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An eco-epidemic model for assessing the application of integrated pest management strategies


  • Mathematical models have become indispensable tools for analyzing pest control strategies. However, in the realm of pest control studies, the consideration of a plant population being affected by a model that incorporates pests, natural enemies and disease in the pest population has been relatively limited. Therefore, this paper aims to formulate and investigate a hybrid impulsive eco-epidemic model that incorporates disease in the pest population. Initially, we examine the existence and stability of the pest-eradication periodic solution. Subsequently, to explore the impact of chemical and biological control methods, we propose an updated eco-epidemic model that incorporates varying frequencies of pesticide sprays and the release of both infected pests and natural enemies for pest control. We establish threshold values for the susceptible pest eradication periodic solution under different scenarios, illustrating the global attractiveness of this solution. Finally, we discuss the obtained results and suggest potential avenues for future research in this field.

    Citation: Wenjie Qin, Yue Xia, Yi Yang. An eco-epidemic model for assessing the application of integrated pest management strategies[J]. Mathematical Biosciences and Engineering, 2023, 20(9): 16506-16527. doi: 10.3934/mbe.2023736

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  • Mathematical models have become indispensable tools for analyzing pest control strategies. However, in the realm of pest control studies, the consideration of a plant population being affected by a model that incorporates pests, natural enemies and disease in the pest population has been relatively limited. Therefore, this paper aims to formulate and investigate a hybrid impulsive eco-epidemic model that incorporates disease in the pest population. Initially, we examine the existence and stability of the pest-eradication periodic solution. Subsequently, to explore the impact of chemical and biological control methods, we propose an updated eco-epidemic model that incorporates varying frequencies of pesticide sprays and the release of both infected pests and natural enemies for pest control. We establish threshold values for the susceptible pest eradication periodic solution under different scenarios, illustrating the global attractiveness of this solution. Finally, we discuss the obtained results and suggest potential avenues for future research in this field.



    Controlling insects and other arthropods plays a crucial role in agriculture due to the potential ecological and economic consequences of pest outbreaks [1,2,3,4,5]. Integrated pest management (IPM) offers a highly effective and safer approach by employing a combination of pest control techniques including biological, cultural and chemical methods. This strategy involves carefully selecting and implementing tactics that are specifically tailored to the unique characteristics of the cropping systems, pest complexes and biological environments involved [6,7,8,9].

    The main objective of IPM is to keep pest populations below the economic injury level (EIL) [10] rather than eradicating them entirely. The selection of suitable tactics is based on the pest densities reaching the economic threshold (ET) [11], which minimizes the negative impact of insecticides on non-target pests and helps maintain environmental quality. The effectiveness of IPM has been demonstrated in various applications [12,13,14,15].

    Biological control, employing microbial pathogens that target pest species, is a crucial pest control technique that has received significant attention in both experimental and theoretical studies. Drawing inspiration from the classical SIR (susceptible-infected-recovered) model introduced by Kermack and McKendrick [16], the pest population is divided into susceptible and infected pests. As a result, epidemiological models have attracted substantial interest from researchers in the field [17,18,19,20,21,22].

    However, conventional ecological models primarily focus on two-species interactions, with many studies emphasizing predator-prey dynamics using Lotka-Volterra type functional responses. Limited attention has been given to IPM models involving a three-species food web. Gakkhar and Naji [23] investigated the dynamics of a tri-trophic food web comprising a generalist-specialist-prey system, incorporating a modified Holling type II functional response. Apreutesei [24] explored the necessary optimality conditions for a tri-trophic food web system. In 2013, Priyadarshi and Gakkhar [25] analyzed the dynamics of a tri-trophic food web system that included a Leslie-Gower type generalist predator. In 2016, Liang et al. [26] proposed an eco-epidemiological model for a plant-pest-predator system, considering the impulsive effect. These studies highlight the importance of considering three-species interactions in IPM models and their ecological implications.

    To achieve effective pest control, it is vital to have a thorough understanding of the ecological dynamics within the cropping system, encompassing the pests, their predators, the environment, and their intricate interrelationships. However, certain control strategies, such as pesticide spraying, natural enemy releases and infected pest releases are implemented instantaneously or over relatively short periods. Hence, determining the optimal timing and frequency of these actions becomes crucial. In this study, we employ impulsive differential equations to model human interventions and develop a novel mathematical model that captures the dynamics of these actions and their impact on pest control.

    The paper is organized as follows. In the following section, we will present a novel three-species mathematical model along with its main biological assumptions. Additionally, we will explore the stability of the susceptible pest-eradication periodic solution in Section 3. Section 4 presents an updated eco-epidemic model that incorporates various frequencies of pesticide sprays, releases of infected pests and releases of natural enemies. The threshold value for achieving the susceptible pest-eradication periodic solution is provided for different scenarios, showcasing the global attractivity of this solution. Subsequently, a concise discussion of the obtained results is presented, followed by potential directions for future research.

    Recently, there has been a growing interest in investigating IPM models using a three-species food web, which includes a predator (the natural enemy of the pest), the pest itself and a basal producer (a renewable biotic resource such as plants or vegetation). Several papers have delved into this topic [23,24,25,26,27,28]. In this context, let R represent the state of the basal producer, while P and N denote the densities of the pest and natural enemy, respectively. In 2006, Apreutesei [24] investigated the following pest-natural enemy-plant model

    {P(t)=P(t)[αPβNN(t)+γRR(t)],N(t)=N(t)[αN+βPP(t)],R(t)=R(t)[αRβRP(t)], (2.1)

    where αP is the intrinsic growth rate for the pest, αN is the death rate for the natural enemy and αR is the growth rate for the plant. βN describes the search rate of the natural enemy, βP denotes the efficiency rate with which captured pests are converted to the new natural enemy, βR describes the search rate of the pest and γR denotes the efficiency rate. Assume that all the coefficients are positive constants.

