in

Persistence and size of seasonal populations on a consumer–resource relationship depends on the allocation strategy toward life-history functions

The long-term population dynamics (i.e., extinction or persistence in an equilibrium value) of the system (2) is mainly dependent on the constant allocation of energy between life-history functions. In the case of population persistence, there is a unique long-term allocation strategy towards reproductive functions that maximizes the population abundance and minimizes individual consumption. In addition, this strategy is dependent on the parameters associated with both fertility ((kappa ) and ({mathscr {B}}_0)) and survival ((xi _{c}) and (e_{1/2})) costs.

Preliminary results

To investigate long-term dynamic patterns, we will relate the energy states of reproduction and maintenance, resource density and population abundance at the end of reproductive seasons, namely in the time sequence ({ntau ^+}_{nge 0}). In the system (4) the relationships between the state variables are the same for each (tau ) unit of time. Then, there is a transformation that relates to the vector ( (R,E_ {r}, E_ {m},P) ((n + 1)tau ^+) ) with ( (R,E_ {r}, E_ {m}, P) (n tau ^+) ) such that ( (n + 1) tau ^+ – ntau ^+ = tau ). This relationship is determined by the following discretization (or stroboscopic map) of the impulsive differential system (4):

$$begin{aligned} left{ begin{array}{lll} E_{r}((n+1)tau ^+)&=(1-kappa gamma )[E_{r}(ntau ^+)+alpha Phi (n,P(ntau ^+))], &{}&{} E_{m}((n+1)tau ^+)&=dfrac{{mathscr {B}}_0[E_{m}(ntau ^+)+(1-alpha )xi _{c}Phi (n,P(ntau ^+))]}{{mathscr {B}}_0+gamma [E_{r}(ntau ^+)+alpha Phi (n,P(ntau ^+))]}, P((n+1)tau ^+)&=left{ 1-mu +dfrac{gamma [E_{r}(ntau ^+)+alpha Phi (n,P(ntau ^+))]E_{m}((n+1)tau ^+)}{e_{1/2}+E_{m}((n+1)tau ^+)}right} P(ntau ^+)e^{-lambda tau } end{array} right. end{aligned}$$

(6)

and (R(ntau ^+)=K), where the function (Phi ) defined by (5) is evaluated at (t=(n+1)tau ) and extended to (p=0):

$$begin{aligned} Phi (n,p)=left{ begin{array}{ll} dfrac{R_{max}(e^{lambda tau }-1)}{lambda }, &quad text {if}, p=0, &{} dfrac{K-R((n+1)tau )e^{lambda tau }}{p}+dfrac{lambda }{p}displaystyle int _{ntau }^{(n+1)tau }{R(s)e^{lambda (s-ntau )}ds}, & quad text {if}, pne 0, end{array} right. end{aligned}$$

(7)

for any (nge 0). Indeed, in non-reproductive seasons the consumer–resource dynamics are described by the continuous component of the system (4), which can be solved. Directly we have (P(t)=P(ntau ^+)e^{-lambda (t-ntau )}) for any (tin (ntau ,(n+1)tau ]). In addition, the per capita consumption rate (1) can be expressed in terms of ( R'(t)). Therefore, reproductive and maintenance energy rates are determined by

$$begin{aligned} E_r'(t)=-alpha frac{R'(t)e^{lambda (t-ntau )}}{P(ntau ^+)}quad text {and}quad E_m'(t)=-(1-alpha )xi _{c}frac{R'(t)e^{lambda (t-ntau )}}{P(ntau ^+)},quad tin (ntau ,(n+1)tau ]. end{aligned}$$

Integrating these functions in the interval ( (n tau , t] ), we obtain

$$begin{aligned} E_r(t)&= {} E_{r}(ntau ^+)+alpha Phi (t,R(t),P(ntau ^+)) end{aligned}$$

(8)

$$begin{aligned} E_m(t)&= {} E_m(ntau ^+)+(1-alpha )xi _{c}Phi (t,R(t),P(ntau ^+)). end{aligned}$$

