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Dynamic analysis of sheep Brucellosis model with environmental infection pathways


  • We develop a mathematical model for the transmission of brucellosis in sheep taking into account external inputs, immunity, stage structure and other factors. We find the the basic reproduction number R0 in terms of the model parameters, and prove the global stability of the disease-free equilibrium. Then, the existence and global stability of the endemic equilibrium is proven. Finally, sheep data from Yulin, China are employed to fit the model parameters for three different environmental infection exposure conditions. The variability between different models in terms of control measures are analyzed numerically. Results show that the model is sensitive to the control parameters for different environmental infection exposure functions. This means that in practical modeling, the selection of environmental infection exposure functions needs to be properly considered.

    Citation: Zongmin Yue, Yuanhua Mu, Kekui Yu. Dynamic analysis of sheep Brucellosis model with environmental infection pathways[J]. Mathematical Biosciences and Engineering, 2023, 20(7): 11688-11712. doi: 10.3934/mbe.2023520

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  • We develop a mathematical model for the transmission of brucellosis in sheep taking into account external inputs, immunity, stage structure and other factors. We find the the basic reproduction number R0 in terms of the model parameters, and prove the global stability of the disease-free equilibrium. Then, the existence and global stability of the endemic equilibrium is proven. Finally, sheep data from Yulin, China are employed to fit the model parameters for three different environmental infection exposure conditions. The variability between different models in terms of control measures are analyzed numerically. Results show that the model is sensitive to the control parameters for different environmental infection exposure functions. This means that in practical modeling, the selection of environmental infection exposure functions needs to be properly considered.



    Brucellae are Gram-negative coccobacilli causing brucellosis, a serious chronic zoonotic infectious disease. The World Organization for Animal Health classifies brucellosis as a notifiable infectious disease category Ⅰ, and China classifies it as a category Ⅱ infectious disease [1]. In China, the main sources of the disease are cattle, sheep and pigs, with brucellosis being the most transmissible, pathogenic and dangerous disease in sheep. Brucellae are resistant to external factors such as dryness and cold, but not to moisture and heat, and die immediately after boiling. Commonly used disinfectants can kill brucellae within a few hours [2]. Brucellosis may be transmitted directly way through the gastrointestinal and respiratory tracts, the genitourinary tract, and infections of damaged or undamaged skin and mucous membranes. There is also an indirect channel of infection through direct contact or contact with the secretions and excretions of diseased animals [3,4]. It is estimated that the disease is endemic in humans and animals in more than 170 countries and territories, with more than 500,000 new cases of brucellosis worldwide each year [5].

    Studying the spread of infectious diseases using dynamical models is an important avenue of research that can provide referable advice for disease control. Of course, when building a model, it is important to include the transmission pattern of the disease, especially the main transmission routes. In the study of brucellosis, the indirect transmission pathway of the bacteria from the environment is a non-negligible part of brucellosis transmission, so the exposure infection function of environmental infection needs to be determined in the modeling analysis. A simple model of Brucella transmission that takes into account both routes of transmission may be written as

    {dSdt=A+αS[β1g(s,I)+β2Sf(W)]dS,dIdt=[β1g(s,I)+β2Sf(W)]dI,dWdt=kI(δ+ηl)W, (1.1)

    where S(t),I(t),W(t) represents the susceptible flock, the infected flock, and the concentration of bacteria in the environment, respectively. The parameter α denotes the birth rate, A is the recruitment rate of the flock, g(s,I) is the contact infection function between susceptible and infected sheep, f(w) is the environmental exposure function, and d is the mortality rate of the flock per unit time. Sheep with brucellosis spread Brucella in the environment at rate k and environmental Brucella had a mortality rate δ. The number of disinfection per unit time is l. The efficiency of each disinfection is η.

    One of the things that we are more interested in is how the environmental exposure function may be described. Li et al. [6] proposed a dynamicak model of brucellosis in sheep consideredin the environmental indirect infection. They used three common environmental exposure functions, which are also present in the literature:

    Case 1. Standard incidence: f(W)=WN [6];

    Case 2. Incidence of saturation: f(W)=WW+ϵ1 [7,8,9];

    Case 3. Incidence of mass action: f(W)=WM [10,11,12,13,14,15,16].

    Here, ϵ1 and M are scaling factors for the Brucella concentration in the environment.

    In ref [6], the authors compared three forms of environmental exposure functions using real data, and indicate the first environmental exposure function as the proper choice. The second environmental exposure function was used by Li et al. [8] to develop a sheep-human Brucella infection model, with particular attention to the role of ewe flocks in disease transmission. Meng et al. [12] used the third environment exposure function to develop a multi-stage dynamic model. Sun et al. [16] used the third environmental exposure function to develop a five-step model of brucellosis transmission based on model (1.1), taking into account vaccination as well as latent period transmission. In fact, the third environmental exposure function is the most used in current literature. Looking at the results obtained so far from a dynamical point of view, the behavior of the models resulting from using the three above environmental exposure functions is relatively similar. The existence and stability of disease-free equilibrium and endemic equilibrium points are determined by the critical values, i.e., the basic reproduction number R0.

    The spread of brucellosis in sheep has actually some specific characteristics. Sheep are managed as domestic animals, so there are some human factors involved, e.g., addition of new sheep, slaughter of adult sheep, environmental disinfection and testing, trapping and killing of infected sheep, etc. In addition, sheep brucellosis has a very obvious stage structure [17], i.e., the probability of lambs being infected by brucellosis in sheep is very low, while adult sheep are easily infected. Morevover, owing to the growing demand for dairy and meat products, large scale live sheep trading and trafficking activities are increasing. Due to lack of disease prevention awareness and lax management, some infected sheep are introduced from outside to the original farming area and spread the disease. Based on the presence of these factors, we here develop a model of brucellosis transmission considering stage structure, external inputs and immune control. In order to describe environmental exposure, unlike in other works, we take an abstract function. Our goals include to study of the transmission pattern of brucellosis and to propose control measures, as well as to examine whether the use of different environmental infection exposure functions has a significant effect on the selection and the strength of the possible control measures.

