Abstract
The restriction point marks a switch in G1 from growth factordependent to growth factorindependent progression of the cell cycle. The proper regulation of this switch is important for normal cell processes; aberrations could result in a number of diseases such as cancer, neurodegenerative disorders, stroke and myocardial infarction. To further understand the regulation of the restriction point, we extended a mathematical model of the RbE2F pathway to include members of the microRNA cluster miR1792. Our mathematical analysis shows that microRNAs play an essential role in finetuning and providing robustness to the switch. We also demonstrate how microRNA regulation can steer cells in or out of cancer states.
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Introduction
The Restriction Point (R) is a checkpoint in G1 that marks the transition from growth factordependent to growth factorindependent cell cycle progression^{1}. Most human cancers exhibit dysfunctional R^{2,3,4,5}, with many of the known genes involved in its regulation acting as either oncogenes or tumor suppressor genes (Fig. 1).
R is marked by an abrupt accumulation of the proproliferative members of the family of transcription factors E2F (namely, E2F1, E2F2 and E2F3) that induce expression of genes required for DNA replication^{6,7,8}. Using fluorescent reporters for E2F transcriptional activity in single cells, Yao et al.^{9} provided the first invitro demonstration that R acts as a bistable switch–as predicted by the authors’ own analysis of a minimal model of the RbE2F pathway that involves positive feedback loops.
In a related study, Aguda et al.^{10} considered an autocatalytic protein module (composed of E2F and cMyc) coupled with the microRNA cluster miR1792 via a negative feedback loop (e.g., E2F1 inducing expression of miR1792, and members of the latter inhibiting E2F1). The 2variable model analyzed by Aguda et al.^{10} – henceforth referred to as the ‘A model’ – elegantly predicted the role of miR1792 in tuning the sequence of cellular states, from quiescence to proliferation and to apoptosis. Furthermore, it was postulated that between normal cell proliferation and onset of apoptosis is a range of oncogenic activity (of E2F1 or cMyc) with significant probability of the cancer state; such a range is referred to as the ‘cancer zone’^{10}.
We extended the model of the RbE2F pathway analyzed by Yao et al.^{9} to include miR1792. This RbE2F pathway could generate a resettable bistable switch^{11}, with the kinetic parameters used by Yao et al.^{9} fitted with their experimental data. The model analyzed in this paper – which we call the R model (shown in Fig. 2) – provides a framework for analyzing the influence of miR1792 on the properties of the restriction point switch. We show that, as the microRNA inhibition efficiency is varied, the influence of miR1792 on the characteristics of the bistable switch of the R model match those of the A model. Furthermore, by showing that the R model allows for a comparative analysis of microRNA regulation of cMyc and E2F, we show that the R model offers predictions beyond those made by the A model.
There is growing evidence that microRNAs play an important role in the development and progression of various diseases^{12,13,14,15,16,17}. In this paper, we are interested in the role of microRNAs in conferring robustness to biological processes^{18,19,20,21,22}. One mechanism by which microRNAs perform this function is by buffering against noise in gene expression. Previous studies have investigated the buffering effect of noise by various microRNA canonical network motifs: positive and negative feedback^{23,24,25} and feedforward loops^{26,27}. The network of the R model (Fig. 2b) includes all these canonical network motifs. First, cMyc and the microRNA cluster form an incoherent feed forward loop in regulating E2F. Second, E2F induces a positive feedback on itself. Third, the microRNA cluster induces a negative feedback on cMyc and on E2F. And finally, cMyc and E2F form a coherent feed forward loop in regulating the microRNA cluster. Thus, the R model provides insights into microRNA buffering of noise that is more comprehensive than analyzing individual canonical network motifs. The R model could therefore help in further understanding the design principles underlying biological robustness.
Results
The R model is bistable
The R model is a mathematical representation of the network of interactions of Fig. 2 (see Methods). It is an extension of the model in Yao et al.^{9} with additional reactions involving the interactions between the miR1792 cluster and the RbE2F pathway. These new interactions include the inhibition of E2F by miR1792, which is well known^{8,28}, and the inhibition of Myc by the miR1792 cluster, which was recently shown to be via an indirect manner^{29}. Chek2 was found to be a target of miR1719b, and downregulation of Chek2 leads to increased recruitment of HuR/RISC to MYC mRNA, which inhibited Myc translation^{29}.
