The concept of robustness of regulatory networks has received much attention in the last decade. One measure of robustness has been associated with the volume of the feasible region, namely, the region in the parameter space in which the system is functional. In this paper, we show that, in addition to volume, the geometry of this region has important consequences for the robustness and the fragility of a network. We develop an approximation within which we could algebraically specify the feasible region. We analyze the segment polarity gene network to illustrate our approach. The study of random walks in the parameter space and how they exit the feasible region provide us with a rich perspective on the different modes of failure of this network model. In particular, we found that, between two alternative ways of activating Wingless, one is more robust than the other. Our method provides a more complete measure of robustness to parameter variation. As a general modeling strategy, our approach is an interesting alternative to Boolean representation of biochemical networks.
Developing models with a large number of parameters for describing the dynamics of a biochemical network is a common exercise today. The dependence of predictions of such a network model on the choice of parameters is important to understand for two reasons. For the purpose of fitting biological data and making predictions, we need to know which combinations of parameters are strongly constrained by observations and also which combinations seriously affect a particular prediction. In addition, we expect naturally evolved networks to be somewhat robust to parameter changes. If the functioning of the network requires fine-tuning in many parameters, then mutations causing changes in regulatory interactions could quickly make the network dysfunctional. For predictions involving gene products being ON or OFF, we found a method that facilitates the study parameter dependence. As an example, we analyzed several competing models of the segment polarity network in Drosophila. We explicitly describe the region in the parameter space where the wild-type expression pattern of key genes becomes feasible for each model. We also study how random walks in the parameter space exit from the feasible region of a network model, allowing us to compare the relative robustness of the alternative models.
Citation: Dayarian A, Chaves M, Sontag ED, Sengupta AM (2009) Shape, Size, and Robustness: Feasible Regions in the Parameter Space of Biochemical Networks. PLoS Comput Biol 5(1): e1000256. doi:10.1371/journal.pcbi.1000256
Editor: Adam P. Arkin, Lawrence Berkeley National Laboratory, United States of America
Received: October 23, 2007; Accepted: November 17, 2008; Published: January 2, 2009
Copyright: © 2009 Dayarian 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.
Funding: EDS's work was partially supported by National Science Foundation grant DMS-0614371 and Air Force Office of Scientific Research grant FA9550-08. AD and AMS's work was partially supported by a National Human Genome Research Institute grant R01HG03470.
Competing interests: The authors have declared that no competing interests exist.
Robustness, in the context of biological networks, broadly indicates that the system remains viable under different perturbations. Defining robustness in a precise form is a challenging task, given that robustness to different kinds of perturbations, e.g., environmental variation, intrinsic fluctuations in chemical networks or changes due to mutations, might involve different features of an existing network ,. In this paper, we are concerned with the robustness of functionality to changes in the kinetic parameters for a given network architecture. In an influential study of the Drosophila segment polarity network, robustness has been associated to the fractional volume of the region in parameter space associated with the wild type gene expression pattern . In this paper we will see that the geometry of the space of feasible parameters contains additional information on essential aspects of robustness and fragility of the network.
In the context of fitting biochemical kinetics models to time series data, investigators have looked at effects of small parametric perturbations on the quality of the fit. Sensitivity analysis ,, namely considering the effect of changing parameters, one at a time, is a common practice by now. Brown and Sethna have looked at correlated changes of parameters and study how moving in different directions in parameter space affects the predictions . Based on the eigenvalues and the eigenvectors of the Hessian of the cost function at the minimum, these authors and their collaborators find that, for many known biochemical networks, only a few directions in the parameter space have stiff constraints whereas the rest of the directions are “sloppy” ,. In this work, we will consider the segment polarity network as an example and will explicitly characterize the region in parameter space where the network could be functional. The anisotropy in the shape of this feasible region will become apparent from our analysis. We should clarify that the robustness of a model to parameter variation, as measured by goodness of fit to data, is distinct from the robustness of the system functionality with respect to parameter variation from mutations. However, at a mathematical level, these two problems just give rise to different ways of scoring parameter choices for a model, and there is much that is parallel in the consideration of the shape of the regions that score well in each of these problems.
The segment polarity network is part of a cascade of gene families responsible for generating the segmentation of the fruit fly embryo. Genes involved in initiating this pattern are transiently expressed, and interactions among the segment polarity genes should maintain and fine-tune this pattern as the embryo grows through cell division. Much of the information about this network comes from genetic analysis and are therefore of qualitative nature. In particular, we do not know many of the parameters necessary to describe this dynamical system. This is a common situation faced in modeling most biochemical networks.
In their work on modeling the segment polarity network, von Dassow et al.  encountered the same problem. Their approach was to solve an ODE model of the network for random choices of parameters and then score the resultant expression patterns based on compatibility with the experimentally observed wild type pattern. If this score is found to be above a certain threshold, the given parameter combination is said to belong to the feasible region of the parameter space. Robustness of a particular architecture is then ascertained by the fractional volume of the feasible region, estimated from their simulation. Ingolia  looked at a set of criteria for bistability in particular submodules of the network and studied the extent to which these criteria describe this feasible region. In general, providing an approximate description of the structure of feasible region, even for a medium size biochemical network, remains an important challenge.
