<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2016.410191</article-id><article-id pub-id-type="publisher-id">JAMP-71362</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>
 
 
  The Effect of State-Dependent Control for an SIRS Epidemic Model with Varying Total Population
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fuwei</surname><given-names>Zhang</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>Linfei</surname><given-names>Nie</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Mathematics and Systems Science, Xinjiang University, Urumqi, China</addr-line></aff><pub-date pub-type="epub"><day>13</day><month>10</month><year>2016</year></pub-date><volume>04</volume><issue>10</issue><fpage>1889</fpage><lpage>1898</lpage><history><date date-type="received"><day>September</day>	<month>24,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>October</month>	<year>16,</year>	</date><date date-type="accepted"><day>October</day>	<month>20,</month>	<year>2016</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>
 
 
  Based on the mechanism of prevention and control of infectious disease, we propose, in this paper, an SIRS epidemic model with varying total population size and state-dependent control, where the fraction of susceptible individuals in population is as the detection threshold value. By the Poincar&#233; map, theory of differential inequalities and differential equation geometry, the existence and orbital stability of the disease-free periodic solution are discussed. Theoretical results show that by state-dependent pulse vaccination we can make the proportion of infected individuals tend to zero, and control the transmission of disease in population.
 
</p></abstract><kwd-group><kwd>SIRS Epidemic Model</kwd><kwd> Varying Total Population</kwd><kwd> State-Dependent Pulse Control</kwd><kwd> Periodic Solution</kwd><kwd> Orbital Stability</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>It is generally known that the spread of infectious diseases has been a threat to healthy of human beings and other species. In order to prevent and control the transmission of disease (such as hepatitis C, malaria, influenza), pulse vaccination as an effective strategy has been widely studied by many scholars in the study of mathematical epidemiology. In the classical research literature it is usually assumed that the pulse vaccination occurs at fixed moment intervals and total population size remains constant [<xref ref-type="bibr" rid="scirp.71362-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.71362-ref2">2</xref>] , and so on. Although fixed time pulse vaccination strategy is better than the traditional vaccination strategies (continuous vaccination), it has a few disadvantages. For these reasons, a new vaccination strategies, state-dependent pulse vaccination is proposed when the number of the susceptible individuals or infected individuals reaches a critical value. Clearly, the latter control strategies are more ra- tional for disease control because of its efficiency, economy, and feasibility. In recent years, mathematical models with state-dependent pulse control strategies have been extensively applied to research fields of applied science, such as pest management model [<xref ref-type="bibr" rid="scirp.71362-ref3">3</xref>] , tumor model [<xref ref-type="bibr" rid="scirp.71362-ref4">4</xref>] , predator-prey model [<xref ref-type="bibr" rid="scirp.71362-ref5">5</xref>] , and others. Particularly, Nie et al. [<xref ref-type="bibr" rid="scirp.71362-ref6">6</xref>] investigated an SIR epidemic model with state-dependent pulse vaccination. In it, authors obtained the existence and stability of positive order-1 and order-2 periodic solution. Tang et al. [<xref ref-type="bibr" rid="scirp.71362-ref7">7</xref>] proposed an SIR epidemic model with state-dependent pulse control strategies. Authors demonstrated that the combination of pulse vaccination and treatment is optimal in terms of cost under certain conditions, and studied the existence and stability of periodic solution.</p><p>On the other hand, the population sizes of all epidemic models with state-dependent pulse control are constant. These types of models have been studied extensively since they are easier to analyze than variable population size models. Obviously, the assum- ption that the total population size which remains constant is reasonable if negligible mortality rate and the disease spread quickly through the population. However, it fails to hold for diseases that are endemic in communities with changing populations, and for diseases which raise the mortality rate substantially. In such situation, we can hardly expect a population remaining constant, and hence more complicated epidemic models with varying population size should be considered. In fact, studies of this type of models have been become a major topic in mathematical epidemiology. For example, an general epidemiological model with vaccination and varying total population was discussed by Yang et al. [<xref ref-type="bibr" rid="scirp.71362-ref8">8</xref>] , in which the global dynamics of this model and it’s corresponding proportionate model are investigated. The conditions between the two models in terms of disease eradication and persistence are obtained. Hui et al. [<xref ref-type="bibr" rid="scirp.71362-ref9">9</xref>] introduced an SEIS epidemic model with total population which is not stationary. Results are obtained in terms of three threshold which respectively determines whether or not the disease dies out and dynamics of epidemic model when births of population are throughout a year. At same time, they also discussed the existence of disease-free periodic solution when births of population are birth pulse. More related literature, we also can be found in [<xref ref-type="bibr" rid="scirp.71362-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.71362-ref11">11</xref>] , and the references therein.</p><p>As far as we know, epidemic model with varying total population and state-de- pendent feedback control strategies had never been done in the literatures. Hence, in this paper, the dynamical behavior of an SIRS epidemic model with varying total population and state-dependent pulse control strategy is studied. The main aim is to explore how the state-dependent pulse control strategy affects the transmission of diseases. The remaining part of this paper is organized as follows. In the next section, an SIRS control model is constructed and some preliminaries are introduced, which are useful for the latter discussion. In section 3, we will focus our attention on the existence and orbital stability of disease-free periodic. Finally, some concluding remarks are presented in the last section.