    This paper is structured as follows. In Section 2, we introduce our models and a unified abstract expression for the environmental exposure function. In Section 3, the stability and persistence of the models are investigated. In Section 4, numerical simulations of our models are performed, and the sensitivities of the models resulting from using three different environmental exposure functions are analyzed and compared. Finally, Section 5 closes the paper with some concluding remarks.

    Sheep are divided into four classes: susceptible young sheep Sj(t), susceptible adult sheep Sa(t), immune sheep V(t) and infected sheep I(t). Let W(t) denote the density of Brucella in the environment, S0(t) the quantity of slaughter sheep, and f(W) the environmental infection exposure function. We also assume that the introduction rate of external sheep per unit time is A, the birth rate of sheep is α, which is limited by the natural mortality rate of sheep d. The probability of external introduction into the infected flock is C, the conversion rate of lambs to adults is m, and the immune loss rate is λ. The ratio of infection rate in adult sheep to lambs is denoted by ϵ, and te slaughter rate by r. Sheep with brucellosis spread Brucella in the environment at rate k and environmental Brucella had a mortality rate δ. The number of disinfection per unit time is l, and the efficiency of each disinfection is η. Direct infection rate is β1, indirect infection rate is β2.

    Some assumptions are embedded in our model:

    1) Brucellosis in the exposure period is hardly detected, hence, we ignore this period in the sheep population.

    2) Once the ewes are infected with brucellosis, they will not be able to reproduce.

    3) All parameters above are non-negative and 0<α<d<1, 0C1, 0<ϵ, r<1.

    According to the flow chart of transmission (see Figure 1), the dynamics of brucellosis is modeled as follows

    {dSjdt=(1C)A+α[V(t)+Sa(t)](d+m)Sj(t)ϵ{β1Sj(t)I(t)+β2Sj(t)f[W(t)]},dSadt=mSj(t)+λV(t){β1Sa(t)I(t)+β2Sa(t)f[W(t)]}rSa(t)θSa(t)dSa(t),dIdt=CA+ϵ{β1Sj(t)I(t)+β2Sj(t)f[W(t)]}+β1Sa(t)I(t)+β2Sa(t)f[W(t)](d+e)I(t),dVdt=θSa(t)(λ+d)V(t)rV(t),dS0dt=r[V(t)+Sa(t)],dWdt=kI(t)(δ+ηl)W(t). (2.1)

    The non-negative functions f(W) and W are differentiable. Based on the three common forms of f(W), we assume that the function f(W) has the following properties.

    Figure 1.  Transmission diagram of brucellosis.

    (H1) f(W)0 with equality if and only if W=0;

    (H2) f(W) is monotone nondecreasing with W;

    (H3) f(W)W is monotone nonincreasing.

    Lemma 1. Supposing all parameters are non-negative and 0<α<d<1, 0C1, 0<ϵ, r<1, then the closed set

    Ω={(Sj(t),Sa(t),S0(t),I(t),V(t),W(t))|Sj(t),Sa(t),S0(t),I(t),V(t),W(t)0,S0(t)rAdα,0Sj(t)+Sa(t)+I(t)+V(t)Adα,W(t)kA(dα)(δ+ηl)}. (2.2)

    is a positive invariant set of the model (2.1) if system (2.1) satisfied initial conditions Sj(0)>0, Sa(0)>0, S0(0)>0, I(0)>0, V(0)>0, W(0)>0.

    Proof. Let N(t)=Sj(t)+Sa(t)+I(t)+V(t), it is easy to obtain

    dNdtA+α[V(t)+Sa(t)]dN(t)eI(t)A(dα)N(t),

    then we have

    limtsupN(t)Adα. (2.3)

    Hence, we have that Sa(t),V(t) are bounded. Suppose 0<V(t)+Sa(t)M0Adα, then we have

    dS0dt=r[Sa(t)+V(t)]rM0.

    It follows that there is a sufficiently large T such that the following expression holds when tT>0:

    0S0(t)rM0[rM0S0(T)]e(tT),

    then, when t, we get

    limtsupS0(t)rM0rAdα. (2.4)

    According to the last equation of model (2.1), we have

    dWdt=kI(t)(δ+ηl)W(t)kAdα(δ+ηl)W(t),

    then we have

    limtsupW(t)kA(dα)(δ+ηl). (2.5)

    By (2.3)–(2.5), we arrive at (2.2), i.e., the solutions of model (2.1) are non-negative for all time t>0 and all solutions are uniformly bounded. The region Ω is a positive invariant. The proof is completed.

    In fact, according to the formulation of model (2.1), it can be seen that S0 is not related to the rest of the variables. We may consider the following equivalent model to describe the dynamics of disease transmission:

    {dSjdt=(1C)A+α[V(t)+Sa(t)](d+m)Sj(t)ϵ{β1Sj(t)I(t)+β2Sj(t)f[W(t)]},dSadt=mSj(t)+λV(t){β1Sa(t)I(t)+β2Sa(t)f[W(t)]}rSa(t)θSa(t)dSa(t),dIdt=CA+ϵ{β1Sj(t)I(t)+β2Sj(t)f[W(t)]}+β1Sa(t)I(t)+β2Sa(t)f[W(t)](d+e)I(t),dVdt=θSa(t)(λ+d)V(t)rV(t),dWdt=kI(t)(δ+ηl)W(t). (3.1)

    If C=0, it is easy to get the disease-free equilibrium (DFE) E0=(S0j,S0a,0,V0,0), from the equations

    { A+α[V(t)+Sa(t)](d+m)Sj(t)ϵβ2Sj(t)f(0)=0, mSj(t)+λV(t)β2Sa(t)f(0)rSa(t)θSa(t)dSa(t)=0,θSa(t)(λ+d)V(t)rV(t)=0. (3.2)

    In particular, we have the following theorem

    Theorem 2. If C=0 and 0<α<d<1, the model (3.1) has one disease-free equilibrium E0=(S0j,S0a,0,V0,0), where

     S0j=A(d+r)d2+(dα)m+r(d+m), S0a=Am(λ+d+r)[d2+(dα)m+r(d+m)](d+r+λ+θ), V0=Amθ[d2+(dα)m+r(d+m)](d+r+λ+θ). (3.3)

