We present a mathematical analysis of a reaction-diffusion model in a bounded open domain which describes vascular endothelial growth factor(VEGF), endothelial cells and oxygen. We use the parabolic theory to prove the existence of the solution in the function space
under the homogeneous Neumann conditions. Then we get the existence of nonnegative solution in
by using the global Schauder estimation.
Angiogenesis is a physiological process, which involves the formation of new capillary network germinated from the existing vascular network, and plays an important role in embryo development, wound healing and tumor growth. For example, it has been recognized that the growth of capillaries through blood vessels leads to the vascularization of tumors, which provides the tumor with its own dedicated blood supply, thus allowing rapid growth and metastasis of tumors. In the past decade, a lot of work has been done on the mathematical model of tumor growth; for example, see 1, 2, 3, 4, 5, 6, 7 and the references therein. In particular, the role of angiogenesis in tumor growth has also attracted wide attention, see 8, 9, 10, 11, 12 and the cited literature.
This paper is concerned with the chemotaxis system which has been proposed in 13 as a modification of the angiogenesis model, in order to describe how cancer cells affect vascular endothelial growth factor (VEGF), endothelial cells and oxygen in angiogenesis. Let be an open and bounded domain, and denote
and
In this paper, we study the following chemotaxis system
![]() | (1.1) |
where is the derivative in the outward normal direction on
and
is the unit outer normal vector field on
is the cancer cell density,
is VEGF density,
is the number of endothelial cells, and
is oxygen,
are positive constants denoting the growth rate and the death rate, respectively.
In the mathematical modeling of self-organization of living cells, the Keller-Segel system of partial differential equations, has played an increasingly important role in the last decades. It is used to describe the overall behavior of a collection of cells under the influence of chemotaxis. Under such circumstances, the movement of each individual cell, though still not precisely predictable, follows a favorite direction, namely that towards higher concentrations of a certain chemical signal substance, see 2. The first equation in (1.1) represents the hypothesis that the model depends on the growth of cancer cells. The second equation in (1.1) thus reflects the interplay of undirected diffusion movement on the hand and chemotactical movement driven by on the other. The third equation in (1.1) expresses the hypothesis that oxygen is produced by endothelial cells in addition to diffusion.
VEGF is an important regulatory specific factor for endothelial cell proliferation, migration, and in physiolo-gical and pathological angiogenesis. Endothelial cells are the cells that line the inner surface of blood vessels, they ensure that blood does not leak out, and if damage occurs, they respond by secreting proteins, signaling for help to other cells. VEGF, when combined with two receptors KDR and Flt-1 on endothelial cells with high affinity, can directly stimulate the proliferation of vascular endothelial cells, induce their migration and form lumen like structure, and finally promote the new blood vessels which can provide extra oxygen and other nutrients to tumor through the induction of interstitial production, see 13.
In the past two decades, a large number of mathematical models describing tumor invasion have been developed from different aspects, see 1, 2. In addition, the model is completely based on the reaction diffusion equation, and the core of these models assumes the convergence mechanism of the tactility, which means that the attractants are non-proliferation. The analysis results of this kind of approach system essentially include the evolution problems of some memory types, such as subsystems, which are still quite fragmentary up to now, mainly concentrated on these systems, see 3, 4.
In this paper, we assume that satisfies the following problem
![]() | (1.2) |
In 13, the original problem is a system of
and
But the equation of
in (1.2) has only its own growth and death, and has no connection with any other cell. Hence, in this paper,
is a known solution obtained from the initial condition of C. Therefore, the aim of this paper is to get clear how does the known solution of
affect
and
The literature 14 shows that this chemotaxis cross diffusion may also have a strong destabilizing effect: for example, the Keller-Segel system
![]() | (1.3) |
is widely considered as the prototype model of chemical attraction process, and its solution is known to be global and bounded. In (1.3) substances secreted by cells immediately induce chemotaxis, while in (1.1), such chemicals only produce indirect chemotaxis by stimulating signals. Based on a good initial boundary value of this paper aims to clarify how
affects other vascular endothelial growth factors
endothelial cells
and oxygen
and to what extent this indirect chemotactic can enhance the regularity and boundedness of the solution.