</p></sec><sec id="s2"><title>2. Models and Preliminaries</title><p>In the study of the dynamic properties of infectious diseases, it was found that when the popularity of disease for a long time total population size change this factor should be considered. In this case, Busenberg et al. [<xref ref-type="bibr" rid="scirp.71362-ref12">12</xref>] proposed the following SIRS epidemic model with varying total population size.</p><disp-formula id="scirp.71362-formula110"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x2.png"  xlink:type="simple"/></disp-formula><p>Here<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x3.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x4.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x5.png" xlink:type="simple"/></inline-formula> denote the numbers of susceptible, infected, and recovered individuals respectively, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x6.png" xlink:type="simple"/></inline-formula> denote the total population size at time t. The parameters in the model have the following features: b is the per capita birth rate with the assumption that all newborns are susceptible; d is the per capita disease free death rate of the population; the constants <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x7.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x8.png" xlink:type="simple"/></inline-formula> denote the excess per capita death rate of infected individuals and recovered individuals, respectively; c is the per capital recovery rate of the infected individuals and e is the per capita loss of immunity rate for recovered individuals. It is assumed that all susceptible group becomes infected at a rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x9.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x10.png" xlink:type="simple"/></inline-formula> is the effective per capita contract rate of infective individuals. All parameter values are assumed to be non- negative and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x11.png" xlink:type="simple"/></inline-formula>.</p><p>Since the susceptible individuals are immunity toward certain infectious diseases in the crowd, once infected individuals get into the susceptible groups, this will lead to the outbreak of the diseases. For this reason, we propose a pulse vaccination function as follows <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x12.png" xlink:type="simple"/></inline-formula> where p <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x13.png" xlink:type="simple"/></inline-formula> is the proportion by which the susceptible individuals numbers is reduced by pulse vaccination.</p><p>Taking into account pulse vaccination as state-dependent feedback control strategies, model (1) can be extend to the following state-dependent pulse differential equation.</p><disp-formula id="scirp.71362-formula111"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x14.png"  xlink:type="simple"/></disp-formula><p>where the critical threshold <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x15.png" xlink:type="simple"/></inline-formula> is a constant. The meaning of model (2) as following: once the fraction of the susceptible individuals in the population reaches the critical value H at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x16.png" xlink:type="simple"/></inline-formula>, vaccination control strategies are carried out which lead to the number of susceptible and recovered individuals abruptly turn to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x17.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x18.png" xlink:type="simple"/></inline-formula> respectively.</p><p>The equation for the total population size <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x19.png" xlink:type="simple"/></inline-formula> can be determined from model (2)</p><disp-formula id="scirp.71362-formula112"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x20.png"  xlink:type="simple"/></disp-formula><p>It means that total population size <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x21.png" xlink:type="simple"/></inline-formula> is not constant. In such situations, to discuss the dynamics behavior of model (2) we need to consider the fraction of indivi- duals in the three epidemiological classes, namely</p><disp-formula id="scirp.71362-formula113"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x22.png"  xlink:type="simple"/></disp-formula><p>It following from (3) that we can transforms model (2) into the following model for these new variables</p><disp-formula id="scirp.71362-formula114"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x23.png"  xlink:type="simple"/></disp-formula><p>Define three threshold parameter as follows</p><disp-formula id="scirp.71362-formula115"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x24.png"  xlink:type="simple"/></disp-formula><p>On the dynamics of model (4) without pulse effect has been studied in [<xref ref-type="bibr" rid="scirp.71362-ref12">12</xref>] . Relevant conclusions can be summarized as the following Theorem 1.</p><p>Theorem 1. For model (4) without pulse control, the following result hold true.</p><p>1) The disease-free equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x25.png" xlink:type="simple"/></inline-formula> always exists and is globally asymptoti- cally stable in the feasibility region <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x26.png" xlink:type="simple"/></inline-formula> when- ever<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x27.png" xlink:type="simple"/></inline-formula>, and unable when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x28.png" xlink:type="simple"/></inline-formula>.