<?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">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1102040</article-id><article-id pub-id-type="publisher-id">OALibJ-68815</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Qualitative Analysis of a Rumor Transmission Model with Incubation Mechanism
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Salma</surname><given-names>Al-Tuwairqi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sarah</surname><given-names>Al-Sheikh</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Reem</surname><given-names>Al-Amoudi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, King Abdulaziz University, Jeddah, Saudi Arabia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>saltuwairqi@kau.edu.sa(SA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>30</day><month>11</month><year>2015</year></pub-date><volume>02</volume><issue>11</issue><fpage>1</fpage><lpage>12</lpage><history><date date-type="received"><day>19</day>	<month>October</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>5</month>	<year>November</year>	</date><date date-type="accepted"><day>11</day>	<month>November</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 propose a rumor transmission model with incubation period considering the fact that incubators may move to stifler class and susceptibles may move to spreader class. The model is formulated with constant recruitment and varying total population. The full system of the model is studied qualitatively producing rumor-free and rumor-existence equilibriums. The existence conditions of the equilibriums are investigated. Moreover, the local and global stability analysis of both equilibriums is examined. Furthermore, numerical simulations are used to support the qualitative analysis. Finally, the impact of different management strategies on the dissipation of rumors is analyzed numerically by varying key parameters in the model. 
  
 
</p></abstract><kwd-group><kwd>Rumor Transmission Model</kwd><kwd> Local Stability Analysis</kwd><kwd> Global Stability Analysis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Rumors disseminate easily these days with expanding social networks. Although rumors are neither true nor false, this does not stop some individuals from spreading it any way before searching for some kind of con- firmation. Transmission of rumors has a major impact on human lives. It may have negative sides such as causing panic and chaos in emergency events or destroying credibility of someone or something. On the other hand, it may create awareness and draw public attention to take action. As a result, great importance lies in studying the dynamics of rumor propagation.</p><p>Researchers have applied epidemiological models to study the dynamics of social systems. Daley and kendall are among the earliest researchers to propose a rumor spread model that has some properties in common with epidemic model [<xref ref-type="bibr" rid="scirp.68815-ref1">1</xref>] . Also Cane [<xref ref-type="bibr" rid="scirp.68815-ref2">2</xref>] showed the similarity among the deterministic forms of models for the spread of an epidemic and of a rumor. This is based on the fact that both biological diseases and social behavior are a result from interactions between individuals. The model in [<xref ref-type="bibr" rid="scirp.68815-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.68815-ref2">2</xref>] divided the population into three disjoint classes of individuals: susceptible, describing people who had not yet been exposed to a particular rumor; infective, referring to people who spread the rumor through social interactions; and recovered, meaning people who had experienced the rumor, but had no interest in spreading it or had lost interest at some point.</p><p>At the beginning of this century, several mathematical models are proposed considering different dynamics of rumor and idea transmission. Thompson et al. [<xref ref-type="bibr" rid="scirp.68815-ref3">3</xref>] explored a model for the dynamics of rumor spreading in chat rooms. Bettencourt et al. [<xref ref-type="bibr" rid="scirp.68815-ref4">4</xref>] applied models similar to epidemiology to study the spread of ideas. Kawachi [<xref ref-type="bibr" rid="scirp.68815-ref5">5</xref>] and Kawachi et al. [<xref ref-type="bibr" rid="scirp.68815-ref6">6</xref>] proposed deterministic models for rumor transmission and explored the effects of various contact interactions among three classes: susceptible (ignorant about the rumor), spreader (spread the rumor) and stifler (don’t spread the rumor). Later, Al-Amoudi et al. [<xref ref-type="bibr" rid="scirp.68815-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.68815-ref8">8</xref>] adopted the models in [<xref ref-type="bibr" rid="scirp.68815-ref5">5</xref>] to study the dynamics of constant and variable meme propagation with a comprehensive qualitative analyses. Also, they proposed a model to examine the impact of stiflers on the transmissions of memes in [<xref ref-type="bibr" rid="scirp.68815-ref9">9</xref>] . Wang and Wood [<xref ref-type="bibr" rid="scirp.68815-ref10">10</xref>] adopted an epidemiological approach to model viral meme propagation. Piqueira [<xref ref-type="bibr" rid="scirp.68815-ref11">11</xref>] examined an equilibrium study of a rumor spreading model according to propagation parameters and initial conditions. Furthermore, Huang [<xref ref-type="bibr" rid="scirp.68815-ref12">12</xref>] established two models for rumor spreading process with denial and skepticism. Recently, Zhao et al. proposed rumor spreading models in social networks considering the forgetting [<xref ref-type="bibr" rid="scirp.68815-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.68815-ref14">14</xref>] and refuting [<xref ref-type="bibr" rid="scirp.68815-ref15">15</xref>] mechanism of spreaders. Moreover, Zan et al. [<xref ref-type="bibr" rid="scirp.68815-ref16">16</xref>] examined the dynamics or rumor spread with counterattack mechanism and self-resistance parameter. Huo et al. [<xref ref-type="bibr" rid="scirp.68815-ref17">17</xref>] investigated