Volume 22, Issue S1 e2754
RESEARCH ARTICLE
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Dynamical analysis of novel COVID-19 epidemic model with non-monotonic incidence function

R. Prem Kumar

R. Prem Kumar

Department of Mathematics, National Institute of Technology Puducherry, Karaikal, Puducherry, India

Avvaiyar Government College for Women, Karaikal, Puducherry, India

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Sanjoy Basu

Corresponding Author

Sanjoy Basu

Arignar Anna Government Arts and Science College, Karaikal, Puducherry, India

Correspondence

Sanjoy Basu, Department of Mathematics, Arignar Anna Government Arts and Science College, Karaikal 609605, Puducherry, India.

Email: [email protected]

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Dipankar Ghosh

Dipankar Ghosh

Department of Mathematics, National Institute of Technology Puducherry, Karaikal, Puducherry, India

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Prasun Kumar Santra

Prasun Kumar Santra

Moulana Abul Kalam Azad University of Technology, Kolkata, West Bengal, India

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G. S. Mahapatra

G. S. Mahapatra

Department of Mathematics, National Institute of Technology Puducherry, Karaikal, Puducherry, India

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First published: 02 September 2021
Citations: 3

Abstract

In this study, we developed and analyzed a mathematical model for explaining the transmission dynamics of COVID-19 in India. The proposed urn:x-wiley:14723891:media:pa2754:pa2754-math-0001 model is a modified version of the existing urn:x-wiley:14723891:media:pa2754:pa2754-math-0002 model. Our model divides the infected class urn:x-wiley:14723891:media:pa2754:pa2754-math-0003 of urn:x-wiley:14723891:media:pa2754:pa2754-math-0004 model into two classes: urn:x-wiley:14723891:media:pa2754:pa2754-math-0005 (unknown infected class) and urn:x-wiley:14723891:media:pa2754:pa2754-math-0006 (known infected class). In addition, we consider urn:x-wiley:14723891:media:pa2754:pa2754-math-0007 a recovered and reserved class, where susceptible people can hide them due to fear of the COVID-19 infection. Furthermore, a non-monotonic incidence function is deemed to incorporate the psychological effect of the novel coronavirus diseases on India's community. The epidemiological threshold parameter, namely the basic reproduction number, has been formulated and presented graphically. With this threshold parameter, the local and global stability analysis of the disease-free equilibrium and the endemic proportion equilibrium based on disease persistence have been analyzed. Lastly, numerical results of long-run prediction using MATLAB show that the fate of this situation is very harmful if people are not following the guidelines issued by the authority.

1 INTRODUCTION

The first case of the coronavirus pandemic was reported on January 30, 2020 in India (Zhu et al., 2020). India's response to COVID-19 has been graded, pro-active, and pre-emptive with high-level political commitment and a “whole government” approach to respond to the COVID-19 pandemic. Educational institutions, various Governments, and non-Government offices, and many commercial establishments have been shut down immediately. Government of India, exercise the Disaster Management Act, 2005, issued an order for State/UT's prescribing lockdown for containment of COVID-19 pandemic in the country for 21 days with effect from March 25, 2020, and announced to maintain mandatory physical distancing in India. Later Government extent the lockdown period up to May 3, 2020 as the number of active cases increases daily. The most common symptoms are dry cough, fever, and tiredness, but some infected people may have aches and pains, running nose, nasal congestion, sore throat, vomiting, or diarrhea. These symptoms usually are severe and begin gradually. Some people become infected, but neither has symptoms nor feels ill. Disease recovery is high without requiring special treatment. The guidelines for preventing the spreading of COVID-19 are wearing a face mask, staying more than 3 ft away from a sick person, washing hands with soap, or using alcohol-based hand rub, and so forth.