</p><p>2) When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x29.png" xlink:type="simple"/></inline-formula>, there exist a unique endemic equilibrium<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x30.png" xlink:type="simple"/></inline-formula>, which is globally asymptotically stable in the feasibility region <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x31.png" xlink:type="simple"/></inline-formula> where</p><disp-formula id="scirp.71362-formula116"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x32.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x33.png" xlink:type="simple"/></inline-formula> can be found by solving equation</p><disp-formula id="scirp.71362-formula117"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x34.png"  xlink:type="simple"/></disp-formula><p>3) The total population <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x35.png" xlink:type="simple"/></inline-formula> has the asymptotic behavior <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x36.png" xlink:type="simple"/></inline-formula> if</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x37.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x38.png" xlink:type="simple"/></inline-formula> if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x39.png" xlink:type="simple"/></inline-formula>.</p><p>4) When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x40.png" xlink:type="simple"/></inline-formula>, the total infected population has the asymptotic behavior</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x41.png" xlink:type="simple"/></inline-formula>if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x42.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x43.png" xlink:type="simple"/></inline-formula> if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x44.png" xlink:type="simple"/></inline-formula>.</p><p>Based on the above discussions, we just need to discuss cases (a) and (b) in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Considering the similarities of cases (a) and (b), throughout of this paper, we discuss only the case (a). That is, in a increasing population, the number of infected individuals is converges to infinity, while the fraction of infected individuals in population is tending to a nonzero constant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x45.png" xlink:type="simple"/></inline-formula>.</p><p>Due to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x46.png" xlink:type="simple"/></inline-formula>, for model (4) we can eliminate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x47.png" xlink:type="simple"/></inline-formula> by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x48.png" xlink:type="simple"/></inline-formula>and consider the two-dimensional model.</p><disp-formula id="scirp.71362-formula118"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x49.png"  xlink:type="simple"/></disp-formula><p>By the biological background, we only focus on model (5) in the biological meaning region<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x50.png" xlink:type="simple"/></inline-formula>. Besides, the globally exis- tence and uniqueness properties of solution of model (5) are guaranteed by the smoo- thness of f, which is the mapping defined by right-side of model (5), for details see [<xref ref-type="bibr" rid="scirp.71362-ref13">13</xref>] .</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x51.png" xlink:type="simple"/></inline-formula> be an arbitrary nonempty set and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x52.png" xlink:type="simple"/></inline-formula> be an arbitrary point. The distance between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x53.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x54.png" xlink:type="simple"/></inline-formula> is defined by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x55.png" xlink:type="simple"/></inline-formula>. Set</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x56.png" xlink:type="simple"/></inline-formula>be a solution of model (5) starting from initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x57.png" xlink:type="simple"/></inline-formula> at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x58.png" xlink:type="simple"/></inline-formula>. We define the positive orbit as follows</p><disp-formula id="scirp.71362-formula119"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x59.png"  xlink:type="simple"/></disp-formula><p>Firstly, on the positivity of solutions of model (5), we have the following Lemma 1.</p><p>Lemma 1. Supposing that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x60.png" xlink:type="simple"/></inline-formula> is a solution of model (5) with the initial condition<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x61.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x62.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x63.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. For any initial value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x64.png" xlink:type="simple"/></inline-formula>, we will discuss all possible cases by the relation of the solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x65.png" xlink:type="simple"/></inline-formula> to the line <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x66.png" xlink:type="simple"/></inline-formula> as follows.</p><p>1) The solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x67.png" xlink:type="simple"/></inline-formula> intersects with line <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x68.png" xlink:type="simple"/></inline-formula> finitely many times.</p><p>For this case, due to the endemic equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x69.png" xlink:type="simple"/></inline-formula> is globally asymptotically</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Threshold criteria and asymptotic behavior</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >case</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x70.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x71.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x72.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x73.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x74.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x75.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >(a)</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x76.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x77.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x78.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x79.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x80.