
This article demonstrates the stability property of two boundary equilibria of a symbiotic model of commensalism and parasitism with harvesting in the commensal population. The model was proposed by Nurmaini Puspitasari, Wuryansari Muharini Kusumawinahyu, Trisilowati (2021). We first give two numeric examples to show that the corresponding results of the mentioned paper may be incorrect. Then, by analysis of the characteristic roots of the characteristic equations, we obtain sufficient conditions that ensure the locally asymptotic stability of the equilibria. After that, by applying the standard comparison theorem, some novel results on the global attractivity of these two equilibria are obtained respectively. Our results complement and supplement some known results.
Citation: Xiaowan Liu, Qin Yue. Stability property of the boundary equilibria of a symbiotic model of commensalism and parasitism with harvesting in commensal populations[J]. AIMS Mathematics, 2022, 7(10): 18793-18808. doi: 10.3934/math.20221034
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This article demonstrates the stability property of two boundary equilibria of a symbiotic model of commensalism and parasitism with harvesting in the commensal population. The model was proposed by Nurmaini Puspitasari, Wuryansari Muharini Kusumawinahyu, Trisilowati (2021). We first give two numeric examples to show that the corresponding results of the mentioned paper may be incorrect. Then, by analysis of the characteristic roots of the characteristic equations, we obtain sufficient conditions that ensure the locally asymptotic stability of the equilibria. After that, by applying the standard comparison theorem, some novel results on the global attractivity of these two equilibria are obtained respectively. Our results complement and supplement some known results.
The aim of this paper is to present an investigation of the dynamic behaviors of the following symbiotic model of commensalism and parasitism with harvesting in the commensal population:
dxdt=r1x(1−xk1+ayk1)−qExm1E+m2x,dydt=r2y(1−yk2−bzk2),dzdt=r3z(1−zk3+cyk3), | (1.1) |
where x(t),y(t) and z(t) denote the commensal population, host population and parasite species, respectively. All parameters used in this model are positive. The definitions of these parameters are as follows: ri,i=1,2,3 represents the intrinsic growth of x,y and z; ki,i=1,2,3 show the carrying capacities of x, y and z. The parameter a is the interaction parameter for x and y and b and c the interaction parameters between y and z. The parameter E is the fishing effort parameter used to harvest, q is the catching power coefficient and m1 and m2 are the suitable constants.
During the lase few decades, many scholars have investigated the dynamic behaviors of the commensalism model [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38]. Biologists have studied the phenomenon of commensalism through direct observation of wild species [7,8,9]. Mathematicians have studied the dynamic behavior of biased populations through hypothesis and theoretical derivation, with relevant topics including the influence of the Allee effect [1,2,3,4,5,6,26,27,28], the influence of functional response [10,13,21,22,25,28,29], the influence of feedback controls [28,29,30], the influence of linear harvesting or Michaelis-Menten type harvesting [15,16,23,31,32,33,34,35,36,37,38], the existence of a positive periodic solution or an almost periodic solution [11,12,14,20,22,31,36], the influence of stage structure [17], the stability of the system [10,18,32,33,34,35], the influence of nonlinear birth rates [19], the influence of noise [24], the influence of delays[25]; These topics have been extensively investigated and many important results were obtained. On the other hand, to meet human needs, the exploitation of biological resources and harvesting of populations are commonly practiced in fishery, forestry and wildlife management. Ecological modeling incorporates linear harvesting or Michaelis-Menten type harvesting, and it has become one of the main study topics in the area of population dynamics [15,16,23], [31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48]. Chen [38] was first to incorporate the Michaelis-Menten-type harvesting into the two species Lotka-Volterra commensalism model, and he investigated the local and global stability of the equilibria. Since then, many scholars have conducted works on commensalism systems with Michaelis-Menten type harvesting [31,32,33,34,35,36,37,38]. However, the commensalism models were not well studied in the sense that to this day, most of the works have focused on the two species case. Only recently did Puspitasari, Kusumawinahyu and Trisilowati[32,33] begin to study three species and four species cases. In [32], Puspitasari, Kusumawinahyu and Trisilowati proposed System (1.1). The system has eight equilibria, which take the following forms:
T0(0,0,0),T1(0,0,k3),T2(0,k2,0),T3(x∗3,0,0),T4(0,k2−bk31+bc,k3+ck21+bc),T5(x∗5,0,k3),T6(x∗6,k2,0),T7(x∗7,y∗7,z∗7). |
Concerned with the local stability property of those equilibria, the authors declared that "of the eight points, only two points are asymptotically stable if they meet certain conditions." Indeed, they showed that T4 and T7 are locally asymptotically stable while the other six equilibria are all unstable. Note that from the third equation of System (1.1), we have that
dzdt=r3z(1−zk3+cyk3)≥r3z(1−zk3). |
Hence,
lim inft→+∞z(t)≥k3. |
That is, for any positive initial conditions, z(t) can not approach 0 as t→+∞, which means that the equilibria T0,T2,T3 and T6 are always unstable. Hence, it is only necessary to investigate the stability property of the remaining four equilibria.
