
In this paper, we explore the existence of fixed points, local dynamics at fixed points, bifurcations and chaos of a discrete prey-predator fishery model with harvesting. More specifically, it is proved that, for all involved parameters, the model has trivial fixed point, but it has semitrivial and interior fixed points under definite parametric condition(s). We study the local behavior at fixed points by applying the theory of linear stability. Furthermore, it is shown that flip bifurcation does not occur at semitrivial and trivial fixed points, but that the model undergoes Neimark-Sacker bifurcation at interior fixed point. It is also proved that, at interior fixed point, the model undergoes the flip bifurcation. By using a feedback control strategy, the chaos control is also examined. Finally, to illustrate the theoretical findings, detailed numerical simulations are provided.
Citation: A. Q. Khan, Ibraheem M. Alsulami, S. K. A. Hamdani. Controlling the chaos and bifurcations of a discrete prey-predator model[J]. AIMS Mathematics, 2024, 9(1): 1783-1818. doi: 10.3934/math.2024087
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In this paper, we explore the existence of fixed points, local dynamics at fixed points, bifurcations and chaos of a discrete prey-predator fishery model with harvesting. More specifically, it is proved that, for all involved parameters, the model has trivial fixed point, but it has semitrivial and interior fixed points under definite parametric condition(s). We study the local behavior at fixed points by applying the theory of linear stability. Furthermore, it is shown that flip bifurcation does not occur at semitrivial and trivial fixed points, but that the model undergoes Neimark-Sacker bifurcation at interior fixed point. It is also proved that, at interior fixed point, the model undergoes the flip bifurcation. By using a feedback control strategy, the chaos control is also examined. Finally, to illustrate the theoretical findings, detailed numerical simulations are provided.
The aquaculture or fish forming in seas, oceans, rivers and streams hold massive potential as a tool to provide us healthy and nutritious food. It also presents a good contribution to development in areas of employment like fish farming, rearing, fish culture, handling and fish processing, etc. Due to population growth, it is a great challenge around the globe to find the sources of food for those people. Fish provide a healthy source of protein. It is highly nutritious and provides a cheap and healthy source of protein. Fish is not only a source of food for humans, it also serves as a source of prey for most of the sea life. Thus, naturally, fish plays an important role in aquatic ecosystems. As the demand for fish increases, the harvesting of fish leads to overfishing, which results in the extinction of some species entirely. Overfishing is the act of catching too many fish before they can reproduce, which depletes fish populations over time. Increased demand for seafood, technologies which make fishing easier and a lack of appropriate fishing laws and enforcement cause overfishing. Overfishing reduces biodiversity and may lead to the extinction of some groups of fish or entire fish species. Those animals that rely on fish for food may struggle to find enough sustenance and also become endangered. Increased investment in fishery management and research is needed to understand the fish populations and ecosystems better. If an all-out extinction is to be prevented, meaningful measures must soon be taken. Scientists and researchers believe that this can be achieved by only harvesting the optimum yield. Scientists and researchers develops several numerical models to estimate the innovative trends in population. Within an environment, the population dynamics can be modeled by a system of autonomous differential equations. However, there is no analytical solution for certain differential equations, such as the nonlinear ones. In these situations, the qualitative approach is applied in addition to the numerical strategy.
A generalized numerical method is added for biological growth; it incorporates the acknowledged capabilities encompassed in generalized logistic, Brody, von Bertalanffy, Gompertz, Richards logistic and other models. In addition, a few theoretical mathematical features of interaction between prey and predator have been provided on the presumption that predation has little or no impact on the prey's growth population. Predator population factors have been integrated into development models to take into account the fact that prey populations grow according to logistic and von Bertalanffy theory. It is difficult to accurately predict the prey-predator interaction. Hence, different results might obviously be produced. Studying various angles of these prey-predator interactions by exploring the dynamical characteristics generates a fascinating and significant biological phenomenon. By examining the effects of toxic substances on aquatic ecosystems, Huda et al. [1] have explored the behavior of the following prey-predator fishery model:
dxdt=r1x(1−xK)−γ1xyA+x−αx2y, dydt=cγ2xyA+x−βxy2−(d+qE)y, | (1.1) |
where K and r1 respectively represent the carrying capacity and logistic growth rate of the prey population; γ1 and γ2 are the rates of interaction between the prey and predator fish populations; α and β respectively denote the prey populations and toxicity coefficients for predatory; A denotes the environmental protection level for prey; c is predator growth rate; d and q respectively denote the natural mortality rate of predatory fish populations and coefficient for predatory population capture activity and the finally; E denotes the harvesting rate of the predator population. Pujaru and Kar [2] have investigated the dynamics of the following predator-prey system:
dxdt=rx(1−xK)−αxy−q1Ex, dydt=sy(1−yL)+αxy−q2Ey, | (1.2) |
where r and s denote the growth rates of the predator and prey populations, and L and K respectively denote the carrying capacities of the predator and prey populations. Kar [3] has examined the behavior of the following fishery model with time delay:
dxdt=x(g(x)−yp(x)), dydt=y(−d+αxp(x))−qEy(t−τ), | (1.3) |
where x(t) and y(t) respectively denote the densities of prey and predator populations; g(x) and xp(x) respectively denote the growth rate of the prey and response function; α and d respectively denote the conversion factor and predator's death rate; q is the predator's catchability coefficient; qEy is the catch rate function and τ denotes the time delay. Liu et al. [4] have studied the dynamical behaviors of the following continuous model:
dxdt=x(a1−b1x−cxyd+y2)−q1mEx, dydt=y(a2−b2y)yu+y−q2mEy, | (1.4) |
where ai,bi (i=1,2), c, d and u are positive constants, yu+y denotes the Allee effect and the algicidal bacteria and harvesting functions for algae are respectively denoted by q2mEy and q1mEx. Moreover E, d and cxyd+y2 respectively denote the combined capture effort, half-saturation constant and algal growth. Keong et al. [5] have examined the behavior of the following fishery model:
dxdt=x(1−αx)−xy−βx−σx2y, dydt=−δy+xy−ϵy−ρxy2, | (1.5) |
where α denotes the ratio of the prey's growth rate; β is the ratio of the product of catchability coefficient of prey and harvesting effort to the growth rate of prey; β is the ratio of the product of coefficient of toxicity and growth rate of prey to the square of growth rate of predator by prey and predator's growth rate is δ. Chen et al. [6] have explored Hopf bifurcation of a species interaction model. Chen and Wu [7] have examined the dynamical behavior of a predator-prey system with a harvesting policy and network connection. For more interesting results in this field, we refer the reader to the work of the most eminent mathematicians [8,9,10] and the references cited therein. On the other hand, many investigators have explored the dynamics of discrete models designated by maps or difference equations rather than continuous models described by differential equations because discrete-time models are more reasonable in the case of non-overlapping generations; additionally, such models give more efficient computational results for numerical simulations [11,12]. For instance, Elettreby et al. [13] have investigated the complex dynamical behavior of the predator-prey model described below:
xt+1=axt(1−xt)−dx2tyte+x2t, yt+1=(1+bλxt)yt−cyt, | (1.6) |
where all parameters are positive. Santra et al. [14] have examined the behavior of the following predator-prey system:
xt+1=axt(1−xt)−c(1−b)xtyt(1+αxt(1−b))(1+βyt), yt+1=d(1−b)xtyt(1+αxt(1−b))(1+βyt), | (1.7) |
with all involved parameters being positive. Zhang et al. [15] have explored the Hopf bifurcation of a delayed biological economic model. Zhang and Zou [16] have explored the dynamics of the following model:
xt+1=xt+r0Kxt(K−xt)(xt−c)−axtyt, yt+1=yt+bxtyt−dyt, | (1.8) |
where x and y respectively denote the prey and predator densities. Moreover, r0K(K−xt)(xt−c) denotes the per capita growth rate of the prey in the absence of a predator. Chakraborty et al. [17] have investigated the dynamical behaviors of the following prey-predator model:
xt+1=xt+h(xt(1−xt2)2−yt2(1+axt)), yt+1=yt+h(−syt+cxtyt(1+axt)−eyt), | (1.9) |
where h and q respectively denote step size and catchability coefficient for the predator population, a, c, e and s are positive constants and E denotes the harvesting effort. On the other hand, in recent years, many authors have investigated the bifurcation behavior of fractional-order systems. For instance, Mua et al. [18] have investigated the bifurcation and hybrid control tactics of a chemical reaction model with delays. Xu et al. [19] have explored the dynamics in a discrete predator-prey competitive model with feedback controls. Xu et al. [20] have explored the bifurcation mechanism for fractional-order three-triangle multi-delayed neural networks. Xu et al. [21] have explored the bifurcation in a fractional-order predator-prey system with mixed delays. For more interesting results in this regard, we refer the reader to [22,23,24,25].
