Research article

Preventing extinction in Rastrelliger brachysoma using an impulsive mathematical model

  • Received: 30 June 2021 Accepted: 25 September 2021 Published: 29 September 2021
  • MSC : 92-10, 34A37, 37G15

  • In this paper, we proposed a mathematical model of the population density of Indo-Pacific mackerel (Rastrelliger brachysoma) and the population density of small fishes based on the impulsive fishery. The model also considers the effects of the toxic environment that is the major problem in the water. The developed impulsive mathematical model was analyzed theoretically in terms of existence and uniqueness, positivity, and upper bound of the solution. The obtained solution has a periodic behavior that is suitable for the fishery. Moreover, the stability, permanence, and positive of the periodic solution are investigated. Then, we obtain the parameter conditions of the model for which Indo-Pacific mackerel conservation might be expected. Numerical results were also investigated to confirm our theoretical results. The results represent the periodic behavior of the population density of the Indo-Pacific mackerel and small fishes. The outcomes showed that the duration and quantity of fisheries were the keys to prevent the extinction of Indo-Pacific mackerel.

    Citation: Din Prathumwan, Kamonchat Trachoo, Wasan Maiaugree, Inthira Chaiya. Preventing extinction in Rastrelliger brachysoma using an impulsive mathematical model[J]. AIMS Mathematics, 2022, 7(1): 1-24. doi: 10.3934/math.2022001

    Related Papers:

    [1] A. Q. Khan, Ibraheem M. Alsulami, S. K. A. Hamdani . Controlling the chaos and bifurcations of a discrete prey-predator model. AIMS Mathematics, 2024, 9(1): 1783-1818. doi: 10.3934/math.2024087
    [2] Xiaohuan Yu, Mingzhan Huang . Dynamics of a Gilpin-Ayala predator-prey system with state feedback weighted harvest strategy. AIMS Mathematics, 2023, 8(11): 26968-26990. doi: 10.3934/math.20231380
    [3] Heping Jiang . Complex dynamics induced by harvesting rate and delay in a diffusive Leslie-Gower predator-prey model. AIMS Mathematics, 2023, 8(9): 20718-20730. doi: 10.3934/math.20231056
    [4] Ramkumar Kasinathan, Ravikumar Kasinathan, Dumitru Baleanu, Anguraj Annamalai . Hilfer fractional neutral stochastic differential equations with non-instantaneous impulses. AIMS Mathematics, 2021, 6(5): 4474-4491. doi: 10.3934/math.2021265
    [5] Dumitru Baleanu, Rabha W. Ibrahim . Optical applications of a generalized fractional integro-differential equation with periodicity. AIMS Mathematics, 2023, 8(5): 11953-11972. doi: 10.3934/math.2023604
    [6] A. M. Elaiw, A. S. Shflot, A. D. Hobiny . Stability analysis of SARS-CoV-2/HTLV-I coinfection dynamics model. AIMS Mathematics, 2023, 8(3): 6136-6166. doi: 10.3934/math.2023310
    [7] Mingzhan Huang, Shouzong Liu, Ying Zhang . Mathematical modeling and analysis of biological control strategy of aphid population. AIMS Mathematics, 2022, 7(4): 6876-6897. doi: 10.3934/math.2022382
    [8] Awatif J. Alqarni . Modeling and numerical simulation of Lumpy skin disease: Optimal control dynamics approach. AIMS Mathematics, 2025, 10(4): 10204-10227. doi: 10.3934/math.2025465
    [9] Yuanfu Shao . Dynamics and optimal harvesting of a stochastic predator-prey system with regime switching, S-type distributed time delays and Lévy jumps. AIMS Mathematics, 2022, 7(3): 4068-4093. doi: 10.3934/math.2022225
    [10] Yuxiao Zhao, Hong Lin, Xiaoyan Qiao . Persistence, extinction and practical exponential stability of impulsive stochastic competition models with varying delays. AIMS Mathematics, 2023, 8(10): 22643-22661. doi: 10.3934/math.20231152
  • In this paper, we proposed a mathematical model of the population density of Indo-Pacific mackerel (Rastrelliger brachysoma) and the population density of small fishes based on the impulsive fishery. The model also considers the effects of the toxic environment that is the major problem in the water. The developed impulsive mathematical model was analyzed theoretically in terms of existence and uniqueness, positivity, and upper bound of the solution. The obtained solution has a periodic behavior that is suitable for the fishery. Moreover, the stability, permanence, and positive of the periodic solution are investigated. Then, we obtain the parameter conditions of the model for which Indo-Pacific mackerel conservation might be expected. Numerical results were also investigated to confirm our theoretical results. The results represent the periodic behavior of the population density of the Indo-Pacific mackerel and small fishes. The outcomes showed that the duration and quantity of fisheries were the keys to prevent the extinction of Indo-Pacific mackerel.



    One of the most important foods for human is fish. It is about 35% of protein humans consumed. The South Pacific jack mackerel (JM) (Trachurus murphyi) is one of the most important fish for consumption in the world [6]. The Atlantic Mackerel (Scomber scombrus) is one of the most fish species in the North Atlantic which is widely spawned to produce human's food [10]. The India mackerel (Rastrilliger kangurta) [4] and Spanish mackerel (Scomberomorus commerson) [17] are also the fish production using for human consumption. In the Asia-Pacific region, Indo-Pacific mackerel (Rastrelliger brachysoma) or short mackerel is a fish indigenous in this region. This species spread almost in coasts and islands in the Gulf of Thailand and the Andaman sea [5]. It is about 14–20 centimeters long. It can spawn about 20,000 eggs at one time. Short mackerel is a pelagic fish that is highly economically important in the region because it is cheap and tasty [12]. It is therefore widely consumed in this region. So, there is high demand in South East Asia, resulting in numerous fisheries.

