A review of electrohydrodynamic casting energy conversion polymer composites

1.   Introduction

Though medicine and living conditions have been constantly improving, infectious diseases are still a global concern. Mathematical modeling can not only enhance our understanding of the transmission mechanisms underlying them but also help us assess the efficacy of control strategies. Among the deterministic models described by ordinary differential equations are compartmental models. One of the basic models is the Kermack-McKendric model,

where $S$, $I$, and $R$ are the densities (or numbers) of susceptible, infectious, and recovered individuals, respectively; $\beta$ is the transmission rate while $\gamma$ is the recovery rate. The incidence rate is the bilinear one, $\beta SI$. To better reflect the actual biology of a given disease, the above model has been significantly modified.

In this paper, we consider the factor of relapse. For certain diseases such as herpes, tuberculosis, simplex virus type 2 (a human disease transmitted by close physical or sexual contacts), recovered individuals may experience relapse, which means that they can revert to the infectious class with the reactivation of a latent infection. For example, this feature of recurrence for tuberculosis is often due to incomplete treatment. Tudor ^[1] was the first to study relapse, who built the so-called SIRI model. In this model, the bilinear incidence rate is used. Tudor investigated the existence and local stability of equilibria. Later on, Moreira and Wang ^[2] modified this model with an incidence rate depending on the size of the susceptible population. By means of an elementary analysis of Liénard's equation and Lyapunov's direct method, they established sufficient conditions on the global asymptotic stability of the disease-free and endemic equilibria.

In the above mentioned studies on relapse, the population size is constant. In particular, there are no disease-induced deaths. Thus, in 2013, Vargas-De-León ^[3] proposed two epidemiological models with relapse and disease-induced deaths. One of them is the following one with the bilinear incidence rate,

where $\Lambda$ represents the recruitment rate, $\beta$ is the transmission rate, $\mu$ is the natural death rate, $\alpha$ is the disease-induced death rate, $\gamma$ is the recovery rate, and $\eta$ is the relapse rate. All the parameters are positive. They constructed suitable Lyapunov functions to obtain threshold dynamics determined by the basic reproduction number $R_0$. If $R_0 < 1$, the disease-free equilibrium is globally asymptotically stable and hence the disease dies out. On the other hand, if $R_0 > 1$, the endemic equilibrium is globally asymptotically stable and hence the disease remains endemic. For more works on SIRI models described by ordinary differential equations, we refer to ^[4,5,6] and references therein.

Note that, due to mobility, the distribution of individuals in an area is not even. Modeling this phenomenon often results in reaction-diffusion equations. Consequently, inspired by ^[3], we have formulated a diffusive epidemic model with relapse and bilinear incidence as follows,

Here $S(x, t)$, $I(x, t)$, and $R(x, t)$ are the densities of susceptible, infective, and recovered individuals at time $t$ and position $x\in\Omega$, respectively; $\Omega$ is a bounded domain in $\mathbb{R}^n$ with a smooth boundary $\partial\Omega$; $\Delta$ is the usual Laplacian operator; $\frac{\partial}{\partial n}$ is the outward normal derivative to $\partial\Omega$; $d$ is the diffusion rate which represents the ability of random mobility of individuals; and the meanings of the other parameters are the same as those in (1.1). Note that the Neumann boundary conditions imply that individuals cannot move across the boundary $\partial\Omega$.

It should be pointed out that any solution of (1.2) is always positive for any time $t > 0$ no matter what the nonnegative nontrivial initial condition is. Thus the disease spreads to the whole area immediately, even though the infectious are confined to a quite small part of the habitat at the beginning. This does not agree with the observed fact that diseases always spread gradually. To compensate for the gradual disease spreading progress, a better modeling technique is to introduce free boundary.

The equation governing the free boundary, $h'(t) = -\mu I_{x}(h(t), t)$, is a special case of the well-known Stefan condition, which has been established in ^[7] for diffusive populations and used in the modeling of a number of applied problems. For example, it was used to describe the melting of ice in contact with water ^[8] and to model oxygen in muscles ^[9] as well as wound healing ^[10]. There is a vast literature on Stefan problems. Some important recent theoretical advances can be found in ^[11]. As a typical case, in 2013, Kim et al. ^[12] studied a diffusive SIR epidemic model in a radially symmetric domain with free boundary. They provided sufficient conditions on disease vanishing and spreading.

Motivated by the above discussion, in this paper, we investigate the behavior of nonnegative solutions $(S(x, t), I(x, t), R(x, t);h(t))$ of the following reaction-diffusion SIRI epidemic with free boundary,

where $x = h(t)$ is the moving boundary to be determined, $\mu$ represents the moving rate of the free boundary, $\delta$ is the natural death rate, and the meanings of the rest parameters are the same as those in model (1.2). All parameters are assumed to be positive. The nonnegative initial functions $S_0$, $I_0$ and $R_0$ satisfy

In reality, $I_0(x) = 0$ for $x\in [h_0, +\infty)$ and $I_0\not \equiv 0$ on $[0, h_0)$. Since for $t > 0$, the solution though the initial condition $(S_0, I_0, R_0;h_0)$ with such an $I_0$ satisfy $I(x, t) > 0$ on $[0, h(t))$ and $I(x, t) = 0$ for $x\in [h(t), +\infty)$. Thus, without loss of generality, we make the assumption (1.4). Biologically, model (1.3) means that beyond the free boundary $x = h(t)$, there are only susceptible individuals. We will also consider the case without relapse, that is, $\eta = 0$. In this case, (1.3) reduces to

The remainder of this paper is organized as follows. In Section 2, we prove some general results on the existence and uniqueness of solutions to (1.3)–(1.4). In particular, solutions are global. Then, in Section 3, we provide some sufficient conditions on disease spreading and vanishing. For (1.5), the disease will die out either if the basic reproduction number $\mathcal{R}_0 < 1$ or if $\mathcal{R}_0 > 1$ and the initial infected area, boundary moving rate, and initial value of infected individuals are sufficiently small; while the disease will spread to the whole area if $\mathcal{R}_0 > 1$ and either the initial infected area is suitably large or the diffusion rate is suitably small. For (1.3), when the basic reproduction number $\tilde{\mathcal{R}}_0 \leq 1$, the disease will disappear, whereas when $\tilde{\mathcal{R}}_0 > \mathcal{R}_0 > 1$ and the initial infected area is suitably large, the disease will successfully spread. The paper ends with a brief conclusion and discussion.

2.   Existence and uniqueness of solutions

First, we state the result on the local existence of solutions to (1.3)–(1.4), which can be proved with some modifications of the arguments in ^[10] and ^[13]. Hence we omit the proof to avoid repetition.

Theorem 2.1. For any given $(S_0, I_0, R_0)$ satisfying (1.4) and any $r\in(0, 1)$, there is a $T > 0$ such that problem (1.3) admits a unique bounded solution

moreover,

where $D^\infty _T = \{(x, t)\in \mathbb{R}^2 : x \in [0, +\infty), t\in [0, T]\}$ and $D_T = \{(x, t)\in \mathbb{R}^2 : x \in [0, h(t)], t \in [0, T]\}$. Here $C$ and $T$ only depend on $h_0$, $r$, $\left\|S_0\right\|_{C^2([0, +\infty))}$, $\left\|I_0\right\|_{C^2([0, h_0])}$, and $\left\|R_0\right\|_{C^2([0, h_0])}$.

Next we make some preparations to show the global existence of solutions.

Lemma 2.1. Problem (1.3)–(1.4) admits a unique and uniformly bounded solution $(S, I, R; h)$ on $(0, T_0)$ for some $T_0\in(0, +\infty]$, that is, there exists a constant $M$ independent of $T_0$ such that

Proof. As long as the solution exists, it is easy to see that $S\geq0$, $I\geq0$, and $R\geq0$ on $[0, +\infty)\times[0, T_0]$. By applying the strong maximum principle to the equations on $\{(x, t):x\in [0, h(t)], t\in[0, T_0]\}$, we immediately obtain

It remains to prove the uniform boundedness of the solution $(S(x, t), I(x, t), R(x, t);h(t))$. For this purpose, define

A direct calculation gives

which gives $U(x, t)\leq \max \left\{\|U_0\|_{\infty}, \frac{\Lambda }{\delta}\right\}\triangleq M$, where

Now the required result follows immediately.

Finally, we show that the free boundary of (1.3)–(1.4) is strictly monotonically increasing.

Lemma 2.2. Let $(S, I, R; h)$ be a solution to problem (1.3)–(1.4) defined for $t\in(0, T_0)$ for some $T_0\in(0, +\infty]$. Then there exists a constant $C_1$ independent of $T_0$ such that

Proof. Using the strong maximum principle and Hopf boundary lemma to the equation of $I$, we can obtain $I_x(h(t), t) < 0$ for $t\in(0, T_0)$. This, combined with the Stefan condition $h'(t) = -\mu I_{x}(h(t), t)$, gives $h'(t) > 0$ for $t\in(0, T_0)$.

In order to get a bound for $h'(t)$, we denote

and construct an auxiliary function

We will choose $N$ so that $\omega_N (x, t)\geq I (x, t)$ holds over $\Omega_N$.

Clearly, for $(x, t)\in\Omega_N$,

Therefore, if $N^2\geq\frac{\beta M+\eta}{2d}$ then

On the other hand, we have the boundary condition

To employ the maximum principle to $(\omega_N-I)$ over $\Omega_N$ to deduce that $I(x, t)\leq\omega_N(x, t)$, we only have to find some $N$ independent of $T_0$ such that $I_0(x)\leq\omega_N(x, 0)$ for $x\in[h_0-N^{-1}, h_0]$. It would then follow that

Note that

and

It suffices to have

Thus choosing

completes the proof.

By a similar argument as the one in ^[12,13], we can have the following result.

Theorem 2.2. The solution of problem (1.3)–(1.4) exists and is unique for all $t\in(0, +\infty)$.

3.   The spreading-vanishing dichotomy

This section is devoted to the spreading-vanishing dichotomy. We distinguish two cases, $\eta = 0$ and $\eta > 0$. We start with a sufficient condition on disease vanishing, which will be used in the coming discussion.

3.1.   Disease vanishing

It follows from Lemma 2.2 that if $x = h(t)$ is monotonically increasing, then $h_{\infty}: = \lim\limits_{t\to\infty}h(t)\in (h_0, +\infty]$ is well defined.

Lemma 3.1. If $h_\infty < +\infty$, then $\lim\limits_{t\rightarrow +\infty} \left\| I(\cdot, t)\right\|_{C([0, h(t)])} = 0$. Moreover, $\lim\limits_{t\rightarrow +\infty} \left\| R(\cdot, t)\right\|_{C([0, h(t)])} = 0$ and $\lim\limits_{t\rightarrow +\infty} S(x, t) = \frac{\Lambda}{\delta}$ uniformly in any bounded subset of $[0, +\infty)$.

Proof. Define

Then it is easy to see that

It follows that $v(s, t)$ satisfies

This means that the transformation changes the free boundary $x = h(t)$ into the fixed line $s = h_0$ and hence we have an initial boundary value problem over a fixed area $s < h_0$.

Since $h_0\leq h(t) < h_\infty < +\infty$, the differential operator is uniformly parabolic. With the bounds in Lemma 2.1 and Lemma 2.2, there exist positive constants $M_1$ and $M_2$ such that

Applying the standard $L^p$ theory and the Sobolev embedding theorem ^[14], we obtain that

for some constant $M_3$ depending on $\alpha$, $h_0$, $M_1$, $M_2$, and $\left\| I_0\right\| _{C^2[0, h_0]}$. It follows that there exists a constant $\tilde{C}$ depending on $\alpha$, $h_0$, $(S_0, I_0, R_0)$, and $h_\infty$ such that

Assume $\limsup\limits_{t\rightarrow +\infty} \left\| I(\cdot, t)\right\|_{C([0, h(t)])} = \varpi > 0$ by contradiction. Then there exists a sequence $\{(x_k, t_k)\}$ in $[0, h_{\infty})\times(0, +\infty)$ such that $I(x_k, t_k)\geq\frac{\varpi}{2}$ for all $k\in\mathbb{N}$ and $t_k\rightarrow+\infty$ as $k\rightarrow+\infty$. Since $I(h(t), t) = 0$ and since (3.1) indicates that $\mid I_x(h(t), t)\mid$ is uniformly bounded for $t\in[0, +\infty)$, there exists $\sigma > 0$ such that $x_k\leq h(t_k)-\sigma$ for all $k\geq1$. Then there is a subsequence of $\{x_k\}$ which converges to $x_0\in[0, h_\infty-\sigma]$. Without loss of generality, we assume $x_k\rightarrow x_0$ as $k\rightarrow+\infty$. Correspondingly,

Define $S_k(x, t) = S(x, t_k+t)$, $I_k(x, t) = I(x, t_k+t)$, and $R_k(x, t) = R(x, t_k+t)$ for $(x, t)\in(0, h(t_k+t))\times(-t_k, +\infty)$. It follows from the parabolic regularity that $\{(S_k, I_k, R_k)\}$ has a subsequence $\{(S_{k_{i}}, I_{k_{i}}, R_{k_{i}})\}$ such that $(S_{k_{i}}, I_{k_{i}}, R_{k_{i}})\rightarrow(\tilde S, \tilde I, \tilde R)$ as $i\rightarrow+\infty$. Since $\left\| h \right\|_{C^{1+\frac{\alpha}{2}}([0, +\infty))} \leq \tilde{C}$, $h'(t) > 0$, and $h(t)\leq h_\infty < +\infty$, it is necessary that $h'(t)\rightarrow0$ as $t\rightarrow+\infty$. Hence $(\tilde{S}, \tilde{I}, \tilde{R})$ satisfies

Since $\tilde{I}(x_0, 0)\geq\frac{\varpi}{2}$, the maximum principle implies that $\tilde{I} > 0$ on $[0, h_\infty)\times(-\infty, +\infty)$. Thus we can apply the Hopf lemma to conclude that $\sigma_0: = \frac{\partial \tilde{I}}{\partial s}(h_0, 0) < 0$. It follows that

for all large $i$. Hence $h'(t_{k_i})\geq-\mu\frac{\sigma_0}{2}\frac{h_0}{h_\infty} > 0$ for all large $i$, which contradicts with $h'(t)\rightarrow0$ as $t\rightarrow+\infty$. This proves $\lim\limits_{t\rightarrow +\infty} \left\| I(\cdot, t)\right\|_{C([0, h(t)])} = 0$.

Using a simple comparison argument, we can deduce that $\lim\limits_{t\rightarrow +\infty} \left\| R(\cdot, t)\right\|_{C([0, h(t)])} = 0$ and $\lim\limits_{t\rightarrow +\infty} S(x, t) = \frac{\Lambda}{\delta}$ uniformly in any bounded subset of $[0, +\infty)$. In fact, for any $\varepsilon > 0$, there exists a $T_0\ge 0$ such that $I(x, t)\le \varepsilon$ for $t\ge T_0$. Then, for $t\ge T_0$, we have

and

It follows that

and

As $\varepsilon$ is arbitrarily, letting $\varepsilon\to 0^+$ gives us

and

This immediately gives $\lim\limits_{t\to+\infty}\|R(, \cdot, t)\|_{C([0, h(t)])} = 0$. Moreover, for $t\ge 0$, we have

Then $S(x, t)\leq\bar{S}(t)$ for $x\in(0, +\infty)$ and $t\in(0, +\infty)$, where

is the solution of the problem

Since $\lim\limits_{t\rightarrow +\infty} \bar S(t) = \frac{\Lambda}{\delta}$, we deduce that

Therefore, we have $\lim\limits_{t\to+\infty}S(x, t) = \frac{\Lambda}{\delta}$ uniformly in any bounded subset of $[0, +\infty)$.

3.2.   The case where $\eta=0$

Consider the following eigenvalue problem,

It admits a principal eigenvalue $\lambda_{1}$, where

The basic reproduction number of (1.5) denoted by $\mathcal{R}_{0}$ is given by

With the assistance of the expression of $\mathcal{R}_0$, we can rewrite the expression of $\lambda_1$ as

It follows that $\lambda_1 > 0$ either if $\mathcal{R}_0\le 1$ or if $\mathcal{R}_0 > 1$ and $h_0 < \sqrt{\frac{d\delta \pi^2}{4\beta \Lambda(1-\frac{1}{\mathcal{R}_0})}}$.

We first give some sufficient conditions on disease vanishing.

Theorem 3.2. If $\mathcal{R}_0 < 1$, then $\lim\limits_{t\rightarrow +\infty} \left\| I(\cdot, t)\right\|_{C([0, h(t)])} = 0$ and $\lim\limits_{t\rightarrow +\infty} \left\| R(\cdot, t)\right\|_{C([0, h(t)])} = 0$. Moreover, $\lim\limits_{t\rightarrow +\infty} S(x, t) = \frac{\Lambda}{\delta}$ uniformly in any bounded subset of $[0, +\infty)$.

Proof. From the proof of Lemma 3.1, we have obtained that

Since $\mathcal{R}_0 < 1$, there exists $T_{0}$ such that $S(x, t)\leq\frac{\Lambda}{\delta}\frac{1+\mathcal{R}_0}{2\mathcal{R}_0}$ on $[0, +\infty)\times(T_{0}, +\infty)$. Then $I(x, t)$ satisfies

We know that $I(x, t)\leq\bar{I}(x, t)$ for $(x, t)\in\{(x, t):x\in [0, h(t)], t\in (T_{0}, +\infty)\}$, where $\bar{I}(x, t)$ satisfies

Since $\frac{\beta\Lambda}{\delta}\frac{1+\mathcal{R}_0}{2\mathcal{R}_0}-(\alpha+\gamma+\delta) = \frac{(\alpha+\gamma+\delta)(\mathcal{R}_0-1)}{2} < 0$, we have $\lim\limits_{t\rightarrow +\infty}\|\bar I(\cdot, t)\|_{C[0, h(t)]} = 0$. Then it follows from $I(x, t)\leq\bar{I}(x, t)$ that $\| I(\cdot, t) \|_{C[0, h(t)]}\rightarrow0$ as $t\rightarrow+\infty$. The remaining part follows from Lemma 3.1.

Theorem 3.2. Suppose $\mathcal{R}_0 > 1$. Then $h_{\infty} < +\infty$ for given initial condition $(S_0, I_0, R_0;h_0)$ satisfying $h_0\leq \min\left\{\sqrt{\frac{d}{16k_0}}, \sqrt{\frac{d}{16\gamma}}\right\}$ and $\mu \leq \frac{d}{8K}$, where $k_0 = \beta M-\alpha-\gamma-\delta > 0$, $M = \max\left\{\left\| S_0 \right\|_\infty, \frac{\Lambda}{\delta}\right\}$, and $K = \frac{4}{3}\max \{ \left\| I_0 \right\|_\infty, \left\| R_0 \right\|_\infty \}$.

Proof. Since $\mathcal{R}_0 > 1$, one can easily see that $k_0 > 0$. Inspired by ^[13], we define

where $\theta$ is a constant to be determined later. In the following, we show that $(\bar{S}, \bar{I}, \bar{R}; \bar{h})$ is an upper solution to (1.5).

For $0 < x < \bar{h}(t)$ and $t > 0$, direct computations yield

Moreover,

Choose $\theta = \frac{d}{16h_0^2}$. Noting $\bar h(t)\leq4h_0$, we have

This verifies that $(\bar{S}, \bar{I}, \bar{R}; \bar{h})$ is an upper solution to (1.5). Then we can apply a result similar as [12,Lemma 4.1] (which can be proved in the same manner as [13,Lemma 5.6]) to conclude that $h(t)\leq\bar h(t)$ for $t > 0$. This implies that $h_\infty\leq \lim\limits_{t\rightarrow +\infty}\bar h(t) = 4h_0 < +\infty$.

Theorem 3.3. Assume that $\mathcal{R}_0 > 1$. For given initial condition $(S_0, I_0, R_0;h_0)$, we have $h_\infty < +\infty$ provided that $h_0 < h_*: = \min\Big\{\sqrt{\frac{d\pi^2}{4[\beta N-(\alpha+\gamma+\delta)]}}, \frac{\sqrt{d\gamma}}{4\gamma}\Big\}$ and both $\|I_0\|_{\infty}$ and $\|R_0\|_{\infty}$ are sufficiently small (which is specified in the proof), where $N = \max\{\frac{\Lambda}{\delta}, \|S_0\|_{\infty}\}$.

Proof. Note that $h_*$ is well defined since $\mathcal{R}_0 > 1$. As in the proof of Theorem 3.2, we will construct a suitable upper solution to (1.5). Since $h_0 < h_*$, there exists $\varepsilon_1 > 0$ such that $h_0 < \sqrt{\frac{d\pi^2}{4[\beta(N+\varepsilon_1)-(\alpha+\gamma+\delta)]}}$. Then the principal eigenvalue of the eigenvalue problem

is

and it is has a normalized positive eigenfunction $\tilde{\phi}$ on $(0, h_0)$. Moreover, $\tilde{\phi}_x < 0$ on $(0, h_0]$. Choose $\varepsilon_2\in (0, \gamma)$ such that

Recall that $\limsup\limits_{t\to+\infty}S(t, x)\le \frac{\Lambda}{\delta}$ uniformly for $x\in [0, +\infty)$. Thus there exists a $T_0 > 0$ such that $0 < S(x, t)\leq (N+\varepsilon_1)$ in $[0, +\infty)\times[T_0, +\infty)$. As in ^[15], we define

where $\iota$ is a positive number to be determined later. As $\tilde{\phi}(h_0) = 0$, it follows that $\bar{I}(\vartheta (t), t) = 0$ for $t\ge T_0$, which implies that the function $\bar{I}(x, t)$ is continuous on $[0, +\infty)\times [0, +\infty)$. Similarly, as $V(1) = 0$, we know that $\bar{R}$ is also continuous on $[0, +\infty)\times [0, +\infty)$. Detailed calculations yield $\bar{S}_t-d\bar{S}_{xx} = 0\ge \Lambda-\delta\bar{S}$ and, for $0\leq x\leq\vartheta(t)$,

Here we have used the fact that $\tilde{\phi}_x < 0$ for $x\in (0, h_0]$. It follows that $\bar{I}_{t}-d \bar{I}_{xx}-\beta \bar{S} \bar{I}+(\alpha+\gamma+\delta) \bar{I}\ge 0$. On the other hand, as $h_0 < h_*$, we can obtain

Moreover,

If we choose $0 < \iota\leq-\varepsilon_2^2h_0(1+\frac{\varepsilon_2}{2})/2\mu\tilde{\phi}_x(h_0)$, then

since $\tilde{\phi}_x(h_0) < 0$. Obviously, $\bar{S}(x, 0)\geq\left\| S_0\right\| _\infty$. If $\|I_0\|_{\infty}\le \iota\phi(\frac{x}{1+\frac{\varepsilon_2}{2}})$ and $\|R_0\|_{\infty}\le V(\frac{x}{h_0(1+\frac{\varepsilon_2}{2})})$ for $x\in [0, h_0]$, then $I_0(x)\leq\bar{I}(x, 0)$ and $R_0(x)\leq\bar{R}(x, 0)$ for $x > 0$. This proves that $(\bar{S}, \bar{I}, \bar{R}; \vartheta(t))$ is an upper solution of (1.5). Thus, similalrly as in the proof of Theorem 3.2, we can get $h(t)\leq\vartheta (t)$, which yields $h_\infty < \lim\limits_{t\rightarrow+\infty}\vartheta(t) = h_0(1+\varepsilon_2) < +\infty$. This completes the proof.

We provide a sufficient condition on disease spreading to conclude this subsection.

Theorem 3.4. If $\mathcal{R}_0 > 1$ and $h_0 > h^{*}: = \sqrt{\frac{d\delta\pi^{2}}{4\beta\Lambda(1-\frac{1}{\mathcal{R}_{0}})}}$, then $h_\infty = +\infty$.

Proof. By way of contradiction, we assume that $h_\infty < +\infty$. It follows from Lemma 3.1 that $\lim\limits_{t\rightarrow +\infty} \left\| I(\cdot, t)\right\|_{C([0, h(t)])} = 0$. Moreover, $\lim\limits_{t\rightarrow +\infty} S(x, t) = \frac{\Lambda}{\delta}$ uniformly in any bounded subset of $[0, +\infty)$.

Since $h_0 > h^{*}$ and $\mathcal{R}_0 > 1$, we have $\lambda_1 < 0$, where $\lambda_1$ is the principal eigenvalue of the eigenvalue problem (3.2). Choose $\iota > 0$ such that $\lambda_1+\beta\iota < 0$ and $\mathcal{R}_0 > 1+\frac{\beta \iota}{\alpha+\delta+\gamma}$ (which implies that $\beta(\frac{\Lambda}{\delta}-\iota)-\delta-\alpha-\gamma > 0$). For this $\iota$, there exists $T^* > 0$ such that $S(x, t)\geq\frac{\Lambda}{\delta}-\iota$ and $I(x, t) < 1$ for $x\in [0, h(t)]$ and $t > T^*$. Then $I(x, t)$ satisfies

It is easy to see that $I(x, t)\ge \underline{I}(x, t)$, where $\underline{I}(x, t)$ satisfies

Consider the following eigenvalue problem

whose principal eigenvalue is

Employing Proposition 3.2 and Proposition 3.3 of ^[16], we obtain that $\lim\limits_{t\rightarrow +\infty}\underline{I}(t, x) = \underline{I}(x)$ uniformly in $x\in [0, h_0]$, where $\underline{I}(x) > 0$ satisfies

It follows that $\liminf\limits_{t\rightarrow +\infty} I(x, t)\geq\lim\limits_{t\rightarrow +\infty} \underline{I}(x, t) = \underline{I}(x) > 0$ uniformly in $x\in [0, h_0]$, which contradicts with $\lim\limits_{t\rightarrow +\infty} \left\| I(\cdot, t)\right\|_{C([0, h(t)])} = 0$. Therefore, we have proved $h_{\infty} = +\infty$.

Remark 3.1. Obviously, $h_0 > h^*$ is equivalent to $d < d^*\triangleq \frac{4h_{0}^2\beta \Lambda(1-\frac{1}{\mathcal{R}_{0}})}{\delta\pi^{2}}$. As a result, if $\mathcal{R}_0 > 1$ and $0 < d < d^{*}$, then $h_\infty = +\infty$.

3.3.   The case where $\eta > 0$

In this case, the basic reproduction number $\widetilde{\mathcal{R}}_0$ of problem (1.3) is given by

As in the case where $\eta = 0$, we start with disease vanishing.

Theorem 3.5. If $\widetilde{\mathcal{R}}_0\leq1$, then $\lim\limits_{t\rightarrow +\infty} \left\| I(\cdot, t)\right\|_{C([0, h(t)])} = 0$. Moreover, $\lim\limits_{t\rightarrow +\infty} \left\| R(\cdot, t)\right\|_{C([0, h(t)])} = 0$ and $\lim\limits_{t\rightarrow +\infty} S(x, t) = \frac{\Lambda}{\delta}$ uniformly in any bounded subset of $[0, +\infty)$.

Proof. Consider the following system of ordinary differential equations,

with $(S(0), I(0), R(0)) = (\left\| S_0\right\|_{\infty}, \left\| I_0\right\|_{\infty}, \left\| R_0\right\|_{\infty})$. As in the proof of Theorem 3.2, a result similar as [12, Lemma 4.1] implies that $S(x, t)\leq S(t)$ for $(x, t)\in[0, +\infty)\times(0, +\infty)$, and $I(x, t)\leq I(t)$ and $R(x, t)\leq R(t)$ for $(x, t)\in\{(x, t):x\in [0, h(t)], t\in (0, +\infty)\}$.

Obviously, (3.4) has a disease-free equilibrium $E_{0} = (\frac{\Lambda}{\delta}, 0, 0)$, which is globally asymptotically stable. Indeed, consider $V:\mathbb{R}^{3}_+\rightarrow\mathbb{R}$ defined by

It is clear that $V (S, I, R)$ reaches its global minimum in $\mathbb{R}^{3}_+$ only at $E_0$. Moreover, the derivative of (3.5) with respect to $t$ along solutions of (3.4) is

Using the expression

we obtain

Since $\widetilde{\mathcal{R}}_0\le 1$, we have $\frac{d}{dt}V(S, I, R)\le 0$ for $S > 0$. Moreover, if $\frac{d}{dt}V(S, I, R) = 0$ holds then $S = S^0$. It is easy to verify from this that the disease-free equilibrium $E_0$ is the largest invariant set in the set where $\frac{d}{dt}V(S, I, R) = 0$. Therefore, by LaSalle's invariance principle ^[17], $E_0$ is globally asymptotically stable. This, combined with the above estimates, gives us

which implies that

Then it follows from Lemma 3.1 that $\lim\limits_{t\to+\infty}S(x, t) = \frac{\Lambda}{\delta}$ uniformly in any bounded subset of $[0, +\infty)$ and this completes the proof.

Now we provide a sufficient condition on disease spreading.