One could also get some insight into the functioning of the network by constructing a model where each gene or gene product is mostly ON or OFF. For example, in the context of this particular network, Boolean models have been employed to study dependence upon initial state or the effect of deletion of particular components . Unfortunately, addressing questions related to parameter dependence is not possible within the conventional Boolean framework. Therefore, we develop a new approximation, within which the treatment of our model shares the simplicity of Boolean analysis without sacrificing the possibility of exploring parameter dependence issues. This approximation enables us to explicitly characterize the feasible region in the parameter space of the model.
If a point in the feasible region of parameters represents a functional biological system, then a mutation causes the system to jump to a new point. If this new point also belongs to the feasible region, the system is robust with respect to that mutation. Otherwise the mutation is deleterious. If the jump in the parameter space, caused by a mutation, is relatively large then the result of successive mutations is to quickly probe different regions of the parameter space. In this case, robustness essentially depends on the volume of the feasible region. On the other hand, if the jumps in the parameter space are relatively small, evolution of parameters due to successive mutations can be represented by a random walk in the parameter space. The idea of representing evolution as a continuous random process has already been used in the adaptive landscape approach . In this case, the random walk exiting the feasible region in the parameter space corresponds to a deleterious mutation. The exit time distribution is very sensitive to the shape of the feasible region. Robustness to mutation is, now, related to the features of this distribution (e.g. half-life, asymptotic decay rate, etc.)  and therefore depends upon the shape and not just the volume of the feasible region.
If we want to choose a single measure for robustness, the inverse of the asymptotic decay rate is a good candidate . This measure is sensitive to the geometry (both volume and shape) of the feasible region. For example, even if the total volume of the feasible region is relatively large, existence of “narrow” directions will greatly affect the decay rate; or if the feasible region is constituted of several disconnected part, the decay rate will again be affected. In addition, it is independent of the initial condition. Also, in the theoretical case, where every mutation leads to a new, uncorrelated point in the parameter space, the inverse of the asymptotic decay rate is a simple function of the fractional volume of the feasible region.
In our study, we will estimate half-life, a different but closely related measure of robustness. In case a single exponential in time gave the probability of remaining in the feasible region, these two measures of robustness would be proportional to each other. In practice, half-life depends partially on short time properties of the system and is initial condition dependent. On the other hand, measuring the asymptotic decay rate accurately for high dimensional stochastic system needs more computational effort than estimating half-life.
Before we go on, let us explain what measure of distance we use when we talk about narrow or wide directions in the parameter space. If we consider the continuous random walk approximation to parameter evolution, then the short-time properties of diffusion set up a metric for the space of parameters. The metric tensor of this space is the inverse of the covariance matrix of infinitesimal displacements divided by the infinitesimal time interval. Once we have this metric, we could decide whether, from a generic point, the distance to reach the boundary in certain direction is relatively small or large. This definition of distance is closely tied to the time the system typically takes to diffuse over a certain separation.
Once we characterize the feasible region in parameter space, we explore how the system fails as a result of such a random walk. For two alternative network models, we compare the exit time distributions. More importantly, we can see how, in a particular model, the feasible region is narrower in certain directions than in others. These narrow directions are associated with the predominant modes of failure of the system in the random walk process. We end by speculating how these methods could be extended to generic biochemical network models.
In the wild type segment polarity pattern, genes are expressed periodically in 14 parasegments along the fly embryo, and each parasegment consists of four stripes of cells. Because of this periodicity, one could focus only on one parasegment or in other words only on 4 cells. Figure 1A shows the wild type gene expression pattern for three key components of the segment polarity network. For simplicity, each cell is assumed to have four faces, rather than six as in the original model . When using abbreviated names for components of the network, we use uppercase letters to refer to proteins and lowercase letters for the corresponding mRNAs. Wingless (WG) is a signaling molecule known experimentally to activate Engrailed (EN) through cell-to-cell communication. EN, itself a transcription factor, in turn triggers the production of another signaling molecule, Hedgehog (HH). HH then gets secreted to the neighboring cell and maintains WG expression by stabilizing an activator of wg, called Cubitus interruptus (CI). Without HH signaling, CI gets proteolytically cleaved, leaving only its amino terminus (denoted by CN), which becomes a repressor of wg. In summary, experimentally it is known that WG and EN maintain the expression of each other through cell-to-cell communication. We represent the wild type expression pattern of these mRNA components as follows:(1)where the four entries of each of the vectors correspond to the gene expression in the four cells of a parasegment. The value “0” means the gene is turned off and the value “1” means it is maximally expressed.