    A novel eco-epidemiological model is proposed, which incorporates the utilization of microbial control through pathogenic agents and the release of natural enemies in integrated pest management. Building upon the research conducted by Xiao et al. [17,18,19] and Apreutesei [24], the pest species P is classified into two categories: susceptible pests and infected pests, with the introduction of a pest pathogen acting as a biotic insecticide within the pest population. Additionally, the following model takes into account the presence of a food source for the pests

    {S(t)=rSS(t)[1S(t)+I(t)K]+μSS(t)R(t)aR+R2(t)βS(t)I(t)S(t)N(t)aS+S2(t),I(t)=βS(t)I(t)δII(t),N(t)=μNS(t)N(t)aS+S2(t)δNN(t),R(t)=rRR(t)S(t)R(t)aR+R2(t), (2.2)

    the parameter definitions for model (2.2) are summarized in Table 1. Specifically, in this model, R(t) represents a basal producer, which corresponds to a renewable biotic resource such as plants or vegetation [26]. Additionally, the non-monotonic (sigmoidal) saturation function is defined as follows

    Ψ(X)XaX+X2,X=S(t),R(t).
    Table 1.  Parameter definitions for models (2.2) and (2.3).
    Parameter Definition Parameter Definition
    S(t) density of the susceptible pest I(t) density of the infected pest
    N(t) density of the natural enemy population R(t) renewable biotic resource [26]
    rS intrinsic growth rate for S(t) {rR intrinsic growth rate for R(t)
    K carrying capacity for S(t) {δI death rate of I(t)
    δN death rate of N(t) β transmission coefficient
    T pulse period μS efficiency rate for S(t)
    μN efficiency rate for N(t) aS half-saturation constant
    pS killing rate for S(t) as pesticide is applied aR half-saturation constant
    pN killing rate for N(t) as pesticide is applied pI killing rate for I(t) as pesticide is applied
    qI proportional increase rate of I(t) θI release amount of I(t)
    qN proportional increase rate of N(t) θN release amount of N(t)
    qR proportional increase rate of R(t) θR release amount of R(t)

     | Show Table
    DownLoad: CSV

    This function is a simplified form of the Monod-Haldane or Holling IV function proposed by Sokol and Howell [29] and it describes the collective defense behavior of the prey population when their density is relatively high. Here, aX>0 denotes the half-saturation constant of species X. It is important to note that only the susceptible pests have the ability to feed on the plants with a Holling type-IV response function, while the infected pests are assumed to be too weak to hunt for food.

    Building upon the pest-natural enemy model and the implementation of IPM strategies, the combined approach of periodic pesticide spraying, release of infected pests and release of natural enemies is employed to effectively control the pest population. The reformulation of model (2.2) is as follows

    {S(t)=rSS(t)[1S(t)+I(t)K]+μSS(t)R(t)aR+R2(t)βS(t)I(t)S(t)N(t)aS+S2(t),I(t)=βS(t)I(t)δII(t),N(t)=μNS(t)N(t)aS+S2(t)δNN(t),R(t)=rRR(t)S(t)R(t)aR+R2(t),}tnT,S(t+)=(1pS)S(t),I(t+)=(1+qI)I(t)+θI,N(t+)=(1+qN)N(t)+θN,R(t+)=(1+qR)R(t)+θR,}t=nT. (2.3)

    The parameter definitions for model (2.3) are summarized in Table 1. It is important to emphasize here that model (2.3) incorporates the impulsive effect at fixed time intervals T, representing the simultaneous application of periodic pesticide sprays, release of infected pests and release of natural enemies to control the pest population. At time points t=nT, the susceptible pest population experiences an instantaneous killing rate pS due to pesticide spraying. Importantly, following pesticide spraying, the susceptible pests become weakened and more susceptible to predation by their natural enemies.

    Since it is well-known that the infective pest does not cause harm to the plant, our main objective in this section is to examine the stability of the periodic solution for eradicating the susceptible pest and establish the conditions for its global attractivity.

    In the following, we investigate the existence and stability of of the susceptible pest-eradication solution, denoted as S(t)0 for all t0. We derive three subsystems from model (2.3):

    {I(t)=δII(t),tnT,I(t+)=(1+qI)I(t)+θI,t=nT, (3.1)
    {N(t)=δNN(t),tnT,N(t+)=(1+qN)N(t)+θN,t=nT, (3.2)

    and

    {R(t)=rRR(t),tnT,R(t+)=(1+qR)R(t)+θR,t=nT. (3.3)

    It follows from the first equation of model (3.1) that I(t)=exp(δI(tnT))I(nT+) for t(nT,(n+1)T]. Consequently, we can conclude that I((n+1)T)=exp(δIT)I(nT+).

    Now, combining the second equation of model (3.1) with the previously mentioned equations results in the following

    I((n+1)T+)=(1+qI)exp(δIT)I(nT+)+θI.

    By denoting I((n+1)T+) as I(n+1), we can rewrite the above equation as the following difference equation

    I(n+1)=F(I(n))(1+qI)exp(δIT)I(nT+)+θI. (3.4)

    Equation (3.4) represents the stroboscopic map of model (3.1). It captures the relationship between the density of infected pests at two consecutive pulse points. Specifically, the presence of a positive steady state in Eq (3.4) indicates the existence of a positive periodic solution in model (3.1). Thus, our initial investigation focuses on determining the positive steady state of the stroboscopic map (3.4). The derivative of F(I(n)) with respect to I(n) is

    F(I(n))=(1+qI)exp(δIT).