Problem (1.1) will be studied in the standard functional spaces denoted by
![]() |
and
![]() |
For is used to represent the linear space composed of all functions u in
satisfying
![]() |
For is used to represent the linear space composed of all functions u in
satisfying
![]() |
and the norm is defined as
![]() |
where
![]() |
![]() |
![]() |
is a sphere about
with X as the center and r as the radius,
is the parabolic distance.
Before stating our main theorem, we present some technical hypotheses that will be assumed through out this article:
(H1) is a bounded
domain;
and
(H2) satisfying
on
;
(H3)
(H4)
Theorem 1.1. Let be positive constants, assume that (H1)-(H3) hold, then for
there exists a unique solution
of the problem (1.1). Furthermore, the following results hold:
(1) Assume that and (H3) is replaced by (H4), then there exists a unique classical solution
of the problem (1.1).
(2) If , then
.
In Theorem 1.1, for the sake of simplicity, we use ,
and
to denote the functions spaces
![]() |
![]() |
and
![]() |
respectively.
This paper is organized as follows. In Section 2, we show some theorems, definitions and Schauder estimate theorem, which will be used in later sections. In Section 3, we prove the existence, uniqueness and the estimates of nonnegative solutions and use the global Schauder estimation in Theorem 2.4 to get the solution
In this section, we present some definitions, theorems and the global Schauder estimation in 15. These definitions, estimates and theorems will be used in the next sections.
For ease of reference, we give the following embedding results for Sobolev space of type The first one is a consequence of Theorem 5.4 in 16. The second one is a particular case of Theorem 3.3 in 17 by taking
and
Theorem 2.1. Suppose that satisfies the cone property and
The following continuous embeddings hold:
(1) for all
if
(2) If then
for all
(3) If then
for all
(4) If then
Theorem 2.2. Let be a domain of
with boundary
satisfying the cone property. Then the functional space
is continuously embedded in
for
satisfying any one of the following conditions:
(i) if
(ii) if
(iii) if
In particular, for such and any function
we have that
![]() |
where is a constant depending only on
and n.
In the cases (ii), (iii) or in (i) when the embeddings mentioned above are compact.
Then, we consider the following general and simple parabolic initial-boundary value problem
![]() | (2.1) |
Existence and uniqueness of solutions for problem (2.1) is a particular case of Theorem 9.1 in 17 for the case of Neumann boundary condition, (see also the remarks at the end of Section 9 in 17). In the following, we state this particular result, stressing the dependencies on certain norms of the coefficients, which will be used in our later arguments.
Theorem 2.3. Let be a bounded domain in
with a
boundary
be bounded continuous functions in
and
Assume that
(1) is a real positive matrix such that for some positive constant
we have
for all
and all
(2)
(3) with either r=max(p, n+2) if
or
for any
if p=n+2;
(4) with either s=max(p, n+2) if
or
for any
, if
(5) and the coefficients
satisfy the condition
for a.e. in
where
is the
-component of the unitary outer normal vector to
in
(6) with
and satisfying the compatibility condition
on
when
Then, there exists a unique solution of the problem (2.1). Moreover, there is a positive Constant
such that the solution satisfies the following estimate
![]() | (2.2) |
Such a constant depends only on
and on the norms
Moreover, we may assume that the dependencies of
on stated the norms are nondecreasing.
We use the definitions and theorems in 15 to promote the solution from space to
space, which will be used in Section 3.
Definition 2.1. For is used to express the linear space composed of all functions
satisfying
![]() |
on which norm is given
![]() |
For positive integers and
the linear space composed of functions satisfying
![]() |
in is used as
or
Theorem 2.4. Let is a solution of equation (2.1) in
and u=0 on
Let
and
satisfy uniform parabolic condition and
for
if
![]() |
if on
then
and satisfy the following estimate
![]() |
Especially, when the above formula can be written as
![]() |
where R is depending on n, and
In this Section, we use Theorem 2.3 to prove the existence and uniqueness of solutions for
and
and then use Theorem 2.4 to improve the solutions from
to
The nonnegativity of
and
are proved when
and
respectively. By the regularity of
we solve the complexity of the convection term in the proof of nonnegativity of E when
Theorem 3.1. Assume that (H1)-(H3) hold, then the following problem
![]() | (3.1) |
exists a unique solution and if
almost everywhere in
, then
almost everywhere in
Moreover, if (H3) is replaced by (H4), there exists solution
of problem (3.1).
