<?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">APM</journal-id><journal-title-group><journal-title>Advances in Pure Mathematics</journal-title></journal-title-group><issn pub-type="epub">2160-0368</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/apm.2018.85030</article-id><article-id pub-id-type="publisher-id">APM-84968</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>
 
 
  Stability Analysis and Stochastic SI Modelling of Endemic Diseases
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Desalegn</surname><given-names>Petros Kelkile</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>Pan Africa University Institute of Basic Sciences, Technology and Innovation, Nairobi, Kenya</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>desye.peter@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>05</month><year>2018</year></pub-date><volume>08</volume><issue>05</issue><fpage>516</fpage><lpage>534</lpage><history><date date-type="received"><day>24,</day>	<month>April</month>	<year>2018</year></date><date date-type="rev-recd"><day>28,</day>	<month>May</month>	<year>2018</year>	</date><date date-type="accepted"><day>31,</day>	<month>May</month>	<year>2018</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, we study a stochastic epidemic model in Meta-population setting. The stochastic model is obtained from the deterministic model by set up random perturbations about the endemic equilibrium state. The outcome of random perturbations on the stability actions of endemic equilibrium is discussed. Stability of the two equilibriums is studied using the Lyapunov function.
 
</p></abstract><kwd-group><kwd>Meta-Population</kwd><kwd> Basic Reproduction Ratio</kwd><kwd> Lyapunov Function</kwd><kwd> Positive Equilibrium</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Modeling of infectious diseases with stochastic differential equation (SDE) has increased foundation lately due to its extensive variety of applications and its aptitude to reflect actuality in epidemiology [<xref ref-type="bibr" rid="scirp.84968-ref1">1</xref>] . The diseases outbreaks in a population of susceptibles rationally go behind stochastic processes [<xref ref-type="bibr" rid="scirp.84968-ref2">2</xref>] . Stochastic process occurs naturally in lots of physical applications where randomness is to be incorporated in the mathematical model [<xref ref-type="bibr" rid="scirp.84968-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.84968-ref4">4</xref>] . In recent years, main studies on stochastic model that have been published by researchers have recognized the growing significance of study the stability of stochastic positive equilibrium, as well as the global stability of the endemic equilibrium [<xref ref-type="bibr" rid="scirp.84968-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.84968-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.84968-ref7">7</xref>] . In this paper we approached by using deterministic and stochastic model. Briefly deterministic models are model processes which are often described by differential equations, with a unique input leading to a unique output for well-defined linear models and with multiple outputs possible for non-linear models. Throughout this paper, let ( Ω , F , P ) be a complete probability space with a filtration ( F t ) t ∈ ℝ satisfying the usual conditions (i.e., it is right continuous and increasing while F 0 contains all P -null sets).</p><p>Considering the general n dimensional stochastic differential equation</p><p>d x ( t ) = f ( x ( t ) , t ) d t + φ ( x ( t ) , t ) d B t</p><p>on t ≥ 0 with initial value x ( 0 ) = x 0 , the solution is denoted by x ( t , x 0 ) . Assume that f ( 0 , t ) = 0 and φ ( 0 , t ) = 0 for all t ≥ 0 , so (1.0) has the solution x ( t ) = 0 . This solution is called the trivial solution.</p><p>Definition 1.1. The trivial solution x ( t ) = 0 of (1.0) is said to be as follows:</p><p>1) stable in probability if for all ϵ &gt; 0 ,</p><p>l i m x 0 → 0 P ( s u p t ≥ 0 | x ( t , x 0 ) ≥ ϵ | ) = 0</p><p>2) asymptotically stable if it is stable in probability and, moreover,</p><p>l i m x 0 → 0 P ( l i m t → ∞ x ( t , x 0 ) = 0 ) = 1</p><p>3) asymptotically stable in the large if it is stable in probability and, moreover, for all x 0 ∈ ℝ</p><p>P ( l i m t → ∞ x ( t , x 0 ) = 0 ) = 1</p><p>In this paper, we consider the epidemic model in Meta-population setting. From the proposed schematics of the compartment model shown in [<xref ref-type="bibr" rid="scirp.84968-ref8">8</xref>] , we will extract a metapopulation model for HIV dynamics among the youth coupled with awareness/education i.e., we extended the single patch disease model to include multiple patches (see <xref ref-type="fig" rid="fig1">Figure 1</xref>).