Nonlinear Evolution Equations and Its Application to a Tumour Invasion Model ()

Akisato Kubo^{1}, Yuto Miyata^{2}, Hidetoshi Kobayashi^{3}, Hiroki Hoshino^{1}, Naoki Hayashi^{4}

^{1}Department of Mathematics, School of Health Sciences, Fujita Health University, Toyoake, Japan.

^{2}Medical Radiation Sciences, Graduate School of Health Sciences, Fujita Health University, Toyoake, Japan.

^{3}Department of Radiation Oncology, School of Medicine, Fujita Health University, Toyoake, Japan.

^{4}Faculty of Radiological Technology, School of Health Sciences, Fujita Health University, Toyoake, Japan.

**DOI: **10.4236/apm.2016.612066
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We consider nonlinear evolution equations with logistic term satisfying initial Neumann-boundary condition and show global existence in time of solutions to the problem in arbitrary space dimension by using the method of energy. Applying the result to a mathematical model of tumour invasion, we discuss the property of the rigorous solution to the model. Finally we will show the time depending relationship and interaction between tumour cells, the surrounding tissue and matrix degradation enzymes in the model by computer simulations. It is seen that our mathematical result of the existence and asymptotic behaviour of solutions verifies our simulations, which also confirm the mathematical result visibly.

Keywords

Nonlinear Evolution Equation, Mathematical Analysis, Tumour Invasion, Proliferation, Re-Establishment

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Kubo, A. , Miyata, Y. , Kobayashi, H. , Hoshino, H. and Hayashi, N. (2016) Nonlinear Evolution Equations and Its Application to a Tumour Invasion Model. *Advances in Pure Mathematics*, **6**, 878-893. doi: 10.4236/apm.2016.612066.

1. Introduction

In this paper we consider the initial Neumann-boundary value problem of nonlinear evolution equations with logistic term, arising from tumour invasion models with proliferation and re-establishment: (NE)

where for, D and μ are positive constants, Ω is a bounded domain in and is a smooth boundary of Ω and is the outer unit normal vector.

Let us introduce function spaces used in below. First, denotes the usual Sobolev space of order l on Ω. For functions and defined in, we denote

where is a multi-index for.

The eigenvalues of with the homogeneous Neumann boundary conditions are denoted by satisfying and indicates the normalized eigenfunction corresponding to. For a non-negative integer l, we set as a closure of in the function space. It is noticed that we have for, which enables us to use Poincare’s Inequality.

Putting in (1) it follows from (1) that

where and are positive parameters. (NE) is rewritten by the following problem.

where We will show the global existence in time of solutions of (RP), which gives our desired result of (NE).

Applying the above result to the following mathematical model of tumour invasion proposed by Chaplain and Lolas [1] , we have a rigorous mathematical understanding to tumour invasion for the key variables, and.

where is the density of tumour cells, is matrix degradation enzymes (MDEs) concentration and is extracellular matrix (ECM) density in and, , , , , , and are positive constants. In the right hand side of (4) the second, third and fourth terms mean chemotaxis, haptotaxis and proliferation of tumour cell respectively. Also the second term of the right hand side of (5) describes the re-establishment of ECM. We consider an initial boundary value problem for (C-L) satisfying

,

where are initial data of.

Chaplain and Anderson [2] , corresponding to the case of in (C-L), proposed a mathematical model on generic solid tumour growth at the avascular stage. While most tumours are asymptomatic at this stage, it is still possible for cells to escape and migrate to the lymph nodes and for more aggressive tumours to invade.

In our previous papers [3] [4] , we consider only the case of and for our convenience. In this paper we may consider the case where is sufficiently small positive constant. Actually compared with the effect of haptotaxis, the one of chemotaxis is very small. Furthermore we study the case of, which describes tumour invasion phenomena with tumour cell proliferation and re-establishment of ECM respectively.

In the final section by computer simulations of our model (by Mathematica 8) we can easily observe time-dependent interaction and the relationship between the above components in complicated procedure of tumour invasion and a comparison to our rigorous mathematical result. Comparing our mathematical result with computer simulations we will gain a better understanding of the mechanism of tumour invasion.

2. Existence Theorem of (NE)

By deriving the energy estimate of (RP) (see [3] - [9] ) and considering the iteration scheme we obtain existence of solutions to (RP) by the standard argument to show the convergence of solutions of the iteration scheme.