(9)

Evaluating Eqs. (8)–(9) at ( t = (n + 1)tau ) (end of the non-reproductive season), we have

$$begin{aligned} E_r((n+1)tau )&= {} E_{r}(ntau ^+)+alpha Phi (n,P(ntau ^+)), end{aligned}$$

(10)

$$begin{aligned} E_m(n+1)tau )&= {} E_m(ntau ^+)+(1-alpha )xi _{c}Phi (n,P(ntau ^+)), end{aligned}$$

(11)

with (Phi (n,P(ntau ^+))= Phi ((n+1)tau ,R((n+1)tau ),P(ntau ^+))) and (P((n+1)tau )=P(ntau ^+)e^{-lambda tau }) for any (nge 0). In addition, evaluating the discrete component of system (4) at (t=(n+1)tau ), we obtain

$$begin{aligned} E_{r}((n+1)tau ^+)&= {} (1-kappa gamma )E_{r}((n+1)tau ), end{aligned}$$

(12)

$$begin{aligned} E_m((n+1)tau ^+)&= {} frac{{mathscr {B}}_0E_m((n+1)tau )}{{mathscr {B}}_0+gamma E_r((n+1)tau )}, end{aligned}$$

(13)

$$begin{aligned} P((n+1)tau ^+)= & {} left[ 1-mu +gamma E_{r}((n+1)tau )frac{E_{m}((n+1)tau ^+)}{e_{1/2}+E_{m}((n+1)tau ^+)}right] P((n+1)tau ). end{aligned}$$

(14)

Finally, substituting the Eqs. (10)–(11) into the Esq. (12)–(14) we obtain the discretization given by Eq. (6).

In order to obtain the equilibrium points of system (6), we can solve the following equations:

$$begin{aligned} e_{r}&= {} (1-kappa gamma )[e_{r}+alpha Phi (rho )], e_{m}&= {} dfrac{{mathscr {B}}_{0}[e_{m}+(1-alpha )xi _{c}Phi (rho )]}{{mathscr {B}}_0+gamma [e_{r}+alpha Phi (rho )]}, rho&= {} left{ 1-mu +gamma [e_{r}+alpha Phi (rho )]dfrac{e_{m}}{e_{1/2}+e_{m}}right} rho e^{-lambda tau }, end{aligned}$$

where (e_{r}:=lim _{nrightarrow +infty }{E_{r}(ntau ^+)}), (e_{m}:=lim _{nrightarrow +infty }{E_{m}(ntau ^+)}), (rho :=lim _{nrightarrow +infty }{P(ntau ^+)}) and then, (Phi (rho ):=lim _{nrightarrow +infty }{Phi (n,P(ntau ^+))}). From the first equation, we have (e_{r}=(1-kappa gamma )alpha Phi (P)/kappa gamma ) and then (e_{m}=kappa {mathscr {B}}_0 (1-alpha )xi _{c}/alpha ) for (Pin {0,rho }) such that (Phi (0)=R_{max}(e^{lambda tau }-1)/lambda ) and

$$begin{aligned} Phi (rho )={mathscr {A}},quad text {where}quad {mathscr {A}}=dfrac{e^{lambda tau }-1+mu }{{mathscr {B}}_0}cdot left{ dfrac{e_{1/2}xi _{c}^{-1}}{1-alpha } +dfrac{kappa {mathscr {B}}_0}{alpha }right} . end{aligned}$$

(15)

Therefore, assuming (lambda =0), we have (Gamma (rho )=K-{mathscr {A}}rho ) (from equations (7) and (15)) where (Gamma :=lim _{nrightarrow +infty }{R((n+1)tau )}), (rho ) is the solution of

$$begin{aligned} r_0ln left( dfrac{K-{mathscr {A}}rho }{K}right) -{mathscr {A}}=-R_{max}tau , end{aligned}$$

if, and only if,

$$begin{aligned} rho =dfrac{K}{{mathscr {A}}}left[ 1-exp left( dfrac{{mathscr {A}}-R_{max}tau }{r_0}right) right] . end{aligned}$$

(16)

Long-term population dynamics

From the discretization (6), there are two dynamic behaviors for the long-term population abundance: extinction (see Fig. 2a) and persistence (see Fig. 2b).