Now let us consider the following two examples.
Example 1.1. Consider the following system
dxdt=x(1−x+y)−3x1+x,dydt=y(1−y−2z),dzdt=z(1−z+y). | (1.2) |
Here, for System (1.1), we chose ri=ki=E=c=a=1,i=1,2,3,b=2,q=3 and m1=m2=1. The results of numerical simulations (Figures 1–3) show that in this case, T1(0,0,1) is locally asymptotically stable.
Example 1.2. Consider the following system
dxdt=x(1−x+y)−0.1x1+x,dydt=y(1−y−2z),dzdt=z(1−z+y). | (1.3) |
Here, all the coefficients are the same as that of System (1.2), only with q changing from 3 to 0.1. The results of numerical simulations (Figures 4–6) show that in this case, T5(x∗5,0,k3)=(0.949,0,1) is locally asymptotically stable.
The above two examples show that in System (1.1), T1(0,0,k3) and T5(x∗5,0,k3) are all possibly asymptotically stable. The conclusion of Puspitasari, Kusumawinahyu and Trisilowati[32] may be incorrect.
Now, one natural problem is to obtain sufficient conditions to ensure the local asymptotic stability of the equilibria T1(0,0,k3) and T5(x∗5,0,k3). Another interesting thing is that the conclusions of Puspitasari, Kusumawinahyu and Trisilowati[32] are all local ones; thus, we wanted to to whether we could obtain some sufficient conditions to ensure the globally stability property of the equilibrium.
The aim of this study was to give definitive answers to the above two problems.
We will investigate the local stability property of T1(0,0,k3) and T5(x∗5,0,k3) in this section.
The variational matrix of System (1.1) is
J(x1,x2,y)=(F11r1xak100F22−r2ybk20r3zck3F33), | (2.1) |
where
F11=r1(1−xk1+ayk1)−r1xk1−qEm1E+m2x+qExm2(m1E+m2x)2,F22=r2(1−yk2−bzk2)−r2yk2,F33=r3(1−zk3+cyk3)−zr3k3. |
Theorem 2.1. Assume that
r1<qm1 | (2.2) |
and
1<bk3k2 | (2.3) |
hold, then, T1(0,0,k3) is locally asymptotically stable.
Proof. The Jacobian matrix of the equilibrium point T1(0,0,k3) is given by
(r1−qm1000r2(1−bk3k2)00cr3−r3). |
The characteristic equation of the above matrix is
(λ−(r1−qm1))(λ−r2(1−bk3k2))(λ+r3)=0. |
Hence, the characteristic roots are
λ1=r1−qm1<0,λ2=r2(1−bk3k2)<0,λ3=−r3<0. |
Consequently, T1(0,0,k3) is locally asymptotically stable. This ends the proof of Theorem 2.1.
Remark 2.1. In Example 1.1, one could easily check that
r1=1<qm1=3 |
and
1<bk3k2=2. |
Hence, it follows from Theorem 2.1 that T1(0,0,1) is locally asymptotically stable, which is consistence with the numerical simulations (Figures 1–3).
Theorem 2.2. Assume that
q<r1m1, | (2.4) |
qm2m21E<r1k1 | (2.5) |
and
1<bk3k2 | (2.6) |
hold, then, T5(x∗5,0,k3) is locally asymptotically stable.