This section presents the mathematical model of a discrete predator-prey fishery model with harvesting. In order to formulate the continuous-time fishery model with harvesting, our investigation has been divided into the following three essential parts [26]:
● Consider the following model equation in which fish harvesting occurs without a predator:
dxdt=rx(1−xK)−Ex, | (1.10) |
where Ex denotes harvesting per unit time and E denotes a positive constant that increased the measure of the effort. Additionally, K denotes the natural carrying capacity and r is the linear per capita growth rate. It is important to denote that, if E=0, then model (1.10) reduces to the non-harvesting fish model.
● Now, consider the following model equation in which fish harvesting occurs in the presence of a predator:
dydt=−νy+sxy, | (1.11) |
where s and ν respectively denote the positive parameters for the birth rate and death rate of the predator population.
● Finally, if one takes into account that competition within the predator population increases the death rate of the species, the desired fish harvesting model takes the following form:
dxdt=rx(1−xK)−Ex−βxy, dydt=−νy+sxy−αy2, | (1.12) |
where β is the measure of the predator's rate of prey consumption and α is the measure of the predator's rate of intra-specific competition. On the other hand, the discrete version of the continuous model (1.12), according to the Euler forward formula takes the following form:
xt+1−xth=rxt(1−xtK)−Ext−βxtyt, yt+1−yth=−νyt+sxtyt−αy2t, | (1.13) |
which further becomes
xt+1=(1−Eh+rh)xt−hrKx2t−βhxtyt, yt+1=(1−hν)yt+shxtyt−αhy2t, | (1.14) |
where the integral step size is h.
The purpose of the present study is to explore the dynamical characteristics of a discrete prey-predator fishery model with harvesting, i.e., model (1.14). More precisely, our key contributions in this paper are as follows:
● Demonstration of the local dynamics at equilibria based on the linear stability theory of the discrete fishery model (1.14).
● Examination of the positive invariance of the discrete fishery model (1.14).
● Identification of bifurcation sets and detailed bifurcation analysis at equilibria of the discrete fishery model (1.14).
● Study of chaos via the state feedback control method.
● Validation of theoretical results numerically through the use of Matlab and Mathematica.
The rest of the paper is organized as follows: In Section 2, a brief local dynamical analysis at fixed points and under the condition of positive invariance are studied, whereas bifurcations and chaos control in the discrete fishery model are examined in Section 3. In Section 4, our main findings are verified numerically. The paper's conclusion, along with future work, is given in Section 5.
The local dynamics of the discrete fishery model (1.14) is examined in this section. To do this, we first determine the equilibria and the linearized form of fishery model (1.14) as follows:
Theorem 2.1. In R2+={(x,y):x, y≥0}, fishery model (1.14) has three fixed points. More precisely the following is true:
(i) ∀ K, r, E, s, α, β, ν, L1=(0,0) is a trivial fixed point of the fishery model (1.14).
(ii) If r>E, then L2=(K(r−E)r,0) is a semitrivial fixed point of fishery model (1.14).
(iii) If E<min{νβ+αrα,rKs−rνKs}, then L3=(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr) is an interior fixed point of fishery model (1.14).
Proof. See in Appendix A.
Now, at L, the linearized form of (1.14) under the map
(f1,f2)↦(xt+1,yt+1) | (2.1) |
is
Ωt+1=V|LΩt, | (2.2) |
where
V|L:=(1−Eh+rh−2hrKxt−βhyt−βhxtshyt(1−hν)+shxt−2αhyt), | (2.3) |
and
f1:=(1−Eh+rh)x−hrKx2−βhxy, f2:=(1−hν)y+shxy−αhy2. | (2.4) |
Now, it should be noted that, at L1, (2.3) becomes
V|L1:=(1−Eh+rh001−hν) | (2.5) |
with
λ1=1−Eh+rh, λ2=1−hν. | (2.6) |
Theorem 2.2. For L1, the following characteristics hold:
(i) If
0<h<min{2E−r,2ν} | (2.7) |
and
E>r, | (2.8) |
then L1 of fishery model (1.14) is a sink.
(ii) If (2.8) holds and
h>max{2E−r,2ν}, | (2.9) |
then L1 of fishery model (1.14) is a source.
(iii) If (2.8) holds and
2ν<h<2E−r | (2.10) |
or
2E−r<h<2ν, | (2.11) |
then L1 of fishery model (1.14) is a saddle.
(iv) If
h=2E−r | (2.12) |
or
h=2ν, | (2.13) |
then L1 of fishery model (1.14) is non-hyperbolic.
Proof. See in Appendix B.
Now, at L2, (2.3) gives
V|L2:=(1+Eh−rh−βhK(r−E)r01−hν+shK(r−E)r) | (2.14) |
with
λ1=1+Eh−rh, λ2=1−hν+shK(r−E)r. | (2.15) |
Theorem 2.3. For L2, the following characteristics hold:
(i) If
0<h<min{2r−E,2rrν−sK(r−E)} | (2.16) |
and
rKs−rνKs<E<r, | (2.17) |
then L2 of fishery model (1.14) is a sink.
(ii) If (2.17) holds and
h>max{2r−E,2rrν−sK(r−E)}, | (2.18) |
then L2 of fishery model (1.14) is a source.
(iii) If (2.17) holds and
2rrν−sK(r−E)<h<2r−E | (2.19) |
or
2r−E<h<2rrν−sK(r−E), | (2.20) |
then L2 of fishery model (1.14) is a saddle.
(iv) If (2.17) holds and
h=2r−E | (2.21) |
or
h=2rrν−sK(r−E), | (2.22) |
then L2 of fishery model (1.14) is non-hyperbolic.
Proof. See in Appendix C.
Finally, at L3, (2.3) gives
V|L3=(1−rh(νβ+αr−αE)Ksβ+αr−βhK(νβ+αr−αE)Ksβ+αrshK(rKs−rν−KsE)Ksβ+αr1−αh(rKs−rν−KsE)Ksβ+αr) | (2.23) |
with
λ2−p(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr)λ+q(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr)=0, | (2.24) |
where
p(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr)={2(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)}Ksβ+αr,q(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr)={(Ksβ+αr)−rh(νβ+αr−αE)−αh×(rKs−rν−KsE)+h2(νβ+αr−αE)×(rKs−rν−KsE)}Ksβ+αr. | (2.25) |
Additionally, the roots of (2.24) are
λ1,2=p(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr)±√Δ2, | (2.26) |
where
Δ=p(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr)2−4q(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr)=(2(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)Ksβ+αr)2−4{(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)+h2(νβ+αr−αE)(rKs−rν−KsE)}Ksβ+αr. | (2.27) |
Theorem 2.4. Let Δ<0; then, for L3, the following holds:
(i) If
0<h<r(νβ+αr−αE)+α(rKs−rν−KsE)(νβ+αr−αE)(rKs−rν−KsE), | (2.28) |
then L3 of fishery model (1.14) is a stable focus.
(ii) If
h>r(νβ+αr−αE)+α(rKs−rν−KsE)(νβ+αr−αE)(rKs−rν−KsE), | (2.29) |
then L3 of fishery model (1.14) is an unstable focus.
(iii) If
h=r(νβ+αr−αE)+α(rKs−rν−KsE)(νβ+αr−αE)(rKs−rν−KsE), | (2.30) |
then L3 of fishery model (1.14) is non-hyperbolic.
Proof. See in Appendix D.
Theorem 2.5. Let Δ>0; then, for L3, the following holds:
(i) If
0<h<min{{r(νβ+αr−αE)+α(rKs−rν−KsE)+√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE),{r(νβ+αr−αE)+α(rKs−rν−KsE)−√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE)}, | (2.31) |
then L3 of fishery model (1.14) is a stable node.
(ii) If
h>max{{r(νβ+αr−αE)+α(rKs−rν−KsE)+√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE),{r(νβ+αr−αE)+α(rKs−rν−KsE)−√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE)}, | (2.32) |
then L3 of fishery model (1.14) is an unstable node.
(iii) If
h={r(νβ+αr−αE)+α(rKs−rν−KsE)+√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE) | (2.33) |
or
h={r(νβ+αr−αE)+α(rKs−rν−KsE)−√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE), | (2.34) |
then L3 of fishery model (1.14) is non-hyperbolic.