(A) Four cells in a parasegment with periodic boundary conditions in both dimensions. Each cell is represented by a square. The convention for numbering cells and cell faces are shown. (B) Interaction network used in reference . Two green lines indicate interactions added by authors to achieve the target pattern. Black lines indicate interactions based on experimental data. Shape of the nodes indicates the corresponding component: Ellipses represent mRNAs; rectangles, proteins.
The abovementioned mechanisms leave room for the following questions. Why is EN expressed only posterior to the WG expressing stripe? The anterior cell also receives a WG signal but does not produce EN. Similarly, one could ask why WG is expressed only anterior to the EN expressing stripe.
Figure 1B shows the interaction network used in reference . In that work, the authors started only with interactions shown by black lines but were unable to reproduce the right pattern in their simulations. The best pattern authors could achieve, using only black lines, was an alternative expression of wg and en in all cells. Therefore, authors decided to add two new interactions shown with green lines. With these links in place, they were able to find many parameter combinations to reproduce the target pattern.
To explore the dependence of robustness of the network on its topology, Albert and Othmer  developed a Boolean model of the segment polarity network, a discrete logical model where each species has only two states (OFF or ON), but no kinetic parameters need to be defined. This Boolean model is amenable to various methods for systematic robustness analysis , –. Unfortunately, the ease of analysis comes at the cost of not being able to address questions related to the parameter dependence.
A Step Function Approach to the Segment Polarity Network Model
We propose an approach which retains the information about kinetic parameters, but, at the same time, keeps part of the simplicity of a Boolean model by having most genes either in the fully ON or the fully OFF state. We approach the problem by first solving the algebraic equations coming from the steady state conditions and writing the steady state solutions in terms of the parameters. Since one of the steady state solutions should match the wild type pattern, one can look for the constraints on parameters that yield this pattern. This procedure provides a family of conditions defining regions of feasible parameters for the wild type steady state. Although all of the parameters in the feasible region can maintain the desired pattern, one aspect we ignore is whether the system can reach the wild type pattern from particular initial conditions.
In our analysis, we used the fact that many of the differential equations in the model involve terms of the Hill form:where X is the concentration of some species, κ is the dissociation constant and ν is the Hill coefficient. The steepness of the Hill function is characterized by the Hill coefficient ν. As X increases from zero and passes the threshold κ, the function φ has a transition from OFF to ON state. For moderately large Hill coefficient, this transition becomes quite steep, and φ is practically insensitive to the actual value of ν. In the model presented in reference , ν is indeed found to be often quite large, between 5 to 10 . Any such term may thus be replaced by a step function with two levels:
Here we use the same notation as in . Xi, i = 1,2,3,4, denotes the total concentration of the protein species X in cell i, with lower case xi referring to the concentration of the corresponding mRNA molecules. In addition, for three of the components involved in cell-to-cell communication, namely, external Wingless (EWG), Patched (PTC) and HH, the concentration on each of the four cell faces could be different. For any of these components, the concentration in cell i at face j is denoted by Xi,j, i = 1,2,3,4, j = 1,2,3,4. For these three species, the sum of the concentration over all four faces of cell i is denoted by Xi,T. The adjacent cell face to face j of cell i is shown by Xi,lr. The opposite cell face to face j of cell i is shown by Xn,j+2.
Also, κXY denotes the dissociation constant for species Y corresponding to the binding that regulates the species X. The range for κXY is chosen to be between zero and one. The equations are in normalized form, meaning that the concentrations of the components have been scaled so that the maximal steady state level is one.
The structure of this particular network allows one to draw several interesting conclusions immediately. For example, the steady state levels for HH and PTC are completely determined once one specifies the mRNA levels of en, hh and ptc (this does not depend on the high Hill coefficient approximation). Assuming that en and hh are expressed only in the cell 3, which is the case in the wild type pattern, it can be shown that ptc2 = ptc4, and PTC2,T = PTC4,T. The reason is as follows. If ptc2>ptc4, cell 2 ends up producing more PTC, part of which get bound to HH diffusing over from cell 3. However, the symmetric nature of the diffusion leads to more PTC in cell 2 than in cell 4: PTC2,T>PTC4,T. Higher level of PTC results in higher rate of proteolysis of CI. Therefore, in the steady state, CIi is a decreasing function of PTCi and CNi is an increasing function of PTCi. This means that (given en is not present in cells 2 and 4, and therefore has no repressive effect on ci production)(15)
However CI is an activator and CN is a repressor of ptc, which together with Equation 15 implies ptc2<ptc4, which contradicts the assumption we started with. Of course, we could have started with ptc2<ptc4 and again end up with contradiction (for the formal proof, see, Chaves, Sengupta and Sontag, Geometry and topology of parameter space: investigating measures of robustness in regulatory networks, to appear in Journal Mathematical Biology). This argument shows that the concentration levels of ptc, PTC, CI, CN and PH is exactly the same in cells 2 and 4:(16)
This observation will turn out to be quite significant for the following reason. The wg level in a cell is controlled by the CI-CN pathway and the postulated feedback  from internal WG (IWG). Since cells 2 and 4 do not differ when it comes to CI and CN levels, any difference in the WG expression has to be attributed to the wg autoregulation.
