<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2015.65070</article-id><article-id pub-id-type="publisher-id">AM-56160</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Modelling and Simulation of the Spread of HBV Disease with Infectious Latent
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>A. Moneim</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>H.</surname><given-names>A. Khalil</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Scientific Computing, Faculty of Computers and Information, Benha University, Benha, Egypt</addr-line></aff><aff id="aff1"><addr-line>Department of Basic and Applied Science, Unaizah Community College, Qassim University, Unaizah, 
Saudi Arabia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>moneim97@yahoo.com(.AM)</email>;<email>moneim97@yahoo.com(HAK)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>05</month><year>2015</year></pub-date><volume>06</volume><issue>05</issue><fpage>745</fpage><lpage>753</lpage><history><date date-type="received"><day>2</day>	<month>April</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>6</month>	<year>May</year>	</date><date date-type="accepted"><day>7</day>	<month>May</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>
 
 
  This paper studies the global behavior of the spread of HBV using a SEIR model with a constant vaccination rate. The infectivity during the incubation period is considered as a second way of transmission. The basic reproduction number 
  <em>R</em>0 is derived as a function of the two contact rates 
  β1 and 
  β2 . There is a disease free equilibrium point (DFE) of our model. When 
  <em>R</em>0 &lt; 1, the (DFE) is asymptotically stable. On the other hand, if 
  <em>R</em>0 &gt; 1, there is a unique endemic equilibrium. We proved that the endemic equilibrium was globally asymptotically stable when 
  <em>R</em>0 &gt; 1 and that the disease persisted in the population. These results are original for our model with vaccination and two contact rates.
 
</p></abstract><kwd-group><kwd>HBV Modelling</kwd><kwd> Global Stability</kwd><kwd> Simulation</kwd><kwd> Two Contact Rates</kwd><kwd> Basic Reproduction Number R0</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Spread of the HBV is a major public health problem. About a third of the worlds population, approximately 2 billion people, get infected with hepatitis B virus in their life time. About 360 million people remain chronically infected carriers of the disease, most of whom are unaware of their HBV status [<xref ref-type="bibr" rid="scirp.56160-ref1">1</xref>] and about 20% - 30% of whom will eventually die from chronic sequel. The prevalence of HBV infection varies from country to country, depending upon a complex behavioral, environmental and host factors [<xref ref-type="bibr" rid="scirp.56160-ref2">2</xref>] . Chronic HBV can lead to hepatocellular carcinoma after 20 years among persons with chronic HBV infection; the risk for premature death from cirrhosis or hepatocellular carcinoma is 15% - 25% [<xref ref-type="bibr" rid="scirp.56160-ref3">3</xref>] .</p><p>Medical observations and statistics show that there are many ways for HBV transmission. Blood to blood product and shared syringes act as medical transmissions for the HBV in the developing countries. Also, HBV can transmit through the use of shared razors and brushes. Mosquitoes and bed-bugs can play as another sort of blood to blood tool to transfer the virus. It has been reported that the HBV can be transmitted among sexual partners. Finally, mothers can pass the infection to their children during pregnancy or breast feeding [<xref ref-type="bibr" rid="scirp.56160-ref4">4</xref>] .</p><p>It is well documented that many diseases, such as tuberculosis, HIV/AIDS and SARS, etc., have a contagious latent period; a latent individual can transmit the disease to the susceptible. This means that there are two forces of infection during both the latent and infectious periods. This fact has been noticed by some researchers [<xref ref-type="bibr" rid="scirp.56160-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.56160-ref7">7</xref>] . HBV has a long incubation period which varies from six weeks to six months. The latent persons can pass the HBV infection during their latent period [<xref ref-type="bibr" rid="scirp.56160-ref3">3</xref>] . So, we add another sort of transmission of the HBV. This second way comes from the contact between the latent persons and the susceptibles.</p><p>Li and Jin [<xref ref-type="bibr" rid="scirp.56160-ref5">5</xref>] consider a SEI epidemic model with general contact rate that incorporates constant recruit- ment and has infectious forces in both the latent and infected periods. In their work, Lyapunov function and LaSalles invariant set theorem have been used to prove the global asymptotical stable results of the disease-free equilibrium. They studied the stability of the epidemic equilibrium by using the Poincare Bendixson property. Also, Li and Jin [<xref ref-type="bibr" rid="scirp.56160-ref6">6</xref>] present a SEIR model which has infectious forces in latent, infected and immune period.</p><p>Li and Fang [<xref ref-type="bibr" rid="scirp.56160-ref8">8</xref>] studied an age structured SEIR epidemic model with infectivity in both the latent and in- fectious periods. By using the theory and methods of Differential and Integral Equations, they obtained that the disease-free equilibrium was expression for the basic reproduction number locally and globally asymptotically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x7.png" xlink:type="simple"/></inline-formula>. In this case, the disease always dies out. When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x8.png" xlink:type="simple"/></inline-formula>, there exists a unique endemic equili- brium which is asymptotically stable under certain conditions [<xref ref-type="bibr" rid="scirp.56160-ref8">8</xref>] .