Journal of Applied Mathematics

Journal of Applied Mathematics / 2012 / Article

Research Article | Open Access

Volume 2012 |Article ID 648067 | 17 pages | https://doi.org/10.1155/2012/648067

Blowup Analysis for a Nonlocal Diffusion Equation with Reaction and Absorption

Academic Editor: Junjie Wei
Received21 Jan 2012
Accepted20 Apr 2012
Published10 Jul 2012

Abstract

We investigate a nonlocal reaction diffusion equation with absorption under Neumann boundary. We obtain optimal conditions on the exponents of the reaction and absorption terms for the existence of solutions blowing up in finite time, or for the global existence and boundedness of all solutions. For the blowup solutions, we also study the blowup rate estimates and the localization of blowup set. Moreover, we show some numerical experiments which illustrate our results.

1. Introduction

In this paper, we devote our attention to the singularity analysis of the following nonlocal diffusion equation: 𝑢𝑡(𝑥,𝑡)=Ω𝐽(𝑥−𝑦)(𝑢(𝑦,𝑡)−𝑢(𝑥,𝑡))𝑑𝑦+𝑢𝑝(𝑥,𝑡)âˆ’ğ‘˜ğ‘¢ğ‘ž(𝑢𝑥,𝑡),𝑥∈Ω,𝑡>0,(𝑥,0)=𝑢0(𝑥),𝑥∈Ω.(1.1) Here Ω is a bounded connected and smooth domain, which contains the origin, and 𝐽∶ℝ𝑁→ℝ is a nonnegative, bounded, symmetric radially and strictly decreasing function with ∫ℝ𝑁𝐽(𝑧)𝑑𝑧=1, and 𝑝, ğ‘ž, 𝑘 are all positive constants. We take the initial datum, 𝑢0(𝑥), nonnegative and nontrivial.

Equation in (1.1) is called a nonlocal diffusion equation in the sense that the diffusion of the density 𝑢 at a point 𝑥 and time 𝑡 does not only depend on 𝑢(𝑥,𝑡), but on all the values of 𝑢 in a neighborhood of 𝑥 through the convolution term. Maybe the simplest linear version of nonlocal model (1.1) is 𝑢𝑡(𝑥,𝑡)=𝑅𝑁𝐽(𝑥−𝑦)(𝑢(𝑦,𝑡)−𝑢(𝑥,𝑡))𝑑𝑦=𝐽∗𝑢(𝑥,𝑡)−𝑢(𝑥,𝑡).(1.2) In recent years, the linear equation (1.2) and its variations have been widely used to model diffusion process, for example, in biology, dislocations dynamics, phase transition model, material science, and network model and so forth (see [1–7] and the references therein). The idea hidden inside those model is simple to understand. As stated in [6], if 𝑢(𝑥,𝑡) is thought of as a density at the point 𝑥 and time 𝑡 and 𝐽(𝑥−𝑦) is thought of as the probability distribution of jumping from location 𝑦 to location 𝑥, then the convolution ∫(𝐽∗𝑢)(𝑥,𝑡)∶=ℝ𝑁𝐽(𝑥−𝑦)𝑢(𝑦,𝑡)𝑑𝑦 is the rate at which individuals are arriving at 𝑥 from all other places and ∫−𝑢(𝑥,𝑡)=−ℝ𝑁𝐽(𝑥−𝑦)𝑢(𝑥,𝑡)𝑑𝑦 is the rate at which they are leaving location 𝑥 to travel to all other sites.

In the past decades, some works have shown that (1.2) shares many properties with the classical heat equation 𝑢𝑡−Δ𝑢=0(1.3) such as the existence of constant bounded stationary solutions and the maximum principle, but there is no regularizing effect in general for the former [8]. Therefore, as mentioned in [9–11], it is an interesting topic to compare the properties of solutions to the nonlocal diffusion equation with that of the corresponding local diffusion cases.

To motivate our works, we would like to remark that, in recent years, (1.3) and its variations have been extensively studied. In particular, a considerable effort has been devoted to studying the blowup properties of the following classical diffusion equation with reaction (𝛼>0) and/or absorption (𝑘>0) under Dirichlet or Neumann boundary 𝑢𝑡−Δ𝑢=ğ›¼ğ‘¢ğ‘âˆ’ğ‘˜ğ‘¢ğ‘ž,𝑥∈Ω,𝑡>0,(1.4) which provides a simple biological or physical model. For instance, by constructing the self-similar weak subsolutions, Bedjaoui and Souplet [12] obtained the following conclusion for (1.4) with 𝛼=1 under Dirichlet or Neumann boundary: if 𝑝<max{ğ‘ž,1}, then all solutions are global. If 𝑝>max{ğ‘ž,1}, there exist solutions of (1.4) which blow up in finite time. In the critical case 𝑝=max{ğ‘ž,1}, the results may depend on the size of the coefficient 𝑘. In the Dirichlet boundary case, Xiang et al. [13] also studied the blowup rate estimates and obtained the following results: if 𝑝>max{ğ‘ž,1} and the solution 𝑢(𝑥,𝑡) of (1.4) blows up at 𝑇, then there exists constants 𝐶>𝑐>0 such that max[]Ω×0,𝑡𝑢(𝑥,𝜏)≥𝑐(𝑇−𝑡)1/(𝑝−1),max[]Ω×0,𝑡𝑢(𝑥,𝜏)≤𝐶(𝑇−𝑡)1/(𝑝−1)2if1<𝑝<1+.𝑁+1(1.5)

In this paper, we will deal with the blowup properties of the nonlocal diffusion problem (1.1) and compare them with that of problem (1.4). In our model (1.1), the absorption term âˆ’ğ‘˜ğ‘¢ğ‘ž(𝑥,𝑡) represents a rate of consumption due to an internal reaction, and we are integrating in Ω and thus imposing the condition that the diffusion takes place only in Ω, which means that the individual may enter or leave the domain. This is so called Neumann boundary conditions, see [14, 15]. We remark that García-Melián and Quirós [16] recently proved the existence of a critical exponent of Fujita type for the nonlocal diffusion problem 𝑢𝑡(𝑥,𝑡)=𝑅𝑁𝐽(𝑥−𝑦)(𝑢(𝑦,𝑡)−𝑢(𝑥,𝑡))𝑑𝑦+𝑢𝑝(𝑥,𝑡)=𝐽∗𝑢(𝑥,𝑡)−𝑢(𝑥,𝑡)+𝑢𝑝(𝑥,𝑡).(1.6) As mentioned in [17], nonlocal diffusion systems are more accurate than the classical diffusion systems in modeling the spatial diffusion of the individuals in some biology areas, such as embryological development process. For more study about the nonlocal diffusion operator, we refer to [8, 18–22] and references therein.