In order to analyze the wg sector, we note that, in this model, the EWG and IWG levels are uniquely determined by a set of linear equations once the wg levels are given. Solving these linear equations, using the periodic boundary conditions and the fact that wg is produced only in cell 2, we find that:(17)
This result is not surprising because the distribution of WG is determined by a symmetric diffusion process from the source in cell 2, the only wg producing cell in each parasegment. Therefore, we expect cells 1 and 3 to have identical amounts of WG signaling. It turns out that EWG at the source, cell 2, is higher than that of the flanking cells (the formal proof is presented in the supplementary material). These observations have important consequences for the regulation of en, as explained below.
Had the en production been solely controlled by EWG, the model would have implied that if EWG3 is high enough to activate en in cell 3, en will be also activated in cells 1 and 2. This is why, in reference , adding repression of en by CN was necessary to achieve the wild type expression pattern. The two new links introduced in reference  (green lines in Figure 1B) give rise to two positive feedback loops. The wg autoactivation gives rise to bistability, allowing cells 2 and 4 to have distinct levels of wg expression. The other loop (En __| ci→CI→CN __| en→EN), generated by adding repression of en by CN, is required to prevent en from being expressed in cells 1 and 2. This also requires CN to be expressed in those cells. The bistability of the EN-CI-CN system allows cells 1 and 3 to have different en level even when the external Wg signal is the same for both of them.
We should note that autoactivation as a way for maintaining the WG expression is problematic in the following sense. In the model described above, wg is always activated via autoactivation and the preexisted CI-CN pathway never contributes to the pattern. This is in contrast with the experimental data, which suggests that HH signaling from the neighboring cell plays a crucial role in maintaining the wg expression. The fact that model  does not depend upon HH signaling for maintaining the expression of wg manifests itself when cell division is considered. In this model, both daughters of a cell in the wg-expressing stripe are able to retain the wg ON state through autoactivation. This causes the stripe to grow wider and wider over cell divisions. However, in wild type fly, the wg-expressing stripe should remain one cell wide. The daughter cell, which is further from the en-expressing stripe, and therefore not exposed to HH signaling, loses wg expression. This means that one stripe of WG is left after each division. Ingolia  has also noticed that in this model, IWG level must always be above KWGwg (the autoactivation threshold) in the cell that expresses wg. When we removed the CI-CN cycle for activation of wg from the simulation performed in reference , the fraction of “good solutions” increased by a factor of 3. This suggests that most of the time the CI-CN pathway is either not contributing to WG expression or it leads to misexpression of WG in cell 4.
The model is too dependent on the bistability of the two sub-networks with positive feedback for maintaining four cell expression patterns. One could avoid this problem by making some of the four cells special, either by inclusion of other genes in the network or by explicitly breaking the symmetry via introducing different gene expression rates from cell to cell for some of the genes already in the model.
The major candidate for inclusion in the model is the Sloppy-paired protein (SLP) as has already been suggested by others ,,. SLP is only present in cells 1 and 2: . It is a necessary (but not sufficient) factor for activation of wg and it also represses en. In the presence of SLP, the reason en is not expressed in cell 1 despite WG signaling is that it is being repressed by SLP. Also, despite HH signaling, wg is not produced in cell 4 because SLP is not present there. With SLP added, the two new interactions introduced in  are not necessary anymore, and also WG expression will depend on the CI-CN pathway.
In this paper, we will analyze the effect of including SLP. We keep SLP as an external factor meaning that the expression pattern of SLP is given. However, it can easily be incorporated into the network. If WG activates SLP, a positive feedback loop is formed which allows for bistability: both WG and SLP can be ON or both can be OFF. On the other hand, if EN represses SLP, another positive feedback loop is formed which again allows for bistability: SLP can be ON and en OFF or vice versa. We have also explored a model with explicitly different rates of production of ptc and ci from cell to cell which will be presented in a separate publication (Chaves, Sengupta and Sontag, Geometry and topology of parameter space: investigating measures of robustness in regulatory networks, to appear in Journal Mathematical Biology). The work also presents a study complimentary to that presented in this paper. It provides an explicit geometric description of the feasible region by partitioning the region into components defined by algebraic inequalities, in other words, by constructing a cylindrical algebraic decomposition.
Here, we consider two particular cases:
- The regulatory network used by von Dassow et al. . This network is shown in Figure 2B. We will refer to this case as von Dassow et al. model.
- The regulatory network including Sloppy-paired protein, but without the two positive feedback links introduced in . This network is shown in Figure 2. We will refer to this case as SLP model.
In this model, the possibility of Wg autoactivation and en repression by CN is not included.