    In 1995, the Department of Fisheries, Ministry of Agriculture and Cooperatives, Thailand reported that short mackerels spawn two periods which are January to March and June to August each year. Moreover, they spawn more than 20 meters below sea level. Recently, the Department of Fisheries reports that the number of catching short mackerel drastically decreased every year. In 2014, on average 145,000 tons were caught per year 70,000 tons were caught in 2015, then 31,000 tons, 25,000 tons and 17,700 tons in 2016–2018, respectively [18]. The major problem is catching fish in the spawning season. The economic value loss caused by catching one ton of Indo-Pacific mackerel fry is about seven to eight million baht. The government proposed a law to protect fry from fisheries in 2015.

    The mathematical model is used for preparing to predict future phenomena in real-world problems. The model allows simulating any possibility. Many mathematical models have been used to describe the dynamic of the fish population. Bueno et al. reviewed the mathematical model for managing the carrying capacity of aquaculture activities in lakes [3]. The model of fish population dynamic was proposed by Hallam et al. by using the ordinary differential equations [7]. The model studied the changes in lipid and structure components which considered the energy demand and available energy. Khatun et al. proposed the mathematical model to studied renewable fishery management [11]. The two new second-order characteristic scheme was proposed to solve an age-structured population model with nonlinear diffusion and reaction [15] which used to consider the environmental and spatial region effect. Raymond et al. proposed the model to describe the dynamics of a two-prey one predator system in fishery [21].

    In addition, the toxicity in the sea is one of the problems which affect the population of short mackerels and their food. Bergami et al. studied the effect of plastic pollution in the marine ecosystem especially nanoplastics [2] to the plankton species which is the food of many fishes in the marine. Hashiguchi et al. identified and evaluated the toxicity of palm oil mill which affected the plankton species [8]. The antifouling compound zinc pyrithione (ZPT) was studied the effect on the natural planktonic communities by Hjorth et al. [9]. They found evidence of the diverse effect of ZPT on marine plankton. Kaur et al. proposed the dynamical model to study the effect of toxicity to the plankton system [19]. Randall and Tsui studied the effect of ammonia in the aquatic environment on the central nervous system of fish [20].

    To prevent the extinction of Indo-Pacific mackerels, we propose a mathematical model to find a way to control the catching of the Indo-Pacific mackerels by using the impulsive model. The novelty of this work is the prey-predator model of Indo-Pacific mackerels (short mackerels) and their foods which composes the toxic environment and impulsive fisheries. The impulsive model is a suitable model for fisheries because the fishermen are allowed to harvest fish on some periods for preventing the extinction of fish. The proposed model can be forecast the population of short mackerel and short mackerel food (plankton and small fishes). We analyze the model to consider the behavior of the model solution. The numerical simulations are used to verify the theoretical results.

    The rest of this paper is organized as follows: The modification model is proposed in Section 2, and model analysis is presented in Section 3. In Section 4, numerical simulations are showed, followed by conclusions in Section 5.

    Now, an impulsive mathematical model was proposed in which the control of the extinction of the short mackerel by considering biological control, toxic environment, and impulsive fisheries are as follows:

    For tnT,

    dx1dt=a1x1(1x1k1)bx1x2k2+x1d1x1u1x21, (2.1)
    dx2dt=a2x2(1x2k3)+rbx1x2k2+x1d2x2u2x22. (2.2)

    For t=nT,

    x1(t+)=(1γ)x1(t), (2.3)
    x2(t+)=(1ω)x2(t), (2.4)

    where x1(t) is the density of small fishes (short mackerel food) population at time t, x2(t) is the density of the short mackerel population at time t, T is the period of impulsive fisheries, γ is the negative effect of fisheries on the density of small fishes population, and ω is the negative effect of fisheries on the density of short mackerel population with nZ+, Z+={1,2,3,...}, 0<γ<1, and 0<ω<1. All parameters in the model are non-negative.

    Equation (2.1) expresses the rate of change of the population density of short mackerel food (small fishes). The small fishes increase by the logistic function with the growth rate a1 and the carrying capacity k1. On the other hand, the density of them decreases due to being hunted by short mackerel with rate b, natural death with the rate d1, and toxic death with the rate u1.

    Equation (2.2) expresses the rate of change of the population density of the short mackerel (Rastrelliger brachysoma). The short mackerels increase by the logistic function with the growth rate a2 and the carrying capacity k3. On the other hand, the density of them increases due to hunting small fishes with the rate r, natural death with the rate d2, and toxic death with the rate u2.

    Let

    V:R+×R2+R+, (3.1)

    where R+=[0,),R2+={XR2:X=(x1,x2),x10,x20}. The map defined by the right hand side of system (2.1)–(2.4) is denoted by F=(F1,F2).

    Definition 3.1 ([1]). The function V defined in (3.1) is said to belong to class V0 if

    (a) V is continuous in (nT,(n+1)T]×R2+R+ and for each XR2+,nZ+, lim(t,Y)(nT+,X)V(t,Y)=V(nT+,X) exists.

    (b) V is locally Lipschitzian in X.

    Definition 3.2 ([1]). Suppose VV0. For (t,X)(nT,(n+1)T]×R2+, the upper right derivative of V(t,X) with respect to system (2.1)–(2.4) is defined by

    D+V(t,X)=lim suph0+1h[V(t+h,X+hF(t,X))V(t,X)]

    where F=(F1,F2).

    The solution of system (2.1)–(2.4), X(t)=(x1(t),x2(t)), is assumed to be a piecewise continuous function. It means that, X(t) is continuous on (nT,(n+1)T], nZ+ and limtnT+X(t)=X(nT+) exists. By the smoothness properties of F, the system (2.1)–(2.4) has a unique solution.

    Lemma 3.3. Suppose X(t)=(x1(t),x2(t)) is a solution of the system (2.1)–(2.4) with the initial value X(0+)0. Then the solution X(t)0 for all t0.

    Proof. The solution x1(t) with non-negative initial value can be negative when the slope of x1(t) at 0 is negative. So, the proof of this Lemma can be expressed as follows:

    Case tnT.

    Consider the Eq (2.1)

    dx1dt=a1x1(1x1k1)bx1x2k2+x1d1x1u1x21.