    According to the stability theory of differential equations, it is necessary to ensure that the condition |F(I(n))|<1 holds true, which is equivalent to the inequality

    λI=(1+qI)exp(δIT)<1.

    Furthermore, we continue to investigate the non-negative fixed point of the stroboscopic map (3.4). For simplicity, we denote the fixed point as ˜I. It can be deduced from Eq (3.4) that ˜I=(1+qI)exp(δT)˜I+RI. This implies that the stroboscopic map (3.4) possesses a single non-negative fixed point, given by

    ˜I=θI1(1+qI)exp(δIT).

    Analogously, we can obtain the non-negative fixed points of the corresponding stroboscopic map for subsystems (3.2) and (3.3)

    ˜N=θN1(1+qN)exp(δNT),˜R=θR1(1+qR)exp(rRT),

    given that

    λN=(1+qN)exp(δNT)<1,λR=(1qR)exp(rRT)<1

    for t(nT,(n+1)T], respectively. Hence, we can conclude the following result.

    Lemma 3.1. Model (3.1) exists a positive periodic solution I. Furthermore, for every positive solution I(t) of model (3.1), it holds that limt+|I(t)I(t)|=0. Here, I(t) is defined as I(t)=exp(δI(tnT))˜I, where

    ˜I=θI1(1+qI)exp(δIT)

    for t(nT,(n+1)T) and nZ.

    Similarly, we can deduce that

    N(t)=exp(δN(tnT))˜N=θNexp(δN(tnT))1(1+qN)exp(δNT)

    and

    R(t)=exp(rR(tnT))˜R=θRexp(rR(tnT))1(1+qR)exp(rRT)

    for all nZ.

    In order to analyze the global asymptotic stability of the periodic solution (0,I(t),N(t),R(t)) of model (2.3), we establish the following two results.

    Theorem 3.2. If min{λS,λI,λR,λN}<1, then the susceptible pest-eradication periodic solution (0,I(t),N(t),R(t)) of model (2.3) is locally asymptotically stable, where

    λS=(1pS)exp{rS{T+(1+Kβ)[exp(δT)1]˜IKδI+[exp(δNT)1]˜NaSδN}+rSμSaRrR[arctan(˜Rexp(rRT)aR)arctan(˜RaR)]}.

    Theorem 3.3. The periodic solution (0,I(t),N(t),R(t)) of model (2.3) is globally asymptotically stable provided that

    RS=(1pS)exp{rST+β[exp(δIT)1]˜IδI+[exp(δNT)1]˜N(aS+K2)δN+[exp(rST)1]˜RaRrR}<1.

    The proofs for Theorems 3.2 and 3.3 can be found in Appendix A. It is worth noting that in practical pest control, the main objective is to manage the population size of pests within a certain range rather than completely eradicating them. This approach helps maintain the balance of the ecosystem and aligns with the fundamental principles of IPM. Therefore, the pest-eradication periodic solution only exists in theory for the system.

    We now extend model (2.3) by incorporating periodic spraying of pesticides and the release of infected pests and natural enemies at specific fixed time intervals, as suggested by Tang et al. [30]. Consequently, we obtain the following revised model.

    {S(t)=rSS(t)[1S(t)+I(t)K]+μSS(t)R(t)aR+R2(t)βS(t)I(t)S(t)N(t)aS+S2(t),I(t)=βS(t)I(t)δII(t),N(t)=μNS(t)N(t)aS+S2(t)δNN(t),R(t)=rRR(t)S(t)R(t)aR+R2(t),}tτn,tλm,S(t+)=(1pS)S(t),I(t+)=(1pI)I(t),N(t+)=(1pN)N(t),R(t+)=R(t),}t=τn,I(t+)=(1+qI)I(t)+θI,N(t+)=(1+qN)N(t)+θN,R(t+)=R(t)+θR,}t=λm, (4.1)

    We assume that the application of pesticides has an impact on the populations of pests and natural enemies. Some parameters remain the same as in model (2.3), other paramaters see Table 1 for details.

    Due to the implementation of different strategies for insecticide applications and releases of infected pests in model (4.1)[30,31], we need to consider two cases regarding the timing of IPM applications.

    Case 1. Spraying pesticides more frequently than releasing infected pests and natural enemies.

    Case 2. Releases of infected pests and natural enemies more frequent than spraying pesticides.

    To facilitate the analysis, we assume that the infected pests and natural enemies are released periodically, with a period denoted as TN. We define λm+1λm=TN, where mZ represents an integer. Additionally, we have τn+kp=TN+τn.

    Now, we define some variables: Δi=τi+1τi Ehi=(hTN+τi,hTN+τi+1], where i=0,1,2,,kp Δ0=τ1, Δkp=TNτkp, τ0=0, τkp+1=TN h represents a non-negative number. Furthermore, we analyze model (4.1) by dividing it into three subsystems where S(t)=0 as follows

    {I(t)=δII(t),tτn,tλm,I(t+)=(1pI)I(t),t=τn,I(t+)=(1+qI)I(t)+θI,t=λm, (4.2)
    {N(t)=δNN(t),tτn,tλm,N(t+)=(1pN)N(t),t=τn,N(t+)=(1+qN)N(t)+θN,t=λm, (4.3)

    and

    {R(t)=rRR(t),tτn,tλm,R(t+)=R(t),t=τn,R(t+)=R(t)+θR,t=λm. (4.4)

    From the first equation of model (4.2) within the interval Eh0, we can deduce that

    I(t)=I(hT+N)exp[δI(thTN)]

    and

    I(t)=I[(hTN+τi)+]exp[δI(thTNτi)],tEhi,i=1,2,,kp1.

