 Research
 Open Access
 Published:
Tracking the evolution of cancer cell populations through the mathematical lens of phenotypestructured equations
Biology Direct volume 11, Article number: 43 (2016)
Abstract
Background
A thorough understanding of the ecological and evolutionary mechanisms that drive the phenotypic evolution of neoplastic cells is a timely and key challenge for the cancer research community. In this respect, mathematical modelling can complement experimental cancer research by offering alternative means of understanding the results of in vitro and in vivo experiments, and by allowing for a quick and easy exploration of a variety of biological scenarios through in silico studies.
Results
To elucidate the roles of phenotypic plasticity and selection pressures in tumour relapse, we present here a phenotypestructured model of evolutionary dynamics in a cancer cell population which is exposed to the action of a cytotoxic drug. The analytical tractability of our model allows us to investigate how the phenotype distribution, the level of phenotypic heterogeneity, and the size of the cell population are shaped by the strength of natural selection, the rate of random epimutations, the intensity of the competition for limited resources between cells, and the drug dose in use.
Conclusions
Our analytical results clarify the conditions for the successful adaptation of cancer cells faced with environmental changes. Furthermore, the results of our analyses demonstrate that the same cell population exposed to different concentrations of the same cytotoxic drug can take different evolutionary trajectories, which culminate in the selection of phenotypic variants characterised by different levels of drug tolerance. This suggests that the response of cancer cells to cytotoxic agents is more complex than a simple binary outcome, i.e., extinction of sensitive cells and selection of highly resistant cells. Also, our mathematical results formalise the idea that the use of cytotoxic agents at high doses can act as a doubleedged sword by promoting the outgrowth of drug resistant cellular clones. Overall, our theoretical work offers a formal basis for the development of anticancer therapeutic protocols that go beyond the ‘maximumtolerateddose paradigm’, as they may be more effective than traditional protocols at keeping the size of cancer cell populations under control while avoiding the expansion of drug tolerant clones.
Reviewers
This article was reviewed by Angela Pisco, Sébastien Benzekry and Heiko Enderling.
Background
A growing body of evidence indicates that cancer progression at the cellular level is, in essence, an evolutionary process [1–6]. During cancer progression, novel phenotypic variants emerge via heritable changes in gene expression. Subsequently, phenotypic variants are subject to natural selection – they survive, reproduce, and die – under the action of the tumour microenvironment and anticancer agents. The scenario is further complicated by celltocell variability in gene expression, which gives rise to phenotypic differences between cancer cells of the same population. This phenotypic heterogeneity is a dynamic source of therapeutic resistance that needs to be accounted for when investigating effective anticancer therapeutic protocols [7].
Novel phenotypic variants in cancer cell populations originate mainly from mutations (i.e., genetic modifications). However, novel phenotypic variants can also emerge due to epimutations (i.e., heritable changes in gene expression that leave the sequence of bases in the DNA unaltered) [8–12]. For instance, recent experiments using fluorescentactivated cell sorting have demonstrated that nongenetic instability mediated by fluctuating protein levels allows cancer cells to reversibly transition between different phenotypic states [13–15]. Such nongenetic source of phenotypic variability has been increasingly recognised as integral to the development of resistance to cytotoxic agents in cancer cell populations [16, 17].
Identifying the ecological and evolutionary mechanisms that drive the phenotypic evolution of neoplastic cell populations is, therefore, a timely and key challenge for the cancer research community. In this regard, mathematical modelling provides additional tools in the fight against cancer, and many biologists and clinicians are now looking for a mathematical approach to complement their research [18–27]. Among others, models arising from mathematical ecology enable falsification of biological hypotheses concerning the principles that underpin the dynamics of neoplastic cell populations, and extrapolation beyond scenarios analysed by means of in vitro and in vivo experiments [28].
During the last fifty years, partial differential equations (PDEs) for populations structured by physiological traits have been extensively used to achieve a better understanding of a wide range of ecological phenomena [29, 30]. These equations describe population dynamics in terms of the evolution of population densities across phenotypic spaces, and can be derived from individualbased (IB) models through suitable asymptotic limits [31–33]. However, unlike IB models, which can be explored mainly through numerical simulations only, PDEs for populations structured by physiological traits make it possible to integrate numerical simulations with rigorous analysis, in order to achieve more robust biological conclusions [34].
In particular, we have recently shown that phenotypestructured PDEs constitute a convenient apparatus to study in silico the dynamics of cancer cell populations. In more detail, we formulated a PDE model for the coevolution of a population of healthy cells and a population of cancer cells structured by the level of resistance to a cytotoxic drug [35]. Further, we extended this model to consider cell populations structured also by a spatial variable [36]. Most recently, we presented a PDE model of phenotypic evolution in a cancer cell population structured by the expression levels of two phenotypic traits, survival potential and proliferation potential [37]. Overall, the results of our analyses and numerical simulations provide a new perspective on the inherent risks of interventional chemotherapy in cancer patients by showing how the adaption of even nongenetically unstable cell populations exposed to antiproliferative drugs can be acted upon by selective forces, which drive the outgrowth of drug resistant cell clones.
To investigate the roles of phenotype plasticity and selection pressures in tumour relapse, here we propose a phenotypestructured PDE model of evolutionary dynamics in a cancer cell population which is exposed to the action of a cytotoxic drug within an in vitro culture system. Our model is informed by a previous conceptual model [38] and focuses on a cancer cell population structured by the expression level of a gene which is linked to both the cellular levels of cytotoxicdrug resistance and proliferative potential – such as ALDH1, CD44, CD117 or MDR1 [39, 40]. We characterise the phenotypic state of each cell by means of a continuous variable related to the level of expression of this gene, and we allow the cell phenotypic state to change in time due to nongenetic instability, which is mediated by random epimutation events. The inclusion of a dynamic continuous population structure and its plasticity makes PDE models a natural framework to study, in silico, the phenotypic evolution of cancer cells. Note that, in the model presented here, nongenetic instability is purely random and represented by a constant rate multiplying a diffusion operator. In more sophisticated models involving metabolismdependent epigenetic dynamics, as those advocated in [41], this constant would be replaced by a suitable function to incorporate the effects of the cell load in histone demethylases, DNA methyltransferases, or other epigenetic enzymes, together with their substrates and coenzymes.
Exploiting the analytical tractability of our model, we dissect the relative contributions of random epimutations, natural selection and competition for resources as drivers of adaptation in cancer cell populations that evolve under the action of cytotoxic drugs. This analytical work builds on recent advances in the study of nonlocal PDEs that arise in models of population dynamics [33, 42, 43], which enable us to explore the parameter space of our model completely. To illustrate analytical results through numerical simulations, we calibrate our model by means of existing data from in vitro experiments on the phenotypic evolution of HL60 leukemic cells exposed to vincristine [14]. Nonetheless, the results of our analyses are qualitatively robust across a wide range of parameter values. This makes the conclusions presented in our current work applicable to a broad spectrum of cancer cell lines evolving under the action of different cytotoxic agents.
Our main findings elucidate how the phenotype distribution, the level of phenotypic heterogeneity and the size of cancer cell populations exposed to cytotoxic drugs are shaped by the strength of natural selection, the rate of random epimutations, the intensity of the competition for limited resources between cells, and the drug dose in use. Moreover, we are able to obtain exact conditions for the successful adaptation of cancer cells, and we find that whilst phenotypic plasticity may facilitate adaptation in neoplastic cell populations exposed to cytotoxic drugs, frequent fluctuations in protein levels can also contribute to extinction in the presence of high drug concentrations. Finally, our mathematical results provide a ‘proof of concept’ of the hypothesis that the use of cytotoxic agents at high doses is a doubleedged sword in the fight against cancer, and offer a formal basis for the development of therapeutic protocols which effectively exploit evolutionary mechanisms to improve the efficacy of cytotoxic therapy.
