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Research article

Global dynamical behavior of solutions for finite degenerate fourth-order parabolic equations with mean curvature nonlinearity

  • In this work, the initial-boundary value problem for the global dynamical properties of solutions to a class of finite degenerate fourth-order parabolic equations with mean curvature nonlinearity is studied. With the help of the Nehari flow and Levine's concavity method, we establish some sharp-like threshold classifications of the initial data under sub-critical, critical and supercritical initial energy levels, that is, we describe the size of an initial data set. It requires the presumption that the initial data starting from one region of phase space have uniform global dynamical behavior, which means that the solution exists globally and decays via energy estimates that ultimately result in the solution tending to zero in the forward time. For the case in which the initial data corresponds to another region, we prove that the solutions related to these initial data are subject to blow-up phenomena in a finite time. In addition, we estimate the corresponding upper bound of the lifespan of the blow-up solution.

    Citation: Yuxuan Chen. Global dynamical behavior of solutions for finite degenerate fourth-order parabolic equations with mean curvature nonlinearity[J]. Communications in Analysis and Mechanics, 2023, 15(4): 658-694. doi: 10.3934/cam.2023033

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  • In this work, the initial-boundary value problem for the global dynamical properties of solutions to a class of finite degenerate fourth-order parabolic equations with mean curvature nonlinearity is studied. With the help of the Nehari flow and Levine's concavity method, we establish some sharp-like threshold classifications of the initial data under sub-critical, critical and supercritical initial energy levels, that is, we describe the size of an initial data set. It requires the presumption that the initial data starting from one region of phase space have uniform global dynamical behavior, which means that the solution exists globally and decays via energy estimates that ultimately result in the solution tending to zero in the forward time. For the case in which the initial data corresponds to another region, we prove that the solutions related to these initial data are subject to blow-up phenomena in a finite time. In addition, we estimate the corresponding upper bound of the lifespan of the blow-up solution.



    Dengue is a viral disease transmitted mainly by Aedes mosquitoes, including Aedes aegypti and Aedes albopictus. Infected human beings carrying dengue viruses may get high fever, headaches, and skin rash, which may progress to dengue shock syndrome or dengue hemorrhagic fever. The annually reported dengue cases increased sharply from 2.2 million in 2010 to 3.2 million in 2015 [1]. More than 500, 000 people with severe dengue are hospitalized annually, and the case fatality percentage is about 2.5%. Due to the lack of commercially available vaccines for dengue control, traditional methods have been focused on vector control by heavy applications of insecticides and environmental management [2]. However, these programs have not prevented the spread of these diseases due to the rapid development of insecticide resistance [3] and the continual creation of ubiquitous breeding sites.

    An innovational mosquito control method utilizes Wolbachia, an intracellular bacterium present in about 60% of insect species [4], including some mosquitoes. Wolbachia can induce cytoplasmic incompatibility (CI) in mosquitoes, which results in early embryonic death from matings between Wolbachia-infected males and females that are either uninfected or harbor a different Wolbachia strain [5,6]. In the world's largest "mosquito factory" located in Guangzhou, China, 20 million Wolbachia-infected males are produced each week. These mosquitoes have been released in several urban and suburb areas since 2015, and killed more than 95% mosquitoes on the Shazai island [7]. Motivated by the success and the challenge in field trials, the study on the complex Wolbachia spread dynamics has become a hot research topic. Various mathematical models have been developed, including models of ordinary differential equations [8,9,10], delay differential equations [9,11,12,13], impulsive differential equations [14], stochastic equations [15], and reaction-diffusion equations [16]. These models are mainly devoted to analyzing the threshold dynamics for population replacement with Wolbachia-infected female mosquitoes or CI-driven population suppression, which only included mosquito population into the models. However, it is usually a formidable task for complete population replacement or eradication in large-scale field trials, and we can only concede mosquito replacement/eradication to virus eradication by restricting the mosquito densities below the epidemic risk threshold.

    To assess the efficacy of blocking dengue virus transmission by Wolbachia, a deterministic mathematical model of human and mosquito populations interfered by the circulation of a single dengue serotype was developed in the framework of SIER model [17]. This important study has inspired further development of compartmental models to analyze the transmission dynamics of dengue [18,19,20,21,22]. In this paper, we extend their efforts by incorporating the Wolbachia-infected male mosquito release into a compartmental model, where the infected males are maintained at a fixed ratio to the adult female mosquito population. We divide the mosquito population into three compartments: susceptible, exposed and infectious, and divide the human population into four compartments: susceptible, exposed, infectious and recovered. In particular, we include the respective extrinsic and intrinsic incubation periods (EIP and IIP) in the mosquito and human populations in our model. These periods have been shown to be crucial in clinical diagnosis, outbreak investigation, and dengue control [23], but have received relatively little attention [9,18]. Further, the release of Wolbachia-infected male mosquitoes is not effective immediately in sterilizing wild females due to the maturation delay between mating and emergence of adults [24]. To characterize the effect of EIP, IIP and the maturation delay on dengue transmission, we introduce three delays into our model.

    The model treats IIP in humans, EIP in mosquitoes, and the maturation delay as three delays. We aim to find the threshold values of the release ratio for mosquito or virus eradication under the proportional release policy. By analyzing the existence and stability of disease-free equilibria, we obtain the sufficient and necessary condition on the existence of the disease-endemic equilibrium. Two threshold values of the release ratio θ, denoted by θ1 and θ2 with θ1>θ2 are explicitly expressed. When θ>θ1, the mosquito population will be eradicated eventually. If it fails for mosquito eradication but θ2<θ<θ1, virus eradication is ensured together with the persistence of susceptible mosquitoes. When θ<θ2, the disease-endemic equilibrium emerges that allows dengue virus to circulate between humans and mosquitoes through mosquito bites. Sensitivity analysis of the threshold values in terms of the model parameters, and numerical simulations on several possible control strategies with different release ratios confirm the public awareness that reducing mosquito bites and killing adult mosquitoes are the most effective strategy to control the epidemic. Our model will provide new insights on the effectiveness of Wolbachia in reducing dengue at a population level.

