<?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.2015.611170</article-id><article-id pub-id-type="publisher-id">AM-60781</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 Stability of SEIQRS Computer Virus Propagation Model with Non-Linear Incidence Function
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>aisar</surname><given-names>Badshah</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>IQRA National University, Peshawar, Pakistan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>qaisarbadshah859@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>10</month><year>2015</year></pub-date><volume>06</volume><issue>11</issue><fpage>1926</fpage><lpage>1938</lpage><history><date date-type="received"><day>21</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>26</month>	<year>October</year>	</date><date date-type="accepted"><day>29</day>	<month>October</month>	<year>2015</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>
 
 
  In this paper, we present an SEIQRS epidemic model with non-linear incidence function. The proposed model exhibits two equilibrium points, the virus free equilibrium and viral equilibrium. The model stability is connected with the basic reproduction number 
  <em>R<sub>0</sub></em>. If 
  <em>R<sub>0</sub></em> &lt; 1 then the virus free equilibrium point is stable locally and globally. In the opposite case 
  <em>R<sub>0</sub></em> &gt; 1, then the model is locally and globally stable at viral equilibrium point. Numerical methods are used for supporting the analytical work.
 
</p></abstract><kwd-group><kwd>Malicious Objects</kwd><kwd> Epidemic Model</kwd><kwd> Viral Equilibrium</kwd><kwd> Virus Free Equilibrium</kwd><kwd> Basic Reproduction Number</kwd><kwd> Stability</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The Malicious objects are harmful codes that reproduce and spread by way of internet [<xref ref-type="bibr" rid="scirp.60781-ref1">1</xref>] . A number of malicious objects have been noticed to appear on the internet for the last decade. They are powerful enough to confront and disfunction the infected computer system. As the internet has been used for a wide range of function so, the malicious objects have become a serious threat to man’s work. They have hampered the economic and financial growth of man. Now it has become an issue of great concern and therefore it is vital to suggest such plans that are effective in combating the malicious objects. The correspondence between the propagation of biological virus and the malicious objects compel the researchers to advocate epidemic models that could explain and overcome the propagation of malicious objects. Re F. Wang et al. in [<xref ref-type="bibr" rid="scirp.60781-ref2">2</xref>] present the SEIQRS model with graded infection rates for internet worms. The infection ratio of exposed class have less then infected ratio and show the worm free and viral equilibrium stability locally as well as globally, which is connected to threshold quantity. In the previous decade or something like that, various epidemic models (see [<xref ref-type="bibr" rid="scirp.60781-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.60781-ref6">6</xref>] ) were essentially obtained to depict the spread of computer virus. B. K. Mishrand G. M. Ansari present an E-SIRS epidemic model for virus and worms in a computer network. In which they consider the immune as well as the latent period and self-replication time. They stated the global stability of the proposed model in term of reproduction number [<xref ref-type="bibr" rid="scirp.60781-ref7">7</xref>] . M. Kumar et.al. studied the quarantine and vaccination role in the control of virus and worms in the computer network [<xref ref-type="bibr" rid="scirp.60781-ref8">8</xref>] . S. T. Ge et al. presented the SEIQR epidemic model with the discrete time in computer networks. The stability of the proposed model was shown by Lyapunove method in [<xref ref-type="bibr" rid="scirp.60781-ref9">9</xref>] . M. Kummar and A. Kumar analyzes the SI<sub>j</sub> RS E-Epidemic model for various groups of infection in computer networking [<xref ref-type="bibr" rid="scirp.60781-ref10">10</xref>] .</p><p>In this paper, we present a Propagation Model with non-linear incidence function, (susceptible, exposed, infected, quarantined, and recovered) which exhibits two equilibria the virus free and viral equilibrium point. The stability of both equilibrium points is connected with the threshold quantity. On the off chance that its value is less then unity then the virus free equilibrium point is locally and additionally globally asymptotically stable and in the opposite case of the threshold quantity, the same condition of stability is satisfied for viral equilibrium point.</p><p>The rest of the paper is set as follows, in Section 2 we shall formulate the new model, in Section 3 the basic propertied is discussed like reproduction number, virus free and viral equilibrium. In Section 4, we shall study the local and global stability of the virus free equilibrium point. In Section 5, we shall examine the local and global stability at viral equilibrium point. Finally, we support our analytical work with numerical simulations.</p></sec><sec id="s2"><title>2. Model Formulation</title><p>As usual the computer it either internal or external (i.e. connected with the internet or not). In this model we divide the internal computers into five states. Susceptible, exposed, infected, quarantined and recovered. Where the variable S(t), E(t), I(t), Q(t) and R(t) denote the sizes of nodes at time t in the states susceptible, exposed, infectious, quarantined and recovered respectively. N(t) the total number of computer at time t, where N(t) = S(t) + E(t) + I(t) + Q(t) + R(t). The governed model is given below:</p><disp-formula id="scirp.60781-formula498"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7402907x5.png"  xlink:type="simple"/></disp-formula><p>With Initial conditions</p><disp-formula id="scirp.60781-formula499"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7402907x6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x7.png" xlink:type="simple"/></inline-formula> is the recruitment rate of the computers. The ratio of crashing nodes without attack of malicious objectsis<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x8.png" xlink:type="simple"/></inline-formula>. The transmission rate is denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x9.png" xlink:type="simple"/></inline-formula>. While <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x10.png" xlink:type="simple"/></inline-formula> is the ratio at which the recovered computers loss their immunity. The contact ratio between exposed and infected computers is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x11.png" xlink:type="simple"/></inline-formula>. The rate of recovery is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x12.