We hypothesized that the R model, like the Yao model, is bistable. To verify this hypothesis, we simulated a pulse experiment where a serum pulse was used to stimulate serumstarved and quiescent cells. Yao et al.^{9} used this experiment to show the history dependence of E2F expression on serum concentration. When a serum pulse of S = 20 μM was introduced for 5 hours and then was dropped to S = 0.8 μM, the E2F values proceeded to the on state even after the serum pulse was removed (Fig. 3a; the on state is E2F > 1.0 μM). In the absence of a serum pulse, E2F levels stayed within the quiescent zone or off state (Fig. 3b; the off state is E2F < 0.01 μM). These results demonstrate the history dependence of the R model. We repeated the simulations using a higher final serum level of S = 1.0 μM, and for the case with a serum pulse, the model behaved similarly as before (Fig. 3a,c). However, when there was no serum pulse, the system switched to the on state (Fig. 3b,d). This history dependence of the R model is a hallmark of a bistable switch.
The bistability of the R model can be analyzed by determining the stability of its equilibrium points (Methods). By calculating the equilibrium curve of the model variables with S as a parameter and all other parameters fixed (Fig. 3e,f), we found that the equilibrium curve of E2F had similar properties to those of the equilibrium curve of protein p of the twodimensional A model^{30}. The curve was “Sshaped” and had a region in which the system had two stable steady states (Fig. 3e). The equilibrium curve of cyclinD also included a region where the system had two stable steady states, but the two states were too close to each other making them distinguishable (Fig. 3f). This agrees with experimental observations where the histogram of single cell measurements of cyclinD did not show a bimodal distribution^{9}.
We also hypothesized that the R model has an excitable state. This is a state where, the input pulse can drive the system to the on state, but due to the insufficiency of either the magnitude or time duration of the serum pulse, the system returns to the off state after a short period. The A model has been shown to have an excitable state^{30} and the R model also exhibited this property (Supplementary Fig. 1).
For a system with relatively stronger microRNA inhibition (Fig. 3a–d, orange and green lines), the E2F values at steady state deviated from those of the plots with no or weak microRNA inhibition (Fig. 3a–d, red and blue lines). This shows one manner in which the microRNA cluster can finetune the RbE2F network, which will be analyzed in detail below.
MiR1792 feedback inhibition confers robustness to the RbE2F pathway
A population of cells synchronized at the same cell cycle phase can exhibit celltocell variation due to stochastic events. Within the RbE2F pathway, these stochastic events could come from mRNA degradation or translation, or from celltocell differences in protein concentrations, or other environmental factors. We incorporated these stochastic effects by adding noise terms to the R model and simulated the model within a population of 10,000 cells (Methods). For a cell population with a constant serum of S = 0.8 μM, the E2F levels exhibited a bimodal distribution when microRNA inhibition was absent or had low strength (Fig. 4a, orange, green, and cyan plots; Supplementary Tables 1 and 2). One mode was at the off state (around E2F < 0.01 μM) and another at the on state (around E2F = 1.0 μM). In the nonstochastic simulations, the constant serum level of S = 0.8 μM was not enough to switch the cells to the on state (Fig. 3b), hence the bimodal distributions in Fig. 4a indicate that noise within the pathway could cause the R switch to turn on in some cells. When microRNA inhibition was strong enough, the distribution was unimodal at the off state (Fig. 4a, purple plot), indicating that this microRNA inhibition strength was effective in guarding against stochastic switching.
When the constant serum level was high (S = 1.0 μM), the stochastic simulations showed a bimodal distribution but with very low numbers at the off state (Fig. 4c, orange, green, and cyan plots). The strongest microRNA inhibition (Fig. 4c, purple plot) was not enough to keep the cells within the off state. This agrees with the result in Fig. 3d, where the cells switched to the on state when a constant serum level of S = 1.0 μM was applied even if there was no serum pulse.