</p>Differential Equation of the Model<disp-formula id="scirp.84968-formula148"><graphic  xlink:href="//html.scirp.org/file/5-5301501x21.png"  xlink:type="simple"/></disp-formula><p>States variables: S C , susceptible children, S Y U F , susceptible uneducated female youth, S Y U F , susceptible educated female youth, S Y U M , susceptible uneducated male youth, S Y E M , susceptible educated male youth, I C , infected children(children who were infected either during pregnancy or at childbirth), I Y U F , infected uneducated female youth, I Y E F , infected educated female youth, I Y U M , infected uneducated male youth, I Y E M , infected educated male youth, and T Y , antiretroviral therapy treatment among the youths. Parameters: μ , death rate of the youth and children, δ , disease induced rate in the youth and children before ART, δ 1 , disease induced deaths in the youth and children after ART, λ , birth rate, θ , rate of vertical transmission, β 1 , probability a susceptible female youth gets infected by infected male youth, β 2 , probability a susceptible male youth gets infected by infected female youth, φ 1 , rate at which children grow to become uneducated female youth, φ 2 , rate at which children grow to become educated female youths, φ 3 , rate at which children grow to become uneducated male youths, φ 4 , rate at which children grow to become educated male youth, ρ , awareness/education rate, α , rate at which infected youth take the ART. The solid lines represent movement between classes and the dashed lines represent rate at which a susceptible individual moves in to infected class.</p><p>The model answers one important underlying research subjects; the determination of the existence of the threshold parameter which hints on the spreading or dying out of an invading epidemic into a population of susceptible. In this research article, we first study the positivity and boundedness of the system (1.0). The basic reproduction ratio is determined. Applying the hypothetical theorem of the Lyapunov functional, we find out the global stability of the two equilibria for system (1.0). We extend our stability analysis to the stochastic system (5.0), which is obtained by random perturbation of the deterministic system (1.0) and find the stability of its positive equilibrium. Finally, numerical examples which shows the dynamics of systems (1.0) and (5.0) are given, which gives the explicit difference in the dynamics of the models.</p></sec><sec id="s2"><title>2. Basic Properties of the Model</title><p>In this section, the basic properties of model system (1.1) which are useful in the proofs of stability are studied. These are the invariant region and positivity of solutions. The former describes the region in which the solutions of system (1.1) makes biological sense while the latter describes non-negativity of solutions of system (1.1). The model under consideration monitors a human population and as such, we need to have that all the parameters and the variables of the model are positive for all t ≥ 0 .</p><sec id="s2_1"><title>2.1. Positivity of Solutions</title><p>The theory of ordinary differential equations requires that, for every set of initial conditions</p><p>( S Y U F , i 0 , S Y E F , i 0 , S Y U M , i 0 , S Y E M , i 0 , I Y U M , i 0 , I Y E M , i 0 , I Y E F , i 0 , I Y U F , i 0 , T i 0 ) the state variables ( S Y U F , i ( t ) , S Y E F , i ( t ) , S Y U M , i ( t ) , S Y E M , i ( t ) , I Y U M , i ( t ) , I Y E M , i ( t ) , I Y E F , i ( t ) , I Y U F , i ( t ) , T i ( t ) ) of the solution must remain non-negative.</p><p>Proposition 2.1 Let the initial data be</p><p>{ ( S c , i &gt; 0, S Y U F , i &gt; 0, S Y E F , i &gt; 0, S Y U M , i &gt; 0, S Y E M , i &gt; 0, I Y U M , i &gt; 0, I Y E M , i &gt; 0, I Y E F , i &gt; 0, I Y U F , i &gt; 0, T i ) ≥ 0 } ∈ Ω   .</p><p>Then, the solution set</p><p>{ ( S Y U F , i ( t ) , S Y E F , i ( t ) , S Y U M , i ( t ) , S Y E M , i ( t ) , I Y U M , i ( t ) , I Y E M , i ( t ) , I Y E F , i ( t ) , I Y U F , i ( t ) , T i ( t ) ) } of system (1.1) is positive for all t ≥ 0</p><p>Proof. Let α = β 1, i U I Y U M , i N Y U M , i γ = β 1, i E I Y E M , i N Y E M , i From the first equation of model</p><p>system (1.1),</p><p>d S Y U F , i d t = ( 1 − Π ) λ − α S Y U F , i − γ S Y U F , i − ( ρ i + μ i ) S Y U F , i</p><p>That is,</p><p>d S Y U F , i d t ≥ − Π λ − ( α + γ + ρ i + μ i ) S Y U F , i</p><p>Integrating (2.0) by separation of variables gives</p><p>∫ d S S ≥ − ∫ ( Π λ + ( α + γ + ρ i + μ i ) S Y U F , i ) d t</p><p>S ( t ) ≥ S ( 0 ) e − ∫ ( Π λ + ( α + γ + ρ i + μ i ) S Y U F , i ) d t &gt; 0</p><p>This proves that S ( t ) &gt; 0 for all t ≥ 0 . Similarly, it can be shown that the remaining variables of system (1.1) are also positive ∀ t &gt; 0 .