
Citation: Yuhua Long, Yining Chen. Global stability of a pseudorabies virus model with vertical transmission[J]. Mathematical Biosciences and Engineering, 2020, 17(5): 5234-5249. doi: 10.3934/mbe.2020283
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Pseudorabies virus (PRV) infection, also known as Aujeszky's disease (AD), which is caused by pseudorabies virus (PRV) or suid herpesvirus 1 (SuHV-1), can be found all over the world and is common in pigs, cattle, sheep and cats, and is a major economic threat to swine producers[1,2,3]. It is an infection and all animals, including pigs, have frequent fevers with typical symptoms such as itching and encephalomyelitis. In particular, pigs are natural hosts and reservoirs of the pseudorabies virus. If a dog or cat contacts with the feed form of an infectious pig, Aujeszky's disease may spread. Cattle and sheep may also be infected if they are in contact with sick pigs, resulting in clinical symptoms and possible death [4]. The infection can also be age-dependent. Once pigs are infected with pseudorabies, the clinical symptoms vary in different age groups. For example, it will make pregnant sows appear some symptoms such as miscarriage, stillbirth, mummified fetus and infertility, whereas adult sows and boars often present with reproductive and respiratory symptoms. For the piglets within 15 days of age, the mortality rate can reach 100%, and the incidence of weaned piglets can reach 40%, and the mortality rate is about 20% [5]. Moreover, PRV can cause adult fat pigs growth stagnation and slow weight gain, and the virus is mainly transmitted through direct or indirect contact. Infected sows can pass to piglets through breast milk.
Pseudorabies virus (PRV) infection is extremely infectious, causing economic losses worldwide in the pig industry. It was first reported in Hungary by Aladar Aujeszky in 1902 [6]. Hanson [7] referred to the description of the disease in the U.S. in 1813 but it was not known as Aujeszky's disease until 1931. In the mid-20th century, PRV infection was more prevalent in Eastern Europe countries and the Balkans. Since the 1990s, Pseudorabies virus (PRV) infection had been controlled by PR vaccine [8] to a certain extent. However, a PR outbreak occurred in northern and eastern China in late 2011 [9]. Each outbreak of PR results in severe economic losses and has a considerable impact in the world. Therefore, Pseudorabies virus (PRV) infection has brought many researchers' attentions to study it. For example, the work in [1] studied the transmission characteristics of pseudorabies and the infection situation in different periods, and phylogenetic analysis was carried out in [8,10,11]. Among those existing results, there were few related mathematical models formulated to study the dynamics of the disease. Recently, PRV becomes more serious concerns for the health of pigs and particularly in the actual pig breeding process in China [12]. Pseudorabies virus is listed in an official document of the Chinese government, as a priority infectious disease that needs to be controlled and eradicated in swine breeding farms by the end of 2020 [13].The control and prevention of the disease thus is more urgent, and further mathematical modeling study becomes important.
Motivated by the observations above, we formulate in this paper a compartmental susceptible-exposed-infectious-treated (SEIT) model with vertical transmission according to the characters of PRV infection, and study the transmission dynamics of the disease. We first give model descriptions in Section 2. We define the basic reproduction number and investigate the dynamical behavior of the disease free equilibrium in Section 3. We study the existence and uniqueness of a disease-endemic equilibrium in Section 4. Using the Lyapunov functional method [14] together with the competitive system theory, we determine the global asymptotic stability of the disease-endemic equilibrium. Finally, we give brief concluding remarks to complete this paper in Section 5.
We divide the swine population into four classes, the susceptible (S), exposed (E), infectious (I) and treated (T), such that the total population size is N = S+E+I+T. When the Pseudorabies virus infection is identified, all swines with no symptoms are tested. Those tested positive carry viruses and are from the exposed class E. They are then treated. The usual treatment is injecting high immune serum antibody against pseudorabies. But it only has certain effect on suckling piglets, for adult pigs, the effect of medical treatment is not obvious, but the symptoms are temporarily relieved. An individual who after treatment can go back to the E class after contacting with infected pigs [15]. Thus, after the treatment, some of them in class E become infective, progressing to class I with rate v1, because the treatment fails to work, and some of them in class E become partially immune, entering class T with rate v2. The symptomatic infected swines in class I are also treated. After the treatment, they become asymptomatic. Some of them still carry viruses but with no immunity and thus reenter class E with fraction p1, and some of them carry viruses but with partial immunity and thus enter class T with fraction p2. Note that the individuals in class T has only partial immunity and thus become infected after contacting infected swines in class I.