Next we repeated the stochastic simulation experiment but this time provided a serum pulse (S = 20 μM for the first 5 hours, Fig. 4b,d). At a final serum level of S = 0.8 μM, we expected the pulse to drive all cells to the on state (see Fig. 3a), but noise can prevent some of the cells from switching on (Fig. 4b, orange, green, and cyan plots show a few cells at the off state; Supplementary Tables 1 and 2). However, the strong microRNA inhibition counteracted the memory dependence of the system (on the serum pulse) since most of the cells did not switch on (Fig. 4b purple plot). When the final serum level was S = 1.0 μM, almost all cells switched on even with weak microRNA inhibition (Fig. 4d, orange, green, and cyan plots), but strong microRNA inhibition was able to keep a significant amount of cells in the off state (Fig. 4d, purple plot; Supplementary Tables 1 and 2).
To further understand the effect of microRNA regulation on the robustness of the system, we performed an analysis on how it affects noise amplification and noise susceptibility (Methods). Noise amplification measures the ratio between the noise in the output (the model output we consider is E2F and noise is defined as the coefficient of variation) and the noise in the input (coefficient of variation of S). On the other hand, noise susceptibility measures the relative change in the model output (E2F) in response to minute changes in the input (S). A previous analysis of noise amplification and susceptibility on the A model has shown that these two robustness measures had properties that depended on whether the system was at the on state or at the off state^{31}.
Here, we analyze three parameters, the microRNA inhibition parameters Γ_{E} and Γ_{M,} and the positive feedback parameter k_{E}, instead of two parameters analyzed in ref. 31 for the A model. We plotted results for two parameters at a time, keeping the values of the other parameters fixed (Fig. 5 and Supplementary Figs 2–6). In Fig. 5, the noise amplification values (SA) and noise susceptibility values (SS) were plotted for each value of Γ_{E} and Γ_{M}, with Γ_{E} on the xaxis and with each plotted line corresponding to a value of Γ_{M}. The noise amplification of variable E2F at the on state showed a local maximum with respect to inhibition parameter Γ_{E}, and trended upward after the peak (Fig. 5b). At the off state, the noise amplification monotonically increased as Γ_{E} increased (Fig. 5d). Thus there is a qualitatively different effect of microRNAs on noise amplification between the on and off states. We obtained the same qualitative difference between noise amplification at the on and off states when we plotted Γ_{M} on the xaxis (Supplementary Fig. 2).
When we paired the positive feedback parameter k_{E} with either Γ_{E} or Γ_{M}, we obtained an opposite effect at the off state where the noise amplification curves decreased with increasing values of k_{E} (Supplementary Figs 3–6). This demonstrates the opposing effects of the positive activation and negative inhibition parameters on noise amplification.
The noise susceptibility curves showed peaks at both on and off states (Fig. 5a,c) and one obvious qualitative difference between the two is that at the on state, the value of Γ_{E} at which the peak occurs decreases as Γ_{M} increases, while the opposite holds at the off state. This also seems to be true when Γ_{M} was plotted on the xaxis (Supplementary Fig. 2).
MiR1792 finetunes the RbE2F pathway in and out of the cancer zone
There are two experimentally observable variables associated with the ‘all or nothing’ switching behavior of the bistable restriction point switch. One variable is the value of the serum growth factor where the switch occurs, and the other is the magnitude of the jump by the E2F concentration to the on value (Fig. 6a). The significance of the magnitude of the on jump, as discussed in Aguda et al.^{8}, is that it determines whether the cell remains quiescent, proliferates, enters the cancer zone, or undergoes apoptosis. In the previous sections, we considered a coarse grained classification of the values of E2F, with E2F < 0.01 being off, and E2F > 1.0 being on. Now, we subdivide the on state into the following cell states: cell cycle, cancer, or apoptosis.
We first extended the switching behavior analysis of the 2dimensional A model to explore other possible model predictions that may carry over to the more complex R model. The parameters of interest in the A model are the microRNA inhibition parameter (Γ_{2}′) and the rate of protein production stimulated by the growth serum (α). The offon value is symbolized by α*, while the magnitude of the on jump is symbolized by ϕ* (Fig. 6a). When there was no microRNA inhibition (Γ_{2}′ = 0), the on jump was extremely large, resulting in cell death, even at very small values of α* (Fig. 6a). This indicates that the initiation of proliferation could be at the mercy of noise (again, this means no control of proliferation). Figure 6b,c show that as the microRNA inhibition parameter Γ_{2}′ increases, ϕ* decreases while α* increases, indicating that varying Γ_{2}′ hits both essential switching features (α* and ϕ*) simultaneously to the “right” values, (i.e., Γ_{2}′ can be used to decrease ϕ* to fall below the cancer region). Thus, α* and ϕ* are coupled, with an inverse relationship, and are optimally controlled by microRNA via the parameter Γ_{2}′.
