Literature DB >> 25667597

Steady-state analysis of necrotic core formation for solid avascular tumors with time delays in regulatory apoptosis.

Fangwei Zhang1, Shihe Xu2.   

Abstract

A mathematical model for the growth of solid avascular tumor with time delays in regulatory apoptosis is studied. The existence of stationary solutions and the mechanism of formation of necrotic cores in the growth of the tumors are studied. The results show that if the natural death rate of the tumor cell exceeds a fixed positive constant, then the dormant tumor is nonnecrotic; otherwise, the dormant tumor is necrotic.

Entities:  

Mesh:

Year:  2014        PMID: 25667597      PMCID: PMC4211211          DOI: 10.1155/2014/467158

Source DB:  PubMed          Journal:  Comput Math Methods Med        ISSN: 1748-670X            Impact factor:   2.238


1. Introduction

The growth of tumors is a highly complex process. To describe this process, mathematical models are needed. A variety of mathematical models for tumor growth have been developed and studied; for example, compare [1-7] and references therein. Most of those models are based on the reaction diffusion equations and mass conservation law. Analysis of such free boundary problems has drawn great interest, and many interesting results have been established; compare [8-14] and references therein. In this paper, we study the following problem: where r is the radial variable, t is the time variable, the variable σ(r, t) represents the scaled nutrient concentration at radius r and time t. The variable R(t) represents the scaled radius of the tumor at time t and ρ(t) represents the scaled radius of the necrotic core of the tumor at time t. The three terms on the right hand side of (5) are explained as follows. The first term is the total volume increase in a unit time interval induced by cell proliferation, which is balance between birth and natural death rates of the cells (in the region ρ(t) < r < R(t)), the birth rate is sσ, and the natural death rate is , where is a constant. The second term is the total volume decrease (or increase) in a unit time interval caused by regulatory apoptosis, where regulatory apoptosis rate is given by sθ(σ − σ ); that is, if the local proliferation rate at time t − τ exceeds (falls below) the critical value sσ , then there will be an increase (decrease) in local rate of apoptotic cell loss at time t, and this increase (decrease) is given by sθ(σ − σ ), where the magnitude of θ indicates the importance of regulatory apoptosis relative to underlying apoptosis: for large values of θ, the regulatory mechanism dominates apoptotic cell loss. s is a scaling constant. The last term is total volume shrinkage in a unit time interval caused by cell apoptosis or cell death due to aging (in the region 0 < r < ρ(t)); the rate of cell apoptosis is assumed to be constant and does not depend on either σ. The above model is similar to the second model of Byrne [1] but with one modification. The modification is as follows. In Byrne [1], the consumption rate of nutrient is assumed to be a constant Γ, instead of that (1) employed here. In this paper, as can be seen from (1), we assume that the consumption rate of nutrient is proportional to its concentration. This assumption is clearly more reasonable. The reason is as follows. From [1], we know that if the consumption rate of nutrient is assumed to be a constant Γ, then σ satisfies where φ(R) is the radius of the necrotic core. Therefore, σ may be negative for some φ(R). If one assumes that the consumption rate of nutrient is proportional to its concentration, then σ cannot be negative for any φ(R) (if it has); see (13) and (14) in Section 2.

2. Stationary Solutions and the Formation of Necrotic Cores

By rescaling the space variable we may assume that Γ = 1 in (1). For a given R, the concentration of nutrient σ = σ (r) in the tumor is given by where U(r, R) is the solution of the problem Denote κ = σ /σ nec. Since κ > 1, there exists a unique R* > 0 such that

Lemma 1 (see [9]).

For any R > R*, the equation has a unique root ρ = φ(R) in the interval (0, R); that is, And the solution to the problem (9) is as follows: if  0 < R < R*, then and if R > R*, then Denote (R , σ (r)) as a stationary solution of the problem (1)–(6); then, it satisfies the following equations: In the rest of this section, we assume that The same technique and method can be used to other conditions besides (H), but the results may be different.

Theorem 2 .

If , then, for any θ ∈ (0, θ 1), there exists a unique one positive solution to the equation f(R) = 0; that is, there exists a unique positive stationary solution to the problem (1)–(6), where .