    Furthermore, we get

    I(t)=I[(hTN+τkp)+]exp[δI(thTNτkp)],tEhkp.

    At the moment hTN+τi, where i=1,2,,kp, corresponding to the application of a pesticide, we observe

    I[(hTN+τi)+]=(1pI)iI(hT+N)exp[δI(i1j=0Δj)]

    and

    I[[(h+1)TN]+]=(1+qI)(1pI)kpI(hT+N)exp[δI(kp1j=0Δj)]exp(δIΔkp)+θI.

    Denote I[(hTN)+]=I(h), we can get the following difference equation

    I(h+1)=(1+qI)(1pI)kpexp(δITN)I(h)+θI.

    It is evident that the linear difference equation mentioned above possesses a unique equilibrium

    I1=θI1(1+qI)(1pI)kpexp(δITN).

    This equilibrium is considered stable globally, given that λ1I=(1+qI)(1pI)kpexp(δITN)<1.

    Therefore, model (4.2) has a globally stable periodic solution denoted as ˜IN1(t) and

    ˜IN1(t)={I1exp(δI(thTN)),tEh0,I((τi)+)exp(δI(thTNτi)),tEhi,

    where

    I[(τi)+]=I1(1pI)iexp[δI(i1j=0Δj)],i=1,2,,kp,

    particularly, I[(τ0)+]=I1.

    Analogously, we can obtain a globally stable periodic solution denoted as ˜NN1(t), for model (4.3). This is achieved under the condition that λ1N=(1+qN)(1pN)kpexp(δNTN)<1 and

    ˜NN1(t)={N1exp(δN(thTN)),tEh0,N((τi)+)exp(δN(thTNτi)),tEhi,

    where

    N[(τi)+]=N1(1pN)iexp[δN(i1j=0Δj)],i=1,2,,kp

    and

    N[τ0)+]=N1=θN1(1+qN)(1pN)kpexp(δNTN).

    Model (4.3) has a globally stable periodic solution, denoted as ˜RN1(t), under the condition that λ1R=exp(rRTN)<1 and

    ˜RN1(t)={rSexp(rR(thTN)),tEh0,R((τi)+)exp(rR(thTNτi)),tEhi,

    where

    R[(τi)+]=rSexp[rR(i1j=0Δj)],i=1,2,,kp.R[(τ0)+]=rS=θR1exp(rRTN).

    To analyze the local and global asymptotic stability of the periodic solution (0,I(t),N(t),R(t)) of model (4.1), we derive the following two results.

    Theorem 4.1. If min{λ1S,λ1I,λ1R,λ1N}<1, then the periodic solution (0,I(t),N(t),R(t)) is locally asymptotically stable for model (4.1), where

    λ1S=(1pS)exp{rSTN+kpi=0{rS(1+Kβ)exp(δ1τi+1)exp(δIτi)I((τi)+)KδI+rS{exp(δNτi+1)exp(δNτi)}N((τi)+)aSδN+rSμSaRrR[arctan(R((τi+1)+) exp(rRτi+1)aR)arctan(R((τi)+)exp(rRτi+1)aR)]}}.

    Theorem 4.2. The periodic solution (0,I(t),N(t),R(t)) is globally asymptotically stable for model (4.1) provided that

    R1S=(1pS)kpexp{rSTN+kpi=0{β{exp(δ1τi+1)exp(δIτi)}I((τi)+)δI+[exp(δNτi+1)exp(δNτi)]N((τi)+)(aS+K2)δN+μS[exp(rτi+1)exp(rτi)]R((τi)+)aRrR}}<1.

    The proofs for Theorems 4.1 and 4.2 can be found in Appendix B.

    Next, we study the impact of important and critical paramters on the threshold R1S. To accomplish this, we select the killing rate pI for the infected pest, and the pesticide application frequency kp as bifurcation parameters, while keeping all other parameters fixed as shown in Figure 1. In fact, the effects of kp and pI on R1S are depicted in Figure 1. The results indicate that if the pesticide kills the infected pests with a relatively lower killing rate pI (such as p2=0.2). Then the threshold value R1S is a monotonically increasing function with respect to kp, as illustrated in Figure 1(a). If pI is increased (in this case, p2=0.7,0.9), Figure 1(b), (c) demonstrates that the threshold value R1S becomes nonmonotonic with respect to kp. This indicates that there exists an optimal number of pesticide applications within the releasing period TN. It can be observed that in this case, the optimal control strategy is to apply pesticides two or three times over the period TN. In this scenario, the threshold value R1S consistently remains greater than 1, as depicted in Figure 1(b). However, Figure 1(c) illustrates that R1S is less than 1 if pesticide applications are applied twice. This demonstrates that if pesticide applications lead to significant effects on the infected pests, then the number of pesticide applications should be increased.

    Figure 1.  The effect of the killing rate pI on R1S. Parameters are: rS=0.04,TN=5,β=0.2, δI=0.2,δN=0.08,rR=0.02,aR=2,aS=2,K=6, Δ=TN/kp,θI=5, θR=0.8,θN=2,pI=0.7, pN=0.3,pR=0.5,pS=0.001, μ1=0.8,qI=0.3,qN=0.4.