Let the birth rate and natural death rate of the population be b and d, respectively. Considering vertical transmission, we assume that a fraction δ of the offspring produced by infectious swines are infectious. We assume that the offspring from other swines are susceptible. Then the total infectious offspring are bδI and the susceptible offspring are b(N−I)+b(1−δ)I=b(N−δI). The horizontal transmission is assumed to take the form of direct contact between the infectious swines and the susceptible or treated swines and the incidence rate βSIN or βTIN thus is of the standard mass-action form. Let α represent the disease-related death rate. The model dynamics are illustrated in Figure 1.
The model dynamics are described by the following differential equations together with non-negative initial conditions:
{dSdt=b(N−δI)−βSIN−dS,dEdt=βSIN+βTIN+p1I−(v1+v2+d)E,dIdt=bδI+v1E−(p1+p2+d+α)I,dTdt=v2E+p2I−βTIN−dT. | (2.1) |
To make the system biologically meaningful, all parameters are supposed to be positive and less than 1.
Adding all four equations of system (2.1) together leads to
dNdt=(b−d)N−αI. | (2.2) |
Let
x=SN,y=EN,z=IN,w=TN |
denote the fractions of the compartments S, E, I, and T in the population, respectively. It follows from (2.2) that
{dSdt=Ndxdt+x((b−d)N−αI),dEdt=Ndydt+y((b−d)N−αI),dIdt=Ndzdt+z((b−d)N−αI),dTdt=Ndwdt+w((b−d)N−αI), |
and then system (2.1) becomes
{dxdt=b−bδz−βxz−bx+αxz,dydt=βxz+βwz+p1z−(v1+v2+b)y+αyz,dzdt=bδz+v1y−(p1+p2+b+α)z+αz2,dwdt=v2y+p2z−βwz−bw+αwz. | (2.3) |
Since x+y+z+w=1, the dynamics of system (2.3) are equivalently described by
{dxdt=b−bδz−βxz−bx+αxz,dydt=β(1−y−z)z+p1z−(v1+v2+b)y+αyz,dzdt=bδz+v1y−(p1+p2+b+α)z+αz2. | (2.4) |
Define a closed set
Ω={(x,y,z)∣x≥0,y≥0,z≥0,0≤x+y+z≤1}. |
Then Ω is a positive invariant set with respect to system (2.4) [16]. We thus focus our investigation on the dynamical features of system (2.4) on Ω.
It is easy to see that system (2.4) always has a disease-free equilibrium, P0=(1,0,0). According to [17,18,19,20], the basic reproduction number of system (2.4) is
ℜ0=v1β(v1+v2+b)(p1+p2+b+α−bδ)−v1p1. |
.
We have the following results.
Theorem 1. Consider system (2.4). If ℜ0<1, then the disease-free equilibrium (DFE) P0=(1,0,0) is the unique equilibrium, which is globally asymptotically stable on Ω (i.e., the disease dies out regardless of its initial values) and if ℜ0>1, then the DFE P0 is unstable.
Proof
The Jacobian matrix of system (2.4) at P0 is
J(P0)=(−b0−bδ−β+α0−(v1+v2+b)β+p10v1bδ−(p1+p2+b+α)). |
It follows from
det(λI−J(P0))=|λ+b0bδ+β−α0λ+(v1+v2+b)−β−p10−v1λ+(p1+p2+b+α−bδ)|=(λ+b)((λ+v1+v2+b)(λ+p1+p2+b+α−bδ)−v1(β+p1))=(λ+b)(λ2+(m+n)λ+mn−v1p1−v1β)=0, | (3.1) |
where m=p1+p2+b+α−bδ>0, n=v1+v2+b>0 and m+n>0, that the eigenvalues of J(P0) satisfy
λ1=−b<0,λ2+λ3=−(m+n)<0,λ2λ3=mn−v1p1−v1β. | (3.2) |
Suppose ℜ0<1. Then mn−v1p1−v1β>0, and (3.2) ensures that all eigenvalues λi, i=1,2,3, are negative. Consequently, P0 is locally stable in Ω.