    We divide adult mosquitoes into subetaoups of susceptible (SM), exposed (EM) and infectious (IM). Let NM=SM+EM+IM be the total number of mosquitoes. The human population is divided into four subpopulations: susceptible (SH), exposed (infected but not infectious, EH), infectious (IH), and recovered (RH). The total number of humans is denoted by NH=SH+EH+IH+RH. Without the bothering of the dengue virus, i.e., EM=IM=EH=IH=RH=0, we assume that mosquito and human populations follow the logistic growth [25] satisfying

    dNHdt=rHNH(t)(1NH(t)κH)μHNH(t),
    dNMdt=rMNM(t)(1NM(t)κM)μMNM(t),

    where rH and μH are respectively the birth rate and the death rate of humans, and κH is a constant which leads the human carrying capacity to [(rHμH)/rH]κH. Similarly, we set rM, μM, and κM as the birth rate, the death rate, and the carrying capacity parameter for mosquitoes. The prevalence of dengue virus disrupts the dynamics of humans and mosquitoes, which are split into SH, EH, IH, RH and SM, EM, IM, respectively.

    Dengue viruses can be transmitted from infectious mosquitoes to susceptible humans through bites. Let b be the average daily biting rate per female mosquito, and βMH be the fraction of transmission from mosquitoes to humans. Then, susceptible humans acquire the infection at the rate [bβMHIM(SH/NH)], and we have

    dSHdt=rHNH(t)(1NH(t)κH)bβMHIM(t)SH(t)NH(t)μHSH(t). (2.1)

    Let τH be the intrinsic incubation period (IIP) in humans between infection and the onset of infectiousness. IIP is an important determinant of dengue transmission dynamics, which varies from 3 to 14 days. Exposed humans become infectious at the rate

    [eμHτHbβMHIM(tτH)(SH(tτH)/NH(tτH))].

    With further assumption that infected but not infectious humans have the same death rate as that of susceptible humans, EH follows

    dEHdt=bβMHIM(t)SH(t)NH(t)eμHτHbβMHIM(tτH)SH(tτH)NH(tτH)μHEH(t). (2.2)

    Let γ be the recovery rate of humans. Then for IH and RH, we arrive at

    dIHdt=eμHτHbβMHIM(tτH)SH(tτH)NH(tτH)(γ+μH)IH(t), (2.3)
    dRHdt=γIH(t)μHRH(t), (2.4)

    where we disregard the negligible dengue mortality in humans [26] and set an identical mortality rate for humans.

    With the release of Wolbachia-infected male mosquitoes, denoted by R(t) at time t, the birth rate of mosquitoes is reduced from rM to

    rM(1Probability of complete CI occurrence).

    Under random mating and equal sex determination, the probability of CI occurrence at time t is the proportion of Wolbachia-infected male mosquitoes among all male mosquitoes, i.e., R(t)/(R(t)+NM(t)). However, there is a delay between the release of Wolbachia-infected males and the reduction of the wild mosquitoes which is caused by the maturation delay between mating and emergence of adult mosquitoes [24], denoted by τe. Hence, the number of susceptible mosquitoes that survive the maturation period is

    rMeμMτe[1R(tτe)NM(tτe)+R(tτe)]NM(tτe)(1NM(tτe)κM).

    The susceptible mosquitoes become exposed at a rate of [bβHMSM(IH/NH)], where βHM is the fraction of virus transmission from infectious humans to susceptible mosquitoes through blood meals. Taking these considerations into account, we have

    dSMdt=rMeμMτeNM(tτe)(1NM(tτe)κM)NM(tτe)NM(tτe)+R(tτe)bβHMSM(t)IH(t)NH(t)μMSM(t). (2.5)

    Exposed mosquitoes spend the extrinsic incubation period (EIP), denoted by τM, which is the viral incubation period between the time when a female mosquito takes a viraemia blood meal from an infectious human and the time when that mosquito becomes infectious [27], typically 8~12 days. EIP has been frequently recognized as a crucial component of dengue virus transmission dynamics [23]. In view of this point, the rate that exposed mosquitoes become infectious per unit time is [eμMτMbβHMSM(tτM)(IH(tτM)/NH(tτM))]. Then the whole set of equations in our model ends with

    dEMdt=bβHMSM(t)IH(t)NH(t)eμMτMbβHMSM(tτM)IH(tτM)NH(tτM)μMEM(t), (2.6)
    dIMdt=eμMτMbβHMSM(tτM)IH(tτM)NH(tτM)μMIM(t) (2.7)

    for exposed and infectious mosquitoes, respectively.

    Our purpose is to find the threshold values in terms of the release ratio for mosquito or virus eradication under the proportional release policy, where the Wolbachia-infected male mosquitoes is maintained in a fixed proportion to the adult female mosquito population, i.e.,

    R(t)=θNM(t). (2.8)

    The explicit expressions of the threshold values are obtained as follows:

    θ1=rMeμMτeμM1,θ2=rMeμMτeμM1rMeμMτeκH(rHμH)(γ+μH)rHκMb2βMHβHMeμHτHμMτM

    with θ1>θ2. We get the following theorem.

    Theorem 1. If θ>θ1, then eradication of mosquitoes occurs. If θ2<θ<θ1, then eradication of virus occurs. If θ<θ2, then there exists a unique disease-endemic equilibrium of system (2.1)-(2.7).

    The proof of Theorem 1 is embodied in the analysis of the existence and stability of equilibrium points of system (2.1)-(2.7) in the following two sections, and we omit it here.