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x81.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >(b)</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x82.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x83.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x84.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x85.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x86.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><p>stable, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x87.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x88.png" xlink:type="simple"/></inline-formula>for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x89.png" xlink:type="simple"/></inline-formula>.</p><p>2) The solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x90.png" xlink:type="simple"/></inline-formula> intersects with line <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x91.png" xlink:type="simple"/></inline-formula> infinitely many times.</p><p>For second situation, assume that solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x92.png" xlink:type="simple"/></inline-formula> intersects with line <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x93.png" xlink:type="simple"/></inline-formula> at times <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x94.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x95.png" xlink:type="simple"/></inline-formula>. If the conclusion of Lemma 1 is false, we obtain that there exists a positive integer n and a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x96.png" xlink:type="simple"/></inline-formula> such that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x97.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x98.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x99.png" xlink:type="simple"/></inline-formula>. The first possibility is that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x100.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x101.png" xlink:type="simple"/></inline-formula>. For this case, it follows from the first and third equation of model (5) that</p><disp-formula id="scirp.71362-formula120"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x102.png"  xlink:type="simple"/></disp-formula><p>which contradicts the fact that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x103.png" xlink:type="simple"/></inline-formula>.</p><p>The other case is that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x104.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x105.png" xlink:type="simple"/></inline-formula>. In this regard, it follows from the second and fourth equation of model (5) that</p><disp-formula id="scirp.71362-formula121"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x106.png"  xlink:type="simple"/></disp-formula><p>which lead to a contradiction with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x107.png" xlink:type="simple"/></inline-formula>. Therefore, according to above discussion, we can obtain that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x108.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x109.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x110.png" xlink:type="simple"/></inline-formula>. This proof is complete.</p><p>In order to address the dynamical behaviors of model (5), we could construct two sections to the vector field of model (5) by</p><disp-formula id="scirp.71362-formula122"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x111.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.71362-formula123"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x112.png"  xlink:type="simple"/></disp-formula><p>Choosing section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x113.png" xlink:type="simple"/></inline-formula> as a Poincar&#233; section. Assume that for any point</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x114.png" xlink:type="simple"/></inline-formula>, the trajectory <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x115.png" xlink:type="simple"/></inline-formula> starting from the initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x116.png" xlink:type="simple"/></inline-formula> in- tersects section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x117.png" xlink:type="simple"/></inline-formula> infinitely many times. That is, trajectory <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x118.png" xlink:type="simple"/></inline-formula> jumps to section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x119.png" xlink:type="simple"/></inline-formula> at point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x120.png" xlink:type="simple"/></inline-formula> due to pulse effect. Moreover, trajectory</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula>will reach at section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula> at point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula>, and then jumps to point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula> on section<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula>. Repeating this procedure, we get two pulse point sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x127.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x128.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x129.png" xlink:type="simple"/></inline-formula> is only determined by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x130.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x131.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x132.png" xlink:type="simple"/></inline-formula>. Therefore, we can define a Poincar&#233; map of section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x133.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.71362-formula124"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x134.png"  xlink:type="simple"/></disp-formula><p>From the definition of Poincar&#233; map<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x135.png" xlink:type="simple"/></inline-formula>, it easy to get that</p><disp-formula id="scirp.71362-formula125"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x136.png"  xlink:type="simple"/></disp-formula><p>Obviously, function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x137.png" xlink:type="simple"/></inline-formula> is continuously differential according to the Cauchy- Lipschitz theorem. If there exist positive integer k such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x138.png" xlink:type="simple"/></inline-formula>, then trajectory <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x139.png" xlink:type="simple"/></inline-formula> of model (5) is said to be order-k periodic solution.