Proof. See in Appendix E.
In order to examine the positively invariant set, it is noted that the model (1.14) can also be expressed as
Ω:={x=x(1−Eh+rh−hrKx−βhy),y=y(1−hν+shx−αhy). | (2.35) |
Definition 2.6. The set S is called invariant with respect to the operator Ω if Ω(S)⊂S.
Regarding the positively invariant set of the discrete model (1.14), one has the following proposition.
Proposition 2.7. The set
S1={(x,y)∈R2+:0<x<K(1−Eh+rh)hr, y=0} |
is positively invariant with respect to Ω.
In the next section, we will analyze bifurcations at L1,2,3 according to the bifurcation theory [27,28].
It is noted that, if (2.12) holds, then from (2.6), one gets
λ1|(2.12)=−1; |
but,
λ2|(2.12)=1−2νE−r≠−1 or 1, |
which suggests that fishery model (1.14) may undergo flip bifurcation if (α,β,ν,r,K,E,s) belongs to the following set:
FB|L1:={(α,β,ν,r,K,E,s), h=2E−r}. | (3.1) |
But, by calculation, flip bifurcation cannot exist; so, L1 is degenerate for higher codimensions. Further, if (2.21) holds, then it is also easy to verify from (2.15) that
λ2|(2.21)=r(r−E)−2νr+2sK(r−E)r(E−r)≠1 or −1; |
but, λ1|(2.21)=−1, which implies that fishery model (1.14) may undergo flip bifurcation if (α,β,ν,r,K,E,s) belongs to the following set:
FB|L2:={(α,β,ν,r,K,E,s), h=2r−E}. | (3.2) |
The following theorem gives the proof of the fact that, if (α,β,ν,r,K,E,s)∈FB|L2, then fishery model (1.14) do not undergo flip bifurcation.
Theorem 3.1. At L2, if (α,β,ν,r,K,E,s)∈FB|L2, then no flip bifurcation occurs.
Proof. Since model (1.14) is invariant with respect to y=0, one can restrict it on y=0 in order to study flip bifurcation, where (1.14) takes the following form
xt+1=(1−Eh+rh)xt−hrKx2t. | (3.3) |
From (3.3), one can write
f1:=(1−Eh+rh)x−hrKx2. | (3.4) |
Finally, if
h=h∗=2r−E |
and
x=x∗=K(r−E)r, |
then, from (3.4), we get
∂f1∂x|h∗=2r−E, x∗=K(r−E)r:=−1, | (3.5) |
∂2f1∂x2|h∗=2r−E, x∗=K(r−E)r:=4rK(E−r) | (3.6) |
and
∂f1∂h|h∗=2r−E, x∗=K(r−E)r:=0. | (3.7) |
From (3.7), it should be noted that no flip bifurcation at L2 occurs if (α,β,ν,r,K,E,s)∈FB|L2.
Further, if (2.30) holds, then V|L3 at L3 has complex eigenvalues where |λ1,2|(2.30)=1, which implies that fishery model (1.14) may undergo Neimark-Sacker bifurcation if (α,β,ν,r,K,E,s) belongs in the following set:
NB|L3:={(α,β,ν,K,s,r,E), h=r(νβ+αr−αE)+α(rKs−rν−KsE)(νβ+αr−αE)(rKs−rν−KsE)}. | (3.8) |
Theorem 3.2. At L3, Neimark-Sacker bifurcation exists if (α,β,ν,r,K,E,s)∈NB|L3.
Proof. If (α,β,ν,r,K,E,s)∈NB|L3 with h as the bifurcation parameter, then model (1.14) takes the following form:
xt+1=(1−E(h∗+ϵ)+r(h∗+ϵ))xt−(h∗+ϵ)rKx2t−β(h∗+ϵ)xtyt,yt+1=(1−(h∗+ϵ)ν)yt+s(h∗+ϵ)xtyt−α(h∗+ϵ)y2t. | (3.9) |
Moreover, the roots of V|L3 at L3 for the ϵ-involving model (3.9) is
λ1,2=p(ϵ)±ι√4q(ϵ)−p2(ϵ)2, | (3.10) |
where
p(ϵ)=2(Ksβ+αr)−(h∗+ϵ)(α(rKs−rν−KsE)+r(νβ+αr−αE))Ksβ+αr,q(ϵ)={(Ksβ+αr)−r(h∗+ϵ)(νβ+αr−αE)−α(h∗+ϵ)×(rKs−rν−KsE)+(h∗+ϵ)2(νβ+αr−αE)×(rKs−rν−KsE)}Ksβ+αr. | (3.11) |
From (3.10) and (3.11), we have
|λ1,2|=√{(Ksβ+αr)−r(h∗+ϵ)(νβ+αr−αE)−α(h∗+ϵ)×(rKs−rν−KsE)+(h∗+ϵ)2(νβ+αr−αE)×(rKs−rν−KsE)}Ksβ+αr | (3.12) |
and
d|λ1,2|dϵ|ϵ=0=r(νβ+αr−αE)+α(rKs−rν−KsE)Ksβ+αr≠0. | (3.13) |
Now, occurrence of Neimark-Sacker bifurcation for fishery model (3.9) at L3 requires that λτ1,2≠1, τ=1,⋯,4 if ϵ=0, which is equivalent to p(0)≠−2,0,1,2. However, if (2.30) holds, then from (3.11), we get that q(0)=1. So, p(0)≠−2,2, and, hence, one only requires that p(0)≠0,1, which gives
E≠{α2r3+α2K2rs2−2αβK2rs2+αβr2ν−α2Krsν+αβKrsν−β2K2s2ν±√−α4r4ν2−2α3βKr3sν2+2αβ3K3rs3ν2+β4K4s4ν4}α2r2+α2K2s2−2αβK2s2,{2α2r3+2α2Kr2s+2α2K2rs2−2αβK2rs2−α2r2ν+2αβr2ν−2α2Krsν+2αβKrsν−β2K2s2ν±√−3α4r4ν2−8α3βKr3sν2−6α2β2K2r2s2ν2+β4K4s4ν2}2(α2r2+α2Krs+α2K2s2−αβK2s2). | (3.14) |
Now, L3 of the discrete fishery model (3.9) is transformed to the origin by using the following transformations:
ut=xt−x∗, vt=yt−y∗, | (3.15) |
where
x∗=K(νβ+αr−αE)Ksβ+αr, |
and
y∗=rKs−rν−KsEKsβ+αr. |
From (3.15) and (3.9), we get
ut+1=(1−Eh∗+rh∗)(ut+x∗)−h∗rK(ut+x∗)2−βh∗(ut+x∗)(vt+y∗)−x∗,vt+1=(1−νh∗)(vt+y∗)+sh∗(ut+x∗)(vt+y∗)−αh∗(vt+y∗)2−y∗. | (3.16) |
Next, if ϵ=0, then we study the normal form of (3.16). For this, system (3.16) becomes
ut+1=Ψ11ut+Ψ12vt+Ψ13u2t+Ψ14utvt+Ψ15v2t,vt+1=Ψ21ut+Φ22vt+Ψ23u2t+Ψ24utvt+Ψ25v2t, | (3.17) |
with
Ψ11=1−Eh∗+rh∗−2rh∗Kx∗−βh∗y∗,Ψ12=−βh∗x∗, Ψ13=−h∗rK,Ψ14=−βh∗, Ψ15=0, Ψ21=sh∗y∗,Ψ22=1−νh∗+sh∗x∗−2αh∗y∗,Ψ23=0, Ψ24=sh∗, Ψ25=−αh∗. | (3.18) |
Now, we can transform the linear part of (3.17) into canonical form by applying the following transformation:
(utvt):=(Ψ120η−Ψ11−ζ)(xtyt), | (3.19) |
with
η=2(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)2(Ksβ+αr),ζ={√4h2(νβ+αr−αE)(rKs−rν−KsE)(Ksβ+αr)−(rh(νβ+αr−αE)+αh(rKs−rν−KsE))2}2(Ksβ+αr). | (3.20) |
From (3.19) and (3.17), we get
xt+1=ηxt−ζyt+B1(xt,yt), yt+1=ζxt+ηyt+B2(xt,yt), | (3.21) |
where