    We derive the basic reproduction number of system (3.1) using the next generation matrix method formulated by Diekmann et al. [18,19]. We order the infection variables first by disease state, only needing the vector X(t)=(I(t),W(t))T. Then, considering the following auxiliary system:

    {dIdt=ϵ[β1Sj(t)I(t)+β2Sj(t)f(W(t))]+β1Sa(t)I(t)+β2Sa(t)f(W(t))(d+e)I(t),dWdt=kI(t)(δ+ηl)W(t). (3.4)

    According to the recipe of van den Driessche and James, the Watmough [20] matrices F and V are given by

    F=(ϵβ1S0j+β1S0aϵβ2S0jf(0)+β2S0af(0)00), V=(d+e0kδ+ηl). (3.5)

    Here f(0) is the derivative of f(W(t)) with respect to W(t) at disease-free equilibrium. The basic reproduction number is defined as the spectral radius of the nonnegative matrix FV1 which is given by

    FV1=(ϵβ1S0j+β1S0ad+e+k[ϵβ2S0jf(0)+β2S0af(0)](d+e)(δ+ηl)ϵβ2S0jf(0)+β2S0af(0)δ+ηl00). (3.6)

    Therefore

    R0=ρ(FV1)=ϵβ1S0j+β1S0ad+e+k[ϵβ2S0jf(0)+β2S0af(0)](d+e)(δ+ηl)=Ri0+Re0. (3.7)

    where Ri0=ϵβ1S0j+β1S0ad+e and Re0=k[ϵβ2S0jf(0)+β2S0af(0)](d+e)(δ+ηl) are the partial reproduction numbers due to environment-to-individual and individual-to-individual transmission, respectively.

    Notice that

     S0a=m(λ+d+r)(r+d)(d+r+λ+θ)S0jq1S0j. (3.8)

    and thus R0 can be written as

     R0=(ϵ+q1)S0jβ1+k(δ+ηl)β2f(0)(d+e). (3.9)

    If we now insert the expression S0j=A(d+r)d2+(dα)m+r(d+m) in the above equation, we arrive at

     R0=Am(λ+d+r)+ϵA[(λ+d+r)(θ+d+r)θλ](d+m)[(λ+d+r)(θ+d+r)θλ]mα(d+r+λ+θ)β1+k(δ+ηl)β2f(0)(d+e). (3.10)

    Theorem 3. If the assumptions (H1)–(H3), 0<α<d<1 and C=0, then the disease-free equilibrium of model (3.1) is globally asymptotically stable in the region Ω if R0<1 and unstable if R0>1.

    Proof. By using assumptions (H1) and (H3), we have

    f(W)WlimW0f(W)W=limW0f(W)f(0)W0=f(0). (3.11)

    Thus by (3.11), we have f(0)Wf(W). Hence, for model (3.4), denoting X(t)=(I(t),W(t))T, it is easy to prove that

    dXdt(FV)X(t). (3.12)

    Let b0 be the left eigenvector of the nonnegative matrix V1F, which satisfies bV1F=R0bT, and define the Lyapunov function L=bTV1X(t). Taking derivative of L and use (3.3) we arrive at

    dLdt=bTV1dXdtbTV1(FV)X(t)=bTV1FX(t)bTX(t)(R01)bTX(t). (3.13)

    Then dLdt0 fpr R0<1. Let Ω={(Sj(t),Sa(t),I(t),V(t),W(t))X(t)|dLdt=0}, we have dLdt=0 if R0=1. This implies that X(t)=0, i.e., I(t)=0,W(t)=0. Therefore, the largest invariant set of Ω is the singleton E0. According to LaSalle's invariance principle [21], E0 is globally asymptotically stable in the region Ω.

    Obviously, if R0>1 and X(t)>0, then (R01)bTX(t)>0. In this case, there must exist a small enough neighborhood of E0 in which dLdt>0 holds. Therefore, E0 is unstable. The proof is completed.

    Theorem 4. If the assumptions (H1)–(H3) and 0<α<d<1 hold,

    (a) if 0<C<1, the model (3.1) has a unique endemic equilibrium E=(Sj,Sa,I,V,W);

    (b) if C=0 and R0>1, the model (3.1) has a unique endemic equilibrium E=(Sj,Sa,I,V,W);

    (c) if C=0 and R01, the model (3.1) has no endemic equilibrium.

    (d) if C=1, the model (3.1) has a boundary point (0,0,Ad+e,0,Ak(d+e)(δ+ηl)), and has no endemic equilibrium E.

    Proof. The endemic equilibrium of model (3.1) satisfies the following equilibrium equations:

    { (1C)A=α(V+Sa)+(d+m)Sj+ϵ[β1SjI+β2Sjf(W)], mSj+λV=[β1SaI+β2Saf(W)]+θSa+dSa+rSa, (d+e)I=CA+ϵ[β1SjI+β2Sjf(W)]+β1SaI+β2Saf(W), θSa=(λ+d+r)V, kI=(δ+ηl)W. (3.14)

    Thus, we have

     W=kδ+ηlI, V=Am(1C)θQ, Sa=Am(1C)(λ+d+r)Q, Sj=A(1C)(λ+d+r)[d+θ+rλθλ+d+r+β1I+β2f(W)]Q, (3.15)

    where

    Q=(λ+d+r){d+m+ϵ[β1I+β2f(W)]}[d+θ+rλθλ+d+r+β1I+β2f(W)]mα(λ+d+r+θ). (3.16)

    From the third equation of (3.14) and Eq (3.15), we also obtain that Sa should satisfy

     Sa=CA+(d+e)Iβ1I+β2f(W)ϵA(1C){(λ+d+r)[θ+d+r+β1I+β2f(W)]λθ}Q. (3.17)

    Assuming I as the independent variable and Sa as the dependent variable, we may write the two following functional expressions

     Sa=Am(1C)(λ+d+r)QF1(I), (3.18)
     Sa=CA+(d+e)IH(I)ϵA(1C){(λ+d+r)[θ+d+r+H(I)]λθ}QF2(I). (3.19)

    where H(I)=β1I+β2f(W)=β1I+β2f(kIδ+ηl). Since f(W) is a monotonic function of W, H(I) is an increasing function. Moreover

     F1(I)=Am(1C)(λ+d+r)2H(I)H(I)ϵ(λ+d+r)Q2+Am(1C)(λ+d+r)H(I)[ϵ(d+r)(λ+d+r+θ)+(d+m)(λ+d+r)]Q2. (3.20)

    It is now clear that F1(I)<0 for all IΓ. In other words, F1(I) decreases monotonically in Γ.