Figure 2

Long-term behavior of solutions of the model (4). Peak values correspond to the solution of the discrete model (6) in its population component. (a) Extinction behavior, considering (alpha in {0.1,,0.8}) as energy allocation strategy toward reproductive and (b) persistence behavior considering (alpha in {0.35,, 0.55}). We consider the following parameter set (eta =(2,0.5,2,0.25,500,2,1,0.5,0.5,0.86,alpha ,0.1)) where the constant of fertility costs is described by (kappa =(1+gamma )^{-1}).

Full size image

The differentiation of these behaviors strongly depends on the individual consumption of resources defined throughout each non-reproductive season by

$$begin{aligned} C_{I}(t) = frac{[K-R(t)]e^{lambda (t-ntau )}}{P(ntau ^+)},, tin (ntau ,(n+1)tau ]. end{aligned}$$

At the end of each non-reproductive season, namely at the time ( t = (n + 1) tau ), the individual consumption is given by

$$begin{aligned} C_I((n+1)tau ) = frac{[K-R((n+1)tau )]e^{lambda tau }}{P(ntau ^+)}, end{aligned}$$

(17)

where (R((n+1)tau )) is the non-consumed resource density by the population, the amount that is obtained from the implicit solution of the resource density equation in the continuous component of the system (4). Thus, projecting the individual consumption of the resource into the long term, and taking (Gamma (rho )=(K-{mathscr {A}}rho +lambda {mathscr {I}})e^{-lambda tau }), the expression (17) assumes the form

$$begin{aligned} C_{I}^{infty }(rho )=left{ begin{array}{ll} {mathscr {A}}+dfrac{K(e^{lambda tau }-1)-lambda {mathscr {I}}}{rho },&{}quad text {if}, rho ne 0, &{} dfrac{R_{max}(e^{lambda tau }-1)}{lambda },&{}quad text {if}, rho =0, end{array}right. end{aligned}$$

(18)

where ({mathscr {I}}:=lim _{nrightarrow +infty }{int _{ntau }^{(n+1)tau }{R(s)e^{lambda (s-ntau )}ds}}). On the one hand, the individual consumption ( C_{I}^{infty } ) is composed of a basis amount corresponding to the term ({mathscr {A}} ) and an amount resulting from the equal division of a resource not consumed by individuals dying during the non-reproductive season, ( K(e^{lambda tau } -1) – lambda {mathscr {I}}). Furthermore, when the population experiences a reduced mortality during the non-reproductive season (i.e., ( lambda approx 0) ), the individual consumption is ( C_{I}^{infty } (rho ) approx {mathscr {A}} ). On the other hand, whether the population abundance is low, the per capita resource is high, implying an individual consumption close to (R_ {max} (e^{lambda tau } -1) / lambda ) (equivalent to taking the limit of ( C_{I}((n+1)tau )) as ( P(ntau ^+)rightarrow 0 )). Certainly, this quantity does not represent the effective individual consumption, but rather establishes an upper limit for this and therefore represents a value of non-persistence. Thus, behaviors related to the equilibrium solutions of the discrete system (6) can be differentiated by the threshold value

$$begin{aligned} {mathscr {U}}=dfrac{C_{I}^{infty }(0)}{C_{I}^{infty }(rho )}. end{aligned}$$

In particular, when the mortality of the population is low, the long-term abundance is described by Eq. (16) and the threshold value assumes the following form ({mathscr {U}}=R_{max}tau /{mathscr {A}}). Thus, we conclude that the persistence of the population is established when ({mathscr {U}}>1) and extinction when ({mathscr {U}}le 1).