If ℜ0>1, then mn−v1p1−v1β<0, and it follows from (3.2) that λ2 and λ3 are of opposite sign; that is, either λ2>0, λ3<0 or λ2<0, λ3>0. As a result, the DFE P0 is unstable if ℜ0>1.
To show that the DFE is globally attractive for ℜ0<1, we consider a Lyapunov functional defined by
V=v1y+(v1+v2+b)z. |
Then V is positive and the derivative of V along the solutions of system (2.4) is given by
dVdt|(2.4)=v1(β(1−y−z)z+p1z−(v1+v2+b)y+αyz)+(v1+v2+b)(bδz+v1y−(p1+p2+b+α)z+αz2)=v1(β(1−y−z)z+p1z+αyz)−(v1+v2+b)(p1+p2+b+α−bδ−αz)z=v1β(1−y−z)z+v1p1z+v1αyz−n(m−αz)z=((v1β+(v1α−v1β)y+(αn−v1β)z+v1p1−mn)z. |
Using the method of calculating the maximum value of multivariate function, we get that in region Ω,
v1β+(v1α−v1β)y+(αn−v1β)z≤max{v1β,v1α,αn}, |
and then
dVdt|(2.4)≤(max{v1β,v1α,αn}−mn+v1p1)z. |
Since ℜ0<1, v1β<mn−v1p1 and thus
mn−v1p1=(v1+v2+b)(p1+p2+b+α−bδ)−v1p1=v1(p2+b+α−bδ)+(v2+b)(p1+p2+b+α−bδ)>α(v1+v2+b)>v1α. |
Recall n=v1+v2+b. Then we have mn−v1p1>max{v1β,v1α,αn} when ℜ0<1. Therefore,
dVdt≤0. |
In addition, dVdt=0 if and only if y=0 and z=0. Moreover, Ω={P0} is the largest invariant set in {(x,y,z)∈Ω|dVdt=0}. According to LaSalle's Invariance Principle ([21], Chapter 2, Theorem 6.4), the DFE P0 is globally asymptotically stable on Ω under the condition ℜ0<1.
In this section, we study the existence and stability of the disease-endemic equilibrium P∗=(x∗,y∗,z∗) with x∗>0, y∗>0 and z∗>0. Let a1=α(β−α), a2=(α−β)m+αn−v1β and a3=v1β+v1p1−mn. We have the following results.
Theorem 2. Suppose ℜ0>1. Then system (2.4) admits a unique disease-endemic equilibrium P∗=(x∗,y∗,z∗), where
x∗=b−bδz∗b+(β−α)z∗>0,y∗=β(1−z∗)+p1(β−α)z∗+(v1+v2+b)z∗>0,z∗=−a2−√a22−4a1a32a1>0. |
The disease-endemic equilibrium P∗ is locally asymptotically stable.