We performed an analogous analysis for the R model using the microRNA parameters Γ_{M} and Γ_{E}. The experimentally observable variables associated with the allornothing switching behavior of the R model are S* and E*, which correspond respectively to the switch variables α* and ϕ* of the A model. The protein we observe for switching, as in the A model, is E2F since its concentration determines whether the switch will turn on or off. We found out that similar to the A model, when there was no microRNA inhibition (Fig. 6d,g dashed lines), the onoff value for the serum level, S*, was relatively small, while the on value E* jumps to the highest level, indicating that the cell fate of either normal proliferation or cell death is susceptible to noise. We also found that, similar to the A model, as the microRNA parameters (Γ_{M} or Γ_{E}) increase, S* increases while E* decreases (Fig. 6e,f,h,i). However, the rates of increase of S* and decrease of E* are qualitatively different from the A model. This indicates that by varying its rate of inhibition on either E or M, or both, the microRNA machinery has enough flexibility to finetune the R switch and to provide robustness against noise.
A comparison of Fig. 6e,h shows that Γ_{M} lowers the on value E* faster than Γ_{E}, suggesting that this parameter could be more useful in controlling the robustness of the system against noise. The inverse relationship between the microRNA inhibition efficiency and the on value agree with the numerical simulations of an engineered microRNA circuit which showed that a stronger microRNA repression corresponds to a smaller difference between the off and on states of the protein expression levels^{23}. Thus, Fig. 6 highlights the importance of the microRNA machinery in steering the cell fate by lowering the on value.
The R model is robust to changes in the microRNA associated parameters Γ_{E} and Γ_{M}
Now that we have gained some insights on how the miR1792 cluster can finetune the expression of its target genes in the RbE2F pathway, we ask how sensitive the RbE2F pathway is with respect to changes in the microRNA parameters Γ_{M} and Γ_{E}. Note that in the noise susceptibility analysis, we quantified the sensitivity of each variable at steady state to the input S. Here, we quantified the sensitivity of the whole system to a particular parameter over a time interval (Methods).
The timedependent sensitivity of the R model to a parameter p_{i} depends on nominal parameter values (Methods). We chose 3,168 parameter sets from the various values of the parameters we used in numerical simulations (Supplementary Table 4; note that only the parameters S, Γ_{M}, Γ_{E} and k_{E} were varied in our analysis) and calculated the timedependent sensitivity (Eq. 10) for each set. We plotted the sensitivity values for each of the 33 parameters in Supplementary Fig. 7. The system did not show a high sensitivity to parameters Γ_{M} and Γ_{E} relative to the other parameters, indicating that microRNA regulation does not introduce drastic changes to the R switch. Furthermore, the relatively low sensitivity of the system to perturbations in these two parameters indicates that the system is robust with respect to small changes in these parameters.
Bifurcation analysis shows that the R model has complex dynamical properties
We performed bifurcation analysis on the R model (Methods) and discovered a codimension 2 bifurcation – a BogdanovTakens bifurcation, together with global bifurcations involving limit cycles (Fig. 7a). The Hopf and saddlenode curves of the A model have been previously reported in Li et al.^{30}, where they delineated the bulk diagram of the dynamical behavior of the A model into four regions, namely monostability, bistability, excitability, and undamped relaxation oscillation. Our discovery of global bifurcations provides a finer decomposition of this bulk diagram. Point p_{1}, which is between the brown and dashed red curves of Fig. 7a, is within the bistable region of Li et al., but one of the stable equilibrium points lies inside an unstable limit cycle (Fig. 7b). At point p_{2}, the system has an unstable equilibrium point inside a stable limit cycle (Fig. 7c), and at point p_{3}, the system has a stable equilibrium point inside a stable limit cycle (Fig. 7d). The complexity of the dynamics of the A model underscores the importance of using a coarsegrained model as it can still exhibit surprising complex dynamical properties.
To plot the analogous bifurcation curves for the R model, we performed two sets of analysis, one with parameters S and Γ_{E} (Fig. 7e) and another with parameters S and Γ_{M} (Fig. 7f). As in the A model, we also found Hopf and saddlenode curves, but these curves delineated the parameter space into more regions than in the A model. We also found BogdanovTakens bifurcations (Fig. 7e,f).