    Furthermore, we can conduct two-parameter bifurcation analyses for R1S, as illustrated in Figure 2. In each subplot, we vary two key parameters simultaneously and observe their impact on R1S. All simulation results presented in Figure 2 indicate that R1S is highly sensitive to slight variations in the release constants θI, θS, θN, the releasing period TN and the killing rates pI, pS and pN. Moreover, these findings emphasize that for a given releasing period, the number of pesticide applications within the period TN, the releasing constants θI, θS, θN and the killing rates pI, pS, pN are crucial for effective pest control. This information can assist pest control experts in designing and determining the optimal timing for spray applications and the appropriate release rates.

    Figure 2.  The effect of two parameters on R1S. Parameters are: rS=0.04,TN=5,β=0.02, δI=0.9,δN=0.08,rR=0.02,aR=1,aS=2,K=10,Δ=TN/kp,qI=0.3, qN=0.4,μI=0.8. (a) θI=1,θR=0.8,θN=2,pN=0.3,pS=0.001; (b) θI=1,θR=0.8, θN=2,pI=0.2,pS=0.001; (c) θI=1,θR=0.8,pI=0.2,pN=0.3; (d) θI=1,θR=0.8,pI=0.2,pN=0.3; (e) θN=2,pI=0.2,pN=0.3,pS=0.001; (f) θI=1,θN=2,pI=0.2,pN=0.3,pS=0.001.

    Although we mentioned in Section 3 that the pest-eradication periodic solution only exist in theory and are difficult to achieve in practical pest control, we have conducted numerical studies to investigate the existence of the pest-eradication periodic solution, which means that the susceptible pest-eradication periodic solution is globally attractive, as shown in Figure 3. The theoretical existence of periodic solutions is indeed correct. In fact, as long as the parameters of the model satisfy the threshold conditions by changing the control strategy in practical pest control, the corresponding pest-eradication periodic solution of system can be obtained.

    Figure 3.  Pest-eradication periodic solution of model (4.1). Parameters are: rS=2,TN=5,β=0.2,δI=0.1, δN=0.1,rR=0.02,aR=0.2,aS=3,K=10,Δ=TN/kp,θI=2,θR=0.1,θN=3, pI=0.4,pN=0.3,pR=0.5,pS=0.9, μS=0.6,μN=0.5,qI=0.7,qN=0.4,kp=5.

    We assume that the pesticide is sprayed periodically, with the period recorded as Tp. This means that τn+1τn=Tp for every n belonging to the set of integers Z. During each pesticide spraying period of Tp, susceptible pests and natural enemies are introduced kp times. Consequently, we have the relationship

    λn+kp=Tp+λn.

    Define

    Δi=λi+1λi,Fhi=(hTp+λi,hTp+λi+1],i=0,1,2,,kq,

    where Δ0=λR,Δkq=Tpλkq,τ0=0,τkq+1=Tp, h is non-negative number, based on these definitions, we can conclude

    {I(t)=δII(t),tτn,tλm,I(t+)=(1pI)I(t),t=τn,I(t+)=(1+qI)I(t)+θI,t=λm, (4.5)
    {N(t)=δNN(t),tτn,tλm,N(t+)=(1pN)N(t),t=τn,N(t+)=(1+qN)N(t)+θN,t=λm, (4.6)

    and

    {R(t)=rRR(t),tτn,tλm,R(t+)=R(t),t=τn,R(t+)=R(t)+θR,t=λm. (4.7)

    It follows from model (4.1) that

    I([(h+1)Tp]+)=(1pI)[c1I((hTp)+)+c2]=(1pI)c1I((hTp)+)+(1pI)c2,

    where

    c1=(1+qI)kpexp(δITp),c2=θIkq1i=0exp((1+qI)iδIkqj=kqiΔj).

    Denote y([(h+1)Tp]+) as y(h+1). Then, the above equation can be rewritten as the following difference equation

    I(h+1)=(1pI)c1I(h)+(1pI)c2.

    It is evident that the above equation has a unique global equilibrium given by

    I2=(1pI)θIkq1i=0exp((1+qI)iδIkqj=kqiΔj)1(1pI)(1+qI)kqexp(δITp).

    This equilibrium is considered unique and globally stable under the condition that

    λ2I=(1pI)(1+qI)kpexp(δITp)<1.

    Therefore, model (4.5) has a globally stable periodic solution

    ˜IN2(t)={I2exp(δI(thTp)),tFh0,I2[(λk)+]exp(δI(thTpτi)),tFhi,

    where

    I2[(λk)+]=I2(1+qI)kexp(δIk1i=0Δi)+θI(Ki=1[(1+qI)iexp(δIk1j=kiΔj)]+1),

    k=1,2,,kp, particularly I2[(λ0)+]=I2.

    Analogously, model (4.6) has a a globally stable periodic solution

    ˜NN2(t)={N2exp(δI(thTp)),tFh0,N2[(λk)+]exp(δN(thTpτi)),tFhi

    as λ2N=(1pN)(1+qN)kexp(δNTp)<1. Here,

    N2[(λk)+]=I2(1+qN)kexp(δNk1i=0Δi)+θN(Ki=1[(1+qN)iexp(θSk1j=kiΔj)]+1),

    k=1,2,,kp and

    N2[(λ0)+]=N2=(1pN)θNkq1i=0exp((1+qN)iδIkqj=kqiΔj)1(1pN)(1+qN)kqexp(δNTp).

    Model (4.7) has a a globally stable periodic solution

    ˜RN2(t)={rRexp(rR(thTp)),tFh0,rR[(λk)+]exp(rR(thTpτi)),tFhi

    as λ2R=(1qR)exp(rRTP)<1. Here,

    rR[(λk)+]=rRexp(rRk1i=0Δi)+θR(Ki=1[exp(rRk1j=kiΔj)]+1),k=1,2,,kp

    and

    rR[(λ0)+]=rR=(1pI)θRkq1i=0exp(rRkqj=kqiΔj)1exp(rRTp).