It is noteworthy that the method used in [12, 13] for problem (1.4) is invalid in our current setting due to the appearance of the nonlocal diffusion term. For example, instead of constructing self-similar weak subsolutions, we will use technique of integration to prove the finite time blowup. As far as the blowup rate is concerned, the scaling argument in [13] is not applicable.

We now state our main results. Our first result determines the complete classification of the parameters for which the solution blows up in finite time or exists globally.

Theorem 1.1. (i) If 𝑝≤max{ğ‘ž,1}, then all solutions of (1.1) are global. Moreover, if 𝑝<ğ‘ž or 𝑝=ğ‘ž and 𝑘≥1, all solutions are uniformly bounded, while if 𝑝=ğ‘ž and 𝑘<1, there exist unbounded global solutions.
(ii) If 𝑝>max{ğ‘ž,1}, then (1.1) with large initial data have solutions blowing up in finite time, while the solutions of (1.1) with small initial data exist globally.

Once we have obtained the values of the parameters for which blowup occurs, the next step is to concern the blowup rate, that is the speed at which solutions are blowing up. Different from the result of problem (1.4), we could have a unified upper and low estimate here.

Theorem 1.2. Let 𝑝>max{ğ‘ž,1} and 𝑢(𝑥,𝑡) be a solution of (1.1) blowing up at time 𝑇. Then lim𝑡→𝑇(𝑇−𝑡)1/(𝑝−1)max𝑥∈Ω𝑢(𝑥,𝑡)=(𝑝−1)−1/(𝑝−1).(1.7)

Remark 1.3. From this result we find that the nonlocal diffusion term plays no role when determining the blowup rate and the blowup rate is just same as that of the ODE 𝑢𝑡=𝑢𝑝. And this phenomena is the same as that of local diffusion case.

Next we consider the spacial location of the blowup set. As usual, the blowup set of solution 𝑢(𝑥,𝑡) is defined as follows: 𝐵(𝑢)=𝑥∈𝑥Ω;thereexist𝑛,𝑡𝑛𝑥⟶(𝑥,𝑇)suchthat𝑢𝑛,ğ‘¡ğ‘›î€¸î‚‡âŸ¶âˆž,(1.8) where 𝑇 is the maximal existence time of 𝑢. For a general domain Ω we can localize the blowup set near any pint in Ω just by taking an initial condition being very large near that point and not so large in the rest of the domain. This is the following result.

Theorem 1.4. Let 𝑝>max{ğ‘ž,2}. For any 𝑥0∈Ω and 𝜀>0, there exists an initial data 𝑢0 such that the corresponding solution 𝑢(𝑥,𝑡) of (1.1) blows up at finite time 𝑇 and its blowup set 𝐵(𝑢) is contained in 𝐵𝜖(𝑥0)={𝑥∈Ω;‖𝑥−𝑥0‖<𝜖}.

Next we consider the radially symmetric case. In this case, single point blowup occurs.

Theorem 1.5. Let 𝑝>max{ğ‘ž,2} and Ω=𝐵𝑅={|𝑥|<𝑅}. If the initial data 𝑢0∈𝐶1(𝐵𝑅) is a radial nonnegative function with a unique maximum at the origin, that is, 𝑢0=𝑢0(𝑟)≥0, ğ‘¢î…ž0(𝑟)<0 for 0<𝑟≤𝑅, 𝑢′(0)=0 and 𝑢0(0)<0, then the blowup set 𝐵(𝑢) of the solution 𝑢 of (1.1) consists only of the original point 𝑥=0.

The remainder of this paper is organized as follows. In Section 2, we give the existence and uniqueness of the solutions as well as the comparison principle. In Section 3, we prove the blowup and global existence condition. And then we prove the blowup rate and blowup set results in Sections 4 and 5, respectively. And in the last section we will give some numerical experiments to demonstrate our results.

2. Existence, Uniqueness, and Comparison Principle

We begin our study of problem (1.1) with a result of existence and uniqueness of continuous solutions and comparison principle.

Firstly, existence and uniqueness of solutions is a consequence of Banach's fixed point theorem. We look for 𝑢∈𝐶1((0,𝑇);𝐶(Ω))∩𝐶([0,𝑇);𝐶(Ω)) satisfying (1.1). Fix 𝑡0>0, and consider the Banach space 𝑋𝑡0=𝑢∈𝐶1((0,𝑇);𝐶(Ω))∩𝐶([0,𝑇);𝐶(Ω)) with the norm ‖𝜔‖𝑋𝑡0=max0≤𝑡≤𝑡0‖‖𝜔(⋅,𝑡)𝐶(Ω)+max0<𝑡≤𝑡0‖‖𝜔𝑡‖‖(⋅,𝑡)𝐶(Ω).(2.1)

We define the following operator 𝑇∶𝑋𝑡0→𝑋𝑡0𝑇𝜔0(𝜔)(𝑥,𝑡)=𝜔0(𝑥)+𝑡0Ω+𝐽(𝑥−𝑦)(𝜔(𝑦,𝑠)−𝜔(𝑥,𝑠))𝑑𝑦𝑑𝑠𝑡0|𝜔|𝑝−1𝜔(𝑥,𝑠)−𝑘|𝜔|ğ‘žâˆ’1𝜔(𝑥,𝑠)𝑑𝑠.(2.2)

Similar to [10, 15] we could prove the solution to (1.1) is a fixed point of operator 𝑇 in a convenient ball of 𝑋𝑡0. Thus, we could obtain the following result.

Theorem 2.1. For every 𝑢0∈𝐶(Ω) there exists a unique solution 𝑢 of (1.1) such that 𝑢∈𝐶1((0,𝑇);𝐶(Ω))∩𝐶([0,𝑇);𝐶(Ω)) and 𝑇 (finite or infinite) is the maximal existence time of solution.

Next, we will study the comparison principle. As usual we first give the definition of supersolution and subsolution.

Definition 2.2. A function 𝑢∈𝐶1((0,𝑇);𝐶(Ω))∩𝐶([0,𝑇);𝐶(Ω)) is a supersolution of (1.1) if it satisfies 𝑢𝑡(𝑥,𝑡)≥Ω𝐽(𝑥−𝑦)𝑢(𝑦,𝑡)−𝑢(𝑥,𝑡)𝑑𝑦+𝑢𝑝(𝑥,𝑡)âˆ’ğ‘˜ğ‘¢ğ‘ž(𝑥,𝑡),𝑢(𝑥,0)≥𝑢0(𝑥).(2.3) Subsolutions are defined similarly by reversing the inequalities.

To obtain the comparison principle for problem (1.1), we first give a maximum principle.