</p></sec><sec id="s3"><title>3. Main Results</title><p>Our main purpose in this section is to investigate the existence and orbital stability of periodic solution of model (5). From the geometrical construction of phase space of model (5), we note that the trajectory <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula> from any initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula> intersects section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula> infinite times with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula>. However, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x144.png" xlink:type="simple"/></inline-formula>, then trajectory <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x145.png" xlink:type="simple"/></inline-formula> from any initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x146.png" xlink:type="simple"/></inline-formula> may be free from pulse effects or intersects section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x147.png" xlink:type="simple"/></inline-formula> infinitely times, which depend on the initial con- ditions. Consequently, based on different positions of section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x148.png" xlink:type="simple"/></inline-formula> we need to discuss the existence and orbital stability of periodic solution of model (5) in the cases of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x149.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x150.png" xlink:type="simple"/></inline-formula>.</p><p>Case I: The case of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x151.png" xlink:type="simple"/></inline-formula>.</p><p>For this case, it will prove that model (5) possesses a disease-free periodic solution, which is orbitally asymptotically stable.</p><p>Suppose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x152.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x153.png" xlink:type="simple"/></inline-formula>, then model (5) degenerates into the following model</p><disp-formula id="scirp.71362-formula126"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x154.png"  xlink:type="simple"/></disp-formula><p>Integrating the first equation of model (7) with the initial condition</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x155.png" xlink:type="simple"/></inline-formula>, one yields</p><disp-formula id="scirp.71362-formula127"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x156.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.71362-formula128"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x157.png"  xlink:type="simple"/></disp-formula><p>Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x158.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x159.png" xlink:type="simple"/></inline-formula>, then we obtain</p><disp-formula id="scirp.71362-formula129"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x160.png"  xlink:type="simple"/></disp-formula><p>Therefore, model (5) possesses the following disease-free periodic solution, denoted by</p><disp-formula id="scirp.71362-formula130"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x161.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x162.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x163.png" xlink:type="simple"/></inline-formula>.</p><p>On the stability of this disease-free periodic solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x164.png" xlink:type="simple"/></inline-formula> we have the following result.</p><p>Theorem 2. For any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x165.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x166.png" xlink:type="simple"/></inline-formula> the disease-free periodic solution (8) of model (5) is orbitally asymptotically stable.</p><p>Proof. We assume that section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x167.png" xlink:type="simple"/></inline-formula> intersects line <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x168.png" xlink:type="simple"/></inline-formula> and x axis at points P and Q, respectively. From the geometrical structure of phase space of model (5), we know that trajectory starts from any point on set</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x169.png" xlink:type="simple"/></inline-formula>will enter set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x170.png" xlink:type="simple"/></inline-formula>. Further, set</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x171.png" xlink:type="simple"/></inline-formula>is mapped to set</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x172.png" xlink:type="simple"/></inline-formula>by Poincar&#233; map (6), where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x173.png" xlink:type="simple"/></inline-formula>. Then, set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x174.png" xlink:type="simple"/></inline-formula> is mapped to set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x175.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x176.png" xlink:type="simple"/></inline-formula>. Repeat above-mentioned procedure, we gain one point sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x177.png" xlink:type="simple"/></inline-formula> and which satisfy</p><disp-formula id="scirp.71362-formula131"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x178.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.71362-formula132"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720706x179.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x180.png" xlink:type="simple"/></inline-formula>.</p><p>From (9), it is concluded that the point sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x181.png" xlink:type="simple"/></inline-formula> is monotonically decrease in the interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x182.png" xlink:type="simple"/></inline-formula> and converge to a fixed point in this bound region. That is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x183.png" xlink:type="simple"/></inline-formula>.