</p><p>Remark 2.1. e k &gt; 0 for all k ∈ R .</p></sec><sec id="s2_2"><title>2.2. Invariant Region</title><p>Note that</p><p>d N i d t ≤ 4 λ i − μ i N i − δ 1, i T i ≤ 4 λ i − μ i N i</p><p>We now apply Birkhoff and Rotas theorem on differential inequality (2.1). By separation of variables of differential inequality (2.1), we get</p><p>d N i 4 λ i − μ i N i ≤ d t</p><p>Integrating (2.2) on both sides gives,</p><p>∫ d N i 4 λ i − μ i N i ≤ ∫   d t = − 1 μ ln ( 4 λ i − μ i N i ) + c</p><p>l n ( 4 λ i − μ i N i ) ≥ − μ ( t + c )</p><p>Therefore,</p><p>4 λ i − μ i N i ≥ A e − μ t</p><p>where A is a constant. Now, applying the initial condition N ( 0 ) = N 0 i in (2.3), we get</p><p>A = 4 λ i − μ i N 0 i</p><p>Substituting (2.4) into (2.3) gives</p><p>4 λ i − μ i N i ≥ 4 λ i − μ N 0 i e − μ t</p><p>Making N the subject in (2.5) we have,</p><p>N ≤ 4 λ i μ − ( 4 λ i − μ i N 0 i μ ) e − μ t</p><p>As t → ∞ in (2.6) above, the population size N, approaches</p><p>0 ≤ N ≤ 4 λ i μ ⇒ N → 4 λ i μ</p><p>Therefore, the feasible solutions set of system (2.7) enters the region</p><p>Ω = { ( S Y U F , i , S Y E F , i , S Y U M , i , S Y E M , i , I Y U M , i , I Y E M , i , I Y E F , i , I Y U F , i , T i ) ∈ R + 9 : N i ≤ 4 λ i μ i }</p><p>In this case, whenever N &gt; 4 λ 0 i μ , then d N d t &lt; 0 which means that N → 4 λ 0 i μ . On the other hand, whenever N i ≤ 4 λ 0 i μ i , every solution with initial</p><p>condition in R + 9 remains in that region for t &gt; 0 . Thus, the region is positively-invariant.</p></sec></sec><sec id="s3"><title>3. Basic Reproduction Number</title><p>The basic reproduction ratio ( R 0 ) is defined as an infections originating from an infected individual that invades a population originally of susceptible individuals.</p><p>The above system can be represented in matrix form as I . = f I + v I where f is the matrix of the infection rates and v is the matrix of the transition rates.</p><p>The spectral radius of the Metzler Matrix, ρ ( − F V − 1 ) , is defined as the largest eigenvalue of the Metzler Matrix. Thus:</p><p>ρ ( − F V − 1 ) = | ( − F V − 1 ) − λ I |</p><p>R 1 = β 2, i U ( N Y E M , i + N Y U M , i ) ( ρ i + μ i + δ i ) N Y U F , i</p><disp-formula id="scirp.84968-formula149"><graphic  xlink:href="//html.scirp.org/file/5-5301501x86.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula150"><graphic  xlink:href="//html.scirp.org/file/5-5301501x87.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula151"><graphic  xlink:href="//html.scirp.org/file/5-5301501x88.png"  xlink:type="simple"/></disp-formula><p>If <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/5-5301501x89.png" xlink:type="simple"/></inline-formula> for j = 1, 2, 3, 4, then each infectious individual in Sub-Population j infects on average less than one other person and the disease is likely to die out Otherwise, If <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/5-5301501x90.png" xlink:type="simple"/></inline-formula> for j = 1, 2, 3, 4, then each infectious individual in Sub-Population j infects on average more than one other person; the infection could therefore establish itself in the population and become endemic. An SIR epidemic model, where the presence or absence of an epidemic wave is characterized by the value of<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/5-5301501x91.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. The Global Stability of the Endemic Equilibrium</title><p>In this part, we analyse the global stability of the endemic equilibrium point <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/5-5301501x92.png" xlink:type="simple"/></inline-formula> by construction a appropriate Lyapunov function. For simplicity, we consider the reduced model system (6) to prove for global stability. We use the come up to of [<xref ref-type="bibr" rid="scirp.84968-ref8">8</xref>] as it is used for several complicated epidemiological models. We consider the Lyapunov function of the form</p><disp-formula id="scirp.84968-formula152"><graphic  xlink:href="//html.scirp.org/file/5-5301501x93.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/5-5301501x94.png" xlink:type="simple"/></inline-formula> (for i = 1, 2, ・・・, 6 is a properly chosen positive constant in the given region<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/5-5301501x95.png" xlink:type="simple"/></inline-formula>. is a population of compartment i and <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/5-5301501x96.png" xlink:type="simple"/></inline-formula> is the equilibrium level. So we define the Lyapunov function as</p><disp-formula id="scirp.84968-formula153"><graphic  xlink:href="//html.scirp.org/file/5-5301501x97.