Lemma 2.3. Suppose that 𝑤(𝑥,𝑡)∈𝐶1((0,𝑇);𝐶(Ω))∩𝐶([0,𝑇);𝐶(Ω)) is nontrivial and satisfies𝑤𝑡(𝑥,𝑡)≥Ω𝐽(𝑥−𝑦)(𝑤(𝑦,𝑡)−𝑤(𝑥,𝑡))𝑑𝑦+𝑐1𝑤(𝑥,𝑡),𝑥∈Ω,𝑡>0(2.4) with 𝑤(𝑥,0)≥0 for 𝑥∈Ω, where 𝑐1 is a bounded function, then 𝑤(𝑥,𝑡)>0 for 𝑥∈Ω and 𝑡>0.

Proof. We first show 𝑤(𝑥,𝑡)≥0 for 𝑥∈Ω,𝑡>0. Assume that 𝑤(𝑥,𝑡) is negative somewhere. Let 𝜃(𝑥,𝑡)=𝑒−𝜆𝑡𝑤(𝑥,𝑡)(𝜆>0,𝜆≥2sup|𝑐1|). If we take (𝑥0,𝑡0) a point where 𝜃 attains its negative minimum, there holds 𝑡0>0 and 𝜃𝑡𝑥0,𝑡0=−𝜆𝑒−𝜆𝑡0𝑤𝑥0,𝑡0+𝑒−𝜆𝑡0𝑤𝑡𝑥0,𝑡0≥𝑒−𝜆𝑡0Ω𝐽𝑥0𝑤−𝑦𝑦,𝑡0𝑥−𝑤0,𝑡0𝑑𝑦+−𝜆+𝑐1𝑤𝑥0,𝑡0>0,(2.5) which is a contradiction. Thus 𝜃(𝑥,𝑡)≥0 for 𝑥∈Ω,𝑡>0. And so does 𝑤(𝑥,𝑡).
Now, we suppose 𝜃(𝑥1,𝑡1)=0 for some (𝑥1,𝑡1); that is, 𝜃 attains its minimum at (𝑥1,𝑡1) from the first step. Notice that the hypotheses on 𝐽 imply 𝐽(0)>0, so that 𝜃(𝑥1,𝑡1)=0 implies that 𝜃(𝑥,𝑡1)=0 for 𝑥 in a neighborhood of 𝑥1. Thus a standard connectedness argument yields 𝜃≡0. This is a contradiction. So we obtain our conclusion.

Lemma 2.4. If 𝑝≥1, ğ‘žâ‰¥1 and 𝑢,  𝑢_are super and subsolutions to (1.1), respectively then 𝑢(𝑥,𝑡)≥𝑢_(𝑥,𝑡) for every (𝑥,𝑡)∈Ω×[0,𝑇).

Proof. Letting  𝑤(𝑥,𝑡)=𝑢−𝑢_, it is easy to verify that 𝑤(𝑥,𝑡) satisfies (2.4) when 𝑝≥1,ğ‘žâ‰¥1. We could obtain our conclusion from Lemma 2.3.

Remark 2.5. When 𝑝<1 or ğ‘ž<1, the conclusion is also validity if 𝑢 and  𝑢_  are bounded away from 0.

3. Blowup and Global Existence

In this section, we will analyze the blowup condition and give the proof of Theorem 1.1.

Proof of Theorem 1.1. (i) We only need to look for a global supersolution of (1.1). Indeed, it is easy to construct spacial homogeneous global supersolution of (1.1). To see this, we set 𝑢=𝐶𝑒𝛼𝑡, where 𝐶 and 𝛼 are positive constants to be determined.
For any given initial data 𝑢0, we note that 𝑢(𝑡0)≥‖𝑢0‖∞ for 𝑡0 sufficiently large and 𝑢 is bounded away from 0. Thus by the comparison principle and Remark 2.5, to make 𝑢 a supersolution of (1.1), we only need to show the existence of 𝐶 and 𝛼 satisfyingğ¶ğ‘ğ‘’ğ‘ğ›¼ğ‘¡â‰¤ğ‘˜ğ¶ğ‘žğ‘’ğ‘žğ›¼ğ‘¡+𝛼𝐶𝑒𝛼𝑡.(3.1) If 𝑝≤1<ğ‘ž, for any given 𝛼, we can take 𝐶=𝑘1/(ğ‘âˆ’ğ‘ž) such that (3.1) holds.  If ğ‘žâ‰¤1 and thus 𝑝≤1, we can choose 𝐶 and 𝛼 satisfying 𝐶𝑝−1=𝛼, which make (3.1) validity.
Next, we show all global solutions are uniformly bounded when 𝑝<ğ‘ž or 𝑝=ğ‘ž and 𝑘≥1. In fact, (1.1) has constant supersolution 𝑢=𝐴 whenever 𝑝<ğ‘ž or 𝑝=ğ‘ž and 𝑘≥1. To see this, we choose 𝐴 large enough such that ğ‘˜ğ´ğ‘žâ‰¥ğ´ğ‘â€–â€–ğ‘¢,𝐴≥0‖‖∞,(3.2) which imply that 𝑢 is a supersolution of (1.1).
At last we show there exist global unbounded solutions when 𝑝=ğ‘ž and 𝑘<1. Indeed, let (𝑓(𝑡)=1−𝑘)(1−𝑝)𝑡+𝑓1−𝑝(0)1/(1−𝑝)𝑒,𝑝=ğ‘ž<1,((1−𝑘)/2)𝑡,𝑝=ğ‘ž=1.(3.3) It is easy to see that if 𝑓(0)≤maxΩ𝑢0(𝑥), 𝑓(𝑡) is a subsolution of (1.1). It is obvious that when 𝑝<1, 𝑓(𝑡) is unbounded.
(ii) We first show that if the initial data 𝑢0(𝑥) is large enough, solutions of (1.1) blow up in finite time.
In the case of 𝑝>ğ‘ž>1. Integrating (1.1)1 in Ω and applying Fubini's theorem, we get 𝑑𝑑𝑡Ω𝑢(𝑥,𝑡)𝑑𝑥=Ω𝑢𝑝(𝑥,𝑡)ğ‘‘ğ‘¥âˆ’ğ‘˜Î©ğ‘¢ğ‘ž(𝑥,𝑡)𝑑𝑥.(3.4) Using Hölder's inequality, we could get 𝑑𝑑𝑡Ω𝑢(𝑥,𝑡)𝑑𝑥≥Ω𝑢𝑝||Ω||(𝑥,𝑡)𝑑𝑥−𝑘(ğ‘âˆ’ğ‘ž)/𝑝Ω𝑢𝑝(𝑥,𝑡)ğ‘‘ğ‘¥ğ‘ž/𝑝=Ω𝑢𝑝(𝑥,𝑡)ğ‘‘ğ‘¥ğ‘ž/𝑝Ω𝑢𝑝(𝑥,𝑡)𝑑𝑥(ğ‘âˆ’ğ‘ž)/𝑝||Ω||−𝑘(ğ‘âˆ’ğ‘ž)/𝑝,(3.5) where |Ω| is assumed to be the measure of Ω. Given positive constant 𝑚>𝑘1/(ğ‘âˆ’ğ‘ž) and 𝑢0≥𝑚, we have by the comparison principle that the solution 𝑢(𝑥,𝑡) of problem (1.1) satisfies 𝑢(𝑥,𝑡)≥𝑚. Thus 𝑑𝑑𝑡Ω𝑢(𝑥,𝑡)𝑑𝑥≥Ω𝑢𝑝(𝑥,𝑡)ğ‘‘ğ‘¥ğ‘ž/ğ‘î‚€ğ‘šğ‘âˆ’ğ‘ž||Ω||(ğ‘âˆ’ğ‘ž)/𝑝||Ω||−𝑘(ğ‘âˆ’ğ‘ž)/𝑝.(3.6) Then we use Jensen's inequality to obtain 𝑑𝑑𝑡Ω𝑢(𝑥,𝑡)𝑑𝑥>𝐶Ω𝑢(𝑥,𝑡)ğ‘‘ğ‘¥ğ‘ž,(3.7) where 𝐶 is a positive constant independent of the solution 𝑢. From this inequality, we could easily obtain that 𝑢(𝑥,𝑡) blow up in finite time.
In the case of 𝑝>1â‰¥ğ‘ž, it follows from ğ‘¢ğ‘žâ‰¤ğ‘¢+1 and Jensen's inequality that Ω𝑢𝑝(𝑥,𝑡)ğ‘‘ğ‘¥âˆ’ğ‘˜Î©ğ‘¢ğ‘ž(𝑥,𝑡)𝑑𝑥≥Ω𝑢𝑝(𝑥,𝑡)𝑑𝑥−𝑘Ω||Ω||≥||Ω||𝑢(𝑥,𝑡)𝑑𝑥−𝑘1−𝑝Ω𝑢(𝑥,𝑡)𝑑𝑥𝑝−𝑘Ω𝑢||Ω||.(𝑥,𝑡)𝑑𝑥−𝑘(3.8) Substituting this inequality into (3.4), we obtain 𝑑𝑑𝑡Ω||Ω||𝑢(𝑥,𝑡)𝑑𝑥≥1−𝑝Ω𝑢(𝑥,𝑡)𝑑𝑥𝑝−𝑘Ω||Ω||.𝑢(𝑥,𝑡)𝑑𝑥−𝑘(3.9)
Therefore, if we take the initial data 𝑢0 large enough such that |Ω|1−𝑝(∫Ω𝑢0(𝑥)𝑑𝑥)𝑝∫−𝑘Ω𝑢0(𝑥)𝑑𝑥−𝑘|Ω|>0, then ∫Ω𝑢(𝑥,𝑡)𝑑𝑥 blows up in finite time. So does 𝑢(𝑥,𝑡).
Next we show when the initial data 𝑢0(𝑥) is small, solutions of (1.1) exist globally. Consider constant 𝐵. Let 0<𝐵≤𝑘1/(ğ‘âˆ’ğ‘ž). Then ğµğ‘¡â‰¥ğµğ‘âˆ’ğ‘˜ğµğ‘ž. Henceforth, if 𝑢0(𝑥)≤𝐵, 𝐵 is a supersolution of (1.1). From the comparison principle, we know solutions of (1.1) are global in this case.