    The derivative of F2(I) is

    F2(I)=CAH(I)+(d+e)H(I)(d+e)IH(I)H2(I)+ϵ(1C)A[mα(λ+r+d)(λ+r+d+θ)H(I)]Q2+ϵ(1C)A{ϵH(I)[(λ+r+d)(θ+d+r+H(I))λθ]2}Q2. (3.21)

    By noticing that

    (d+e)H(I)(d+e)IH(I)=(d+e)[β1I+β2f(W)](d+e)I[β1+β2f(kIδ+ηl)kδ+ηl]=(d+e)β2[f(W)If(kIδ+ηl)kδ+ηl]. (3.22)

    and (f(W)I)0, (If(W))=f(W)If(kIδ+ηl)kδ+ηlf2(W)0 for all IΓ, we have that F2(I)>0.

    Let

    G(I)=F1(I)F2(I). (3.23)

    This means that

    G(I)=CA(d+e)IH(I)+Am(1C)(λ+d+r)+ϵA(1C){(λ+d+r)[θ+d+r+H(I)]λθ}Q. (3.24)

    Thus, we have G(I)=F1(I)F2(I)<0. G(I) is a monotonically decreasing function when 0<I<Adα. If the function G(I) has a zero point, it must be unique. This means that if model (3.1) has a positive equilibrium point, it must be unique. Let us now address the value of the G function at G(Ad+e) and G(0+). First we consider G(Ad+e),

    G(Ad+e)=(C1)AH(I)+Am(1C)(λ+d+r)+ϵA(1C){(λ+d+r)[θ+d+r+H(I)]λθ}Q. (3.25)

    Next, consider G(Ad+e) as a function on C, say J(C). Then J(1)=0, and

    J(C)=Am(λ+d+r)ϵA{(λ+d+r)[θ+d+r+H(I)]λθ}Q+AH(I)=P[d+m+ϵH(I)]{(λ+d+r)[H(I)+d+θ+r]λθ}mα(λ+d+r+θ)1H(I). (3.26)

    where

    P=A[d+m+ϵH(I)]{(λ+d+r)[H(I)+d+θ+r]λθ}mAα(λ+d+r+θ)Am(λ+d+r)H(I)ϵA{(λ+d+r)[θ+d+r+H(I)]λθ}H(I)=A(d+m){(λ+d+r)[H(I)+d+θ+r]λθ Amα(λ+d+r+θ)Am(λ+d+r)H(I)=Am(λ+d+r)[dα+H(I)H(I)]+Am{(λ+d+r)(θ+r)λθαθ}+Ad{(λ+d+r)[H(I)+d+θ+r]λθ}. (3.27)

    Since d>α, we havet p>0, i.e., J(C)>0. If 0C<1,J(C)<J(1)=0 always holds. Therefore G(Ad+e)<0. When C=1, G(Ad+e)=0.

    Let us now focus on the sign of G(0). There are three cases: 0<C<1, C=1 and C=0.

    Case1 0<C<1. Noticing that H(0)=0, we have I0, G(0)+, i.e., δ1>0 s.t. as I(0,δ1), G(I)>0 holds. The function G(I) has a unique zero point between 0 and Ad+e.

    Case2 C=1. G(Ad+e)=0, and G(I) is a monotonically decreasing function when 0<I<Adα. The function G(I) has thus a unique zero point at I=Ad+e, and model (3.1) has only one boundary equilibrium point (0,0,Ad+e,0,Ak(d+e)(δ+ηl)).

    Case3 C=0. We have

    limI0G(I)=Am(λ+d+r)+ϵA{(λ+d+r)[θ+d+r]λθ}[d+m]{(λ+d+r)[d+θ+r]λθ}mα(λ+d+r+θ)+limI0(d+e)IH(I).

    Since

    limI0(d+e)IH(I)=limI0(d+e)β1+β2f(W)kδ+ηl=(d+e)β1+β2f(0)kδ+ηl,limI0G(I)=Am(λ+d+r)+ϵA{(λ+d+r)[θ+d+r]λθ}[d+m]{(λ+d+r)[d+θ+r]λθ}mα(λ+d+r+θ)+(d+e)β1+β2f(0)kδ+ηl=d+eβ1+β2f(0)kδ+ηl(R01). (3.28)

    Thus G(0+)>0 if and only if R0>1. The function G(I) has a unique zero point between 0 and Ad+e if R0>1. When R0=1 or R0<1, there are no zero points for G(I). The proof is completed.

    Remark. From the above proof, it can be seen that the model (3.1) does not have a disease-free equilibrium point when 0<C1. When C=0, the disease-free equilibrium point exists if and only if R01. When C=1, the model (3.1) has only one boundary equilibrium point.

    Next we prove the global stability of the endemic equilibrium point. For the sake of convenience, we omit the t-dependence and use Sj, Sa, I, V, W to denote Sj(t), Sa(t), I(t), V(t), W(t). The following lemma will be useful later.

    Lemma 5. [22] Supposing that assumptions (H1)–(H3) hold,

    F(W)=ϕ(f(W)f(W)ϕ(WW)0,

    where ϕ is defined by ϕ(x)=x1ln(x).

    Theorem 6. Assuming (H1)–(H3) and 0<α<d<1, the endemic equilibrium E of system (3.1) is globally asymptotically stable if any one of the following conditions holds: (a) 0<C<1; (b) C=0 and R0>1.