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x13.png" xlink:type="simple"/></inline-formula> is the contact ratio between infected and recovered computers. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x14.png" xlink:type="simple"/></inline-formula>is the contact ratio between infected and recovered computers. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x15.png" xlink:type="simple"/></inline-formula>is the fraction of computers to be immune from virus.</p><p>We suppose that the like transmission rate in the form of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x16.png" xlink:type="simple"/></inline-formula>, where f is a positive function with, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x17.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x18.png" xlink:type="simple"/></inline-formula>, used by [<xref ref-type="bibr" rid="scirp.60781-ref11">11</xref>] . This is the generalized form of mass action law, that is, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x19.png" xlink:type="simple"/></inline-formula>, and the incidence rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x20.png" xlink:type="simple"/></inline-formula>. The function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x21.png" xlink:type="simple"/></inline-formula> is increasing for small values of I and decreasing in the opposite case where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x22.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. Basic Reproduction Number and Equilibrium Points</title><p>In this subsection, we shall investigate the feasible region and the threshold quantity for the proposed model (1). Where the size of total population is represented by N satisfy the following equation.</p><disp-formula id="scirp.60781-formula500"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x23.png"  xlink:type="simple"/></disp-formula><p>and then</p><disp-formula id="scirp.60781-formula501"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x24.png"  xlink:type="simple"/></disp-formula><p>Therefore, for the system (1) the positively invariant feasible region is given below.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x25.png" xlink:type="simple"/></inline-formula>,</p><p>Thus, the solution with initial condition will be analyzes inside the feasible region<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x26.png" xlink:type="simple"/></inline-formula>.</p><p>For viral free equilibrium point we take<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x27.png" xlink:type="simple"/></inline-formula>, thus from the system (1) we get</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x28.png" xlink:type="simple"/></inline-formula>.</p><p>To investigate the reproduction Number for system (1) we use the next generation method [<xref ref-type="bibr" rid="scirp.60781-ref12">12</xref>] .</p><p>Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x29.png" xlink:type="simple"/></inline-formula> then from system (1) we can write.</p><disp-formula id="scirp.60781-formula502"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x30.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.60781-formula503"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x31.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula504"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x32.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula505"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x33.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula506"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x34.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula507"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x35.png"  xlink:type="simple"/></disp-formula><p>The spectral radius of the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x36.png" xlink:type="simple"/></inline-formula> is represented by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x37.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60781-formula508"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x38.png"  xlink:type="simple"/></disp-formula><p>Now we examine the virus equilibrium point for the given system (1) and denoted by</p><disp-formula id="scirp.60781-formula509"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x39.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x40.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x42.png" xlink:type="simple"/></inline-formula>,</p><p>Now by substituting the above mention values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x44.png" xlink:type="simple"/></inline-formula>, in equation</p><disp-formula id="scirp.60781-formula510"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x45.png"  xlink:type="simple"/></disp-formula><p>we get</p><disp-formula id="scirp.60781-formula511"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x46.png"  xlink:type="simple"/></disp-formula><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x47.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x48.png" xlink:type="simple"/></inline-formula>is non-negative then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x49.png" xlink:type="simple"/></inline-formula> is a decreasing function Moreover.</p><disp-formula id="scirp.60781-formula512"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x50.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula513"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7402907x51.png"  xlink:type="simple"/></disp-formula><p>Next to take the derivative of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x52.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.60781-formula514"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x53.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x54.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x55.png" xlink:type="simple"/></inline-formula> also for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x56.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x57.png" xlink:type="simple"/></inline-formula>is follows that</p><disp-formula id="scirp.60781-formula515"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x58.png"  xlink:type="simple"/></disp-formula><p>Therefore, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x59.png" xlink:type="simple"/></inline-formula>has a unique positive zero if and only if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x60.png" xlink:type="simple"/></inline-formula>, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x61.png" xlink:type="simple"/></inline-formula>. It can be stated as below.</p><p>Proposition 3.1. Suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x62.png" xlink:type="simple"/></inline-formula> holds the conditions imposed on it. Then, the system (1) has virus free equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x63.png" xlink:type="simple"/></inline-formula> which is true for all parameter values. When, the system (1) admits also a unique viral equilibrium point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x64.