the psychological effect with rumor spreading in emergency event. In addition, Afassinou [<xref ref-type="bibr" rid="scirp.68815-ref18">18</xref>] analyzed the impact of education rate on rumor final size. Zhao and Wang [<xref ref-type="bibr" rid="scirp.68815-ref19">19</xref>] established a dynamic rumor model considering the medium as a new subclass. Later, they refined the model by adding another subclass for government measures to control rumor propagation [<xref ref-type="bibr" rid="scirp.68815-ref20">20</xref>] . Also, they examined a model of information transmission with isolation [<xref ref-type="bibr" rid="scirp.68815-ref21">21</xref>] . Zhao et al. investigated a rumor model by extending a new class named hibernators. This class refers to spreaders who enter it due to forgetting mechanism and later leave it to become spreaders again due to remembering mechanism. They studied the model in homogeneous [<xref ref-type="bibr" rid="scirp.68815-ref22">22</xref>] and inhomogeneous [<xref ref-type="bibr" rid="scirp.68815-ref23">23</xref>] networks.</p><p>The above rumor models do not consider the fact that an individual may take time before accepting or rejecting what they hear or read. Some individuals think about rumors for some time before they become spreaders or stiflers. This period is called rumor incubation time. Huo et al. [<xref ref-type="bibr" rid="scirp.68815-ref24">24</xref>] introduced incubation class in studying rumor spreading model. They assumed that ignorants (susceptibles) entered first incubation class as a result of spreader and incubator contact. After some time the incubators become either spreaders or stiflers. But they overlook the option that ignorants may move directly to the spreader class. They examined qualitatively the limiting dynamical system of the model. Later, Chen et al. [<xref ref-type="bibr" rid="scirp.68815-ref25">25</xref>] proposed another rumor transmission model with latent class. They assumed that ignorants might move at first to three classes: latent, spreader and stifler. However, the possibility that latents may move to stifler class after the latent period is ignored in the model. They also qualitatively studied the limiting system of the model. In this paper, we propose a rumor propagation model with incubation mechanism that accommodates for both possibilities: incubators move to stifler class and susceptibles move to spreader class. In reality, not all individuals seek more information to ascertain the validity of a rumor before spreading it. At the same time, when some individuals do seek authenticity of a rumor, they may find it false or not worth spreading. Our aim here is to investigate the full dynamics of the model system using qualitative theory to have a better understanding and acquire more insight on the key parameters for controlling the dissipation of rumors. The rest of this paper is organized as follows. We describe the formulation of the proposed rumor transmission model with incubation mechanism and examine the existence of equilibriums and basic reproduction number in Section 2. In Section 3, we analyze the model system qualitatively and derive the local and global stability conditions for the equilibriums. In Section 4, we illustrate numerical simulations of the model and discuss the parameters that have impacts on the cessation of rumors. Finally, a brief conclusion is given in Section 5.</p></sec><sec id="s2"><title>2. Mathematical Model</title><p>We consider a variable population size at any time t and denote it by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x7.png" xlink:type="simple"/></inline-formula>. We divide the population into four disjoint classes of individuals: Susceptible, Incubator, Spreader, and Stifler denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x8.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x10.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x11.png" xlink:type="simple"/></inline-formula>, respectively.</p><p>The susceptible class<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x12.png" xlink:type="simple"/></inline-formula>, describes people who have not yet been exposed to a particular rumor. The incubator class<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x13.png" xlink:type="simple"/></inline-formula>, refers to people who are thinking about the rumor, but has not taken any action towards it. The spreader class<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x14.png" xlink:type="simple"/></inline-formula>, refers to people who take an active interest in the idea or concept that a rumor represents, and therefore have a tendency to talk about the rumor in social interactions. The stifler class<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x15.png" xlink:type="simple"/></inline-formula>, indicates people who have experienced the rumor, but have no interest or have lost interest at some point. The mathematical model is illustrated in the transfer diagram (<xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the dynamics of the model are based on the following assumptions. The rumor is constant, that is, the same rumor is being propagated throughout the classes at all times. Individuals are recruited through the susceptible class and it occurs at a positive constant B, namely immigration constant. They leave each class at the same emigration rate,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x16.png" xlink:type="simple"/></inline-formula>. A susceptible know about the rumor when contacting a spreader at a rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x17.png" xlink:type="simple"/></inline-formula>, namely transmitting rate, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x18.png" xlink:type="simple"/></inline-formula> such that c is the average number of contact per unit time and q is the probability of transmitting the rumor. After knowing about the rumor from a spreader, some susceptibles with probability <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x19.png" xlink:type="simple"/></inline-formula> experience an incubation