During an epidemic, reported cases of coronavirus disease are rising worldwide day by day due to human-to-human transmission; the study for prevention and control of infectious COVID-19 disease is essential. The modernized mathematical model is necessary to give a deeper understanding and perception of disease transmission mechanisms and find how to control the spread of the COVID-19 disease. Xiao and Ruan (2007) studied an epidemic model with a non-monotonic incidence rate, which describes the psychological effect of certain serious diseases on the community when the number of infectives is getting larger. Xu and Ma (2009) investigated a SIR epidemic model with nonlinear incidence rate and time delay. Yang et al. (2010) formulated a SIR model with vaccination and varying population. Sun and Hsieh (2010) investigated an susceptible exposed infected recovered (SEIR) model with varying population size and vaccination strategy. Zhou and Cui (2011) studied an SEIR epidemic model with a saturated recovery rate. Bai and Zhou (2012) proposed an SEIRS epidemic model with a general periodic vaccination strategy and seasonally varying contact rates. Khan et al. (2015) considered an SEIR model with nonlinear saturated incidence rate and temporary immunity. Elkhaiar and Kaddar (2017) studied the dynamics of an SEIR epidemic model with nonlinear treatment function that takes into account the limited availability of resources in the community. Wang et al. (2018) extended the incidence rate of an SEIR epidemic model with relapse and varying total population size to a general nonlinear form. Tiwari et al. (2017) investigated an SEIRS epidemic model with nonlinear saturated incidence rate. Lahrouz et al. (2012) studied the global dynamics of a SIRS epidemic model for infections with non-permanent acquired immunity. Tian and Wang (2011) discussed the global stability analysis for several deterministic cholera epidemic models. Samanta (2011) discussed the permanence and extinction of a non-autonomous HIV/AIDS epidemic model with distributed time delay. Cai et al. (2014) investigated an HIV/AIDS treatment model.

Gralinski and Menachery (2020) studied the return of novel coronavirus in 2019. Chen et al. (2020) developed a mathematical model for calculating the transmissibility of the novel coronavirus. Saldana et al. (2020) developed a compartmental epidemic model to study the transmission dynamics of the COVID-19 epidemic outbreak, with Mexico as a practical example. Silva et al. (2020) proposed a new SEIR agent-based COVID-19 model to simulate the pandemic dynamics using a society of agents emulating people, business, and government. Pal et al. (2020) proposed a COVID-19 model for stability analysis with five compartments. Lee et al. (2020) proposed a COVID-19 epidemic model for estimating the unidentified infected population in China. Maheshwari et al. (2020) forecasted the epidemic spread of COVID-19 in India using the ARIMA model. Zakharov et al. (2020) predicted the dynamics of the COVID-19 epidemic in real-time using the case-based rate reasoning model. Bonnas and Gianatti (2020) proposed a COVID-19 epidemic model where the population is partitioned into classes corresponding to ages. Roda et al. (2020) demonstrated the reasons for wide variations in numerous model predictions of the COVID-19 epidemic in China. Liu et al. (2020a) developed two differential equations models to account for the latency period of COVID-19 infection. Basnarkov (2021) studied a SEAIR epidemic spreading model of COVID-19. Yang and Wang (2020) proposed a mathematical model for the novel coronavirus epidemic in Wuhan, China. Wang, Lu, et al. (2020) performed the dynamical analysis of a COVID-19 epidemic model. Zlatic et al. (2020) developed a COVID-19 epidemics model spreading on the availability of tests for the disease. Xue et al. (2020) proposed a data-driven network model for the COVID-19 epidemics in Wuhan, Toronto, and Italy. Neves and Guerrero (2020) presented the A-SIR model to predict the evolution of the COVID-19 epidemic. Ndairou et al. (2020) proposed a mathematical model for COVID-19 epidemic with a case study of Wuhan.