    Whenever x1(t)=0, the slope of x1(t) can be described by dx1dt=0. This means that x1(t) cannot be negative. So, x1(t) is a non-negative solution.

    Consider the Eq (2.2)

    dx2dt=a2x2(1x2k3)+rbx1x2k2+x1d2x2u2x22.

    Whenever x2(t)=0, the slope of x2(t) can be described by dx2dt=0. This means that x2(t), cannot be negative. So, x2(t) is a non-negative solution.

    Case t=nT.

    Consider the Eq (2.3)

    x1(t+)=(1γ)x1(t).

    Since x10 and condition 0<γ<1, we have that x1(t+)0.

    Consider the Eq (2.4)

    x2(t+)=(1ω)x2(t).

    Since x20 and condition 0<ω<1, we have that x2(t+)0.

    Lemma 3.4. The solution X(t)=(x1(t),x2(t)) has upper bound i.e. x1(t)M and x2(t)M, for sufficiently large t, provided that

    d2>brk2. (3.2)

    Proof. We let V(t)=x1(t)+x2(t),

    M1=max(a1x1(1x1k1)u1x21)=a21k14(a1+u1k1),
    M2=max(a2x2(1x2k3)u2x22)=a22k34(a2+u2k3),

    and

    M3=sup(rbx11+k2x1)=rbk2.

    Consider tnT, we choose ˆc>0 and

    ˆc=min{d1,d2M3}.

    Then,

    D+V+ˆcV=dx1dt+dx2dt+ˆcx1+ˆcx2=a1x1(1x1k1)bx1x21+k2x1d1x1u1x21+a2x2(1x2k3)+rbx1x21+k2x1d2x2u2x22+ˆcx1+ˆcx2(ˆcd1)x1+(ˆc+M3d2)x2+M1+M2M1+M2M0.

    Hence D+V+ˆcVM0.

    Consider t=nT,

    V(nT+)=x1(nT+)+x2(nT+)=(1γ)x1(nT)+(1ω)x2(nT)=x1(nT)+x2(nT)γx1(nT)ωx2(nT)V(nT).

    By Lemma 2.2 of Liu et al. [16] we obtain that, for t(nT,(n+1)T],

    V(t)V(0)eˆct+t0M0eˆc(ts)dsV(0)eˆct+M0(1ˆceˆctˆc)<M0ˆcMast.

    Since there exists M>0 such that x1(t)M and x2(t)M for sufficiently large t thus V(t) is uniformly ultimately bounded.

    The reduced impulsive system of system (2.1)–(2.4) when the population density of small fishes is zero (x1=0) is:

    dx2dt=Bx2Ax22,tnT (3.3)
    x2(nT+)=(1ω)x2(nT),t=nT (3.4)
    x2(0+)=x20 (3.5)

    where Aa2k3+u2>0 and Ba2d2.

    We obtain B>0 if

    a2>d2. (3.6)

    The solution of Eq (3.3) is

    1x2(t)=AB+ceBt (3.7)

    where c is arbitrary constant.

    By the conditions (3.4), (3.6) and x2 is increasing function, a periodic solution of system (3.3)–(3.5) is

    1˜x2(t)=AB+ωAeB(tnT)B(1ωeBT),t(nT,(n+1)T] (3.8)

    with ˜x2(0+)=B(1ωeBT)A(1eBT)>0.

    Therefore, the system (3.3)–(3.5) has the positive solution

    1x2(t)=(1x20ABωAB(1ωeBT))eBt+1˜x2(t),t(nT,(n+1)T]. (3.9)

    Lemma 3.5. The periodic solution ˜x2(t) of system (3.3)(3.5) exists and x2(t)˜x2(t) as t for all solution x2(t) of system (3.3)(3.5). Hence,

    (0,˜x2(t))=(0,B(1ωeBT)ωAeB(tnT)+A(1ωeBT)),t(nT,(n+1)T]

    is a periodic solution of the original system (2.1)(2.4) at the zero density of small fishes for t(nT,(n+1)T] and

    ˜x2(nT+)=˜x2(0+)=B(1ωeBT)A(1eBT),nZ+.

    Theorem 3.6. Suppose

    Tmin<T<Tmax, (3.10)
    a1>d1+bBk2A, (3.11)

    and

    ln(11γ)>bk2Aln(11ω), (3.12)

    where

    Tmin1Bln(11ω),

    and

    Tmax1a1d1bBk2A[ln(11γ)bk2Aln(11ω)].

    Then the solution (0,~x2(t)) of the system (2.1)(2.4) is locally asymptotically stable.

    Proof. Here, we focus on a small perturbation (v1(t),v2(t)) from the point (0,˜x2(t)):

    x1(t)=v1(t),x2(t)=˜x2(t)+v2(t).

    Then,

    (v1(t)v2(t))=Φ(t)(v1(0)v2(0)),0<t<T

    where Φ(t) satisfies

    dΦ(t)dt=(a1d1b˜x2(t)k20B2A˜x2(t))Φ(t)

    with the identity matrix Φ(0)=I.

    Therefore, the matrix of fundamental solution is

    Φ(t)=(expt0(a1d1b˜x2(s)k2)ds0expt0(B2A˜x2(s))ds).

    Note that the terms (*) and (**) are not necessary to be calculated because the further analysis does not require these terms.

    Linearization of Eqs (2.3)–(2.4) yields

    (v1(nT+)v2(nT+))=(1γ001ω)(v1(nT)v2(nT)).

    The eigenvalues of the following matrix W,

    W=(1γ001ω)Φ(T),

    are

    λ1=(1γ)exp((a1d1)Tbk2A[ln(1ω)+BT]),λ2=(1ω)exp(BT2ln(1ω)).

    Since 0<γ<1,0<ω<1, and the conditions (3.6), (3.10)–(3.12) hold, it implies that

    1Bln(11ω)<T<1a1d1bBk2A[ln(11γ)bk2Aln(11ω)].