</p><p>Suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x184.png" xlink:type="simple"/></inline-formula> is a solution of small-amplitude perturbation of disease- free periodic solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x185.png" xlink:type="simple"/></inline-formula> with initial value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x186.png" xlink:type="simple"/></inline-formula>, which first intersects section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x187.png" xlink:type="simple"/></inline-formula> at point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x188.png" xlink:type="simple"/></inline-formula> and then jumps to point</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula>. Further, solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula> insects section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x191.png" xlink:type="simple"/></inline-formula> at point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x192.png" xlink:type="simple"/></inline-formula> again. Repeating the above process, we have two point sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x193.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x194.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x195.png" xlink:type="simple"/></inline-formula>. Furthermore, by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x196.png" xlink:type="simple"/></inline-formula>, it is clear that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x197.png" xlink:type="simple"/></inline-formula>. This shows that the disease-free periodic solution (8) of model (5) is orbitally asymptotically stable. This proof is complete.</p><p>Case II: The case of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x198.png" xlink:type="simple"/></inline-formula>.</p><p>For this case, we know that there a point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x199.png" xlink:type="simple"/></inline-formula> such that tra- jectory <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x200.png" xlink:type="simple"/></inline-formula> is tangent to section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x201.png" xlink:type="simple"/></inline-formula> at the point</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x202.png" xlink:type="simple"/></inline-formula>. Then the point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x203.png" xlink:type="simple"/></inline-formula> is jump to the po- int <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x204.png" xlink:type="simple"/></inline-formula> on section <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x205.png" xlink:type="simple"/></inline-formula> after pulse effect. According to the different positions of point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x206.png" xlink:type="simple"/></inline-formula> we has the following results.</p><p>Theorem 3. For any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x207.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x208.png" xlink:type="simple"/></inline-formula>, if</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x209.png" xlink:type="simple"/></inline-formula>, then model (5) exists a positive order-1 periodic solution. Further, if</p><disp-formula id="scirp.71362-formula133"><graphic  xlink:href="http://html.scirp.org/file/5-1720706x210.png"  xlink:type="simple"/></disp-formula><p>then model (5) exists a disease-free periodic solution (8), which is orbitally asympto- tically stable.</p><p>For this case, (8) is a disease-free periodic solution of model (5), and the proof of stability is similar to the proof of Theorem 2, we therefore omit here.</p></sec><sec id="s4"><title>4. Concluding Remarks</title><p>In order to explore the effects of the state-dependent pulse control strategies on the transmission of the infectious diseases in a population of varying size, an SIRS epidemic model with varying total population and state-dependent pulse control strategy is proposed and analyzed in this paper. Theoretically analyzing this control model, we find that a disease-free periodic solution always exists and orbitally stable when condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x211.png" xlink:type="simple"/></inline-formula> holds. Theoretical results shows that the disease finally disappears if we control the fraction of susceptible individuals in relatively low levels. Furthermore, we obtained some sufficient condition on existence and stability of the positive order-1 periodic solution when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720706x212.png" xlink:type="simple"/></inline-formula>. This amounts to that we can control the fraction of susceptible individuals and infected individuals within a retain range for a long time by appropriately choose the immune strength p and critical threshold H. Therefore, we can concluded that state-dependent pulse vaccination is a feasible, eco- nomic, and high efficient method to prevention and control spread of diseases.</p></sec><sec id="s5"><title>Conflict of Interests</title><p>The authors declare that there is no conflict of interests regarding the publication of this paper.</p></sec><sec id="s6"><title>Fund</title><p>This research has been partially supported by the Natural Science Foundation of Xinjiang (Grant no. 2016D01C046).</p></sec><sec id="s7"><title>Cite this paper</title><p>Zhang, F.W. and Nie, L.F. (2016) The Effect of State-Depen- dent Control for an SIRS Epidemic Model with Varying Total Population. Journal of Ap- plied Mathematics and Physics, 4, 1889- 1898. http://dx.doi.org/10.4236/jamp.2016.410191</p></sec></body><back><ref-list><title>References</title><ref id="scirp.71362-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hu, Z., Ma, W. and Ruan, S. (2012) Analysis of SIR Epidemic Models with Nonlinear Incidence Rate and Treatment. Mathematical Biosciences, 238, 12-20. http://dx.doi.org/10.1016/j.mbs.2012.03.010</mixed-citation></ref><ref id="scirp.71362-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Meng, X. and Chen, L. (2008) The Dynamics of a New SIR Epidemic Model Concerning Pulse Vaccination Strategy. Applied Mathematics and Computation, 197, 582-597. http://dx.doi.org/10.1016/j.amc.2007.07.083</mixed-citation></ref><ref id="scirp.71362-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Zhang, T., Meng, X., Liu, R. and Zhang, T. 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