Methods
We study evolutionary dynamics in a wellmixed population of cancer cells that is structured by the expression level \(y \in \mathbb {R}_{+}\) of a gene which is linked to both the cellular levels of cytotoxicdrug resistance and proliferative potential. Following Pisco and Huang [38], we assume that there is a level of expression y ^{H} which endows cells with the highest level of cytotoxicdrug resistance, and a level of expression y ^{L}<y ^{H} conferring the highest proliferative potential when there are no xenobiotic agents. In this framework, we characterise the phenotypic state of each cell by means of the variable \(x \in \mathbb {R}\) with
so that the state x=1 corresponds to the highest level of cytotoxicdrug resistance, while the state x=0 corresponds to the highest level of proliferative potential in the absence of xenobiotic agents.
Cells inside the population proliferate or die, compete for limited resources, and undergo variation in phenotype due to random epimutation events. Furthermore, a cytotoxic drug can be present, which acts by increasing the death rate of cancer cells. The function n(x,t)≥0 stands for the population density, so that the total number of cells at time t is computed as
while the average phenotypic state and the related variance at time t are computed, respectively, as
In this mathematical framework, the function σ ^{2}(t) provides a measure of the level of intrapopulation heterogeneity at time t. Finally, we introduce the function c(t)≥0 to model the concentration of cytotoxic drug at time t. Throughout the paper, we will mainly focus on the case of continuous drug infusion, and we will use the parameter C>0 to model the constant concentration of cytotoxic drug inside the system.
PDE model
We describe the evolution of the cell population density n(x,t) by means of the following phenotypestructured PDE
which we complete with the boundary conditions
and the initial condition
In the above equation, Ω is a compact subset of \(\mathbb {R}\). Eq. (3) relies on the assumptions and the modelling strategies presented in the following subsections.
Mathematical modelling of nongenetic instability
To reduce biological complexity to its essence, we make the prima facie assumption that random epimutations yield infinitesimally small phenotypic modifications [44, 45]. Therefore, we model the effects of nongenetic instability through a diffusion operator. The diffusion coefficient β>0 in Eq. (3) stands for the rate of epimutation of cancer cells, which is assumed to be constant, as mentioned earlier.
Mathematical modelling of natural selection
Natural selection is driven here by the function R(x,ρ(t),c(t)), which represents the fitness of cancer cells in the phenotypic state x at the time t, given the total number of cells ρ(t) and the concentration of cytotoxic drug c(t). Throughout this paper, we make use of the following definition:
Definition (6) relies on the idea that a higher total number of cells corresponds to less available resources; therefore, we let cells inside the population die at rate d ρ(t), where the parameter d>0 models the rate of death due to intrapopulation competition. The function p(x) stands for the net proliferation rate of cancer cells in the phenotypic state x, while the function k(x,c(t)) is the rate of death caused by the cytotoxic drug. Since the phenotypic state x=1 corresponds to the highest level of cytotoxicdrug resistance, we assume that the function k is strictly convex with minimum in x=1. Furthermore, because the death rate of cancer cells will increase as the concentration of the cytotoxic drug increases, we assume that k is an increasing function of c. On the other hand, to take into account the fact that the phenotypic state x=0 corresponds to the highest level of proliferative potential when there are no xenobiotic agents (i.e., when c(·)=0), we assume that p is a strictly concave function with maximum in x=0. In this setting, we follow the modelling strategies presented in [42] and define the functions p and k as:
In the above definitions, the parameter γ>0 corresponds to the maximum fitness of cancer cells, and the nonlinear selection gradient η>0 provides a measure of the strength of natural selection in the absence of xenobiotic agents.
Setup of numerical simulations and model parametrisation
We numerically solve the mathematical problem defined by completing Eq. (3) with boundary conditions (4) and the following initial condition
where b and L are positive numbers, a _{ i }>0 are uniformly distributed random numbers between 0 and 1, x _{ i } are uniformly distributed random numbers between −L and L, and K>0 is the carrying capacity of the population. The above definition represents an initial population composed of different cellular clones labelled by the index i=1,…,N. To perform numerical simulations, we set N=20.
Numerical computations are performed in MATLAB. We select a uniform discretisation consisting of 1200 points on the interval [−2L,2L] with L=2 as the computational domain. The method for calculating numerical solutions is based on a time splitting scheme between the conservative part and the reaction term [46]. As for the conservative part, we approximate the diffusion term through a threepoint explicit scheme. On the other hand, we use an implicitexplicit finite difference scheme for the reaction term [35]. For all simulations, we set the time step d t=10^{−4}, in order to ensure the stability of the numerical scheme.
We set the maximum fitness γ=0.66, so that the doubling time of cells in the highly proliferative state x=0 is about 25 h (cf. data in [47]). Furthermore, the in vitro experiments presented in [14] on the phenotypic evolution of HL60 leukemic cells exposed to vincristine have shown that, in the absence of xenobiotic agents, highly cytotoxicdrug resistant cells take approximatively 18 days to accomplish the repopulation of the equilibrium cell distribution observed without xenobiotic agents. Also, according to the same experiments, the ratio between the proliferation rate of the cells with the highest level of cytotoxicdrug resistance and the proliferation rate of the cells with the highest proliferative potential is equal to 5. Therefore, we choose the nonlinear selection gradient η and the rate of epimutations β to be such that, when c(·)=0, it takes approximatively 18 days for an initial population mainly composed of cells in the phenotypic state x=1 to reconstitute the equilibrium phenotypic distribution corresponding to c(·)=0, with the value of η being constrained by the condition p(x=0)/p(x=1)=5 (vid. Additional file 1). Moreover, we define the average rate of death due to intrapopulation competition as d:=γ/K, so that the equilibrium value of the total number of cells in the absence of xenobiotic agents and without epimutations (i.e., when c(·)=0 and β=0) is equal to the carrying capacity K=10^{8} (cf. Figure S5 in [14]). Based on these considerations, unless otherwise stated, we perform numerical simulations using the parameter values listed in Table 1, which are consistent with previous reports [14, 47–49]. Finally, the concentration of cytotoxic drug is expressed in terms of the LC_{ α } – i.e., the value of c that is required to reduce the equilibrium value of the total number of cells by α %.
Results and discussion
Cell dynamics in the absence of xenobiotic agents
As mentioned earlier, in the framework of our model, the total number of cells ρ(t), the average phenotypic state μ(t) and the level of intrapopulation heterogeneity σ ^{2}(t) are computed according to Eqs. (1)–(2). Then, in the absence of xenobiotic agents (i.e., when c(·)=0), a complete characterisation of the cancer cell population at equilibrium is provided by the following theorem:
Theorem 1
Let c(·)=0, and denote by \(\overline {n}(x)\) the equilibrium population density for c(·)=0. Then:

(i)
if γ−(β η)^{1/2}≤0,
$$ \rho(t) \rightarrow 0, \qquad \text{as }\, t \rightarrow \infty; $$(9) 
(ii)
if γ−(β η)^{1/2}>0,
$$ \rho(t) \rightarrow \overline{\rho} = \frac{1}{d}\left[ \gamma(\beta\eta)^{1/2} \right], \qquad \text{as }\, t \rightarrow \infty $$(10)and
$$ \overline{n}(x) = \overline{\rho} \; \frac{{(\eta/\beta)^{1/4}}}{(2\pi)^{1/2}} \exp\left[\frac{1}{2}\left(\frac{\eta}{\beta}\right)^{1/2} x^{2}\right], $$(11)so that
$$ \mu(t) \rightarrow \overline{\mu} = 0~~\text{and} \quad \sigma^{2}(t) \rightarrow \overline{\sigma}^{2} = \sqrt{\frac{\beta}{\eta}},~~~\text{as }\, t \rightarrow \infty. $$(12)
The results established by Theorem 1 are discussed, as points R1  R4 below, and illustrated by means of numerical simulations in the following subsections. The proof is detailed in Appendix 1 – to which we refer the mathematically inclined reader – and it follows from a general analysis that we have presented in two recent papers [33, 42].
R1. Higher rates of random epimutations can drive the cancer cell population to extinction under strong selective pressures
Point (i) of Theorem 1 shows that the total number of cells ρ(t) converges to zero when the value of the product between the epimutation rate β and the nonlinear selection gradient η exceeds the square of the maximum fitness γ. Hence, in the presence of large selection gradients, high rates of random epimutations increase the probability of ultimate extinction. This suggests that frequent random epimutations can drive cancer cell populations to extinction under strong selective pressures.