We can explicitly write down the conditions characterizing the feasible region for these two models. The results are presented in Tables 1 and 2 (see Materials and Methods for the derivation of these conditions). We could easily estimate the associated volume of feasible region by randomly choosing points in the parameter space and check whether they satisfy the appropriate conditions. As we discussed in the introduction, the fate of random walks, especially where they exit the feasible region, teaches us a lot about relative vulnerability of different constraints.
Random Walk in the Feasible Region
We explore the feasible region by following random walks starting from random points. Whenever one of the random trajectories hits a boundary and exits the feasible region, we terminate the walk and keep track of the inequality that was violated. This process can be viewed as a simulation of parameter evolution due to mutations in a fitness landscape that looks like a plateau. The points in the feasible region have a constant high fitness, and the rest of the points have zero fitness. The result of the simulation is presented in Figure 3.
We choose a random point from admissible parameter set and follow a random walk until it hits a boundary after t steps. (A) The red (and dashed) and the blue (and solid) graphs represent the probability of survival as a function of time for von Dassow et al. and SLP models, respectively. These graphs results from 30,000 runs of random walks. The results given for volume are based on the fraction of feasible parameter combinations found in 1,000,000 randomly chosen combinations. (B) Histogram of violated conditions for the random walk in (A). The number above each bin indicates the corresponding condition in Tables 1 and 2.
For the two models discussed, the graphs in Figure 3A show the probability of survival as a function of time. This is the probability that the random walk has not exited the feasible region in the first t steps. From the graph, we can easily measure T1/2, defined as the time for which there is a 50% chance that the system has already suffered a deleterious mutation. As we discussed in the introduction, this number is a possible indicator of robustness.
Figure 3B shows the histogram of violated conditions. The number below each bin indicates the corresponding condition in Tables 1 and 2. The lead cause of failure in the von Dassow et al. model is the constraint on κWGwg whereas in the SLP model it is the constraints on κEWGen. Higher vulnerability of the SLP model with respect to the constraint on κEWGen can be understood by comparing condition 3 in Table 1 and the corresponding condition in Table 2. In the SLP model there is a lower bound on κEWGen coming from the fact that κEWGen should be greater than EWG4 to prevent activation of en in cell 4. However in the von Dassow et al. model, en is being repressed by CN and therefore there is no lower limit on κEWGen.
One might raise the question of whether including repression of en by CN in the SLP model changes the constraints on κEWGen. In high Hill coefficient limit, adding this interaction does not change the conditions in Table 2. To see this, notice that as was mentioned before, requiring CI and CN levels to be different in cells 1 and 2 forces us to have CN2 = CN4 = 0. In cell 4, CN is not expressed, and in cells 1 and 2, en is already being repressed by SLP. Therefore, adding the possibility of en repression by CN does not change any of the constraints.
If we consider the case where Hill coefficients in the CI-CN-PTC sector are small, the transition from high to low in concentration value for ptc-nullcline and CN-nullcline would not be sharp. Instead, the transition would happen over a wide range. This means that we would get a non zero value for CN4. In that case, adding repression of en by CN can indeed help in maintaining the wild type pattern, thereby increasing the robustness of the model.
The parameters κCIwg, κCNwg and κWGwg are related to alternative routes controlling wg expression. The first two parameters play an important role in deciding WG expression in the SLP model, while this role is played by κWGwg in the von Dassow et al. model. Comparison of the frequency of failure for conditions 2 and 5 in the histogram in Figure 3B suggests that controlling wg via the CI-CN pathway in the presence of SLP is the more robust way of achieving the target gene expression pattern for wg.
What about adding the WG autoactivation to the SLP model? If one just cares about producing the right four-cell pattern for en, hh and wg, then this addition could give rise to more solutions. However, as we discussed before, not having wg production to be sensitive to HH signaling from the neighboring cell is problematic and gives rise to wide stripes of wg expression under cell division. If we constrain the model so that wg is sensitive to HH signaling via CI-CN pathway, we find that adding wg autoactivation to a functional solution in the SLP model often leads to misexpression of wg in cell 1 or cell 3, thereby shrinking the feasible region in parameter space.
Our results imply that the lack of robustness is not only dependent upon the size of the feasible region, but also upon the existence of critical directions along which this region is globally very narrow. We found relatively few constraints on the parameters given that we have specified the gene expression patterns for en, hh and wg in each of the four cells. Much has been said about the relation between the topology of the network and robustness. In practice, we found that it is not only the structure of the network but also the nature of the wild type expression pattern which plays an important role in the ultimate simplicity of the constraints that dictate robustness. For example, the fact that only one cell is expressing en and hh and that wg had no direct effect on the CI-CN-PTC sector allowed us to draw several conclusions about certain variables being the same in cell 2 and cell 4. If one only pays attention to the network structure, wg indeed has an effect on the CI-CN-PTC sector via its effect on en. However, specifying the en expression pattern hides the influence of wg and helps us disentangle the constraints. The role of wg shows up only when one insists upon self-consistency, namely, the wg expression pattern is going to lead to the target en expression pattern. Simplicity of the final constraints is not a result of some obvious modularity in the network itself but some combination of the network structure as well as of the sparseness of the expression pattern. We cannot be sure that this is a general feature of robust genetic networks. A broader study, which takes into account the role of the wild type pattern on the robustness of a network, would be a welcome deviation from discussions centered purely on network architecture.