Proof. Since the coefficients of (3.1) satisfy the hypotheses of Theorem 2.3, there exists a unique solution of (3.1) by Theorem 2.3. Moreover,
satisfies the following estimate:
![]() | (3.2) |
Multiplying the first equation in (3.1) by and integrating in
, we have
![]() |
Using the fact that , we get
![]() |
We conclude that for all
that is
almost everywhere in
by using Gronwall’s in-equality and the fact that
almost everywhere in
Therefore
almost everywhere in
Because is a solution of problem (3.1), and
, the right coefficients of the first equation in (3.1) are 1,
respectively. It follows that
. When
, from Theorem 2.4, we conclude that
Theorem 3.2. Assume that (H1)-(H3) hold, then the following problem
![]() | (3.3) |
exists a unique solution and if
almost everywhere in
, then
almost everywhere in
. Moreover, if (H3) is replaced by (H4), there exists solution
of problem (3.3).
Proof. Since the coefficients of (3.3) satisfy the hypotheses of Theorem 2.3, there exists a unique solution of (3.3) by Theorem 2.3. Moreover,
satisfies the following estimate:
![]() | (3.4) |
Multiplying the first equation in (3.3) by and integra-ting in
, we have
![]() |
Using the fact that , we get
![]() |
Let , we have
![]() |
and
![]() |
From the above inequalities, we get
![]() |
Let , we have
![]() |
Hence, by Gronwall’s inequality we get
![]() |
We conclude that for all
that is
almost everywhere in
By using Gronwall’s inequality and the fact that
almost everywhere in
Therefore
almost everywhere in
Because is a solution of problem (3.3), and
the right coefficients of the first equation in (3.3) are 1,
re-spectively. It follows that
When
from Theorem 2.4, we conclude that
Remark 3.1. If the cancer cell density is not smooth enough, then the regularity of
will be reduced, and the nonnegativity of
can not be proved using the argument in Theorem 3.2.
Theorem 3.3. Assume that (H1)-(H3) hold, then the following problem
![]() | (3.5) |
exists a unique solution and if
almost everywhere in
, then
almost everywhere in
Moreover, if (H3) is replaced by (H4), there exists solution
of problem (3.5).
Proof. Since the coefficients of (3.5) satisfy the hypotheses of Theorem 2.3, there exists a unique solution of (3.5) by Theorem 2.3. Moreover,
satisfies the following estimate:
![]() | (3.6) |
Multiplying the first equation in (3.5) by and integrating in
, we have
![]() |
Using the fact that we get
![]() |
We conclude that for all
that is
almost everywhere in
by using Gronwall’s inequality and the fact that
almost everywhere in
Therefore
almost everywhere in
Because is a solution of problem (3.5), and
the right coefficients of the first equation in (3.5) are 1,
respectively. It follows that
When
from Theorem 2.4, we conclude that
We will prove the existence of problem (1.1). The uniqueness of problem (1.1) will be proved by using Young’s inequality and Gronwall’s inequality. Then the main result, Theorem 1.1, readily follows.
Theorem 3.4. Assume that (H1)-(H4) hold, there is a unique nonnegative solution of the problem (1.1).
Proof. From Theorem 3.1, Theorem 3.2 and Theorem 3.3, we conclude that there exists and
and
are nonnegative. Let
and
be solutions to problem (1.1). Setting
then
and
satisfy the following problems, respectively:
![]() | (3.7) |
![]() | (3.8) |
and
![]() | (3.9) |
Multiplying the first equation in by
and integrating in
, we have
where depends on
. Multiplying the first equation in
by
and integrating in
, we have
![]() |
where depends on
. Multiplying the first equation in
by
and integrating in
, we have
![]() |
where depends on
. Thus, we obtain
![]() |
By Gronwall’s inequality, we get
![]() |
namely,
![]() |
for all We then have
almost everywhere in
and hence
almost everywhere in
Then the uniqueness assertion is proved.