    Hence, we have determined the local and global stability conditions for the periodic solution of model (4.1).

    Theorem 4.3. If min{λ2S,λ2I,λ2R,λ2N}<1, then the periodic solution (0,I(t),N(t),R(t)) of model (4.1) is locally asymptotically stable, where

    λ2S=(1pS)exp{rSTp+kpi=0{rS(1+Kβ)[exp(δ1λi+1)exp(δIλi)]I2[(λi)+]KδI+rS[exp(δNλi+1)exp(δNλi)]N2[(λi)+]aSδN+rSμSaRrR[arctan(rR[(λi)+]exp(rRλi+1)aR)arctan(rR[(λi)+]exp(rRλi)aR)]}}<1.

    Theorem 4.4. The periodic solution (0,I(t),N(t),R(t)) of model (4.1) is globally asymptotically stable provided that

    R2S=exp{rSTP+kpi=0{β[exp(δ1λi+1)exp(δIλi)]I2[(λi)+]δI+[exp(δNλi+1)exp(δNλi)]N2[(λi)+](aS+K2)δN+μS[exp(rRλi+1)exp(rRλi)]R[(λi)+]aRrR}}<1.

    By employing the same methods as those used in Section 4.1, we can investigate the impact of key parameters on the threshold value R2S and discuss its biological implications. Figure 4 provides detailed information on how different release constants θI affect the threshold value R2S. Regarding the parameters δI,δS,rR, Figure 4 suggests that even small changes can significantly influence R2S, indicating that a slight increase in the release constant θI of infected pests can considerably reduce the threshold parameter R2S. The larger the release rate θI of infective pests, the smaller the resulting threshold value, thereby benefiting pest control efforts.

    Figure 4.  The effects of kp and θI on R2S. Parameters are: rS=0.14,TN=5,β=0.2,Tp=10, aR=10,aS=2,K=5,Δ=Tp/kq,θR=0.2,θN=2,pI=0.6,pN=0.3, pS=0.001,μS=0.8,qI=0.003,qN=0.004. (a) δI=0.2,δS=0.08,rR=0.13; (b) δI=0.3,δS=0.08,rR=0.13; (c) δI=0.2,δS=0.1rR=0.13; (d) δI=0.2,δS=0.08,rR=0.2.

    The objective of this paper is to introduce and analyze an eco-epidemiological pest-natural enemy-plant model that investigates the synergistic combination of chemical and biological control methods. Our model examines the effects of varying frequencies of pesticide sprays and releases of infected pests and natural enemies on the suppression of pest populations. Through the use of impulsive differential equations, we establish threshold conditions for achieving a periodic solution that eradicates the susceptible pest population under different scenarios.

    We examine two distinct strategies for releasing natural enemies and two different tactics for pest control. One strategy involves more frequent pesticide sprays, while the other focuses on more frequent releases of susceptible pests. We establish sufficient conditions for the global attraction of the periodic solution that eradicates the susceptible pest population. This finding implies that complete elimination of the pest population is achievable under certain conditions regarding the release quantities of infected pests and natural enemies. In fact, in practical pest control, it is difficult to achieve the complete eradication of pests if the implemented control strategies cannot precisely bring the relevant parameter set to meet the theoretical threshold. In other words, the complete eradication of pests is a challenging goal to achieve.

    The theoretical findings presented in Section 4 offer several pest management control strategies. Nevertheless, complete eradication of the pest population is often unattainable in practice. Instead, the primary objective is to prevent the pest population from reaching harmful levels and to maintain its density below the economic threshold. To address this goal, we propose the development of a state-dependent impulsive differential equation, which will serve as a threshold control model. This approach will be explored as a potential future direction for our research.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    We would like to thank the editor and the anonymous referees for their valuable comments and suggestions that greatly improved the presentation of this work. This work is supported by National Natural Science Foundation of China (12261104, W. J. Qin) and Youth Talent of Xingdian Talent Support Program (XDYC-QNRC-2022-0708, W. J. Qin). Meanwhile, it is partly supported by National Natural Science Foundation of China (12201086, Y. Yang) and Youth Project of Science and Technology Research Program of Chongqing Municipal Education Commission (KJQN202201209, Y. Yang).

    No potential conflict of interest was reported by the authors.

    The proof of Theorem 3.2. To establish the local stability of the periodic solution, we employ the small amplitude perturbation method. Let

    S(t)=s(t),I(t)=i(t)+I(t),N(t)=n(t)+N(t),R(t)=r(t)+R(t),

    where s(t),i(t),n(t), and r(t) represent small perturbations. By employing Taylor expansions and disregarding higher-order terms, we can linearize model (2.3), resulting in the following set of linearized equations

    {s(t)=s(t)A(t),i(t)=βs(t)I(t)δIi(t),n(t)=μNs(t)N(t)aSδNn(t),r(t)=rRr(t)s(t)R(t)aR+(R(t))2,}tnT,s(t+)=(1pS)s(t),i(t+)=(1+qI)i(t),n(t+)=(1+qN)n(t),r(t+)=(1+qR)r(t),}t=nT. (A.1)

    where

    A=rS{1(1+Kβ)K+μSR(t)aR+(R(t))2N(t)aS}.

    Let Φ(t) be the fundamental solution matrix of (A.1), Φ(t) must satisfy

    dΦ(t)dt=(A000βI(t)δI00μNI(t)aS0δN0R(t)aR+(R(t))200rR)Φ(t),

    Φ(0)=I4 is the identical matrix. For all t(nT,(n+1)T], the fundamental solution matrix is

    Φ(t)=(exp[tnTA(τ)dτ]000exp(δI(tnT))00exp(δN(tnT))0exp(rR(tnT))).