R2. The population evolves to be mainly composed of highly proliferative cells
Point (ii) of Theorem 1 demonstrates that, for any initial population density n(x,0), the equilibrium phenotype distribution \(\overline {n}(x)\) is unimodal with the average phenotypic state \(\overline {\mu }\) being at the maximum point of the distribution x=0, and the total number of cells converges to the stable positive value \(\overline {\rho }\). This holds true for all parameter settings, on the condition that the maximum fitness γ, the nonlinear selection gradient η and the rate of random epimutations β satisfy the relation γ−(β η)^{1/2}>0.
These results are illustrated by the plots in Fig. 1, which present sample dynamics of the population density n(x,t) and the total number of cells ρ(t) when c(·)=0, for the parameter values listed in Table 1. Independently of the phenotypic composition of the initial population, cells in the phenotypic state x=0 (i.e., the phenotypic state corresponding to the highest level of proliferative potential in the absence of xenobiotic agents) become the most abundant within the population [vid. Fig. 1 a and inset of Fig. 1 b], and the total number of cells reaches the stable value \(\overline {\rho }\) [vid. Fig. 1 b].
R3. The number of cells and the level of intrapopulation heterogeneity at equilibrium depend on the rate of random epimutations and on the strength of natural selection
Point (ii) of Theorem 1 also sheds some light on the way the size of the population and the level of phenotypic diversity are affected by nongenetic instability and natural selection. This is highlighted by the phase diagrams in Fig. 2, which show how the total number of cells \(\overline {\rho }\) and the level of intrapopulation heterogeneity \(\overline {\sigma }^{2}\) at equilibrium vary as a function of the rate of epimutations β and the nonlinear selection gradient η. In summary, the total number of cells is a decreasing function of β and η, while the level of intrapopulation heterogeneity increases with β and decreases with η. These results formalise the idea that more intense nongenetic instability and stronger selection pressures bring about cancer cell populations of a smaller size. Also, more frequent phenotypic fluctuations lead to higher levels of intrapopulation heterogeneity, whilst intense selective pressures support less phenotypic diversity.
R4. The population size at equilibrium depends also on the maximum fitness and on the rate of cell death due to intrapopulation competition
The results established by point (ii) of Theorem 1 and illustrated by the phase diagram in Fig. 3 indicate, as one could expect, that the total number of cells at equilibrium is an increasing function of the maximum fitness γ and a decreasing function of the average rate of death due to intrapopulation competition d. In the framework of our model, lower values of the parameter γ are associated with more hostile environmental conditions, while higher values of the parameter d correspond to stronger intrapopulation competition. Therefore, these results formalise the idea that cancer cell populations shrink in the presence of harsh environments and intense cellular competition for limited resources.
Cell dynamics under the action of cytotoxic drug
The plots in Fig. 4 depict sample dynamics of the population density n(x,t) and the total number of cells ρ(t) in the case when the drug concentration c(·)=C corresponds to the LC_{70} dose, for the parameter values listed in Table 1. These plots illustrate how the cytotoxic drug triggers a population bottleneck by causing a sharp reduction in the number of cells, followed by approximatively 1 day of relatively constant population level before cells in a phenotypic state close to x=1 (i.e., the phenotypic state corresponding to the highest level of cytotoxicdrug resistance) are selected and start proliferating. Subsequently, the population size grows again and, ultimately, attains a stable value.
Although the phenotype distribution and the number of cells at equilibrium, as well as the time required for the population to recover, vary depending on the choice of the drug dose, the dynamics of the population density and the total number of cells remain qualitatively similar to those shown in Fig. 4. A complete characterisation of the cancer cell population at equilibrium is provided by the following theorem:
Theorem 2
Let c(·)=C>0, define
and denote by \(\overline {n}_{c}(x)\) the equilibrium population density for c(·)=C. Then:

(i)
if γ _{ c }−(β η _{ c })^{1/2}≤0,
$$ \rho(t) \rightarrow 0, \qquad \text{as }\, t \rightarrow \infty; $$(14) 
(ii)
if γ _{ c }−(β η _{ c })^{1/2}>0,
$$ \rho(t) \rightarrow \overline{\rho}_{c} = \frac{1}{d}\left[\gamma_{c}(\beta\eta_{c})^{1/2} \right], \qquad \text{as }\, t \rightarrow \infty $$(15)and
$$ \overline{n}_{c}(x) = \overline{\rho}_{c} \; \frac{{(\eta_{c}/\beta)^{1/4}}}{(2\pi)^{1/2}} \exp\left\{\frac{1}{2}\left(\frac{\eta_{c}}{\beta}\right)^{1/2} \left[x\overline{x}_{c}\right]^{2}\right\}, $$(16)with
$$ \overline{x}_{c} := \frac{C}{\eta+C}, $$(17)so that
$${} \mu(t) \rightarrow \overline{\mu}_{c} = \overline{x}_{c}~~\text{and} \quad \sigma^{2}(t) \rightarrow \overline{\sigma}^{2}_{c} = \sqrt{\frac{\beta}{\eta_{c}}},~~\text{as }\, t \rightarrow \infty. $$(18)
As explained in Appendix 2, the proof of Theorem 2 follows the method of proof of Theorem 1. Here we proceed by discussing, as points R5  R8 below, the pieces of biological information which are conveyed by the above mathematical results. Furthermore, in order to extend the analytical results established by Theorem 2, we perform numerical simulations letting the drug concentration vary over time. The obtained results are discussed as points R9 and R10 below.
R5. Higher rates of random epimutations can drive the population to extinction in the presence of high drug doses
Point (i) of Theorem 2 shows that the total number of cells ρ(t) converges to zero when the value of the product between the rate of random epimutations β and the sum of the nonlinear selection gradient η and the drug concentration C is larger than the square of the maximum fitness γ. This supports the idea that higher rates of random epimutations increase the chance that cancer cell populations go extinct when exposed to sufficiently high concentrations of cytotoxic agents.
R6. Higher drug doses correspond to lower cell numbers
Point (ii) of Theorem 2 reveals that, if the condition γ _{ c }−(β η _{ c })^{1/2}>0 is satisfied, the total number of cells ρ(t) converges to the stable positive value \(\overline {\rho }_{c}\). By analogy with the case when there is no cytotoxic drug inside the system, \(\overline {\rho }_{c}\) increases with the maximum fitness γ, and decreases with the nonlinear selection gradient η, the rate of epimutations β, and the rate of cell death due to intrapopulation competition d. Moreover, as one could expect, the cytotoxic drug has a detrimental effect on the population size, and the number of cells at equilibrium is a decreasing function of the drug dose C [vid. Fig. 5].
R7. Higher drug doses promote a selective sweep towards more resistant phenotypic variants
Point (ii) of Theorem 2 demonstrates that – for all values of the model parameters satisfying the condition γ _{ c }>(β η _{ c })^{1/2} – the equilibrium phenotype distribution given by \(\overline {n}_{c}(x)\) is unimodal with the average phenotypic state \(\overline {\mu }_{c}\) being at the maximum point of the distribution \(\overline {x}_{c}\). Also, the population density at equilibrium does not depend on the initial population density. As illustrated by Fig. 6, the values of \(\overline {x}_{c}\) and \(\overline {\mu }_{c}\) continuously increase from 0 to 1 as the drug dose increases.
The results established by Point (ii) of Theorem 2 indicate that, during cytotoxicdrug treatment, the surviving cells can reside within a spectrum of intermediate phenotypic states – ranging from less drug resistant states to more drug tolerant states – depending on the dose in use. These results indicate that different concentrations of the same cytotoxic drug can lead to the selection of cancer cells in different phenotypic states. In particular, while high doses confer a competitive advantage to highly resistant phenotypic variants, lower concentrations of cytotoxic drugs promote the selection of intermediate levels of cytotoxicdrug resistance and proliferative potential, which may result in an advantageous therapeutic outcome.