Proof. x∗5 satisfies the equation
r1(1−xk1)−qEm1E+m2x=0. | (2.7) |
It is easy to verify that under the assumption that Eq (2.4) holds, Eq (2.7) admits a unique positive equilibrium, indeed, x∗5 could be expressed as follows:
x∗5=−B2+√B22−4B1B32B1, | (2.8) |
where
B1=r1m2,B2=r1m1E−k1m2r1,B3=Ek1q−Ek1m1r1. |
The Jacobian matrix of the system about the equilibrium point T5(x∗5,0,k3) is given by
(G11r1x∗5ak100r2(1−bk3k2)00cr3−r3), | (2.9) |
where
G11=r1(1−x∗5k1)−r1x∗5k1−qEm1E+m2x∗5+qEx∗5m2(m1E+m2x∗5)2=−r1x∗5k1+qEx∗5m2(m1E+m2x∗5)2(byusingEq(2.6)). |
The characteristic equation of the above matrix is
(λ−G11)(λ−r2(1−bk3k2))(λ+r3)=0. |
Hence, it follows from Eqs (2.5) and (2.6) that the characteristic roots are
λ1=−r1x∗5k1+qEx∗5m2(m1E+m2x∗5)2<−r1x∗5k1+qm2x∗5m21E<0, |
λ2=r2(1−bk3k2)<0,λ3=−r3<0. |
Consequently, T5(x∗5,0,k3) is locally asymptotically stable. This ends the proof of Theorem 2.2.
Remark 2.2. In Example 1.2, one could easily check that
q=0.1<r1m1=1, |
qm2m21E=0.1<1=r1k1 |
and
1<bk3k2=2. |
Hence, it follows from Theorem 2.2, T5(x∗5,0,k3) is locally asymptotically stable. This is consistent with the numerical simulations (Figures 4–6).
We showed in the previous section that T1(0,0,k3) and T5(x∗5,0,k3) could be locally asymptotically stable under some suitable assumption. In this section we will further show that, under some suitable assumption, T1(0,0,k3) and T5(x∗5,0,k3) could be globally attractive.
Theorem 3.1. Assume that
r1<qEm1E+m2k1 | (3.1) |
and
1<bk3k2 | (3.2) |
hold, then, T1(0,0,k3) is globally attractive.
Proof. For ε>0 sufficiently small, Condition (3.1) implies that
r1+ar1εk1<qEm1E+m2(k1+ε). | (3.3) |
Condition (3.2) implies that
1<b(k3−ε)k2. | (3.4) |
From the third equation of System (1.1), we have that
dzdt≥r3z(1−zk3), | (3.5) |
hence
lim inft→+∞z(t)≥k3. | (3.6) |
For aforementioned ε>0, there exists a T1>0 such that
z(t)>k3−εforallt>T1. |
From this and the second equation of System (1.1), for t>T1, we have that
dydt≤r2y(1−yk2−bk3−εk2)<r2y(1−bk3−εk2). |
Hence, it follows from Eq (3.4) that
y(t)<y(T1)exp{r2(1−bk3−εk2)(t−T1)}→0ast→+∞. |
The nonnegative of y(t) together with the above inequality leads to
limt→+∞y(t)=0. | (3.7) |
From Eq (3.7), for aforementioned ε>0, there exists a T2>T1 such that
y(t)<εast≥T2. | (3.8) |
For t≥T2, from the above inequality and the third equation of System (1.1), we have that
dzdt≤r3z(1−zk3+cεk3); |
so,
lim supt→+∞z(t)≤k3(1+cεk3). | (3.9) |
Equation (3.6) together with Eq (3.9) leads to
k3≤lim inft→+∞z(t)≤lim supt→+∞z(t)≤k3(1+cεk3). | (3.10) |
With ε as sufficiently small positive constants, setting ε→0 in Eq (3.10) leads to
limt→+∞z(t)=k3. | (3.11) |
For t≥T2, from Eq (3.8) and the first equation of System (1.1), we have that
dxdt≤r1x(1−xk1+aεk1). |
Thus,
lim supt→+∞x(t)≤k1(1+aεk1). |
Setting ε→0 in the above inequality leads to
lim supt→+∞x(t)≤k1. |
Consequently, for ε>0 sufficiently small, there exists a T3>T2 such that
x(t)<k1+εforallt≥T3. |
From the above inequality and the first equation of System (1.1), for t≥T3, we also have that
dxdt≤r1x(1−xk1+aεk1)−qExm1E+m2(k1+ε)≤x(r1+ar1εk1−qEm1E+m2(k1+ε)). |
It immediately follows from Eq(3.3) and the above inequality that
x(t)≤x(T3)exp{(r1+ar1εk1−qEm1E+m2(k1+ε))(t−T3)}→0ast→+∞, |
that is
limt→+∞x(t)=0. | (3.12) |
Equations (3.7), (3.11) and (3.12) show that T1(0,0,k3) is globally attractive.
This completes the proof of Theorem 3.1.