Jiao and Huang (2020) proposed a SIHR COVID-19 epidemic model with effective control strategies. Zhao and Chen (2020) modeled the epidemic dynamics and control of the COVID-19 outbreak in China. Li et al. (2020) modeled the impact of mass influenza vaccination and public health interventions on COVID-19 epidemics. Pizzuti et al. (2020) investigated the prediction accuracy of the SIR model on networks for Italy. Wang, Zheng, et al. (2020) used the logistic model and machine learning technics to predict the COVID-19 epidemics. Pongkitivanichkul et al. (2020) estimated the size of the COVID-19 epidemic outbreak. Liu et al. (2020b) predicted the cumulative number of cases for the COVID-19 epidemic in China. Zhu and Zhu (2020) devised a method to analyze the COVID-19 epidemic. Kantner and Koprucki (2020) computed a strategy for the case that a vaccine is never found and complete containment is impossible. Engbert et al. (2021) presented a Stochastic SEIR epidemic model for regional COVID-19 dynamics by sequential data assimilation. Several researcher investigated the dynamics of COVID-19 using fractional order models (Askar et al., 2021; Awais et al., 2020; Rezapour et al., 2020). Rihan et al. (2020) analyzed a stochastic SIRC epidemic model with time-delay for COVID-19. Bambusi and Ponno (2020) explained the linear behavior in COVID-19 epidemic as an effect of lockdown. Alberti and Faranda (2020) presented statistical predictions of COVID-19 infections by fitting asymptotic distributions to actual data. Abbasi et al. (2020) discussed the Optimal control for Impulsive SQEIAR Epidemic model on COVID-19 epidemic. Lobato et al. (2020) identified an epidemiological model to simulate the COVID-19 epidemic. Khan and Atangana (2020) modeled the dynamics of novel coronavirus with fractional derivative. Alshammari and Khan (2021) analyzed the dynamics of modified SIR model with nonlinear incidence and recovery rates. Pal et al. (2021) presented a COVID-19 model with optimal treatment of infected individuals and the cost of necessary treatment. Khan et al. (2021) focused on the novel coronal virus model to understand its dynamics and possible control. Khajanchi and Sarkar (2020) developed a new compartment model that explains the transmission dynamics of COVID-19. Rai et al. (2021) studied the social media advertisements in combating the coronavirus pandemic in India. Tuncer (2020) explored globalization's effect on the spread of fear across the world by focusing on the case of COVID-19. Adekola et al. (2020) examined various forms of mathematical models relevant to the containment, risk analysis, and features of COVID-19.

This paper determines the fate of coronavirus infective individuals introduced into the population in India. The dynamics of the nonlinear system have been considered in the study with reinfection turned off. The basic reproduction number (BRN) urn:x-wiley:14723891:media:pa2754:pa2754-math-0008 is estimated and analyzed as a threshold parameter for the stability analysis of the disease-free equilibrium (DFE) and endemic equilibrium. The uniform persistence of the disease near the threshold parameter is also determined.

2 FORMULATION OF COVID-19 MATHEMATICAL MODEL

The proposed COVID-19 model involves a specific postulate considered for developing mathematical modeling in the Indian perspective. Hypothetically, we imagine unknown infected peoples are spreading the diseases. Known infected peoples are isolated, so they are not able to spread the diseases. In the model, susceptible individuals enter into the unknown infected population by adequate personal contact with the unknown infected individuals given by non-monotonic incidence function urn:x-wiley:14723891:media:pa2754:pa2754-math-0009. Here urn:x-wiley:14723891:media:pa2754:pa2754-math-0010 describes the infection force of the disease and urn:x-wiley:14723891:media:pa2754:pa2754-math-0011 measures the inhibition effect from the behavioral change of the susceptible individuals when the number of infectious individuals increases. Some susceptible class individuals move to the reserved area, which is considered a safe zone during the pandemic. The known infected individuals entered the recovered class after recovered from the COVID-19. Here in this model, we consider the recovered class and the reserved class as the same and denote the density at time urn:x-wiley:14723891:media:pa2754:pa2754-math-0012 by urn:x-wiley:14723891:media:pa2754:pa2754-math-0013. The model of the study has been taken in the following form
urn:x-wiley:14723891:media:pa2754:pa2754-math-0014(1)
The above model is defined on the set urn:x-wiley:14723891:media:pa2754:pa2754-math-0015 subject to initial conditions
urn:x-wiley:14723891:media:pa2754:pa2754-math-0016(2)
where urn:x-wiley:14723891:media:pa2754:pa2754-math-0017 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0018 are the densities at the time urn:x-wiley:14723891:media:pa2754:pa2754-math-0019 of susceptible population, unknown infected population (incubate the illness but do not have any symptoms and not identified), known infected population (in the isolated ward), and recovered or reserved population, respectively, and the parameters urn:x-wiley:14723891:media:pa2754:pa2754-math-0020 urn:x-wiley:14723891:media:pa2754:pa2754-math-0021, urn:x-wiley:14723891:media:pa2754:pa2754-math-0022, urn:x-wiley:14723891:media:pa2754:pa2754-math-0023, urn:x-wiley:14723891:media:pa2754:pa2754-math-0024 urn:x-wiley:14723891:media:pa2754:pa2754-math-0025, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0026 are all positive. Here, urn:x-wiley:14723891:media:pa2754:pa2754-math-0027 is defined as the total number of population under risk at the time urn:x-wiley:14723891:media:pa2754:pa2754-math-0028 (Figure 1).
Details are in the caption following the image
Transfer diagram of the COVID-19 model