[1] | A.R.A. Anderson, M.A.J. Chaplain, Continuous and discrete mathematical models of tumor-induced angiogenesis, Bull. Math. Biol., 60(1998), 857-899. | ||
In article | View Article PubMed | ||
[2] | N. Bellomo, A. Bellouquid, Y. Tao, M. Winkler, Toward a mathematical theory of Keller-Segel models of pattern formation in biological tissues, Math. Models Methods Appl., 25(2015), 1663-1763. | ||
In article | View Article | ||
[3] | M.A.J. Chaplain, G. Lolas, Mathematical modelling of cancer cell invasion of tissue: the role of the urokinase plasminogen activation system, Math. Models Methods Appl., 18(2005), 1685-1734. | ||
In article | View Article | ||
[4] | M.A.J. Chaplain, G. Lolas, Mathematical modelling of cancer invasion of tissue: dynamic heterogeneity, Net. Hetero. Med., 1(2006), 399-439. | ||
In article | View Article | ||
[5] | Y. Li. K. Lin, C. Mu, Boundedness and asymptotic behavior of solutions to a chemotaxis haptotaxis model in high dimensions, Appl. Math. Lett., 50(2015), 91-97. | ||
In article | View Article | ||
[6] | C. Stinner, C. Surulescu, G. Meral, A multiscale model for pH-tactic invasion with time-varying carrying capacities, IMA J. Appl. Math., 80(2015), 1300-1321. | ||
In article | View Article | ||
[7] | C. Stinner, C. Surulescu, A. Uatay, Global existence for a go-or-grow multiscale model for tumor invasion with therapy, Math. Models Methods Appl., 26(2016), 2163-2201. | ||
In article | View Article | ||
[8] | A.R.A. Anderson, M.A.J. Chaplain, A mathematical model for capillary network formation in the absence of endothelial cell proliferation, Appl. Math. Lett., 11(1998), 109-116. | ||
In article | View Article | ||
[9] | M.A.J. Chaplain, A.M. Stuart, A model mechanism for the chemotactic response of endothelial cells to tumor angiogenesis factor, IMA J. Math. Appl. Med. Biol., 10(1993), 149-168. | ||
In article | View Article PubMed | ||
[10] | H.A. Levine, B.D. Sleeman, M. Nilsen-Hamilton, Mathematical modeling of the onset of capillary formation initiating angiogenesis, J. Math. Biol., 42(2001), 195-238. | ||
In article | View Article PubMed | ||
[11] | N. Paweletz, M. Knierim, Tumor related angiogenesis, Crit. Rev. Oncal. Hematol., 9(1989), 197-242. | ||
In article | View Article | ||
[12] | B.D. Sleeman, Mathematical modelling of tumor growth and angiogenesis, Adv. in Exp. Med. Bio., 428(1997), 671-677. | ||
In article | View Article PubMed | ||
[13] | A. Friedman, Mathematical biology. Modeling and analysis. CBMS Regional Conference Series in Mathematics, 127. Published for the Conference Board of the Mathematical Sciences, Washington, DC; by the American Mathematical Society, Providence, RI, 2018. | ||
In article | View Article | ||
[14] | E. Keller, L. Segel, Model for chemotaxis, J. Theor. Biol., 30(1970), 225-234. | ||
In article | View Article | ||
[15] | Y.Z. Chen, Second order parabolic partial differential equation(In Chinese), Peking University Press, 2003. | ||
In article | |||
[16] | R. Adams, Sobolev spaces. New York: Academic press, 1975. | ||
In article | |||
[17] | O. Ladyzhenskaky, V. Solonnikov, N. Uraltseva, Linear and quasilinear equations of parabolic type, Amer. Math., 1968. | ||
In article | View Article | ||
[18] | A. C. Fassoni, Mathematical modeling in cancer addressing the early stage and treatment of avascular tumors, PhD thesis, University of Campinas, 2016. | ||
In article | |||
[19] | A. Friedman, Partial differential equations of parabolic type, Prentice-Hall. Inc., Englewood Cliffs, N.J., 1964. | ||
In article | |||
Published with license by Science and Education Publishing, Copyright © 2020 Gang Li, Hui Min Hu, Xi Chen and Fei Da Jiang
