This paper deals with the initial value problem of a predator-prey system with dispersal and delay, which does not admit the classical comparison principle. When the initial value has nonempty compact support, the initial value problem formulates that two species synchronously invade the same habitat in population dynamics. By constructing proper auxiliary equations and functions, we confirm the faster invasion speed of two species, which equals to the minimal wave speed of traveling wave solutions in earlier works.
Citation: Shuxia Pan. Asymptotic spreading in a delayed dispersal predator-prey system without comparison principle[J]. Electronic Research Archive, 2019, 27: 89-99. doi: 10.3934/era.2019011
[1] | Shuxia Pan . Asymptotic spreading in a delayed dispersal predator-prey system without comparison principle. Electronic Research Archive, 2019, 27(0): 89-99. doi: 10.3934/era.2019011 |
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This paper deals with the initial value problem of a predator-prey system with dispersal and delay, which does not admit the classical comparison principle. When the initial value has nonempty compact support, the initial value problem formulates that two species synchronously invade the same habitat in population dynamics. By constructing proper auxiliary equations and functions, we confirm the faster invasion speed of two species, which equals to the minimal wave speed of traveling wave solutions in earlier works.
Spatial propagation dynamics of parabolic type systems has been widely investigated in literature, and two important indices on spatial propagation are minimal wave speed and spreading speed. Here, the minimal wave speed is the threshold on the existence of specific traveling wave solutions and the spreading speed of a nonnegative function
Definition 1.1. Assume that
a):
b):
From the viewpoint of mathematical biology, the above speed characterizes the spatial expansion of the individuals [28,34]. In the past decades, some important results on these two thresholds have been established for monotone semiflows, see [12,18,26,37,38] and a survey paper by Zhao [43]. When some special cooperative systems are concerned, it has been proven that all components governed by a system have the same spreading speed that is also the minimal wave speed of traveling wave solutions [18,26,38]. At the same time, it has been shown that different components may have different spreading speeds in several noncooperative systems [19,20,21,22,30,33], and at least the spreading speed of one species equals to the minimal wave speed of traveling wave solutions.
Recently, Li et al. [17] investigated the following nonmonotone system
{∂u1(x,t)∂t=d1[J1∗u1](x,t)+r1u1(x,t)F1(u1,u2)(x,t),∂u2(x,t)∂t=d2[J2∗u2](x,t)+r2u2(x,t)F2(u1,u2)(x,t), | (1) |
where
F1(u1,u2)(x,t)=1−u1(x,t)−b1∫0−τu1(x,t+s)dη11(s)−a1∫0−τu2(x,t+s)dη12(s),F2(u1,u2)(x,t)=1−u2(x,t)−b2∫0−τu2(x,t+s)dη22(s)+a2∫0−τu1(x,t+s)dη21(s) |
with constants
ηij(s) is nondecreasing on [−τ,0] and ηij(0)−ηij(−τ)=1,i,j=1,2. |
In this system,
[Ji∗ui](x,t)=∫RJi(x−y)[ui(y,t)−ui(x,t)]dy,i=1,2, |
where
(J1):
(J2): for any
(J3):
Clearly, (1) is a predator-prey system in population dynamics. In Li et al. [17], Yu and Yuan [41], Zhang et al. [42], the authors investigated its traveling wave solutions connecting
c∗i=infλ>0di[∫RJi(y)eλydy−1]+riλ,i=1,2. |
From the viewpoint of initial value problem, let any fixed time be the initial time, the traveling wave solutions in [17,41,42] indicate the initial size of habitat of both species is infinite, which contradicts to some natural phenomena because the initial invasion often begins in finite domain. The purpose of this paper is to explore the dynamics when the initial habitats of two invaders are finite and investigate the long time behavior of
{∂u1(x,t)∂t=d1[J1∗u1](x,t)+r1u1(x,t)F1(u1,u2)(x,t),∂u2(x,t)∂t=d2[J2∗u2](x,t)+r2u2(x,t)F2(u1,u2)(x,t),ui(x,s)=ϕi(x,s),x∈R,t>0,s∈[−τ,0],i=1,2, | (2) |
in which
(Ⅰ): For
ϕi(x,s)=0,|x|>L,s∈[−τ,0],ϕi(xi,0)>0 |
for some
0≤ϕ1(x,s)≤1,0≤ϕ2(x,s)≤1+a2,x∈R,s∈[−τ,0]. |
Since (2) involves delay effect of intraspecific competition if
In this section, we shall give and prove the main results on (2). Before giving the main results, we first define some positive constants as follows
c1=infλ>0d1[∫RJ1(y)eλydy−1]+r1(1−a1(1+a2))λ,c2=infλ>0d2[∫RJ2(y)eλydy−1]+r2(1+a2)λ,c∗2=d2[∫RJ2(y)eλ2ydy−1]+r2λ2, |
in which the existence and uniqueness of
Theorem 2.1. Assume that the mild solution
(0,0)≤(u1(x,t),u2(x,t))≤(1,1+a2),x∈R,t>0. | (3) |
Moreover,
(1): If
(2): Further suppose that
d1[∫RJ1(y)eλ2ydy−1]−c∗2λ2+r1≤0. | (4) |
If
We now prove the above theorem by several lemmas. Let
∂ui(x,t)∂t=di[Ji∗ui](x,t),ui(x,0)∈X |
generates a positive
ui(x,t)=Ti(t)ui(x,0)=Ti(t−s)ui(x,s) |
for any
{∂u(x,t)∂t=d[J∗u](x,t)+u(x,t)[r−u(x,t)],u(x,0)=χ(x)∈X,x∈R, | (5) |
where
![]() |
(6) |
By Jin and Zhao [15], we have the following conclusion.