The biological meanings of the model parameters are listed below:

urn:x-wiley:14723891:media:pa2754:pa2754-math-0029 The recruitment rate at which new individuals enter the Indian population.

urn:x-wiley:14723891:media:pa2754:pa2754-math-0030 The homogeneous transmission coefficient from the susceptible population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0031) to the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0032). The rate of transmission of infection is given by urn:x-wiley:14723891:media:pa2754:pa2754-math-0033.

urn:x-wiley:14723891:media:pa2754:pa2754-math-0034 The parameter measures the psychological or inhibitory effect.

urn:x-wiley:14723891:media:pa2754:pa2754-math-0035 The transmission coefficient from the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0036) to the known infected population (treatment population) (urn:x-wiley:14723891:media:pa2754:pa2754-math-0037).

urn:x-wiley:14723891:media:pa2754:pa2754-math-0038 The transmission coefficient from the susceptible population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0039) to the recovered or reserved population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0040).

urn:x-wiley:14723891:media:pa2754:pa2754-math-0041 The transmission coefficient from the known infected population (treatment population) (urn:x-wiley:14723891:media:pa2754:pa2754-math-0042) to the recovered population or reserved population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0043).

urn:x-wiley:14723891:media:pa2754:pa2754-math-0044 The natural death rate.

urn:x-wiley:14723891:media:pa2754:pa2754-math-0045 The death rate of the known infected class (urn:x-wiley:14723891:media:pa2754:pa2754-math-0046).

The above mathematical model involves certain assumptions which is stated below:
  1. The susceptible population urn:x-wiley:14723891:media:pa2754:pa2754-math-0047 are those people who are not yet infected by the COVID-19 disease but may be infected when contacted with the unknown infected individuals urn:x-wiley:14723891:media:pa2754:pa2754-math-0048. One section of this susceptible population move directly to the reserved compartment which is also same as the recovered compartment (urn:x-wiley:14723891:media:pa2754:pa2754-math-0049)
  2. The unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0050) is composed of individuals who have COVID-19 infection without symptoms. These individuals are capable of infecting anyone who comes in contact with them.
  3. The known infected population urn:x-wiley:14723891:media:pa2754:pa2754-math-0051 is composed of individuals who have COVID-19 disease with symptoms and undergo best available treatment in isolation ward. The individuals in this compartment undergo the supportive care treatment or treatment to support the vital organs of the body. These individuals do not spread the COVID-19 disease as they are in isolation.
  4. The recovered population and reserved population together named as urn:x-wiley:14723891:media:pa2754:pa2754-math-0052 is composed of two kinds of individuals namely the individuals who are recovered from the COVID-19 disease after the best available treatment in the treatment compartment (urn:x-wiley:14723891:media:pa2754:pa2754-math-0053) and those individuals who move to the reserved or safer areas from the susceptible compartment (urn:x-wiley:14723891:media:pa2754:pa2754-math-0054).

3 ANALYSIS OF THE MODEL AND BASIC PROPERTIES

3.1 Non-negativity of solutions

Theorem 1.Every solution of the system (1) with initial conditions (2) are non-negative for every t urn:x-wiley:14723891:media:pa2754:pa2754-math-0055 0.

Proof.The right hand side of the dynamical system (1) is completely continuous and locally Lipschitzian on urn:x-wiley:14723891:media:pa2754:pa2754-math-0056 and hence the solution urn:x-wiley:14723891:media:pa2754:pa2754-math-0057 of the system (1) with the initial conditions (2) exists and is unique on the interval urn:x-wiley:14723891:media:pa2754:pa2754-math-0058 with urn:x-wiley:14723891:media:pa2754:pa2754-math-0059. From the first equation of the system (1) with initial condition urn:x-wiley:14723891:media:pa2754:pa2754-math-0060, we get

urn:x-wiley:14723891:media:pa2754:pa2754-math-0061
and hence
urn:x-wiley:14723891:media:pa2754:pa2754-math-0062
where
urn:x-wiley:14723891:media:pa2754:pa2754-math-0063