R8. The level of intrapopulation heterogeneity decreases as the drug dose increases
As in the case when there is no cytotoxic drug, the level of intrapopulation heterogeneity at equilibrium \(\overline {\sigma }^{2}_{c}\) is an increasing function of the rate of random epimutations β, and a decreasing function of the nonlinear selection gradient η. Furthermore, as illustrated by Fig. 7, point (ii) of Theorem 2 reveals that \(\overline {\sigma }^{2}_{c}\) is a decreasing function of the drug concentration C.
R9. The cancer cell population regains cytotoxicdrug sensitivity when drug delivery is discontinued
In order to extend the analytical results established by Theorem 2, we perform numerical simulations letting the drug concentration vary over time [i.e., we consider the case in which the drug concentration is modelled by a function of time c(t)]. In particular, we explore the dynamics of the cancer cell population exposed to a piecewisecontinuous periodic delivery of the cytotoxic drug. As illustrated by the results presented in the Additional file 2, our model predicts the selection of cells in a more resistant phenotypic state in the presence of the cytotoxic drug, whereas selection is reverted in favour of drugsensitive cells when drug delivery is discontinued. Also, the same results clearly show that administering the cytotoxic drug in an alternate fashion leads to the emergence of cycling subpopulations of drugresistant and drugsensitive cells.
R10. Comparing the administration of highdrug doses separated by drugfree periods with the continuous delivery of relatively lowdrug doses
The results established by Theorem 2 demonstrate that higher doses of cytotoxic drug reduce the size of the cancer cell population at the cost of promoting the selection of more resistant phenotypic variants. Therefore, a natural question arises: how do therapeutic protocols relying on periodic phases of highdose delivery separated by drugfree periods compare to protocols based on the administration of a continuous and relatively low drug dose? The results presented in Fig. 8 suggest that the first type of protocol causes a drastic reduction in the number of cancer cells, although it fosters an increase in the average level of resistance. On the other hand, the second type of protocol maintains a larger stable population of less resistant cells that suppress the growth of highly resistant clones. A more accurate comparison between the efficacy of the two therapeutic approaches would require a careful investigation of the respective adverse effects on healthy cells, which cannot be performed using our model. However, we can envisage a lower druginduced toxicity being associated to the second type of protocols [50]. In the light of this observation, the analytical results of Theorem 2 and the numerical results summarised in Fig. 8 suggest that therapeutic protocols consisting of phases of highdose delivery separated by drugfree periods may not offer the best longterm strategy for tumour control, and that protocols based on the continuous delivery of relatively lowdrug doses may represent a suitable alternative.
Conclusions
Although technological progress in molecular cell biology has resulted in large amounts of data documenting cancer progression, our understanding of the principles that underpin the development of resistance to anticancer agents and the emergence of phenotypic heterogeneity in neoplastic cell populations is filled with gaps and unresolved questions.
This work is presented with the perspective that mathematical modelling can help to address some of these gaps in our knowledge by capturing, in abstract terms, the crucial assumptions that underlie given hypotheses, and by offering alternative means of understanding experimental results that are currently available. With this perspective, our goal here is to contribute to a systematic identification of the way in which the phenotypic distribution, the level of intrapopulation heterogeneity and the size of cancer cell populations depend on the rate of random epimutations, the strength of natural selection, the intensity of the competition for resources, and the stress exerted by cytotoxic agents.
We have presented and analysed a PDE model of adaptive dynamics in a cancer cell population that is structured by the level of expression of a gene which is linked to cytotoxicdrug resistance and proliferative potential. While the parameter values that we have used to perform numerical simulations are derived from leukemia datasets, our analytical results are characterised by broad structural stability under parameter changes, and can accommodate parameter values from any other type of cancer.
The results of our analyses show that more intense nongenetic instability, stronger selection pressures and fierce competition for limited resources bring about cancer cell populations of smaller size. A more subtle question is how phenotypic heterogeneity is maintained or suppressed in cancer cell populations. Our model predicts that higher rates of random epimutations lead to higher phenotypic diversity, whilst intense selection pressures and high doses of cytotoxic drugs can deplete variation in the phenotypic pool of cancer cell populations, thus causing lower levels of intrapopulation heterogeneity. These findings recapitulate the results presented in previous theoretical and experimental studies of phenotypic evolution in neoplastic cell populations exposed to cytotoxic drugs [51–56].
Epigenetic mechanisms are increasingly implicated in the adaptation of neoplastic cells which face environmental changes. However, since epimutation rates are small in comparison to selection gradients, it might be speculated that the direction of evolution in cancer cell populations is determined exclusively by natural selection. On the contrary, our analytical results suggest that, in the presence of high concentrations of cytotoxic agents, frequent fluctuations in the cellular protein levels can trigger a type of ‘epimutational meltdown’ and contribute to extinction in nonfluctuating environments. This effect escalates under harsher environmental conditions (i.e., for lower maximum fitness and higher selection gradients). Since we have derived a simple and general condition that can lead to population extinction – which is embodied by an explicit relation between the proliferation and death rates of cancer cells, the rate of epimutations and the concentration of the cytotoxic drug [vid., point (i) of Theorem 2] – the validity of this argument can be tested in vitro. Because of the striking similarities between populations of cancer cells and microbial populations [57], an experimental setting analogous to that presented in [58] – where the authors made use of isogenic populations of engineered bacteria that randomly transitions between different phenotypic states to study adaptation to artificial environments – may prove to be useful for this purpose.
Here we have found that the same cell population exposed to different concentrations of the same cytotoxic drug can take different evolutionary trajectories, which culminate in the selection of phenotypic variants characterised by different levels of drug tolerance. This supports the notion that the response of cancer cells to cytotoxic agents is more complex than a simple binary outcome, i.e., extinction of sensitive cells and selection of highly resistant cells, and agrees with insights from empirical works that highlight how different phenotypic variants can be selected inside the same solid tumour depending on the local concentrations of cytotoxic agents [59–61]. Also, in agreement with the experimental results presented by Sun et al. [62], our model suggests that cancer cell populations may regain sensitivity to cytotoxic drugs after a ‘drug holiday’.
In current clinical practice, it is common to give the maximum tolerated dose (MTD) of cytotoxic agents at the beginning of a therapy cycle, and then let the patient recover from toxicities. In the last decade, experimental and theoretical efforts have been made to determine the best scheduling of cytotoxic agents in anticancer therapy; unfortunately, there is still no clear answer about optimal administration protocols. Our work demonstrates that higher doses of cytotoxic drugs reduce the size of cancer cell populations at the cost of promoting the selection of more resistant phenotypic variants. Moreover, our analyses support the development of therapeutic approaches that go beyond the ‘MTD paradigm’. For instance, our results provide a theoretical basis for the benefits of metronomic therapy [63–66] – which relies on the continuous delivery of cytotoxic agents at relatively low, minimally toxic doses – and adaptive therapy [67] – which aims at enforcing a stable tumour burden by permitting sensitive cells to suppress highly resistant cells in low drug pressure conditions – as they may be more effective than traditional protocols at keeping the size of cancer cell populations under control while avoiding the expansion of drug tolerant clones.
We conclude with an outlook on possible extensions of the present work. Here, we have assumed that cell proliferation and drug resistance are interconnected. A natural way to extend our study would be to take into account a degree of independence in these processes by incorporating a second phenotypic variable. In this setting, we could also introduce an advection term to explore the effects of environmental stresses (e.g., hypoxia, acidity or starvation) that may induce cells to actively acquire a more stress resistant phenotype. In so doing, we would be in the position to analyse how the interplay between selection, nongenetic instability and stressinduced adaptation governs the emergence of intratumour heterogeneity and the development of drug tolerance inside solid tumours, which is a theme that we began exploring in a previous paper [37].