    Therefore, |λ1|<1 and |λ2|<1. We can conclude that the solution (0,~x2(t)) of the system (2.1)–(2.4) is locally asymptotically stable by Floquet thery. The proof is completed.

    Definition 3.7 ([1]). The system (2.1)(2.4) is permanent if the solution is bounded. That is, there are positive constants ˉa and ˉb and a finite time t0 such that for all solution with the positive initial values x1(0+)>0 and x2(0+)>0

    ˉax1(t)ˉb,ˉax2(t)ˉb,

    for all t>t0.

    Theorem 3.8. The system (2.1)(2.4) is permanent if inequalities (3.2), (3.6), (3.11), (3.12) hold and the following conditions:

    T>Tmax (3.13)

    and

    A>B+M3 (3.14)

    are satisfied.

    Proof. By Lemma 3.4, there is a constant M>0 such that the solution x1(t)M and x2(t)M for sufficiently large t.

    Since rbx1x21+k2x10, Eq (2.2) implies that

    dx2dt=a2x2(1x2k3)+rbx1x2k2+x1d2x2u2x22Bx2Ax22,tnTx2(nT+)=(1ω)x2(nT),t=nT

    then we obtain

    x2(t)>˜x2(t)ϵ

    for some positive ϵ and large enough t.

    Hence,

    x2(t)>B(1ωeBT)A(1eBT)ϵm1

    for large enough t.

    Hence, the remaining proof is the system has a lower bound. That is, there exists a positive constant m2 such that x(t)>m2. To obtain the result, we let

    ˆM1=a1(1m3k1)d1u1m3,

    for some m3>0.

    Next, there are two steps as follows:

    Step 1. Prove by contradiction that there is t1 such that x1(t1)m3. Suppose that x1(t)<m3 for all t>0. From Eqs (2.2) and (2.4), we get

    dx2dt=a2x2(1x2k3)+rbx1x2k2+x1d2x2u2x22,tnTa2x2(1x2k3)+M3x2d2x2u2x22=(B+M3)x2Ax22,x2(t+)=(1ω)x2(t),t=nT.

    Let us consider the comparison system

    dYdt=(B+M3)YAY2,tnT (3.15)
    Y(t+)=(1ω)Y(t),t=nT (3.16)

    and

    Y(0+)=x2(0+). (3.17)

    Hence,

    1˜Y(t)=A(B+M3)+ωAe(B+M3)(tnT)(B+M3)(1ωe(B+M3)T),t(nT,(n+1)T] (3.18)

    is a positive periodic solution of system (3.15)–(3.17) with

    1Y(0+)=A(B+M3)+ωA(B+M3)(1ωe(B+M3)T)>0.

    The system (3.15)–(3.17) has a positive solution

    1Y(t)=(ωA(B+M3)(1ωe(B+M3)T)+1Y(0+)A(B+M3))e(B+M3)t+1˜Y(t), (3.19)

    with t(nT,(n+1)T] and 1Y(t)1˜Y(t) as t, where

    1˜Y(t)=ωAe(B+M3)(tnT)(B+M3)(1ωe(B+M3)T)+A(B+M3).

    By the comparison theorem in [14], we obtain that

    x2(t)Y(t).

    Now, we consider (2.1)

    dx1dt=a1x1(1x1k1)bx1x2k2+x1d1x1u1x21(a1(1m3k1)bx2k2d1u1m3)x1=(^M1bx2k2)x1.

    Since x2(t)Y(t), there is a T>0 such that,

    x2(t)Y(t)<˜Y(t)+ϵ1,tnT,tT

    for a sufficiently small ϵ1>0.

    Therefore,

    dx1dt>(ˆM1bk2(˜Y(t)+ϵ1))x1, (3.20)

    for tnT,tT and

    x1(t+)=(1γ)x1(t), (3.21)

    for t=nT,tT.

    Letting NZ+ and NTT, and integrating over (nT,(n+1)T],nN, we get

    x1((n+1)T)x1(nT)(1γ)exp((n+1)TnT(ˆM1bk2(˜Y(t)+ϵ1))dt)=x1(nT)(1γ)exp((ˆM1bk2ϵ1b(B+M3)k2A)T+bk2Aln(11ω)),=x1(nT)η

    where

    η(1γ)exp((ˆM1bk2ϵ1b(B+M3)k2A)T+bk2Aln(11ω)).

    Consider

    lnη=ln(1γ)+(ˆM1bk2ϵ1b(B+M3)k2A)T+bk2Aln(11ω).

    For sufficiently small ϵ1>0,

    lnηln(11γ)+(ˆM1b(B+M3)k2A)T+bk2Aln(11ω).

    Since ^M1<a1d1 and (3.11) is satisfied, a small positive m3 is chosen so that lnη>0.

    We get

    η(1γ)exp((ˆM1bk2ϵ1b(B+M3)k2A)T+bk2Aln(11ω))>1. (3.22)

    We observe that x1((n+k)T)x1(nT)ηk as k which contradicts the boundedness of x1(t). Therefore, there exists t1>0 such that x1(t1)m3.

    Step 2. The proof is completed if x1(t)m3 for all t>t1. Otherwise, x1(t)<m3 for some t>t1. Setting t=inft>t1{x1(t)<m3}. There are two cases as follows:

    Case 1: t=n1T for some n1Z+. That is x1(t)m3 for t(t1,t] and x1(t)=m3 by continuity of the solution x1(t).

    Since x1(t)<M and m1<x2(t)<M for some positive M and m1 with sufficiently large t, we can choose ˉM>0 and ˉm1>0 so that

    x1(t)<ˉMandˉm1<x2(t)<ˉM

    and

    ^M1<bk2ˉM, (3.23)

    such that

    1ˉm1>|1x2(t+)A(B+M3)ωA(B+M3)(1ωe(B+M3)T)|ω. (3.24)

    Then, we choose n2,n3Z+ such that

    n2T>1(B+M3)ln(1ˉm1+ωϵ1) (3.25)

    and

    (1γ)n2exp((n2+1)η1T)ηn3>1, (3.26)

    where

    η1^M1bk2ˉM<0.