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. The Stability Analysis of the Virus Free Equilibrium Point</title><p>In this section, we shall study the local and global stability of the given system (1) at virus free equilibrium point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x65.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 4.1. The given system (1) is locally asymptotically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x66.png" xlink:type="simple"/></inline-formula>, otherwise unstable.</p><p>Proof:</p><p>To examine the local stability of the given system (1) we construct the jacobian matrix at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x67.png" xlink:type="simple"/></inline-formula>, which is given below.</p><disp-formula id="scirp.60781-formula516"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x68.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula517"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x69.png"  xlink:type="simple"/></disp-formula><p>With row operation we can get the characteristic equation of the above jacobian matrix is</p><disp-formula id="scirp.60781-formula518"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x70.png"  xlink:type="simple"/></disp-formula><p>The first three roots of the above equation is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x71.png" xlink:type="simple"/></inline-formula> and the other roots will be find on the following way.</p><disp-formula id="scirp.60781-formula519"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x72.png"  xlink:type="simple"/></disp-formula><p>After a little algebraic calculation we can get the following equation</p><disp-formula id="scirp.60781-formula520"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x73.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.60781-formula521"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x74.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula522"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x75.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x76.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x77.png" xlink:type="simple"/></inline-formula> if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x78.png" xlink:type="simple"/></inline-formula> then according to Routh-Hurtwiz criteria the virus free equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x79.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x80.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x81.png" xlink:type="simple"/></inline-formula> and hence one of the eigenvalue have positive real part. So the virus free equilibrium point is unstable.</p>Global Stability of Viral Free Equilibrium Point<p>Theorem 4.2. The system (1) at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x82.png" xlink:type="simple"/></inline-formula> is globally stable when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x83.png" xlink:type="simple"/></inline-formula> otherwise unstable.</p><p>Proof: To examine the global stability of the proposed model consider a Lyapunov function as below:</p><disp-formula id="scirp.60781-formula523"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x84.png"  xlink:type="simple"/></disp-formula><p>Taking the derivative i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x85.png" xlink:type="simple"/></inline-formula>, we get the following</p><disp-formula id="scirp.60781-formula524"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x86.png"  xlink:type="simple"/></disp-formula><p>Since for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x87.png" xlink:type="simple"/></inline-formula> and after a little simplification we get the following results</p><disp-formula id="scirp.60781-formula525"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x88.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x89.png" xlink:type="simple"/></inline-formula>if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x90.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x91.png" xlink:type="simple"/></inline-formula> then according to Lasalle’s invariance principle the virus free equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x92.png" xlink:type="simple"/></inline-formula> is globally stable and in case of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x93.png" xlink:type="simple"/></inline-formula> the mention result is failed and hence the system is unstable [<xref ref-type="bibr" rid="scirp.60781-ref13">13</xref>] .</p></sec><sec id="s5"><title>5. The Local Stability Analysis of Viral Equilibrium Point</title><p>In this section we will discuss the local as well as the global stability of the system (1) for the viral equilibrium point.</p><p>Theorem 5.1. The given system (1) at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x94.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x95.png" xlink:type="simple"/></inline-formula>.</p><p>Proof: Toinvestigate the local stability of the given system (1) we find the jacobian matrix at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x96.png" xlink:type="simple"/></inline-formula>, which is given below.</p><disp-formula id="scirp.60781-formula526"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x97.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula527"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x98.png"  xlink:type="simple"/></disp-formula><p>Trace of the above jacobian Matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x99.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.60781-formula528"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x100.png"  xlink:type="simple"/></disp-formula><p>And after some row operation we get the following matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x101.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60781-formula529"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x102.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula530"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x103.png"  xlink:type="simple"/></disp-formula><p>Thus, the system (1) at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x104.png" xlink:type="simple"/></inline-formula> has eigenvalues, that contains negative real part. So, we conclude that the model (1) is locally asymptotically stable.</p>Global Stability of Viral Equilibrium Point<p>In this segment we should look at the global stability of the given system (1) at viral equilibrium point. We use the method presented in [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] established by Li and Mouldowney. According to which we find sufficient condition for the global stability of the model (1) at viral equilibrium point. First we shall discuss the method briefly.