The present model could also be extended to include the effects of the phenotypic coevolution and spatial interaction between cancer cells and cells of the tumour microenvironment. In fact, the growth and death of neoplastic cells is determined not only by their phenotype, but also by the microenvironment they inhabit. In particular, accumulating in vitro and in vivo evidence suggests that the interplay between cancer cells and stromal cells can induce mutual phenotype modifications promoting tumour growth and the emergence of resistance to anticancer agents [68–71]. As a first step, we may incorporate an additional structuring variable that stands for the spatial position of cells, and we could include an additional evolution equation for the local density of stromal cells, in order to investigate, in silico, the existence of ecological mechanisms which can foster the spreading of more proliferative and drug resistant phenotypic variants at the interface between solid tumours and host tissues.
Another track to follow to further enrich our model would be to include metabolic determinants of epigenetic dynamics in single cells. Simple phenomenological models have been proposed to describe the influence of oxygen and proton concentration in cancer tissues (see, for instance, [72, 73]). More recently the influence of metabolism on key epigenetic enzymes determining stemness (such as TET1/2, IDH1/2, DNMT3A) has been investigated in detail, setting the focus on DNA methylation dynamics [41, 74]. Mutations of such enzymes have been evidenced in leukemia and preleukemic states [75, 76]. Nevertheless, even without the occurrence of mutations, unequal repartition of these enzymes could be found to be a source of heterogeneity in cancer cell populations making cells diversely sensitive to their metabolic environment. Some cells, heavily loaded in these enzymes, may revert to a stemlike state, yielding germs for drugresistant clones, while the others, not endowed with such abilities, would readily die when exposed to high doses of cytotoxic drugs. In this regard, mathematical modelling is still dependent on more biological knowledge to come about metabolism, stemness and epigenetic dynamics.
Appendix 1. Proofs of Theorem 1 and Theorem 2
When c(·)=0, plugging definitions (6)–(7) into Eq. (3) we obtain
The proof of Theorem 1 follows from a more general analysis that we have developed in two recent papers [33, 42], and it uses the results established by the following two lemmas:
Lemma 1
If γ>(β η)^{1/2}, the problem defined by completing (19) with (4)–(5) admits a unique nonnegative nontrivial equilibrium solution \(\overline {n}(x)\) which is given by (11).
Proof of Lemma 1
Consider the PDE problem
Writing
we find that Y(z) satisfies the differential equation
with
It is known that Eq. (21) has solutions which are bounded for all z if and only if a=−m−1/2, where m is a nonnegative integer [77, 78]. These bounded solutions are the Gaussians exp(−z ^{2}/4) multiplied by polynomials of degree m, which form an orthogonal set of functions, and so are everywhere nonnegative if and only if m=0. Therefore, the existence of a nontrivial nonnegative solution of the PDE problem (20) requires a=−1/2. This implies that to have a nontrivial nonnegative equilibrium solution the condition
must be satisfied. If this condition is met, for some \(A \in \mathbb {R}_{+}\)
The constant A can be evaluated in terms of \(\overline {\rho }\) by integrating Eq. (22). We find that
and this concludes the proof of Lemma 1. □
Lemma 2
The integral ρ(t) of the solution of the problem defined by completing (19) with (4)–(5) has the following longtime behaviour:
Proof of Lemma 2
Following the method of proof that we presented in [33], it is possible to prove that, for all nonnegative initial conditions n(x,0) such that 0<ρ(0)<∞,
with the function g(t) satisfying
In the limit t→∞:

if γ<(β η)^{1/2}, then g(t)→0 exponentially rapidly;

if γ=(β η)^{1/2}, then g(t) converges to a positive constant;

if γ>(β η)^{1/2}, then g(t)→∞ exponentially rapidly.
Therefore:

if γ<(β η)^{1/2}, then \({\lim \limits _{t \rightarrow \infty } \rho (t) = 0}\);

if γ=(β η)^{1/2}, then \({\lim \limits _{t \rightarrow \infty } \rho (t) = 0}\);

if γ>(β η)^{1/2}, then \({\lim \limits _{t \rightarrow \infty } \rho (t) = \frac {1}{d}\left [ \gamma  (\beta \eta)^{1/2} \right ]}\).
This concludes the proof of Lemma 2. □
Taken together, Lemma 1 and Lemma 2 allow us to reach the following conclusions:

(i)
if c(·)=0 and γ−(β η)^{1/2}≤0, then
$$ \rho(t) \rightarrow 0, \qquad \text{as }\, t \rightarrow \infty; $$(24) 
(ii)
if c(·)=0 and γ−(β η)^{1/2}>0, then
$$\rho(t) \rightarrow \overline{\rho} = \frac{1}{d}\left[ \gamma(\beta\eta)^{1/2} \right], \qquad \text{as }\, t \rightarrow \infty $$and
$$\overline{n}(x) = \overline{\rho} \; \frac{{(\eta/\beta)^{1/4}}}{(2\pi)^{1/2}} \exp\left[\frac{1}{2}\left(\frac{\eta}{\beta}\right)^{1/2} x^{2}\right]. $$
This establishes the claims of Theorem 1.
Appendix 2: Proof of Theorem 2
When c(·)=C>0, plugging definitions (6)–(7) into Eq. (3) we obtain
Defining
we can rewrite the above equation as
Since \(x \in \mathbb {R}\), there is no loss of generality in translating coordinates so that \(\overline {x}_{c}=0\). Hence, to adapt the method of proof of Theorem 1 to prove Theorem 2 is purely technical. For this reason, we leave Theorem 2 without proof.
Reviewers’ comments
We thank the Reviewers for their comments, all of which are addressed below. Quotations from the Reviewers’ reports are italicised. It was apparent from the comments that some matters required clearer explanation, additional results or greater emphasis, so we have amended the manuscript appropriately.
Reviewer 1  Angela Pisco
In the present paper Lorenzi and coauthors offer a sound theoretical framework to address a critical point on development of drug resistance following treatment. The authors are able to numerically replicate the problem of cell state switching within cancer cell populations composed of cells with different sensitivities to drug. It is now becoming established that cancer treatment is a double edge sword, while the majority of cells die following chemo/radiotherapy, the surviving cells are no innocent bystanders and lead to a more aggressive tumour, mostly composed of cells with a stemcell like phenotype that are multidrug resistant. The authors’ original PDE model is able to replicate published experimental results taking into consideration both nongenetic and environmental conditions. Lorenzi et al. model simulations lead to import conclusions, namely the mathematical demonstration that higher drug doses promote resistant phenotypes and less heterogeneity within cancer cell populations. The entire work is novel and valuable for the community and because of that I’d endorse this paper for publication with minor changes. While I agree that the presented model is general enough for the conclusions to be valid in a panoply of cancers other than leukaemia, I’d like to inquire whether it is feasible with this model to replicate the cycle of sensitivity  resistance  sensitivity... in line with what was described by Sun et al. [Reversible and adaptive resistance to BRAF(V600E) inhibition in melanoma, Nature, 2014].
Authors’ response: We thank the Reviewer for this question. To address the Reviewer’s question, we have performed new numerical simulations considering piecewisecontinuous periodic delivery of the cytotoxic drug. The results obtained are summarised by the movie ‘Additional file 2 ’ and are discussed at point R9 in the revised manuscript. In agreement with the experimental results presented by Sun et al., these results clearly show that administering the cytotoxic drug in an alternate fashion leads to the emergence of cycling subpopulations of drugresistant and drugsensitive cells.
All minor issues pointed out by the Reviewer have been addressed.
Reviewer 2  Sébastien Benzekry
In their manuscript, Lorenzi et al. addressed, from a theoretical perspective, the fundamental issue of drug resistance in cancer cell populations. The article is well written and based on solid biological literature. The authors derived, mathematically analysed and simulated a phenotypestructured PDE model that essentializes key aspects of the problem, including the balance between level of resistance to the drug assault and proliferative rate. This is set in the context of adaptive dynamics driven by inheritable epigenetic changes. In doing so, they add another study to several works of them using the same methodology, with sometimes minor differences among them. Here, one interesting result obtained by the authors is that, depending on the dose of a cytotoxic drug delivered to the tumour, the average phenotypical trait toward which the population concentrates (a fact that is rigorously proven) is not always the same. This result is nontrivial and relevant since it demonstrates from basic and minimal biological hypotheses that the dosing has an impact on the phenotypic distribution of a cancer cell population, a topic with increasingly recognised importance for the treatment of cancers. However, no directly applicable recommendation can be derived for the clinical use of cytotoxic agents. I am not a biologist but I find it debatable that the cells closest to stemness (with x=1) are the ones having the smallest proliferative ability. From my understanding, stem cells could be at the same time more resistant and more proliferatively active.