Proof
The components of the disease-endemic equilibrium must satisfy the following system
{b−bδz−βxz−bx+αxz=0,β(1−y−z)z+p1z−(v1+v2+b)y+αyz=0,bδz+v1y−(p1+p2+b+α)z+αz2=0. | (4.1) |
Obviously, (4.1) has no solutions in the form of (x1,y1,0) or (x2,0,z2) with x1>0, y1>0 or x2>0, z2>0. In the following, we look for the solution (x∗,y∗,z∗) of (4.1) with x∗>0, y∗>0 and z∗>0. It is straightforward to find that
x∗=b−bδz∗b+(β−α)z∗, | (4.2) |
y∗=β(1−z∗)+p1(β−α)z∗+(v1+v2+b)z∗, | (4.3) |
y∗=p1+p2+b+α−bδ−αz∗v1z∗. | (4.4) |
From (4.3) and (4.4), we have
β(1−z∗)+p1(β−α)z∗+(v1+v2+b)=p1+p2+b+α−bδ−αz∗v1. | (4.5) |
Thus
α(β−α)(z∗)2+((α−β)m+αn−v1β)z∗+v1β+v1p1−mn=0. | (4.6) |
Recall a1=α(β−α), a2=(α−β)m+αn−v1β and a3=v1β+v1p1−mn. Then (4.6) can be rewritten as
f(z∗)≜a1(z∗)2+a2z∗+a3=0. | (4.7) |
Notice that m=p1+p2+b+α−bδ>0 and n=v1+v2+b>0. Then, for ℜ0>1, we have
v1β>(v1+v2+b)(p1+p2+b+α−bδ)−v1p1=v1(p2+b+α−bδ)+(v2+b)(p1+p2+b+α−bδ)>α(v1+v2+b)>v1α, | (4.8) |
and thus β>α. Further, it follows from
a1=α(β−α)>0,a2=(α−β)m+αn−v1β<0,a3=v1β+v1p1−mn>0, | (4.9) |
that the associated discriminant of the quadratic equation f(z∗)=0 is
Δ=a22−4a1a3≥0. | (4.10) |
Moreover, from (4.7) and (4.9), we have
f(0)=a3>0 |
and
f(1)=a1+a2+a3=α(β−α)+(α−β)m+αn−v1β+v1β+v1p1−mn=α(β−α)−(β−α)(p1+p2+b+α−bδ)+α(v1+v2+b)+v1p1−(v1+v2+b)(p1+p2+b+α−bδ)<α(β−α)−(β−α)(p1+p2+α)+α(v1+v2+b)+v1p1−α(v1+v2+b)−(v1+v2+b)(p1+p2)=−(β−α)(p1+p2)−v1p2−(v2+b)(p1+p2)<0. |
Therefore, there is at least one positive z∗ satisfying 0<z∗<1.
We next show the uniqueness of z∗ in the interval (0,1) in the following two cases.
(I) If Δ=0, direct computation yields that z∗=−a22a1>0 is the unique solution of the quadratic equation (4.7).
(II) if Δ>0, we suppose f(z∗)=0 admits two unequal roots z∗1 and z∗2. Without loss of generality, let z∗1<z∗2. Then
z∗1=−a2−√a22−4a1a32a1, and z∗2=−a2+√a22−4a1a32a1. |
If 0<z∗1<1<z∗2, then obviously, z∗1 is the unique solution of equation (4.7) in the interval (0,1).
If 0<z∗1<z∗2<1, since a1>0 and the expression of f(z∗) in (4.7), we get both f(0)>0 and f(1)>0, which contradicts f(0)⋅f(1)<0. Hence, equation (4.7) possesses only one root, say z∗1.
Based on (4.2), (4.3), and the analysis above, it follows that if ℜ0>1, system (2.4) admits a unique disease-endemic equilibrium P∗=(x∗,y∗,z∗), where
x∗=b−bδz∗b+(β−α)z∗>0,y∗=β(1−z∗)+p1(β−α)z∗+(v1+v2+b)z∗>0,z∗=−a2−√a22−4a1a32a1>0. |
We now investigate the local stability of P∗ as follows.