Discussion
Stochastic simulations illustrating noise buffering of microRNAs at low serum levels (Fig. 4) support currently held ideas that microRNAs appear to be nonessential under normal conditions, but are essential under environmental and genetic perturbations^{20,32}. Furthermore, these results are consistent with experimental observations based on an engineered microRNA circuit which showed that the presence of a microRNAmediated feedback loop consistently conferred robustness to the positive feedback loop motif, allowing the cells to maintain their off state for a longer time^{23}. Moreover, the importance of the microRNA cluster in regulating the RbE2F pathway is also emphasized by previous results that the use of transcriptional repressor instead of microRNAs was not as effective in dampening fluctuations in the output of the target protein^{27,33}. Aside from robustness to noise, the R model has also been shown to be robust with respect to perturbations on the connectivity of the network^{34}. Our timedependent sensitivity analysis showed that the whole system is robust with respect to small changes of the microRNA inhibition parameters. Taken together, our results and those of others indicate that microRNAs play an essential role in providing phenotypic robustness to the RbE2F pathway.
The noisebuffering role of the miR1792 cluster aids the R switch in correctly processing the input signal, and demonstrates its important role in the decision process within the cell cycle^{28,35}. Our analysis of the switching characteristics of the model with respect to the microRNA inhibition parameters emphasize the role of microRNAs in steering the cell away from the cancer zone by lowering the on value (Fig. 6). This result further provides a concrete framework for experimentally controlling the R switch: the experimentally observable quantities S* and E* can be controlled by varying the strength of the microRNA inhibition, which can be performed using synthetic biology.
The noise amplification curves showed a different qualitative behavior of noise amplification between the on and off states. Furthermore, the two microRNA parameters Γ_{M} and Γ_{E} displayed similar qualitative effects on noise amplification (Fig. 5b, Supplementary Figs 2, 5 and 6). This consistency is not surprising since although Γ_{M} does not directly inhibit E2F, its inhibition of cMyc will decrease the positive influence of cMyc on E2F. The effect of parameter k_{E} on noise amplification is opposite that of Γ_{M} and Γ_{E}: at the on state, the peaks of the noise amplification curves move to the right (Supplementary Figs 3 and 4), instead of moving to the left (Supplementary Fig. 2) as k_{E} increases. Parameter k_{E} also had the opposite noise amplification effect at the off state: the noise amplification increases with increasing value of k_{E} (Supplementary Figs 3 and 4). These results are consistent with previous results in the analysis of the A model where it was shown that the positive feedback parameter κ and the negative feedback parameter Γ_{2} produced opposing effects on noise^{27}. Thus, our results demonstrate that the insights obtained from network motifs can be extended to more realistic models. In particular, we have exhibited in the larger RbE2F network the result from an analysis of the A model^{27} that interlinked positive and negative feedback loops dynamically tune propagation signals.
Comparing properties of the R model with those of the A model, we were able to identify robust properties of the simple 2D model that carry over to the more complex model. These properties are the switching curve characteristics, bifurcation properties, noise susceptibility, and noise amplification. The R model also presents insights that could not be gained from the A model. In particular, as mentioned above, the R model provides two parameters Γ_{M} and Γ_{E} that could be experimentally varied to determine how microRNAs control experimentally observable quantities S* and E*.
We anticipate that a similar role of microRNAs in conferring robustness could also be identified in other systems using the same analysis that we have performed. But we also anticipate that an analysis of a much larger miR1792 network, of which the RbE2F pathway is just a subnetwork, will also be of interest in modeling the cell cycle. For example, a recent study showed that out of the thousands of genes controlled by Myc, the miR1792 cluster plays a special role in maintaining the neoplastic state of Mycinduced tumors^{36}. The authors showed that Myc through miR1792 directly suppresses the expression of chromatin regulatory genes, which causes autonomous proliferation and selfrenewal. For such larger networks, the analysis we have performed can be used for investigating the robustness of the system.