Finally, we can see that the stabilization of population size in the long term is in response to a dense-dependent behaviour where the per capita growth rate in the long term is (r_{infty }:={alpha {mathscr {A}}/kappa }{mathscr {S}}(e_m)) equivalent to mortality fraction (mu ), where (e_{m}=kappa {mathscr {B}}_{0}(1-alpha )xi _{c}/alpha ) is the equilibrium value of energy maintenance after the reproductive season. In addition, the derivative of r with respect to P is

$$begin{aligned} dfrac{dr}{dP} = gamma dfrac{dPhi }{d P}left{ alpha {mathscr {S}}(E_{m})+(E_{r}+alpha Phi )dfrac{d{mathscr {S}}}{dE_{m}}cdot dfrac{dE_{m}}{dPhi }right} , end{aligned}$$

where (dPhi /d P<0), (dr/d P<0) and (dr/dPhi >0) are obtained, which explains the expected dense-dependency.

Then, we can derive the following conclusion.

Theorem 1

We consider the threshold value ({mathscr {U}}=R_{max}tau /{mathscr {A}}).

  1. 1.

    If ({mathscr {U}}le 1) then the long-term population behavior is extinction.

  2. 2.

    If ({mathscr {U}}>1) then the long-term population behavior is persistence.

Proof

We divide the proof into two cases: (kappa gamma =1) and (0<kappa gamma <1). In the first case we define the functions

$$begin{aligned} G(e_{m},p)&= frac{{mathscr {B}}_0[e_{m}+(1-alpha )xi _{c}Phi (p)]}{{mathscr {B}}_{0}+gamma alpha Phi (p)}, H(e_{m},p) &= left{ 1-mu +gamma alpha Phi (p)frac{G(e_{r},e_{m},p)}{e_{1/2}+G(e_{r},e_{m},p)}right} p. end{aligned}$$

Therefore, the discrete system defined by equations (e_{m}^{k+1}=G(e_{m}^{k},p^{k})) and (p^{k+1}=H(e_{m}^{k},p^{k})) with (kge 0) has two equilibrium solutions: ({mathscr {E}}(P)=(E_{m},P)) where (E_{m}={mathscr {B}}_0 (1-alpha )xi _{c}/alpha gamma ) and (Pin {0,rho }). Thus,

$$begin{aligned} dfrac{partial G}{partial e_m}&= {} dfrac{{mathscr {B}}_0}{{mathscr {B}}_0+gamma alpha Phi (p)}, quad dfrac{partial G}{partial p}=dfrac{{mathscr {B}}_0[{mathscr {B}}_0(1-alpha )xi _{c}-alpha gamma e_{m}]Phi ‘(p)}{{{mathscr {B}}_0+gamma [e_{r}+alpha Phi (p)]}^2}, dfrac{partial H}{partial e_m}= & {} dfrac{gamma e_{1/2}alpha Phi (p)p}{(e_{1/2}+G)^2}cdot dfrac{partial G}{partial e_{m}}, quad dfrac{partial H}{partial p}=1-mu +dfrac{gamma alpha Phi (p)G}{e_{1/2}+G}+dfrac{gamma p}{e_{1/2}+G}left{ alpha Phi ‘(p)G+dfrac{e_{1/2}alpha Phi (p)}{e_{1/2}+G}cdot dfrac{partial G}{partial p}right} , end{aligned}$$

with (Phi ‘(p)=-r_{0}Phi (p)/[r_{0}p+Gamma (p)]) where ((,)’) means the derivative with respect to p. Then, the matrix of linearization around the equilibrium point ({mathscr {E}}(P)) is given by the Jacobian matrix in ({mathscr {E}}(P)),

$$begin{aligned} J({mathscr {E}}(P))=begin{pmatrix} dfrac{{mathscr {B}}_0}{{mathscr {B}}_0+gamma alpha Phi (P)}&{}quad 0 dfrac{gamma alpha e_{1/2}{mathscr {B}}_0{mathscr {A}}P}{(e_{1/2}+E_{m})^{2}({mathscr {B}}_0+gamma alpha {mathscr {A}})}&{}quad 1-dfrac{mu r_0P}{r_0P+K-{mathscr {A}}P} end{pmatrix}. end{aligned}$$

Therefore, ({mathscr {E}}(0)) is uniformly asymptotically stable and ({mathscr {E}}(rho )) is locally asymptotically stable.