Linearizing (2.4) around P∗=(x∗,y∗,z∗), we obtain the characteristic equation given by
g(η)=det(η+(β−α)z∗+b0(β−α)x∗+bδ0η+n+(β−α)z∗−β−p1+(β−α)y∗+2βz∗0−v1η+m−2αz∗)=(η+(β−α)z∗+b)(η2+(m1+m3)η+v1m2+m1m3) | (4.11) |
where m1=n+(β−α)z∗, m2=−β−p1+(β−α)y∗+2βz∗, m3=m−2αz∗,
Recall that (4.8) implies β>α. Then from (4.11), we have η1=−(β−α)z∗−b<0 and η2 and η3 satisfying the equation
η2+(m1+m3)η+v1m2+m1m3=0. | (4.12) |
Write Δ=a22−4a1a3. Then it follows from (4.9) and
z∗=−a2−√Δ2a1<−a22a1 |
that
−2αz∗>αa2a1=(α−β)m+αn−v1ββ−α, | (4.13) |
and together with ℜ0>1
−(η2+η3)=m1+m3=n+(β−α)z∗+m−2αz∗>(β−α)(m+n)β−α+(α−β)m+αn−v1ββ−α=β(v2+b)β−α>0. | (4.14) |
On the other hand, it follows from y∗=m−αz∗v1z∗ that
η2η3=v1m2+m1m3=−v1β−v1p1+v1(β−α)y∗+2v1βz∗+(n+(β−α)z∗)(m−2αz∗)=−v1β−v1p1+mn+2(v1β−αn)z∗+2m(β−α)z∗−3α(β−α)(z∗)2=−3α(β−α)(z∗)2+2(v1β−αn+m(β−α))z∗−v1β−v1p1+mn=−3a1(z∗)2−2a2z∗−a3. | (4.15) |
Substituting z∗=−a2−√Δ2a1 into (4.15), we then have
η2η3=−3(a22−2a1a3+a2√Δ)2a1−2a2(−a2−√Δ)2a1−2a1a32a1=4a1a3−a22−a2√Δ2a1=−Δ−a2√Δ2a1=√Δ(−√Δ−a2)2a1>√Δ(a2−a2)2a1=0, | (4.16) |
since Δ=a22−4a1a3<a22 and a2<0 which yields −√Δ>a2.
Hence, both η2 and η3 have negative real parts and thus we complete the proof of Theorem 2.
In addition to Theorem 2, we state our main result of the present section below.
Theorem 3. When ℜ0>1, if p1≥max{β,b}, then the disease-endemic equilibrium P∗ of System (2.4) is globally asymptotically stable.
Inspired by [22,23], we use the theory of competitive systems of differential equations to prove global stability of the endemic equilibrium P∗ of system (2.4). We first state the definition of competitive systems as follows.
Let h(x) be continuously differentiable and ∂h(x)∂x be the Jacobian matrix of h(x). If there is a diagonal matrix H=diag(ϵ1,ϵ2,…,ϵn), where each ϵi is either 1 or -1 (i=1,2,…,n), such that the non-diagonal elements of H∂h(x)∂xH are non-positive for all x∈Ω, then the differential equations dxdt=h(x) are called competitive systems [21,22,24,25].
For system (2.4), the associated Jacobian matrix J(x,y,z) is given by
J(x,y,z)=((α−β)z−b0(α−β)x−bδ0−(n+(β−α)z)(α−β)y−2βz+β+p10v1−m+2αz). |
Take matrix H as H=diag(−1,1,−1). Then
HJ(x,y,z)H=((α−β)z−b0(α−β)x−bδ0−(n+(β−α)z)(β−α)y+2βz−β−p10−v1−(m−2αz)). |
Let p1≥β. Then
(α−β)x−bδ<0, | (4.17) |
and
(β−α)y+2βz−β−p1≤(β−α)(1−z)+2βz−β−p1=βz−p1−α(1−z)<βz−p1<0. | (4.18) |
By (4.17), (4.18) and −v1<0, it is easy to obtain that the non-diagonal elements of HJ(x,y,z)H are all non-positive in Ω. Hence System (2.4) is a competitive system in region Ω. It is known that 3-dimensional competitive systems have the Poincaré-Bendixson property [25,26]. Similar to [21,22], we have:
Lemma 4.1. Consider system (2.4). An arbitrary nonempty compact ω-limit set of system (2.4), in the interior of Ω, can only be a periodic solution or the endemic equilibrium P∗.
To get the global stability of the endemic equilibrium P∗, we state a criterion for the asymptotic stability of a non-constant periodic solution to System (2.4) as follows.
Lemma 4.2. Suppose that γ={p(t):0≤t≤ω} is a non-constant periodic solution of system (2.4). If ℜ0>1, p1≥max{β,b}, then p(t) is asymptotically stable.