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula154"><graphic  xlink:href="//html.scirp.org/file/5-5301501x98.png"  xlink:type="simple"/></disp-formula><p>The time derivative of L is</p><disp-formula id="scirp.84968-formula155"><graphic  xlink:href="//html.scirp.org/file/5-5301501x99.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula156"><graphic  xlink:href="//html.scirp.org/file/5-5301501x100.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula157"><graphic  xlink:href="//html.scirp.org/file/5-5301501x101.png"  xlink:type="simple"/></disp-formula><p>At an endemic equilibrium point <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x102.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.84968-formula158"><graphic  xlink:href="//html.scirp.org/file/5-5301501x103.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula159"><graphic  xlink:href="//html.scirp.org/file/5-5301501x104.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula160"><graphic  xlink:href="//html.scirp.org/file/5-5301501x105.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula161"><graphic  xlink:href="//html.scirp.org/file/5-5301501x106.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula162"><graphic  xlink:href="//html.scirp.org/file/5-5301501x107.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula163"><graphic  xlink:href="//html.scirp.org/file/5-5301501x108.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.84968-formula164"><graphic  xlink:href="//html.scirp.org/file/5-5301501x109.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula165"><graphic  xlink:href="//html.scirp.org/file/5-5301501x110.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula166"><graphic  xlink:href="//html.scirp.org/file/5-5301501x111.png"  xlink:type="simple"/></disp-formula><p>Simplification yields</p><disp-formula id="scirp.84968-formula167"><graphic  xlink:href="//html.scirp.org/file/5-5301501x112.png"  xlink:type="simple"/></disp-formula><p>let<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x113.png" xlink:type="simple"/></inline-formula>, where</p><disp-formula id="scirp.84968-formula168"><graphic  xlink:href="//html.scirp.org/file/5-5301501x114.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula169"><graphic  xlink:href="//html.scirp.org/file/5-5301501x115.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula170"><graphic  xlink:href="//html.scirp.org/file/5-5301501x116.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula171"><graphic  xlink:href="//html.scirp.org/file/5-5301501x117.png"  xlink:type="simple"/></disp-formula><p>F is non-positive by following the approach of [<xref ref-type="bibr" rid="scirp.84968-ref9">9</xref>] . Thus, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x118.png" xlink:type="simple"/></inline-formula>for</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x119.png" xlink:type="simple"/></inline-formula>. Hence <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x120.png" xlink:type="simple"/></inline-formula> and is zero when<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x121.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x122.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x123.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x124.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x125.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x126.png" xlink:type="simple"/></inline-formula>. Therefore, the largest</p><p>invariant set in <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x127.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x128.png" xlink:type="simple"/></inline-formula> is the singleton <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x129.png" xlink:type="simple"/></inline-formula> which is our</p><p>endemic equilibrium point. By LaSalles invariant principle [<xref ref-type="bibr" rid="scirp.84968-ref9">9</xref>] we conclude that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x130.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable (g.a.s). Thus, we establish the following theory.</p><p>Theorem 3.1 When<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x131.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x132.png" xlink:type="simple"/></inline-formula>the endemic equilibrium point <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x133.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable in<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x134.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s5"><title>5. The Stochastic Model</title><p>Stochastic perturbations were bring in some of the major parameters involved in the model equations.