</p></sec><sec id="s2"><title>2. The Model</title><p>We have considered a more complicated and realistic SEIR model with vaccination. This type of model which takes account of the infectiousness of disease in the latency state. Here we investigate the effect of the infectivity of the latent population in addition to the transmission between the susceptibles and infective populations. The model makes the following assumptions:</p><p>1) The total population size is a constant N, and the population is divided into four groups:</p><p>a) The susceptible class, S, comprising those people who are capable of catching the disease;</p><p>b) The exposed (or latent) class, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x9.png" xlink:type="simple"/></inline-formula>, comprising those individuals who are infected but not yet infectious;</p><p>c) The infectives, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x10.png" xlink:type="simple"/></inline-formula>, comprising those who are infected and capable of transmitting the disease;</p><p>d) The recovered class, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x11.png" xlink:type="simple"/></inline-formula>, comprising those individuals who are immune.</p><p>2) The per capita birth rate is a constant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x12.png" xlink:type="simple"/></inline-formula>. As births balance deaths we must have that the per capita death rate is also<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x13.png" xlink:type="simple"/></inline-formula>.</p><p>3) The population is uniform and mixes homogeneously.</p><p>4) The infection rates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x14.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x15.png" xlink:type="simple"/></inline-formula> are defined as the total rates at which potentially infectious contacts occur between two individuals (in other words contacts which will result in the transmission of infection if one of the individuals is susceptible and the other is infectious for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x16.png" xlink:type="simple"/></inline-formula>) and latent for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x17.png" xlink:type="simple"/></inline-formula>.</p><p>5) The exposed individuals move from the latent class to the infective class at a constant rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x18.png" xlink:type="simple"/></inline-formula> and so the average latent period, conditional on survival to the end of it, is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x19.png" xlink:type="simple"/></inline-formula>.</p><p>6) The infectives move from the infective class to the recovered class at a constant rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x20.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x21.png" xlink:type="simple"/></inline-formula> is the average infectious period, conditional on survival to the end of it.</p><p>The SEIR model for the spread of infectious diseases can be written as a set of four coupled non-linear ordinary differential equations as follows:</p><disp-formula id="scirp.56160-formula265"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x22.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula266"><label>, (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x23.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula267"><label>, (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x24.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x25.png" xlink:type="simple"/></inline-formula> (4)</p><p>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x26.png" xlink:type="simple"/></inline-formula>.</p><p>The basic reproduction number is defined as the average value of the expected number of secondary cases produced by a single newly infected person entering the population at the disease free state. In this model the average value of the expected number of secondary cases produced by a single infected person is</p><disp-formula id="scirp.56160-formula268"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x27.png"  xlink:type="simple"/></disp-formula><p>It has been shown that with constant transmission rates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x28.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x29.png" xlink:type="simple"/></inline-formula> our model has one and only one disease free equilibrium (DFE) and another endemic equilibrium state of our SEIR model. In this paper, simulation results have been conducted for parameter values which insure that if the vaccination parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x30.png" xlink:type="simple"/></inline-formula> is not large enough, to force the basic reproductive number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x31.png" xlink:type="simple"/></inline-formula> to be less than one in value, the disease remains endemic in the population. In the other hand simulations of our model are conducted to show up the effect of introducing the disease transmission between latent and susceptible populations.</p></sec><sec id="s3"><title>3. Equilibrium Points</title><p>The system (1)-(4) has two equilibria points the first one is the disease free equilibrium (DFE) point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x32.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.56160-formula269"><graphic  xlink:href="http://html.scirp.org/file/2-7402706x33.