Proof

By Lemma 1, we find that R satisfies the equation for 0 < R < R*, and for R > R*, where and ρ = φ(R). From [9] we know that the function g is strictly monotone decreasing for all R > R* and φ(R)/R is monotone increasing for all R > R*. Using the similar process used in Lemmas 4.1 and 4.2 of [9], one can get the following assertion: for any θ ∈ (0,1), the function f is continuously differentiable and f′(R) < 0 for all R > 0. Since, for 0 < R < R*, (17) holds, then where we have used the fact lim⁡(Rcoth⁡R − 1)/R 2 = 1/3. By direct computation, noticing , one can get From [9] we know lim⁡ φ(R)/R = 1 and lim⁡(R − φ(R)) = A, where A is a constant. Then for ,  θ ∈ (0, θ 1)(⊂(0,1)). By the fact that f′(R) < 0 for all R > 0, we have that there exists a unique positive costant R that satisfies the equation f(R ) = 0. This completes the proof of Theorem 2. Let p(x) = (xcosh⁡x − 1)/x 2, x > 0. From [13], we know that p′(x) < 0 for all x > 0, and Since, for and , then there exists a unique positive solution x = R such that

Theorem 3 .

Assume that condition (H) and are satisfied. Then the following assertions hold: if R ≤ R*, then the dormant tumor ensured by Theorem 2 does not have a necrotic core; if R > R*, then the dormant tumor ensured by Theorem 2 has a necrotic core and the radius of the necrotic core is equal to φ(R ). By (17) and (25) one can get that if R ≤ R*, then f(R ) = 0. It follows that (R , σ (r)) = (R , U(r, R )) is the stationary solution of the problem (1)–(6). Since R < R* implies that U(r, R ) > U(0, R ) ≥ σ nec for 0 < r ≤ R , we can get that the dormant tumor does not have a necrotic core. If R > R*, then from (17) and (25) and the fact that p′(R) < 0 we can get f(R) > 0 for 0 < R < R*. Then the solution R to the equation f(R) = 0 satisfies R > R*. Consequently, in this case, the stationary solution (R , σ (r)) = (R , U(r, R )) satisfies σ (r) = σ nec for r ≤ φ(R ). Thus, the dormant tumor has a necrotic core with radius r = φ(R ). This completes the proof of Theorem 3. Denote By the fact that q(R*) = κ = σ /σ nec and q(R) is strictly monotone increasing for R > 0, we have R* = q −1(κ). Since by the fact p′(x) < 0, one can get that the condition R ≤ R* is equivalent to the following condition: and the condition R > R* is equivalent to the condition . From the above analysis, in view of biology sense, the meaning of Theorem 3 is as follows. If the natural death rate is large enough such that , then the dormant tumor is nonnecrotic, and if , then dormant tumor is necrotic. From [9], we know the function ηp(q −1(η)) is strictly monotone increasing for η > 1 and ηp(q −1(η)) > 1/3 for η > 1. Then we can get the following. Increasing the nutrient supply σ from surface will increase the threshold value of . This implies that the dormant tumor furnished with a small number of nutrients can possibly be nonnecrotic, whereas the dormant tumor furnished with a large number of nutrients can possibly be necrotic.
  8 in total

1.  Mathematical modelling of avascular-tumour growth. II: Modelling growth saturation.

Authors:  J P Ward; J R King
Journal:  IMA J Math Appl Med Biol       Date:  1999-06

2.  Analysis of a mathematical model for the growth of tumors.

Authors:  A Friedman; F Reitich
Journal:  J Math Biol       Date:  1999-03       Impact factor: 2.259

3.  Time delay in necrotic core formation.

Authors:  Marek Bodnar; Urszula Forys
Journal:  Math Biosci Eng       Date:  2005-07       Impact factor: 2.080

4.  On the growth and stability of cell cultures and solid tumors.

Authors:  H P Greenspan
Journal:  J Theor Biol       Date:  1976-01       Impact factor: 2.691

5.  The effect of time delays on the dynamics of avascular tumor growth.

Authors:  H M Byrne
Journal:  Math Biosci       Date:  1997-09       Impact factor: 2.144

6.  The ecology and evolutionary biology of cancer: a review of mathematical models of necrosis and tumor cell diversity.

Authors:  John D Nagy
Journal:  Math Biosci Eng       Date:  2005-04       Impact factor: 2.080

7.  Growth of necrotic tumors in the presence and absence of inhibitors.

Authors:  H M Byrne; M A Chaplin
Journal:  Math Biosci       Date:  1996-07-15       Impact factor: 2.144

8.  Growth of nonnecrotic tumors in the presence and absence of inhibitors.

Authors:  H M Byrne; M A Chaplain
Journal:  Math Biosci       Date:  1995-12       Impact factor: 2.144

  8 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.