Methods
The R model
The R model is the mathematical representation of the dynamics of the network interactions in Fig. 2, and is given by the following system of differential equations
The model variables M, E, CD, CE, R, RP, RE and μ denote the concentrations, respectively, of cMyc, E2F, cyclinD, cyclinE, retinoblastoma protein, phosphorylated retinoblastoma protein, retinoblastoma proteinE2F complex, and the miR1792 cluster. The terms v_{i} denote the reaction rate of the corresponding numbered reactions in Fig. 2b and are given by
S is the concentration of the growth signal which will be used as the input in the analyses below, Γ_{M} is the inhibition coefficient of miR1792 on cMyc, and Γ_{E} is the inhibition coefficient of miR1792 on E2F. The values of the parameters are given in Table 1.
The expressions above (Eq. (2)) are the same as in the Yao model^{9}, except for the steps that embody microRNA inhibition, v_{1} and v_{3}. The reaction rate v_{1} is the rate of cMyc synthesis which phenomenologically models microRNA inhibition. The rate of E2F expression (v_{3}) is given by two terms: the first term corresponds to the synergy between the transcription factors E2F and cMyc, while the second term is due to cMycinduced transcription of E2F. The variable μ does not appear in the denominators of the expression involving M in v_{3} since those expressions model the positive regulation of E2F by cMyc and thus are not directly affected by microRNAs (Fig. 2). Each model variable has a decay rate (with parameter d subscripted by the corresponding variable), which is given in the last term in each of the equations in Eq. (1). Note that although there are at least two mature microRNAs from the mir1792 cluster that target cMyc and E2F, we assume here that these microRNAs are all represented by the single variable μ^{8}.
To simplify notation, we write Eq. (1) concisely as
where X(t) is the vector with 8 components (M, E, CD, CE, R, RP, RE, μ), and F(X) is the right hand side of of Eq. (1). The initial conditions are given in Table 1.
Yan et al.^{37} extended the model of Yao et al.^{9} to include miR449 inhibition. However, there are two fundamental differences between their model and our R model: miR449 only inhibits cMyc (and not E2F) and they modeled microRNA inhibition of cMyc in a different manner. Thus, due to the differences in the network connectivity and model kinetics, the two models are qualitatively and quantitatively distinct.
The initial conditions and parameter values in Table 1 were taken from Yao et al.^{9}, except for the microRNA parameters d_{μ}, K_{Mμ} and K_{Eμ}. We chose the value d_{μ} = 0.001 since microRNAs are assumed to be more stable than the mRNAs they regulate. The values of K_{Mμ} and K_{Eμ} were chosen to be slightly lower than those of K_{M} and K_{E}. The various values of the parameters S, Γ_{E} and Γ_{M} used in the analyses are given either in the text or in figure captions.
The R model is provided as a Matlab function in Supplementary File 1. We also provide a Matlab script that uses the function to plot Fig. 3a–d.
Stochastic simulations
To model stochastic effects, we added noise to the R model of the form
Here W(t) is the Brownian motion and F(X(t)) is the right hand side of the system of ordinary differential equations from Eq. (1). To perform numerical simulations, we modified a C implementation of a 4^{th} order RungeKutta method for stochastic differential equations (http://people.sc.fsu.edu/~jburkardt/cpp_src/stochastic_rk/stochastic_rk.html)^{38}. We used a noise level of 0.01 and a time step of 5e4. For each set of parameters in Fig. 4, we performed 10,000 numerical integrations to simulate a clonal population of 10,000 cells. We recorded the values of the variables at t = 100. The initial conditions and parameter values are given in Table 1.
Noise amplification and noise susceptibility
To analyze the effect of the microRNA inhibition parameters on the noise amplification and noise susceptibility of the R model, we used the Fluctuation Dissipation Theorem (FDT)^{39}, with the serum S as the input to the system. The steady state susceptibility or noise sensitivity (SS) is defined as the relative change in the output in response to the change in the input
The subscripts denote the model variables, while the symbol indicates the average value at steady state. We denote S by X_{0}, and rewrite the system of ODEs as
At steady state, the derivative of F with respect to X_{0}, …, X_{8} is given by
The system of equations above can be written as
where
After solving for x from the linear system, the sensitivity to noise input, SS_{i} (Eq. 5) is obtained from
Note that for convenience, we dropped the use of the notation .