4. Blowup Rate Estimate

In this section, we study the blowup rate and prove Theorem 1.2.

Proof of Theorem 1.2. Let 𝑈(𝑡)=𝑢(𝑥(𝑡),𝑡)=max𝑥∈Ω𝑢(𝑥,𝑡). It is easy to see that 𝑈(𝑡) is Lipschitz continuous and thus it is differential almost everywhere [23]. From the first equality of (1.1) we have 𝑈′(𝑡)≤Ω𝐽(𝑥−𝑦)(𝑢(𝑦,𝑡)−𝑢(𝑥(𝑡),𝑡))𝑑𝑦+𝑢𝑝(𝑥(𝑡),𝑡)âˆ’ğ‘˜ğ‘¢ğ‘ž(𝑥(𝑡),𝑡)≤𝑢𝑝(𝑥(𝑡),𝑡)(4.1) at any point of differentiability of 𝑈(𝑡). Here we used ∇𝑢(𝑥(𝑡),𝑡)=0. Noticing that 𝑝>1 and integrating (4.1) from 𝑡 to 𝑇, we obtain max𝑥∈Ω𝑢(𝑥,𝑡)≥(𝑝−1)−1/(𝑝−1)(𝑇−𝑡)−1/(𝑝−1).(4.2)
Next we will establish the upper estimate. For any (𝑥,𝑡)∈Ω×[0,𝑇), we have 𝑢𝑡(𝑥,𝑡)≥−𝑢(𝑥,𝑡)+𝑢𝑝(𝑥,𝑡)âˆ’ğ‘˜ğ‘¢ğ‘ž(𝑥,𝑡)=𝑢𝑝(𝑥,𝑡)1−𝑢−(𝑝−1)(𝑥,𝑡)−𝑘𝑢−(ğ‘âˆ’ğ‘ž).(𝑥,𝑡)(4.3) In particular, ğ‘ˆî…ž(𝑡)≥𝑈𝑝(𝑡)1−𝑈(𝑡)−(𝑝−1)−𝑘𝑈(𝑡)−(ğ‘âˆ’ğ‘ž).(4.4)
From the lower estimate (4.2) we get ğ‘ˆî…ž(𝑡)≥𝑈𝑝(𝑡)1−(𝑝−1)(𝑇−𝑡)−𝑘(𝑝−1)(ğ‘âˆ’ğ‘ž)/(𝑝−1)(𝑇−𝑡)(ğ‘âˆ’ğ‘ž)/(𝑝−1).(4.5)
Integrating in (𝑡,𝑇), we get max𝑥∈Ω≤𝑢(𝑥,𝑡)(𝑝−1)(𝑇−𝑡)−(𝑝−1)22(𝑇−𝑡)2−𝑘(𝑝−1)(3ğ‘âˆ’ğ‘žâˆ’2)/(𝑝−1)2ğ‘âˆ’ğ‘žâˆ’1(𝑇−𝑡)(2ğ‘âˆ’ğ‘žâˆ’1)/(𝑝−1)−1/(𝑝−1),(4.6) combining with (4.2), the conclusion of Theorem 1.2 is proved if one takes the limit as 𝑡→𝑇.

5. Blowup Set

Next we will concern the blowup set for the solution to problem (1.1). We will first localize the blowup set near any point in Ω just by taking an initial condition being very large near that point and not so large in the rest of the domain.