</p><p>Consider</p><disp-formula id="scirp.60781-formula531"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7402907x105.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x106.png" xlink:type="simple"/></inline-formula> is simply connected, open set and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x107.png" xlink:type="simple"/></inline-formula>. The solution of Equation (4) is denoted by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x108.png" xlink:type="simple"/></inline-formula> Let us suppose that the assumptions given below are true:</p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x109.png" xlink:type="simple"/></inline-formula>There exist a compact absorbing set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x110.png" xlink:type="simple"/></inline-formula></p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x111.png" xlink:type="simple"/></inline-formula>Equation (4) admit a unique equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x112.png" xlink:type="simple"/></inline-formula></p><p>We know that equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula> is globally stable in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula> when it locally stable as well as all the orbits in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x115.png" xlink:type="simple"/></inline-formula> converges to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x116.png" xlink:type="simple"/></inline-formula>. Bendixson criterion for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x117.png" xlink:type="simple"/></inline-formula> we mean that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x118.png" xlink:type="simple"/></inline-formula> satisfied a condition which prohibit the existence of non-constant periodic solutions of (4) The classical Bendixson’s condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x119.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x120.png" xlink:type="simple"/></inline-formula>, is robust under <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x121.png" xlink:type="simple"/></inline-formula>robust properties are discussed in [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.60781-ref15">15</xref>] .</p><p>If a neighborhood <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x122.png" xlink:type="simple"/></inline-formula> exist for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x123.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x124.png" xlink:type="simple"/></inline-formula> such that i.e. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x125.png" xlink:type="simple"/></inline-formula>Then the point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x126.png" xlink:type="simple"/></inline-formula> is wandering for the Equation (4). The following principle for global stability is established in [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] for any finite dimension autonomous systems.</p><p>Lemma 5.1. Assume that conditions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x127.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x128.png" xlink:type="simple"/></inline-formula> holds. Such that (4) satisfies a Bendixson criterion that is robust under <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x129.png" xlink:type="simple"/></inline-formula> local perturbations of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x130.png" xlink:type="simple"/></inline-formula> at all non-equilibrium non-wandering points for (4). Then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x131.png" xlink:type="simple"/></inline-formula> is globally stable in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x132.png" xlink:type="simple"/></inline-formula> provided it is stable.</p><p>The accompanying Bandixson criterion is displayed in [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] and indicates to have the heartiness needed by Lemma (5.1). Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x133.png" xlink:type="simple"/></inline-formula> be a nonsingular matrix and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x134.png" xlink:type="simple"/></inline-formula> is a matrix valued function that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x135.png" xlink:type="simple"/></inline-formula> on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x136.png" xlink:type="simple"/></inline-formula>. Suppose that for a compact absorbing set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x137.png" xlink:type="simple"/></inline-formula> not only exist but also continues for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x138.png" xlink:type="simple"/></inline-formula>. A <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x139.png" xlink:type="simple"/></inline-formula> quantity is defined as.</p><disp-formula id="scirp.60781-formula532"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x140.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.60781-formula533"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x141.png"  xlink:type="simple"/></disp-formula><p>The matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x142.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.60781-formula534"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x143.png"  xlink:type="simple"/></disp-formula><p>And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x144.png" xlink:type="simple"/></inline-formula> represents the second additive compound matrix of the Jacobian matrix J, i.e.,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x145.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x146.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x147.png" xlink:type="simple"/></inline-formula> be the Lozinskii measure of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x148.png" xlink:type="simple"/></inline-formula> with respect to a vector norm <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x149.png" xlink:type="simple"/></inline-formula> in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x150.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.60781-formula535"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x151.png"  xlink:type="simple"/></disp-formula><p>It is shown in [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] that, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x152.png" xlink:type="simple"/></inline-formula> is simply connected, the condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x153.png" xlink:type="simple"/></inline-formula> rules out the presence of any trajectory that fives rise to a simple closed rectifiable curve, like periodic orbits, and heteroclinic cycles it is invariant for system (4). The accompanying result for the global stability is displayed in [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] by Li and Muldowney.