Integrating the second equation of the system (1) with initial condition urn:x-wiley:14723891:media:pa2754:pa2754-math-0064, the solution can be written in the form as

urn:x-wiley:14723891:media:pa2754:pa2754-math-0065
where
urn:x-wiley:14723891:media:pa2754:pa2754-math-0066

From the third and fourth equations of the system (1) with initial conditions urn:x-wiley:14723891:media:pa2754:pa2754-math-0067 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0068, we have

urn:x-wiley:14723891:media:pa2754:pa2754-math-0069
and hence
urn:x-wiley:14723891:media:pa2754:pa2754-math-0070
and
urn:x-wiley:14723891:media:pa2754:pa2754-math-0071
and hence
urn:x-wiley:14723891:media:pa2754:pa2754-math-0072

urn:x-wiley:14723891:media:pa2754:pa2754-math-0073. This completes the proof of the theorem.■

3.2 Boundedness of the system and invariant region

Theorem 2.All solutions of system (1) which lies in urn:x-wiley:14723891:media:pa2754:pa2754-math-0074 are uniformly bounded and are confined to the invariant region urn:x-wiley:14723891:media:pa2754:pa2754-math-0075 defined by urn:x-wiley:14723891:media:pa2754:pa2754-math-0076 as t urn:x-wiley:14723891:media:pa2754:pa2754-math-0077, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0078

Proof.Let us assume that urn:x-wiley:14723891:media:pa2754:pa2754-math-0079 is a solution of (1). Since,

urn:x-wiley:14723891:media:pa2754:pa2754-math-0080(3)

The time derivative of Equation (3) is

urn:x-wiley:14723891:media:pa2754:pa2754-math-0081

For each a urn:x-wiley:14723891:media:pa2754:pa2754-math-0082, we get

urn:x-wiley:14723891:media:pa2754:pa2754-math-0083

Assuming urn:x-wiley:14723891:media:pa2754:pa2754-math-0084, we get

urn:x-wiley:14723891:media:pa2754:pa2754-math-0085

Applying the theory of differential inequality (Birkhoff & Rota, 1989), we find that

urn:x-wiley:14723891:media:pa2754:pa2754-math-0086
which yields urn:x-wiley:14723891:media:pa2754:pa2754-math-0087 as urn:x-wiley:14723891:media:pa2754:pa2754-math-0088. Thus, all solutions of the COVID-19 system (1) which initiate in urn:x-wiley:14723891:media:pa2754:pa2754-math-0089 are uniformly bounded and confined to the region urn:x-wiley:14723891:media:pa2754:pa2754-math-0090, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0091. Hence the feasible region urn:x-wiley:14723891:media:pa2754:pa2754-math-0092 with initial conditions (2) is positively invariant region under the flow induced by the system (1) in urn:x-wiley:14723891:media:pa2754:pa2754-math-0093.■

Remark.All solutions of system (1) have non-negative components, given non-negative initial values in urn:x-wiley:14723891:media:pa2754:pa2754-math-0094 and stay in urn:x-wiley:14723891:media:pa2754:pa2754-math-0095 for t urn:x-wiley:14723891:media:pa2754:pa2754-math-0096 0 and globally attracting in urn:x-wiley:14723891:media:pa2754:pa2754-math-0097 with respect to the system (1). Therefore, we restrict our attention to the dynamics of the system (1) in urn:x-wiley:14723891:media:pa2754:pa2754-math-0098. Thus the system (1) with initial conditions (2) defined on urn:x-wiley:14723891:media:pa2754:pa2754-math-0099 is well-posed mathematically and epidemiologically and it is sufficient to study the dynamics of the dynamical system (1) with initial conditions (2) defined on urn:x-wiley:14723891:media:pa2754:pa2754-math-0100.

3.3 Equilibrium of system

To evaluate the equilibrium points of the system (1), we have to study the zero growth isoclines and the point of interaction. The possible steady-state boundary equilibrium point is urn:x-wiley:14723891:media:pa2754:pa2754-math-0101, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0102 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0103. Since the last equation of system (1) does not depend on other equations, we simply study the reduced system
urn:x-wiley:14723891:media:pa2754:pa2754-math-0104(4)
where urn:x-wiley:14723891:media:pa2754:pa2754-math-0105 is increasing when urn:x-wiley:14723891:media:pa2754:pa2754-math-0106 is small and decreasing when urn:x-wiley:14723891:media:pa2754:pa2754-math-0107 is large. The DFE point becomes urn:x-wiley:14723891:media:pa2754:pa2754-math-0108, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0109, urn:x-wiley:14723891:media:pa2754:pa2754-math-0110 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0111, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0112. The endemic equilibrium point of the system (4) is urn:x-wiley:14723891:media:pa2754:pa2754-math-0113, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0114, urn:x-wiley:14723891:media:pa2754:pa2754-math-0115, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0116. The endemic equilibrium point exists if urn:x-wiley:14723891:media:pa2754:pa2754-math-0117.