Authors’ response: We thank the Reviewer for having stressed this point. Following the advice of Reviewer 3, we do not mention stemness anymore in the revised manuscript, as it is unnecessary for our conclusions to hold. Therefore, we state that the phenotypic state x=1 corresponds to the highest level of cytotoxicdrug resistance, without making any reference to stemness.
I don’t understand why functions k and p have to be respectively convex and concave. Wouldn’t it be enough to consider them decreasing/increasing (as functions of the norm of x)?
Authors’ response: This may be an alternative modelling strategy and, from the mathematical perspective, it may be interesting to explore it. However, concavity and convexity assumptions lead naturally to smooth fitness landscapes which are close to the approximate fitness landscapes inferred from experimental data through regression techniques [see, for instance, Otwinowski, J., and Plotkin, J.B. (2014). Inferring fitness landscapes by regression produces biased estimates of epistasis. Proc. Natl. Acad. Sci. USA 111(22), E2301–E2309 and references therein].
I also find it surprising, if not inconsistent, that the proliferation rate p(x) can take negative values, while being defined to be the “proliferation due to the assumed velocity of the cell cycle in the absence of betweencell competition for nutrients, and in the absence of druginduced death”. This appears to me to be the underlying reason of the possibility of extinction of the population (first part of Theorem 1), which is quite surprising and sounds biologically unrealistic, in the absence of treatment.
Authors’ response: We thank the Reviewer for his observation. As stated both in the old version version of the manuscript and in the updated manuscript, the function p(x) “stands for the net proliferation rate of cancer cells in the phenotypic state x”. The sentence quoted by the Reviewer from the old version of manuscript was not pertinent and it has been removed from the updated manuscript.
In Table 1, units of the parameters should be provided, when appropriate. What motivated the choice of K=10^{8} cells (no reference is provided)?
Authors’ response: Units have been included in Table 1, and a reference motivating the choice of the value of the carrying capacity K has been added.
What biological situation is modelled here: an in vitro cell line? in vivo tumours in animal models? a clinical patient tumour?
Authors’ response: We thank the Reviewer for this observation. We have clarified this point. As stated in the updated manuscript, we consider an in vitro culture system.
I appreciate the efforts of the authors to adopt relevant values of the parameters based on the literature. However, the value of γ taken seems particularly high (it gives a doubling time of l o g(2)/g a m m a∗24=3.34 hours, which is much faster than the fastest mammalian cell cycle time [1]). This explains why, in Fig. 1 b, the cell population reaches the carrying capacity so fast, probably much faster than in the biological reality. The authors might want to choose a more meaningful value for the duration of the fittest cancer cells’ cycle duration, such as about 25 h. [1] Steel, G. G. and Lamerton, L. F. (1966). The growth rate of human tumours. Br. J. Cancer, 20(1):74–86
Authors’ response: We thank the Reviewer for this suggestion. Following the Reviewer’s advice, we updated the value of the parameter γ so that the duration of the fittest cancer cells’ cycle duration is about 25 h. Because of this, we updated also the values of the parameters β and η following the reasonings presented in the updated manuscript, and we rerun all simulations. Therefore, all figures in the paper have been updated.
All minor issues pointed out by the Reviewers have been addressed.
Reviewer 3  Heiko Enderling
Lorenzi et al. present a mathematical model of phenotypically structured cancer cell populations, and track the evolution of phenotype heterogeneity in the absence of or under selection pressure of a cytotoxic drug. The model is based on previous literature and extended to study continuous heterogeneity and plasticity. The manuscript is well prepared, the work is coherently presented, and the results are clearly discussed. Most of the results are as one would expect, attributing to careful model development. Some results are intriguing, for example indications that maximum tolerable dose may not be the best longterm strategy for tumour control, and that a metronomic scheme may provide a suitable alternative. While certainly plausible, these scenarios can be readily explored with the model and should be included in the manuscript. In particular, it would be interesting to see the temporal evolution of tradeoffs between tumour volume reduction and selection for resistance in an MTD vs. metronomic setting.
Authors’ response: We thank the Reviewer for this suggestion. To address the Reviewer’s question, we have performed new numerical simulations comparing the administration of highdrug doses separated by drugfree periods with the continuous delivery of relatively lowdrug doses. The results obtained are summarised by Fig. 8 and are discussed at point R10 in the revised manuscript. These results suggest that the first type of protocol causes a drastic reduction in the number of cancer cells, although it fosters an increase in the average level of resistance in the population. On the other hand, the second type of protocol maintains a larger tumour burden characterised by a relatively lower average level of resistance. A more accurate comparison between the efficacy of the two therapeutic approaches would require a careful investigation of the respective adverse effects on healthy cells, which cannot be performed using our model. However, we can envisage a lower druginduced toxicity being associated to the second type of protocols [see, for instance, Gately, S., Kerbel, R. (2001). Antiangiogenic scheduling of lower dose cancer chemotherapy. Cancer J., 7(5), 427–436]. In the light of this observation, the analytical results of Theorem 2 and the numerical results summarised in Fig. 8 suggest that therapeutic protocols consisting of phases of highdose delivery separated by drugfree periods may not offer the best longterm strategy for tumour control, and that protocols based on the continuous delivery of relatively lowdrug doses may represent a suitable alternative.
My major critique is the discussion of cancer stem cells for treatment resistance. The authors introduce a trade off between proliferation and quiescence opposing a gradient of differentiated and cancer stem cells. While this might be biologically realistic, the developed mathematical model does not reflect a cellular hierarchy. In contrast, in the model as is, a population of nonstem cancer cells would grow infinitely in the absence of an initiating and propagating cancer stem cell – a clear violation of the biological concept. As the presented model, results and discussion are solely dependent and reproducible with a proliferation gradient alone, I recommend the stem cell component to be dropped. The oftenattributed cancer stem cell quiescence may be discussed as further support for applicability of the model at the end of the manuscript.
Authors’ response: We thank the Reviewer for this observation. Following the Reviewer’s advice, we do not make any reference to stemness in the revised manuscript, as it is unnecessary for our conclusions to hold.
References
Aktipis CA, Boddy AM, Gatenby RA, Brown JS, Maley CC. Life history tradeoffs in cancer evolution. Nat Rev Cancer. 2013; 13(12):883–92.
Dexter DL, Kowalski HM, Blazar BA, Fligiel Z, Vogel R, Heppner GH. Heterogeneity of tumor cells from a single mouse mammary tumor. Cancer Res. 1978; 38(10):3174–81.
Greaves M, Maley CC. Clonal evolution in cancer. Nature. 2012; 481(7381):306–13.
Korolev KS, Xavier JB, Gore J. Turning ecology and evolution against cancer. Nat Rev Cancer. 2014; 14(5):371–80.
Merlo LM, Pepper JW, Reid BJ, Maley CC. Cancer as an evolutionary and ecological process. Nat Rev Cancer. 2006; 6(12):924–35.
Nowell PC. The clonal evolution of tumor cell populations. Science. 1976; 194(4260):23–8.
Marusyk A, Almendro V, Polyak K. Intratumour heterogeneity: a looking glass for cancer?Nat Rev Cancer. 2012; 12(5):323–34.
Brock A, Chang H, Huang S. Nongenetic heterogeneity—a mutationindependent driving force for the somatic evolution of tumours. Nat Rev Genet. 2009; 10(5):336–42.
Glasspool R, Teodoridis JM, Brown R. Epigenetics as a mechanism driving polygenic clinical drug resistance. Br J Cancer. 2006; 94(8):1087–92.