    To determine the steady-state solutions of system (2.1)-(2.7), we set the right sides of (2.1)-(2.7) to zero and ignore the time lags to arrive at

    rHNH(1NHκH)bβMHIMSHNHμHSH=0, (3.1a)
    bβMHIMSHNHeμHτHbβMHIMSHNHμHEH=0, (3.1b)
    eμHτHbβMHIMSHNH(γ+μH)IH=0, (3.1c)
    γIHμHRH=0, (3.1d)
    rMeμMτeNM(1NMκM)11+θbβHMSMIHNHμMSM=0, (3.1e)
    bβHMSMIHNHeμMτMbβHMSMIHNHμMEM=0, (3.1f)
    eμMτMbβHMSMIHNHμMIM=0. (3.1g)

    Adding (3.1a) to (3.1d) together, we have

    rHNH(1NHκH)=μHNH,

    which yields

    NH=0orNH=κH(1μHrH):=NH, (3.2)

    provided that μH<rH holds. Similarly, adding (3.1e) to (3.1g) together, we have

    rMeμMτeNM(1NMκM)11+θ=μMNM,

    which leads to

    NM=0orNM=κM[1μM(1+θ)eμMτerM]:=NM. (3.3)

    Define the net reproductive numbers for humans and mosquitoes respectively by

    RH0:=rHμH,RM0:=rMμM(1+θ)eμMτe.

    Theorem 2. Assume that

    RH0>1 and  RM0>1. (3.4)

    Besides the zero equilibrium, system (2.1)-(2.7) admits two disease-free equilibrium points

    E01:=(NH,0,0,0,0,0,0),E02:=(NH,0,0,0,NM,0,0).

    Remark 1. The equilibrium point E01 corresponds to mosquito eradication as well as the infectious-free state for humans. The equilibrium point E02 biologically corresponds to the coexistence of mosquitoes and humans, without the infection of dengue virus, which more closely fits the actual situation. In the following discussion, we always assume that RH0>1.

    To find the disease-endemic equilibrium point of system (2.1)-(2.7), denoted by

    E:=(SH,EH,IH,RH,SM,EM,IM),

    we need to solve the algebraic equations (3.1a)-(3.1g). If we define the basic reproduction number by

    R0:=b2βMHβHMeμHτHμMτMNMμM(γ+μH)NH,

    then we obtain the existence of the disease-endemic equilibrium as follows.

    Theorem 3. The unique disease-endemic equilibrium of system (2.1)-(2.7) exists if and only if R0>1 and RM0>1.

    Proof. From (3.1d), we have

    RH=γμHIH. (3.5)

    From (3.1b) and (3.1c), we respectively have

    μHEH=bβMHIMSHNH(1eμHτH),(γ+μH)IH=bβMHIMSHNHeμHτH.

    Hence we get the relation between EH and IH as

    μHEH(γ+μH)IH=1eμHτHeμHτH,

    i.e.,

    EH=(eμHτH1)(γ+μH)μHIH. (3.6)

    Recall that at any steady state, we have

    rHNH(1NHκH)=μHNH.

    Combining (3.1a) and (3.1c), one has

    μH(NHSH)=bβMHIMSHNH=eμHτH(γ+μH)IH,

    and hence

    SH=NHeμHτH(γ+μH)μHIH. (3.7)

    From (3.1f) by (3.1g), we have

    μMEM=bβHMSMIHNH(1eμMτM),
    μMIM=bβHMSMIHNHeμMτM.

    Hence, we get the relation between EM and IM which reads as

    EM=(eμMτM1)IM. (3.8)

    Again, notice that at any steady state, we have

    rMeμMτeNM(1NMκM)11+θ=μMNM.

    Then from (3.1e) and (3.1g), we arrive at

    μM(NMSM)=bβHMSMIHNH=μMeμMτMIM,

    which leads to

    SM=NMeμMτMIM. (3.9)

    From (3.5) to (3.9), to get the explicit expression of the disease-endemic equilibrium point, we only need to solve for IH and IM. To this end, combining (3.1c) and (3.7), we have

    IH=eμHτHbβMH(γ+μH)NH[NHeμHτH(γ+μH)μHIH]IM=(eμHτHbβMHγ+μHbβMHμHNHIH)IM. (3.10)

    Similarly, from (3.1g) and (3.9), we have

    IM=eμMτMbβHMμMNH(NMeμMτMIM)IH=(eμMτMbβHMNMμMNHbβHMμMNHIM)IH. (3.11)

    Tedious but direct computations from (3.10)-(3.11) offers a linear relation between IM and IH as

    (bβHMμMNH+bβMHμHNHeμMτMbβHMNMμMNH)IH=(bβMHμHNH+bβHMμMNHeμHτHbβMHγ+μH)IM. (3.12)

    Plugging (3.12) into (3.10) and (3.11) yields the unique IH and IM as

    IH=[eμHτHμMτMb2βMHβHMNM(γ+μH)μMNH]μHNHbβHM(eμMτMbβMHNM+μHNH)(γ+μH), (3.13)
    IM=[eμHτHμMτMb2βMHβHMNM(γ+μH)μMNH]μHbβMH[eμHτHbβHMμH+(γ+μH)μM]. (3.14)

    It is easy to see from (3.5), (3.6), and (3.8) that RH, EH, and EM are positive provided that IM and IH are positive. From (3.7) and (3.13), we have

    SH=NHeμHτH[eμHτHμMτMb2βMHβHMNM(γ+μH)μMNH]NHbβHM(eμMτMbβMHNM+μHNH)=NHbβHM(eμMτMbβMHNM+μHNH)[bβHMμH+(γ+μH)μMeμHτH]NH>0

    always holds provided NM>0 and NH>0. Similarly, to guarantee SM>0, (3.9) requires again NM>0. From (3.9) and (3.14), with NH>0, we have

    SM=NMeμMτM[eμHτHμMτMb2βMHβHMNM(γ+μH)μMNH]μHbβMH[eμHτHbβHMμH+(γ+μH)μM]=1bβMH[eμHτHbβHMμH+(γ+μH)μM]μM(γ+μH)(NM+eμMτMμHNH)>0.