    Furthermore, the last four equations of model (A.1) can be expressed as follows

    (s[(n+1)T+]i[(n+1)T+]n[(n+1)T+]r[(n+1)T+])=diag{1pS,1+qI,1+qN,1+qR}(s[(n+1)T]i[(n+1)T]n[(n+1)T]r[(n+1)T]).

    Hence, the eigenvalues of

    M=diag{1pS,1+qI,1+qN,1+qR}Φ((n+1)T)

    are

    λI=(1+qI)exp(δIT),λN=(1+qN)exp(δNT),λR=(1+qR)exp(rRT),
    λS=(1pS)exp((n+1)TnTA(τ)dτ)=(1pS)exp{rS{T+(1+Kβ)[exp(δT)1]˜IKδI+[exp(δNT)1]˜NaSδN}+rSμSaRrR[arctan(˜Rexp(rRT)aR)arctan(˜RaR)]}.

    Since min{λS,λI,λR,λN}<1, then the periodic solution is locally stable. The proof is complete.

    The proof of Theorem 3.3. The periodic solution (0,I(t),N(t),R(t)) exhibits local asymptotic stability, and we are primarily concerned with its global attractiveness. Let

    ϕ(t,ε)rSβ(I(t)ε1)+μS[R(t)+ε1]aRN(t)ε1aS+K2,

    where ε1>0. Furthermore, we have I(t)=βS(t)I(t)δII(t)δII(t). By utilizing the comparison principle and Lemma (3.1), we can establish the existence of n1 such that I(t)I(t)ε1 for all tn1T. Similarly, we can find a n2 (here n2>n1) such that N(t)N(t)ε1 for all tn2T. Additionally, there exists a n3 (here n3>n2) such that R(t)R(t)ε1 for all tn3T. Consequently, we can conclude that

    S(t)=rSS(t)[1S(t)+I(t)K]+μSS(t)R(t)aR+R2(t)βS(t)I(t)S(t)N(t)aS+S2(t)rSS(t)βS(t)I(t)+μSS(t)R(t)aRS(t)N(t)aS+K2S(t){rSβ(I(t)ε1)+μS[R(t)+ε1]aRN(t)ε1aS+K2}

    for tn3T. The first equation of model (2.3) can be expressed as follows

    {S(t)ϕ(t,ε1)S(t),tnT,S(t+)=(1pS)S(t),tnT.

    By integrating over the interval (n3+k)T to (n3+k+1)T, we can obtain

    S[(n3+k+1)T+]S[(n3+k)T+](1pS)exp((n3+k+1)T(n3+k)Tϕ(t,ε1)dt)=S[(n3+k)T+]R5=S[T+]Rn3+k5,

    where

    R5=(1pS)exp((n3+k+1)T(n3+k)Tϕ(t,ε1)dt).

    Since R5<1, we get S(t)0 as k. Thus, for an arbitrary positive constant ε2 small enough, there exists a n3 (n3>n2) such that S(t)<ε2 for all tn3T.

    Next, we will demonstrate that I(t) approaches I(t). For 0<ε2<δI/β, there exists 0<S(t)<ε1 such that 0<S(t)<ε1 for t>n4T (here n4>n3). By considering the second equation of model (2.3), we can conclude that

    (βε2δI)I(t)I(t)=βS(t)I(t)δII(t)<(βε2δI)I(t).

    Let I1(t) and I2(t) be the solutions of the following equations, respectively

    {I(t)=(βε2+δI)I(t),tnT,I(t+)=(1+qI)I(t)+θI,tnT,

    and

    {I(t)=(βε2+δI)I(t),tnT,I(t+)=(1+qI)I(t)+θI,tnT.

    From here it is easy to show that

    I1(t)=θRexp[(βε2+δI)(tnT)]1+(1+qI)exp(δIT),I2(t)=θRexp[(βε2+δI)(tnT)]1+(1+qI)exp(δIT).

    It can be easily deduced that I(t) approaches I(t) as t tends to infinity.

    Similarly, we can prove that N(t) tends to N(t) as t approaches infinity. For R(t), the following inequality holds

    R(t)(rRε2aR)<˙R(t)<rRR(t)

    for t>n5T (here n5>n4). By combining the solution of model (3.3) with the comparison theorem, we obtain the following result

    exp[(rRε2aR(tnT))]˜R<R(t)<exp[rR(tnT)]˜R.

    Therefore, as ε2 approaches 0, we have R(t)R(t). In fact, if R5<1, then I(t)I(t), N(t)N(t), and R(t)R(t) as t0. This implies that the periodic solution (0,I(t),N(t),R(t)) is globally asymptotically stable. Thus, the proof is complete.

    The proof of Theorem 4.1. We define

    S(t)=s(t),I(t)=i(t)+I(t),N(t)=n(t)+N(t),R(t)=r(t)+R(t),

    where s(t),i(t),n(t), and r(t) represent small perturbations. By linearizing model (4.1) through Taylor expansions and neglecting higher-order terms, the resulting linearized equations are given by

    {s(t)=s(t)A1(t),i(t)=βs(t)I(t)δIi(t),n(t)=μNs(t)N(t)aSδNn(t),r(t)=rRr(t)s(t)R(t)aR+[R(t)]2,}tτn,tλm,s(t+)=(1pS)s(t),i(t+)=(1pI)i(t),n(t+)=(1pN)n(t),r(t+)=r(t),}t=τn,s(t+)=s(t),i(t+)=(1+qI)i(t),n(t+)=(1+qN)n(t),r(t+)=r(t),}t=λm, (B.1)

    where

    A1(t)=rS{1(1+Kβ)˜IN1(t)K+μS˜RN1(t)aR+[˜RN1(t)]2˜NN1(t)aS}.