This work is licensed under a Creative Commons Attribution 4.0 International License. To view a copy of this license, visit
https://creativecommons.org/licenses/by/4.0/
[1] | A.R.A. Anderson, M.A.J. Chaplain, Continuous and discrete mathematical models of tumor-induced angiogenesis, Bull. Math. Biol., 60(1998), 857-899. | ||
In article | View Article PubMed | ||
[2] | N. Bellomo, A. Bellouquid, Y. Tao, M. Winkler, Toward a mathematical theory of Keller-Segel models of pattern formation in biological tissues, Math. Models Methods Appl., 25(2015), 1663-1763. | ||
In article | View Article | ||
[3] | M.A.J. Chaplain, G. Lolas, Mathematical modelling of cancer cell invasion of tissue: the role of the urokinase plasminogen activation system, Math. Models Methods Appl., 18(2005), 1685-1734. | ||
In article | View Article | ||
[4] | M.A.J. Chaplain, G. Lolas, Mathematical modelling of cancer invasion of tissue: dynamic heterogeneity, Net. Hetero. Med., 1(2006), 399-439. | ||
In article | View Article | ||
[5] | Y. Li. K. Lin, C. Mu, Boundedness and asymptotic behavior of solutions to a chemotaxis haptotaxis model in high dimensions, Appl. Math. Lett., 50(2015), 91-97. | ||
In article | View Article | ||
[6] | C. Stinner, C. Surulescu, G. Meral, A multiscale model for pH-tactic invasion with time-varying carrying capacities, IMA J. Appl. Math., 80(2015), 1300-1321. | ||
In article | View Article | ||
[7] | C. Stinner, C. Surulescu, A. Uatay, Global existence for a go-or-grow multiscale model for tumor invasion with therapy, Math. Models Methods Appl., 26(2016), 2163-2201. | ||
In article | View Article | ||
[8] | A.R.A. Anderson, M.A.J. Chaplain, A mathematical model for capillary network formation in the absence of endothelial cell proliferation, Appl. Math. Lett., 11(1998), 109-116. | ||
In article | View Article | ||
[9] | M.A.J. Chaplain, A.M. Stuart, A model mechanism for the chemotactic response of endothelial cells to tumor angiogenesis factor, IMA J. Math. Appl. Med. Biol., 10(1993), 149-168. | ||
In article | View Article PubMed | ||
[10] | H.A. Levine, B.D. Sleeman, M. Nilsen-Hamilton, Mathematical modeling of the onset of capillary formation initiating angiogenesis, J. Math. Biol., 42(2001), 195-238. | ||
In article | View Article PubMed | ||
[11] | N. Paweletz, M. Knierim, Tumor related angiogenesis, Crit. Rev. Oncal. Hematol., 9(1989), 197-242. | ||
In article | View Article | ||
[12] | B.D. Sleeman, Mathematical modelling of tumor growth and angiogenesis, Adv. in Exp. Med. Bio., 428(1997), 671-677. | ||
In article | View Article PubMed | ||
[13] | A. Friedman, Mathematical biology. Modeling and analysis. CBMS Regional Conference Series in Mathematics, 127. Published for the Conference Board of the Mathematical Sciences, Washington, DC; by the American Mathematical Society, Providence, RI, 2018. | ||
In article | View Article | ||
[14] | E. Keller, L. Segel, Model for chemotaxis, J. Theor. Biol., 30(1970), 225-234. | ||
In article | View Article | ||
[15] | Y.Z. Chen, Second order parabolic partial differential equation(In Chinese), Peking University Press, 2003. | ||
In article | |||
[16] | R. Adams, Sobolev spaces. New York: Academic press, 1975. | ||
In article | |||
[17] | O. Ladyzhenskaky, V. Solonnikov, N. Uraltseva, Linear and quasilinear equations of parabolic type, Amer. Math., 1968. | ||
In article | View Article | ||
[18] | A. C. Fassoni, Mathematical modeling in cancer addressing the early stage and treatment of avascular tumors, PhD thesis, University of Campinas, 2016. | ||
In article | |||
[19] | A. Friedman, Partial differential equations of parabolic type, Prentice-Hall. Inc., Englewood Cliffs, N.J., 1964. | ||
In article | |||