</p><p>Here, we bring in stochastic perturbations in the major parameters of the deterministic model (1.1). Thus we permit stochastic perturbations of the variable</p><disp-formula id="scirp.84968-formula172"><graphic  xlink:href="//html.scirp.org/file/5-5301501x135.png"  xlink:type="simple"/></disp-formula><p>around their values at positive equilibrium<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x136.png" xlink:type="simple"/></inline-formula>. Hence, we assume that the white noise of the stochastic perturbations of the variable around values of are proportional to the distances of</p><disp-formula id="scirp.84968-formula173"><graphic  xlink:href="//html.scirp.org/file/5-5301501x137.png"  xlink:type="simple"/></disp-formula><p>from</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x138.png" xlink:type="simple"/></inline-formula>Hence the stochastic version of model (1.1) is</p><disp-formula id="scirp.84968-formula174"><graphic  xlink:href="//html.scirp.org/file/5-5301501x139.png"  xlink:type="simple"/></disp-formula><p>With <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x140.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x141.png" xlink:type="simple"/></inline-formula> are real constants, and</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x142.png" xlink:type="simple"/></inline-formula>are independent wiener processes. We examine the asymptotic stability behavior of the equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x143.png" xlink:type="simple"/></inline-formula> of the stochastic equation (5.0) and contrast results with the deterministic model (1.1).</p>Stochastic Stability of the Positive Equilibrium<p>It can be shown clearly that, the deterministic model (1.1) has one disease-free equilibrium</p><disp-formula id="scirp.84968-formula175"><graphic  xlink:href="//html.scirp.org/file/5-5301501x144.png"  xlink:type="simple"/></disp-formula><p>which is globally asymptotically stable when<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x145.png" xlink:type="simple"/></inline-formula>. However, when<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x146.png" xlink:type="simple"/></inline-formula>, the disease-free equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x147.png" xlink:type="simple"/></inline-formula> is unstable. Obviously, there is also a unique positive endemic equilibrium</p><disp-formula id="scirp.84968-formula176"><graphic  xlink:href="//html.scirp.org/file/5-5301501x148.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula177"><graphic  xlink:href="//html.scirp.org/file/5-5301501x149.png"  xlink:type="simple"/></disp-formula><p>This equilibrium is globally asymptotically stable. The stochastic system (5.0) has the similar equilibria as the deterministic system (1.1). Assuming that<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x150.png" xlink:type="simple"/></inline-formula>, we examine the stability of the endemic equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x151.png" xlink:type="simple"/></inline-formula> of (5.0). The stochastic differential equation (5.0) can be centered at its positive equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x152.png" xlink:type="simple"/></inline-formula> by the change of variables</p><disp-formula id="scirp.84968-formula178"><graphic  xlink:href="//html.scirp.org/file/5-5301501x153.png"  xlink:type="simple"/></disp-formula><p>The linearized system of the stochastic model (5.0) around <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x154.png" xlink:type="simple"/></inline-formula> takes the form</p><disp-formula id="scirp.84968-formula179"><graphic  xlink:href="//html.scirp.org/file/5-5301501x155.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.84968-formula180"><graphic  xlink:href="//html.scirp.org/file/5-5301501x156.png"  xlink:type="simple"/></disp-formula><p>and equals</p><disp-formula id="scirp.84968-formula181"><graphic  xlink:href="//html.scirp.org/file/5-5301501x157.png"  xlink:type="simple"/></disp-formula><p>Clearly, the endemic equilibrium <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x158.png" xlink:type="simple"/></inline-formula> corresponds to the trivial solution <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x159.png" xlink:type="simple"/></inline-formula> in (5.2). We denote L to be the differential operator associated with (5.2), defined for the family of nonnegative functions <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x160.png" xlink:type="simple"/></inline-formula> such that it is continuously differentiable with respect to t and twice with respect to x.</p><p>According to Afanas ev et al. [<xref ref-type="bibr" rid="scirp.84968-ref9">9</xref>] , the differential operator L for a function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x161.