In the second case, (0<kappa gamma <1), we define the functions

$$begin{aligned} F(e_{r},e_{m},p)= & {} (1-kappa gamma )[e_{r}+alpha Phi (p)], G(e_{r},e_{m},p)= & {} frac{{mathscr {B}}_0[e_{m}+(1-alpha )xi _{c}Phi (p)]}{{mathscr {B}}_{0}+gamma [e_{r}+alpha Phi (p)]}, H(e_{r},e_{m},p)= & {} left{ 1-mu +gamma [e_{r}+alpha Phi (p)]frac{G(e_{r},e_{m},p)}{e_{1/2}+G(e_{r},e_{m},p)}right} p. end{aligned}$$

Then, the discrete system is defined by equations (e_{r}^{k+1}=F(e_{r}^{k},e_{m}^{k},p^{k})), (e_{m}^{k+1}=G(e_{r}^{k},e_{m}^{k},p^{k})) and (p^{k+1}=H(e_{r}^{k},e_{m}^{k},p^{k})) with (kge 0) which has two equilibrium solutions: ({mathscr {E}}(P)=(E_{r}(P),E_{m},P)) where (E_{r}(P)=(1-kappa gamma )alpha Phi (P)/kappa gamma ), (E_{m}=kappa {mathscr {B}}_0 (1-alpha )xi _{c}/alpha ) and (Pin {0,rho }). Then, (partial F/partial e_r=(1-kappa gamma )), (partial F/partial e_m=0), (partial F/partial p=(1-kappa gamma )alpha Phi ‘(p)), (partial H/partial e_{r}=gamma p G / (e_{1/2}+G)),

$$begin{aligned} dfrac{partial G}{partial e_r}= & {} -dfrac{gamma {mathscr {B}}_0[e_{m}+(1-alpha )xi _{c}Phi (p)]}{{{mathscr {B}}_0+gamma [e_{r}+alpha Phi (p)]}^2}, quad dfrac{partial G}{partial e_m}=dfrac{{mathscr {B}}_0}{{mathscr {B}}_0+gamma [e_{r}+alpha Phi (p)]}, dfrac{partial G}{partial p}= & {} dfrac{{mathscr {B}}_0[(1-alpha )xi _{c}({mathscr {B}}_0+gamma e_{r})-alpha gamma e_{m}]Phi ‘(p)}{{{mathscr {B}}_0+gamma [e_{r}+alpha Phi (p)]}^2}, quad dfrac{partial H}{partial e_m}=dfrac{gamma e_{1/2}[e_{r}+alpha Phi (p)]p}{(e_{1/2}+G)^2}cdot dfrac{partial G}{partial e_{m}}, end{aligned}$$

and

$$begin{aligned} dfrac{partial H}{partial p}=1-mu +dfrac{gamma [e_{r}+alpha Phi (p)]G}{e_{1/2}+G}+dfrac{gamma p}{e_{1/2}+G}left{ alpha Phi ‘(p)G+dfrac{e_{1/2}[e_{r}+alpha Phi (p)]}{e_{1/2}+G}cdot dfrac{partial G}{partial p}right} . end{aligned}$$

The analysis of stability for the equilibrium solution ({mathscr {E}}(0)) is equivalent to that carried out in the first case. Thus, ({mathscr {E}}(0)) is uniformly asymptotically stable.