    Hence, the disease-endemic equilibrium point exists if and only if

    eμHτHμMτMb2βMHβHMNM(γ+μH)μMNH>0,

    i.e., R0>1. With the conclusion of Theorem 2, we complete the proof.

    Because we are dealing with a system of delay differential equations, the characteristic equation has an infinite number of roots satisfying

    det(J+eλτHJτH+eλτMJτM+eλτeJτeλI)=0, (4.1)

    where I is the identity matrix and the matrices J, JτH, JτM and Jτe have entries that are the partial derivatives of the right sides of (2.1)-(2.7) with respect to, respectively,

    (SH(t),EH(t),IH(t),RH(t),SM(t),EM(t),IM(t)),
    (SH(tτH),EH(tτH),IH(tτH),RH(tτH),SM(tτH),EM(tτH),IM(tτH)),
    (SH(tτM),EH(tτM),IH(tτM),RH(tτM),SM(tτM),EM(tτM),IM(tτM)),
    (SH(tτe),EH(tτe),IH(tτe),RH(tτe),SM(tτe),EM(tτe),IM(tτe)).

    Theorem 4. The disease-free equilibria E01 is locally asymptotically stable if and only if RM0<1.

    Proof. The matrices in (4.1) at E01 are

    J=(μHrH2μHrH2μHrH2μHrH00bβMH0μH0000bβMH00(γ+μH)000000γμH0000000μM0000000μM0000000μM), (4.2)
    JτH=(0000000000000eμHτHbβMH000000eμHτHbβMH0000000000000000000000000000), JτM=0,
    Jτe=(00000000000000000000000000000000rMeμMτe1+θrMeμMτe1+θrMeμMτe1+θ00000000000000).

    The characteristic matrix at E01 is (A01(λ)B010C01(λ)) with

    A01(λ)=(μHrHλ2μHrH0μHλ) (4.3)
    B01=(2μHrH2μHrH00bβMH0000bβMHe(λ+μH)τHbβMH) (4.4)
    C01(λ)=((γ+μH)λ000e(λ+μH)τHbβMHγμHλ00000μMλ+e(λ+μM)τerM1+θe(λ+μM)τerM1+θe(λ+μM)τerM1+θ000μMλ00000μMλ). (4.5)

    We firstly notice that when RH0>1, μHrH<0. To prove the conclusion, we only need to prove that all roots of

    μMλ+e(λ+μM)τerM1+θ=0 (4.6)

    have negative real parts if and only if RM0<1. Recall Theorem 4.7 in Smith [28] which states that λ=a+beλτ has no roots with non-negative real parts if a+b<0 and ba, irrelevant of the value of τ>0. By this theorem, we see that when

    μM+rMeμMτe1+θ<0, (4.7)

    i.e., RM0<1, all roots of (4.6) have negative real parts.

    Next we prove that the condition (4.7) is also sufficient to exclude the possibility for (4.6) to have roots with non-negative real parts. To proceed, assume that λ=z1+iz2 with z10 is a solution of (4.6). Then

    rMeμMτe1+θeτez1cos(τez2)=μM+z1, (4.8)
    rMeμMτe1+θeτez1sin(τez2)=z2, (4.9)

    It is easy to see that if (z1,z2) satisfies (4.8)-(4.9), so does (z1,z2). Without loss of generality, we assume that z20. Taking square of (4.8) and (4.9) and adding them together, we have

    r2M(1+θ)2e2τez12μMτe=(μM+z1)2+z22. (4.10)

    If z2=0, then z1>0 due to (4.7), and from (4.10), we have

    μ2M<(μM+z1)2=r2M(1+θ)2e2τez12μMτe<r2M(1+θ)2e2μMτe,

    a contradiction to (4.7). If z2>0, from (4.10), we have

    μ2M<(μM+z1)2+z22=r2M(1+θ)2e2τez12μMτer2M(1+θ)2e2μMτe,

    also a contradiction to (4.7). This completes the proof.

    Remark 2. Theorem 4 implies that if the proportion of Wolbachia-infected males to wild mosquito population, θ, satisfies θ>θ1, then wild mosquitoes will be eradicated eventually, which has proved the first conclusion of Theorem 1.

    Next we consider the stability of E02. The Jacobian matrices in (4.1) at E02 are

    J=(μHrH2μHrH2μHrH2μHrH00bβMH0μH0000bβMH00(γ+μH)000000γμH00000bβHMNMNH0μM0000bβHMNMNH00μM0000000μM), (4.11)
    JτH=(0000000000000eμHτHbβMH000000eμHτHbβMH0000000000000000000000000000),JτM=(0000000000000000000000000000000000000eμMτMbβHMNMNH000000eμMτMbβHMNMNH0000),
    Jτe=(000000000000000000000000000000002μMrMeμMτe1+θ2μMrMeμMτe1+θ2μMrMeμMτe1+θ00000000000000).

    The characteristic matrix at E02 is (A02(λ)B02C02D02(λ)) with

    A02(λ)=(μHrHλ2μHrH2μHrH0μHλ000(γ+μH)λ) (4.12)
    B02=(2μHrH00bβMH000bβMHe(λ+μH)τHbβMH000e(λ+μH)τHbβMH), (4.13)
    C02=(00γ00bβHMNMNH00bβHMNMNHe(λ+μM)τMbβMHNMNH00e(λ+μM)τMbβMHNMNH), (4.14)
    D02(λ)=(μHλ0000S1(λ)eλτe(2μMrMeμMτe1+θ)eλτe(2μMrMeμMτe1+θ)00μMλ0000μMλ), (4.15)

    where

    S1(λ)=μMλ+eλτe(2μMrMeμMτe1+θ). (4.16)

    By direct computation, roots of (4.1) at E02 are μHrH, μH together with roots of

    (μHλ)(μMλ)S1(λ)S2(λ)=0, (4.17)

    where

    S2(λ)=(γ+μH+λ)(μM+λ)b2βMHβHMeμHτHμMτMe(τH+τM)λNMNH. (4.18)

    On the roots of S1(λ)=0 and S2(λ)=0, we have the following two lemmas.