B1=s11x2t+s12xtyt+s13y2t, B2=s21x2t+s22xtyt+s23y2t, | (3.22) |
and
s11=Ψ12Ψ13+(η−Ψ11)Ψ14+(η−Ψ11)2Ψ15Ψ12,s12=−ζΨ14−2ζ(η−Ψ11)Ψ15Ψ12, s13=ζ2Ψ15Ψ12,s21=η−Ψ11ζΨ12Ψ13−η−Ψ11ζΨ12Ψ24−1ζΨ23Ψ212+(η−Ψ11)2ζΨ14−(η−Ψ11)3ζΨ25−(η−Ψ11)2ζΨ25,s22=Ψ12Ψ24−(η−Ψ11)Ψ14−2(η−Ψ11)2Ψ15Ψ12+2(η−Ψ11)Ψ25,s23=ζ(η−Ψ11)Ψ15Ψ12−ζΨ25. | (3.23) |
From (3.22), we get
B1xtxt|O=2s11, B1xtyt|O=s12, B1ytyt|O=2s13,B1xtxtxt|O=B1xtxtyt|O=B1xtytyt|O=B1ytytyt|O=0,B2xtxt|O=2s21, B2xtyt|O=s22,B2ytyt|O=B2xtxtxt|O=B2xtxtyt|O=B2xtytyt|O=B2ytytyt|O=0. | (3.24) |
Finally, regarding the occurrence of Neimark-Sacker bifurcation, it is required that the following quantity be non-zero [29,30,31]:
Γ=−ℜ((1−2ˉλ)ˉλ21−λυ11υ20)−12‖υ11‖2−‖υ02‖2+ℜ(ˉλυ21), | (3.25) |
where
υ02=18(B1xtxt−B1ytyt+2B2xtyt+ι(B2xtxt−B2ytyt+2B1xtyt))|O,υ11=14(B1xtxt+B1ytyt+ι(B2xtxt+B2ytyt))|O,υ20=18(B1xtxt−B1ytyt+2B2xtyt+ι(B2xtxt−B2ytyt−2B1xtyt))|O,υ21=116(B1xtxtxt+B1ytytyt+B2xtxtyt+B2ytytyt+ι(B2xtxtxt+B2xtytyt−B1xtxtyt−B1ytytyt))|O. | (3.26) |
So, the computation yields
υ02=14(s11−s13+s22+ι(s21−s23+s12)),υ11=12(s11+s13+ι(s21+s23)),υ20=14(s11−s13+s22+ι(s21−s23−s12)), υ21=0. | (3.27) |
Finally, from (3.25) and (3.27), if we get that Γ≠0 as (α,β,ν,r,K,E,s)∈NB|L3, then, at L3, the discrete fishery model (1.14) undergo Neimark-Sacker bifurcation. In addition, supercritical (resp. subcritical) Neimark-Sacker bifurcation occurs if Γ<0 (resp. Γ>0).
Remark 1. The Neimark-Sacker bifurcation has important biological implications in prey-predator models. In these models, the Neimark-Sacker bifurcation indicates the beginning of periodic decreases and increases in the populations of the predator and prey species. It has similar cycles: as the prey population grows, more predators become available, which, in turn, leads to a decline in the prey population, and so on. Because of the complex and reciprocal links that exist between various species, this pattern emerges.
Finally, if (2.33) holds, then the eigenvalues of V|L3 at L3 satisfy that λ1|(2.33)=−1, but
λ2|(2.33)={(3Ksβ+αr)(νβ+αr−αE)(rKs−rν−KsE)−(r(νβ+αr−αE)−α(rKs−rν−KsE))2−(r(νβ+αr−αE)+α(rKs−rν−KsE))×√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−(4Ksβ(νβ+αr−αE)(rKs−rν−KsE))}(Ksβ+αr)(νβ+αr−αE)(rKs−rν−KsE)≠1 or −1, | (3.28) |
which confirms that the discrete fishery model (1.14) may undergo flip bifurcation if (r,s,K,E,α,β,ν) belongs in the following set:
FB|L3={(r,s,K,E,α,β,ν), h={r(νβ+αr−αE)+α(rKs−rν−KsE)×√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE)}. | (3.29) |
But, the following theorem shows that flip bifurcation must exist if (r,s,K,E,α,β,ν)∈FB|L3.
Theorem 3.3. At L3, flip bifurcation exists if (r,s,K,E,α,β,ν)∈FB|L3.
Proof. Since (r,s,K,E,α,β,ν)∈FB|L3, the discrete fishery model (1.14) takes the form of (3.9) if h is in a neighborhood of h∗. Additionally, fishery model (1.14) becomes
ut+1=^Ψ11ut+^Ψ12vt+^Ψ13u2t+^Ψ14utvt+^Ψ15v2t+τ01utϵ+τ02vtϵ+τ03u2tϵ+τ04utvtϵ+τ05v2tϵ,vt+1=^Ψ21ut+^Ψ22vt+^Ψ23u2t+^Ψ24utvt+^Ψ25v2t+τ06utϵ+τ07vtϵ+τ08u2tϵ+τ09utvtϵ+τ10v2tϵ, | (3.30) |
where
^Ψ11=1−Eh+rh−2hrKx∗−βhy∗, ^Ψ12=−βhx∗, ^Ψ13=−βh,^Ψ14=−hrK, ^Ψ15=0, τ01=r−E−2rx∗K−βy∗, τ02=−βx∗,τ03=−hrK, τ04=−β, τ05=0, ^Ψ21=shy∗, ^Ψ22=1−νh+shx∗−2αhy∗,^Ψ23=0, ^Ψ24=sh, ^Ψ25=−αh, τ06=sy∗, τ07=sx∗−ν−2αy∗,τ08=0, τ09=s, τ10=−α | (3.31) |
by (3.15). Moreover, system (3.30) becomes
(xt+1yt+1)=(−100λ2)(xtyt)+(^B1(ϵ)^B2(ϵ)), | (3.32) |
where
^B1(ϵ)=^Ψ13(λ2−^Ψ11)−^Ψ12^Ψ23^Ψ12(1+λ2)u2t+^Ψ14(λ2−^Ψ11)−^Ψ12^Ψ24^Ψ12(1+λ2)utvt+^Ψ15(λ2−^Ψ11)−^Ψ12^Ψ25^Ψ12(1+λ2)v2t+τ01(λ2−^Ψ11)−^Ψ12τ06^Ψ12(1+λ2)utϵ+τ02(λ2−^Ψ11)−^Ψ12τ07^Ψ12(1+λ2)vtϵ+τ03(λ2−^Ψ11)−^Ψ12τ08^Ψ12(1+λ2)u2tϵ+τ04(λ2−^Ψ11)−^Ψ12τ09^Ψ12(1+λ2)utvtϵ+τ05(λ2−^Ψ11)−^Ψ12τ10^Ψ12(1+λ2)v2tϵ,^B2(ϵ)=^Ψ13(1+^Ψ11)+^Ψ12^Ψ23^Ψ12(1+λ2)u2t+^Ψ14(1+^Ψ11)+^Ψ12^Ψ24^Ψ12(1+λ2)utvt+^Ψ15(1+^Ψ11)+^Ψ12^Ψ25^Ψ12(1+λ2)v2t+τ01(1+^Ψ11)+^Ψ12τ06^Ψ12(1+λ2)utϵ+τ02(1+^Ψ11)+^Ψ12τ07^Ψ12(1+λ2)vtϵ+τ03(1+^Ψ11)+^Ψ12τ08^Ψ12(1+λ2)u2tϵ+τ04(1+^Ψ11)+^Ψ12τ09^Ψ12(1+λ2)utvtϵ+τ05(1+^Ψ11)+^Ψ12τ10^Ψ12(1+λ2)v2tϵ,ut=^Ψ12xt+^Ψ12yt,vt=−(1+^Ψ11)xt+(λ2−^Ψ11)yt,u2t=^Ψ122(x2t+2xtyt+y2t),v2t=(1+^Ψ11)2x2t+(λ2−^Ψ11)2y2t−2(1+^Ψ11)(λ2−^Ψ11)xtyt,utvt=−^Ψ12(1+^Ψ11)x2t+(^Ψ12(λ2−^Ψ11)−^Ψ12(1+^Ψ11))xtyt+^Ψ12(λ2−^Ψ11)y2t,utϵ=^Ψ12xtϵ+^Ψ12ytϵ,vtϵ=−(1+^Ψ11)xtϵ+(λ2−^Ψ11)ytϵ,u2tϵ=ϵ^Ψ122(x2t+2xtyt+y2t),v2tϵ=(1+^Ψ11)2x2tϵ+(λ2−^Ψ11)2y2tϵ−2(1+^Ψ11)(λ2−^Ψ11)xtytϵ,utvtϵ=−^Ψ12(1+^Ψ11)x2tϵ+(^Ψ12(λ2−^Ψ11)−^Ψ12(1+^Ψ11))xtytϵ+^Ψ12(λ2−^Ψ11)y2tϵ | (3.33) |
by
(utvt):=(^Ψ12^Ψ12−1−^Ψ11λ2−^Ψ11)(xtyt). | (3.34) |
Now, in a small neighborhood of ϵ, the center manifold McO at O for the map (3.32) is studied. Precisely, McO at O can be expressed as
McO={(xt,yt):yt=R0ϵ+R1x2t+R2xtϵ+R3ϵ3+O((|xt|+|ϵ|)3)}, | (3.35) |
where, by computation, one gets
R0=0,R1=(1+^Ψ11)1−λ22(^Ψ12^Ψ13−(1+^Ψ11)^Ψ14−^Ψ12^Ψ24)+(1+Ψ11)21−λ22^Ψ25,R2=(τ01−τ07)(1+^Ψ11)^Ψ12+τ06^Ψ122−τ02(1+^Ψ11)2^Ψ12(1−λ22),R3=0. | (3.36) |