period and move to incubation class. However, other susceptibles with probability <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x20.png" xlink:type="simple"/></inline-formula> believe the rumor and start spreading it immediately without any confirmation and move to spreader class. During the incubation period, the incubators try to think about the rumor and acquire more information to decide whether, on the one hand, the rumor is valid or not, and on the other hand, is it worth spreading or not. Based on the incubators judgement, they either move to spreader class at a rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x21.png" xlink:type="simple"/></inline-formula>, namely spreading rate, or move to stifler class at a rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x22.png" xlink:type="simple"/></inline-formula>, namely stifling rate. At any time, a spreader may lose interest in spreading the rumor, as a result becomes a stifler at a rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x23.png" xlink:type="simple"/></inline-formula>, namely removed rate. All rates are positive constants.</p><p>Taking the above considerations, the model is described according to the dynamic theory by the following nonlinear system of ordinary differential equations:</p><disp-formula id="scirp.68815-formula1248"><graphic  xlink:href="http://html.scirp.org/file/68815x24.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1249"><graphic  xlink:href="http://html.scirp.org/file/68815x25.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1250"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68815x26.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1251"><graphic  xlink:href="http://html.scirp.org/file/68815x27.png"  xlink:type="simple"/></disp-formula><p>Note that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x28.png" xlink:type="simple"/></inline-formula>. It follows from system (1) that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x29.png" xlink:type="simple"/></inline-formula> which can be solved easily to give <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x30.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x31.png" xlink:type="simple"/></inline-formula> and therefore, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x32.png" xlink:type="simple"/></inline-formula>. Thus, the considered region for system (1) is</p><disp-formula id="scirp.68815-formula1252"><graphic  xlink:href="http://html.scirp.org/file/68815x33.png"  xlink:type="simple"/></disp-formula><p>The vector field points into the interior of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x34.png" xlink:type="simple"/></inline-formula> on the part of its boundary when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x35.png" xlink:type="simple"/></inline-formula> Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x36.png" xlink:type="simple"/></inline-formula>is positively invariant, i.e., every solution of system (1), with initial conditions in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x37.png" xlink:type="simple"/></inline-formula> remains there for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x38.png" xlink:type="simple"/></inline-formula>.</p><p>To find the equilibriums of system (1), we set the rates in (1) to zero:</p><disp-formula id="scirp.68815-formula1253"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68815x39.png"  xlink:type="simple"/></disp-formula><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The flowchart of rumor spreading model with incuba- tion mechanism.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/68815x40.png"/></fig></fig-group><disp-formula id="scirp.68815-formula1254"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68815x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1255"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68815x42.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1256"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68815x43.png"  xlink:type="simple"/></disp-formula><p>The model has a rumor free equilibrium if there are no spreaders and no incubators, that is, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x44.png" xlink:type="simple"/></inline-formula>, which means that the rumor dies out. By solving Equations (2)-(5), we find that the rumor free equilibrium is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x45.png" xlink:type="simple"/></inline-formula>. Before obtaining the other equilibriums, we first find the basic reproduction number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x46.png" xlink:type="simple"/></inline-formula> using the method of next generation matrix [<xref ref-type="bibr" rid="scirp.68815-ref26">26</xref>] . Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x47.png" xlink:type="simple"/></inline-formula> is defined as the expected number of secondary cases of rumor spreaders produced by a single spreader. The basic reproduction number plays a significant role when designing control intervention for a system. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x48.png" xlink:type="simple"/></inline-formula> then system (1) can be written as:</p><disp-formula id="scirp.68815-formula1257"><graphic  xlink:href="http://html.scirp.org/file/68815x49.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.68815-formula1258"><graphic  xlink:href="http://html.scirp.org/file/68815x50.png"  xlink:type="simple"/></disp-formula><p>The Jacobian matrices of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x51.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x52.png" xlink:type="simple"/></inline-formula> at the rumor free equilibrium point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x53.png" xlink:type="simple"/></inline-formula>, are</p><disp-formula id="scirp.68815-formula1259"><graphic  xlink:href="http://html.scirp.org/file/68815x54.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1260"><graphic  xlink:href="http://html.scirp.org/file/68815x55.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x56.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x57.png" xlink:type="simple"/></inline-formula>.