Proof
Suppose p(t) is a non-constant periodic solution of system (2.4). Let dy(t)dt=∂h(p(t))∂xy(t) be the linearized system of system (2.4) at p(t). According to Muldowney [27], when the zero solution of the second compound equation dz(t)dt=∂h(p(t))[2]∂xz(t) is asymptotically stable, the zero solution of dy(t)dt=∂h(p(t))∂xy(t) is also asymptotically stable. Therefore, in order to get the asymptotical stability of p(t), we show that the zero solution of dz(t)dt=∂h(p(t))[2]∂xz(t) is asymptotically stable.
Write p(t)=(˜x(t),˜y(t),˜z(t)) and let X=x−˜x(t), Y=y−˜y(t) and Z=z−˜z(t), then the linearized System (2.4) at p(t) is
{dXdt=(−b−β˜z(t)+α˜z(t))X−(bδ+β˜x(t)−α˜x(t))Z,dYdt=−(v1+v2+b+(β−α)˜z(t))Y−((β−α)˜y(t)+2β˜z(t)−β−p1)Z,dZdt=v1Y−(p1+p2+b+α−bδ−2α˜z(t))Z. | (4.19) |
Thus the second compound matrix J[2](x,y,z) of J(x,y,z) is
J[2](x,y,z)=(a11+a22(α−β)y−2βz+β+p1(β−α)x+bδv1a11+a33000a22+a33), |
where
a11+a22=2(α−β)z−(v1+v2+2b),a11+a33=(3α−β)z−(p1+p2+2b+α−bδ),a22+a33=(3α−β)z−(v1+v2+p1+p2+2b+α−bδ). |
Therefore, the corresponding dz(t)dt=∂h(p(t))[2]∂xz(t) can be expressed by
{dXdt=−(v1+v2+2b+2(β−α)˜z(t))X +((α−β)˜y(t)−2β˜z(t)+β+p1)Y+((β−α)˜x(t)+bδ)Z,dYdt=v1X−(p1+p2+2b+α−bδ+(β−3α)˜z(t))Y,dZdt=−(v1+v2+p1+p2+2b+α−bδ+(β−3α)˜z(t))Z. | (4.20) |
In order to show the asymptotic stability of system (4.20) around the solution zero, consider the following functional:
V(X,Y,Z;˜x(t),˜y(t),˜z(t))=sup{|X|,˜y(t)˜z(t)(|Y|+|Z|)}. | (4.21) |
Then V(X,Y,Z;˜x(t),˜y(t),˜z(t))≥0 for ˜x(t), ˜y(t) and ˜z(t)) all positive periodic functions. Moreover, V(X,Y,Z;˜x(t),˜y(t),˜z(t))=0 only if X=Y=Z=0. Since V(X,Y,Z;˜x(t),˜y(t),˜z(t)) is not continuously differentiable, similar to [21,24,28,29] or [30], we consider the right-upper derivative of V(X,Y,Z;˜x(t),˜y(t),˜z(t)) along the solution curve of System (4.20). Let D+ denote the right-upper derivative. Since p1≥max{β,b}, β>α and 0<˜x(t)<1, (β−α)˜x(t)+bδ<β˜x(t)+p1<β+p1. Direct calculation then yields
D+|X|≤−(v1+v2+2b+2(β−α)˜z(t))|X|+((α−β)˜y(t)−2β˜z(t)+β+p1)|Y|+((β−α)˜x(t)+bδ)|Z|≤−(v1+v2+2b+2(β−α)˜z(t))|X|+((α−β)˜y(t)−2β˜z(t)+β+p1)|Y|+(β+p1)|Z|=−(v1+v2+2b+2(β−α)˜z(t))|X|+((α−β)˜z(t)−2β˜z2(t)˜y(t))˜y(t)˜z(t)|Y|+((β+p1)˜z(t)˜y(t))˜y(t)˜z(t)(|Y|+|Z|),D+|Y|≤v1|X|−(p1+p2+2b+α−bδ+(β−3α)˜z(t))|Y|,D+|Z|≤−(v1+v2+p1+p2+2b+α−bδ+(β−3α)˜z(t))|Z|. | (4.22) |