To analyze the stability of the equilibrium point ( {mathscr {E}}: = {mathscr {E}}(rho ) ), we consider the characteristic polynomial of the linearization matrix around this point, (tilde{F}(x)=x^3+ax^2+bx+c=0), where

$$begin{aligned} a= & {} -left( dfrac{partial F}{partial e_r}({mathscr {E}})+dfrac{partial G}{partial e_m}({mathscr {E}})+dfrac{partial H}{partial p}({mathscr {E}})right) , b= & {} dfrac{partial F}{partial e_r}({mathscr {E}})left( dfrac{partial G}{partial e_m}({mathscr {E}})+dfrac{partial H}{partial p}({mathscr {E}})right) +dfrac{partial G}{partial e_m}({mathscr {E}})dfrac{partial H}{partial p}({mathscr {E}})-left( dfrac{partial F}{partial p}({mathscr {E}})dfrac{partial H}{partial e_r}({mathscr {E}})+dfrac{partial G}{partial p}({mathscr {E}})dfrac{partial H}{partial e_m}({mathscr {E}})right) , c= & {} dfrac{partial F}{partial p}({mathscr {E}})left( dfrac{partial G}{partial e_m}({mathscr {E}})dfrac{partial H}{partial e_r}({mathscr {E}})-dfrac{partial G}{partial e_r}({mathscr {E}})dfrac{partial H}{partial e_m}({mathscr {E}})right) +dfrac{partial F}{partial e_r}({mathscr {E}})left( dfrac{partial G}{partial p}({mathscr {E}})dfrac{partial H}{partial e_m}({mathscr {E}})-dfrac{partial G}{partial e_m}({mathscr {E}})dfrac{partial H}{partial p}({mathscr {E}})right) . end{aligned}$$

From the sign of the derivatives (a,, c<0) and (b>0) are obtained. Thus, the necessary conditions of Jury’s criteria: (i) ({tilde{F}}(1)>0), (ii) ({tilde{F}}(-1)<0) and (iii) (|c|<1), are met. Indeed, ({tilde{F}}(1)=kappa gamma A_{1}A_{3}[1+(1-kappa gamma )A_{2}A_{3}]), ({tilde{F}}(-1)=-(1+|a|+b+|c|)) and (|c|=(1-kappa gamma )(1-A_3)(1+kappa gamma A_1 A_2 A_3)) where (A_{1}=mu r_{0}rho /(r_0rho +K-{mathscr {A}}rho )), (A_2=e_{1/2}/(e_{1/2}+E_{m})) and (A_{3}=alpha {mathscr {A}}/(kappa {mathscr {B}}_0+alpha {mathscr {A}})) with (0<A_{i}<1) for (iin {1,2,3}). Note that (|c|<(1-A_3)[1-(kappa gamma )^2]<1). In addition, the sufficient condition (1-c^2>|ac-b|) is equivalent to (c^2-1<ac-b<1-c^2). From (i), we have that (1-c^2-(ac-b)+(a-bc)>0) and (1-c^2-(ac-b)-(a-bc)>0). Adding these expressions, (ac-b<1-c^2) is obtained. Whereas for analyzing the inequality (c^2-1<ac-b) we consider the expression

$$begin{aligned} c^2-ac+b&= {} (1-kappa gamma )(1+kappa gamma A_{1}A_{2}A_{3})(1-A_3)left{ (1-kappa gamma )(1+kappa gamma A_{1}A_{2}A_{3})(1-A_3)right. nonumber &left. -, left[ (1-kappa gamma )+(1-A_3)+1-A_{1}(kappa gamma +(1-kappa gamma )A_{2}A_{3})right] right} +(1-kappa gamma )nonumber &+,(1-A_3)+1-A_1[kappa gamma (1-A_3)+(1-kappa gamma )^2 A_{2}A_{3}]-left[ 1-(1-kappa gamma )(1-A_3)right] . end{aligned}$$

(19)