In the same way as used in [3] [4] [5] [6] [7] we have the following estimates of (RP). We begin with in order to obtain a basic estimate of (RP). Then we have for,

by the integration by parts

(7)

It is noticed that the following estimate is obtained in [4] [5] [6] [7] for,

(8)

Then for the nonlinear term we have by using (8)

(9)

where we used Dionne [10] for the estimate of nonlinear terms and is sufficiently small positive constant. Therefore we have by integrating the both sides of (7) over and using (9)

(10)

where we denote

Since the last term of the right hand side of (10) is negligible for sufficiently small, we have by integration by parts with respect to t

(11)

Taking sufficiently large for the second term of the right hand side of (11) is negligible. Since if, the third term in the left hand side of (11) is positive. Then we obtain a basic energy estimate

(12)

Replacing, instead of in the above procedure, we obtain the following estimate of higher order.

Lemma 1 (Energy estimate of (RP)) Assume that for satisfies appropriate smooth regularity condition. Supposed that we have the energy estimate of (RP) for

(13)

where we denote for any non-negative integer,

We consider the iteration scheme of (RP):

where

(13) guarantees the uniformly bounded estimate of for. We determine by the solution of the following ordinary equations with initial data.

The local existence in time of is shown by the theory of ordinary differential equations. Therefore, by the energy estimates, the global existence in time of the solution satisfying the regularity required for Lemma 1 and justification of the limiting process are assured by the standard method. The energy estimate enables us to get the solution of (RP) in

by considering and standard argument of convergence for (see [3] - [9] ).

Then we obtain the following result of (NE) by using the above result of (RP).

Theorem 2 Assume that for satisfies appropriate smooth regularity condition, initial data are sufficiently smooth for, and that is small enough. For sufficiently large, there is a solution for

to (NE) such that it satisfies the following asymptotic behavior

3. Application to a Tumour Invasion Model

Their mathematical approach to above models mainly depends on numerical analysis. In this paper first we show the rigorous mathematical result of (C-L) and then computer simulations, of which the validity is guaranteed by our mathematical result.

On the other hand, there are many mathematical models which can be found in the literature describing tumour angiogenesis. In [20] Levine and Sleeman applied the mathematical model of Othmer and Stevens [21] for the understanding of tumour angiogenesis, which arises in the theory of reinforced random walk. Anderson and Chaplain [12] proposed a model of tumour angiogenesis taking account of endothelial tip-cell migration. The model describes cell migration governed by three factors: diffusion, chemotaxis and haptotaxis.

Rigorous Mathematical approaches to tumour growth models have been known (see [3] - [9] [20] [21] [22] [23] [24] ). Levine and Sleeman [20] and Yang, Chen and Liu [24] studied the global existence in time of solutions and blow up ones to a simplified Othmer and Stevens model. Kubo et al. [3] - [9] show the time global solution and asymptotic behavior of the solution to the mathematical models proposed by [2] [12] [20] [21] [23] .

3.1. Reduced Problem

Following to Levine and Sleeman [20] we reduce our problem to a simpler system (see [3] - [9] [20] ). It is easily seen in (5) that is written by

(14)

Integrating (14) over for

Put and for a constant. Then we have

denoting and

(15)

Substituting by the right hand side of (14), from (4) and (6) it follows that for

(16)

and

(17)

The nonlinear evolution Equation (1) involves (16) and so we can apply Theorem 2 to (16).

3.2. Existence Theorem of (C-L) with

The Equations (16) and (17) are essentially regarded as the same type of equation as (1). Hence the energy estimates of and are obtained and combining these estimates we obtain the desired estimate (cf. [3] [4] [5] [6] [7] ).

Lemma 3 (Energy estimate of (C-L)) We obtain the energy inequality of the reduced problem (16) and (17) with zero-Neumann boundary condition for and sufficiently large

(18)

where as.

Then applying the same argument as used for Theorem 2 to the above mathematical model, we obtain global existence in time and asymptotic behaviour of the solutions to our mathematical model.

Our main result for is as follows.

Theorem 4 For smooth initial data assume that - norms of, and are sufficiently small, then there are classical solutions of (C-L) for: such that they satisfy the following asymptotic behavior for

Also we can deal with the case of as follows.

3.3. Existence Theorem of (C-L) with

In for, especially we may consider -inner product composed of the chemotaxis term and

in the same way as in Section 2

where we can take small enough for sufficiently small. It is noticed that compared with the effect of haptotaxis, the one of chemotaxis may be quite small. Hence since we can have the same estimate as Lemma 3 for sufficiently small, the same result as in Theorem 4 holds for this case too.

Theorem 5 Under the same assumption as in Theorem 4 we further assume that is sufficiently small, then we obtain the same result as stated in Theorem 4.

4. Computer Simulations

In Kolev and Zubik-Kowal [16] the same type model of (C-L) for was considered and they obtained numerical solutions. In this paper our advantage is to show global existence in time of rigorous mathematical smooth solutions of the model and based on it carry out computer simulations.