    Proof. For model (3.1), we construct the following Lyapunov function:

    L=b1(SjSj+SjlnSjSj)+b2(SaSa+SalnSaSa)+b3(II+IlnII)+b4(VV+VlnVV)+b5(WW+WlnWW), (3.29)

    where

    b1=b2=b3=1,b4=b4+b4=λVθSab2+dVθSab2,b5=b5+b5=1kI[b1ϵβ2Sjf(W)+b2β2Saf(W)]. (3.30)

    The derivative of L, according to (3.7), is

    dLdt=dSjdt(1SjSj)+dSadt(1SaSa)+dIdt(1II)+b4dVdt(1VV)+b5dWdt(1WW). (3.31)

    Moreover, we have that:

    dSjdt(1SjSj)=(d+m)Sj(1SjSj)(1SjSj)+ϵβ1ISj(1SjISjI)(1SjSj)+ϵβ2Sjf(W)(1Sjf(W)Sjf(W))(1SjSj)+αSa(SaSa1)(1SjSj)+αV(VV1)(1SjSj). (3.32)
    dSadt(1SaSa)=(r+θ+d)Sa(1SaSa)(1SaSa)+β1ISa(1SaISaI)(1SaSa)+β2Saf(W)(1Saf(W)Saf(W))(1SaSa)+mSj(SjSj1)(1SaSa)+λV(VV1)(1SaSa). (3.33)
    dIdt(1II)=CA(1II)(1II)+ϵβ1SjI(SjISjIII)(1II)+ϵβ2Sjf(W)(Sjf(W)Sjf(W)II)(1II)+β1SaI(SaISaIII)(1II)+β2Saf(W)(Saf(W)Saf(W)II)(1II). (3.34)
    b4dVdt(1VV)=b4θSa(SaSaVVSaVSaV+1)=λV(SaSaVVSaVSaV+1)+dV(SaSaVVSaVSaV+1). (3.35)
    b5dWdt(1WW)=b5kI(IIWWWIWI+1)=(b5+b5)kI(IIWWWIWI+1). (3.36)

    Let us now introduce the quantities

    A1=ϵβ1SjI(1SjISjI)(1SjSj)+ϵβ2Sjf(W)(1Sjf(W)Sjf(W))(1SjSj)+ϵβ1SjI(SjISjIII)(1II)+ϵβ2Sjf(W)(Sjf(W)Sjf(W)II)(1II)=ϵβ1SjI(2SjSjSjSj)+ϵβ2Sjf(W)(2SjSjIISjIf(W)SjIf(W)Sjf(W)Sjf(W)+f(W)f(W))ϵβ1SjI(2SjSjSjSj)+ϵβ2Sjf(W)(f(W)f(W)lnf(W)f(W)II+lnII)ϵβ2Sjf(W)(f(W)f(W)lnf(W)f(W)II+lnII). (3.37)
    A2=β1ISa(1SaISaI)(1SaSa)+β2Saf(W)(1Saf(W)Saf(W))(1SaSa)+β1SaI(SaISaIII)(1II)+β2Saf(W)(Saf(W)Saf(W)II)(1II)=β1ISa(2SaSaSaSa)+β2Saf(W)(2SaSaIISaIf(W)SaIf(W)Saf(W)Saf(W)+f(W)f(W))β1ISa(2SaSaSaSa)+B. (3.38)
    A3=λV(VV1)(1SaSa)+(r+θ)Sa(1SaSa)(1SaSa)+λV(SaSaVVSaVSaV+1)=λV(2SaVSaVSaVSaV)+[(r+θ)SaλV](2SaSaSaSa)[(r+θ)SaλV](2SaSaSaSa). (3.39)
    A4=mSj(SjSj1)(1SaSa)+mSj(1SjSj)(1SjSj)=mSj(1SjSjSjSaSaSj+SaSa)=[(r+θ+d)SaλV+β1SaI+β2Saf(W)](1SjSjSjSaSaSj+SaSa)=[(r+d)Sa+(d+r)V+β1SaI+β2Saf(W)](1SjSjSjSaSaSj+SaSa). (3.40)
    A5=dSj(1SjSj)(1SjSj)+CA(1II)(1II)=dSj(2SjSjSjSj)+CA(2IIII)0, (3.41)

    which allow us to rewrite the derivative as

    dLdt=A1+A2+A3+A4+A5+dSa(1SaSa)(1SaSa)+αSa(SaSa1)(1SjSj)+αV(VV1)(1SjSj)+dV(SaSaVVSaVSaV+1)+b5kI(IIWWWIWI+1)A1+B+β1ISa(2SaSaSaSa)+[(r+θ)SaλV](2SaSaSaSa)+[(r+θ+d)SaλV+β1SaI+β2Saf(W)](1SjSjSjSaSaSj+SaSa)+b5kI(IIlnII+lnWWWW)+dSa(1SaSa)(1SaSa)+αSa(SaSa1)(1SjSj)+αV(VV1)(1SjSj)+dV(SaSaVVSaVSaV+1)=A1+B+(3SaSaSjSjSjSaSaSj)[(d+r)Sa+(d+r)V+β1SaI]+β2Saf(W)(1SjSjSjSaSaSj+SaSa)+b5kI(IIlnII+lnWWWW)+αSa(SaSa1)(1SjSj)+αV(VV1)(1SjSj)+dV(SaSaVVSaVSaV+1)A1+b5kI(IIlnII+lnWWWW)+B+β2Saf(W)(1SjSjSjSaSaSj+SaSa)+(3SaSaSjSjSjSaSaSj)(dSa+dV)+αSa(SaSa1)(1SjSj)+αV(VV1)(1SjSj)+dV(SaSaVVSaVSaV+1). (3.42)

    Noticing that

    B+β2Saf(W)(1SjSjSjSaSaSj+SaSa)=β2Saf(W)(3IISaIf(W)SaIf(W)Saf(W)Saf(W)SjSjSaSjSaSj+f(W)f(W))β2Saf(W)(f(W)f(W)lnf(W)f(W)II+lnII). (3.43)

    and

    d(3SaSaSjSjSjSaSaSj)(Sa+V)+αSa(SaSa1)(1SjSj)+αV(VV1)(1SjSj)+dV(SaSaVVSaVSaV+1)=(dα)Sa(3SaSaSjSjSjSaSaSj)+αSa(2SaSjSaSjSjSaSaSj)+dV(4VVSaVSaVSjSjSjSaSjSa)+αV(VV1)(1SjSj)=(dα)Sa(3SaSaSjSjSjSaSaSj)+αSa(2SaSjSaSjSjSaSaSj)+(dα)V(4VVSaVSaVSjSjSjSaSjSa)+αV(3SaVSaVSjSaSaSjVSjVSj)0. (3.44)