So, the map (3.32), restricted to McO, can be expressed as
f1(xt)=−xt+l1x2t+l2xtϵ+l3x2tϵ+l4xtϵ2+l5x3t+O((|xt|+|ϵ|)4), | (3.37) |
where
l1=11+λ2[^Ψ12^Ψ13(λ2−^Ψ11)−(1+^Ψ11)(^Ψ14(λ2−^Ψ11)−^Ψ12^Ψ24)−^Ψ25(1+^Ψ11)2],l2=1(1+λ2)[(τ01(λ2−^Ψ11)−τ06^Ψ12)−(1+^Ψ11)(τ02(λ2−^Ψ11)−^Ψ12τ07)^Ψ12],l3=1^Ψ12(1+λ2)[2R2^Ψ122(^Ψ13(λ2−^Ψ11)−^Ψ12^Ψ23)+R2^Ψ12((λ2−^Ψ11)−(1+^Ψ11))(^Ψ14(λ2−^Ψ11)−^Ψ12^Ψ24)))+(τ01(λ2−^Ψ11)−^Ψ12τ06)R1^Ψ12+R1(λ2−^Ψ11)(τ02(λ2−^Ψ11)−^Ψ12τ07)+(τ03(λ2−^Ψ11)−^Ψ12τ08)^Ψ122−^Ψ12(1+^Ψ11)(τ04(λ2−^Ψ11)−^Ψ122τ09)−2R2(1+^Ψ12)(λ2−^Ψ12)(^Ψ15(λ2−^Ψ11−^Ψ12^Ψ25))+(1+^Ψ11)2(τ05(λ2−^Ψ11−^Ψ12τ10))],l4=R2(1+λ2)^Ψ12[(^Ψ12(τ01(λ2−^Ψ11)−^Ψ12τ06))+(λ2−^Ψ11)(τ02(λ2−^Ψ11)−^Ψ12τ07)],l5=R1^Ψ12(1+λ2)[^Ψ12(λ2−2^Ψ11−1)(^Ψ14(λ2−^Ψ11)−^Ψ12^Ψ24)−2(1+^Ψ11)(λ2−^Ψ11)(^Ψ15(λ2−^Ψ11)−^Ψ12^Ψ25)]. | (3.38) |
Finally, the following non-zero discriminatory quantities imply that map (3.37) undergoes flip bifurcation [32,33,34]:
ϵ1=(f1xtϵ+12f1ϵf1xtxt)|(0,0),ϵ2=(16f1xtxtxt+(12f1xtxt)2)|(0,0). | (3.39) |
After extensive manipulation, one gets
ϵ1=1λ2{α(rKs−rν−KsE)(Ksβ+αr)(1−λ2)+h(Ksβ+αr)(rKs−rν−KsE)(νβ+αr−αE)}(Ksβ+αr)2+1λ2{rh(νβ+αr−αE)−2(Ksβ+αr)}{Kβh(νβ+αr−αE)}×{Kβ(Ksβ+αr)(νβ+αr−αE)(1−λ2)−Krhβ(νβ+αr−αE)2−Khαβ(νβ+αr−αE)(rKs−rν−KsE)}(Ksβ+αr)2≠0 | (3.40) |
and
ϵ2=11+λ2{(λ2−1)h2rβ(Ksβ+αr)(νβ+αr−αE)+h3r2β(νβ+αr−αE)2(2βh(Ksβ+αr)−h2rβ(νβ+αr−αE))((Ksβ+αr)(λ2−1)+rh(νβ+αr−αE))−2Ksβh2(Ksβ+αr)(νβ+αr−αE)+Ksβh3r(νβ+αr−αE)2+αh[2(Ksβ+αr)−rh(νβ+αr−αE)]2}(Ksβ+αr)2+R11+λ2{{(λ2−3)(Ksβ+αr)+2rh(νβ+αr−αE)}×{βh(Ksβ+αr)(1−λ2)+βh2(νβ+αr−αE)(Ks+r)}+{3(Ksβ+αr)−2rh(νβ+αr−αE)}×{αh(Ksβ+αr)(1−λ2)+αh2r(νβ+αr−αE)}}(Ksβ+αr)2, | (3.41) |
where
R1=11−λ22{(βh(νβ+αr−αE))(2(Ksβ+αr)−rh(νβ+αr−αE))(rh+shK)+(2(Ksβ+αr)−rh(νβ+αr−αE))2(βh−αh)}(Ksβ+αr)2,λ2={(3Ksβ+αr)(νβ+αr−αE)(rKs−rν−KsE)−(r(νβ+αr−αE)−α(rKs−rν−KsE))2−(r(νβ+αr−αE)+α(rKs−rν−KsE))×√r(νβ+αr−αE)−α(rKs−rν−KsE)2−4Ksβ(νβ+αr−αE)(rKs−rν−KsE)}(Ksβ+αr)(νβ+αr−αE)(rKs−rν−KsE). | (3.42) |
Therefore, from (3.41), along with (3.42), if ϵ2≠0 as (α,β,ν,r,s,K,E)∈FB|L3, then, at L3, fishery model (1.14) undergoes flip bifurcation. Additionally, by the bifurcation theory [35,36,37], if ϵ2>0 (resp. ϵ2<0), then period-2 points bifurcated from L3 are stable (resp. unstable).
Remark 2. We are choosing the step size, represented by the symbol h, as the bifurcation parameter, and it is significant. This is because h represents the time interval between successive iterations in a discrete-time model. By changing the value of h, we can simulate different rates at which populations of prey and predators change over time. Biologically, h reflects the reproductive and growth rates of these populations. A smaller value of h means that we have a finer time resolution, allowing for more frequent population size updates. This can help to capture rapid population changes, such as fast reproduction or predation events, and to provide a more detailed representation of the dynamics. A larger value of h means that we have a coarser time resolution, with fewer updates of the population sizes. This can be useful in scenarios in which the population changes occur over longer time scales, such as seasonal variations or slower ecological processes. A larger value of h can help to capture the overall trends and dynamics of the populations. By varying the step size as the bifurcation parameter, we can explore how different rates of population change affect the stability and bifurcation behavior of the system. This can provide insights into the resilience of the ecological system and its response to changes in reproductive rates, predation rates or other important ecological processes. In summary, choosing the step size h as the bifurcation parameter in a discretized prey-predator system with harvesting allows us to analyze how different rates of population change influence the system's dynamics. This can have biological significance as a result of capturing the effects of reproductive and growth rates on the stability and behavior of the ecological system.
Hereafter, chaos control is studied by adding ut as the control force to fishery model (1.14), as motivated by the existing literature [38,39]:
xt+1=(1−Eh+rh)xt−hrKx2t−βhxtyt+ut, yt+1=(1−hν)yt+shxtyt−αhy2t, | (3.43) |
where
ut=−k1(xt−x)−k2(yt−y), |
k1, k2 denotes feedback gains and
x=K(νβ+αr−αE)Ksβ+αr, y=rKs−rν−KsEKsβ+αr. |
Moreover, VC|L3 at L3 for control system (3.43) becomes
VC|L3=(ℓ11−k1ℓ12−k2ℓ21ℓ22), | (3.44) |
where
ℓ11=Ksβ+αr−rh(νβ+αr−αE)Ksβ+αr, ℓ12=−βhK(νβ+αr−αE)Ksβ+αr,ℓ21=sh(rKs−rν−KsE)Ksβ+αr, ℓ22=Ksβ+αr−αh(rKs−rν−KsE)Ksβ+αr. | (3.45) |
Next, if λ1,2 are roots of VC|L3 at L3, then
λ1+λ2=ℓ11+ℓ22−k1, | (3.46) |
λ1λ2=ℓ22(ℓ11−k1)−ℓ21(ℓ12−k2). | (3.47) |
Theorem 3.4. Controlled system (3.43) is asymptotically stable if both eigenvalues of VC|L3 at L3 satisfy that |λ1,2|<1 where k1 and k2 denote the feedback gains.