We noted that capturing the CI-CN-PTC negative feedback in the Boolean model is difficult. For example, in the Boolean model constructed by Albert and Othmer , they are forced into a situation where ptc mRNA is OFF but PTC protein is ON. This is achieved because of an exception made in PTC production rule, namely, PTC can continue to be in the ON state even if there is no ptc. Of course, this implausible rule results in a distribution of ptc and ci products which mimics the wild type pattern. For example cell 1 has less ptc but more CN compared to cell 2. In our model, we partially capture the effect of the feedback. We can indeed get the ptc levels to vary between cell 1 and cell 2. Unfortunately, we saw that in the high Hill coefficient model, producing different CN levels requires fine-tuning of the parameters. Therefore, we understand why von Dassow et al. find that setting the Hill coefficients in the CI-CN-PTC sector to be small enhances their chance of finding good solutions .
The present approach shows that, in addition to volume, the topology and geometry of the feasible region have important consequences for the robustness of a system. Of special interest is the structure of the boundary in the parameter space that separates between functional and non-functional systems. In the models studied here, it was possible to describe this boundary explicitly as a collection of constraints. For a generic biochemical network model with a scoring function it may not be feasible to explicitly write down the boundary surface corresponding to the threshold of functionality. However, one could generate a sampling of the boundary surface by following random walks in the parameter space until it hits the boundary of the functional region (decided by a threshold score). Instead of what we did in this study, we could slightly alter our strategy and let the walk be reflected off the boundary. In that process the same walk would hit many neighboring points on the boundary surface. If one generates a large enough sample of boundary points, one could use methods like manifold learning , to approximately reconstruct the boundary.
Contrast this method to boundary reconstruction from uncorrelated random sampling. One could generate many points some of which are inside the region and many others that are outside. Indeed, many machine learning techniques for classification involve learning decision boundaries from such data. However, when the good region has a very small fractional volume and many of the randomly sampled points outside this region are far from the decision boundary, most of the sampled points have very little impact on boundary reconstruction. The uncorrelated nature of the sampling is useful for getting a good estimate for the fractional volume, but makes the process of mapping the geometry inefficient. It would be better to take advantage of one good solution to generate other good ones for the purpose of exploring local geometry.
Whether these approaches work for analyzing biologically motivated network models remains to be seen. For an arbitrary random network, with an equally arbitrary random choice of gene expression pattern, the feasible region could have a very complex structure and the methods outlined would not be particularly useful for characterizing it. The hope is that, for biologically relevant networks with wild type gene expression patterns, the feasible region may be quite simple, geometrically, and could be approximately described by the approaches suggested above.
To summarize, our analysis of the segment polarity network provides us with insights regarding the constraints that are crucial for functioning of the system. We showed how the system is particularly vulnerable to parametric perturbations in certain directions in the parameter space. We believe that the ideas developed here could be applied to other regulatory networks, to explore how the shape of feasible region in the parameter space contributes to its robustness. Hill terms appear often in models of biochemical networks. A simpler model, obtained by replacing these terms with step function, could be useful, because such a model enjoys some of the simplicity of the Boolean networks, while retaining many of the parameters of the original model.
Materials and Methods
Derivation of Conditions Characterizing the Feasible Region
Here we analyze two particular cases:
- The regulatory network used by von Dassow et al.  which we refer to as von Dassow et al. model (Figure 2B).
- The regulatory network including Sloppy-paired protein, but without the two positive feedback links introduced in . We will refer to this case as SLP model (Figure 2).
We first focus on case I. Equations 2–14 characterize this network. The wild type expression pattern for wg, en and hh is given in Equation 1. Since en is only expressed in cell 3, ci and ptc are expressed in all cells except cell 3:(20)
This is because in the absence of EN, ci is basally expressed which also leads to production of ptc. We will allow Ti to take values between zero and one. The reason for the special, non-Boolean, treatment of ptc has to do with capturing the effect of the negative feedback loop in the CI-CN-PTC sector properly. This negative feedback loop leads to lower ptc level in cell 1 than in cells 2 and 4, as we shall see. The ptc level in cells 2 and 4 turn out to be comparable (T2 = T4). This is also the experimentally observed expression pattern of ptc .