    Define T=n2T+n3T. There exists t2(t,t+T] so that x1(t2)>m3.

    Otherwise, considering Eq (3.19) with

    1Y(t+)=1x2(t+),

    we obtain

    1Y(t)=(ωA(B+M3)(1ωe(B+M3)T)+1Y(t+)A(B+M3))e(B+M3)(tt)+1˜Y(t)

    for t(nT,(n+1)T] where n1nn1+n2+n3.

    For n2TttT, we have

    |1Y(t)1˜Y(t)|=|ωA(B+M3)(1ωe(B+M3)T)+1Y(t+)A(B+M3)|e(B+M3)(tt)=|ωA(B+M3)(1ωe(B+M3)T)+1x2(t+)A(B+M3)|e(B+M3)(tt)<(1ˉm1+ω)e(B+M3)(tt)<(1ˉm1+ω)e(B+M3)n2T<ϵ1.

    Since the condition (3.14), we get

    |Y(t)˜Y(t)|<|Y(t)˜Y(t)||Y(t)˜Y(t)|=|1Y(t)1˜Y(t)|<ϵ1.

    Then,

    x2(t)Y(t)<˜Y(t)+ϵ1.

    According to Step 1, we obtain

    x1(t+T)=x1(n1T+n2T+n3T)x1(t+n2T)ηn3.

    From Eq (2.1), we have

    dx1dt=a1x1(1x1k1)bx1x2k2+x1d1x1u1x21(a1(1m3k1)bx2k2d1u1m3)x1=(^M1bx2k2)x1(^M1bk2ˉM)x1=η1x1,tnTx1(t+)=(1γ)x1(t),t=nT. (3.27)

    Integrating inequality (3.27) over [t,t+n2T], we have

    x1(t+n2T)x1(t)(1γ)n2exp(n1T+n2Tn1Tη1dt)m3(1γ)n2exp(n2η1T)m3(1γ)n2exp((n2+1)η1T),

    hence,

    x1(t+T)x1(t+n2T)ηn3m3(1γ)n2exp((n2+1)η1T)ηn3>m3.

    It is in contradiction to the definition of m3. Therefore, there exists t2(t,t+T] so that x1(t2)>m3.

    Now, we define ˜t=inft>t{x1(t)>m3}. This means that, x1(t)<m3 for t(t,˜t) and x1(˜t)=m3 by the continuity of x1(t). Then, we choose pZ+ so that pn2+n3 and t+pT˜t, and suppose t(t+(p1)T,t+pT]. By inequality (3.27), we get

    x1(t)x1(t+)(1γ)p1exp((p1)η1T)exp(η1(t(t+(p1)T)))=x1(t)(1γ)pexp((p1)η1T)exp(η1(t(t+(p1)T)))=m3(1γ)pexp(η1(tt))m3(1γ)n2+n3exp(η1pT)m3(1γ)n2+n3exp((n2+n3)η1T).

    Since η1<0 and pn2+n3.

    Let

    ˉm2=m3(1γ)n2+n3exp((n2+n3)η1T).

    Thus, x1(t)ˉm2 for t(t,˜t). Similarly, we use

    ˜t instead of t. Then, we will obtain x1(t)ˉm2 for all sufficiently large t.

    Case 2: tnT for all nZ+. That is x1(t)m3 for t[t1,t) and x1(t)=m3. We assume that t(ˉn1T,(ˉn1+1)T), for some ˉn1Z+. We can consider this in two subcases.

    Case 2.1: x1(t)m3 for all t(t,(ˉn1+1)T]. Suppose that there is t2[(ˉn1+1)T,(ˉn1+1)T+T] so that x1(t2)>m3. Otherwise, considering Eq (3.19) with

    1Y((ˉn1+1)T+)=1x2((ˉn1+1)T+).

    For t(nT,(n+1)T], ˉn1+1nˉn1+1+n2+n3, we obtain

    1Y(t)=(1Y((ˉn1+1)T+)A(B+M3)ωA(B+M3)(1ωe(B+M3)T))e(B+M3)(t(ˉn1+1)T)+1˜Y(t).

    In a similar way to Case 1, for n2Ttt, we get

    |Y(t)˜Y(t)|<ϵ1.

    Thus,

    x2(t)Y(t)<˜Y(t)+ϵ1.

    Since n2T(ˉn1+1+n2)Tt, we get

    x1((ˉn1+1+n2)T)x1(t)(1γ)n2exp(η1((ˉn1+1+n2)Tt))m3(1γ)n2exp(η1((ˉn1+1+n2)Tˉn1T))m3(1γ)n2exp((n2+1)η1T).

    Then,

    x1((ˉn1+1+n2+n3)T)x1((ˉn1+1+n2)T)ηn3m3(1γ)n2exp((n2+1)η1T)ηn3>m3.

    It is in contradiction to the definition of m3. Thus, there exists t2[(ˉn1+1)T,(ˉn1+1)T+T] so that x1(t2)>m3.

    Now, we define ˉt=inft>t{x1(t)>m3}. Thus, x1(t)m3 for t[t,ˉt), and x1(ˉt)=m3. We choose pZ+ such that pn2+n3+1 and suppose t(ˉn1T+(p1)T,ˉn1T+pT]. From inequality (3.27), we get

    x1(t)x1((ˉn1T+(p1)T)+)exp(η1(t(ˉn1T+(p1)T)))=x1(ˉn1T+(p1)T)(1γ)exp(η1(t(ˉn1T+(p1)T)))x1(t)(1γ)p1exp(η1(tt))m3(1γ)p1exp(η1(tt)).

    Since η1<0 and ttpT. Then,

    x1(t)m3(1γ)n2+n3exp((n2+n3+1)η1T).

    Let

    m2=m3(1γ)n2+n3exp((n2+n3+1)η1T).

    Therefore, x1(t)m2 for t(t,ˉt). We do the same way by using ˉt instead of t. Then, we will obtain x1(t)m2 for all sufficiently large t.