Proof. See in Appendix F.
To validate the theoretical findings, the following simulations are presented.
Case A: Let
α=1.42, β=2.30, ν=1.017, r=3.82, s=2.1, K=3.07andE=0.75, |
then, from (2.30), we obtain that
h=1.5509052171807427, |
which implies that, if
0<h<1.5509052171807427, |
then L3 of fishery model (1.14) is a stable focus. Further, if
h=1.446<1.5509052171807427, |
then Figure 1a shows that
L3=(0.59172285875895,0.15888591788295456) |
of the discrete fishery model (1.14) is a stable focus. Also, if
h=1.447,1.4476,1.44775,1.447753,1.44775345<1.5509052171807427, |
then Figure 1b–1f shows that the corresponding equilibrium L3 of fishery model (1.14) is a stable focus.
On the other hand, if
h=1.56>1.5509052171807427, |
then Figure 2a shows that the interior fixed point
L3=(0.59172285875895,0.15888591788295456) |
changes the dynamics and, as a result, stable curves appear. Now, we further numerically prove that, if
h=1.56>1.5509052171807427, |
then the discrete fishery model (1.14) undergoes supercritical Neimark-Sacker bifurcation, that is, Γ<0. So, if h=1.56, then, from (3.13), we obtain
d|λ1,2|dϵ|ϵ=0=0.9618985638039548>0. |
Additionally, from (3.10) and (3.27), one has
λ1,2=0.24971912023291512±0.9728514382264002ι, | (4.1) |
and
υ02=−2.1078848913821764+1.4116762802263008ι,υ11=−0.5703582999144139+3.2331175862335613ι,υ20=−2.1078848913821764−0.33361919995186096ι,υ21=0. | (4.2) |
Applying (4.1) and (4.2) in (3.25), one gets
Γ=−10.963304854495894<0, |
which confirms that our findings are numerically true; so fishery model (1.14) undergoes supercritical Neimark-Sacker bifurcation. Similarly, if
1.564,1.565,1.59,1.6,1.62>1.5509052171807427, |
Figure 2b–2f implies that stable curves also appear, and therefore, the discrete fishery model (1.14) undergoes supercritical Neimark-Sacker bifurcation. If
1.564,1.565,1.59,1.6,1.62>1.5509052171807427, |
then Γ<0 (see Table 1).
Certain values of h if h>1.5509052171807427 | Respective values of Γ |
1.56 | −10.963304854495894<0 |
1.564 | −10.986742612429822<0 |
1.565 | −10.992429264118307<0 |
1.59 | −11.111070997936235<0 |
1.6 | −11.145158489428379<0 |
1.62 | −11.188517048312367<0 |
Finally, the maximum Lyapunov exponent and bifurcation diagrams are plotted in Figure 3.
Case B: Let α=5.8, β=3.0, ν=0.09, r=15.52, s=4.501, K=0.52 and E=0.001; then, from (2.33), we obtain
h={r(νβ+αr−αE)+α(rKs−rν−KsE)+√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE)=0.8768402339312452. |
Moreover, for α=5.8, β=3.0, ν=0.09, r=15.52, s=4.501, K=0.52 and E=0.001, we also get
h={r(νβ+αr−αE)+α(rKs−rν−KsE)−√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE)=0.14039168498087434. |
From a theoretical point of view, the interior fixed point L3 of the discrete two-dimensional fishery model (1.10) is a stable node if
0<h<min{0.8768402339312452,0.14039168498087434}. |
So, if
0<h=0.1<min{0.8768402339312452,0.14039168498087434}, |
then Figure 4a implies that the interior fixed point
L3=(0.48378899881654075,0.3599197040815949) |
of fishery model (1.14) is a stable node. Also, if
h=0.127,0.13,0.135<min{0.8768402339312452,0.14039168498087434}, |
then Figure 4b–4d also implies that
L3=(0.48378899881654075,0.3599197040815949) |
of fishery model (1.14) is also a stable node.
Further, if
h>0.8768402339312452, |
then L3 becomes an unstable node and, meanwhile, flip bifurcation occurs, that is, if
h=0.9>0.8768402339312452, |
then, from (3.40), one gets
ϵ1=−3.979605153624144≠0. |
Moreover, in view of (3.41) and (3.42), one gets
ϵ2=1.359449192759867>0, |
which shows that stable period-2 points bifurcate from
L3=(0.48378899881654075,0.3599197040815949). |
Finally, the maximum Lyapunov exponent and bifurcation diagrams are plotted in Figure 5.
Case C: The results of Section 3 will be verified in this case. For this, if α=5.8, β=3.0, ν=0.09, r=15.52, s=4.501, K=0.52, E=0.001 and h=0.95, then, from (F.1)–(F.3), one gets
L1:1591.5334625453052k1+6986.8991691679485k2+8804.286159826777=0, | (4.3) |
L2:11007.821513298903k1+8542.449074372133k2+95951.97647578613=0, | (4.4) |
L3:7824.754588208292k1−8542.449074372133k2+40678.25195311818=0. | (4.5) |
Therefore, lines (4.3)–(4.5) give the triangular region for (3.43) that satisfies that |λ1,2|<1 (see Figure 6).
In this work, we have examined the local behavior at fixed points, chaos control via the state feedback control method and bifurcations of the fishery model (1.14). Moreover, it is shown that, for all of the model's parameters, the discrete fishery model (1.14) has trivial fixed point; however, it has semitrivial and interior fixed points under certain parametric condition(s). By using linear stability theory, we have examined the local stability at equilibria of the discrete fishery model (1.14). Further, we have also examined the existence of bifurcations at fixed points and proved that, at trivial and semitrivial fixed points, the discrete fishery model (1.14) does not undergo flip bifurcation, whereas, at interior fixed point, model (1.14) undergoes both Neimark-Sacker and flip bifurcations, and we have studied these bifurcations by applying bifurcation theory accordingly. Further, chaos control has been studied by using the state feedback control method. Finally, the main results have been confirmed numerically. Our numerical simulations shows that, at interior fixed point, the discrete fishery model (1.14) undergoes supercritical Neimark-Sacker bifurcation and biologically, the occurrence of supercritical Neimark-Sacker bifurcation means that there exists a periodic or quasiperiodic oscillations between prey and predator populations.
Future work: Bifurcation analysis of the (ⅰ) fractional-order discrete-time prey-predator model (1.14) and (ⅱ) discrete-time prey-predator model (1.14) with time delay, are our next goals of study.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
The authors declare that they have no conflicts of interest regarding the publication of this paper.
If L=(x,y) is a fixed point of fishery model (1.14), then
x=(1−Eh+rh)x−hrKx2−βhxy, y=(1−hν)y+shxy−αhy2. | (A.1) |
After straightforward calculation, from (A.1), one gets
x=K(νβ+αr−αE)Ksβ+αr, y=rKs−rν−KsEKsβ+αr, |
which implies that, if
E<min{νβ+αrα,rKs−rνKs}, |
then
L3=(K(νβ+αr−αE)Ksβ+αr,rKs−rν−KsEKsβ+αr) |
is an interior fixed point of fishery model (1.14). On the other hand, for
(x,y)=(0,0),(K(r−E)r,0). |
Equation (A.1) is satisfied in an identical manner; so, L1,2 respectively denote trivial and semitrivial fixed points of fishery model (1.14).