How could we ever get such an intermediate values in our approach? First, from Equations 13 and 14, in the cells where en is not expressed and therefore ci is not repressed, namely in cells 1, 2 and 4, we have CI+CN = 1⇒CI = 1−CN (this does not depend on the high Hill coefficient approximation). Since ptc is regulated by CI-CN, we could draw one nullcline expressing ptc concentration as a function of CN. This curve is represented by the green graph in Figure 4. We will call it the ptc-nullcline. Here it is assumed that the negative feedback on ptc coming from repression by CN is active. This means that CN and ptc are not expressed maximally. For ptc to be expressed, the activation by CI requires 1−CN>κCIptc⇒CN<1−κCIptc. In addition, we need CN to be smaller than κCNptc to avoid repression of ptc by CN. Thus, for values of CN smaller than the threshold of min(1−κCIptc, κCNptc), ptc is fully expressed. As CN passes this point, the value of ptc will drop sharply. In the high Hill coefficient limit, ptc will abruptly fall to zero.
The green curve shows the ptc-nullcline. In the high Hill coefficient limit, ptc value drops sharply from one to zero as CN passes the threshold of min(1−κCIptc, κCNptc). Blue and red curves show the CN-nullclines for relatively higher and lower values of HH signaling levels, respectively. Intersection points 1 and 2 determine CI, CN and ptc in cell 1 and 2/4, respectively. Here it is assumed that the negative feedback on ptc coming from repression by CN is active. Therefore, ptc and CN are not maximally expressed. Dashed blue line shows the CN-nullcline for a fine-tuned set of parameters.
On the other hand, CN production itself is dependent upon PTC protein. PTC is a monotonically increasing function of ptc and a decreasing function of HH signaling. Therefore, for a fixed value of HH level, we can also look at the concentration of CN as a function of ptc. This provides us with the CN-nullcline which depends upon the HH signaling strength. If we think of CN as a function of ptc level, the transition in CN from low level to its highest value happens at a particular ptc threshold, where the PTC level is just enough to start producing CN. If the cell is exposed to more HH signaling, sequestering away a larger fraction of total Patched protein, one needs more ptc to reach this threshold. The blue and the red graphs in Figure 4 show the CN-nullclines for relatively higher and lower values of HH signaling levels, respectively.
Because cell 1 receives less external HH signaling than cells 2 and 4, generally the red curve could be associated to cell 1 and the blue one to cells 2 and 4. The intersection points 1 and 2 determine CI, CN and ptc level in cell 1 and 2/4, respectively. As we see, ptc value could indeed be higher in cell 2 than in cell 1. However, CN concentration seems to be comparable in those cells. This is an artifact of our model where Hill coefficients are very large, which causes the transition from high to low in concentration value to happen in a very narrow range. The only way to have CN2 to be non-zero but different from CN1 is to be in the situation where the CN-nullcline for cell 2 is like the dashed blue line in Figure 4. In this case, the ptc threshold for CN production in cell 2 is fine-tuned to be very close to maximal ptc level. In a model with small Hill coefficients in the CI-CN-PTC sector, we would get CN1>CN2 and ptc1<ptc2 without such fine-tuning. We will come back to this point later.
We should point out that, in this study, we lay down the conditions only on the expression levels of key components en, wg and hh as specified in Equation 1. The reason, other than the simplicity of analysis, is that we believe the requirement of proper segment formation lays much stronger constraints on these key components compared to the rest. It is not clear to us that the CI-CN-PTC negative feedback has an extremely important role in segment formation stage of development. The study of von Dassow et al.  also uses a scoring function which rewards wild type levels only for these key components.
Having specified the requirements of functionality, let us now analyze what conditions are laid on the parameters of the model. Table 1 shows the set of inequalities characterizing the feasible region in the parameter space. Here we present the arguments leading to these conditions. The presence of EN in cell 3 requires the WG signaling for this cell to be above the activation threshold for en. This requirement is condition 3 in Table 1 (recall that κXY can take value only between zero and one). Also, in this cell, EN will shut off the expression of ci (Equation 12) which is necessary for the production of CI, ptc, PTC and PH. Therefore, none of those components are expressed in cell 3. In cells 2 and 4, the expression level of these components has been shown to be the same (Equation 16). Therefore, we only need to focus on the expression of these components in cells 1 and 2.
Let be the PTC level corresponding to the maximal ptc mRNA (ptc = 1) in cell i. If the threshold to produce CN is above , then cell i would not produce CN. As we pointed out before, the presence of CN in cells 1 and 2 is essential to repress en in those cells. These facts together necessitate condition 1 in Table 1.
What would the CN level in cells 1 and 2 be when condition 1 is satisfied? As one sees from Figure 5A, there are two possibilities depending upon whether min(1−κCIptc, κCNptc) is smaller or larger than . The case corresponding to ptc-nullcline in solid green has been discussed before. This is the case where ptc levels are affected by the negative feedback, and CN level is equal to min(1−κCIptc, κCNptc), which is less than its maximal possible value of . When the ptc-nullcline is like the dashed green line in Figure 5, CN levels in both cell 1 and cell 2 is equal to the maximal amount of , which is lower than min(1−κCIptc, κCNptc). In this case, the negative feedback is not active and ptc is maximally expressed (ptc = 1). We conclude that CN level is given by , which we call ZC. We will now discuss the conditions to be satisfied by ZC for proper expression pattern of en and wg.
