Local Stability Analysis of an SVIR Epidemic Model CAUCHY –Jurnal Matematika Murni dan Aplikasi Volume 5(1)(2017), Pages 20-28 p-ISSN: 2086-0382; e-ISSN: 2477-3344 Submitted: 26 August 2017 Reviewed: 10 October 2017 Accepted: 2 November 2017 DOI: http://dx.doi.org/10.18860/ca.v5i1.4388 Local Stability Analysis of an SVIR Epidemic Model Joko Harianto1, Titik Suparwati2 1, 2 Mathematics Department, Cenderawasih University Email: joharijpr88@gmail.com ABSTRACT In this paper, we present an SVIR epidemic model with deadly deseases. Initially the basic formulation of the model is presented. Two equilibrium point exists for the system; disease free and endemic equilibrium point. The local stability of the disease free and endemic equilibrium exists when the basic reproduction number less or greater than unity, respectively. If the value of 𝑅0 less than or equal one then the desease free equilibrium point is locally asymptotically stable, and if its exceeds, the endemic equilibrium point is locally asymptotically stable. The numerical results are presented for illustration. Keywords: SVIR Model, Local Stability, Basic Reproduction Number INTRODUCTION Health problems are closely associated with a disease. It is motivating humans to study health as well as illness. One of the goals of a nation to achieve prosperity in the future is the creation of a healthy living environment. One of the indicators of a healthy environment involves a high level of quality health services. Quality health care issues need to be addressed systematically, effectively and efficiently. Analysis of the spread of a disease is one step to address the problem of quality health services. The spread of disease due to virus or bacteria that enter into the body will lead to human health disorders and will affect the socio-economic development of the community. Efforts to prevent a spreading disease can work optimally if several stages such as research, development of various diagnostic tools, drugs, and new vaccines, has achieved. Mathematical models are one of a useful tool for reviewing or analyse the patterns of a disease spread. According to [2] and [4] the spread of infectious diseases can be described mathematically through a model, such as SIR and SIRS. The most basic procedure in modelling the spread of disease is by using the compartment model. In this case, the population is divided into three different classes namely, Susceptible, Infected, and Recovered which then shortened to SIR. Vaccination can be considered as the addition of a class naturally into the epidemic base model for some types of diseases. Along with the development of knowledge in the field of health, control of an epidemic disease can be done by vaccination action. Then the SIR model develops with the addition of a vaccinated population class. Some researchers have proposed models of the dynamics of vaccination. Among others is SVI type, which has been developed by [5], [6] and [7]. Several studies have stated that the threshold mailto:joharijpr88@gmail.com Local Stability Analysis of an SVIR Epidemic Model Joko Hariantoianto 21 to determine the occurrence of endemic disease seen from the value of Basic Reproduction Number (𝑅0). The disease distribution model will be locally stable if 𝑅0 ≀ 1 and the disease will be present if 𝑅0 > 1. Paper [8] discusses the SVIR epidemic model for non-lethal diseases that does not involve the individual's mortality rate due to the disease. From these studies, we can build some further assumptions related to the SVIR epidemic model that developed in public life. In this paper, we analyse the SVIR epidemic model for a deadly disease. We hope the model can be useful to analyse the disease outbreaks so that we can take optimal precautions. METHODS This research used literature study with literature sources from some reputable journal. The simulation of model SVIR used mathematical software, i.e. Maple 2016. RESULTS AND DISCUSSION 2.1. Formulation Model The following are assumptions used in modelling: 1. Closed population (no migration) 2. Births occur in every sub populations and enter in vulnerable subpopulations. 3. Natural death occurs on each sub populations at the same rate. 4. Illness can cause death. 5. Individuals who have cured cannot return to susceptive class (permanent cure). 6. Short incubation period. 7. Vaccination has given to susceptible subpopulations. 8. We do not distinguish the rate of recovery for a child has been infected and for the adult. 9. Vaccination will reach the level of immunity over time and finally enters the sub populations that heals. 10. Individuals who have vaccinated become infected if they lose immunity. 11. Contact between infected and susceptive individuals can lead to disease transmission, and so are contact between infected and those have vaccinated. We investigate the basic model formulation by dividing the total population into four compartments, such as S(t) for susceptible, V(t) for vaccinated, I(t) for infected and R(t) for recovered individuals. Let 𝛽 is the rate of contact that is sufficient to transmit the disease. We also assume a constant recovery rate 𝛾. The rate at which the susceptible population is vaccinated is 𝛼. We assume that there can be disease related death and define πœ” to be the rate of disease related death, while πœ‡ is the rate of natural death that is not related to the disease. We assume that all newborns enter the susceptible class at the constant rate of πœ‡. Let 𝛾1 be the average rate for susceptible individuals to obtain immunity and moved into recovered population. We do not distinguish the natural immunity and vaccine-induced immunity here because vaccine-induced immunity can also last for a long term. We assume that before obtaining immunity the vaccinees still have possibility of infection with a disease transmission rate 𝛽1 while contacting with infected individuals. 𝛽1 may be assume to be less than 𝛽 because the vaccinating individuals may have some partial immunity during the process or they may recognize the transmission characters of the disease and hence decrease the effective contacts with infected individuals. Figure 1 shows the details of the population transfer diagram of the SVIR model. Local Stability Analysis of an SVIR Epidemic Model Joko Hariantoianto 22 πœ”π‘… Figure.1 Transfer diagram of the SVIR model The following form presents the system model of differential equations. 𝑑𝑆 𝑑𝑑 = πœ‡ βˆ’πœ‡π‘† βˆ’π›½π‘†πΌ βˆ’π›Όπ‘† 𝑑𝑉 𝑑𝑑 = 𝛼𝑆 βˆ’π›½1𝑉𝐼 βˆ’π›Ύ1𝑉 βˆ’πœ‡π‘‰ (1) 𝑑𝐼 𝑑𝑑 = 𝛽𝑆𝐼 +𝛽1𝑉𝐼 βˆ’π›ΎπΌ βˆ’πœ‡πΌ βˆ’πœ”πΌ 𝑑𝑅 𝑑𝑑 = 𝛾1𝑉 +𝛾𝐼 βˆ’πœ‡π‘… where 𝑆(0) > 0,𝑉(0) > 0,𝐼(0) > 0,𝑅(0) = 0, 𝑆 +𝑉 +𝐼 +𝑅 = 1,βˆ€ 𝑑 β‰₯ 0 and all parameters are positive. The parameters with their description are presented in Table 1. Table 1. Parameter Description Parameter Description πœ‡ Natural death rate (and equally, the birth rate) 𝛽 The transmission rate of disease when susceptible individuals contact with infected individuals 𝛼 The rate of migration of susceptible individuals to the vaccination process 𝛽1 The transmission rate for vaccination individuals to be infected before gaining immunity 𝛾1 The average rate for vaccination individuals to obtain immunity and move into recovered population πœ” The death rate due to disease 𝛾 Recovery rate 2.2 . Equilibrium Point Next, we will study system dynamics in equation (1). Since the last equation does not depend on other equations, we simply study the following system. 𝑑𝑆 𝑑𝑑 = πœ‡ βˆ’πœ‡π‘† βˆ’π›½π‘†πΌ βˆ’π›Όπ‘† 𝑑𝑉 𝑑𝑑 = 𝛼𝑆 βˆ’π›½1𝑉𝐼 βˆ’π›Ύ1𝑉 βˆ’πœ‡π‘‰ (2) 𝑑𝐼 𝑑𝑑 = 𝛽𝑆𝐼 +𝛽1𝑉𝐼 βˆ’π›ΎπΌ βˆ’πœ‡πΌ βˆ’πœ”πΌ Local Stability Analysis of an SVIR Epidemic Model Joko Hariantoianto 23 Furthermore, we performed a SVIR model stability analysis around the equilibrium point of the system (2). As a first step, we define system equilibrium points (disease free points and endemic points). In general, according to [1] and [3] there exist two equilibrium points of epidemic model, i.e. the disease free equilibrium point and the endemic equilibrium point. The two equilibrium points are reviewed based on the existence of the disease in a population with a continuous time. The disease-free equilibrium point is the point at which the disease is unlikely to spread in an area because the infected population is equal to zero (I=0) for 𝑑 β†’ ∞. While the endemic equilibrium point is the point at which the disease must spread (I>0) for 𝑑 β†’ ∞, in a defined closed area. Theorem 1 There are two equilibrium points in the system (2), namely: a) The disease-free equilibrium point, that is, 𝐸0 = (𝑆0,𝑉0, 𝐼0) = ( πœ‡ 𝛼 +πœ‡ , π›Όπœ‡ (𝛼 +πœ‡)(𝛾1 +πœ‡) ,0) b) The endemic equilibrium point, that is, πΈβˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—) = ( πœ‡ (𝛼 +πœ‡ +π›½πΌβˆ—) , π›Όπœ‡ (𝛼 +πœ‡ +π›½πΌβˆ—)(πœ‡ +𝛾1 +𝛽1𝐼 βˆ—) , πΌβˆ—), where πΌβˆ— is the positive root of 𝐴1𝐼 2 +𝐴2𝐼 +𝐴3(1βˆ’πΆ) = 0, for C > 1, and 𝐴1 = (𝛾 +πœ‡ +πœ”)𝛽𝛽1 > 0 𝐴2 = ( 𝛾 +πœ‡ +πœ”)(( 𝛼 +πœ‡)𝛽1 + (𝛾1 + πœ‡)𝛽))βˆ’π›½1π›½πœ‡ 𝐴3=(𝛾 +πœ‡ +πœ”)( 𝛼 +πœ‡)( 𝛾1 + πœ‡) > 0 Proof: The equilibrium point of system (2) exists when 𝑑𝑆 𝑑𝑑 = 0, 𝑑𝑉 𝑑𝑑 = 0, 𝑑𝐼 𝑑𝑑 = 0, so that: πœ‡ βˆ’πœ‡π‘† βˆ’π›½π‘†πΌ βˆ’π›Όπ‘† = 0 (3) 𝛼𝑆 βˆ’π›½1𝑉𝐼 βˆ’π›Ύ1𝑉 βˆ’πœ‡π‘‰ = 0 (4) 𝛽𝑆𝐼 +𝛽1𝑉𝐼 βˆ’π›ΎπΌ βˆ’πœ‡πΌ βˆ’πœ”πΌ = 0 (5) From equation (5), we have 𝐼(𝛽𝑆 +𝛽1𝑉 βˆ’π›Ύ βˆ’πœ‡ βˆ’πœ”) = 0, and the solutions are 𝐼 = 0 or 𝛽𝑆 + 𝛽1𝑉 βˆ’π›Ύ βˆ’πœ‡ βˆ’πœ” = 0, consequently, we have to situation, namely: a) Situation at 𝑰 = 𝟎 It is the necessary condition for the disease-free equilibrium point. Note that, ο‚· From equation (3), πœ‡ βˆ’πœ‡π‘† βˆ’π›Όπ‘† = 0 ⟺ 𝑺 = 𝝁 𝜢+𝝁 ο‚· From (4), 𝛼𝑆 βˆ’π›Ύ1𝑉 βˆ’πœ‡π‘‰ = 0 ⟺ 𝑽 = 𝛼𝝁 (𝜢+𝝁)(𝜸𝟏+𝝁) So we get the equilibrium point of disease-free, that is, 𝐸0 = (𝑆0,𝑉0, 𝐼0) = ( πœ‡ 𝛼 +πœ‡ , π›Όπœ‡ (𝛼 +πœ‡)(𝛾1 +πœ‡) ,0) b) Situation at 𝑰 β‰  𝟎, or 𝑰 > 0, This situation is a necessary condition for an endemic equilibrium point. Note that: ο‚· From equation (3), πœ‡ βˆ’πœ‡π‘† βˆ’π›½π‘†πΌ βˆ’π›Όπ‘† = 0 ⟺ π‘Ίβˆ— = 𝝁 (𝜢+𝝁+πœ·πΌβˆ—) ο‚· From (4): 𝛼𝑆 βˆ’π›½1𝑉𝐼 βˆ’π›Ύ1𝑉 βˆ’πœ‡π‘‰ = 0 ⟺ 𝑽 βˆ— = 𝛼𝝁 (𝜢+𝝁+πœ·πΌβˆ—)(𝜸𝟏+𝝁+𝜷𝟏𝐼 βˆ—) From (5), if 𝐼 β‰  0, then 𝛽𝑆 +𝛽1𝑉 βˆ’π›Ύ βˆ’πœ‡ βˆ’πœ” = 0 , consequently, with substitute 𝑺 βˆ— and π‘½βˆ— we have: π›Όπœ‡π›½1 (𝛼 +πœ‡ +π›½πΌβˆ—)(𝛾1 +πœ‡ +𝛽1𝐼 βˆ—) = πœ‡ +𝛾 +πœ” βˆ’ π›½πœ‡ (𝛼 +πœ‡ +π›½πΌβˆ—) ⟺ 𝛽1𝛽(πœ‡ +𝛾 +πœ”) 𝐼 βˆ—2 +((πœ‡ +𝛾 +πœ”)(( 𝛼 +πœ‡)𝛽1 +(πœ‡ +𝛾1)𝛽)βˆ’π›½1π›½πœ‡) 𝐼 βˆ— + Local Stability Analysis of an SVIR Epidemic Model Joko Hariantoianto 24 (πœ‡ + 𝛾 + πœ”)(πœ‡ + 𝛾1)(𝛼 + πœ‡)(1βˆ’ ( π›½πœ‡ (𝛼 +πœ‡)(πœ‡ + 𝛾 + πœ”) + 𝛼𝛽1πœ‡ (𝛼 + πœ‡)(πœ‡ + 𝛾1)(πœ‡ + 𝛾 + πœ”) )) = 0 By applying: 𝐴1 = (𝛾 +πœ‡ +πœ”)𝛽1𝛽 > 0 𝐴2 =( 𝛾 +πœ‡ +πœ”)(( 𝛼 +πœ‡) 𝛽1 + (𝛾1 + πœ‡)𝛽)βˆ’ 𝛽1π›½πœ‡ 𝐴3=(𝛾 +πœ‡ +πœ”)( 𝛼 +πœ‡)( 𝛾1 + πœ‡) > 0 𝐢 = π›½πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾 +πœ”) + 𝛼𝛽1πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾1)(πœ‡ +𝛾 +πœ”) , the above equation becomes: 𝐴1𝐼 βˆ—2 +𝐴2𝐼 βˆ— +𝐴3(1βˆ’πΆ) = 0 (6) with the roots of equation (6), 𝐼1,2 βˆ— = βˆ’π΄2 ±√𝐴2 2 βˆ’4𝐴1𝐴3(1βˆ’πΆ) 2𝐴1 where πΌβˆ— > 0 and 𝐢 > 1. Thus, we obtain an endemic equilibrium point, that is, πΈβˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—) = ( πœ‡ (𝛼 +πœ‡ +π›½πΌβˆ—) , π›Όπœ‡ (𝛼 +πœ‡ +𝛽𝐼)(πœ‡ +𝛾1 +𝛽1𝐼 βˆ—) , πΌβˆ—). 2.3. Basic Reproduction Number (π‘ΉπŸŽ) The equilibrium point stability analysis on the SVIR model depends on the value of basic reproduction number 𝑅0 (the number of susceptible individuals who are then infected if they interact with patients in an entirely vulnerable population). A selection of this number is by observing the state of the endemic equilibrium point. Consider Eq. (6), an endemic equilibrium point only applicable to positive roots (πΌβˆ— > 0) when C > 1. In conclusion, the value of a positive endemic equilibrium point lies in the value of C, so that it can be defined the value basic reproduction number, that is, 𝑅0 = π›½πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾 +πœ”) + 𝛼𝛽1πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾1)(πœ‡ +𝛾 +πœ”) 2.4. LOCAL STABILITY OF EQUILIBRIUM POINT We will determine the stability of the equilibrium point of the SVIR model around the disease-free equilibrium and the endemic equilibrium point. Equations (3), (4), and (5) are nonlinear equations, so by using Taylor series at each equilibrium point, there will be a system of linear differential equations. Theorem 2 Defined: 𝑅0 = π›½πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾 +πœ”) + 𝛼𝛽1πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾1)(πœ‡ +𝛾 +πœ”) i. If 𝑅0 ≀ 1, then there is exist one (unique) equilibrium of system (1), that is, the disease- free equilibrium point 𝐸0 . Furthermore, if 𝑅0 > 1, then there are two equilibrium points of system (1), that is, the disease-free equilibrium points 𝐸0 dan 𝐸 βˆ—. ii. If 𝑅0 ≀ 1, then the equilibrium point 𝐸0 is locally asymptotically stable and if 𝑅0 > 1, then the equilibrium point 𝐸0 is unstable. iii. If 𝑅0 > 1, then the endemic equilibrium 𝐸 βˆ— is locally asymptotically stable. Proof: (i) We have discussed the existence of the equilibrium point of disease-free in Theorem 1. In the discussion, we obtain a point of equilibrium when I = 0 and is singular if 𝑅0 ≀ 1. The equilibrium point is the disease-free equilibrium point. Next, let's look at the equation 𝐴1𝐼 2 +𝐴2𝐼 +𝐴3(1βˆ’π‘…0) = 0, if 𝑅0 > 1, then 𝐴3(1βˆ’π‘…0) < 0 and 𝐴1 > 0, consequently, the equation has two real roots (positive and negative). Therefore, a necessary condition that ensures the existence and unique equilibrium πΈβˆ— has been fulfilled. Furthermore, when 𝑅0 ≀ 1, we will show that the above quadratic equation has no positive roots. Note that, Local Stability Analysis of an SVIR Epidemic Model Joko Hariantoianto 25 𝑅0 ≀ 1 ⟹ π›½πœ‡ ≀ (𝛼 +πœ‡)(𝛾 +πœ‡ +πœ”) ⟹ 𝐴2 β‰₯ ( 𝛾 +πœ‡ +πœ”)(( 𝛼 +πœ‡) 𝛽1 + (𝛾1 + πœ‡)𝛽)βˆ’ 𝛽1(𝛼 +πœ‡)(𝛾 +πœ‡ +πœ”) > ( 𝛾 +πœ‡ +πœ”)(𝛾1 + πœ‡)𝛽 > 0 So if 𝐴1 > 0, 𝐴3(1βˆ’π‘…0) > 0 then the function of 𝐴1𝐼 2 +𝐴2𝐼 +𝐴3(1βˆ’π‘…0) will rise and 𝐴1𝐼 2 + 𝐴2𝐼 +𝐴3(1βˆ’π‘…0) > 𝐴3(1βˆ’π‘…0) β‰₯ 0, for 𝐼 > 0, which means the quadratic function has no positive roots. (ii) The Jacobian Matrix of system (2) is 𝐽(𝑆,𝑉,𝐼) = ( βˆ’πœ‡ βˆ’π›Ό βˆ’π›½πΌ 0 βˆ’π›½π‘† 𝛼 βˆ’πœ‡ βˆ’π›Ύ1 βˆ’π›½1𝐼 βˆ’π›½1𝑉 𝛽𝐼 𝛽1𝐼 𝛽𝑆 +𝛽1𝑉 βˆ’πœ‡ βˆ’π›Ύ βˆ’πœ” ) So the Jacobian matrix around the point 𝐸0 = (𝑆0,𝑉0, 𝐼0) = ( πœ‡ 𝛼+πœ‡ , π›Όπœ‡ (𝛼+πœ‡)(𝛾1+πœ‡) ,0) is 𝐽(𝐸0) = ( βˆ’πœ‡ βˆ’π›Ό 0 βˆ’π›½π‘†0 𝛼 βˆ’πœ‡ βˆ’π›Ύ1 βˆ’π›½1𝑉0 0 0 𝛽𝑆0 +𝛽1𝑉0 βˆ’πœ‡ βˆ’π›Ύ βˆ’πœ” ) The characteristic equation is ⟺ [βˆ’(πœ‡ +𝛼)βˆ’πœ†][βˆ’(πœ‡ +𝛾1)βˆ’πœ†][ 𝛽𝑆0 +𝛽1𝑉0 βˆ’πœ‡ βˆ’π›Ύ βˆ’πœ” βˆ’πœ†] = 0 where πœ†1 = βˆ’(πœ‡ +𝛼) < 0 πœ†2 = βˆ’(πœ‡ +𝛾1)< 0 πœ†3 = 𝛽𝑆0 +𝛽1𝑉0 βˆ’πœ‡ βˆ’π›Ύ βˆ’πœ” = (𝛾 +πœ‡ +πœ”)(𝑅0 βˆ’1) It is clear if 𝑅0 < 1 then all the eigenvalues of 𝐽(𝐸0) are negative, hence the point 𝐸0 is locally asymptotically stable. Meanwhile, if 𝑅0 > 1, then there is a positive eigenvalue, hence the point 𝐸0 is unstable. (iii) It is clear that the endemic point πΈβˆ— exist when 𝑅0 > 1, so the Jacobian matrix around the point πΈβˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—) is 𝐽(πΈβˆ—) = ( βˆ’πœ‡ βˆ’π›Ό βˆ’π›½πΌβˆ— 0 βˆ’π›½π‘† 𝛼 βˆ’πœ‡ βˆ’π›Ύ1 βˆ’π›½1𝐼 βˆ— βˆ’π›½1𝑉 π›½πΌβˆ— 𝛽1𝐼 βˆ— π›½π‘†βˆ— +𝛽1𝑉 βˆ— βˆ’πœ‡ βˆ’π›Ύ βˆ’πœ” ) We can modify the element π‘Ž11,π‘Ž22, π‘Ž33, from matrix above into βˆ’πœ‡ βˆ’π›Ό βˆ’π›½πΌβˆ— = βˆ’ πœ‡ π‘†βˆ— βˆ’πœ‡ βˆ’π›Ύ1 βˆ’π›½1𝐼 βˆ— = βˆ’ π›Όπ‘†βˆ— π‘‰βˆ— Based on the evaluation results around the endemic equilibrium point we are getting π›½π‘†βˆ— +𝛽1𝑉 βˆ— βˆ’πœ‡ βˆ’π›Ύ βˆ’πœ” = 0, and the matrix become 𝐽(πΈβˆ—) = ( βˆ’ πœ‡ π‘†βˆ— 0 βˆ’π›½π‘† 𝛼 βˆ’ π›Όπ‘†βˆ— π‘‰βˆ— βˆ’π›½1𝑉 π›½πΌβˆ— 𝛽1𝐼 βˆ— 0 ) The characteristic equation of matrix 𝐽(πΈβˆ—) is πœ†3 +π‘Ž1πœ† 2 +π‘Ž2πœ† +π‘Ž3 = 0 where π‘Ž1 = πœ‡ π‘†βˆ— + π›Όπ‘†βˆ— π‘‰βˆ— > 0 π‘Ž2 = π›Όπ‘†βˆ— π‘‰βˆ— +𝛽1 2 π‘‰βˆ—πΌβˆ— + 𝛽2π‘†βˆ—πΌβˆ— > 0 π‘Ž3 = 𝛼𝛽1𝛽𝑆 βˆ—πΌβˆ— + 𝛼𝛽2π‘†βˆ— 2 πΌβˆ— π‘‰βˆ— + πœ‡π›½1 2 π‘‰βˆ—πΌβˆ— π‘†βˆ— > 0 hence, π‘Ž1π‘Ž2 βˆ’π‘Ž3 = π›Όπœ‡2 π‘†βˆ—π‘‰βˆ— +(πœ‡ +π›½πΌβˆ—)𝛽2π‘†βˆ—πΌβˆ— + 𝛼2πœ‡π‘†βˆ— π‘‰βˆ—2 +π›ΌπΌβˆ—π‘†βˆ—(𝛽 βˆ’π›½1) 2 +𝛼𝛽1𝛽𝑆 βˆ—πΌβˆ— > 0 Local Stability Analysis of an SVIR Epidemic Model Joko Hariantoianto 26 has been fulfilled. According to the Routh-Hurwitz criterion, all the eigenvalues of the above characteristic equations have a negative real part. So, the equilibrium point πΈβˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—) is locally asymptotically stable. Based on the results, we will interpret the results biologically as follows, ο‚· If 𝑅0 ≀ 1, then for 𝑑 β†’ ∞ and (𝑆,𝑉,𝐼) that close enough to 𝐸0 = (𝑆0,𝑉0, 𝐼0), the solution of system (1) will move to 𝐸0 = (𝑆0,𝑉0, 𝐼0). It means that if 𝑅0 ≀ 1, then for the number of susceptible, vaccinated and infected individuals close to 𝐸0 = (𝑆0,𝑉0, 𝐼0), the disease will not plague and tends to disappear indefinitely time. This condition is then called asymptotically stable around the equilibrium point 𝐸0 = (𝑆0,𝑉0, 𝐼0), and we interpret as a disease-free equilibrium point. ο‚· If 𝑅0 > 1, then for 𝑑 β†’ ∞ and (𝑆,𝑉,𝐼) that close enough to 𝐸 βˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—), the solution of system (1) will move to πΈβˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—). This means if 𝑅0 > 1, then for the number of susceptible, vaccinated and infected individuals close to πΈβˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—), the disease will plague but does not reach extinction in an infinite time. This condition is then called asymptotically stable around the equilibrium point πΈβˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—), and we interpret as an endemic equilibrium point. 2.5. NUMERICAL RESULTS In this section, we investigate the numerical solution of the system (1) by using the Runge- Kutta order four scheme. The state variables are chosen with same initials conditions. The numerical results are shown in Figure 1 and 2. Figure 1, illustrate the fact, when the basic reproduction number less than unity, when the value of basic reproduction number exceeds than unity, Figure 2 illustrate this fact. Figure 1. The dynamical behavior of system (1), for same initial conditions and different parameters: when 𝑅0 = 0,22 ≀ 1,the desease free equilibrium point is locally asymptotically stable where πœ‡ = 1, 𝛽 = 10,𝛽1 = 2,𝛾 = 4,𝛾1 = 8,𝛼 = 10,πœ” = 0,01. Local Stability Analysis of an SVIR Epidemic Model Joko Hariantoianto 27 Figure 2. The dynamical behavior of system (1), for same initial conditions and different parameters: when 𝑅0 = 3,17 > 1, endemic equilibrium is locally asymptotically stable where πœ‡ = 1, 𝛽 = 20,𝛽1 = 15,𝛾 = 1,𝛾1 = 2,𝛼 = 10,πœ” = 0,01. CONCLUSION From the results of endemic equilibrium point analysis, we define the basic reproduction number parameter, that is, 𝑅0 = π›½πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾 +πœ”) + 𝛼𝛽1πœ‡ (𝛼 +πœ‡)(πœ‡ +𝛾1)(πœ‡ +𝛾 +πœ”) Furthermore, 𝑅0 is a necessary condition for the existence of the two points of equilibrium as well as its local stability. When 𝑅0 ≀ 1, there is only one (unique) equilibrium point of disease-free, that is, 𝐸0 = (𝑆0,𝑉0, 𝐼0) = ( πœ‡ 𝛼+πœ‡ , π›Όπœ‡ (𝛼+πœ‡)(𝛾1+πœ‡) ,0). Conversely, if 𝑅0 > 1, then there are two equilibrium points, that is, 𝐸0 and an endemic equilibrium point 𝐸 βˆ— = (π‘†βˆ—,π‘‰βˆ—, πΌβˆ—) = ( πœ‡ (𝛼+πœ‡+π›½πΌβˆ—) , π›Όπœ‡ (𝛼+πœ‡+𝛽𝐼)(πœ‡+𝛾1+𝛽1𝐼 βˆ—) , πΌβˆ—) where πΌβˆ— is the positive root of the equation 𝐴1𝐼 2 +𝐴2𝐼 + 𝐴3(1βˆ’π‘…0) = 0. Results of local stability analysis indicates if 𝑅0 ≀ 1, then the disease free equilibrium point 𝐸0 is locally asymptotically stable. It means if the terms 𝑅0 ≀ 1 fulfilled, then in a long time, there would have no spread of disease in susceptible and vaccinated subpopulations, or in other words, the epidemic will stop. Conversely, if 𝑅0 > 1 then the endemic equilibrium point E ο€ͺ is locally asymptotically stable. 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