    Then, we have

    dLdtϵβ2Sjf(W)(f(W)f(W)lnf(W)f(W)II+lnII)+b5kI(IIlnII+lnWWWW)+β2Saf(W)(f(W)f(W)lnf(W)f(W)II+lnII)+b5kI(IIlnII+lnWWWW)=ϵβ2Sjf(W)(f(W)f(W)lnf(W)f(W)II+lnII)+ϵβ2Sjf(W)kI(IIlnII+lnWWWW)+β2Saf(W)(f(W)f(W)lnf(W)f(W)II+lnII)+β2Saf(W)kI(IIlnII+lnWWWW)=ϵβ2Sjf(W)(f(W)f(W)lnf(W)f(W)+lnWWWW)+β2Saf(W)(f(W)f(W)lnf(W)f(W)+lnWWWW)=[ϵβ2Sjf(W)+β2Saf(W)](f(W)f(W)lnf(W)f(W)+lnWWWW)=[ϵβ2Sjf(W)+β2Saf(W)][Φ(f(W)f(W))Φ(WW)]. (3.45)

    According to Lemma 5, we have dLdt0. On the other hand dLdt=0 holds if and only if (Sj,Sa,I,V,W)=(Sj,Sa,I,V,W). From Lyapunov's Direct Method, one concludes that E=(Sj,Sa,I,V,W) is globally asymptotically stable if it exists. The proof is completed.

    Remark. From the above theorem, it can be seen that endemic equilibrum is globally asymptotically stable iff it exist.

    Theorem 7. Supposing that assumptions (H1)–(H3), 0<α<d<1 and C=1 hold, the boundary equilibrium point E1=(0,0,Ad+e,0,Ak(d+e)(δ+ηl)) of system (3.1) is globally asymptotically stable.

    Proof. For model (3.1), we construct the following Lyapunov function:

    L1=a1Sj+a2Sa+a3(II1+I1lnII1)+a4V+a5(WW1+W1lnWW1), (3.46)

    where

    a1=a2=a3=a4,a5=AkI1a3. (3.47)

    The derivative of L1 along model is

    dL1dt=a1dSjdt+a2dSadt+a3dIdt(1I1I)+a4dVdt+a5dWdt(1W1W). (3.48)

    Moreover, we have that

    a1dSjdt=a1{α(V+Sa)(d+m)Sjϵ[β1SjI+β2Sjf(W)]},a2dSadt=a2{mSj+λV[β1SaI+β2Saf(W)](r+θ+d)Sa},a3dIdt(1I1I)=a3(1I1I){A+ϵ[β1SjI+β2Sjf(W)]+β1SaI+β2Saf(W)dIeI},=a3(1I1I){ϵ[β1SjI+β2Sjf(W)]+β1SaI+β2Saf(W)}+a3A(1I1I)(1II1),a4dVdt=a4[θSa(λ+d+r)V],a5dWdt(1W1W)=a5(1W1W)[kI(δ+ηl)W]=a5kI1(II1WW1W1IWI1+1). (3.49)

    Thus

    dL1dt=a1αV+a1αSaa1(d+m)Sja1ϵβ1SjIa1ϵβ2Sjf(W)+a2mSj+a2λVa2β1SaIa2β2Saf(W)(r+θ+d)a2Sa+a3ϵβ1SjI+a3ϵβ2Sjf(W)+a3β1SaI+a3β2Saf(W)a3ϵβ1SjI1a3β1SaI1a3I1I[ϵβ2Sjf(W)+β2Saf(W)]+a4θSaa4(λ+d+r)V+Aa3(2II1I1I)+a5kI1(II1WW1W1IWI1+1)=[a1α(r+θ+d)a2+a4θa3β1I1]Sa+[a1α+a2λa4(λ+d+r)]V+[a1(d+m)+a2ma3ϵβ1I1]Sj+β1SaI(a2+a3)+β2Saf(W)(a2+a3)+ϵβ1SjI(a1+a3)+ϵβ2Sjf(W)(a1+a3)a3β2Sjf(W)II1a3β2Saf(W)II1+Aa3(2II1I1I)+a5kI1(II1WW1W1IWI1+1)Aa3(3I1IWW1W1IWI1)0. (3.50)

    We get \frac{dL}{dt} \le 0 . And \frac{dL}{dt} = 0 holds if and only if I = I_1 , W = W_1 . From Lyapunovs Direct Method, the boundary equilibrium point E_1 is globally asymptotically stable if it exists. The proof is completed.

    In this section, we first study the dynamics of the model using the value of parameters from references [6,12] as well as hypothetical data. We then fit the model to real data provided by our collaborators about sheep infections in the Yulin region of China from 2005 to 2014. Finally, we perform some numerical analysis to assess the effects of the control measures using different environmental infection functions.

    Taking f(W) = \frac{W}{N} as an example, the parameters are selected as in Table 1. In this paper all the parameters are measured in years, in addition to environmental disinfection frequency units is times/year.

    Table 1.  Values of parameters.
    Parameter Range Value Origin
    \alpha 0–0.015 0.015 assumption
    m 0–2 1.06 [19]
    d 0–1 0.25 [20]
    \epsilon 0–1 0.4 assumption
    e 0.2–0.3 0.25 [20]
    \lambda 0–1 0.4 [10]
    \theta 0.05–0.15 0.1 [10]
    k 10–20 16 [20]
    \delta 0–0.9 0.6 [10]
    \eta 0.5–0.75 0.6 [10]
    l 1–4 2 assumption
    r 0–1 0.0328 assumption

     | Show Table
    DownLoad: CSV

    We assume that the initial values are S_j(0) = 1860 , S_a(0) = 1845 , I(0) = 110 , V(0) = 1185 , W(0) = 50 and the exposure infection rates are given by \beta_1 = 0.000038 , \beta_2 = 0.0000135 .

    Example 1: Let C = 0 , A = 3000 , e = 0.25 , then R_0 = 0.7455 < 1 . Figure 2 shows that the disease-free equilibrium point of the model is globally asymptotically stable.

    Figure 2.  Dynamic behavior of model (3.1).

    Example 2: Let C = 0 , A = 3000 , e = 0.05 , then R_0 = 1.24244 > 1 . The presence and stability of the positive equilibrium point in Figure 3 can be observed.