Recall from (2.6) that, at L1, the characteristic roots of V|L1 are
λ1=1−Eh+rhandλ2=1−hν. |
Therefore, by the stability theory L1, of the fishery model (1.14) is a sink if
|λ1|=|1−Eh+rh|<1, |
and
|λ2|=|1−hν|<1, |
which imply that if
0<h<min{2ν,2E−r}, |
and E>r then L1 is a sink. In similar way, one can obtain that L1 is a source if
h>max{2ν,2E−r}, |
a saddle if
2ν<h<2E−r |
or
2E−r<h<2ν, |
and non-hyperbolic if
h=2E−rorh=2ν. |
From (2.15), if
|λ1|=|1+Eh−rh|<1 |
and
|λ2|=|1−hν+shK(r−E)r|<1, |
i.e.,
0<h<min{2r−E,2rrν−sK(r−E)} |
and
rKs−rνKs<E<r, |
then L2 of fishery model (1.14) is a sink. Similarly, it is also easy to prove that L2 of fishery model (1.14) is a source if (2.17) holds and
h>max{2r−E,2rrν−sK(r−E)}, |
a saddle if (2.17) holds and
2rrν−sK(r−E)<h<2r−E |
or
2r−E<h<2rrν−sK(r−E), |
and, finally, non-hyperbolic if (2.17) holds and
h=2r−Eorh=2rrν−sK(r−E). |
If Δ<0, then the characteristic roots of V|L3 at L3 are
λ1,2={2(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)}2(Ksβ+αr)±ι2√{4{(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)+h2(νβ+αr−αE)(rKs−rν−KsE)}Ksβ+αr−(2(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)Ksβ+αr)2}, |
which yield that, if
|λ1,2|=√{(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)+h2(νβ+αr−αE)(rKs−rν−KsE)}Ksβ+αr<1, |
i.e.,
0<h<r(νβ+αr−αE)+α(rKs−rν−KsE)(νβ+αr−αE)(rKs−rν−KsE) |
then L3 of fishery model (1.14) is a stable focus. In a similar way, one can obtain that L3 of fishery model (1.14) is an unstable focus if
h>r(νβ+αr−αE)+α(rKs−rν−KsE)(νβ+αr−αE)(rKs−rν−KsE) |
and non-hyperbolic if
h=r(νβ+αr−αE)+α(rKs−rν−KsE)(νβ+αr−αE)(rKs−rν−KsE). |
If Δ>0, then the roots are
λ1,2={2(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)}2(Ksβ+αr)±12√{(2(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)Ksβ+αr)2−4{(Ksβ+αr)−rh(νβ+αr−αE)−αh(rKs−rν−KsE)+h2(νβ+αr−αE)(rKs−rν−KsE)}Ksβ+αr}. |
By the linear stability theory, L3 of the discrete of fishery model (1.14) is a stable node if |λ1,2|<1, i.e.,
0<h<min{{r(νβ+αr−αE)+α(rKs−rν−KsE)+√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE),{r(νβ+αr−αE)+α(rKs−rν−KsE)−√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE)}. |
In a similar way, one can also establish that L3 of fishery model (1.14) is an unstable node if
h>max{{r(νβ+αr−αE)+α(rKs−rν−KsE)+√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE),{r(νβ+αr−αE)+α(rKs−rν−KsE)−√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE)}, |
and non-hyperbolic if
h={r(νβ+αr−αE)+α(rKs−rν−KsE)+√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE) |
or
h={r(νβ+αr−αE)+α(rKs−rν−KsE)−√(r(νβ+αr−αE)−α(rKs−rν−KsE))2−4Ksβ(νβ+αr−αE)×(rKs−rν−KsE)}(νβ+αr−αE)(rKs−rν−KsE). |
It is noted that marginal stability can arise from the restrictions λ1=±1 and λ1λ2=1, which imply that |λ1,2|<1. If λ1λ2=1, then, from (3.47), we get
L1:k1(αh(rKs−rν−KsE)(Ksβ+αr)−(Ksβ+αr)2)+k2(sh(rKs−rν−KsE)(Ksβ+αr))+h2(rKs−rν−KsE)(νβ+αr−αE)(Ksβ+αr)−[rh(νβ+αr−αE)+αh(rKs−rν−KsE)](Ksβ+αr)=0. | (F.1) |
If λ1=1, then, from (3.46) and (3.47), we get
L2:k1(αh(rKs−rν−KsE)(Ksβ+αr))+k2(sh(rKs−rν−KsE)(Ksβ+αr))+h2(νβ+αr−αE)(rKs−rν−KsE)(Ksβ+αr)=0. | (F.2) |
Finally, if λ1=−1 then from (3.46) and (3.47) we get
L3:k1(2(Ksβ+αr)2−αh(rKs−rν−KsE)(Ksβ+αr))−k2(sh(rKs−rν−KsE)(Ksβ+αr))−h2(rKs−rν−KsE)(νβ+αr−αE)(Ksβ+αr)+2h(Ksβ+αr)(r(νβ+αr−αE)+α(rKs−rν−KsE))−4(Ksβ+αr)2=0. | (F.3) |
Therefore, from (F.1)–(F.3), lines L1–L3 in the (k1,k2)-plane from the triangular region, which implies that the characteristic roots of controlled system (3.43) satisfy that |λ1,2|<1.
[1] | M. N. Huda, F. D. T. Amijaya, I. Purnamasari, The effect of harvesting activities on prey-predator fishery model with Holling type-Ⅱ in toxicant aquatic ecosystem, Aust. J. Math. Anal. Appl., 17 (2020), 13. |
[2] |
K. Pujaru, T. K. Kar, Impacts of predator-prey interaction on managing maximum sustainable yield and resilience, Nonlinear Anal., 25 (2020), 400–416. https://doi.org/10.15388/namc.2020.25.16657 doi: 10.15388/namc.2020.25.16657
![]() |
[3] |
T. K. Kar, Selective harvesting in a prey-predator fishery with time delay, Math. Comput. Modell., 38 (2003), 449–458. https://doi.org/10.1016/S0895-7177(03)90099-9 doi: 10.1016/S0895-7177(03)90099-9
![]() |
[4] |
H. Liu, H. Yu, C. Dai, Z. Ma, Q. Wang, M. Zhao, Dynamical analysis of an aquatic amensalism model with non-selective harvesting and Allee effect, Math. Biosci. Eng., 18 (2021), 8857–8882. https://doi.org/10.3934/mbe.2021437 doi: 10.3934/mbe.2021437
![]() |
[5] |
A. T. Keong, H. M. Safuan, K. Jacob, Dynamical behaviours of prey-predator fishery model with harvesting affected by toxic substances, Matematika, 34 (2018), 143–151. https://doi.org/10.11113/matematika.v34.n1.1018 doi: 10.11113/matematika.v34.n1.1018
![]() |
[6] |
M. Chen, R. Wu, X. Wang, Non-constant steady states and Hopf bifurcation of a species interaction model, Commun. Nonlinear Sci. Numer. Simul., 116 (2023), 106846. https://doi.org/10.1016/j.cnsns.2022.106846 doi: 10.1016/j.cnsns.2022.106846
![]() |
[7] |
M. Chen, R. Wu, Patterns in the predator-prey system with network connection and harvesting policy, Math. Methods Appl. Sci., 46 (2023), 2433–2454. https://doi.org/10.1002/mma.8653 doi: 10.1002/mma.8653
![]() |
[8] |
M. Chen, R. Wu, Dynamics of a harvested predator-prey model with predator-taxis, Bull. Malays. Math. Sci. Soc., 46 (2023), 76. https://doi.org/10.1007/s40840-023-01470-w doi: 10.1007/s40840-023-01470-w
![]() |
[9] |
M. Chen, H. Srivastava, Existence and stability of bifurcating solution of a chemotaxis model, Proc. Amer. Math. Soc., 151 (2023), 4735–4749. https://doi.org/10.1090/proc/16536 doi: 10.1090/proc/16536
![]() |
[10] |
M. Chen, H. M. Srivastava, Stability of bifurcating solution of a predator-prey model, Chaos Solitons Fract., 168 (2023), 113153. https://doi.org/10.1016/j.chaos.2023.113153 doi: 10.1016/j.chaos.2023.113153
![]() |
[11] |
S. M. Salman, A. M. Yousef, A. A. Elsadany, Stability, bifurcation analysis and chaos control of a discrete predator-prey system with square root functional response, Chaos Solitons Fract., 93 (2016), 20–31. https://doi.org/10.1016/j.chaos.2016.09.020 doi: 10.1016/j.chaos.2016.09.020
![]() |
[12] |
X. Liu, D. Xiao, Complex dynamic behaviors of a discrete-time predator-prey system, Chaos Solitons Fract., 32(2007), 80–94. https://doi.org/10.1016/j.chaos.2005.10.081 doi: 10.1016/j.chaos.2005.10.081
![]() |
[13] |
M. F. Elettreby, T. Nabil, A. Khawagi, Stability and bifurcation analysis of a discrete predator-prey model with mixed Holling interaction, Comput. Model. Eng. Sci., 122 (2020), 907–922. https://doi.org/10.32604/cmes.2020.08664 doi: 10.32604/cmes.2020.08664