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.84968-formula182"><graphic  xlink:href="//html.scirp.org/file/5-5301501x162.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.84968-formula183"><graphic  xlink:href="//html.scirp.org/file/5-5301501x163.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.84968-formula184"><graphic  xlink:href="//html.scirp.org/file/5-5301501x164.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x165.png" xlink:type="simple"/></inline-formula>, “T” and “Tr” are the transposition and trace respectively. With reference to Afanas?? ev et al. [<xref ref-type="bibr" rid="scirp.84968-ref9">9</xref>] , the following results hold.</p><p>Theorem 5.1: Suppose a function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x166.png" xlink:type="simple"/></inline-formula> exist, satisfying the following inequalities</p><disp-formula id="scirp.84968-formula185"><graphic  xlink:href="//html.scirp.org/file/5-5301501x167.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula186"><graphic  xlink:href="//html.scirp.org/file/5-5301501x168.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x169.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x170.png" xlink:type="simple"/></inline-formula>. Then the trivial solution of (5.2) is p<sup>th</sup> moment exponentially stable. Again, given that p = 2 the trivial solution is supposed to be exponentially stable in mean square and the equilibrium x = 0 is globally asymptotically stable. From theorem 5.1, the conditions for stochastic asymptotic stability of trivial solution of (5.0) are given theorem 5.2.</p><p>Theorem 5.2: Suppose</p><disp-formula id="scirp.84968-formula187"><graphic  xlink:href="//html.scirp.org/file/5-5301501x171.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula188"><graphic  xlink:href="//html.scirp.org/file/5-5301501x172.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula189"><graphic  xlink:href="//html.scirp.org/file/5-5301501x173.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula190"><graphic  xlink:href="//html.scirp.org/file/5-5301501x174.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula191"><graphic  xlink:href="//html.scirp.org/file/5-5301501x175.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula192"><graphic  xlink:href="//html.scirp.org/file/5-5301501x176.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula193"><graphic  xlink:href="//html.scirp.org/file/5-5301501x177.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula194"><graphic  xlink:href="//html.scirp.org/file/5-5301501x178.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula195"><graphic  xlink:href="//html.scirp.org/file/5-5301501x179.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula196"><graphic  xlink:href="//html.scirp.org/file/5-5301501x180.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula197"><graphic  xlink:href="//html.scirp.org/file/5-5301501x181.png"  xlink:type="simple"/></disp-formula><p>and hold, then the zero solution of (5.0) is asymptotically mean square stable.</p><p>Proof: We consider the Lyapunov</p><disp-formula id="scirp.84968-formula198"><graphic  xlink:href="//html.scirp.org/file/5-5301501x182.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x183.png" xlink:type="simple"/></inline-formula> non-negative constants that will be chosen in the course of the proof. It can be easily ascertained that inequality (5.4) hold true when <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x184.png" xlink:type="simple"/></inline-formula> Applying the operator L on <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x185.png" xlink:type="simple"/></inline-formula> gives</p><disp-formula id="scirp.84968-formula199"><graphic  xlink:href="//html.scirp.org/file/5-5301501x186.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula200"><graphic  xlink:href="//html.scirp.org/file/5-5301501x187.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula201"><graphic  xlink:href="//html.scirp.org/file/5-5301501x188.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula202"><graphic  xlink:href="//html.scirp.org/file/5-5301501x189.png"  xlink:type="simple"/></disp-formula><p>Further</p><disp-formula id="scirp.84968-formula203"><graphic  xlink:href="//html.scirp.org/file/5-5301501x190.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula204"><graphic  xlink:href="//html.scirp.org/file/5-5301501x191.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula205"><graphic  xlink:href="//html.scirp.org/file/5-5301501x192.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula206"><graphic  xlink:href="//html.scirp.org/file/5-5301501x193.png"  xlink:type="simple"/></disp-formula><p>Now remark that</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x194.