    Figure 3.  Annual stocking, slaughter, and brucellosis-infected sheep in elmwood, from 2005 to 2014.

    Example 3: Let C = 0.03 , at this point, the endemic equilibrium point is always present and globally stable, which is independent of whether R_0 is larger than one or not.

    In order to simulate real-world situations, one set a specific environmental exposure function. The results of the previous Sections show that the three commonly used environmental exposure functions lead to consistent results for the dynamics of the model. A question however arises abut the sensitivity the models employing different exposure functions with respect to control parameters In order to facilitate the comparison, we use flock data from Yulin, China and establish a common range of variations.

    Using the statistical bulletin of national economic and social development of Yulin City [from the website of Yulin municipal government (www.yl.gov.cn)], we obtain the stock and slaughter of sheep for each year from 2005 to 2014, and combined with the annual infection rate of sheep, we get the number of infected sheep, see the Figure below.

    We use the least square method to estimate the parameters. Through DEDiscover software (DEDiscover is a general-purpose tool to perform simulation), we fit each of the three cases to find a combination of parameters that is closer to the actual results. The fit parameters can be seen in Tables 24. Figure 4 illustrates the results of the three fits against the actual data, and show the good quality of the fits. The sum of squared residuals for all three sets of parameters is about 0.044. Using the method of Akaike information criterion (AIC) [23,24] to compare the three models, we get AIC_1 = -162.832 , AIC_2 = -162.401 , AIC_3 = -162.609 . Case 1 is more suitable for the data, but the three values do not differ much.

    Table 2.  The fitting parameters of model (2.1), case 1.
    Parameteres estimated Value Standard error CI Low Bound CI High Bound p-value t-statistc
    A 56.4259 0.313 55.7545 57.0973 5.7578e-25 180.2584
    C 0.0511 0.0024 0.0460 0.0562 3.8467e-12 21.5719
    \alpha 0.0763 0.0085 0.0579 0.0946 3.7566e-07 8.9233
    \beta_1 0.0025 1.0611e-04 0.0022 0.0027 1.4638e-12 23.1552
    \beta_2 0.0047 0.0018 8.5601e-04 0.0086 0.0203 2.6181
    d 0.3976 0.0025 0.3923 0.4029 3.0768e-24 159.9128
    \delta 0.3327 0.0244 0.2804 0.3850 1.7633e-09 13.6483
    e 0.5082 0.0114 0.4838 0.5326 1.6559e-16 44.7058
    \epsilon 0.9967 0.0331 0.9256 1.0677 4.0378e-14 30.0711
    k 17.5393 0.2112 17.0862 17.9923 2.9419e-20 83.0345
    l 1.4690 0.0598 1.3407 1.5973 6.5367e-13 24.5603
    \lambda 0.1496 0.0123 0.1233 0.1758 7.5555e-09 12.2009
    m 0.9912 0.0525 0.8787 1.1037 2.3150e-11 18.8982
    r 0.0328 37793e-04 0.0320 0.0336 1.5785e-201 86.8174
    \theta 0.0501 0.0076 0.0339 0.0664 1.1311e-05 6.6307
    \eta 0.1416 0.0214 0.0957 0.1876 1.1722e-05 6.6089

     | Show Table
    DownLoad: CSV
    Table 3.  The fitting parameters of model (2.1), case 2 ( \beta_2 = 0.000089823 ).
    Parameteres estimated Value Standard error CI Low Bound CI High Bound p-value t-statistc
    A 12.2853 0.2742 11.6972 12.8734 1.6061e-16 44.8041
    C 0.1904 0.0072 0.1749 0.2059 2.5258e-13 26.3226
    \alpha 0.1353 0.0082 0.1178 0.1529 1.3772e-10 16.5493
    \beta_1 0.0022 1.6176e-04 0.0019 0.0026 1.4636e-09 13.8439
    d 0.2625 0.0122 0.2364 0.2887 3.9324e-12 21.5371
    \delta 0.4176 0.0394 0.3332 0.5020 4.4754e-08 10.6080
    e 0.3992 0.0223 0.3512 0.4471 4.9353e-11 17.8659
    \epsilon 0.4917 0.0835 0.3127 0.6708 3.9362e-05 5.8899
    \epsilon_1 0.4270 0.0229 0.3778 0.4762 2.8413e-11 18.6135
    k 19.3771 0.4363 18.4414 20.3129 1.8132e-16 44.4150
    l 2.4550 0.3113 1.7873 3.1227 1.6182e-06 7.8858
    \lambda 0.4027 0.0330 0.3320 0.4735 7.5501e-09 12.2016
    m 0.9990 0.0290 0.9368 1.0612 6.1839e-15 34.4425
    r 0.0324 1.5958e-04 0.0321 0.0328 1.0809e-25 203.1440
    \theta 0.0505 0.0116 0.0256 0.0755 6.7570e-04 4.3425
    \eta 0.9073 0.0551 0.7890 1.0256 1.4868e-10 16.4547

     | Show Table
    DownLoad: CSV
    Table 4.  The fitting parameters of model (2.1), case 3 ( \beta_1 = 0.000038 ).
    Parameteres estimated Value Standard error CI Low Bound CI High Bound p-value t-statistc
    A 63.0960 0.6672 61.6651 64.5270 4.7739e-21 94.5722
    C 0.0499 0.0028 0.0439 0.0559 5.1580e-11 17.8074
    M 1.0807 0.1112 0.8422 1.3193 1.3344e-07 9.7152
    \alpha 0.0773 0.0069 0.0626 0.0921 2.1972e-08 11.2233
    \beta_2 6.7353e-04 8.8527e-05 4.8366e-04 8.6340e-04 2.4445e-06 7.6083
    d 0.3936 0.0066 0.3795 0.4078 2.9666e-18 59.6700
    \delta 0.9913 0.0575 0.8679 1.1147 8.0195e-11 17.2316
    e 0.6220 0.0537 0.5068 0.7373 1.4805e-08 11.5770
    \epsilon_1 0.8998 0.0638 0.7630 1.0365 1.1364e-09 14.1134
    k 13.7981 0.4110 12.9166 14.6797 8.8192e-15 33.5705
    l 3.8894 0.2323 3.3911 4.3877 1.1816e-10 16.7400
    \lambda 0.4033 0.0358 0.3265 0.4800 2.0793e-08 11.2722
    m 0.6428 0.0173 0.6057 0.6799 2.1942e-15 37.1164
    r 0.0350 2.8065e-04 0.0344 0.0356 9.7852e-23 124.8799
    \theta 0.0504 0.0053 0.0391 0.0618 1.6581e-07 9.5449
    \eta 0.7207 0.0690 0.5727 0.8686 5.4081e-08 10.4489

     | Show Table
    DownLoad: CSV
    Figure 4.  Fitting results against actual data. N, S_0, I denote the number of livestock, slaughter, and infected sheep, respectively.