    Case 2.2: There exists t(t,(ˉn1+1)T] so that x1(t)>m3. Define t_=inft>t{x1(t)>m3}. Hence, x1(t)<m3 for t[t,t_), and x1(t_)=m3. For t[t,t_), inequality (3.27) holds, we get

    x1(t)x1(t)exp(ttη1dt)=m3exp(η1(tt))m3exp(η1T)>m2,

    since t<ˉn1T+T<t+T. For t>t_, we can do the same way since x1(t_)m3. Since m2<ˉm2<m3, we can conclude that x1(t)m2 for tt1. The proof is completed.

    Now, we carry out the conditions to guarantee the positive periodic solution of the system (2.1)–(2.4) near the periodic solution (0,˜x2). For more convenience, we change the variables, and then the new system is shown as follows:

    dx1dt=a2x1(1x1k3)+rbx1x2k2+x2d2x1u2x21, (3.28)
    dx2dt=a1x2(1x2k1)bx1x2k2+x2d1x2u1x22, (3.29)

    for tnT with

    x1(nt+)=(1ω)x1(t),t=nT, (3.30)
    x2(nt+)=(1γ)x2(t),t=nT. (3.31)

    Let

    F1(x1,x2)=a2x1(1x1k3)+rbx1x2k2+x2d2x1u2x21,F2(x1,x2)=a1x2(1x2k1)bx1x2k2+x2d1x2u1x22.

    According to Lakmeche and Arini [13],

    Θ1(x1,x2)=(1ω)x1,Θ2(x1,x2)=(1γ)x2,ζ(t)=(˜x2(t),0)T,X0=(˜x2(τ0),0)T,τ0=Tmax,

    and

    Φ1(τ0,X0)τ=˜x2(τ0,X0)t=ωAexp(Bτ0)˜x22(τ0,X0)1ωexp(Bτ0)>0,Φ1(τ0,X0)x1=exp(τ00F1(ζ(s))x1ds)>11ω>0,Φ1(τ0,X0)x2=τ00[exp(τ0υF1ζ(s)x1ds)F1(ζ(υ))x2exp(υ0F2(ζ(s))x2ds)]dυ=τ00[exp(τ0υ(B2A˜x2(s))ds)rb˜x2(υ)k2exp(υ0(a1d1b˜x2(s)k2)ds)]dυ,Φ2(τ0,X0)x2=exp(τ00F2(ζ(s))x2ds)=exp(τ00(a1d1b˜x2(s)k2)ds),2Φ2(τ0,X0)x1x2=τ00[exp(τ0υF2(ζ(s))x2ds)2F2(ζ(υ))x1x2exp(υ0F2(ζ(s))x2ds)]dυ=bτ0k2(1γ)<0,
    2Φ2(τ0,X0)x22=τ00exp(τ0υF2(ζ(s))x2ds)2F2(ζ(υ))x22exp(υ0F2(ζ(s))x2ds)dυ+τ00[exp(τ0υF2(ζ(s))x2ds)2F2(ζ(υ))x1x2]×[υ0exp(υθF1(ζ(s))x1ds)F1(ζ(θ))x2exp(θ0F2(ζ(s))x2ds)dθ]dυ=τ00(2b˜x2(υ)k222a1k12u1)exp(τ00(a1d1b˜x2(s)k2)ds)dυbk2τ00[exp(τ0υ(a1d1b˜x2(s)k2)ds)]×[υ0exp(υθ(B2A˜x2(s))ds)rb˜x2(θ)k2exp(θ0(a1d1b˜x2(s)k2)ds)dθ]dυ,
    2Φ2(τ0,X0)x2τ=F2(ζ(τ0))x2exp(τ00F2(ζ(s))x2ds)=(a1d1b˜x2(τ0)k2)exp(τ00(a1d1b˜x2(s)k2)ds)=11γ(a1d1bB(1ωexp(Bτ0))β5),

    where

    β5=k2ωAexp(Bτ0)+k2A(1ωexp(Bτ0)).

    Now, we can compute

    d0=1(Θ2x2Φ2x2)(τ0,X0)=1(1γ)exp(τ00(a1d1b˜x2(s)k2)ds),

    where τ0 is the root of d0=0. Note that d0>0 if T<Tmax and d0<0 if T>Tmax.

    a0=1(Θ1x1Φ1x1)(τ0,X0)=1(1ω)exp(τ00(B2A˜x2(s))ds).

    Note that a0>0 if T>Tmin.

    b0=Θ1x1Φ1(τ0,X0)x2=(1ω)τ00exp(τ0υ(B2A˜x2(s))ds)rb˜x2(υ)k2exp(υ0(a1d1rb˜x2(s)k2)ds)dυ<0,G=(a1d1)+bB(1ωexp(Bτ0)β5)+bτ0(1ω)ωexp(Bτ0)k2(1((1ω)exp(Bτ0)+11ω))×B2(1ωexp(Bτ0))A[ωexp(Bτ0)+(1ωexp(Bτ0))]2,H=2(1γ)b0a02Φ2x1x2(1γ)2Φ2x22.

    Note that G<0 if

    a1k2(a2k3+u2)>b(a2d2), (3.32)

    and H>0 if

    k22(a1k1+u1)(a2k3+u2)>b(a2d2). (3.33)

    Thus, GH<0, and by Lakmeche and Arini [13], we obtain the following theorem.

    Theorem 3.9. If all conditions (3.2), (3.6), (3.11), (3.12), (3.14), (3.32), (3.33) and T>Tmax>Tmin hold, then the system (3.28)(3.31) has a positive periodic solution which is supercritical.

    In this section, the numerical results of the system (2.1)–(2.4) are carried out by using ode15 package in MATLAB to confirm the analysis of solutions.

    The numerical simulations of the (2.1)–(2.4) are computed by using the parameters and initial conditions given in Table 1.