    Lemma 4.1. All roots of S1(λ)=0 have negative real parts if and only if RM0>1.

    Proof. Notice that S1(λ) as λ+. Then it is necessary to have S1(0)<0 to guarantee that all roots of S1(λ)=0 have negative real parts. Since

    S1(0)=μMrMeμMτe1+θ=μM(1RM0),

    S1(0)<0 if RM0>1. We claim that the condition RM0>1 is also sufficient. In fact, assume that λ=α+iβ satisfies S1(λ)=0. Then

    μMαiβ+(2μMrMeμMτe1+θ)eατe[cos(βτe)isin(βτe)].

    Separating the real and imaginary parts yields

    eατecos(βτe)=μM+α2μMrMeμMτe1+θ, (4.19)
    eατesin(βτe)=β2μMrMeμMτe1+θ. (4.20)

    If (α,β) satisfies (4.19)-(4.20), so does (z1,z2). Without loss of generality, we assume that β0. If α0, then eατe1. Equation (4.19) implies that

    μM+α2μMrMeμMτe1+θ,

    and hence

    αμMrMeμMτe1+θ=μM(1RM0)<0,

    a contradiction, which completes the proof.

    Lemma 4.2. All roots of S2(λ)=0 have negative real parts if and only if R0<1.

    Proof. Notice that S2(λ) is increasing with λ, and S2(λ)+ as λ+. Hence to make sure that all roots of S2(λ)=0 have negative real parts, the necessary condition is that S2(0)>0, that is,

    b2βMHβHMeμHτHμMτMNMμM(γ+μH)NH<1, (4.21)

    i.e., R0<1. We claim that condition (4.21) is also sufficient to guarantee that all roots of S2(λ)=0 have negative real parts. For notation simplicity, we define

    B:=b2βMHβHMeμHτHμMτMNMNH,τ:=τH+τM.

    Assume that λ=z1+iz2 is a solution of S2(λ)=0. Then

    Beτz1cos(τz2)=z21z22+(γ+μH+μM)z1+(γ+μH)μM, (4.22a)
    Beτz1sin(τz2)=2z1z2(γ+μH+μM)z2. (4.22b)

    It is easy to see that if (z1,z2) is a solution of (4.22a)-(4.22b), so does (z1,z2). Thus we can assume z2>0. Next we prove that z1<0 holds. If not, assume z1=0. Then (4.22a)-(4.22b) are reduced to

    Bcos(τz2)=z22+(γ+μH)μM, (4.23a)
    Bsin(τz2)=(γ+μH+μM)z2, (4.23b)

    which produces

    B2=[z22+(γ+μH)2](z22+μ2M).

    Therefore,

    B2μ2M(γ+μH)2=(1+z22μ2M)[1+z22(γ+μH)2]>1,

    a contradiction to (4.21). On the other hand, if z1>0, then from (4.22a)-(4.22b), we have

    B2e2τz1=[z21z22+(γ+μH+μM)z1+(γ+μH)μM]2+[2z1z2+(γ+μH+μM)z2]2=(z21+z22)2+z1(γ+μH+μM)[2z21+2z22+(γ+μH+μM)z1+2μM(γ+μH)z1]+2(γ+μH)μMz21+[(γ+μH)2+μ2M]z22+(γ+μH)2μ2M>(γ+μH)2μ2M.

    Therefore,

    B2μ2M(γ+μH)2>e2τz1>1,

    also a contradiction to (4.21). This completes the proof.

    From Lemmas 4.1 and 4.2, we have

    Theorem 5. The disease-free equilibrium point E02, if exists, is locally asymptotically stable.

    Results on the existence and stability of equilibria for system (2.1)-(2.2) are summarized in Table 1. Noticing the fact that

    RM0<1θ>θ1,R0<1θ>θ2,
    Table 1.  Conditions for the existence and stability of equilibria of system (2.1)-(2.7) with RH0>1.
    Condition on RM0 Condition on R0 Equilibria and stability
    RM0<1 R0<1 E01 stable, E02(NA), E(NA)
    RM0<1 R0>1 E01 stable, E02(NA), E (NA)
    RM0>1 R0<1 E01 unstable, E02 stable, E(NA)
    RM0>1 R0>1 E01 unstable, E02 unstable, E exists

     | Show Table
    DownLoad: CSV

    we conclude that Theorem 1 holds.

    The basic reproduction number R0 is a function of the parameters listed in Table 2.

    Table 2.  Parameter description.
    Parameter Description Baseline Range References
    rH Birth rate of humans 12.43‰ year1 [29]
    rM Birth rate of mosquitoes 2 day1 011.2 [19]
    μH Death rate of humans 7.11‰ year1 [29]
    μM Death rate of mosquitoes 1/14 day1 1/301/10 [19]
    b Average daily biting rate 0.63 day1 0.53 [30]
    γ Recovery rate of humans 1/5 day1 1/141/3 [26]
    βHM Fraction of transmission from humans to mosquitoes 0.33 0.21 [31]
    βMH Fraction of transmission from mosquitoes to humans 0.33 0.21 [31]
    rMH=κM/κH The carrying capacity ratio of mosquitoes to humans 0.5 01 Modelled
    τH Intrinsic incubation period of humans 7 days 314 [32]
    τM Extrinsic incubation period of mosquitoes 9 days 812 [17,32]
    τe Delay between mating and emergence of adult mosquitoes 10 days 719 [24]
    θ The release ratio 1 1 10 Modelled

     | Show Table
    DownLoad: CSV

    To estimate the response of R0 to different parameters, following the procedure in [20], we define the relative sensitivity index of R0 with respect to each parameter p in Table 2 by