</p><p>Lemma 5.2. Let the simply connected set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x154.png" xlink:type="simple"/></inline-formula> satisfy the conditions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x155.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x156.png" xlink:type="simple"/></inline-formula>. Then the system (4) is globally stable in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x157.png" xlink:type="simple"/></inline-formula> at a unique equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x158.png" xlink:type="simple"/></inline-formula> if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x159.png" xlink:type="simple"/></inline-formula>.</p><p>Now for the analysis of global stability at viral equilibrium we follow the method presented by Li and Muldowney in [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] . The unstable viral equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x160.png" xlink:type="simple"/></inline-formula> means that the viruses will persists [<xref ref-type="bibr" rid="scirp.60781-ref16">16</xref>] , i.e., for any solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x161.png" xlink:type="simple"/></inline-formula> with initial conditions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x162.png" xlink:type="simple"/></inline-formula> in the trajectory of the model (1) there exist a constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x163.png" xlink:type="simple"/></inline-formula> which satisfy the following</p><disp-formula id="scirp.60781-formula536"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x164.png"  xlink:type="simple"/></disp-formula><p>Theorem 5.2. The viral equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x165.png" xlink:type="simple"/></inline-formula> of the system (1) is globally stable in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x166.png" xlink:type="simple"/></inline-formula> if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x167.png" xlink:type="simple"/></inline-formula>.</p><p>Proof: For the global stability of the system (1) we find the second additive compound matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x168.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60781-formula537"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x169.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula538"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x170.png"  xlink:type="simple"/></disp-formula><p>Let us choose a function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x171.png" xlink:type="simple"/></inline-formula>.</p><p>Then,</p><disp-formula id="scirp.60781-formula539"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x172.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula540"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x173.png"  xlink:type="simple"/></disp-formula><p>So,</p><disp-formula id="scirp.60781-formula541"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x174.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.60781-formula542"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x175.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula543"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x176.png"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.60781-formula544"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x177.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.60781-formula545"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x178.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula546"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x179.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula547"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x180.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula548"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x181.png"  xlink:type="simple"/></disp-formula><p>Suppose the norm in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x182.png" xlink:type="simple"/></inline-formula> as:</p><disp-formula id="scirp.60781-formula549"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x183.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x184.png" xlink:type="simple"/></inline-formula> be the vector in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x185.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x186.png" xlink:type="simple"/></inline-formula> signify the Lozinskii measure as regard to this norm follows [<xref ref-type="bibr" rid="scirp.60781-ref17">17</xref>] .</p><disp-formula id="scirp.60781-formula550"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x187.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.60781-formula551"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x188.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula552"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x189.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.60781-formula553"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x190.png"  xlink:type="simple"/></disp-formula><p>using second equation of system (1) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x191.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60781-formula554"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x192.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula555"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x193.png"  xlink:type="simple"/></disp-formula><p>Again,</p><disp-formula id="scirp.60781-formula556"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x194.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.60781-formula557"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x195.png"  xlink:type="simple"/></disp-formula><p>And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x196.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60781-formula558"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x197.png"  xlink:type="simple"/></disp-formula><p>using third equation of system (1), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x198.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60781-formula559"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x199.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula560"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x200.png"  xlink:type="simple"/></disp-formula><p>With a compact absorbing set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x201.png" xlink:type="simple"/></inline-formula> every solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x202.png" xlink:type="simple"/></inline-formula> of the model (1) with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x203.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.60781-formula561"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x204.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula562"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x205.png"  xlink:type="simple"/></disp-formula><p>Thus the viral equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x206.