Note that in Eq. (19), ( kappa gamma ) is the amount that provides the greatest variability to this expression. Then, we define the function

$$begin{aligned} g(x)&= {} (1-x)(1+x A_{1}A_{2}A_{3})(1-A_3)left{ (1-x)(1+x A_{1}A_{2}A_{3})(1-A_3)-[(1-x)+(1-A_3)+1-A_{1}(x+(1-x)A_{2}A_{3})]right} &+(1-x)+(1-A_3)+1-A_1[x(1-A_3)+(1-x)^2 A_{2}A_{3}]-left[ 1-(1-x)(1-A_3)right] , end{aligned}$$

for any (xin [0,1]). Now, we will show that (0<g(x)<1) for any (xin [0,1]). The function g is a fourth degree polynomial (g(x)=B_{4}x^4+B_{3}x^3+B_{2}x^2+B_{1}x+B_0) with coefficients

$$begin{aligned} B_{4}&= {} A_{1}^2 A_{2}^2 A_{3}^{2} (1-A_{3})^2>0, B_{3}&= {} A_{1}A_{2}A_{3}(1-A_3)[(1-A_1 A_2 A_3)(1-2A_3)-A_1], B_{2}&= {} -{A_{1}[A_{2}A_{3}^2(1-A_{1}A_{2})(1-A_3)+1-A_{1}A_{2}A_{3}(1-A_{3})]+A_3(1-A_1)}<0, B_{1}&= {} -A_{3}{A_{1}A_{2}[1-A_{3}^2(1-A_{1}A_{2})]+A_{3}[2-(1+A_{1}A_{2})^2]}, B_{0}&= {} 1-A_{1}A_{2}A_{3}^2>0, end{aligned}$$

where the values of (B_3) and (B_1) depend on the following three disjoint regions (see Fig. 3):

$$begin{aligned} {mathscr {R}}_1&= {} {(A_1,A_2,A_3)in (0,1)^3: B_3ge 0wedge B_1<0}, {mathscr {R}}_2&= {} {(A_1,A_2,A_3)in (0,1)^3: B_3<0wedge B_1le 0}, {mathscr {R}}_3&= {} {(A_1,A_2,A_3)in (0,1)^3: B_3<0wedge B_1>0}. end{aligned}$$

Figure 3

Disjoint regions of the unit cube ((0,1)^{3}). (a) ({mathscr {R}}_1), (b) ({mathscr {R}}_2) and (c) ({mathscr {R}}_3).

Full size image

Some important properties of the function g are: (g(0)=B_0in (0,1)), (g(1)=(1-A_1)(1-A_3)>0), (g(0)-g(1)=A_1(1-A_3)+A_3(1-A_1A_2A_3)>0) which implies that (0<g(1)<g(0)<1). Also, (g'(0)=B_1) and (g'(1)=-{(1-A_3)(2A_1+A_3)+A_3(1-A_1 A_2)^2+A_1 A_2 A_3^{2}(A_1+3-A_3)}<0) (see Fig. 4).

Figure 4

Graphical representation of some important properties of the polynomial g in the interval [0, 1]. (a) ((A_1,A_2,A_3)in {mathscr {R}}_1cup {mathscr {R}}_2), and (b) ((A_1,A_2,A_3)in {mathscr {R}}_3). The arrow on the axes ( x = 0 ) and (x = 1) represent the sign of ( g'(0)) and (g'(1)) respectively.

Full size image

Therefore, by the method of Descartes, we have the five admissible cases which are presented in Table 1. On the one hand, in the cases (C_1), (C_3), (C_4) and (C_5), (g’) has there is only one positive real root ({overline{x}}={overline{x}}(A_1,A_2,A_3)) where ((, )’) means the derivative with respect to x. Note that ({overline{x}}>1), because otherwise there would be at least one additional zero of (g’) on the interval (0, 1) for the basic properties are met. Then, the function g is a positive and decreasing function for any (xin [0,1]) with maximum value (g(0)=B_0<1). On the other hand, in case (C_2), (g’) has one positive real root ({overline{x}}in (0,1)) at which the polynomial g has a local maximum. Taking (g({overline{x}})) to define a function (f(A_1,A_2,A_3)) for ((A_1, A_2, A_3)in {mathscr {R}}_3), we have that (0<f(A_1,A_2,A_3)<1) if and only if ((A_1,A_2,A_3)in {mathscr {R}}_3) (using the application Mathematica). Thus, in all cases, (0<g(x)<1) for any (xin [0,1]), which implies (c^2-ac+b<1) and hence (c^2-1<ac-b). Therefore, ({mathscr {E}}(rho )) is locally asymptotically stable. (square )