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x195.png" xlink:type="simple"/></inline-formula></p><p>with</p><disp-formula id="scirp.84968-formula207"><graphic  xlink:href="//html.scirp.org/file/5-5301501x196.png"  xlink:type="simple"/></disp-formula><p>Now, from Equation (5.5), if we choose</p><disp-formula id="scirp.84968-formula208"><graphic  xlink:href="//html.scirp.org/file/5-5301501x197.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula209"><graphic  xlink:href="//html.scirp.org/file/5-5301501x198.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula210"><graphic  xlink:href="//html.scirp.org/file/5-5301501x199.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula211"><graphic  xlink:href="//html.scirp.org/file/5-5301501x200.png"  xlink:type="simple"/></disp-formula><p>and then from Equation (5.5), it is easy to verify that,</p><disp-formula id="scirp.84968-formula212"><graphic  xlink:href="//html.scirp.org/file/5-5301501x201.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.84968-formula213"><graphic  xlink:href="//html.scirp.org/file/5-5301501x202.png"  xlink:type="simple"/></disp-formula><p>From the assumptions of the theorem, we deduce that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula>. Hence, D is a symmetric positive definite matrix. Let <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula> denote the minimum of its eleven positive eigenvalues<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x207.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x208.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x209.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x210.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic 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xlink:href="//html.scirp.org/file/5-5301501x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x214.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x215.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x216.png" xlink:type="simple"/></inline-formula>; then,we can easily get</p><disp-formula id="scirp.84968-formula214"><graphic  xlink:href="//html.scirp.org/file/5-5301501x217.png"  xlink:type="simple"/></disp-formula><p>According to Theorem 5.1, we conclude that the trivial solution of stochastic system is globally asymptotically stable.</p><p>Hence, according to theorem 5.1, the proof is completed.</p></sec><sec id="s6"><title>6. Conclusion</title><p>In this article, the dynamics of deterministic epidemic model and its stochastic variant are presented. The stability analyses of the deterministic model were investigated. Suitable Lyapunov functions were constructed for the global stability of the two equilibria. Mathematical analysis was done and it was established that in the absence of the disease a disease free equilibrium will always exist if <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x218.png" xlink:type="simple"/></inline-formula> for j = 1, 2, 3, 4,. We also established that the endemic equilibrium exists in the presence of the disease that is when <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x219.png" xlink:type="simple"/></inline-formula> for j = 1, 2, 3, 4, with the infectious population greater than zero. Reducing the infection in the vector population reduces <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x219.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x220.png" xlink:type="simple"/></inline-formula> for j = 1, 2, 3, 4, greatly. Thus the best methods of controlling HIV transmission is to target the Infected uneducated female youth, Infected educated female youth, Infected uneducated male youth, Infected educated male youth. <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x219.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/5-5301501x221.png" xlink:type="simple"/></inline-formula>is a threshold that completely determines the global dynamics of disease transmission. Our major purpose of the study was to examine the asymptotic stability behavior of the endemic equilibrium of the stochastic version of the deterministic epidemic model in Metapopulation setting.</p></sec><sec id="s7"><title>Conflict of Interest</title><p>The author(s) declare(s) that there is no conflict of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Kelkile, D.P. (2018) Stability Analysis and Stochastic SI Modelling of Endemic Diseases. Advances in Pure Mathematics, 8, 516-534. https://doi.org/10.4236/apm.2018.85030</p></sec></body><back><ref-list><title>References</title><ref id="scirp.84968-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Damian, C. (2005) A Stochastic SIS Infection Model Incorporating Indirect Transmission. 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