Remark 3.1. In Example 1.1, one could easily check that
r1=1<qEm1E+m2k1=32 |
and
1<bk3k2=2. |
Hence, it follows from Theorem 3.1 that T1(0,0,1) is globally attractive, which is consistent with the numerical simulations (Figures 1–3).
Theorem 3.2. Assume that
q<r1m1, | (3.13) |
qm2m21E<r1k1 | (3.14) |
and
1<bk3k2 | (3.15) |
hold, then, T5(x∗5,0,k3) is globally attractive.
Proof. The idea for the proof of this theorem comes from the work of Chen [38].
By using Eq (3.15), similar to the analysis of Eqs (3.5)–(3.11) in the proof of Theorem 3.1, we have that
limt→+∞y(t)=0,limt→+∞z(t)=k3. | (3.16) |
Let ε>0 be a sufficiently small positive constant; it follows from Eq (3.16) that there exists T>0 such that
y(t)<εforallt>T. |
From the above inequality and the first equation of System (1.1), we have that
dxdt≤r1x(1−xk1+αεk1)−qExm1E+m2x. | (3.17) |
Now, let us consider the equation
dudt=r1u(1−uk1+αεk1)−qEum1E+m2u. | (3.18) |
Condition (3.13) implies that
r1(1+αεk1)>qm1 |
holds. Let
F(u)=r1(1−uk1+αεk1)−qEm1E+m2u. |
Then, we have the following:
(1) There is a unique u∗ε, such that F(u∗ε)=0, where, by simple computation,
u∗ε=−A2+√A22−4A1A32A1. | (3.19) |
A1=m2r1,A2=Em1r1−εαm2r1−k1m2r1,A3=Ek1q−Ek1m1r1−Eαm1r1ε. |
(2) For all u∗ε>u>0,F(u)>0.
(3) For all u>u∗ε>0,F(u)<0.
Hence, it follows from Lemma 2.1 in [49] that the unique positive equilibrium u∗ε of System (3.18) is globally stable. By the comparison theorem of the differential equation, it immediately follows from Eqs (3.17) and (3.18) that
lim supt→+∞x(t)≤u∗ε. | (3.20) |
Since ε>0 is an arbitrary small positive constant, if we let ε→0 in Eq (3.19), from the expression of x∗5 (see Eq (2.8)), we have that
lim supt→+∞x(t)≤x∗5. | (3.21) |
From the first equation of Eq (1.1), we have that
dxdt≥r1x(1−xk1)−qExm1E+m2x. |
Now let us consider the equation
dwdt=r1w(1−wk1)−qEwm1E+m2w. | (3.22) |
Similar to the above analysis, we could show that (3.22) admits a unique positive equilibrium w=x∗5 that is globally stable. By the comparison theorem, it immediately follows that
lim inft→+∞x(t)≥x∗5. | (3.23) |
It follows from Eqs (3.21) and (3.23) that
limt→+∞x(t)=x∗5. | (3.24) |
Equations (3.16) and (3.24) show that T5(x∗5,0,k3) is globally attractive.
This ends the proof of Theorem 3.2.
Remark 3.2. In Example 1.2, one could easily check that all the conditions of Theorem 3.2 are satisfied; hence, it follows from Theorem 3.2 that T5(x∗5,0,k3) is globally attractive. This assertion is consistent with the numerical simulations (Figures 4–6).
Puspitasari, Kusumawinahyu and Trisilowati [32] proposed System (1.1). The system has eight equilibria. By computation, they showed that T4 and T7 are locally asymptotically stable while the other six equilibria are all unstable. However, our numerical simulations (Examples 1.1 and 1.2) showed that T1 and T5 are also possibly locally stable.
By analyzing the Jacobian matrix's characteristic equation for the equilibria T1 and T5, some suitable conditions that ensure the local asymptotical stability of the equilibria T1 and T5 were obtained.
Next, by developing the analysis technique of Baoguo Chen[38], we also obtained sufficient conditions that ensure the global attractivity of the two equilibria.
At the end of the paper, we would like to mention that to this day, most of the works on commensalism models focused on the two species case, and seldom did scholars study the more complicated multispecies case; we will try to do more works on this topic.
The research was supported by the Key Project of Humanities and Social Sciences in Anhui Province, (SK2020A0395), Key Research Project of College Level Humanities and Social Sciences of West Anhui University, (WXSK202037) and Key Program of Anhui Provincial Education Department (KJ2019A0618).
The authors would like to thank the two anonymous reviewers for their valuable comments, which have greatly improved the final expression of the paper.
The authors declare that there is no conflict of interest regarding the publication of this paper.
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