    Table 1.  Parameter values.
    parameter value
    a1 20
    a2 20 [18]
    b 0.1
    d1 0.2
    d2 0.4
    k1 0.2
    k2 0.6
    k3 0.3
    r 0.5
    u1 0.1
    u2 0.1
    x1(0) 10
    x2(0) 10

     | Show Table
    DownLoad: CSV

    The remaining parameters γ=0.9,ω=0.1,T=0.1 are used to simulate the solutions as shown in Figures 1. All parameters are satisfied the conditions in Theorem 3.6. The trend of solution is close to a limit cycle (0,˜x2) as proved.

    Figure 1.  Simulation results of system (2.1)–(2.4). The parametric values are chosen to satisfy the conditions in Theorem 3.6. (1a) The phase-portrait of (x1,x2). (1b) The population time series of small fishes (x1) tending to zero. (1c) The population time series of short mackerel (x2) exhibiting positive pulsation. The solution goes toward the periodic solution (0,˜x2) as time passess.

    The initial situation starts with 10 units in both of population density of small fishes x1(0) and short mackerel x2(0). After that, the population of small fishes continues to decrease and tends to zero due to the short period and high quantity of fisheries. However, the population of shot mackerel decreases in the beginning then it tends to a closed orbit between 0.25930.2881 because of the low rate of toxic death and high capacity of hunting with the same period of fisheries.

    The computer simulations of the system (2.1)–(2.4) with setting parameters in Table 1 and γ=0.5,ω=0.2,T=0.5 are shown in Figure 2. For this case, we have that all parameters are satisfied the conditions in Theorem 3.8. The solution is permanent as proved.

    Figure 2.  Simulation results of system (2.1)–(2.4). The parametric values are chosen to satisfy the conditions in Theorem 3.8. (2a) The phase-portrait of (x1,x2). (2b), (2c) The population time series of small fishes (x1) and short mackerel (x2) showing boundedness. The solution of the system is permanent.

    The initial situation starts with 10 units in both of population density of small fishes x1(0) and short mackerel x2(0). After that, both small fishes and shot mackerel decrease until tending to a range of 0.09870.1974 and 0.23470.2934, respectively. The fisherman catches enough of them for the economy and they remain alive in the system. The long period of fisheries, low-frequency fisheries, and the appropriate number of fishing are the most of factors in persistence.

    The computer simulations of the system (2.1)–(2.4) with the parametric values γ=0.7,ω=0.3,T=1.5 and the remaining parameters as in Table 1 are shown in Figure 3. All parameters in this case are satisfied the conditions in Theorem 3.9. The system has a positive periodic solution as proved.

    Figure 3.  Simulation results of system (2.1)–(2.4). The parametric values are chosen to satisfy the conditions in Theorem 3.9. (3a) The phase-portrait of (x1,x2). (3b), (3c) The population time series of small fishes (x1) and short mackerel (x2) exhibiting positive oscillation. The system has a positive periodic solution.

    The initial situation start with 10 units both of population density of small fishes x1(0) and short mackerel x2(0). Then both small fishes and shot mackerel decrease until tending to oscillatory in a narrow range of 0.0592–0.1974 and 0.2054–0.2934, respectively. The decreased population of small fishes and shot mackerel occurs when the period of fisheries starts while the population of them back hits the peak when fisherman do not allow to fishing like a periodic behavior. The suitable amount and period of fisheries like this case to prevent the extinction of small fishes and short mackerel and to prevent the damage of economic are expected situation.

    The computer simulations of the system (2.1)–(2.4) with the parametric values in Table 1 and γ=0.5,ω=0.2 which focused on changes in the period of impulsive fisheries (T) and the negative effect of fisheries on the density of short mackerel population (ω) with γ=0.1,T=0.2 are shown in Figure 4 and Figure 5 respectively. The results indicated that the densities of the short mackerel were in periodic fashions. Moreover, the different values of T and ω provided the different highest densities of x2(t).

    Figure 4.  Simulation results of short mackerel density focused on changes in the period of impulsive fisheries (T).
    Figure 5.  Simulation results of short mackerel density focused on changes in the negative effect of fisheries on the density of short mackerel population (ω).

    We propose the modification mathematical model to forecast the population density dynamic of Indo-Pacific mackerel (Rastrelliger brachysoma) or short mackerel. The proposed model is utilized to control the population of short mackerel by considering the decrease population affected by catching, toxic, and natural death. The suitable period T and the quantity affecting the decreasing rate of small fishes population γ and the decreasing rate of short mackerel population ω are essential things to maintain short mackerel population and small fish population without extinction. The numerical results show the periodic behavior of the density population. Moreover, there are enough short mackerel for fishermen and humans for a long time.

    This research project was financially supported by Thailand Science Research and Innovation (TSRI) 2021.

    All authors declare no conflicts of interest in this paper.