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x34.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x35.png" xlink:type="simple"/></inline-formula>. The other one is the endemic equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x36.png" xlink:type="simple"/></inline-formula> which is represented by</p><disp-formula id="scirp.56160-formula270"><graphic  xlink:href="http://html.scirp.org/file/2-7402706x37.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x38.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x39.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x40.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x41.png" xlink:type="simple"/></inline-formula>.</p><p>Here, it straightforward to show that, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x42.png" xlink:type="simple"/></inline-formula>exists if and only if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x43.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Stability of the Disease Equilibrium Point (DFE)</title><p>This section studies the stability of the disease free equilibrium (DFE) point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x44.png" xlink:type="simple"/></inline-formula>. In this case, there is no disease in the population as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x45.png" xlink:type="simple"/></inline-formula>. The Jacobian matrix of the system (1)-(4) at the point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x46.png" xlink:type="simple"/></inline-formula>, (DFE) is given by</p><disp-formula id="scirp.56160-formula271"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x47.png"  xlink:type="simple"/></disp-formula><p>Theorem 1 The disease free equilibrium point, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x48.png" xlink:type="simple"/></inline-formula>is locally asymptotically stable for the system (1)-(4) if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x49.png" xlink:type="simple"/></inline-formula>, and unstable when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x50.png" xlink:type="simple"/></inline-formula>.</p><p>Proof</p><p>From the characteristic equation of the matrix (6) we have two negative eigenvalues, both of them equals to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x51.png" xlink:type="simple"/></inline-formula>. The rest of the characteristic equation is given by,</p><disp-formula id="scirp.56160-formula272"><graphic  xlink:href="http://html.scirp.org/file/2-7402706x52.png"  xlink:type="simple"/></disp-formula><p>From Equation (5), if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x53.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x54.png" xlink:type="simple"/></inline-formula>. So, we found that all the eigenvalues of the matrix (6) have negative real parts. Therefore, using the Routh-Hurwitz conditions for the stability of linear differential Equ- ations [<xref ref-type="bibr" rid="scirp.56160-ref9">9</xref>] , the disease free equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x55.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x56.png" xlink:type="simple"/></inline-formula>. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x57.png" xlink:type="simple"/></inline-formula> this implies that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x58.png" xlink:type="simple"/></inline-formula>. Thus the characteristic equation of the matrix (6) must have a positive eigenvalue. Therefore, the disease free equilibrium point, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x59.png" xlink:type="simple"/></inline-formula>is unstable for the system (1)-(4). This completes the proof of Theorem (1).</p></sec><sec id="s5"><title>5. Global Stability of the Endemic Equilibrium Point</title><p>This section concerned with global stability of the endemic equilibrium point. The necessary and sufficient con- dition to the existence of the endemic point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x60.png" xlink:type="simple"/></inline-formula>, is that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x61.png" xlink:type="simple"/></inline-formula>. Similar technique to the proof to Theorem 1 in Korobeinikov and Wake [<xref ref-type="bibr" rid="scirp.56160-ref10">10</xref>] is been used in this section.</p><p>We start off by calculating the parameter values of the model at the equilibrium. From Equation (1) at the equilibrium, we have that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x62.png" xlink:type="simple"/></inline-formula>, therefore</p><disp-formula id="scirp.56160-formula273"><label>. (7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x63.png"  xlink:type="simple"/></disp-formula><p>Similarly, from Equation (2), we get,</p><disp-formula id="scirp.56160-formula274"><label>. (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x64.png"  xlink:type="simple"/></disp-formula><p>finally, from Equation (3), we can deduce that,</p><disp-formula id="scirp.56160-formula275"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x65.png"  xlink:type="simple"/></disp-formula><p>Substituting in (1), (2) and (3), we find that,</p><disp-formula id="scirp.56160-formula276"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x66.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula277"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x67.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x68.png" xlink:type="simple"/></inline-formula> (12)</p><p>Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x69.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x70.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x71.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x72.png" xlink:type="simple"/></inline-formula>. Then substituting these values in Equations (10)-(12) we find that,</p><disp-formula id="scirp.56160-formula278"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x73.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula279"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x74.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x75.png" xlink:type="simple"/></inline-formula> (15)</p><p>Theorem 2 If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x76.png" xlink:type="simple"/></inline-formula>, then the endemic equilibrium point, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x77.png" xlink:type="simple"/></inline-formula>is globally asymptotically stable for the system (1)-(4).</p><p>Proof</p><p>Define a positive definite function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x78.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x79.png" xlink:type="simple"/></inline-formula>, where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x80.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x81.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x82.png" xlink:type="simple"/></inline-formula>. Now we prove that, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x83.png" xlink:type="simple"/></inline-formula>is nonpositive definite function. Differentiat-</p><p>ing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x84.png" xlink:type="simple"/></inline-formula> and substituting by the values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x85.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x86.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x87.png" xlink:type="simple"/></inline-formula> we have,</p><disp-formula id="scirp.56160-formula280"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x88.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula281"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x89.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula282"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x90.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula283"><label>. (19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x91.png"  xlink:type="simple"/></disp-formula><p>therefore,</p><disp-formula id="scirp.56160-formula284"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x92.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56160-formula285"><label>. (21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x93.png"  xlink:type="simple"/></disp-formula><p>Rearranging Equation (21) we deduce that,</p><disp-formula id="scirp.56160-formula286"><label>. (22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x94.png"  xlink:type="simple"/></disp-formula><p>As the arithmetic mean is greater than or equal to the geometric mean we find that, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x95.png" xlink:type="simple"/></inline-formula>iff <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x96.png" xlink:type="simple"/></inline-formula></p><p>and all of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x97.png" xlink:type="simple"/></inline-formula> and e are nonnegative. Equation (7) ensures that,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x98.png" xlink:type="simple"/></inline-formula>. Moreover <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x99.png" xlink:type="simple"/></inline-formula> iff <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x100.png" xlink:type="simple"/></inline-formula></p><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x101.png" xlink:type="simple"/></inline-formula> which can be represented by the following set,</p><disp-formula id="scirp.56160-formula287"><label>. (23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x102.png"  xlink:type="simple"/></disp-formula><p>The equilibrium point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x103.png" xlink:type="simple"/></inline-formula> is the only invariant set of the system (1)-(4) which contained entirely in the set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x104.png" xlink:type="simple"/></inline-formula>. Hence by Liapunov’s direct methods <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x105.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x106.png" xlink:type="simple"/></inline-formula> for the system (1)-(4). This completes the proof of Theorem (2).</p></sec><sec id="s6"><title>6. Simulation Results</title><p>In this section we study numerically the behaviour of the system. The system of linear ordinary differential Equations (1)-(4) is been solved numerically by using the software package XPPAUTO and using the following parameter set from the literature, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x107.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.56160-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.56160-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.56160-ref13">13</xref>] . Also we simulate our system for two different states one if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x108.png" xlink:type="simple"/></inline-formula> and the other one when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x109.png" xlink:type="simple"/></inline-formula> we found that, disease has a thre- shold level <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x110.png" xlink:type="simple"/></inline-formula> for the reproductive number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x111.png" xlink:type="simple"/></inline-formula> to be under one in value which the disease to die out. If the vaccination value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x112.png" xlink:type="simple"/></inline-formula> is not sufficient then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x113.png" xlink:type="simple"/></inline-formula> stays above one in value and the disease becomes endemic.</p><p>The first result of our simulations confirms that the disease free equilibrium is globally asymptotically stable when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x114.png" xlink:type="simple"/></inline-formula>. On the other hand if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x115.png" xlink:type="simple"/></inline-formula> there is a stable endemic solution. Here we present a sample of the results obtained in these simulations. We give a sample of the effect of considering the transition rate between latent and susceptibles. Also we give a bifurcation diagram of the infected population against the vaccination rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x116.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) shows that when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x117.png" xlink:type="simple"/></inline-formula> the values of the infected population <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x118.png" xlink:type="simple"/></inline-formula> tends to its disease free equilibrium values. <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) shows that when the vaccination fails to force the basic reproduction number to be less than one in value the disease fires up and approaches an endemic level. This result is obtained for the case that the vaccination rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x119.png" xlink:type="simple"/></inline-formula>.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> studies numerically the behaviour of the system in response to changes in p, the vaccination rate. We use the basic idea that, sectioning the endemic stable equilibrium solutions by looking at Poincar&#233; sections and plotting the sections of the endemic equilibrium solutions against the vaccination value p to obtain the number</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The number of infected population against time corresponding to parameter values of HBV (a) when the vaccination rate (p = 0.96) which is large enough so that, R<sub>0</sub> &lt; 1 and (b) when the vaccination rate, p = 0.5, is not sufficient enough to keep R<sub>0</sub> &lt; 1</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7402706x120.png"/></fig><p>of points in each section [<xref ref-type="bibr" rid="scirp.56160-ref14">14</xref>] . These points represent the period of the stable long term periodic solution of our model. We have taken the simulation parameters for all of the bifurcation diagrams presented here as stated above and the total population size N was 1,000,000.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> represents the bifurcation diagram for HBV with two transmission rates for the infected and the susceptibles. This figure shows that at small values of vaccination parameter the disease has a periodic solution of period one year. Increasing the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x121.png" xlink:type="simple"/></inline-formula> produces a two year periodic further increases generate a series of period doubling solutions until the behaviour of the system appears to become aperiodic and possibly chaotic. However, increasing the vaccination rate more forces the infected number to drop down until approaching zero at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x122.png" xlink:type="simple"/></inline-formula>.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> represents the number of infected population against time corresponding to parameter values of HBV when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x123.png" xlink:type="simple"/></inline-formula>. The black line plots the infected against time when, the latent are infectious. In this case, there is another contact rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x124.png" xlink:type="simple"/></inline-formula> between susceptibles and latent. The black line shows that, there is an endemic solution which is going up rapidly. This solution has some peaks which look to be periodic of long period. The</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The bifurcation diagrams of HBV parameter values of the number of infected against vaccination parameter p</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7402706x125.png"/></fig><p>red line plots the infected against time when infectivity of the latent is ignored<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x126.png" xlink:type="simple"/></inline-formula>. The red line in <xref ref-type="fig" rid="fig2">Figure 2</xref> shows that there are some peaks which have larger tops than the black one but, the line has small values all over the whole diagram. The green line represents the case that, there is a total isolation of the infected persons<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x127.png" xlink:type="simple"/></inline-formula>. The green line shows the smallest peaks in the diagram. These peaks decay smoothly to be almost steady state.</p></sec><sec id="s7"><title>7. Summary and Discussion</title><p>This paper investigates the effect of using another way of producing new cases. This way is the fact that latent persons can pass the disease into susceptibles [<xref ref-type="bibr" rid="scirp.56160-ref3">3</xref>] . Also, vaccination of all newborns, at a constant rate, has been considered. It is documented that vaccination strategies are applied worldwide to vaccinate children in the early ages. For example, in China an effective vaccination program has been established for newborn babies since the 1990s, which has reduced chronic HBV infection in children. Unfortunately, the incidence of hepatitis B is still increasing [<xref ref-type="bibr" rid="scirp.56160-ref13">13</xref>] . This means that the vaccinated proportion is large enough to force the reproduction number to be less than one in value. Therefore, to control HBV infection vaccination, strategies need a treatment scheme as another leg to have a better control strategy for the disease [<xref ref-type="bibr" rid="scirp.56160-ref15">15</xref>] .</p><p>The first result of this paper comes from the stability analysis of the DFE of our model. We find that the DFE is locally asymptotically stable when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x128.png" xlink:type="simple"/></inline-formula>, the basic reproduction number, is less than one. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x129.png" xlink:type="simple"/></inline-formula> exceeds one, then the DFE point is unstable. When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x130.png" xlink:type="simple"/></inline-formula>, there exists another equilibrium point which is the endemic point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x131.png" xlink:type="simple"/></inline-formula>. We deduced that if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x132.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x133.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable for the system (1)-(4). We used Liapunov’s direct methods to prove this result.</p><p>Simulation results of our model have been conducted for HBV parameter set using different vaccination parameter values. From these results, we find that there is a critical ratio <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x134.png" xlink:type="simple"/></inline-formula> approximately, from which all the newborns must be vaccinated. This value is the sufficient condition to reduce susceptible number to be less than a critical value S<sub>C</sub>. This forces the basic reproduction number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x135.png" xlink:type="simple"/></inline-formula> to be less than one in value and the disease dies out. The threshold value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x136.png" xlink:type="simple"/></inline-formula> can be driven as follows. From Equation (5), we have that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x137.png" xlink:type="simple"/></inline-formula>. Therefore, to keep<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x138.png" xlink:type="simple"/></inline-formula>, we must keep the susceptibles below the certain threshold</p><p>value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7402706x139.png" xlink:type="simple"/></inline-formula> which is given by</p><disp-formula id="scirp.56160-formula288"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7402706x140.png"  xlink:type="simple"/></disp-formula><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The number of infected population against time corresponding to parameter values of HBV when the vaccination rate is not sufficient enough to keep R<sub>0</sub> &lt; 1, the black, red and green lines corresponding to (β<sub>1</sub> = β<sub>2</sub> = 0.000025), (β<sub>1</sub> = 0.000025, β<sub>2</sub> = 0) and (β<sub>1</sub> = 0, β<sub>2</sub> = 0.000025) respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7402706x141.png"/></fig><p>If this condition fails, the susceptibles will be large enough to make the disease firs up and become endemic in the population. In this case, we got some high peaks as shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. It is important to note that <xref ref-type="fig" rid="fig3">Figure 3</xref> indicates that the black line which includes the infectivity of the latent is going up continuously and has a sustainable long term period solution.</p><p>The bifurcation diagram <xref ref-type="fig" rid="fig2">Figure 2</xref> indicates that the vaccination parameter p can play as a key value of our model. This figure also shows that there are many endemic periodic solutions of our model. These solutions vary from biennial to large period or chaotic solutions. It is obvious to conclude that bifurcation diagram <xref ref-type="fig" rid="fig2">Figure 2</xref> gives a wide range of information about the dynamics of the HBV disease and indicates how the values of the vaccination rate affect the behaviour of the disease dynamics.</p><p>Finally, vaccinating all newborns by a rate greater than 96% is not reachable in practice. Therefore, from our results, it is important to declare that treatments or additional vaccination strategies are needed to control the spread of HBV in population. Controlling the disease means that reducing the susceptibles by vaccination or reducing latent and infected by treatments scheme.</p></sec><sec id="s8"><title>Acknowledgements</title><p>This research is funded by the deanship of scientific research, Qassim University, KSA.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.56160-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Abdulrahman, S., Akinwande, N.I., Awojoyogbe, O.B. and Abubakar, U.Y. (2013) Sensitivity Analysis of the Parameters of a Mathematical Model of Hepatitis B Virus Transmission. Universal Journal of Applied Mathematics, 1, 230-241.</mixed-citation></ref><ref id="scirp.56160-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Saher, F., Rahman, K., Quresh, J.A., Irshad, M. and Iqbal, H.M. (2012) Investigation of an Inflammatory Viral Disease HBV in Cardiac Patients through Polymerase Chain Reaction. 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