    SR0p=pR0×R0p|p=p,

    where p is taken as the baseline value in Table 2 which also yields R0=1.5869. The relative sensitivity indices are shown in Figure 1 which are ranked in their absolute values. It turns out that avoiding mosquito bites through physical and chemical means or a combination of both is the most direct and effective method to reduce the transmission of dengue virus, which has comparable performance of elevating the death rate of mosquitoes, μM. Compared with the parameter μM, the birth rate of mosquitoes, rM, has much less contribution to R0. The elevation of R0 due to the increase of μH can be almost equally offset by the decrease of rH. Parameters βMH, βHM, the ratio of the carrying capacities of mosquitoes to humans, rMH, and the recovery rate of humans γ, contribute equally to R0. Among the three delay parameters, the extrinsic incubation period of mosquitoes, τM, is the most sensitive parameter, while the intrinsic incubation period of humans, τH, is the least sensitive one. Unexpectedly, the release ratio, θ, only plays a minor role in controlling the basic reproduction number. The most likely reason is that the baseline value of θ is set as 1, much smaller than the release ratio in field trials. Coincidentally, further computation shows that when the release ratio is increased from 5 to 6, the basic reproduction number is decreased from 1.0447 to 0.9092(<1). This observation is in line with our claim that for mosquito eradication or virus eradication, the optimal release ratio of Wolbachia-infected male mosquitoes to wild males is about 5 to 1 [9,33].

    Figure 1.  The relative sensitivity indices of R0 changing with parameters in Table 2.

    Theorem 2.1 shows that θ1 is the threshold value for mosquito eradication. If mosquito eradication fails, then θ2 is the threshold value for virus eradication. Dynamics of θ1 and θ2 are shown in Figure 2, which are in terms of the designated parameter while letting other parameters in system (2.1)-(2.7) be fixed as the baseline values in Table 2. The threshold values θ1 and θ2 increase as rM increase; see Figure 2(a), which decrease as μM or τe decrease; see Figure 2(b) and (c). The threshold value θ1 is fixed at 12.7072 when rM, μM and τe are fixed. In terms of b, βHM, βMH, and rMH, the threshold θ2 presents a quasi-logistic growth mode; see Figure 2(d), (e), and (f). The threshold θ2 is a linear decreasing function of γ or τM; see Figure 2(g) and (i). When τH lies between 3 and 14, it only brings a negligible change of θ2; see Figure 2(h) which is consistent with the observation in Figure 1 that the relative sensitivity index of τH is very close to 0.

    Figure 2.  Dynamics of the threshold values θ1 and θ2.

    Given the baseline values in Table 2, we have

    θ1=12.7072,θ2=5.3298

    which offer the threshold values of mosquito and virus eradication, respectively. We initiate system (2.1)-(2.7) with one infectious human, and a mosquito population size about 25,000 with one infectious mosquito. Figure 3 shows that if we take the release ratio θ=13>θ1, then both the virus and mosquito will eventually be eradicated. When the production of Wolbachia-infected male mosquitoes fails to meet θ1, we can only concede mosquito eradication to virus eradication.

    Figure 3.  The release ratio greater than θ1 is capable of wiping both virus and mosquito.

    Figure 4 shows that the release ratio θ=6 successfully clears the virus, together with the persistence of mosquito populations. However, further lower of the release ratio to 2 which is less than the threshold value θ2 can neither clear virus nor eradicate mosquitoes. To see this, we initiate system (2.1)-(2.7) near the disease-endemic equilibrium point E, with

    E(29492.13,1.8144,1.2958,13304.4331,39095.3777,1.6320,1.8095).
    Figure 4.  The release ratio lying in (θ1,θ2) clears virus, while leaving mosquito population size at a nonzero steady states eventually.

    When θ=2, Figure 5 shows that the number of infectious humans oscillates in the vicinity of their steady-state IH1.2958, and the number of infectious mosquitoes oscillates in the vicinity of their steady-state IM1.8095.

    Figure 5.  The release ratio less than θ2 can neither clear virus nor eradicate mosquitoes.

    Dengue fever is one of the most common mosquito-borne viral diseases. Due to the lack of commercially available vaccines and efficient clinical cures, traditional methods have been focused on vector control by heavy applications of insecticides and environmental management. However, these programs have not prevented the spread of these diseases due to the rapid development of insecticide resistance and the continual creation of ubiquitous larval breeding sites. One novel dengue control method involves the intracellular bacterium Wolbachia, whose infection in Aedes aegypti or Aedes albopictus, the major mosquito vector of dengue virus, can greatly reduce the virus replication in mosquitoes. Wolbachia can also induce cytoplasmic incompatibility (CI) in mosquitoes, which results in early embryonic death from matings between Wolbachia-infected males and females that are either uninfected or harbor a different Wolbachia strain.

    CI mechanism drives Wolbachia-infected male mosquitoes as a new weapon to suppress or eradicate wild females. However, complete population eradication in large-scale field trials is usually formidable, and we can only concede mosquito eradication to virus eradication by restricting the mosquito densities below the epidemic critical threshold. Motivated by the success and the challenge in field trials, we developed a deterministic mathematical model of human and mosquito populations interfered by the circulation of a single dengue serotype in the framework of SIER model to assess the efficacy of blocking dengue virus transmission by Wolbachia. We extended the SIER model by incorporating the Wolbachia-infected male mosquito release, where the infected males are maintained at a fixed ratio to the adult female mosquito population. Furthermore, the extrinsic incubation period in mosquito (EIP), the intrinsic incubation period in human (IIP), and the maturation delay between mating and emergence of adult mosquitoes were embedded as three delays in our model.

    The threshold values of the release ratio θ for mosquito or virus eradication were found by seeking the sufficient and necessary condition on the existence of the disease-endemic equilibrium. Two explicit expressions on threshold values of θ, denoted by θ1 and θ2 with θ1>θ2, were obtained. When θ>θ1, the mosquito population will be eradicated eventually. If it fails for mosquito eradication but θ2<θ<θ1, virus eradication is ensured together with the persistence of susceptible mosquitoes. When θ<θ2, the emergence of the disease-endemic equilibrium makes dengue virus circulation between humans and mosquitoes possible. Sensitivity analysis of the threshold values showed that avoiding mosquito bites through physical and chemical means is the most direct and effective method to reduce the transmission of dengue virus, which has comparable performance of elevating the death rate of mosquitoes. Results from numerical simulations also confirmed our previous claim that for mosquito eradication or virus eradication, the optimal release ratio of Wolbachia-infected male mosquitoes to wild males is about 5 to 1.