On the other hand, the noise amplification (SA) is defined as the ratio between the output and input noise, with the noise defined as the coefficient of variation
To compute the noise amplification SA_{i} (Eq. (6)), we form the 9 × 9 linear system that arises from the normalized FDT equation at steady state^{39,40}
where
The components of matrices M and D are given in the Supplementary Material. For a given set of parameter values and initial conditions, we numerically solved the system of ODEs until steady state and then formed the FDT linear system (Eq. (7)). Then we numerically solved the linear system Eq. (7) for η using Matlab’s solver for Lyapunov equations lyap. The diagonal elements of η are the noise approximations (σ_{i}^{2}/μ_{i}^{2}) and Eq. (6) is calculated as
The range of the values of the parameters used in plotting Fig. 5 and Supplementary Figs 2–6 were dependent on the maximum value where the parameter space could still yield a bistable system (Supplementary Table 3).
Switching characteristic analysis
In order to analyze how microRNAs finetune the RbE2F pathway in and out of the cancer zone^{10}, we computed the values of the serum (S) at which the system jumps from one stable steady state to the other. To this end, we created a custom Matlab script that integrated the system until steady state and calculated the eigenvalues of the Jacobian at the steady state. The eigenvalues indicated the stability of the equilibrium point. An initial equilibrium point was obtained by running the Matlab ODE solver until steady state (t = 10,000 hr). Starting from the steady state, we calculated equilibrium points by implementing a continuation method as described in Kuznetsov^{41}. We calculated the eigenvalues to determine the stability of the system within the parameter space. For the A model (model equations are in the Supplementary Material), the initial conditions were ϕ = 0.13 and μ = 0.35, and the fixed parameters were ε = 0.1, κ = 5, Γ_{1}′ = 1. For the R model, the initial conditions and parameter values are in Table 1, and we performed analysis with Γ_{E} on the interval [0, 0.007], and Γ_{M} on the interval [0, 0.5].
Calculation of bifurcation points
We used Matlab and the MATCONT Matlab package^{42} to plot the bifurcation diagrams of the A and R models. The “continuation data” parameters we used were: maximum stepsize of 1e8 and the “correction data” parameter we used were: variable tolerance of 1e8, function tolerance of 1e8 and test tolerance of 1e6.
Parameter sensitivity analysis
The first order sensitivity
quantifies the effect of small perturbations in parameter values on the model variables. Equation (8) was calculated for each of the 33 model parameters (j = 1… 33, including Γ_{M}, Γ_{E} and S), and for each of the 8 model variables (i = 1… 8). This involved numerically solving an augmented ODE system of dimension 272 (272 = 8 + 8*33), given by
where k = 8 + (j − 1)*33 + i (i = 1…8; j = 1…33). In order to capture timedependent parameter sensitivities, we integrated Eq. (9) over the timeinterval t = 0 to t = 1,000 hr, at 1000 points (k = 1…1000). After solving the augmented ODE, we consolidated the timesensitivities in a manner that takes into account possible noise in measurements^{43}
Here, p_{j} is the nominal parameter value, and σ_{i,k} = 1e6 × X_{i}(t_{k}) + 1e8. The relative and absolute tolerances we used in the ODE simulation were 1e6 and 1e8, respectively. The initial conditions used were in Table 1 for the model variables (k = 1… 8) and zero for all other variables (k > 8). The nominal parameter values are in Supplementary Table 4 and a Matlab code for parameter sensitivity analysis is provided in Supplementary File 1.
Additional Information
How to cite this article: del Rosario, R. C. H. et al. MicroRNA inhibition finetunes and provides robustness to the restriction point switch of the cell cycle. Sci. Rep. 6, 32823; doi: 10.1038/srep32823 (2016).
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Acknowledgements
We would like to acknowledge support from the Philippine Genome Center, University of the Philippines Diliman and the Office of the Vice President for Academic Affairs, University of the Philippines.
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B.D.A. created the R model; R.C.H.d.R. performed all numerical computation and analysis except for Figure 7a–d that was performed by J.R.C.G.D., B.D.A. and R.C.H.d.R. analyzed the results and wrote the manuscript; all authors approved the manuscript.
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del Rosario, R., Damasco, J. & Aguda, B. MicroRNA inhibition finetunes and provides robustness to the restriction point switch of the cell cycle. Sci Rep 6, 32823 (2016). https://doi.org/10.1038/srep32823
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DOI: https://doi.org/10.1038/srep32823
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