Lemma 2.2. Assume that
u(x,t)=T(t−s)u(x,s)+∫tsT(t−θ)[u(x,θ)[r−u(x,θ)]]dθ |
for
{∂w(x,t)∂t≥(≤)d[J∗w](x,t)+w(x,t)[r−w(x,t)],x∈R,t>0,w(x,0)≥(≤)χ(x),x∈R, |
or
w(x,t)≥(≤)T(t−s)w(x,s)+∫tsT(t−θ)[w(x,θ)[r−w(x,θ)]]dθ |
for
w(x,t)≥(≤)u(x,t),x∈R,t>0. |
If
lim inft→∞inf|x|<ctu(x,t)=lim supt→∞sup|x|<ctu(x,t)=r. |
If
limt→∞sup|x|>ctu(x,t)=0,c>c′. |
Remark 1. By the positivity of the semigroup, if
{∂wi(x,t)∂t≥d[J∗wi](x,t)+wi(x,t)[r−wi(x,t)],x∈R,t>0,wi(x,0)≥χ(x),x∈R |
for
min{w1(x,t),w2(x,t),w3(x,t)}≥u(x,t),x∈R,t>0. |
On the existence of mild solution of (1), we have the following result.
Lemma 2.3. The positive mild solution
Proof. The local existence is evident by the theory of abstract functional differential equations [27], here the mild solution is defined by
u1(x,t)=T1(t−θ)u1(x,θ)+∫tθT1(t−s)[r1u1(x,s)F1(u1,u2)(x,s)]ds,u2(x,t)=T2(t−θ)u2(x,θ)+∫tθT2(t−s)[r2u2(x,s)F2(u1,u2)(x,s)]ds |
for
Further by the quasipositivity in
limt→T−supx∈Ru1(x,t)=∞, |
then
u1(x,t)≤T1(t−θ)u1(x,θ)+∫tθT1(t−s)[r1u1(x,s)[1−u1(x,s)]]ds |
for
0≤u1(x,t)≤1,x∈R,t∈[0,T). |
A contradiction occurs. The proof is complete by similar discussion on
To continue the discussion, we investigate the following scalar equation
{∂v(x,t)∂t=d[J∗v](x,t)+rv(x,t)[1−v(x,t)−b∫0−τv(x,t+s)dη(s)],v(x,s)=ν(x,s), | (7) |
where
η(s) is nondecreasing on [−τ,0] such that η(0)−η(−τ)=1. |
Furthermore,
Lemma 2.4. Assume that
Proof. We now prove it by the idea in Liu and Pan [25]. If
b∫0−τv(x,t+s)dη(s)=bv(x,t), |
then the result is clear by Lemma 2.2. Otherwise, the positivity implies that
v(x,t)≤T(t−s)v(x,s)+∫tsT(t−θ)[rv(x,θ)[1−v(x,θ)]]dθ |
for any
limt→∞sup|x|>ctv(x,t)=0,c>c′. |
For any fixed
lim inft→∞inf|x|<ctv(x,t)>0. |
For the purpose, we select
![]() |
and
b∫0−τ′dη(s)<ϵ. |
If
rv(x,t)[1−v(x,t)−b∫0−τv(x,t+s)dη(s)]≥rv(x,t)[1−3ϵ−v(x,t)]. |
When
v(x,s0)≥2ϵbτ, |
and the uniform continuity implies
v(y,s0)≥ϵbτ,|x−y|≤σ |
for some
{∂v_(x,t)∂t=d[J∗v_](x,t)+rv_(x,t)[1−b−v_(x,t)],v_(x,0)=ν_(x), | (8) |
where
(1):
(2):
(3):
By the positivity of
b∫0−τv(x,t+s)dη(s)≤b=bρρ≤bρv(x,t). |
That is,
v(x,t)≥T(t−s)v(x,s)+∫tsT(t−θ)[rv(x,θ)[1−3ϵ−(1+b/ρ)v(x,θ)]]dθ |
for all
Lemma 2.5. If
Proof. By (3),
u2(x,t)≤T2(t−θ)u2(x,θ)+∫tθT2(t−s)[r2u2(x,s)[1+a2−u2(x,s)]]ds |
for
lim supt→∞sup3|x|>(2c2+c1)tu2(x,t)=0. | (9) |
Again by (3), we see that
u1(x,t)≥T1(t−θ)u1(x,θ)+∫tθT1(t−s)[r1u1(x,s)×[1−a1(1+a2)−u1(x,s)−b1∫0−τu1(x,s+γ)dη11(γ)]]ds |
for all
lim inft→∞inf3|x|<(c2+2c1)tu1(x,t)>0. | (10) |
We now verify that
u1(x,t)≤T1(t−θ)u1(x,θ)+∫tθT1(t−s)[r1u1(x,s)[1−u1(x,s)]]ds |
for all
lim inft→∞inf|x|<ctu1(x,t)>0 | (11) |
for any given
c<infλ>0d[∫RJ(y)eλydy−1]+r(1−2ϵ)λ. |
By (9) and (10), there exists
![]() |
and
inft>Tinf2|x|≤(c2+c1)tu1(x,t)>0, |