And
D+˜y(t)˜z(t)(|Y|+|Z|)=˜y′(t)˜z(t)−˜y(t)˜z′(t)˜z2(t)(|Y|+|Z|)+˜y(t)˜z(t)D+(|Y|+|Z|)≤(˜y′(t)˜y(t)−˜z′(t)˜z(t))˜y(t)˜z(t)(|Y|+|Z|)+v1˜y(t)˜z(t)|X|−˜y(t)˜z(t)(p1+p2+2b+α−bδ+(β−3α)˜z(t))|Y|−˜y(t)˜z(t)(v1+v2+p1+p2+2b+α−bδ+(β−3α)˜z(t))|Z|=v1˜y(t)˜z(t)|X|+(˜y′(t)˜y(t)−˜z′(t)˜z(t)−(p2+2b+α−bδ+(β−3α)˜z(t)))˜y(t)˜z(t)(|Y|+|Z|)−p1˜y(t)˜z(t)|Y|−(v1+v2+p1)˜y(t)˜z(t)|Z|. | (4.23) |
In virtue of (4.22) and (4.23), we get
D+V(X,Y,Z;˜x(t),˜y(t),˜z(t))≤max{g1(t),g2(t)}V(X,Y,Z;˜x(t),˜y(t),˜z(t)), | (4.24) |
where
g1(t)=−((v1+v2+2b)+2(β−α)˜z(t))+(α−β)˜z(t)−2β˜z2(t)˜y(t)+(β+p1)˜z(t)˜y(t)=−(v1+v2+2b)−3(β−α)˜z(t)−2β˜z2(t)˜y(t)+(β+p1)˜z(t)˜y(t),g2(t)=v1˜y(t)˜z(t)+˜y′(t)˜y(t)−˜z′(t)˜z(t)−(p2+2b+α−bδ+(β−3α)˜z(t))−(v1+v2+2p1)=v1˜y(t)˜z(t)+˜y′(t)˜y(t)−˜z′(t)˜z(t)−(p1+p2+2b+α−bδ+(β−2α)˜z(t))−(v1+v2+p1−α˜z(t)). | (4.25) |
Notice that (˜x(t),˜y(t),˜z(t)) is the positive solution of system (2.4). Then
˜y′(t)˜y(t)=(α−β)˜z(t)+(β+p1)˜z(t)˜y(t)−(v1+v2+b)−β˜z2(t)˜y(t),˜z′(t)˜z(t)=bδ+v1˜y(t)˜z(t)−(p1+p2+b+α)+α˜z(t). | (4.26) |
ℜ0>1, p1≥β>α and 0<˜z(t)<1, which deduces p1−α˜z(t)>0, and substituting (4.26) into (4.25) yields
g1(t)=˜y′(t)˜y(t)−b−2(β−α)˜z(t)−β˜z2(t)˜y(t)<˜y′(t)˜y(t)−b−(β−α)˜z(t),g2(t)=˜y′(t)˜y(t)−b−(β−α)˜z(t)−(v1+v2+p1−α˜z(t))<˜y′(t)˜y(t)−b−(β−α)˜z(t). | (4.27) |
Meanwhile, since ˜w(t)=1−˜x(t)−˜y(t)−˜z(t),
˜w′(t)˜w(t)=v2˜y(t)˜w(t)+p2˜z(t)˜w(t)−b−(β−α)˜z(t). |
Hence,
max{g1(t),g2(t)}≤˜y′(t)˜y(t)+˜w′(t)˜w(t)−v2˜y(t)˜w(t)−p2˜z(t)˜w(t), |
and
∫ω0max{g1(t),g2(t)}dt≤∫ω0˜y′(t)˜y(t)+˜w′(t)˜w(t)−v2˜y(t)˜w(t)−p2˜z(t)˜w(t)dt≤ln˜y(t)|ω0+ln˜w(t)|ω0−v2∫ω0˜y(t)˜w(t)dt−p2∫ω0˜z(t)˜w(t)dt=−v2∫ω0˜y(t)˜w(t)dt−p2∫ω0˜z(t)˜w(t)dt<0. |
In view of above analysis, we have
V(X,Y,Z;˜x(t),˜y(t),˜z(t))≤V0exp(∫t0max{g1(t),g2(t)}dt), | (4.28) |
and
limt→+∞V(X,Y,Z;˜x(t),˜y(t),˜z(t))=0, | (4.29) |
which indicates that the zero solution of system (4.20) is asymptotically stable. Therefore, the non-constant periodic solution p(t) of system (2.4) is asymptotically stable.