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable according to [<xref ref-type="bibr" rid="scirp.60781-ref14">14</xref>] .</p><p>Next we talk about the given subsystem of system (1)</p><disp-formula id="scirp.60781-formula563"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7402907x207.png"  xlink:type="simple"/></disp-formula><p>And it limit system is</p><disp-formula id="scirp.60781-formula564"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7402907x208.png"  xlink:type="simple"/></disp-formula><p>Based on (6), we get</p><disp-formula id="scirp.60781-formula565"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x209.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60781-formula566"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x210.png"  xlink:type="simple"/></disp-formula><p>This implies that as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x211.png" xlink:type="simple"/></inline-formula> then</p><disp-formula id="scirp.60781-formula567"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x212.png"  xlink:type="simple"/></disp-formula><p>Then according to [<xref ref-type="bibr" rid="scirp.60781-ref18">18</xref>] the system (1) at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x213.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable.</p></sec><sec id="s6"><title>6. Discussion</title><p>The aim of this work is to study and analyze the dynamic behavior of an epidemic model SEIQRS with a nonlinear incidence function. We consider a mathematical model of the type SEIQRS and obtained the basic reproduction number, to determine its dynamical behavior. In epidemiology, the reproduction ratio is very important, because the stability of the proposed model is associated with reproduction ratio. For virus free equilibrium point, the model is stable locally and globally if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x214.png" xlink:type="simple"/></inline-formula>. In the case of when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x215.png" xlink:type="simple"/></inline-formula> exceeds then unity then the system (1) is asymptotically stable at viral equilibrium point.</p><p>The purpose of this section is to support the analytic results mentioned in above work are supported through numerical results. Numerical results we choose different values of parameters, which we discuss below with the help of graph. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x216.png" xlink:type="simple"/></inline-formula>, the reproduction ratio for immune free system is</p><disp-formula id="scirp.60781-formula568"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x217.png"  xlink:type="simple"/></disp-formula><p>Thus we can write <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x218.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.60781-formula569"><graphic  xlink:href="http://html.scirp.org/file/11-7402907x219.png"  xlink:type="simple"/></disp-formula><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x220.png" xlink:type="simple"/></inline-formula>, then clearly the virus is vanished. But if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x221.png" xlink:type="simple"/></inline-formula> (see <xref ref-type="fig" rid="fig1">Figure 1</xref>), then the vaccination <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x222.png" xlink:type="simple"/></inline-formula> is needed so that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x223.png" xlink:type="simple"/></inline-formula> or equivalently to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x224.png" xlink:type="simple"/></inline-formula>.</p><p>Thereby, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x225.png" xlink:type="simple"/></inline-formula>is the vaccination able to exterminate the virus from the internal computers <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref>. In the opposite case<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x226.png" xlink:type="simple"/></inline-formula>, the virus will persists, even if we can vaccinate all recruitment <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><p>Nothing that when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x227.png" xlink:type="simple"/></inline-formula>, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x228.png" xlink:type="simple"/></inline-formula> is an increasing function of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x229.png" xlink:type="simple"/></inline-formula>, and the value of the vaccination cover</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The dynamical behaviour of system (1), for different initial conditions and parameters: ∂ = 5, ϑ = 0.05, β = 0.02, ћ = 0.02, η<sub>1</sub> = 0.009, η<sub>2</sub> = 0.001, η<sub>1</sub> = 0.03, ξ = 0.01, ψ = 0.01, φ = 0, Here<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x231.png" xlink:type="simple"/></inline-formula>, R<sub>1</sub> = 1.9068</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-7402907x230.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The dynamical behaviour of system (1), for different initial conditions and parameters of <xref ref-type="fig" rid="fig1">Figure 1</xref> except φ = 0.6 &lt; φ<sub>v</sub> = 0.6658</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-7402907x232.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The dynamical behaviour of system (1), for different initial conditions and parametes of <xref ref-type="fig" rid="fig1">Figure 1</xref> except φ = φ<sub>v</sub> = 0.6658</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-7402907x233.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The dynamical behaviour of system (1), for different initial conditions and parametes ∂ = 8, ϑ = 0.03, β = 0.02, ћ = 0.02, η<sub>1</sub> = 0.009, η<sub>2</sub> = 0.01, η<sub>1</sub> = 0.03, ξ = 0.01, ψ = 0.01, φ = 1. Here<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x235.png" xlink:type="simple"/></inline-formula>, φ<sub>v</sub> = 1.5150</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-7402907x234.png"/></fig><p>age <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x236.png" xlink:type="simple"/></inline-formula> exceed then unity when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x237.png" xlink:type="simple"/></inline-formula>. Therefore, for the reduction of vaccination coverage it is important through vaccination <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7402907x238.png" xlink:type="simple"/></inline-formula> increase the time period of the loss of immunity.</p></sec><sec id="s7"><title>Acknowledgements</title><p>The author is grateful to the anonymous reviewers for their constructive suggestions that greatly improve the quality of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>QaisarBadshah, (2015) Global Stability of SEIQRS Computer Virus Propagation Model with Non-Linear Incidence Function. 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