Proof of Theorem 1.4. Given 𝑥0∈Ω and 𝜀>0, we could construct an initial condition 𝑢0 such that 𝐵(𝑢)⊂𝐵𝜀𝑥0=𝑥∈‖‖Ω∶𝑥−𝑥0‖‖<𝜀.(5.1)
In fact, we will consider 𝑢0 concentrated near 𝑥0 and small away from 𝑥0.
Let 𝜑 be a nonnegative smooth function such that supp(𝜑)⊂𝐵𝜀/2(𝑥0) and 𝜑(𝑥)>0 for 𝑥∈𝐵𝜀/2(𝑥0).
Next, let 𝑢0(𝑥)=𝑀𝜑(𝑥)+𝛿.(5.2) We want to choose 𝑀 large and 𝛿 small such that (5.1) holds.
First we can assume that 𝑇 is as small as we need by taking 𝑀 large enough. Indeed, we have 𝑇≤𝐶(Ω,𝑝,𝜑)ğ‘€ğ‘žâˆ’1or𝑇≤𝐶(Ω,𝑝,𝜑)𝑀𝑝−1(5.3) from the proof of Theorem 1.1.
Now, from the proof of blowup rate, we havemax𝑥∈Ω≤𝑢(𝑥,𝑡)(𝑝−1)(𝑇−𝑡)−(𝑝−1)22(𝑇−𝑡)2−𝑘(𝑝−1)(3ğ‘âˆ’ğ‘žâˆ’2)/(𝑝−1)2ğ‘âˆ’ğ‘žâˆ’1(𝑇−𝑡)(2ğ‘âˆ’ğ‘žâˆ’1)/(𝑝−1)−1/(𝑝−1)≤𝐶(𝑇−𝑡)−1/(𝑝−1).(5.4) Henceforth, for any 𝑥∈Ω, 𝑢𝑡=𝑥,𝑡Ω𝐽(𝑥,𝑦)𝑢(𝑦,𝑡)−𝑢𝑥,𝑡𝑑𝑦+𝑢𝑝𝑥,ğ‘¡âˆ’ğ‘˜ğ‘¢ğ‘žî€·î€¸â‰¤î€œğ‘¥,𝑡Ω𝐽𝑥,𝑦𝑢(𝑦,𝑡)𝑑𝑦+𝑢𝑝𝑥,𝑡≤𝐶(𝑇−𝑡)−1/(𝑝−1)+𝑢𝑝.𝑥,𝑡(5.5) Therefore, if 𝑥∈Ω⧵𝐵𝜖(𝑥0), then 𝑢(𝑥,𝑡) is a subsolution to 𝑤𝑡=𝐶(𝑇−𝑡)−1/(𝑝−1)+𝑤𝑝𝑤(𝑡),(0)=𝛿,(5.6) which shows 𝑢𝑥,𝑡≤𝑤(𝑡).(5.7)
Next, we only need to prove that a solution 𝑤 to (5.6) remains bounded up to 𝑡=𝑇, provided that 𝛿 and 𝑇 are small enough.
Let 𝑧(𝑠)=(𝑇−𝑡)1/(𝑝−1)𝑤(𝑡),𝑠=−ln(𝑇−𝑡).(5.8) Then 𝑧(𝑠) satisfies ğ‘§î…ž(𝑠)=𝐶𝑒−𝑠−1𝑝−1𝑧(𝑠)+𝑧𝑝(𝑠),𝑧(−ln𝑇)=𝛿𝑇1/(𝑝−1),(5.9) which show that for 𝑇 and 𝛿 small (𝑇 is small if 𝑀 is large), we have 1𝐶𝑇−𝑝−1𝛿𝑇1/(𝑝−1)+𝛿𝑝𝑇𝑝/(𝑝−1)<0.(5.10) So 𝑧′(𝑠)<0 for all 𝑠>−ln𝑇. From this and Lemma 4.2 of [24], we know 𝑧(𝑠)⟶0,ğ‘ âŸ¶âˆž.(5.11) Combining the equation verified by 𝑧 we obtain that, for given positive constant 𝛾(<1/𝑝(𝑝−1)), there exists 𝑠0>0 such that ğ‘§î…ž(𝑠)≤𝐶𝑒−𝑠−1𝑝−1−𝛾𝑧(𝑠)(5.12) for 𝑠>𝑠0.
Let 𝑣(𝑠) be a solution of ğ‘£î…ž(𝑠)=𝐶𝑒−𝑠−1𝑝−1−𝛾𝑣(𝑠)(5.13) with 𝑣(𝑠0)≥𝑧(𝑠0). Integrating this equation we get 𝑣(𝑠)=𝐶1𝑒−𝑠+𝐶2𝑒−(1/(𝑝−1)−𝛾)𝑠.(5.14) By a comparison argument we could get that for every 𝑠>𝑠0, 𝑧(𝑠)≤𝑣(𝑠)=𝐶1𝑒−𝑠+𝐶2𝑒−(1/(𝑝−1)−𝛾)𝑠.(5.15) Now we go back to 𝑧′(𝑠)=𝐶𝑒−𝑠−(1/(𝑝−1))𝑧(𝑠)+𝑧𝑝(𝑠). We have ğ‘§î…ž(𝑠)+(1/(𝑝−1))𝑧(𝑠)=𝐶𝑒−𝑠+𝑧𝑝(𝑠),(5.16) then 𝑒(1/(𝑝−1))𝑠𝑧(𝑠)=𝑒(1/(𝑝−1))𝑠(𝐶𝑒−𝑠+𝑧𝑝).(5.17) Integrating form 𝑠0 to 𝑠, one could get 𝑧(𝑠)=𝑒−(1/(𝑝−1))𝑠𝐶1+𝑠𝑠0𝑒(1/(𝑝−1))ğœŽ(ğ¶ğ‘’âˆ’ğœŽ+𝑧𝑝(𝑠))ğ‘‘ğœŽ=𝑒−(1/(𝑝−1))𝑠𝐶1+𝑠𝑠0𝑒−((𝑝−2)/(𝑝−1))ğœŽ(𝐶+ğ‘’ğœŽğ‘§ğ‘î‚¶.(𝑠))ğ‘‘ğœŽ(5.18) Using (5.15) and 𝛾<1/𝑝(𝑝−1), we have 𝑒𝑠𝑧𝑝≤𝐶𝑝1𝑒−(𝑝−1)𝑠+𝐶𝑝2𝑒−(𝑝/(𝑝−1)−𝑝𝛾−1)𝑠⟶0(5.19) as 𝑠→+∞.
And thus from (5.18), we get 𝑧(𝑠)≤𝑒−(1/(𝑝−1))𝑠𝐶1+𝐶3𝑠𝑠0𝑒−((𝑝−2)/(𝑝−1))ğœŽî‚¶ğ‘‘ğœŽâ‰¤ğ¶1𝑒−(1/(𝑝−1))𝑠+𝐶4𝑒−𝑠.(5.20)
As 𝑝>2, we have 𝑧(𝑠)≤𝐶𝑒−(1/(𝑝−1))𝑠.(5.21) This implies that 𝑤(𝑡)≤𝐶, for 0≤𝑡<𝑇. From the boundedness of 𝑤 and (5.7) we get 𝑢(𝑥,𝑡)≤𝑤(𝑡)≤𝐶 for every 𝑥∈Ω⧵𝐵𝜖(𝑥0), as we wished.