</p><p>Thus the next generation matrix is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x58.png" xlink:type="simple"/></inline-formula> Hence, the basic reproduction number of system (1) is the spectral radius of matrix<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x59.png" xlink:type="simple"/></inline-formula>, that is, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x60.png" xlink:type="simple"/></inline-formula></p><p>Next, we solve Equations (2)-(5) to find a positive (rumor existence) equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x61.png" xlink:type="simple"/></inline-formula> of system (1). From Equation (2), (3) and (5) we find that:</p><disp-formula id="scirp.68815-formula1261"><graphic  xlink:href="http://html.scirp.org/file/68815x62.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1262"><graphic  xlink:href="http://html.scirp.org/file/68815x63.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1263"><graphic  xlink:href="http://html.scirp.org/file/68815x64.png"  xlink:type="simple"/></disp-formula><p>Substituting for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x65.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x66.png" xlink:type="simple"/></inline-formula> in Equation (4), we get:</p><disp-formula id="scirp.68815-formula1264"><graphic  xlink:href="http://html.scirp.org/file/68815x67.png"  xlink:type="simple"/></disp-formula><p>The non trivial root of the above equation is: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x68.png" xlink:type="simple"/></inline-formula>In terms of the basic reproduction number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x69.png" xlink:type="simple"/></inline-formula>is rewritten as:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x70.png" xlink:type="simple"/></inline-formula>. So, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x71.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x72.png" xlink:type="simple"/></inline-formula> which means that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x73.png" xlink:type="simple"/></inline-formula> does not exist biologically.</p><p>Theorem 1 System (1) has two equilibria: the rumor free equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x74.png" xlink:type="simple"/></inline-formula> which exists always; and the rumor existence equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x75.png" xlink:type="simple"/></inline-formula> which exists if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x76.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. Stability Analysis</title><sec id="s3_1"><title>3.1. Local Stability</title><p>Here we investigate the local stability of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x77.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x78.png" xlink:type="simple"/></inline-formula> using linearization method [<xref ref-type="bibr" rid="scirp.68815-ref27">27</xref>] and matrix analysis [<xref ref-type="bibr" rid="scirp.68815-ref28">28</xref>] . We state the following theorems:</p><p>Theorem 2 (stability of E<sub>0</sub>) If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x80.png" xlink:type="simple"/></inline-formula>, the rumor free equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x81.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x82.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x83.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x84.png" xlink:type="simple"/></inline-formula>is locally stable. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x85.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x86.png" xlink:type="simple"/></inline-formula>is unstable.</p><p>Proof. Linearizing system (1) (by linearization method [<xref ref-type="bibr" rid="scirp.68815-ref27">27</xref>] ) we obtain the Jacobian matrix evaluated at the equilibrium<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x87.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.68815-formula1265"><graphic  xlink:href="http://html.scirp.org/file/68815x88.png"  xlink:type="simple"/></disp-formula><p>Clearly the eigenvalues of the characteristic equation [<xref ref-type="bibr" rid="scirp.68815-ref28">28</xref>] are: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x89.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x90.png" xlink:type="simple"/></inline-formula> satisfy the equation</p><disp-formula id="scirp.68815-formula1266"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/68815x91.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.68815-formula1267"><graphic  xlink:href="http://html.scirp.org/file/68815x92.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1268"><graphic  xlink:href="http://html.scirp.org/file/68815x93.png"  xlink:type="simple"/></disp-formula><p>Based on Routh-Hurwitz Criteria [<xref ref-type="bibr" rid="scirp.68815-ref28">28</xref>] , Equation (6) has two negative eigenvalues if both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x94.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x95.png" xlink:type="simple"/></inline-formula>. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x96.png" xlink:type="simple"/></inline-formula>, that is, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x97.png" xlink:type="simple"/></inline-formula>Then also <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x98.png" xlink:type="simple"/></inline-formula>. Now, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x99.png" xlink:type="simple"/></inline-formula>, then</p><disp-formula id="scirp.68815-formula1269"><graphic  xlink:href="http://html.scirp.org/file/68815x100.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1270"><graphic  xlink:href="http://html.scirp.org/file/68815x101.png"  xlink:type="simple"/></disp-formula><p>Simplifying<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x102.png" xlink:type="simple"/></inline-formula>, we have:</p><disp-formula id="scirp.68815-formula1271"><graphic  xlink:href="http://html.scirp.org/file/68815x103.png"  xlink:type="simple"/></disp-formula><p>Therefore, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula> and the eigenvalues <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula> have negative real parts. So, all eigenvalues have negative real part if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula>, and hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula>is locally asymptotically stable. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x112.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x113.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x114.png" xlink:type="simple"/></inline-formula>, thus <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x115.png" xlink:type="simple"/></inline-formula> is locally stable. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x116.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x117.png" xlink:type="simple"/></inline-formula>, therefore <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x118.png" xlink:type="simple"/></inline-formula> is unstable.</p><p>Theorem 3 (stability of E<sup>*</sup>) The rumor existence equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x119.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x120.png" xlink:type="simple"/></inline-formula></p><p>Proof. Linearizing system (1) at the equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x121.png" xlink:type="simple"/></inline-formula> gives</p><disp-formula id="scirp.68815-formula1272"><graphic  xlink:href="http://html.scirp.org/file/68815x122.png"  xlink:type="simple"/></disp-formula><p>The eigenvalues of the characteristic equation are: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x123.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x124.png" xlink:type="simple"/></inline-formula> satisfy the equation</p><disp-formula id="scirp.68815-formula1273"><graphic  xlink:href="http://html.scirp.org/file/68815x125.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.68815-formula1274"><graphic  xlink:href="http://html.scirp.org/file/68815x126.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1275"><graphic  xlink:href="http://html.scirp.org/file/68815x127.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1276"><graphic  xlink:href="http://html.scirp.org/file/68815x128.png"  xlink:type="simple"/></disp-formula><p>From (4), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x129.png" xlink:type="simple"/></inline-formula>since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x130.png" xlink:type="simple"/></inline-formula> Moreover, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x131.png" xlink:type="simple"/></inline-formula> if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x132.png" xlink:type="simple"/></inline-formula> Therefore, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x133.png" xlink:type="simple"/></inline-formula>Now,</p><disp-formula id="scirp.68815-formula1277"><graphic  xlink:href="http://html.scirp.org/file/68815x134.png"  xlink:type="simple"/></disp-formula><p>If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x135.png" xlink:type="simple"/></inline-formula> then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x136.png" xlink:type="simple"/></inline-formula>. Hence by Routh-Hurwitz Criteria [<xref ref-type="bibr" rid="scirp.68815-ref29">29</xref>] <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x137.png" xlink:type="simple"/></inline-formula>have negative real parts if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x138.png" xlink:type="simple"/></inline-formula> Thus, all eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x139.png" xlink:type="simple"/></inline-formula> have negative real parts. Consequently <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x140.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable.</p></sec><sec id="s3_2"><title>3.2. Global Stability</title><p>First, we explore the global stability of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula>. Consider the Lyapunov function [<xref ref-type="bibr" rid="scirp.68815-ref30">30</xref>] : <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula>Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula> and we have, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x146.png" xlink:type="simple"/></inline-formula>if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x147.png" xlink:type="simple"/></inline-formula>. Moreover, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x148.png" xlink:type="simple"/></inline-formula> is non-negative, it follows that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x149.png" xlink:type="simple"/></inline-formula> if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x150.png" xlink:type="simple"/></inline-formula>; with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x151.png" xlink:type="simple"/></inline-formula> if and only if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x152.png" xlink:type="simple"/></inline-formula>.</p><p>Hence, the only solution of system (1) in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x153.png" xlink:type="simple"/></inline-formula> on which <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x154.png" xlink:type="simple"/></inline-formula> is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x155.png" xlink:type="simple"/></inline-formula>. Therefore, by LaSalle’s Invariance Principle [<xref ref-type="bibr" rid="scirp.68815-ref30">30</xref>] , every solution of system (1), with initial conditions in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x156.png" xlink:type="simple"/></inline-formula>, approaches <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x157.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x158.png" xlink:type="simple"/></inline-formula>. Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x159.png" xlink:type="simple"/></inline-formula>is globally asymptotically stable and we can state the following theorem.</p><p>Theorem 4 (stability of E<sub>0</sub>) If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x160.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x161.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x162.png" xlink:type="simple"/></inline-formula>.