Gupta PB, Fillmore CM, Jiang G, Shapira SD, Tao K, Kuperwasser C, Lander ES. Stochastic state transitions give rise to phenotypic equilibrium in populations of cancer cells. Cell. 2011; 146(4):633–44.
Newman JR, Ghaemmaghami S, Ihmels J, Breslow DK, Noble M, DeRisi JL, Weissman JS. Singlecell proteomic analysis of s. cerevisiae reveals the architecture of biological noise. Nature. 2006; 441(7095):840–6.
Raj A, van Oudenaarden A. Nature, nurture, or chance: stochastic gene expression and its consequences. Cell. 2008; 135(2):216–26.
Chang HH, Oh PY, Ingber DE, Huang S. Multistable and multistep dynamics in neutrophil differentiation. BMC Cell Biol. 2006; 7(1):11.
Pisco AO, Brock A, Zhou J, Moor A, Mojtahedi M, Jackson D, Huang S. Nondarwinian dynamics in therapyinduced cancer drug resistance. Nat Commun. 2013; 4:2467.
Sharma SV, Lee DY, Li B, Quinlan MP, Takahashi F, Maheswaran S, McDermott U, Azizian N, Zou L, Fischbach MA, et al.A chromatinmediated reversible drugtolerant state in cancer cell subpopulations. Cell. 2010; 141(1):69–80.
Chisholm RH, Lorenzi T, Clairambault J. Cell population heterogeneity and evolution towards drug resistance in cancer: biological and mathematical assessment, theoretical treatment optimisation. Biochimica et Biophysica Acta (BBA)  General Subjects, in press. 2016.
Huang S. Genetic and nongenetic instability in tumor progression: link between the fitness landscape and the epigenetic landscape of cancer cells. Cancer Metastasis Rev. 2013; 32(3–4):423–48.
Altrock PM, Liu LL, Michor F. The mathematics of cancer: integrating quantitative models. Nat Rev Cancer. 2015; 15(12):730–45.
Anderson AR, Quaranta V. Integrative mathematical oncology. Nat Rev Cancer. 2008; 8(3):227–34.
Byrne HM. Dissecting cancer through mathematics: from the cell to the animal model. Nat Rev Cancer. 2010; 10(3):221–30.
Davies P, Demetrius L, Tuszynski JA. Cancer as a dynamical phase transition. Theor Biol Med Modell. 2011; 8:30.
Enderling H, AJ Chaplain M. Mathematical modeling of tumor growth and treatment. Curr Pharm Des. 2014; 20(30):4934–40.
Enderling H, Rejniak KA. Simulating cancer: computational models in oncology. Front Oncol. 2013; 3:233.
Gatenby RA, Maini PK. Mathematical oncology: cancer summed up. Nature. 2003; 421(6921):321.
Powathil GG, Swat M, Chaplain MA. Systems oncology: Towards patientspecific treatment regimes informed by multiscale mathematical modelling. Semin Cancer Biol. 2015; 30:13–20.
Stiehl T, Baran N, Ho AD, MarciniakCzochra A. Cell division patterns in acute myeloid leukemia stemlike cells determine clinical course: a model to predict patient survival. Cancer Res. 2015; 75(6):940–9.
Tuszynski JA, Winter P, White D, Tseng CY, Sahu KK, Gentile F, Spasevska I, Omar SI, Nayebi N, Churchill CD, et al.Mathematical and computational modeling in biology at multiple scales. Theor Biol Med Modell. 2014; 11(1):52.
Thomas F, Fisher D, Fort P, Marie JP, Daoust S, Roche B, Grunau C, Cosseau C, Mitta G, Baghdiguian S, et al.Applying ecological and evolutionary theory to cancer: a long and winding road. Evol Appl. 2013; 6(1):1–10.
Perthame B. Transport Equations in Biology. Basel: Birkhäuser; 2006.
Perthame B. Parabolic Equations in Biology. BerlinHeidelberg: Springer; 2015.
Champagnat N, Ferrière R, Ben Arous G. The canonical equation of adaptive dynamics: a mathematical view. Selection. 2002; 2(1–2):73–83.
Champagnat N, Ferrière R, Méléard S. Unifying evolutionary dynamics: from individual stochastic processes to macroscopic models. Theor Popul Biol. 2006; 69(3):297–321.
Chisholm RH, Lorenzi T, Desvillettes L, Hughes BD. Evolutionary dynamics of phenotypestructured populations: from individuallevel mechanisms to populationlevel consequences. Z Angew Math Phys. 2016; 67(4):1–34.
Clairambault J. Can theorems help treat cancer?J Math Biol. 2012; 66(7):1555–8.
Lorz A, Lorenzi T, Hochberg ME, Clairambault J, Perthame B. Populational adaptive evolution, chemotherapeutic resistance and multiple anticancer therapies. ESAIM: Math Modell Numer Anal. 2013; 47(02):377–99.
Lorz A, Lorenzi T, Clairambault J, Escargueil A, Perthame B. Modeling the effects of space structure and combination therapies on phenotypic heterogeneity and drug resistance in solid tumors. Bull Math Biol. 2015; 77(1):1–22.
Chisholm RH, Lorenzi T, Lorz A, Larsen AK, De Almeida LN, Escargueil A, Clairambault J. Emergence of drug tolerance in cancer cell populations: An evolutionary outcome of selection, nongenetic instability, and stressinduced adaptation. Cancer Res. 2015; 75(6):930–9.
Pisco A, Huang S. Nongenetic cancer cell plasticity and therapyinduced stemness in tumour relapse:‘what does not kill me strengthens me’. Br J Cancer. 2015; 112(11):1725–32.
Hanahan D, Weinberg RA. Hallmarks of cancer: the next generation. Cell. 2011; 144(5):646–74.
Medema JP. Cancer stem cells: the challenges ahead. Nat Cell Biol. 2013; 15(4):338–44.
Menendez JA, Alarcón T. Metabostemness: A new cancer hallmark. Front Oncol. 2014; 4:121–262.
Lorenzi T, Chisholm RH, Desvillettes L, Hughes BD. Dissecting the dynamics of epigenetic changes in phenotypestructured populations exposed to fluctuating environments. J Theor Biol. 2015; 386:166–76.
Chisholm RH, Lorenzi T, Lorz A. Effects of an advection term in nonlocal lotkavolterra equations. Commun Math Sci. 2016; 14:1181–8.
Becker C, Hagmann J, Müller J, Koenig D, Stegle O, Borgwardt K, Weigel D. Spontaneous epigenetic variation in the arabidopsis thaliana methylome. Nature. 2011; 480:245–9.
Navin NE. Cancer genomics: one cell at a time. Genome Biol. 2014; 15(8):452.
LeVeque RJ, Vol. 98. Finite Difference Methods for Ordinary and Partial Differential Equations: Steadystate and Timedependent Problems. Philadelphia: Society for Industrial and Applied Mathematics (SIAM); 2007.
Steel G, Lamerton L. The growth rate of human tumours. Br J Cancer. 1966; 20(1):74.
Bozic I, Reiter JG, Allen B, Antal T, Chatterjee K, Shah P, Moon YS, Yaqubie A, Kelly N, Le DT, et al.Evolutionary dynamics of cancer in response to targeted combination therapy. Elife. 2013; 2:00747.
Bozic I, Allen B, Nowak MA. Dynamics of targeted cancer therapy. Trends Mol Med. 2012; 18(6):311–6.
Gately S, Kerbel R. Antiangiogenic scheduling of lower dose cancer chemotherapy. Cancer J. 2001; 7(5):427–36.
Cohen AA, GevaZatorsky N, Eden E, FrenkelMorgenstern M, Issaeva I, Sigal A, Milo R, CohenSaidon C, Liron Y, Kam Z, et al.Dynamic proteomics of individual cancer cells in response to a drug. Science. 2008; 322(5907):1511–6.
Delitala M, Lorenzi T. A mathematical model for the dynamics of cancer hepatocytes under therapeutic actions. J Theor Biol. 2012; 297:88–102.
Delitala M, Lorenzi T. A mathematical model for progression and heterogeneity in colorectal cancer dynamics. Theor Popul Biol. 2011; 79(4):130–8.