Next, we will consider the radial symmetric case, that is, the proof of Theorem 1.5. For the convenience of writing, we only deal with the one dimensional case, Ω=(−𝑙,𝑙). The radial case is analogous; we leave the details to the reader.

Proof of Theorem 1.5. Under the hypothesis on the initial condition imposed in Theorem 1.5 we have that the solution is symmetric and 𝑢𝑥<0 in (0,𝑙]×(0,𝑇) from the stand parabolic theorem and Lemma 4.1 of [10]. Therefore the solution has a unique maximum at the origin for every 𝑡∈(0,𝑇).
Let us perform the following change of variables 𝑧(𝑥,𝑠)=(𝑇−𝑡)1/(𝑝−1)𝑢(𝑥,𝑡),𝑠=−ln(𝑇−𝑡).(5.22) Our remainder proof consist of two steps.
Step 1. We first prove the only blowup point that verifies the blowup estimate (1.7) is 𝑥=0. And this shows that for 𝑥≠0, 𝑧(𝑥,𝑠) does not converge to 𝐶𝑝=(𝑝−1)−1/(𝑝−1) as 𝑠→+∞.
We conclude by contradiction. Assume that (𝑇−𝑡)1/(𝑝−1)𝑢(𝑥0,𝑡)→𝐶𝑝 for a 𝑥0>0.
Let 𝑣(𝑡)=𝑢(0,𝑡)−𝑢(𝑥0,𝑡). Then ğ‘£î…žî€œ(𝑡)=𝑙−𝑙𝐽(−𝑦)(𝑢(𝑦,𝑡)−𝑢(0,𝑡))𝑑𝑦−𝑙−𝑙𝐽𝑥0𝑥−𝑦𝑢(𝑦,𝑡)−𝑢0,𝑡𝑑𝑦+𝑝𝜉𝑝−1(𝑡)𝑣(𝑡)âˆ’ğ‘˜ğ‘žğœ‚ğ‘žâˆ’1(𝑡)𝑣(𝑡),(5.23) where 𝜉(𝑡) and 𝜂(𝑡) are between 𝑢(0,𝑡) and 𝑢(𝑥0,𝑡). Hence ğ‘£î…žî€œ(𝑡)≥𝑙−𝑙𝑥𝐽(−𝑦)−𝐽0+−𝑦𝑢(𝑦,𝑡)𝑑𝑦𝑙−𝑙𝐽𝑦−𝑥0−𝐽(𝑦)𝑢(0,𝑡)𝑑𝑦−𝑣(𝑡)+𝑝𝜉𝑝−1(𝑡)𝑣(𝑡)âˆ’ğ‘˜ğ‘žğœ‚ğ‘žâˆ’1(=𝑡)𝑣(𝑡)𝑙−𝑙𝐽𝑦−𝑥0−𝐽(𝑦)(𝑢(0,𝑡)−𝑢(𝑦,𝑡))𝑑𝑦−𝑣(𝑡)+𝑝𝜉𝑝−1(𝑡)𝑣(𝑡)âˆ’ğ‘˜ğ‘žğœ‚ğ‘žâˆ’1≥(𝑡)𝑣(𝑡)−𝐶1+𝑝𝜉𝑝−1(𝑡)âˆ’ğ‘˜ğ‘žğœ‚ğ‘žâˆ’1(𝑡)𝑣(𝑡),(5.24) for some positive constant.
Integrating the above inequality, we obtain 𝑡ln(𝑣)(𝑡)−ln(𝑣)0≥𝑡𝑡0−𝐶1+𝑝𝜉𝑝−1(𝑠)âˆ’ğ‘˜ğ‘žğœ‚ğ‘žâˆ’1(𝑠)𝑑𝑠.(5.25) Remember that (𝑇−𝑡)1/(𝑝−1)𝑢(𝑥0,𝑡)→𝐶𝑝, (𝑇−𝑡)1/(𝑝−1)𝑢(0,𝑡)→𝐶𝑝, we have lim𝑡→𝑇𝜉(𝑡)(𝑇−𝑡)1/(𝑝−1)=lim𝑡→𝑇𝜂(𝑡)(𝑇−𝑡)1/(𝑝−1)=𝐶𝑝.(5.26) And this implies that 𝑡𝑡0−𝐶1+𝑝𝜉𝑝−1(𝑠)âˆ’ğ‘˜ğ‘žğœ‚ğ‘žâˆ’1(𝑠)𝑑𝑠≥𝑝𝑡𝑡0𝐶𝑝𝑝−1−𝛿1î€œğ‘‡âˆ’ğ‘ ğ‘‘ğ‘ âˆ’ğ‘˜ğ‘žğ‘¡ğ‘¡0î‚€ğ¶ğ‘ğ‘žâˆ’1+𝛿2(𝑇−𝑠)−(ğ‘žâˆ’1)/(𝑝−1)𝑑𝑠−𝐶2.(5.27)𝑝>ğ‘ž implies that (𝑇−𝑠)−(ğ‘žâˆ’1)/(𝑝−1)≤𝛿3(𝑇−𝑠)−1 as 𝑠→𝑇 for given 𝛿3>0. Hence 𝑡𝑡0−𝐶1+𝑝𝜉𝑝−1(𝑠)âˆ’ğ‘˜ğ‘žğœ‚ğ‘žâˆ’1(𝑠)𝑑𝑠≥𝑝𝑡𝑡0𝐶𝑝𝑝−1−𝛿𝑇−𝑠𝑑𝑠−𝐶2𝐶=−𝑝𝑝𝑝−1−𝛿ln(𝑇−𝑡)−𝐶2(5.28) for some 𝛿>0.
Hence 𝑣(𝑡)≥𝐶(𝑇−𝑡)−𝑝(𝐶𝑝𝑝−1−𝛿)=𝐶(𝑇−𝑡)𝑝𝛿−𝑝/(𝑝−1).(5.29) Using this fact, we have 0=lim𝑡→𝑇(𝑇−𝑡)1/(𝑝−1)𝑣(𝑡)≥𝐶lim𝑡→𝑇(𝑇−𝑡)1/(𝑝−1)−𝑝/(𝑝−1)+𝑝𝛿=+∞.(5.30) This contradiction proves our claim.