</p><p>Next, we examine the global stability of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x163.png" xlink:type="simple"/></inline-formula>. Consider the Lyapunov function [<xref ref-type="bibr" rid="scirp.68815-ref30">30</xref>] :</p><disp-formula id="scirp.68815-formula1278"><graphic  xlink:href="http://html.scirp.org/file/68815x164.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68815-formula1279"><graphic  xlink:href="http://html.scirp.org/file/68815x165.png"  xlink:type="simple"/></disp-formula><p>Here, we used<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x166.png" xlink:type="simple"/></inline-formula>. Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x167.png" xlink:type="simple"/></inline-formula>is globally stable and we can state the following theorem.</p><p>Theorem 5 (stability of E<sup>*</sup>) The rumor existence equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x168.png" xlink:type="simple"/></inline-formula> is globally stable.</p><p>We summarize the result of this section as follows:</p><p>• If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x169.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x170.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x171.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x172.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x173.png" xlink:type="simple"/></inline-formula> is globally asymp- totically stable and in this case <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x174.png" xlink:type="simple"/></inline-formula> does not exist.</p><p>• If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x175.png" xlink:type="simple"/></inline-formula> then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x176.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable. It is globally stable unconditionally whenever it exists.</p></sec></sec><sec id="s4"><title>4. Discussions and Simulation</title><p>In this section, we illustrate numerical simulations of system (1) to support the qualitative analysis. Furthermore, we examine key parameters that may contribute in controlling the spread of rumors.</p><p>Numerical simulations of system (1), with different initial conditions, show that the rumor disappears at an equilibrium level <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x177.png" xlink:type="simple"/></inline-formula> when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x178.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x179.png" xlink:type="simple"/></inline-formula> (<xref ref-type="fig" rid="fig2">Figure 2</xref>). However, the rumor persists at an equilibrium level <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x180.png" xlink:type="simple"/></inline-formula> when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x181.png" xlink:type="simple"/></inline-formula> (<xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>In reality, rumors prevail if there exist many spreaders. Therefore, It is clear that the parameters: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x182.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x183.png" xlink:type="simple"/></inline-formula> in system (1) may affect the size of the spreader class. To have a better understanding of the role of these parameters, we carry out numerical simulations by varying only one parameter to see its impact on the spread of a rumor. These investigations give more insight on useful management strategies to control the dissipation of a rumor.</p><p>By varying the transmitting rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x184.png" xlink:type="simple"/></inline-formula> and holding all other parameters at a fixed value, we can see in <xref ref-type="fig" rid="fig4">Figure 4</xref> the changes in the size of the spreader class over time. It is clear that the lower the transmitting rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x185.png" xlink:type="simple"/></inline-formula>, the smaller the size of the spreader class. With a lower <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x186.png" xlink:type="simple"/></inline-formula> value, fewer susceptibles become spreaders and incubators. This means that the chances of a spreader having contact with susceptibles is small. Therefore, the</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x189.png" xlink:type="simple"/></inline-formula>.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/68815x187.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/68815x188.png"/></fig></fig-group><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x191.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/68815x190.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Size of the spreader class over time under different transmitting rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x193.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x194.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/68815x192.png"/></fig><p>transmission of a rumor becomes difficult. This implies that governments should impose laws with strict punishment as a control measurement to stop the transmission of rumors in order to preserve the stability of a society.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> demonstrates how the size of the spreader class changes with time by varying the probability parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x195.png" xlink:type="simple"/></inline-formula> and fixing all other parameters. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x196.png" xlink:type="simple"/></inline-formula> is large, then the probability of susceptibles becoming incubators is greater than the probability of becoming spreaders. As shown in <xref ref-type="fig" rid="fig5">Figure 5</xref> the higher the probability parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x197.png" xlink:type="simple"/></inline-formula>, the smaller the size of the spreader class. With a higher <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x197.