Jänne PA, Gray N, Settleman J. Factors underlying sensitivity of cancers to smallmolecule kinase inhibitors. Nat Rev Drug Discov. 2009; 8(9):709–23.
Lavi O, Greene JM, Levy D, Gottesman MM. The role of cell density and intratumoral heterogeneity in multidrug resistance. Cancer Res. 2013; 73(24):7168–75.
Spencer SL, Gaudet S, Albeck JG, Burke JM, Sorger PK. Nongenetic origins of celltocell variability in trailinduced apoptosis. Nature. 2009; 459(7245):428–32.
De Bruin EC, Taylor TB, Swanton C. Intratumor heterogeneity: lessons from microbial evolution and clinical implications. Genome Med. 2013; 5(11):101.
Acar M, Mettetal JT, van Oudenaarden A. Stochastic switching as a survival strategy in fluctuating environments. Nat Genet. 2008; 40(4):471–5.
Gerlinger M, Rowan AJ, Horswell S, Larkin J, Endesfelder D, Gronroos E, Martinez P, Matthews N, Stewart A, Tarpey P, et al.Intratumor heterogeneity and branched evolution revealed by multiregion sequencing. N Eng J Med. 2012; 366(10):883–92.
Minchinton AI, Tannock IF. Drug penetration in solid tumours. Nat Rev Cancer. 2006; 6(8):583–92.
Trédan O, Galmarini CM, Patel K, Tannock IF. Drug resistance and the solid tumor microenvironment. J Nat Cancer Inst. 2007; 99(19):1441–54.
Sun C, Wang L, Huang S, Heynen GJ, Prahallad A, Robert C, Haanen J, Blank C, Wesseling J, Willems SM, et al.Reversible and adaptive resistance to braf (v600e) inhibition in melanoma. Nature. 2014; 508(7494):118–22.
André N, Carré M, Pasquier E. Metronomics: towards personalized chemotherapy?Nat Rev Clin Oncol. 2014; 11(7):413–31.
Benzekry S, Pasquier E, Barbolosi D, Lacarelle B, Barlési F, André N, Ciccolini J. Metronomic reloaded: theoretical models bringing chemotherapy into the era of precision medicine: 2015. p 53–61.
Hanahan D, Bergers G, Bergsland E. Less is more, regularly: metronomic dosing of cytotoxic drugs can target tumor angiogenesis in mice. J Clin Investig. 2000; 105(8):1045–7.
Scharovsky OG, Mainetti LE, Rozados VR. Metronomic chemotherapy: changing the paradigm that more is better. Curr Oncol. 2009; 16(2):7–15.
Gatenby RA, Silva AS, Gillies RJ, Frieden BR. Adaptive therapy. Cancer Res. 2009; 69(11):4894–903.
Bremnes RM, Dønnem T, AlSaad S, AlShibli K, Andersen S, Sirera R, Camps C, Marinez I, Busund LT. The role of tumor stroma in cancer progression and prognosis: emphasis on carcinomaassociated fibroblasts and nonsmall cell lung cancer. J Thoracic Oncol. 2011; 6(1):209–17.
Cirri P, Chiarugi P. Cancerassociatedfibroblasts and tumour cells: a diabolic liaison driving cancer progression. Cancer Metastasis Rev. 2012; 31(1–2):195–208.
Mao Y, Keller ET, Garfield DH, Shen K, Wang J. Stromal cells in tumor microenvironment and breast cancer. Cancer Metastasis Rev. 2013; 32(1–2):303–15.
Nieman KM, Kenny HA, Penicka CV, Ladanyi A, BuellGutbrod R, Zillhardt MR, Romero IL, Carey MS, Mills GB, Hotamisligil GS, et al.Adipocytes promote ovarian cancer metastasis and provide energy for rapid tumor growth. Nat Med. 2011; 17(11):1498–503.
MendozaJuez B, MartínezGonzález A, Calvo GF, PérezGarcía VM. A mathematical model for the glucoselactate metabolism of in vitro cancer cells. Bull Math Biol. 2011; 74(5):1125–42.
Smallbone K, Gatenby RA, Gillies RJ, Maini PK, Gavaghan DJ. Metabolic changes during carcinogenesis: Potential impact on invasiveness. J Theor Biol. 2007; 244(4):703–13.
Goding CR, Pei D, Lu X. Cancer: pathological nuclear reprogramming?Nat Rev Cancer. 2014; 14(8):568–73.
Delhommeau F, Dupont S, Della Valle V, et al.Mutation in TET2 in myeloid cancers. N Eng J Med. 2009; 360(22):2289–301.
Solary E, Bernard OA, Tefferi A, Fuks F, Vainchenker W. The teneleven translocation2 (tet2) gene in hematopoiesis and hematopoietic diseases. Leukemia. 2013; 28(3):485–96.
Miller J. Parabolic cylinder functions. In: Handbook of Mathematical Functions. Washington, DC: U.S. Government Printing Office: 1964. p. 686–720.
Temme NM. Parabolic cylinder functions In: Olver FWJ, Lozier DW, Boisvert RF, Clark CW, editors. NIST Handbook of Mathematical Functions, Ch. 12. Cambridge University Press: 2010.
Acknowledgements
This work was supported in part by the French National Research Agency through the “ANR blanche” project Kibord [ANR13BS010004]. The authors thank the Reviewers for their most helpful and insightful comments on the article.
Authors’ contributions
TL performed mathematical study of the model, carried out data processing, and was involved in interpretation of results and drafting of the manuscript. RC made substantial contributions to interpretation of data and critical revision of the manuscript. JC made substantial contributions to critical revision of the manuscript and coordinated the project. All authors gave final approval for publication. All authors read and approved the final manuscript.
Competing interests
The authors declare that they have no competing interests.
Author information
Authors and Affiliations
Corresponding author
Additional files
Additional file 1: Evolution of an initial population which is mainly composed of cells in the phenotypic state that corresponds to the highest level of cytotoxicdrug resistance, in the absence of xenobiotic agents. This movie shows the evolution of an initial population which is mainly composed of cells in the phenotypic state x=1 (i.e., the phenotypic state that corresponds to the highest level of cytotoxicdrug resistance) for c(·)=0 (i.e., in the absence of xenobiotic agents). The values of the model parameters are as in Table 1. The pink line indicates the equilibrium population density for c(·)=0 [i.e., the population density \(\overline {n}(x)\) of Eq. (11)]. In agreement with the experimental results presented in [14], it takes approximatively 18 days for the population to reconstitute the equilibrium phenotypic distribution. (MOV 203 kb)
Additional file 2: The cancer cell population regains cytotoxicdrug sensitivity when drug delivery is discontinued. This movie shows the evolution of an initial population which is mainly composed of highly proliferative cells (i.e., cells in the phenotypic state x=0) exposed to periodic phases of highdose delivery (drug dose corresponding to the LC_{90}) separated by drugfree periods. The values of the model parameters are as in Table 1. The red and blue lines highlight the highly proliferative state x=0 and the highly drugresistant state x=1. In agreement with the experimental results presented in [62], these results clearly show that administering the cytotoxic drug in an alternate fashion leads to the emergence of cycling subpopulations of drugresistant and drugsensitive cells. (MOV 415 kb)
Rights and permissions
Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License(http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The Creative Commons Public Domain Dedication waiver(http://creativecommons.org/publicdomain/zero/1.0/) applies to the data made available in this article, unless otherwise stated.
About this article
Cite this article
Lorenzi, T., Chisholm, R.H. & Clairambault, J. Tracking the evolution of cancer cell populations through the mathematical lens of phenotypestructured equations. Biol Direct 11, 43 (2016). https://doi.org/10.1186/s1306201601434
Received:
Accepted:
Published:
DOI: https://doi.org/10.1186/s1306201601434
Keywords
 Cancer cell populations
 Phenotypic evolution
 Natural selection
 Phenotype plasticity
 Epimutations
 Cytotoxicdrug resistance
 Phenotypic heterogeneity
 Mathematical oncology
 Phenotypestructured equations