    In order to put the three sets of values in a unified coordinate system, we used logarithmic values and then compared them. From Figure 4, we conclude that in three cases, there is no obvious difference in the simulation results.

    In this section, we numerically compare and analyze results from the perspective of disease control. Our main concern is to assess how sensitive are the different environmental infection exposure functions to control measures. If the magnitude of the variation is comparable, then we can choose the first form containing fewer parameters. However, if the variations are larger, then we are also reminded that the formulation of the environmental infection pathway is something that needs to be chosen carefully in the modeling stage.

    The following control measures are investigated:

    1) Improve source management efforts of sheep to control the inflow of diseased sheep.

    2) Increase culling of diseased sheep to reduce the infection base.

    3) Standardize the disinfection of the environment to reduce the risk of environmental infection.

    Based on the assumed values of the model parameters, we then change the control parameters in the above strategies to achieve a reduction in the number of infected sheep (I) . Obviously, some of these parameters need to be increased (such as e and l ) and some need to be decreased (such as \beta_2 and C ). Here, we consider a 50 \% range of parameter changes to analyze the changes in the number of infected sheep.

    In the above plots, we use a superimposed quantized visualization to show the range and the magnitude of the variationa of I across the parameter range. This facilitates the comparison of three models.

    As can be seen in Figures 58, all the control measures lead to a decrease in the number of infected sheep. However, the dynamics of the model is different for the three functions. In particular, the magnitude of the change of I with the parameters is different. The effects of parameters C and e is not much different in the three cases, whereas for parameter \beta_2 , the magnitude of change in I is significantly greater in case 3 than in the first two cases, with case 2 being almost insensitive. Concerning parameter l , case 2 remains insensitive, whereas in case 3 the number of infected sheep can be reduced by 50 \% of the initial value, while this is not possible in the first two cases. For case 2, we scaled the upper limit of the environmental exposure rate to 0.0078 and scaled the environmental modulation parameter \epsilon_1 to a range of values of (0,150) . As it can be seen in Figure 9, the magnitude of the change in I is small and still reflects the insensitivity to the environmental modulation parameter.

    Figure 5.  Comparison among the reductions in the number of infected sheep by adjusting the magnitude of parameter C by 50\%.
    Figure 6.  Comparisno among the reductions the environmental exposure to infection by adjusting the magnitude of parameter \beta_2 by 50\%.
    Figure 7.  Comparison among the numbers of culled infected sheep by adjusting the parameter magnitude e by 50\%.
    Figure 8.  Comparison among the average number of disinfections per year by adjusting the parameter magnitude l by 50\%.
    Figure 9.  Quantile plots of the number of infected sheep and the magnitude of the environmental virulence load versus the variation with \beta_2 \in (0, 0.0078) and \epsilon_1 \in (0,150).

    In this paper, a stage-specific dynamic model of brucellosis in sheep has been suggested and analyzed. Due to the constant input of infected sheep, there is no disease-free equilibrium point in the model, which means that Brucella is always transmitted in the flock. Numerical simulationz show that the following measures can effectively reduce the scale of the epidemic and control the occurrence of brucellosis: 1) Strengthen the monitoring of imported individuals; 2) Disinfect the environment regularly; 3) Once infected sheep are found, they should be promptly slaughtered.

    Looking at the index parameters of the fitting for the three models, we have found that case l is closer to actual data, and this is consistent with the conclusions of reference [6]. If the second environmental exposure function is chosen, for C = 0 , our results are consistent with the results of reference [8]. If the third environmental exposure function is chosen our results are consistent with those of reference [12] for C = 0 . However, when 0 < C < 1 , we have found that the epidemic of persists because a disease-free equilibrium points does not exist. In particular, when C = 1 , the disease-free equilibrium point, and the positive equilibrium point do not exist. On the contrary, there exists a boundary equilibrium point with global asymptotic stability, which corresponds to a situation in which all sheep are eventually infected.

    Although the dynamical behavior is similar for the three environmental exposure functions, we have found that the sensitivity may be considerably different. Results from numerical simulations for cases 1 and 2 have shown that the number of infections is not much affected by changes in the environmental control parameters. On the contrary, in case 3 the sensitivity is significant. In particular, in the third case it is possible to achieve a control goal to reduce the number of infections to less than half of the initial value.

    In the literature about infections by Brucellae, specific functional expressions of environmental infections have been.employed and pathways of environmental infection are considered. However, little attention has been paid to the variability exhibited by the different environmental functional expressions. To fill this gap, we have compared those common forms and found that their differences have a significant effect on the selection of optimal control methods. Our results clearly show that different function expressions yield different optimal control results, and that the expressions of environmental infection pathwayswe should be chosen carefully.

    In this paper we have adopted a relatively simple ODE model for the spread of brucellosis virus in sheep, unifying the results of the analysis of the dynamical behavior of the environmental exposure function under certain characteristics. However, in practice, there is a certain time delay from exposure to the virus to infection with the virus, and this phenomenon is more common in disease transmission including pathogenic infections [25,26,27,28]. Then whether different environmental infection exposure functions will show greater variability under the infectious disease model of delayed infection or delayed distribution will be the next step of our research.

    The authors acknowledge the useful suggestions and thoughtful comments made by the referees on their earlier version of this work. This work has been supported by the Industry-University-Research project of science and technology plan of Yulin City, Shaanxi Province (CXY-2020-087), Natural Science Foundation Project of Shaanxi Province, China (2023-JC-YB-084).

    The authors declare there is no conflict of interest.



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