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x198.png" xlink:type="simple"/></inline-formula> value, fewer susceptibles become spreaders. This means that the incubator class is a significant cause of decreasing the number of spreaders. In other words, acquiring more information about a rumor before deciding to take any action minimizes rumor dissipation. This indicates that increasing public awareness towards the importance of thinking before speaking is an essential strategy to control rumor spreading. In addition, awareness towards the role and responsibility of individuals in dealing with rumors is of great benefit to the society.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> illustrates the changes in the size of the spreader class over time with different values of the stifling rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x199.png" xlink:type="simple"/></inline-formula>, while holding other parameters fixed. It is clear that the higher the stifling rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x200.png" xlink:type="simple"/></inline-formula>, the smaller the size of the spreader class. With a higher <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x201.png" xlink:type="simple"/></inline-formula> value, fewer incubators become spreaders. The increase of the stifling rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x202.png" xlink:type="simple"/></inline-formula> depends on the incubators’ scientific knowledge during the incubation period. If incubators have logical reasoning, then it is easy to discriminate a rumor. On the other hand if not, then more information must be available for incubators in order to reach a good judgement. This implies that the incubation period is crucial to crack down a rumor. Therefore, a powerful strategy to cease a rumor is to release information with logical facts about it. For this strategy to be effective it must be carried out as soon as a rumor starts to circulate.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, we formulated a rumor transmission model with incubation period, constant recruitment and varying total population. The model accommodates for both possibilities: incubators move to stifler class and susceptibles move to spreader class. The full dynamical system of the model is studied qualitatively producing two equilibrium points: rumor-free and rumor-existence. The existence conditions of the equilibriums are investigated. The rumor free equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x203.png" xlink:type="simple"/></inline-formula> exists always, whereas the rumor existence equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x204.png" xlink:type="simple"/></inline-formula></p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Size of the spreader class over time under different parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x206.png" xlink:type="simple"/></inline-formula> with β = 0.05, μ = 0.34, γ = 0.015, α = 0.4, ε = 0.0044, B = 2</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/68815x205.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Size of the spreader class over time under different stifling rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x208.png" xlink:type="simple"/></inline-formula> with β = 0.05, μ = 0.34, θ = 0.015, α = 0.4, ε = 0.0044, B = 2</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/68815x207.png"/></fig><p>exists only if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x209.png" xlink:type="simple"/></inline-formula>. The local and global stability analysis of both equilibriums is examined. We find that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula>is locally and asymptotically stable if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula>, and is globally and asymptotically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula>. Moreover, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula>is locally and asymptotically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x215.png" xlink:type="simple"/></inline-formula>, and is globally and unconditionally stable whenever it exists. The results of the numerical simulations are found to be in good agreement with the qualitative analysis. In other words, a rumor terminates when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x216.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x217.png" xlink:type="simple"/></inline-formula> and prevails when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x218.png" xlink:type="simple"/></inline-formula>. The impact of different management strategies on the dissipation of rumors is analyzed numerically by varying key parameters in the model. It is found that the number of spreaders is minimized if the transmitting rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x219.png" xlink:type="simple"/></inline-formula> is small and both the probability parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x219.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x220.png" xlink:type="simple"/></inline-formula> and the stifling rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x219.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/68815x221.png" xlink:type="simple"/></inline-formula> are large. Consequently, some effective strategies for rumor disappearance are: strict laws imposed by govern- ments, public awareness towards thinking before speaking, and the immediate release of information with logical facts about a rumor.</p></sec><sec id="s6"><title>Cite this paper</title><p>Salma Al-Tuwairqi,Sarah Al-Sheikh,Reem Al-Amoudi, (2015) Qualitative Analysis of a Rumor Transmission Model with Incubation Mechanism. Open Access Library Journal,02,1-12. doi: 10.4236/oalib.1102040</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.68815-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Dietz, K. (1967) Epidemics and Rumors: A Survey. Journal of the Royal Statistical Society, Series A (General), 130, 505-528. http://dx.doi.org/10.2307/2982521</mixed-citation></ref><ref id="scirp.68815-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Cane, V. 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