    This work was supported by National Natural Science Foundation of China (11826302, 11631005, 11871174), Program for Changjiang Scholars and Innovative Research Team in University (IRT_16R16) and Science and Technology Program of Guangzhou (201707010337).

    The authors have declared that no competing interests exist.



    [1] L. Hörmander, Hypoelliptic second order differential equations, Acta Math., 119 (1967), 147–171. https://doi.org/10.1007/BF02392081 doi: 10.1007/BF02392081
    [2] B. Jacob, S. He, Suppression of blow-up in Patlak-Keller-Segel via shear flows, SIAM J. Math. Anal., 49 (2017), 4722–4766. https://doi.org/10.1137/16M1093380 doi: 10.1137/16M1093380
    [3] H. Berestycki, A. Kiselev, A.Novikov, L. Ryzhik, The explosion problem in a flow, JAMA, 110 (2010), 31–65. https://doi.org/10.1007/s11854-010-0002-7 doi: 10.1007/s11854-010-0002-7
    [4] L. Agélas, Global regularity of solutions of equation modeling epitaxy thin film growth in Rd, d=1,2, J. Evol. Equ., 15 (2015), 89–106. https://doi.org/10.1007/s00028-014-0250-6 doi: 10.1007/s00028-014-0250-6
    [5] T. P. Schulze, R. V. Kohn, A geometric model for coarsening during spiral-mode growth of thin films, Phys. D, 132 (1999), 520–542. https://doi.org/10.1016/S0167-2789(99)00108-6 doi: 10.1016/S0167-2789(99)00108-6
    [6] M. Ortiz, E. A. Repetto, H. Si, A continuum model of kinetic roughening and coarsening in thin films, J. Mech. Phys. Solids, 47 (1999), 697–730. https://doi.org/10.1016/S0022-5096(98)00102-1 doi: 10.1016/S0022-5096(98)00102-1
    [7] T. J. Willmore, A survey on Willmore immersions, In Geometry and Topology of Submanifolds, World Sci. Publ., IV (1991), 11–16.
    [8] W. K. Burton, N. Cabrera, F. C. Frank, The growth of crystals and the equilibnum structure of their surfaces, Phil. Trans. Royal Soc. London, 243 (1951), 299–358. https://doi.org/10.1098/rsta.1951.0006 doi: 10.1098/rsta.1951.0006
    [9] C. Gerhardt, Boundary value problems for surfaces of prescribed mean curvature, J. Math. Pures Appl., 58 (1979), 75–109.
    [10] D. Farrukh, On a boundary control problem for a pseudo-parabolic equation, Commun. Anal. Mech., 15 (2023), 289–299. https://doi.org/10.3934/cam.2023015 doi: 10.3934/cam.2023015
    [11] C. Corsato, C. De Coster, P. Omari, The Dirichlet problem for a prescribed anisotropic mean curvature equation: Existence, uniqueness and regularity of solutions, J. Differential Equations, 260 (2016), 4572–4618. https://doi.org/10.1016/j.jde.2015.11.024 doi: 10.1016/j.jde.2015.11.024
    [12] G. Ehrlich, F. G. Hudda, Atomic view of surface self-diffusion: Tungsten on tungsten, J. Chem. Phys., 44 (1966), 1039–1049. https://doi.org/10.1063/1.1726787 doi: 10.1063/1.1726787
    [13] G. Métivier, Fonction spectrale et valeurs propres d'une classe d'opŕateurs non elliptiques, Comm. Partial Differential Equations, 5 (1976), 467–519.
    [14] H. Lewy, An example of a smooth linear partial differential equation without solution, Ann. Math., 66 (1956), 155–158. https://doi.org/10.2307/1970121 doi: 10.2307/1970121
    [15] J. J. Kohn, Subellipticity of the ˉ-Neumann problem on pseudo-convex domains: sufficient conditions, Acta Math., 142 (1979), 79–122. https://doi.org/10.1007/BF02395058 doi: 10.1007/BF02395058
    [16] Z. Schuss, Theory and Application of Stochastic Differential Equations, Wiley, New York, 1980.
    [17] M. Bramanti, An Invitation to Hypoelliptic Operators and Hörmander's Vector Fields, Springer-Verlag, 2014.
    [18] D. Gbargil, N. S. Trudinger, Elliptic partial differential equations of second order, Springer-Verlag, 1983.
    [19] D. Jerison, The Poincaré inequality for vector fields satisfying Hörmader's condition, Duke Math., 53 (1968), 503–523. https://doi.org/10.1215/S0012-7094-86-05329-9 doi: 10.1215/S0012-7094-86-05329-9
    [20] J. M. Bony, Principe du maximum, inégalité de Harnack et unicité du probleme de Cauchy pour les opérateurs elliptiques dégénérés, Ann. Inst. Fourier, 19 (1969), 277–304. https://doi.org/10.5802/aif.319 doi: 10.5802/aif.319
    [21] L. P. Rothschild, E. M. Stein, Hypoelliptic differential operators and nilpotent groups, Acta Math., 137 (1976), 247–320. https://doi.org/10.1007/BF02392419 doi: 10.1007/BF02392419
    [22] G. Métivier, Fonction spectrale et valeurs propres d'une classe d'opérateurs non elliptiques, Comm. Partial Differ. Equations, 1 (1976), 467–519. https://doi.org/10.1080/03605307608820018 doi: 10.1080/03605307608820018
    [23] R. Montgomery, A tour of subriemannian geometries. Their geodesics and applications, Mathematical Surveys and Monographs, 91. American Mathematical Society, Providence, RI, 2002.