![]() |
[14] |
P. K. Santra, G. S. Mahapatra, G. R. Phaijoo, Bifurcation and chaos of a discrete predator-prey model with Crowley-Martin functional response incorporating proportional prey refuge, Math. Probl. Eng., 2020 (2020), 5309814. https://doi.org/10.1155/2020/5309814 doi: 10.1155/2020/5309814
![]() |
[15] |
G. Zhang, L. Zhu, B. Chen, Hopf bifurcation in a delayed differential-algebraic biological economic system, Nonlinear Anal., 12 (2011), 1708–1719. https://doi.org/10.1016/j.nonrwa.2010.11.003 doi: 10.1016/j.nonrwa.2010.11.003
![]() |
[16] |
L. Zhang, L. Zou, Bifurcations and control in a discrete predator-prey model with strong Allee effect, Int. J. Bifurc. Chaos, 28 (2018), 1850062. https://doi.org/10.1142/S0218127418500621 doi: 10.1142/S0218127418500621
![]() |
[17] |
P. Chakraborty, U. Ghosh, S. Sarkar, Stability and bifurcation analysis of a discrete prey-predator model with square-root functional response and optimal harvesting, J. Biol. Syst., 28 (2020), 91–110. https://doi.org/10.1142/S0218339020500047 doi: 10.1142/S0218339020500047
![]() |
[18] |
D. Mua, C. Xub, Z. Liua, Y. Panga, Further insight into bifurcation and hybrid control tactics of a chlorine dioxide-iodine-malonic acid chemical reaction model incorporating delays, MATCH Commun. Math. Comput. Chem., 89 (2023), 529–566. https://doi.org/10.46793/match.89-3.529M doi: 10.46793/match.89-3.529M
![]() |
[19] |
C. Xu, X. Cui, P. Li, J. Yan, L. Yao, Exploration on dynamics in a discrete predator-prey competitive model involving feedback controls, J. Biol. Dyn., 17 (2023), 2220349. https://doi.org/10.1080/17513758.2023.2220349 doi: 10.1080/17513758.2023.2220349
![]() |
[20] |
C. Xu, Z. Liu, P. Li, J. Yan, L. Yao, Bifurcation mechanism for fractional-order three-triangle multi-delayed neural networks, Neural Process. Lett., 55 (2023), 6125–6151. https://doi.org/10.1007/s11063-022-11130-y doi: 10.1007/s11063-022-11130-y
![]() |
[21] |
C. Xu, D. Mu, Y. Pan, C. Aouiti, L. Yao, Exploring bifurcation in a fractional-order predator-prey system with mixed delays, J. Appl. Anal. Comput., 13 (2023), 1119–1136. https://doi.org/10.11948/20210313 doi: 10.11948/20210313
![]() |
[22] |
P. Li, Y. Lu, C. Xu, J. Ren, Insight into hopf bifurcation and control methods in fractional order bam neural networks incorporating symmetric structure and delay, Cogn. Comput., 15 (2023), 1825–1867. https://doi.org/10.1007/s12559-023-10155-2 doi: 10.1007/s12559-023-10155-2
![]() |
[23] |
C. Xu, Q. Cui, Z. Liu, Y. Pan, X. Cui, W. Ou, et al., Extended hybrid controller design of bifurcation in a delayed chemostat model, MATCH Commun. Math. Comput. Chem., 90 (2023), 609–648. https://doi.org/10.46793/match.90-3.609X doi: 10.46793/match.90-3.609X
![]() |
[24] |
P. Li, X. Peng, C. Xu, L. Han, S. Shi, Novel extended mixed controller design for bifurcation control of fractional-order Myc/E2F/miR-17-92 network model concerning delay, Math. Methods Appl. Sci., 46 (2023), 18878–18898. https://doi.org/10.1002/mma.9597 doi: 10.1002/mma.9597
![]() |
[25] |
Y. Zhang, P. Li, C. Xu, X. Peng, R. Qiao, Investigating the effects of a fractional operator on the evolution of the enso model: bifurcations, stability and numerical analysis, Fractal Fract., 7 (2023), 602. https://doi.org/10.3390/fractalfract7080602 doi: 10.3390/fractalfract7080602
![]() |
[26] | K. H. Hntsa, Z. T. Mengesha, Mathematical modelling of fish resources harvesting with predator at maximum sustainable yield, Int. J. Integr. Sci. Innovation Technol., 5 (2016), 7–24. |
[27] | J. Guckenheimer, P. Holmes, Nonlinear oscillations, dynamical systems and bifurcation of vector fields, Springer, 1983. https://doi.org/10.1007/978-1-4612-1140-2 |
[28] | Y. A. Kuznetsov, Elements of applied bifurcation theorey, Springer, 2004. https://doi.org/10.1007/978-1-4757-3978-7 |
[29] |
W. Liu, D. Cai, Bifurcation, chaos analysis and control in a discrete-time predator-prey system, Adv. Differ. Equations, 2019 (2019), 11. https://doi.org/10.1186/s13662-019-1950-6 doi: 10.1186/s13662-019-1950-6
![]() |
[30] |
Y. Liu, X. Li, Dynamics of a discrete predator-prey model with Holling-Ⅱ functional response, Int. J. Biomath., 14 (2021), 2150068. https://doi.org/10.1142/S1793524521500686 doi: 10.1142/S1793524521500686
![]() |
[31] |
Q. Shu, J. Xie, Stability and bifurcation analysis of discrete predator-prey model with nonlinear prey harvesting and prey refuge, Math. Methods Appl. Sci., 45 (2022), 3589–3604. https://doi.org/10.1002/mma.8005 doi: 10.1002/mma.8005
![]() |
[32] |
P. K. Santra, H. S. Panigoro, G. S. Mahapatra, Complexity of a discrete-time predator-prey model involving prey refuge proportional to predator, Jambura J. Math., 4 (2022), 50–63. https://doi.org/10.34312/jjom.v4i1.11918 doi: 10.34312/jjom.v4i1.11918
![]() |
[33] |
M. Chen, R. Wu, H. Liu, X. Fu, Spatiotemporal complexity in a Leslie-Gower type predator-prey model near Turing-Hopf point, Chaos Solitons Fract., 153 (2021), 111509. https://doi.org/10.1016/j.chaos.2021.111509 doi: 10.1016/j.chaos.2021.111509
![]() |
[34] |
A. Q. Khan, M. B. Javaid, Discrete-time phytoplankton-zooplankton model with bifurcations and chaos, Adv. Differ. Equations, 2021 (2021), 415. https://doi.org/10.1186/s13662-021-03523-5 doi: 10.1186/s13662-021-03523-5
![]() |
[35] |
A. Q. Khan, J. Ma, D. Xiao, Bifurcations of a two-dimensional discrete time plant-herbivore system, Commun. Nonlinear Sci. Numer. Simul., 39 (2016), 185–198. https://doi.org/10.1016/j.cnsns.2016.02.037 doi: 10.1016/j.cnsns.2016.02.037
![]() |
[36] |
A. Q. Khan, J. Ma, D. Xiao, Global dynamics and bifurcation analysis of a host-parasitoid model with strong Allee effect, J. Biol. Dyn., 11 (2017), 121–146. https://doi.org/10.1080/17513758.2016.1254287 doi: 10.1080/17513758.2016.1254287
![]() |
[37] |
M. Parsamanesh, M. Erfanian, Stability and bifurcations in a discrete-time SIVS model with saturated incidence rate, Chaos Solitons Fract., 150 (2021), 111178. https://doi.org/10.1016/j.chaos.2021.111178 doi: 10.1016/j.chaos.2021.111178
![]() |
[38] | S. N. Elaydi, An Introduction to difference equations, Springer-Verlag, 1996. https://doi.org/10.1007/0-387-27602-5 |
[39] | S. Lynch, Dynamical systems with applications using mathematica, Birkhäuser, 2007. https://doi.org/10.1007/978-0-8176-4586-1 |
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Certain values of h if h>1.5509052171807427 | Respective values of Γ |
1.56 | −10.963304854495894<0 |
1.564 | −10.986742612429822<0 |
1.565 | −10.992429264118307<0 |
1.59 | −11.111070997936235<0 |
1.6 | −11.145158489428379<0 |
1.62 | −11.188517048312367<0 |