Step 2. We will show the only possible blowup point is 𝑥=0.
Remembering the transform (5.22), 𝑧(𝑥,𝑠) satisfies 𝑧𝑠=𝑒−𝑠𝑙−𝑙1𝐽(𝑥−𝑦)(𝑧(𝑦,𝑠)−𝑧(𝑥,𝑠))𝑑𝑦−𝑝−1𝑧+𝑧𝑝−𝑘𝑒((ğ‘žâˆ’ğ‘)/(𝑝−1))ğ‘ ğ‘§ğ‘ž.(5.31) Note that the blowup rate of 𝑢 implies that 𝑧(𝑥,𝑠)≤𝐶 for every (𝑥,𝑠)∈[−𝑙,𝑙]×(−ln𝑇,∞). Therefore, 𝑧𝑠(𝑥,𝑠)≤𝐶𝑒−𝑠−1𝑝−1𝑧(𝑥,𝑠)+𝑧𝑝(𝑥,𝑠).(5.32) From this we know that if there exists 𝑠0 such that 𝑧𝑝(𝑥,𝑠0)−(1/(𝑝−1))𝑧(𝑥,𝑠0)<−𝐶𝑒−𝑠0, then 𝑧(𝑥,𝑠)→0 as ğ‘ â†’âˆž (see Lemma 4.2 in [24]).
Moreover, if there exists 𝑠0 such that 𝑧𝑝(𝑥,𝑠0)−(1/(𝑝−1))𝑧(𝑥,𝑠0)>𝐶𝑒−𝑠0 then 𝑧(𝑥,𝑠) blows up in finite time 𝑠. This follows from Lemma 4.3 of [24] using that 𝑧𝑠(𝑥,𝑠)≥−𝐶𝑒−𝑠−1𝑝−1𝑧(𝑥,𝑠)+𝑧𝑝(𝑥,𝑠).(5.33)
Thus if 𝑧(𝑥,𝑠) does not converge to zero and does not blow up in finite time, then 𝑧(𝑥,𝑠) satisfies 𝐶𝑒−𝑠≥𝑧𝑝1(𝑥,𝑠)−𝑝−1𝑧(𝑥,𝑠)≥−𝐶𝑒−𝑠.(5.34) Henceforth, 𝑧𝑝1(𝑥,𝑠)−𝑝−1𝑧(𝑥,𝑠)⟶0(𝑠⟶+∞).(5.35) As 𝑧(𝑥,𝑠) is continuous, bounded and does not go to zero, we conclude that 𝑧(𝑥,𝑠)→𝐶𝑝.
Now we could conclude that 𝑧(𝑥,𝑠) verifies 𝑧(𝑥,𝑠)→0(𝑠→+∞), or 𝑧(𝑥,𝑠)→𝐶𝑝(𝑠→+∞), or 𝑧(𝑥,𝑠) blows up in finite time.
From Step 1 we know for 𝑥≠0, 𝑧(𝑥,𝑠) is bounded and does not converge to 𝐶𝑝, so 𝑧(𝑥,𝑠)→0 as 𝑠→+∞. Combined with inequality (5.32), we could get 𝑧𝑠(𝑥,𝑠)≤𝐶𝑒−𝑠−1𝑝−1−𝜃𝑧(𝑥,𝑠)(5.36) for any 𝜃>0.
By a comparison argument as in the proof of Theorem 1.4, it follows that 𝑧(𝑥,𝑠)≤𝐶1𝑒−𝑠+𝐶2𝑒−(1/(𝑝−1)−𝜃)𝑠.(5.37) Going back to the equation verified by 𝑧(𝑥,𝑡) we obtain 𝑒(1/(𝑝−1))𝑠𝑧(𝑥,𝑠)𝑠=𝑒(1/(𝑝−1))𝑠𝑒−𝑠𝑙−𝑙𝐽(𝑥−𝑦)(𝑧(𝑦,𝑠)−𝑧(𝑥,𝑠))𝑑𝑦+𝑧𝑝(𝑥,𝑠)−𝑘𝑒((ğ‘žâˆ’ğ‘)/(𝑝−1))𝑠.𝑧(𝑥,𝑠)(5.38) Integrating we get 𝑧(𝑥,𝑠)=𝑒−(1/(𝑝−1))𝑠𝐶1+𝑠𝑠0𝑒−((𝑝−2)/(𝑝−1))ğœŽî‚µî€œğ‘™âˆ’ğ‘™ğ½(𝑥−𝑦)(𝑧(𝑦,𝑠)−𝑧(𝑥,𝑠))𝑑𝑦+ğ‘’ğœŽğ‘§ğ‘(𝑥,𝑠)−𝑘𝑒((ğ‘žâˆ’1)/(𝑝−1))ğœŽ.𝑧(𝑥,𝑠)ğ‘‘ğœŽî‚¶î‚¶(5.39) On the other hand, (5.37) implies that 𝑒𝑠𝑧𝑝(𝑥,𝑠)→0 as ğ‘ â†’âˆž. Henceforth, 𝑧(𝑥,𝑠)≤𝑒−(1/(𝑝−1))𝑠𝐶1+𝐶2𝑠𝑠0𝑒−((𝑝−2)/(𝑝−1))ğœŽî‚¶.ğ‘‘ğœŽ(5.40) Using that 𝑝>2, one could have 𝑧(𝑥,𝑠)≤𝐶3𝑒−(1/(𝑝−1))𝑠.(5.41) Remembering the transform (5.22), we have 𝑢(𝑥,𝑡)=𝑒(1/(𝑝−1))𝑠𝑧(𝑥,𝑠)≤𝑐3.(5.42) And so our proof is complete.

