needs to model cellcell (pointtopoint) relationships. The most relevant work to the cellgraph approach is a Delaunay graph of cells obtained from a processed tissue image to compute graphtheoretical features for tissue quantification [28–30]. In this approach, nuclei are the vertices, the Voronoi diagram of the image is constituted, and its Delaunay triangulation is built. The Delaunay triangulation allows the existence of edges between only the adjacent vertices, such that only the relationships between closely located nuclei are represented. There are two main limitations of Delaunay graphs that cellgraphs successfully remedy. First, Delaunay graphs are restricted to planar graphs which are very limited in their structure and do not allow crossing of edges. There is no evidence to justify such a limitation in 3D tissue structural organization. Second, a Delaunay graph has a single connected component (i.e., the tissue is represented by a connected graph) which may not be a valid assumption for sparse tissues. Third, the girth of a Delaunay graph is always a triangle which is also a special case. Thus, the cellgraphs are a generalization of Delaunay graphs to arbitrary edge functions that can provide formulation of different cellcell interactions and eliminate such constraints. Furthermore, our previous work [39] reports on a comprehensive comparison between graphbased metrics and spatial distributionbased approaches, showing that the former has greater predictive power when coupled to machine learning approaches.
Therefore, there are several advantages of our cellgraph approach to tissue modeling: First, cellgraphs enable us to benefit from well established principles of graph theory and provide a rich set of features defined precisely by these principles to be used as quantitative descriptor features. These features could be defined and computed locally from a single node’s point of view (e.g., number of its neighbors) or globally for the entire tissue sample (i.e., the shortest or longest distance in the cellgraph between any two nodes). Second, cellgraphs benefit from sophisticated segmentation algorithms that can provide cell level attributes such as convexity, size, physical contact, and shape. to establish links between a pair of nodes. Furthermore, molecular details of a particular cell type (e.g., is it diseased?) do not need to be resolved, and a specific textural change in the image is not required. Third, cellgraphs provide a precise mathematical representation of cellular organization and the ECM that surrounds cells. If the images carry multichannel information by applying more sophisticated staining techniques (e.g., multispectral fluorescence imaging), it is possible to build cellgraphs that have different types of nodes corresponding to different types of cells that coexist (e.g., epithelial versus fibroblast) and other ECM entities (e.g., basement membrane underlying epithelial cell layers and blood vessels). With 3D images and 3D cellgraphs, such representation becomes more accurate and powerful.
5. Conclusions
The demonstration of higher order in biological structures is evidence of recurring principles that govern the design and therefore development of metabolic networks, proteininteractions, neural circuitry, and tissue. Cells interact with one another and their extracellular environment in nonrandom, defined patterns, and these patterns are consistent in terms of their spatial and temporal organization. Understanding the temporal order of this patterning provides organizing principles that can be used to help biologists and tissue engineers understand or optimize processes of natural and synthetic tissue development.
Acknowledgments
This work was supported in part by the National Institutes of Health, Grant no. RO1 EB008016 and no. RO1 AR053231. The first and the second authors contributed equally to this work.
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Copyright
Copyright © 2009 A. W. Lund et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.