which implies that there exists
u1(x,t)≥T1(t−θ)u1(x,θ)+∫tθT1(t−s)[r1u1(x,s)[1−ϵ−Mu1(x,s)−b1∫0−τu1(x,s+γ)dη11(γ)]]ds |
for any
∂v(x,t)∂t=d[J∗v](x,t)+rv(x,t)[1−ϵ−Mv(x,t)−b∫0−τv(x,t+s)dη(s)] |
by repeating the proof of Lemma 2.4. The proof is complete.
Lemma 2.6. Assume that (4) is true. If
Proof. By the positivity of (3),
u1(x,t)≤T1(t−θ)u1(x,θ)+∫tθT1(t−s)[r1u1(x,s)[1−u1(x,s)]ds |
for any
On the other hand,
u2(x,t)≥T2(t−θ)u2(x,θ)+∫tθT2(t−s)[r2u2(x,s)[1−u2(x,s)−b2∫0−τu2(x,s+γ)dη22(γ)]]ds |
for any
lim supt→∞sup|x|>ctu2(x,t)=0 |
for any fixed
u2(x,t)≤T2(t−θ)u2(x,θ)+∫tθT2(t−s)[r2u2(x,s)[1−u2(x,s)+a2∫0−τu1(x,s+γ)dη21(γ)]]ds, |
and the result is true if the spreading speed of the following equation is
∂u_2(x,t)∂t=d2[J2∗u_2](x,t)+r2u_2(x,t)[1−u_2(x,t)+a2∫0−τ¯u1(x,s)dη21(s)], | (12) |
where
¯u1(x,t)=T1(t)¯u1(x,0)+∫t0T1(t−s)[r1¯u1(x,s)[1−¯u1(x,s)]]ds. |
The main reason why the above claim is true is that the above equation (12) is monotone and admits comparison principle.
By Remark 1 and (4), we see that there exists
¯u1(x,t)≤min{eλ2(x+c2t+T1),eλ2(−x+c2t+T1),1},x∈R,t≥0. |
In fact, let
∂ˆu1(x,t)∂t≥d1[J1∗ˆu1](x,t)+r1ˆu1(x,t), |
and
∂ˆu1(x,t)∂t≥d1[J1∗ˆu1](x,t)+r1ˆu1(x,t)[1−ˆu1(x,t)] |
if
eλ2(T2−T1)>a2 |
and
min{eλ2(x+T2−c2τ),eλ2(−x+T2−c2τ),1+a2}≥sups∈[−τ,0]ϕ2(x,s),x∈R. |
Then Remark 1 implies that
u2(x,t)≤min{eλ2(x+c2t+T2),eλ2(−x+c2t+T2),1+a2},x∈R,t≥0 |
because
∂ˆu2(x,t)∂t≥d2[J2∗ˆu2](x,t)+r2ˆu2(x,t)[1−ˆu2(x,t)+a2∫0−τ¯u1(x,s)dη21(s)]. |
The proof is complete.
The propagation dynamics of predator-prey systems has important ecology background, one typical case is the evolution of insect herbivores and lupins on Mount St Helens, see [11,29]. Another related topic is the asymptotic spreading in epidemic models because of the similar monotone conditions. In literature, much attention has been paid to the traveling wave solutions since the work of Dunbar [10]. However, there are a few results on asymptotic spreading of predator-prey systems, see part results by Ducrot [7,8], Ducrot et al. [9], Lin [19], Lin et al. [23], Pan [30,32], Wang and Zhang [36].
The model in this paper admits nonlocal dispersal and time delays, the mechanism has significant biological reasons and other backgrounds [4,5,13,14,28], and the monotone case has been widely studied, see some recent works by [2,3,6]. Similar to that in [16,24], the model in this paper is not a monotone system [35] and time delay is not small enough. When the diffusion is of the classical Ficker type in (1), Pan [31] studied its minimal wave speed of traveling wave solutions connecting trivial steady state with the positive one.
In this paper, we show that
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