Table 1 Admissible cases given by the method of Descartes applied to the polynomial g assuming that its coefficients (B_{i}) with (iin {0,1,2,3,4}) take the values according to ((A_1,A_2,A_3)in (0,1)^{3}). Each row corresponds to the case in which the signs of the coefficients of g are as indicated depending on the region ({mathscr {R}}_{j}) with (jin {1,2,3}).

Full size table

Optimal strategy

The validity of the condition ( {mathscr {U}}> 1 ) depending on ( alpha ) establishes a range of allocation strategies ( (alpha _m, alpha _M) ) in the which the persistence of the population is guaranteed (see Fig. 5). Thus, ( alpha in (alpha _{m}, alpha _{M}) ) if and only if ( {mathscr {U}}> 1 ), where (alpha _{m}) and (alpha _{M}) are the limits of this range such that ( {mathscr {U}} = 1 ) is obtained.

Figure 5

The individual consumption in the long term versus allocation strategy towards reproduction. Note that the size of the persistence range reduces with decreasing length of the cycle (tau ) or of the maximum rate of consumption (R_{max}), which is indicated by the respective arrows. In addition, ({mathscr {A}}={mathscr {A}}(alpha )) is a convex function, which implies that there is a unique allocation strategy, into the persistence range, that minimizes individual consumption in the long term.

Full size image

In this persistence range we find a unique allocation strategy described by

$$begin{aligned} alpha _ {op} =left( 1+sqrt{dfrac{e_{1/2}xi _{c}^{-1}}{kappa {mathscr {B}}_0}},right) ^{-1}, end{aligned}$$

which maximizes the population abundance and minimizes the individual consumption in the long term (see Fig. 6). This allocation strategy satisfies ( rho ‘(alpha _ {op}) = 0) if, and only if, also satisfies ({mathscr {A}}'(alpha _ {op}) = 0 ) where ( (,)’ ) means the derivative with respect to (alpha ) and

$$begin{aligned} {mathscr {A}}'(alpha )=dfrac{mu }{{mathscr {B}}_0}left{ dfrac{e_{1/2}xi _{c}^{-1}}{(1-alpha )^2}-dfrac{kappa {mathscr {B}}_0}{alpha ^2}right} . end{aligned}$$

In addition, the strategy ( alpha _ {op}) is dependent on the parameters associated with both the costs of fertility ((kappa ) and ({mathscr {B}}_0)) and survival ((xi _{c}) and (e_{1/2})), so that if the fertility costs (Delta :=kappa {mathscr {B}}_0) are greater than the maintenance ratio (delta :=e_{1/2}/xi _{c}), the allocation is to favor reproduction, i.e., (alpha _{op}>0.5) (see Fig. 6a). Otherwise, the allocation is to favor maintenance, i.e., (1-alpha _{op}ge 0.5) (see Fig. 6b).

Figure 6

Comparison of the long-term behavior of the population size after the reproductive season (population component of the system (6)) using various allocation strategies towards reproduction. (a) We consider the parameter set (eta =(2,1,1,0,200,2,2,1/3,0.1,0.39,alpha ,0.2)) with (alpha in {0.5,0.67,0.85}) and (b) (eta =(2,1,0.5,0,400,1,2,1/3,0.1,0.63,alpha ,0.2)) with (alpha in {0.1,0.26,0.4}). In both cases, the constant of fertility costs is described by (kappa =(1+gamma )^{-1}). In addition, note that in (a) (Delta =2/3>delta approx 0.165) and (b) (Delta =1/3<delta approx 2.718).

Full size image


Source: Ecology - nature.com

Field geology at a distance

MISTI pilots conversations in energy