(A) Blue and red curves show the CN-nullclines for relatively higher and lower values of HH signaling levels, respectively. The green curve shows the ptc-nullcline when . In this case, the negative feedback on ptc coming from repression by CN is active. Therefore, ptc and CN are not maximally expressed. The dashed green curve shows the other case where . In this case, both CN and ptc are maximally expressed. This means that the negative feedback on ptc is inactive. (B) The green curve shows the ptc-nullcline. Blue and red curves show the CN-nullclines for relatively higher and lower values of HH signaling levels, respectively. The blue curve shows the situation where HH signaling is strong enough so that the ptc concentration needed to produce CN is higher than the maximal possible value for ptc, namely, one. Therefore, CN will not be produced in the corresponding cell. In the high Hill coefficient approximation, this is the only way that we can have CN level in cell 2 (intersection point 2) to be different from cell 1 (intersection point 1).
The en repression in cells 1 and 2 gives rise to condition 4 in Table 1. The fact that CI-CN pathway should not activate wg in cell 4 is guaranteed by condition 2 in Table 1. Consequently, WG in cell 2 has no contribution from CI-CN pathway (remember that cells 2 and 4 have the same CI and CN levels) and is solely produced by the autoactivation term. The autoactivation should only operate in cell 2 and nowhere else. This is condition 4 in Table 1.
von Dassow and Odell analyzed randomly generated solutions for the segment polarity model in reference  and plotted the marginal distribution of parameters (see Figure 6 of ). We can relate their results to the constraints presented in Table 1. From condition 1, we expect κPTCCI to have tendency for lower values. From condition 2, we expect κCNwg to have tendency for lower values and κCIwg for higher values. Also, in order to have higher values for ZC, we expect κCIptc to have tendency for lower values and κCNptc for higher values. From condition 3 and 4, we expect κEWGen and κCNen to have tendency for lower values. From condition 5, we expect κWGwg to have tendency for intermediate values. These expectations agree qualitatively with the results presented in Figure 6 of .
From Figure 6 of reference , we see that many of the parameters are uniformly distributed. One should note that a uniform distribution for a certain parameter could arise from two different scenarios. It could be the case that changing the parameter over a wide range of values does not influence the final outcome of the network. The other possibility is that the effect of changing the particular parameter could be compensated by changes in other parameters in such a way that for each value of the parameter, there is roughly equal number of solutions.
Now, let us contrast these set of conditions to the one obtained for the SLP model. Table 2 shows the conditions defining the feasible region for this case. For this regulatory network (Figure 2), instead of Equations 2 and 5, we have:(21)(22)
The rest of equations are the same as before (Equations 3, 4 and 6–14). Since SLP is present only in cells 1 and 2, wg has the possibility to be expressed only in those two cells. The decisive factor is CN levels in cells 1 and 2 (remember that, in these cells, CI = 1-CN). In the wild type pattern, wg is expressed only in cell 2 and this means that CN levels cannot be the same in cells 1 and 2. The only way to have less CN in cell 2 compared to cell 1 is to have . The condition corresponds to the plateau in the CN-nullcline for cell 2 being higher or equal to the maximal ptc level (blue graph in Figure 5B). When it is higher, CN2 is zero and when it is fine-tuned to be equal, CN2 is between 0 and 1. If we had , given that , we would have CN1 = CN2 = 0. This is inconsistent with our requirement that CN1 and CN2 be different. Therefore, we have . For our discussion, we will ignore the fine-tuned cases, leaving us with condition 1 in Table 2. This mean CN2 = 0 and which we again call ZC. The condition 2 in Table 2 guarantees the absence of wg in cell 1. The fact that external WG signaling has to be strong enough in cell 3 to activate en but has to be weak enough in cell 4 not to produce en is coded in the condition 3 of Table 2.
Random Walk in the Feasible Region
To get an estimate for the fractional volume of feasible region in the parameter space, we randomly chose 106 parameter combinations and checked if they satisfy the conditions given in Tables 1 and 2 for the corresponding model. We perform the random walk by first selecting a random point, P0, from the set of admissible parameters and follow successive random perturbations . Each component of is selected from an independent Gaussian distribution with a standard deviation of 2*10−3. We follow this random walk until it hits a boundary and exits the space. This happens when one of the inequalities, which characterize the feasible region, is violated. Whenever the random walk exits the region, we record the time as well as the condition that was violated and therefore caused the exit. The parameter ranges were similar to those used in , except that we facilitated the transport processes for hh and PTC. We simulated the random walk for 30,000 runs.
AMS thanks Pankaj Mehta for discussions that lead to the formulation of the high Hill coefficient version of the segment polarity network model. We also thank Viji Nagaraj for carefully reading the final manuscript.
Conceived and designed the experiments: AMS. Performed the experiments: MC. Analyzed the data: AD MC EDS AMS. Contributed reagents/materials/analysis tools: AD MC EDS. Wrote the paper: AD MC EDS AMS.
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