    [1] G. Ballinger, X. Liu, Permanence of population growth models with impulsive effects, Math. Comput. Model., 26 (1997), 59–72. doi: 10.1016/s0895-7177(97)00240-9. doi: 10.1016/s0895-7177(97)00240-9
    [2] E. Bergami, S. Pugnalini, M. Vannuccini, L. Manfra, C. Faleri, F. Savorelli, et al., Long-term toxicity of surface-charged polystyrene nanoplastics to marine planktonic species dunaliella tertiolecta and artemia franciscana, Aquat. Toxicol., 189 (2017), 159–169. doi: 10.1016/j.aquatox.2017.06.008. doi: 10.1016/j.aquatox.2017.06.008
    [3] G. Bueno, D. Bureau, J. Skipper-Horton, R. Roubach, F. Mattos, F. Bernal, Mathematical modeling for the management of the carrying capacity of aquaculture enterprises in lakes and reservoirs, Pesq. Agropec. Bras., 52 (2017), 695–706. doi: 10.1590/S0100-204X2017000900001. doi: 10.1590/S0100-204X2017000900001
    [4] B. R. Chavan, A. Yakupitiyage, S. Kumar, Mathematical modeling of drying characteristics of indian mackerel (Rastrilliger kangurta) in solar-biomass hybrid cabinet dryer, Dry. Technol., 26 (2018), 1552–1562. doi: 10.1080/07373930802466872. doi: 10.1080/07373930802466872
    [5] B. Collette, C. Nauen, Fao species catalogue, Vol. 2: Scombrids of the world: An annotated and illustrated catalogue of tunas, mackerels, bonitos and related species known to date, Food and Agriculture Organization of the United Nations (FAO) Fisheries Synopsis, 1983.
    [6] A. C. Dragon, I. Senina, N. T. Hintzen, P. Lehodey, Modelling south pacific jack mackerel spatial population dynamics and fisheries, Fish. Oceanogr., 27 (2018), 97–113. doi: 10.1111/fog.12234. doi: 10.1111/fog.12234
    [7] T. Hallam, R. Lassiter, S. Henson, Modeling fish population dynamics, Nonlinear Anal.: Theory Methods Appl., 40 (2000), 227–250. doi: 10.1016/s0362-546x(00)85013-0. doi: 10.1016/s0362-546x(00)85013-0
    [8] Y. Hashiguchi, M. R. Zakaria, T. Maeda, M. Z. M. Yusoff, M. A. Hassan, Y. Shirai, Toxicity identification and evaluation of palm oil mill effluent and its effects on the planktonic crustacean daphnia magna, Sci. Total Environ., 710 (2020), 136277. doi: 10.1016/j.scitotenv.2019.136277. doi: 10.1016/j.scitotenv.2019.136277
    [9] M. Hjorth, I. Dahllöf, V. E. Forbes, Effects on the function of three trophic levels in marine plankton communities under stress from the antifouling compound zinc pyrithione, Aquat. Toxicol., 77 (2006), 105–115. doi: 10.1016/j.aquatox.2005.11.003. doi: 10.1016/j.aquatox.2005.11.003
    [10] T. Jansen, H. Gislason, Population structure of Atlantic Mackerel (Scomber scombrus), PloS One, 8 (2018), e64744. doi: 10.1371/journal.pone.0064744. doi: 10.1371/journal.pone.0064744
    [11] R. Khatun, H. Biswas, Mathematical modeling applied to renewable fishery management, Math. Model. Eng. Probl., 6 (2019), 121–128. doi: 10.18280/mmep.060116. doi: 10.18280/mmep.060116
    [12] S. Kongseng, R. Phoonsawat, A. Swatdipong, Individual assignment and mixed-stock analysis of short mackerel (Rastrelliger brachysoma) in the inner and eastern gulf of Thailand: Contrast migratory behavior among the fishery stocks, Fish. Res., 221 (2020), 105372. doi: 10.1016/j.fishres.2019.105372. doi: 10.1016/j.fishres.2019.105372
    [13] A. Lakmeche, O. Arini, Bifurcation of non-trivial periodic solutions of impulsive differential equations arising chemotherapeutic treatment, Dynam. Contin. Discrete Impuls., 7 (2000), 265–287.
    [14] V. Lakshmikantham, D. Bainov, P. Simeonov, Theory of impulsive differential equations, World Scientific, 1989.
    [15] D. Liang, G. Y. Sun, W. Q. Wang, Second-order characteristic schemes in time and age for a nonlinear age-structured population model, J. Comput. Appl. Math., 235 (2011), 3841–3858. doi: 10.1016/j.cam.2011.01.031. doi: 10.1016/j.cam.2011.01.031
    [16] B. Liu, Y. Zhi, L. S. Chen, The dynamics of a predator-prey model with ivlev's functional response concerning integrated pest management, Acta Math. Applicatae Sin., 20 (2004), 133–146. doi: 10.1007/s10255-004-0156-0. doi: 10.1007/s10255-004-0156-0
    [17] N. Niamaimandi, F. Kaymaram, J. P. Hoolihan, G. H. Mohammadi, S. M. R. Fatemi, Population dynamics parameters of narrow-barred spanish mackerel, Scomberomorus commerson (lacèpéde, 1800), from commercial catch in the northern Persian Gulf, Glob. Ecol. Conserv., 4 (2015), 666–672. doi: 10.1016/j.gecco.2015.10.012. doi: 10.1016/j.gecco.2015.10.012
    [18] Fisheries statistics of thailand 2018, Fisheries Development Policy and Planning Division, Department of Fisheries, Ministry of Agriculture and Cooperatives, 2020. Available from: https://www4.fisheries.go.th/local/file_document/20210520115148_new.pdf.
    [19] R. P. Kaur, A. Sharma, A. K. Sharma, The impact of additional food on plankton dynamics in the absence andpresence of toxicity, Biosystems, 202 (2021), 104359. doi: 10.1016/j.biosystems.2021.104359. doi: 10.1016/j.biosystems.2021.104359
    [20] D. Randall, T. Tsui, Ammonia toxicity in fish, Mar. Pollut. Bull., 45 (2002), 17–23. doi: 10.1016/s0025-326x(02)00227-8.
    [21] C. Raymond, A. Hugo, M. Kungaro, Modeling dynamics of prey-predator fishery model with harvesting: A bioeconomic model, J. Appl. Math., 2019 (2019), 2601648. doi: 10.1155/2019/2601648. doi: 10.1155/2019/2601648
  • This article has been cited by:

    1. Attaullah Attaullah, Adil Khurshaid, Zeeshan Zeeshan, Sultan Alyobi, Mansour F. Yassen, Din Prathumwan, Computational Framework of the SVIR Epidemic Model with a Non-Linear Saturation Incidence Rate, 2022, 11, 2075-1680, 651, 10.3390/axioms11110651
    2. Gang Wang, Ming Yi, Zaiyun Zhang, Global Dynamics of a Predator–Prey System with Variation Multiple Pulse Intervention Effects, 2025, 13, 2227-7390, 1597, 10.3390/math13101597
  • Reader Comments
  • © 2022 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(3014) PDF downloads(293) Cited by(2)

Figures and Tables

Figures(5)  /  Tables(1)

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog