<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2018.95036</article-id><article-id pub-id-type="publisher-id">AM-84855</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Global Dynamic Analysis of a Vector-Borne Plant Disease Model with Discontinuous Treatment
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hengmin</surname><given-names>Lv</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Lizhi</surname><given-names>Fei</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhen</surname><given-names>Yuan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fumin</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Key Laboratory of Jiangxi Province for Numerical Simulation and Emulation Techniques, Gannan Normal University, Ganzhou,
China</addr-line></aff><aff id="aff1"><addr-line>Department of Basic Course Education, Ji’an College, Ji’an, China</addr-line></aff><aff id="aff2"><addr-line>College of Mathematics, Sichuan University, Chengdu, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>lvhengmin2005@163.com(HL)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>05</month><year>2018</year></pub-date><volume>09</volume><issue>05</issue><fpage>496</fpage><lpage>511</lpage><history><date date-type="received"><day>2,</day>	<month>May</month>	<year>2018</year></date><date date-type="rev-recd"><day>25,</day>	<month>May</month>	<year>2018</year>	</date><date date-type="accepted"><day>28,</day>	<month>May</month>	<year>2018</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  
    This paper proposes a vector-borne plant disease model with discontinuous treatment strategies. Constructing Lyapunov function and applying non-smooth theory to analyze discontinuous differential equations, the basic reproductive number 
   R
   <sub style="text-align:justify;white-space:normal;">0</sub> is proved, which determines whether the plant disease will be extinct or not. If R
   <sub>0</sub> &lt; 1 , the existence and global stability of disease-free equilibrium is established; If 
   R
   <sub style="text-align:justify;white-space:normal;">0</sub> &gt; 1 , there exists a unique endemic equilibrium which is globally stable. The numerical simulations are provided to verify our theoretical results, which indicate that after infective individuals reach some level, strengthening treatment measures is proved to be beneficial in controlling disease transmission. 
  
 
</p></abstract><kwd-group><kwd>Vector-Borne</kwd><kwd> Plant Disease Model</kwd><kwd> Basic Reproduction Number</kwd><kwd> Discontinuous Treatment</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The plants play an important role in our lives, as most of our daily food, clothing and building materials come from plants. With the change of environment, there are outbreaks of plant diseases, which seriously affect the health of plants and people’s life, such as huanglongbing [<xref ref-type="bibr" rid="scirp.84855-ref1">1</xref>] , Blackleg [<xref ref-type="bibr" rid="scirp.84855-ref2">2</xref>] . We know that plant diseases have been responsible for the death and suffering of millions of people and countless animals [<xref ref-type="bibr" rid="scirp.84855-ref3">3</xref>] . Controlling the outbreak and spread of plant diseases has become the common goal of scientists. Available control measures include biological, cultural, and chemical methods [<xref ref-type="bibr" rid="scirp.84855-ref4">4</xref>] . Chemical control is a quite effective method, but the residues of chemical drugs have a direct negative impact on environment and thus are not encouraged. To effectively control plant disease and to reduce the harm to environment, it is crucial to understand disease transmission dynamics.</p><p>The prevention and control of plant infectious diseases is of vital importance in agricultural production [<xref ref-type="bibr" rid="scirp.84855-ref5">5</xref>] . To work with the plant disease, we first understand how they spread. There are many ways that plant viruses interact with the vectors; this transmission works in the following way. The vectors consume sap from an infected host through their stylet. When the infected vector contacts a healthy plant, some virus particles leave the vector and invade the plant [<xref ref-type="bibr" rid="scirp.84855-ref6">6</xref>] . So the vector-borne is a very important part of the transmission of plant diseases.</p><p>Treatment plays a very important role to control the spread of diseases. In recent years, many researchers [<xref ref-type="bibr" rid="scirp.84855-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.84855-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.84855-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.84855-ref10">10</xref>] have studied some mathematical models incorporating treatment. For example, in [<xref ref-type="bibr" rid="scirp.84855-ref11">11</xref>] , Wang and Ruan studied an epidemic model, and provide the limited resources for the treatment of patients. In [<xref ref-type="bibr" rid="scirp.84855-ref12">12</xref>] , Wang proposed constant treatment, which simulates a limited capacity for treatment. In practice, when the number of infectives is large, the constant treatment is suitable for hypothesis of model. Recently, discontinuous treatment strategies are proposed by [<xref ref-type="bibr" rid="scirp.84855-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.84855-ref14">14</xref>] . The results show that discontinuous treatment strategies would be accord with real condition. Applying this discontinuous treatment strategy makes the mathematical model a discontinuous system. At the same time, some non-smooth analysis techniques [<xref ref-type="bibr" rid="scirp.84855-ref15">15</xref>] are used for this system.</p><p>In [<xref ref-type="bibr" rid="scirp.84855-ref16">16</xref>] , Shi and Zhao presented a vector-borne plant disease model, but they do not studied treatment to the infected plant host. Treating infected plant is a quite effective method which to control the outbreak of the plant disease. Although continuous treatment is an effective method, the outbreak of the plant disease is periodic, and continuing treatment can be a huge waste of resources. In order to be realistic, we built a vector-borne plant disease model with discontinuous treatment.</p><p>The paper is organized as follows. In the next section, we will construct the model and introduce the rational assumptions for model. In Section 3, positivity of the solution for the model will be clearly discussed. We obtain the existence of possible equilibria, the basic reproductive number, and the stability of equilibria in Section 4. In Section 5 and Section 6, we summarize our main results and main results are numerically simulated.</p></sec><sec id="s2"><title>2. Model and Preliminaries</title><p>To construct the model, the following assumptions are being made by Shi et al. in [<xref ref-type="bibr" rid="scirp.84855-ref16">16</xref>] .</p><p>(A1) The total of the insect vector population is divided into X and Y, which denotes the densities of the susceptible vector and infective vector at time t, respectively. The total of the plant host population is divided into S, I, and R, which represents the numbers of the susceptible, infective, and recovered host plant population at time t, respectively. At the same time, we assume that the number of plants in one area is fixed. The total number of plants K = S + I + R is a positive constant. In fact, when a plant has died, it would be replaced by a new plant to keep the total number of plants. Further, we assume that those new plants are susceptible, i.e., we chose the birth rate of susceptible plant host as f ( S , I ) = μ K + d I .</p><p>(A2) The susceptible plants can be infected not only by the infected insect vectors but also by the infected plants.</p><p>(A3) A susceptible vector can be infected only by an infected plant host, and after it is infected, it will hold the virus for the rest of its life. Further, there is no vertical infection being considered.</p><p>(A4) The replenishment rate of insect vectors is a positive constant, and all of the new born vectors are susceptible.</p><p>According to the principle of the compartmental model, consider the following model with discontinuous treatment:</p><p>{ S ˙ = f ( S , I ) − μ S − ( β P Y + β s I ) S , I ˙ = ( β P Y + β s I ) S − ( d + μ + γ ) I − h ( I ) , R ˙ = γ I + h ( I ) − μ R , X ˙ = Λ − β 1 I X − m X , Y ˙ = β 1 I X − m Y . (2.1)</p><p>Here the dimensionless variables and parameters (with parameter values) are given in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The function h ( I ) = φ ( I ) I represents the treatment rate. φ ( I ) satisfies the following assumptions. Obviously, the treatment rate should be nondecreasing as the number of infectious individuals is increasing. The following assumption will be needed throughout the paper.</p><p>(H<sub>1</sub>) φ : [ 0, ∞ ) → [ 0, ∞ ) is nondecreasing and has at most a finite number of jump discontinuities in every compact interval. No loss of generality, we always assume that φ is continuous at I = 0 , otherwise we define φ ( 0 ) to be φ ( 0 + ) . Here φ ( 0 + ) denotes the right limit of φ ( I ) as I → 0 + .</p><p>By adding the fourth and fifth equations of system (2.1), we get</p><p>N ˙ = Λ − m N (2.2)</p><p>where N = X + Y . From Equation (2.2), we easily get N → Λ m as t → ∞ .</p><p>Note that S + I + R = K . Since the variable R and X does not appear in the first two equations of model (2.1), meanwhile, let’s substitute X for ( Λ m − Y ) in</p><p>the fifth equation. We only need to study the first two equations and the fifth</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Dimensionless variables and parameters (with illustrative parameter values) in system (2.1)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameter</th><th align="center" valign="middle" >Description</th><th align="center" valign="middle" >Default value</th></tr></thead><tr><td align="center" valign="middle" >S</td><td align="center" valign="middle" >number of the susceptible plant hosts</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >I</td><td align="center" valign="middle" >number of the infected plant hosts</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >R</td><td align="center" valign="middle" >number of the recovered plant hosts</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >K</td><td align="center" valign="middle" >sum of the total plant hosts</td><td align="center" valign="middle" >50 - 1000</td></tr><tr><td align="center" valign="middle" >X</td><td align="center" valign="middle" >density of the susceptible insect vectors</td><td align="center" valign="middle" >..</td></tr><tr><td align="center" valign="middle" >Y</td><td align="center" valign="middle" >density of the infected insect vectors</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >N</td><td align="center" valign="middle" >sum of the total insect vectors density</td><td align="center" valign="middle" >50 - 100</td></tr><tr><td align="center" valign="middle" >β<sub>1</sub></td><td align="center" valign="middle" >infection ratio between infected hosts and susceptible vectors</td><td align="center" valign="middle" >0.01 - 0.02</td></tr><tr><td align="center" valign="middle" >β<sub>P</sub></td><td align="center" valign="middle" >biting rate of an infected vector on the susceptible host plants</td><td align="center" valign="middle" >0.01 - 0.02</td></tr><tr><td align="center" valign="middle" >β<sub>S</sub></td><td align="center" valign="middle" >infection incidence between infected and susceptible hosts</td><td align="center" valign="middle" >0.01 - 0.02</td></tr><tr><td align="center" valign="middle" >γ</td><td align="center" valign="middle" >the conversion rate of infected hosts to recovered hosts</td><td align="center" valign="middle" >0 - 0.4</td></tr><tr><td align="center" valign="middle" >μ</td><td align="center" valign="middle" >natural death rate of plant hosts</td><td align="center" valign="middle" >0 - 0.1</td></tr><tr><td align="center" valign="middle" >Λ</td><td align="center" valign="middle" >birth or immigration of insect vectors</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >m</td><td align="center" valign="middle" >natural death rate of insect vectors</td><td align="center" valign="middle" >0 - 0.5</td></tr><tr><td align="center" valign="middle" >d</td><td align="center" valign="middle" >disease-induced mortality of infected hosts</td><td align="center" valign="middle" >0.1</td></tr></tbody></table></table-wrap><p>equation of model (2.1), thereby lowering the order of the system to be studied, i.e.</p><p>{ S ˙ = μ ( K − S ) − ( β P Y + β s I ) S + d I , I ˙ = ( β P Y + β s I ) S − ω I − h ( I ) , Y ˙ = Λ β 1 I m − ( β 1 I + m ) Y . (2.3)</p><p>where ω = d + μ + γ . Obviously,</p><p>Ω = { ( S , I , Y ) ∈ R + 3 : 0 ≤ S + I ≤ K ,0 ≤ Y ≤ Λ m } (2.4)</p><p>is the positively invariant set for system (2.3).</p><p>According to the definition of solutions for differential equations with discontinuous right-hand sides in [<xref ref-type="bibr" rid="scirp.84855-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.84855-ref17">17</xref>] , ( S ( t ) , I ( t ) , Y ( t ) ) is called a solution with initial condition</p><p>( S ( 0 ) , I ( 0 ) , Y ( 0 ) ) = ( S 0 , I 0 , Y 0 ) ,   S 0 , I 0 , Y 0 ≥ 0 (2.5)</p><p>of model (2.3) on [ 0 , T ) , 0 &lt; T ≤ ∞ , if it is absolutely continuous on any compact subinterval of [ 0, T ) , and almost everywhere on [ 0, T ) (abbreviated to a.e. on [ 0, T ) ) satisfies the following differential inclusion:</p><p>{ S ˙ = μ ( K − S ) − ( β P Y + β s I ) S + d I , I ˙ ∈ ( β P Y + β s I ) S − ω I − c o &#175; [ h ( I ) ] , Y ˙ = Λ β 1 I m − ( β 1 I + m ) Y . (2.6)</p><p>where c o &#175; [ h ( I ) ] = [ h ( I − 0 ) , h ( I + 0 ) ] . Here, h ( I − 0 ) and h ( I + 0 ) denote the left limit and the right limit of the function h ( I ) at I, respectively.</p><p>From (H<sub>1</sub>), it is clear that the set map</p><p>( S , I , Y ) ↦ ( μ ( K − S ) − ( β P Y + β s I ) S + d I , ( β P Y + β s I ) S − ω I − c o &#175; [ h ( I ) ] , Λ β 1 I m − ( β 1 I + m ) Y ) (2.7)</p><p>is an upper semi-continuous set-valued map with non-empty compact convex values. By the measurable selection theorem [<xref ref-type="bibr" rid="scirp.84855-ref15">15</xref>] , if ( S ( t ) , I ( t ) , Y ( t ) ) is a solution of model (2.3) on [ 0, T ) , then there is a measurable function m ( t ) ∈ c o &#175; [ h ( I ( t ) ) ] such that</p><p>{ S ˙ = μ ( K − S ) − ( β P Y + β s I ) S + d I , I ˙ ∈ ( β P Y + β s I ) S − ω I − m ( t ) ,   a . e .   on   [ 0 , T ) . Y ˙ = Λ β 1 I m − ( β 1 I + m ) Y . (2.8)</p></sec><sec id="s3"><title>3. Positivity</title><p>In this section, we will prove the positive of the solution to the initial condition of the model (2.3) with positive initial value. First, we will prove the following theorem.</p><p>Theorem 3.1. Suppose that assumption (H<sub>1</sub>) holds and let ( S ( t ) , I ( t ) , Y ( t ) ) be the solution with initial condition (2.5) of model (2.3) on [ 0, T ) . Then ( S ( t ) , I ( t ) , Y ( t ) ) is nonnegative on [ 0, T ) .</p><p>Proof: By the definition of a solution of (2.3) in the sense of Filippov, ( S ( t ) , I ( t ) , Y ( t ) ) must be a solution to differential inclusion (2.6). From the first equation of (2.6), we have</p><p>[ S 0 + ∫ 0 t ( μ k + d I ( u ) ) exp ( ∫ 0 u ( μ + β P Y ( ρ ) + β s I ( ρ ) ) d ρ ) d u ]   ⋅ exp ( − ( ∫ 0 t ( μ + β P Y ( ρ ) + β s I ( ρ ) ) d ρ ) ) &gt; 0 (3.1)</p><p>for all t ∈ ( 0, T ) .</p><p>Based on the previous hypothesis of (H<sub>1</sub>), we have c o &#175; [ h ( 0 ) ] = 0 and h ( I ) is continuous at I = 0 . Combining the continuity of φ at I = 0 , it may be concluded that there exists a positive constant δ such that φ ( I ) is continuous as | I | &lt; δ . On this account, when | I | &lt; δ the differential inclusion (2.6) becomes the following system of differential equations:</p><p>{ I ˙ = ( β P Y + β s I ) S − ( ω + φ ( I ) ) I , Y ˙ = Λ β 1 I m − ( β 1 I + m ) Y . (3.2)</p><p>We divide this into four cases to discuss the positivity of the solutions for (2.6).</p><p>1) I 0 = Y 0 = 0 .</p><p>From (3.2), we see that I ( t ) = Y ( t ) = 0 for all t ∈ [ 0, T ) .</p><p>2) I 0 &gt; 0 , Y 0 = 0 .</p><p>By the continuity of I ( t ) at t = 0 and d Y d t | t = 0 = Λ β 1 I 0 m &gt; 0 , we conclude I ( t ) &gt; 0 and Y ( t ) &gt; 0 for all t ∈ ( 0, T ) . If it is not true, then we can set</p><p>t 1 = inf { t : I ( t ) = 0   or   Y ( t ) = 0 } ∈ ( 0 , T ) . (3.3)</p><p>If I ( t 1 ) = 0 , then from d I d t ≥ − ( ω + φ ( I ) ) I for 0 ≤ t ≤ t 1 , we have I ( t 1 ) ≥ I 0 exp ( − ( ω + φ ( I ) ) t 1 ) &gt; 0 . This is a contradiction.</p><p>If I ( t 1 ) = 0 , then there is a θ such that t 1 − θ &gt; 0 and 0 &lt; I ( t ) &lt; δ on [ t − θ , t 1 ) . Therefore, the second equation of (3.2) implies</p><p>d Y d t ≥ − ( β 1 I + m ) Y (3.4)</p><p>We have</p><p>Y ( t 1 ) ≥ Y ( t 1 − θ ) exp ( − ∫ t 1 − θ t 1 ( β 1 I ( ξ ) + m ) d ξ ) &gt; 0 (3.5)</p><p>This is also a contradiction. Hence, I ( t ) and Y ( t ) are positive for all t ∈ ( 0, T ) . The same conclusion can be reached for the following two cases.</p><p>3) I 0 = 0 , Y 0 &gt; 0 .</p><p>4) I 0 &gt; 0 , Y 0 &gt; 0 . This completes the proof.</p></sec><sec id="s4"><title>4. The Equilibria and Their Stability</title><p>In this section, we will discuss the existence of equilibria of system (2.3). First, we prove the existence of endemic equilibrium.</p><p>Let ( S ( t ) , I ( t ) , Y ( t ) ) = ( S * , I * , Y * ) is a constant solution of (2.3), where ( S * , I * , Y * ) satisfies the following system:</p><p>{ 0 = μ ( K − S * ) − ( β P Y * + β s I * ) S * + d I * , 0 ∈ ( β P Y * + β s I * ) S * − ω I * − c o &#175; [ h ( I * ) ] , 0 = β 1 I * Λ m − ( β 1 I * + m ) Y * . (4.1)</p><p>Since h ( 0 ) = 0 , there always exists a disease-free equilibrium P 0 of the model (2.3), where P 0 = ( K , 0 , 0 ) . Next, we consider that the existence of an endemic equilibrium of the model (2.3).</p><p>It follows from the first and third equations of (4.1), we conclude that</p><p>S * = d I * + μ K μ + β P Y * + β s I * ,     Y * = Λ β 1 I * m ( β 1 I * + m ) . (4.2)</p><p>Substituting (4.2) into the second inclusion of (4.1), we have the follows</p><p>A 1 I * 2 + B 1 I * + C 1 A 2 I * 2 + B 2 I * + C 2 − ω ∈ c o &#175; [ φ ( I ) ] = [ φ ( I * − 0 ) , φ ( I * + 0 ) ] (4.3)</p><p>where</p><p>A 1 = m d β 1 β s</p><p>B 1 = d Λ β p β 1 + m 2 d β s + μ m K β 1 β s ,</p><p>C 1 = μ K ( Λ β p β 1 + m 2 β s ) ,</p><p>A 2 = m β 1 β s ,</p><p>B 2 = μ m β 1 + Λ β 1 β p + m 2 β s ,</p><p>C 2 = μ m 2 .</p><p>Denote</p><p>g ( I * ) = A 1 I * 2 + B 1 I * + C 1 A 2 I * 2 + B 2 I * + C 2 − ω (4.4)</p><p>and let</p><p>R 0 = K ( Λ β p β 1 + β s m 2 ) m 2 ( ω + φ ( 0 ) ) (4.5)</p><p>We next claim that R 0 is the basic reproductive number for the model (2.3) which will determine the existence of an endemic equilibrium.</p><p>Theorem 4.1. Suppose that assumption (H1) holds. If R 0 ≤ 1 , then there only exists a disease-free equilibrium P 0 ( K ,0,0 ) . If R 0 &gt; 1 , then there exists a unique positive endemic equilibrium P * ( S * , E * , I * ) except P 0 .</p><p>Proof: By R 0 ≤ 1 , we get g ( 0 ) ≤ φ ( 0 ) . Since g ( I ) is nonincreasing on I and φ ( I ) is nondecreasing on I. For this reason, the inclusion (4.3) is only valid at I = 0 . Hence, the model (2.3) has a unique disease-free equilibrium as long as R 0 ≤ 1 .</p><p>From (4.4), we have the following</p><p>A I 2 + B I + C = 0 (4.6)</p><p>where</p><p>A = m β 1 β s ( m d − ω ) &lt; 0 ,</p><p>B = Λ d β 1 β p + m 2 d β s + μ m K β 1 β s − ω m μ β 1 − Λ ω β 1 β p − ω m 2 β s ,</p><p>C = μ ω m 2 ( R 0 − 1 ) + μ m 2 φ ( 0 ) .</p><p>If R 0 ≥ 1 , then C &gt; 0 , and the Equation (4.6) has a unique positive root I, where</p><p>I = − B + Δ 1 2 2 A ,   Δ = B 2 − 4 A C . (4.7)</p><p>If R 0 &gt; 1 , then<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x123.png" xlink:type="simple"/></inline-formula>. Meanwhile, the inequality<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x124.png" xlink:type="simple"/></inline-formula>, it implies<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x125.png" xlink:type="simple"/></inline-formula>. Therefore, the set</p><disp-formula id="scirp.84855-formula77"><label>(4.8)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x126.png"  xlink:type="simple"/></disp-formula><p>is bounded and non-empty. We can write</p><disp-formula id="scirp.84855-formula78"><graphic  xlink:href="//html.scirp.org/file/3-7403933x127.png"  xlink:type="simple"/></disp-formula><p>It follows easily that</p><disp-formula id="scirp.84855-formula79"><label>(4.9)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x128.png"  xlink:type="simple"/></disp-formula><p>We claim<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x129.png" xlink:type="simple"/></inline-formula>. Assumption, contrary to our claim, that</p><disp-formula id="scirp.84855-formula80"><graphic  xlink:href="//html.scirp.org/file/3-7403933x130.png"  xlink:type="simple"/></disp-formula><p>From (H<sub>1</sub>), there exists a <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x131.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.84855-formula81"><label>(4.10)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x132.png"  xlink:type="simple"/></disp-formula><p>This contradicts the definition of<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x133.png" xlink:type="simple"/></inline-formula>. Thus, we have <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x134.png" xlink:type="simple"/></inline-formula>. That is to say, <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x135.png" xlink:type="simple"/></inline-formula>is a positive solution of the inclusion (4.3). We proceed to show that <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x136.png" xlink:type="simple"/></inline-formula> is the only one positive solution of the inclusion (4.3). If the inclusion (4.3) has another positive solution<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-7403933x137.png" xlink:type="simple"/></inline-formula>, then there must exist two numbers</p><disp-formula id="scirp.84855-formula82"><label>(4.11)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x138.png"  xlink:type="simple"/></disp-formula><p>which satisfy</p><disp-formula id="scirp.84855-formula83"><label>(4.12)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x139.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.84855-formula84"><label>(4.13)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x140.png"  xlink:type="simple"/></disp-formula><p>Subtracting (4.13) from (4.12) gives</p><disp-formula id="scirp.84855-formula85"><label>(4.14)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x141.png"  xlink:type="simple"/></disp-formula><p>which implies</p><disp-formula id="scirp.84855-formula86"><label>(4.15)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x142.png"  xlink:type="simple"/></disp-formula><p>This is a contradiction. Hence, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x143.png" xlink:type="simple"/></inline-formula>is the unique positive solution of the inclusion (4.3). Combining it with (4.2), we conclude that the <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x144.png" xlink:type="simple"/></inline-formula> is the unique endemic equilibrium of (2.3). The proof is completed.</p><p>Next, we prove the global stability of the disease-free equilibrium and the endemic equilibrium. We do this in several steps. We first investigate the local properties of the equilibria of system (2.3).</p><p>Theorem 4.2. Assume (H<sub>1</sub>) holds. The disease-free equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x145.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable if<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x146.png" xlink:type="simple"/></inline-formula>, and is unstable if<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x147.png" xlink:type="simple"/></inline-formula>.</p><p>Proof: We analyze the stability of the disease-free equilibrium by investigating the eigenvalues of the Jacobian matrix of model (2.3) at<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x148.png" xlink:type="simple"/></inline-formula>. The matrix is</p><disp-formula id="scirp.84855-formula87"><label>(4.16)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x149.png"  xlink:type="simple"/></disp-formula><p>Thus, the characteristic equation at the disease-free equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x150.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.84855-formula88"><label>(4.17)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x151.png"  xlink:type="simple"/></disp-formula><p>It is easy to see that one of the roots with respect to <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x152.png" xlink:type="simple"/></inline-formula> of (4.14) is<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x153.png" xlink:type="simple"/></inline-formula>. the other two roots are determined by the following characteristic equation of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x154.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.84855-formula89"><label>(4.18)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x155.png"  xlink:type="simple"/></disp-formula><p>From (4.18) and Routh-Hurwitz criteria [<xref ref-type="bibr" rid="scirp.84855-ref18">18</xref>] , it is easily seen that both the real parts of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula> and of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x157.png" xlink:type="simple"/></inline-formula> are negative when<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x158.png" xlink:type="simple"/></inline-formula>. When<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x159.png" xlink:type="simple"/></inline-formula>, one of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x160.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x161.png" xlink:type="simple"/></inline-formula> is a number with a positive real part. Thus the disease-free equilibrium is locally asymptotically stable if <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x162.png" xlink:type="simple"/></inline-formula> and unstable if<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x163.png" xlink:type="simple"/></inline-formula>.,</p><p>We have shown that there exists a positive endemic equilibrium if and only if <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x164.png" xlink:type="simple"/></inline-formula> in Theorem 4.1. Here, we will establish its local stability.</p><p>Theorem 4.3. Suppose that assumption (H1) holds. If<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x165.png" xlink:type="simple"/></inline-formula>, the endemic equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x166.png" xlink:type="simple"/></inline-formula> of the system (2.3) is locally asymptotically stable.</p><p>Proof: The Jacobian matrix of (2.3) at the endemic equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x167.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.84855-formula90"><label>(4.19)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x168.png"  xlink:type="simple"/></disp-formula><p>Replacing<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x169.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x170.png" xlink:type="simple"/></inline-formula>by<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x171.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x172.png" xlink:type="simple"/></inline-formula>, respectively. So we have</p><disp-formula id="scirp.84855-formula91"><label>(4.20)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x173.png"  xlink:type="simple"/></disp-formula><p>The characteristic equation of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x174.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.84855-formula92"><label>(4.21)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x175.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.84855-formula93"><graphic  xlink:href="//html.scirp.org/file/3-7403933x176.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84855-formula94"><graphic  xlink:href="//html.scirp.org/file/3-7403933x177.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84855-formula95"><graphic  xlink:href="//html.scirp.org/file/3-7403933x178.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x179.png" xlink:type="simple"/></inline-formula> is nondecreasing,<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x180.png" xlink:type="simple"/></inline-formula>. This implies<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x181.png" xlink:type="simple"/></inline-formula>.</p><p>Then</p><disp-formula id="scirp.84855-formula96"><graphic  xlink:href="//html.scirp.org/file/3-7403933x182.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84855-formula97"><graphic  xlink:href="//html.scirp.org/file/3-7403933x183.png"  xlink:type="simple"/></disp-formula><p>Hence, all of the Routh-Hurwitz criteria are satisfied. Thus it follows that the endemic equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x184.png" xlink:type="simple"/></inline-formula> of (2.3), which exists if<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x185.png" xlink:type="simple"/></inline-formula>, is always locally asymptotically stable. The proof is completed.,</p><p>Next, we will prove global stability of the disease-free equilibrium and endemic equilibrium of (2.3). We need to use the LaSalle-type invariance principle for the differential inclusion (Theorem 3 in [<xref ref-type="bibr" rid="scirp.84855-ref19">19</xref>] ) to prove their global stability.</p><p>Let<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x186.png" xlink:type="simple"/></inline-formula>. We obtain the following system analogous to (2.5)</p><disp-formula id="scirp.84855-formula98"><label>(4.22)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x187.png"  xlink:type="simple"/></disp-formula><p>Set</p><disp-formula id="scirp.84855-formula99"><label>(4.23)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x188.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.84855-formula100"><graphic  xlink:href="//html.scirp.org/file/3-7403933x189.png"  xlink:type="simple"/></disp-formula><p>For any<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x190.png" xlink:type="simple"/></inline-formula>, there exists an <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x191.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.84855-formula101"><label>(4.24)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x192.png"  xlink:type="simple"/></disp-formula><p>Hence,</p><disp-formula id="scirp.84855-formula102"><label>(4.25)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x193.png"  xlink:type="simple"/></disp-formula><p>When<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x194.png" xlink:type="simple"/></inline-formula>, the nondecreasing of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x195.png" xlink:type="simple"/></inline-formula> implies</p><disp-formula id="scirp.84855-formula103"><label>(4.26)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x196.png"  xlink:type="simple"/></disp-formula><p>It shows that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x197.png" xlink:type="simple"/></inline-formula> is a Lyapunov function of (4.23).</p><p>Furthermore, when<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x198.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.84855-formula104"><label>(4.27)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x199.png"  xlink:type="simple"/></disp-formula><p>When<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x200.png" xlink:type="simple"/></inline-formula>, we have<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x201.png" xlink:type="simple"/></inline-formula>, which implies<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x202.png" xlink:type="simple"/></inline-formula>. For any<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x203.png" xlink:type="simple"/></inline-formula>, we set</p><disp-formula id="scirp.84855-formula105"><label>(4.28)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x204.png"  xlink:type="simple"/></disp-formula><p>Hence, the largest weakly invariant subset of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x205.png" xlink:type="simple"/></inline-formula> is the singleton<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x206.png" xlink:type="simple"/></inline-formula>.</p><p>When<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x207.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.84855-formula106"><label>(4.29)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x208.png"  xlink:type="simple"/></disp-formula><p>From the first equation of (4.23) and x = 0, it may be concluded that<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x209.png" xlink:type="simple"/></inline-formula>. Therefore, we see that the largest weakly invariant subset of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x210.png" xlink:type="simple"/></inline-formula> is also the singleton<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x211.png" xlink:type="simple"/></inline-formula>. By the LaSalle-type invariance principle, the equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x212.png" xlink:type="simple"/></inline-formula> of (4.23) is globally asymptotically stable as<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x213.png" xlink:type="simple"/></inline-formula>. Summarizing the above analysis, we obtain the following theorem.</p><p>Next, we demonstrate the global stability of the endemic equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x214.png" xlink:type="simple"/></inline-formula> of (2.3). So, we have the following theorem.</p><p>Theorem 4.4. Suppose that assumption (H1) holds. If<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x215.png" xlink:type="simple"/></inline-formula>, the disease-free equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x216.png" xlink:type="simple"/></inline-formula> of the system (2.3) is globally asymptotically stable.</p><p>Proof: Let</p><disp-formula id="scirp.84855-formula107"><label>(4.30)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x217.png"  xlink:type="simple"/></disp-formula><p>Write</p><disp-formula id="scirp.84855-formula108"><graphic  xlink:href="//html.scirp.org/file/3-7403933x218.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.84855-formula109"><label>(4.31)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x219.png"  xlink:type="simple"/></disp-formula><p>For any<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x220.png" xlink:type="simple"/></inline-formula>, there exists an <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x221.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.84855-formula110"><label>(4.32)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x222.png"  xlink:type="simple"/></disp-formula><p>Hence</p><disp-formula id="scirp.84855-formula111"><label>(4.33)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x223.png"  xlink:type="simple"/></disp-formula><p>The monotonicity of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x224.png" xlink:type="simple"/></inline-formula> implies<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x225.png" xlink:type="simple"/></inline-formula>. Thus<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x226.png" xlink:type="simple"/></inline-formula>. This shows that V is a Lyapunov function of (2.24). Define</p><disp-formula id="scirp.84855-formula112"><label>(4.34)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x227.png"  xlink:type="simple"/></disp-formula><p>If<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x228.png" xlink:type="simple"/></inline-formula>, then the first equation of (2.6) implies<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x229.png" xlink:type="simple"/></inline-formula>. Consequently, for any<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x230.png" xlink:type="simple"/></inline-formula>, the largest weakly invariant subset of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x231.png" xlink:type="simple"/></inline-formula> of (2.6) is the singleton overline<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x232.png" xlink:type="simple"/></inline-formula>. Here</p><disp-formula id="scirp.84855-formula113"><graphic  xlink:href="//html.scirp.org/file/3-7403933x233.png"  xlink:type="simple"/></disp-formula><p>Therefore, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x234.png" xlink:type="simple"/></inline-formula>is globally asymptotically stable if<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x235.png" xlink:type="simple"/></inline-formula>. This completes the proof.,</p></sec><sec id="s5"><title>5. Numerical Simulation</title><p>To make our analysis more intuitive, some numerical simulations of solutions of the model (2.6) is provided which to illustrate the influence of insect vector and discontinuous treatment on the spread of plant disease. We apparent a treatment function satisfying (H<sub>1</sub>) as follows:</p><disp-formula id="scirp.84855-formula114"><label>(5.1)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/3-7403933x236.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x237.png" xlink:type="simple"/></inline-formula>. The treatment function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x238.png" xlink:type="simple"/></inline-formula> is applied at the following case: when the infective individuals I attain some threshold<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x239.png" xlink:type="simple"/></inline-formula>, the treatment rate should be strengthened to control the spread of the plant disease.</p><p>To better illustrate the effects of non-continuous healing on the spread of plant disease, the following parameters are derived from [<xref ref-type="bibr" rid="scirp.84855-ref16">16</xref>] . Let<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x246.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x246.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x247.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x246.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x248.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x246.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x249.png" xlink:type="simple"/></inline-formula>, then we easily calculate <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x246.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x250.png" xlink:type="simple"/></inline-formula> by using (4.5). <xref ref-type="fig" rid="fig1">Figure 1</xref> shows that the infective individuals I and the infective insect vectors Y tend to 0, and it means that the disease goes to extinction. In addition, we find that the peak values of the infective is affected by the different values of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x246.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x251.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows that larger values of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x243.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x244.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x246.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x250.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x251.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x252.png" xlink:type="simple"/></inline-formula> can reduce the peak values of the infective. Therefore, we can increase the treatment rate to prevent the spread of disease after the number infective individuals reaching some high level. From <xref ref-type="fig" rid="fig1">Figure 1</xref>, the infective individuals reach some level and strengthening the treatment rate is also effective for disease control, even though we do not take any treatment measures at the initial time of the diseases outbreak.</p><p>If we fixed all parameter values as follows:<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x259.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x260.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x261.png" xlink:type="simple"/></inline-formula>one could easily see that<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x261.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x262.png" xlink:type="simple"/></inline-formula>, by using (4.5). <xref ref-type="fig" rid="fig2">Figure 2</xref> shows that the endemic equilibrium is globally asymptotically stable. By (4.5), it’s obvious find that the basic reproductive number <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x261.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x263.png" xlink:type="simple"/></inline-formula> is independent of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x261.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x264.png" xlink:type="simple"/></inline-formula>, and the different values of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x254.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x261.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x263.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x265.png" xlink:type="simple"/></inline-formula> can affect the stability level of the infective. That is to say, larger values of</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x279.png" xlink:type="simple"/></inline-formula>can impact level of the infective. It implies that the strengthening of the treatment rate can effectively control the spread of plant disease after the number of infective individuals has increased to some high level.</p></sec><sec id="s6"><title>6. Discussion</title><p>As for the plant infectious disease model, our main object is to investigate the effect of the insect vector and discontinuous treatment function on the dynamics of spreading the plant disease. We calculated the basic reproduction number<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x280.png" xlink:type="simple"/></inline-formula>, which is derived under some reasonable assumptions on the discontinuous treatment function. It is an important threshold parameter which plays an important role in determining the global dynamics of the model (2.6) and whether it persists or dies out of the disease. When<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x280.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x281.png" xlink:type="simple"/></inline-formula>, the disease-free equilibrium is globally stable, which means that the disease always dies out, and when<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x280.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x281.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x282.png" xlink:type="simple"/></inline-formula>, the plant disease will be permanent which means that after some period of time the plant disease will become endemic and it is global stable.</p><p>In this paper, we studied the existence, local stability and global stability of the disease-free equilibrium and endemic equilibrium of the system (2.3) in detail. By building a suitable Lyapunov function, and the Jacobian matrix method,</p><p>employing Routh-Hurwitz criteria and LaSalle-type invariance principle, the main results as shown in Theorems 4.2, 4.3 and 4.4 have been derived. Our main results indicate that if<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x293.png" xlink:type="simple"/></inline-formula>, then the disease-free equilibrium is globally asymptotically stable, if<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x293.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x294.png" xlink:type="simple"/></inline-formula>, the unique endemic equilibrium is globally asymptotically stable of the system (2.3). From above results, it is easy to find that the basic reproduction number <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x293.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x294.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/3-7403933x295.png" xlink:type="simple"/></inline-formula> plays an important role in determining the persistence or dying out of the disease.</p></sec><sec id="s7"><title>Acknowledgements</title><p>The research have been supported by The Natural Science Foundation of China (11561004), the Science and Technology research project of Jiangxi Provincial Education Department (171373, 171374, GJJ170815), The bidding project of Gannan Normal University (16zb02).</p></sec><sec id="s8"><title>Cite this paper</title><p>Lv, H.M., Fei, L.Z., Yuan, Z. and Zhang, F.M. (2018) Global Dynamic Analysis of a Vector-Borne Plant Disease Model with Discontinuous Treatment. Applied Mathematics, 9, 496-511. https://doi.org/10.4236/am.2018.95036</p></sec></body><back><ref-list><title>References</title><ref id="scirp.84855-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Lee, J.A., Halbert, S.E., Dawson, W.O., et al. (2015) Asymptomatic Spread of Huanglongbing and Implications for Disease Control. Proceedings of the National Academy of Sciences, 112, 7605-7610. https://doi.org/10.1073/pnas.1508253112</mixed-citation></ref><ref id="scirp.84855-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Smith, A.B., Beeck, C.P., Cowling, W.A., et al. (2013) A Bivariate Mixed Model Approach for the Analysis of Plant Survival Data. Euphytica, 190, 371-383.  
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