    Let Φ(t) be the fundamental solution matrix of (B.1). In this case, Φ(t) must satisfy the following

    dΦ(t)dt=(A1(t)000βI(t)δI00μNI(t)aS0δN0R(t)aR+[R(t)]200rR)Φ(t),

    where Φ(0)=I4 is the identical matrix. For all tEhi, the fundamental matrix is

    Φ(t)=(exp(thTpA1(τ)dτ)000exp(δI(thTp))00exp(δN(thTp))0exp(rR(tnTp))).

    Furthermore, system (B.1) can be expressed as

    (s[(h+1)T+p]i[(h+1)T+p]n[(h+1)T+p]r[(h+1)T+p])=M(s[(hTp)+]i[(hTp)+]n[(hTp)+]r[(hTp)+]),

    where

    M=diag{(1pS)kp,(1+qI)(1pI)kp,(1+qN)(1pN)kp,1}Φ(h+1)T.

    Given that minλ1S,λ1I,λ1R,λ1N<1, indicating that all eigenvalues of matrix M

    λ1S=R9=(1ps)kpexp((n+1)TnTA1(τ)dτ)=(1pS)exp{rSTp+kpi=0{rS(1+Kβ)exp(δ1τi+1)exp(δIτi)I((τi)+)KδI+rS{exp(δNτi+1)exp(δNτi)}N((τi)+)aSδN+rSμSaRrR[arctan(R((τi+1)+)exp(rRτi+1)aR)arctan(R((τi)+)exp(rRτi+1)aR)]}}<1,
    λ1I=(1+qI)(1pI)kpexp(δIT)<1,
    λ1N=(1+qN)(1pN)kpexp(δNT)<1,λ1R=R8=exp(rRT)<1,

    thus, the periodic solution (0,I(t),N(t),R(t)) is locally asymptotically stable. Hence, the proof is complete.

    The proof of Theorem 4.2. We define

    ϕ(t,ε1){rSβ(˜IN1(t)ε1)+μS[˜RN1(t)+ε1]aR˜NN1(t)ε1aS+K2},

    where ε1>0. By utilizing the comparison principle, we can establish the existence of n1 such that I(t)I(t)ε1 for all tn1T. Similarly, there exists a n2 (here n2>n1) such that N(t)N(t)ε1 for all tn2T. Additionally, there is a n3 (here n3>n2) such that R(t)R(t)+ε1 for all tn3T. Hence, we can conclude that

    S(t)=rSS(t)+μSS(t)R(t)aR+R2(t)βS(t)I(t)S(t)N(t)aS+S2(t)rSS(t)βS(t)I(t)+μSS(t)R(t)aRS(t)N(t)aS+K2S(t){rSβ(˜IN1(t)ε1)+μS[˜RN1(t)+ε1]aR˜NN1(t)ε1aS+K2}

    for tn3T. It is follows from model (4.1) that

    {S(t)φ(t,ε1)S(t),tτn,tλm,S(t+)=(1pS)S(t),t=τn,S(t+)=S(t),t=λm,

    Taking integral on Ehi,i=1,2,,kp that

    S[(hTN+τi+1)+]S[(hTN+τi)+](1pS)exp(hTN+τi+1hTN+τiϕ(t,ε1)dt)

    and

    S[((h+1)TN)+]S[(hTN)+](1pS)kpexp((h+1)TNhTNϕ(t,ε1)dt).

    We define

    λ1S=(1pS)kpexp(hTN(h+1)TNϕ(t,ε1)dt),t((n3+k)T,(n3+k+1)T],kZ+.

    If λ1S<1, we can observe that S(t)0 as k. Consequently, for any sufficiently small positive constant ε2, there exists an n3 (here n3>n2) such that S(t)<ε2 for all tn3T.

    Next, we will prove that I(t) approaches I(t). For 0<ε2<δIβ, there exists ε1 such that 0<S(t)<ε1 for t>n4T (here n4>n3). Consequently, we have

    (βε2δI)I(t)I(t)=βS(t)I(t)δII(t)<(βε2δI)I(t).

    Let I1(t) and I2(t) denote the solutions of the following equations, respectivelyd

    {I(t)=(βε2+δI)I(t),tτn,tλmI(t+)=(1pI)I(t),t=τn,I(t+)=(1+qI)I(t)+θI,t=λm,

    and

    {I(t)=(δIβε2)I(t)tτn,tλm,I(t+)=(1pI)I(t),t=τn,I(t+)=(1+qI)I(t)+θI,t=λm.

    Therefore, we can conclude that

    I1(t)=θI1(1+qI)(1pI)kpexp[(βε2+δI)TN],
    I2(t)=θR1(1+qI)(1pI)kpexp[(δIβε2)TN].

    So it gives that limε20Ii(t)=I(t) from limtI(t)=I(t).

    Analogously, we can prove that N(t)N(t) as t.

    For R(t), it gives that

    R(t)(rRε2aR)<˙R(t)<rRR(t)

    for t>n5T (here n5>n4), and we have

    exp[(rRε2aR(tnTN))]˜R<R(t)<exp[rR(thTN)]˜R.

    Therefore, we can conclude that limε20R(t)=R(t). In summary, if λ1S<1, it follows that I(t)I(t), N(t)N(t), and R(t)R(t) as t0. This implies that the periodic solution (0,I(t),N(t),R(t)) is globally asymptotically stable. Hence, the proof is complete.



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