    [24] L. Chen, G. Z. Lu, M. C. Zhu, Least energy solutions to quasilinear subelliptic equations with constant and degenerate potentials on the Heisenberg group, Proc. Lond. Math. Soc., 126 (2023), 518–555. https://doi.org/10.1112/plms.12495 doi: 10.1112/plms.12495
    [25] L. Capogna, Regularity for quasilinear equations and 1-quasiconformal maps in Carnot groups, Math. Ann., 313 (1999), 263–295. https://doi.org/10.1007/s002080050261 doi: 10.1007/s002080050261
    [26] B. B. King, O. Stein, M. Winkler, A fourth-order parabolic equation modeling epitaxial thin film growth, J. Math. Anal. Appl., 286 (2003), 459–490. https://doi.org/10.1016/S0022-247X(03)00474-8 doi: 10.1016/S0022-247X(03)00474-8
    [27] R. Dal Passo, H. Garcke, G. Grün, On a fourth-order degenerate parabolic equation: global entropy estimates, existence, and qualitative behavior of solutions, SIAM J. Math. Anal., 29 (1998), 321–342. https://doi.org/10.1137/S0036141096306170 doi: 10.1137/S0036141096306170
    [28] B. Guo, W. Gao, Study of weak solutions for a fourth-order parabolic equation with variable exponent of nonlinearity, Z. Angew. Math. Phys., 62 (2011), 909–926. https://doi.org/10.1007/s00033-011-0148-x doi: 10.1007/s00033-011-0148-x
    [29] X. Zhang, J. Zhou, Well-posedness and dynamic properties of solutions to a class of fourth order parabolic equation with mean curvature nonlinearity, Discrete Contin. Dyn. Syst. Ser. B, 28 (2023), 3768–3806. https://doi.org/10.3934/dcdsb.2022240 doi: 10.3934/dcdsb.2022240
    [30] A. L. Bertozzi, M. C. Pugh, Finite-time blow-up of solutions of some long-wave unstable thin film equations, Indiana Univ. Math. J., 49 (2000), 1323–1366.
    [31] J. B. Han, R. Z. Xu, C. Yang, Continuous dependence on initial data and high energy blowup time estimate for porous elastic system, Commun. Anal. Mech., 15 (2023), 214–244. https://doi.org/10.3934/cam.2023012 doi: 10.3934/cam.2023012
    [32] H. Chen, H. Y. Xu, Global existence, exponential decay and blow-up in finite time for a class of finitely degenerate semilinear parabolic equations, Acta Math. Sci. Ser. B, 39 (2019), 1290–1308. https://doi.org/10.1007/s10473-019-0508-8 doi: 10.1007/s10473-019-0508-8
    [33] H. Y. Xu, Existence and blow-up of solutions for finitely degenerate semilinear parabolic equations with singular potentials, Commun. Anal. Mech., 15 (2023), 132–161. https://doi.org/10.3934/cam.2023008 doi: 10.3934/cam.2023008
    [34] H. Chen, X. Liu, Y. Wei, Cone Sobolev inequality and Dirichlet problem for nonlinear elliptic equations on a manifold with conical singularities, Calc. Var., 43 (2012), 463–484. https://doi.org/10.1007/s00526-011-0418-7 doi: 10.1007/s00526-011-0418-7
    [35] R. Z. Xu, W. Lian, Y. Niu, Global well-posedness of coupled parabolic systems, Sci. China Math., 63 (2020), 321–356. https://doi.org/10.1007/s11425-017-9280-x doi: 10.1007/s11425-017-9280-x
    [36] X. Y. Chen, V. D. Rădulescu, R. Z. Xu, High energy blowup and blowup time for a class of semilinear parabolic equations with singular potential on manifolds with conical singularities, Commun. Math. Sci., 21 (2023), 25–63. https://dx.doi.org/10.4310/CMS.2023.v21.n1.a2 doi: 10.4310/CMS.2023.v21.n1.a2
    [37] N. H. Tuan, V. V. Au, R. Z. Xu, Semilinear Caputo time-fractional pseudo-parabolic equations, Commun. Pure Appl. Anal., 20 (2021), 583–621. https://doi.org/10.3934/cpaa.2020282 doi: 10.3934/cpaa.2020282
    [38] L. E. Payne, D. H. Sattinger, Saddle points and instability of nonlinear hyperbolic equations, Israel J. Math., 22 (1975), 273–303. https://doi.org/10.1007/BF02761595 doi: 10.1007/BF02761595
    [39] R. Z. Xu, J. Su, Global existence and finite time blow-up for a class of semilinear pseudo-parabolic equations, J. Funct. Anal., 264 (2013), 2732–2763. https://doi.org/10.1016/j.jfa.2013.03.010 doi: 10.1016/j.jfa.2013.03.010
    [40] X. C. Wang, R. Z. Xu, Global existence and finite time blowup for a nonlocal semilinear pseudo-parabolic equation, Adv. Nonlinear Anal., 10 (2021), 261–288. https://doi.org/10.1515/anona-2020-0141 doi: 10.1515/anona-2020-0141
    [41] W. Lian, J. Wang, R. Z. Xu, Global existence and blow up of solutions for pseudo-parabolic equation with singular potential, J. Differential Equations, 269 (2020), 4914–4959. https://doi.org/10.1016/j.jde.2020.03.047 doi: 10.1016/j.jde.2020.03.047
    [42] C. J. Xu, Semilinear subelliptic equations and Sobolev inequality for vector fields satisfying Hörmander's condition, Chinese J. Contemp. Math., 15 (1994), 183–192.
    [43] P. L. Yung, A sharp subelliptic Sobolev embedding theorem with weights, Bull. Lond. Math. Soc., 47 (2015), 396–406. https://doi.org/10.1112/blms/bdv010 doi: 10.1112/blms/bdv010
    [44] A. Yagi, Abstract Parabolic Evolution Equations and Lojasiewicz-Simon Inequality I and II, Springer Briefs in Mathematics, Springer, 2021.
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