Theorem 3.6. If $\widetilde{\mathcal{R}}_0 > \mathcal{R}_0 > 1$ and $h_0 > h^{*}: = \sqrt{\frac{d\delta\pi^{2}}{4\beta\Lambda(1-\frac{1}{\mathcal{R}_{0}})}}$, then $h_\infty = +\infty$.

Proof. We know that $(S(x, t), I(x, t), R(x, t);h(t))$ satisfies

A result similar as [12, Lemma 4.1] for lower solutions gives $S(x, t)\geq\underline{S}(x, t)$ for $0 < x < +\infty$ and $t > 0$; $I(x, t)\geq\underline{I}(x, t)$ and $R(x, t)\geq\underline{R}(x, t)$ for $0 < x < \underline{h}(t)$ and $t > 0$; and $h(t)\geq\underline{h}(t)$ for $t > 0$, where $(\underline{S}(x, t), \underline{I}(x, t), \underline{R}(x, t);\underline{h}(t))$ satisfies

It follows from Theorem 3.4 that if $\widetilde{\mathcal{R}}_0 > \mathcal{R}_0 > 1$ and $h_0 > h^{*}$ then $\underline{h}_\infty = +\infty$, which implies $h_\infty = +\infty$.

4.   Conclusion and discussion

In this paper, we proposed and analyzed a free boundary problem of a reaction-diffusion SIRI model with the bilinear incidence rate. We first obtained the existence and uniqueness of global solutions. Then we established several criteria on disease vanishing and spreading. Roughly speaking, for the case without relapse, the disease will vanish if one of the following three conditions holds. (a) The basic reproduction number $\mathcal{R}_0 < 1$; (b) $\mathcal{R}_0 > 1$ and the initial infected area $h_0$ and the boundary moving rate $\mu$ are small enough; (c) $\mathcal{R}_0 > 1$ together with the initial values $\|I_0\|_{\infty}$, $\|R_0\|_{\infty}$, and $h_0$ being small enough. The disease will spread to the whole area if $\mathcal{R}_0 > 1$ and either $h_0$ is large enough or the diffusion rate $d$ is small enough. For the case with relapse, the disease will die out if the basic reproduction number $\widetilde{\mathcal{R}}_0\le 1$ whereas the disease will spread to the whole area if $\widetilde{\mathcal{R}}_0 > \mathcal{R}_0 > 1$ and $h_0$ is large enough. Unfortunately, we have not considered the case where $\widetilde {R}_0 > 1 > \mathcal{R}_0$. In this case, the disease transmission is complex, which we are working on. Moreover, when the free boundaries can extend to the whole area, we also gave an estimate on the spreading speed.

Compared with the ordinary differential equation model (1.1), the model we studied with free boundary allows more reasonable sufficient conditions on the disease spreading and vanishing. With the main results obtained, we can better understand the phenomenon of relapse. To illustrate this, we demonstrate how the basic reproduction numbers rely on the relapse rate $\eta$. For system (1.3), fix other parameters except $\eta$, we see that $\mathcal{R}^{*}_{0}(\eta) = \widetilde{\mathcal{R}}_0 = \frac{\beta\Lambda(\delta+\eta)}{\delta(\gamma\delta+(\delta+\eta)(\alpha+\delta))}$, which is a strictly increasing function of $\eta$. Thus there exists an $\eta^*\in [0, +\infty)$ such that $\mathcal{R}^*_0(\eta)\ge 1$ when $\eta\geq\eta^*$ and $\mathcal{R}^{*}_{0}(\eta) < 1$ when $\eta < \eta^*$. Then the relapse rate $\eta$ plays an important role in $\mathcal{R}^{*}_{0}(\eta)$. In other words, when $\eta$ varies, disease spreading and vanishing will change. Since $\mathcal{R}^*_0(\eta) > \mathcal{R}_0$ always holds, with relapse the disease will be more easily spread to the whole area than without relapse.

Acknowledgements

The authors would like to thank the two anonymous reviewers for their valuable suggestions and comments, which greatly improve the presentation of the paper. QD, YL, and ZG were supported by the National Natural Science Foundation of China (No. 11771104) and by the Program for Chang Jiang Scholars and Innovative Research Team in University (IRT-16R16). YC was supported partially by NSERC.

Conflict of interest

All authors declare no conflicts of interest in this paper.