In the following Figures 1-7 illustrated below we show the graphs along the time by the computer simulations of the model at and 1.35 by Mathematica 8. We use the parameter values of, , , , , , , and specified below.

We will observe the time dependent relationship and interaction between tumour cells (Red line), the surrounding tissue (Black line) and degradation enzymes (Green line). In the graphs below a coordinate axis of the horizontal direction indicates the spatial position and vertical direction indicates the density or concentration of each component of the model.

Figure 1. Interactions between the tumour and the surrounding tissue without proliferation of tumour cell, migration, and ECM re-establishment: The parameter values d_{n} = 0.001, d_{m} = 0.001, γ = 0.02, η = 10, μ_{1} = 0, μ_{2} = 0, α = 0 and β = 0.1, x_{n} = 0. We can observe that MDEs degradates the surrounding tissue, and makes space into which tumour cells move. Further tumour cells form a small peak and keep going forward inside ECM, preserving the shape.

Figure 2. Tumour cell proliferation, migration, and interactions between the tumour and the surrounding tissue without ECM re-establishment: The parameter values d_{n} = 0.001, d_{m} = 0.001, γ = 0.02, η = 10, μ_{1} = 5, μ_{2} = 0, α = 0.1 and β = 0.1, x_{n} = 0. It is seen that tumour cell density becomes much higher than in Figure 1 inside ECM and maintains the upper bound of the logistic curve constantly.

Figure 3. Tumour cell proliferation, migration, without ECM re-establishment, and interactions between the tumour and the surrounding tissue: The parameter values d_{n} = 0.001, d_{m} = 0.001, γ = 0.02, η = 10, μ_{1} = 10, μ_{2} = 0, α = 0.1 and β = 0.1, x_{n} = 0. Increasing μ_{1} more, it is observed that tumour cell density inside ECM become higher than in Figure 2.

Figure 4. Tumour cell proliferation, migration, ECM re-establishment, and interactions between the tumour and the surrounding tissue: The parameter values d_{n} = 0.001, d_{m} = 0.001, γ = 0.02, η = 10, μ_{1} = 5, μ_{2} = 0.001, α = 0.1 and β = 0.1, x_{n} = 0. We take μ_{2} = 0.001 only and other parameters are same as in Figure 2. Then the tumour cell density is almost same as in Figure 2.

Figure 5. Tumour cell proliferation, migration, ECM re-establishment, and interactions between the tumour and the surrounding tissue: The parameter values d_{n} = 0.001, d_{m} = 0.001, γ = 0.02, η = 10, μ_{1} = 5, μ_{2} = 1, α = 0.1 and β = 0.1, x_{n} = 0. When taking μ_{2} = 0.001, compared with Figure 2 and Figure 4, it is clear that the invasive area of tumour cells inside ECM is much more limited.

Figure 6. Tumour cell proliferation, migration, ECM re-establishment, and interactions between the tumour and the surrounding tissue: The parameter values d_{n} = 0.001, d_{m} = 0.001, γ = 0.02, η = 10, μ_{1} = 5, μ_{2} = 5, α = 0.1 and β = 0.1, x_{n} = 0. Compared with Figure 4 and Figure 5, the reachable range of tumour cells is observed to be more suppressed by taking μ_{2} = 5.

Figure 7. Tumour cell proliferation, chemotaxis, migration, ECM re-establishment, and interactions between the tumour and the surrounding tissue: The parameter values d_{n} = 0.001, d_{m} = 0.001, γ = 0.02, η = 10, μ_{1} = 5, μ_{2} = 0, α = 0.1 and β = 0.1, x_{n} = 0.01. By the effect of chemotaxis (x_{n} = 0.01), tumour cells are attracted by MDEs, the density is beyond 1 at t = 0.25 ~ 0.5, eventually it converges to 1 and after that keeps it constantly.

5. Conclusions

In order to obtain the global existence in time and asymptotic profile of solutions of a mathematical model of tumour invasion proposed by Chaplain and Lolas, we investigate nonlinear evolution equations with logistic term related to our mathematical models as an initial Neumann-boundary value problem. We could show the global existence in time of rigorous mathematical solutions to the initial boundary value problem for the model in arbitrary space dimension by using the energy inequalities. Applying the result to our model we show global existence in time of mathematical solutions of the model.

By Figures 1-7, it is recognized that our rigorous mathematical result of the existence and asymptotic behaviour of smooth solutions verifies our computer simulations and confirms the pattern form of each component of the model in the graphs respectively. Then we can gain the understanding of the process of tumour invasion more in details.

Acknowledgements

This work was supported in part by the Grants-in-Aid for Scientific Research (C) 19540200, 22540208, 25400148 and 16K05214 from Japan Society for the Promotion of Science.

Conflicts of Interest

The authors declare no conflicts of interest.

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