In order to present the proof of Theorem 3 by the result given in [31], we need the following results:
Lemma 4.3. The DFE P0 of system (2.4) is the unique ω-limit point of system (2.4) on the boundary of Ω. If ℜ0>1, P0 cannot be the ω-limit point of any orbit starting in the interior of Ω.
Proof When ℜ0<1, the DFE P0 is the unique disease-free equilibrium of system (2.4). We say that for any t0≥0, the trajectory φ(P,t) (t0≤t<+∞) is the positive half orbit of system (2.4). From Theorem 1, we know that P0 is also a singular point on boundary Ω and Ω={P0}. Thus, the DFE P0 is the unique ω-limit point of System (2.4) on the boundary of Ω. When ℜ0>1, besides the disease-free equilibrium P0, there is a unique disease-endemic equilibrium P∗. Since P0 is unstable when ℜ0>1, P0 can not be the ω-limit point of any orbit starting in the interior of Ω. The proof is complete.
With the aid of Lemmas 4.3, 4.4 and 4.5, we are in the position to complete the proof of Theorem 3.
Proof of Theorem 4.2
When ℜ0>1, system (2.4) admits a unique disease-endemic equilibrium P∗. The asymptotic stability of the disease-endemic equilibrium P∗ has been proved previously. Now we show that the attraction domain of P∗ is the interior of Ω.
Let U be the domain of attraction of P∗ in Ω. From the asymptotic stability of P∗, U is a nonempty open subset in Ω. Otherwise, suppose U is not the interior of Ω. Then the boundary ∂U of U has a nonempty intersection with the interior of Ω. We denote this intersection by Γ. Since both U and ¯U are positive invariant sets of System (2.4), ∂U=¯U−U and Γ are also positive invariant sets of system (2.4). The limit set γ of system (4.22) is contained in Γ. By Lemma 4.3, the limit set of system (2.4) can only be P∗ or periodic solution p(t). Lemma 4.4 tells us that the periodic solution p(t) of system (2.4) is asymptotically stable. Then Γ is bound to attract solutions in its domain, which contradicts that of Γ in ∂U. Therefore, the disease-endemic equilibrium of System (2.4) is globally asymptotically stable. This completes the proof.
Remark 1. From the result in Theorem 3 and its proof, we obtain that system (2.4) is persistent under the condition of ℜ0>1 and p1≥max{β,b} [32].
In this paper, we formulated a susceptible-incubating-infected-treated (SEIT) mathematical model with vertical transmission for the Porcine pseudorabies infection transmission and studied the model dynamics. We defined a threshold, the basic reproduction number, ℜ0, and showed that the DFE P0 is globally asymptotically stable and the disease will die out, regardless its initial sizes, if ℜ0<1. The DFE P0 is unstable and invasion is always possible if ℜ0>1 [18,33]. We also showed that there is only one positive equilibrium P∗ in Ω, which is globally asymptotically stable and the disease is persistent under the conditions ℜ0>1 and p1≥max{β,b}. Furthermore, the basic reproduction number ℜ0 is strictly increasing with respect to the contact rate β. Therefore, isolation of infected pigs and appropriate feeding densities will facilitate the prevention and control of outbreaks of pseudorabies in pigs.
The authors gratefully acknowledge Prof. Jia Li of University of Alabama in Huntsville for his constructive suggestions and useful corrections. The authors also wish to thank the handling editor and the anonymous referees for their valuable comments and suggestions.
The authors declare no conflicts of interest in this paper.
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1. | Yining Chen, Yuhua Long, Jianshe Yu, Global asymptotic stability in a pseudorabies virus model with age structure, 2023, 8, 24680427, 865, 10.1016/j.idm.2023.07.003 | |
2. | Yuhua Long, Yining Chen, Modeling porcine pseudorabies with age structure , 2021, 2021, 1072-6691, 45, 10.58997/ejde.2021.45 |