6. Numerical Experiments

At the end of this paper, we will use several numerical examples to demonstrate our results about the location of blowup points. For this purpose, we discretize the problem in the spacial variable to obtain an ODE system. Taking Ω=[−4,4] and −4=𝑥−𝑁<⋯<𝑥𝑁=4,𝑁=100, we consider the following system: ğ‘¢î…žğ‘–(𝑡)=𝑁𝑗=−𝑁𝐽𝑥𝑖−𝑥𝑗𝑢𝑗(𝑡)−𝑢𝑖+𝑢(𝑡)𝑖𝑝𝑢(𝑡)âˆ’ğ‘˜ğ‘–î€¸ğ‘žğ‘¢(𝑡),𝑖(0)=𝑢0𝑥𝑖.(6.1) Next we choose 𝑝=3, ğ‘ž=1, 𝑘=1 and ⎧⎪⎨⎪⎩1𝐽(𝑧)=1,|𝑧|≤,1100,|𝑧|>.10(6.2)

In Figure 1 we choose a nonsymmetric initial condition very large near the point 𝑥0=1,  𝑢0(𝑥)=1/4+100(1−|𝑥−1|)+. We observe that the blowup set is localized in a neighborhood of 𝑥0=1.

Next we choose a symmetric initial condition with a unique maximum at the origin, 𝑢0(𝑥)=16−𝑥20. We observe that the solution blows up only at the origin, Figure 2.

Acknowledgments

Y. Wang is supported by the Key Scientific Research Foundation of Xihua University (no.  Z0912611), the Scientific Research Found of Sichuan Provincial Education Department (no. 09ZB081) and the Research Fund of Key Disciplinary of Application Mathematics of Xihua University (no. XZD0910-09-1). Z. Xiang is supported by NNSF of China (11101068), the Sichuan Youth Science & Technology Foundation (2011JQ0003), the Fundamental Research Funds for the Central Universities (ZYGX2009X019) and the SRF for ROCS, SEM. J. Hu is supported by the Scientific Research Found of Sichuan Provincial Education Department (no. 11ZB009).

References

  1. P. W. Bates, P. C. Fife, X. Ren, and X. Wang, “Traveling waves in a convolution model for phase transitions,” Archive for Rational Mechanics and Analysis, vol. 138, no. 2, pp. 105–136, 1997. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  2. P. W. Bates, “On some nonlocal evolution equations arising in materials science,” in Nonlinear Dynamics and Evolution Equations, H. Brunner, X. Zhao, and X. Zou, Eds., vol. 48 of Fields Institute Communications, pp. 13–52, American Mathematical Society, Providence, RI, USA, 2006. View at: Google Scholar | Zentralblatt MATH
  3. P. W. Bates and J. Han, “The Dirichlet boundary problem for a nonlocal Cahn-Hilliard equation,” Journal of Mathematical Analysis and Applications, vol. 311, no. 1, pp. 289–312, 2005. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  4. P. W. Bates and J. Han, “The Neumann boundary problem for a nonlocal Cahn-Hilliard equation,” Journal of Differential Equations, vol. 212, no. 2, pp. 235–277, 2005. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  5. G. B. Ermentrout and J. B. McLeod, “Existence and uniqueness of travelling waves for a neural network,” Proceedings of the Royal Society of Edinburgh A, vol. 123, no. 3, pp. 461–478, 1993. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  6. P. Fife, “Some nonclassical trends in parabolic and parabolic-like evolutions,” in Trends in Nonlinear Analysis, pp. 153–191, Springer, Berlin, Germany, 2003. View at: Google Scholar | Zentralblatt MATH
  7. C. Lederman and N. Wolanski, “Singular perturbation in a nonlocal diffusion problem,” Communications in Partial Differential Equations, vol. 31, no. 1–3, pp. 195–241, 2006. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  8. E. Chasseigne, M. Chaves, and J. D. Rossi, “Asymptotic behavior for nonlocal diffusion equations,” Journal de Mathématiques Pures et Appliquées. Neuvième Série, vol. 86, no. 3, pp. 271–291, 2006. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  9. M. Bogoya, R. Ferreira, and J. D. Rossi, “A nonlocal nonlinear diffusion equation with blowing up boundary conditions,” Journal of Mathematical Analysis and Applications, vol. 337, no. 2, pp. 1284–1294, 2008. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  10. M. Pérez-Llanos and J. D. Rossi, “Blow-up for a non-local diffusion problem with Neumann boundary conditions and a reaction term,” Nonlinear Analysis: Theory, Methods & Applications A, vol. 70, no. 4, pp. 1629–1640, 2009. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  11. J. Terra and N. Wolanski, “Asymptotic behavior for a nonlocal diffusion equation with absorption and nonintegrable initial data: the supercritical case,” Proceedings of the American Mathematical Society, vol. 139, no. 4, pp. 1421–1432, 2011. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  12. N. Bedjaoui and P. Souplet, “Critical blowup exponents for a system of reaction-diffusion equations with absorption,” Zeitschrift für Angewandte Mathematik und Physik, vol. 53, no. 2, pp. 197–210, 2002. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  13. Z. Xiang, Q. Chen, and C. Mu, “Blow-up rate estimates for a system of reaction-diffusion equations with absorption,” Journal of the Korean Mathematical Society, vol. 44, no. 4, pp. 779–786, 2007. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  14. C. Cortazar, M. Elgueta, J. D. Rossi, and N. Wolanski, “How to approximate the heat equation with Neumann boundary conditions by nonlocal diffusion problems,” Archive for Rational Mechanics and Analysis, vol. 187, no. 1, pp. 137–156, 2008. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  15. C. Cortazar, M. Elgueta, J. D. Rossi, and N. Wolanski, “Boundary fluxes for nonlocal diffusion,” Journal of Differential Equations, vol. 234, no. 2, pp. 360–390, 2007. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  16. J. García-Melián and F. Quirós, “Fujita exponents for evolution problems with nonlocal diffusion,” Journal of Evolution Equations, vol. 10, no. 1, pp. 147–161, 2010. View at: Publisher Site | Google Scholar
  17. J. D. Murray, Mathematical Biology: I. An introduction, vol. 17 of Interdisciplinary Applied Mathematics, Springer, New York, NY, USA, 3rd edition, 2002.
  18. M. Bogoya, “A nonlocal nonlinear diffusion equation in higher space dimensions,” Journal of Mathematical Analysis and Applications, vol. 344, no. 2, pp. 601–615, 2008. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  19. A. Buades, B. Coll, and J. M. Morel, “Image denoising methods—a new nonlocal principle,” SIAM Review, vol. 52, no. 1, pp. 113–147, 2010. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  20. C. Cortazar, M. Elgueta, and J. D. Rossi, “Nonlocal diffusion problems that approximate the heat equation with Dirichlet boundary conditions,” Israel Journal of Mathematics, vol. 170, pp. 53–60, 2009. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  21. L. I. Ignat and J. D. Rossi, “Decay estimates for nonlocal problems via energy methods,” Journal de Mathématiques Pures et Appliquées, vol. 92, no. 2, pp. 163–187, 2009. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  22. Y. Lou, X. Zhang, S. Osher, and A. Bertozzi, “Image recovery via nonlocal operators,” Journal of Scientific Computing, vol. 42, no. 2, pp. 185–197, 2010. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  23. A. Friedman and B. McLeod, “Blow-up of positive solutions of semilinear heat equations,” Indiana University Mathematics Journal, vol. 34, no. 2, pp. 425–447, 1985. View at: Publisher Site | Google Scholar | Zentralblatt MATH
  24. P. Groisman and J. D. Rossi, “Asymptotic behaviour for a numerical approximation of a parabolic problem with blowing up solutions,” Journal of Computational and Applied Mathematics, vol. 135, no. 1, pp. 135–155, 2001. View at: Publisher Site | Google Scholar

Copyright © 2012 Yulan Wang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

668 Views | 450 Downloads | 0 Citations
 PDF  Download Citation  Citation
 Download other formatsMore
 Order printed copiesOrder