4 DFE AND STABILITY ANALYSIS

To eradicate the disease from a varying size population, the more stringent way requires that the total number of the virus-infected population urn:x-wiley:14723891:media:pa2754:pa2754-math-0118, while a weaker requirement is that proportion sum of the same tends to zero (Busenberg et al., 1991). Thus we need to find the conditions for the existence and stability of the DFE urn:x-wiley:14723891:media:pa2754:pa2754-math-0119 and the endemic equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0120. Therefore, urn:x-wiley:14723891:media:pa2754:pa2754-math-0121 is the DFE of (4), which exists for all positive parameters.

4.1 The basic reproduction number

The BRN is the average number of secondary infections generated by a single infection and is one of the most vital threshold quantities which mathematically represent the spreading of the virus infection.

The Jacobian matrix of system (4) at an arbitrary point urn:x-wiley:14723891:media:pa2754:pa2754-math-0122 becomes
urn:x-wiley:14723891:media:pa2754:pa2754-math-0123(5)

The stability of urn:x-wiley:14723891:media:pa2754:pa2754-math-0124 is equivalent to all the eigenvalues of the characteristic equation of urn:x-wiley:14723891:media:pa2754:pa2754-math-0125 at urn:x-wiley:14723891:media:pa2754:pa2754-math-0126 being with negative real parts, which can be assured by the BRN (urn:x-wiley:14723891:media:pa2754:pa2754-math-0127) obtained by the next-generation matrix method (Van den Driessche & Watmough, 2002), where urn:x-wiley:14723891:media:pa2754:pa2754-math-0128 is the epidemiological threshold parameter.

Let urn:x-wiley:14723891:media:pa2754:pa2754-math-0129. Then the system (1) can be written as
urn:x-wiley:14723891:media:pa2754:pa2754-math-0130
urn:x-wiley:14723891:media:pa2754:pa2754-math-0131
The Jacobian matrices of urn:x-wiley:14723891:media:pa2754:pa2754-math-0132 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0133 at the DFE urn:x-wiley:14723891:media:pa2754:pa2754-math-0134 are given by
urn:x-wiley:14723891:media:pa2754:pa2754-math-0135
from the above two matrices we get the matrices urn:x-wiley:14723891:media:pa2754:pa2754-math-0136 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0137 as below
urn:x-wiley:14723891:media:pa2754:pa2754-math-0138

The next generation matrix for the system (1) is urn:x-wiley:14723891:media:pa2754:pa2754-math-0139.

The spectral radius of the matrix urn:x-wiley:14723891:media:pa2754:pa2754-math-0140 is urn:x-wiley:14723891:media:pa2754:pa2754-math-0141 which is the BRN urn:x-wiley:14723891:media:pa2754:pa2754-math-0142. Now, it has been observed that urn:x-wiley:14723891:media:pa2754:pa2754-math-0143. From this observation, it is obvious that if the transmission coefficient urn:x-wiley:14723891:media:pa2754:pa2754-math-0144 from the susceptible population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0145) to unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0146) decreases, then the BRN urn:x-wiley:14723891:media:pa2754:pa2754-math-0147 also decreases and therefore reduces the burden on the infection. Otherwise, if urn:x-wiley:14723891:media:pa2754:pa2754-math-0148 increase, then urn:x-wiley:14723891:media:pa2754:pa2754-math-0149 would also increase, and thus, the transmission of virus infection will also rise; therefore, the scenario will be very harmful to society.

Now, the BRN urn:x-wiley:14723891:media:pa2754:pa2754-math-0150 has been presented graphically in Figure 2 with respect to related estimated or hypothetical parameter values given in Table 1. From Figure 2, it is observed that as the value of urn:x-wiley:14723891:media:pa2754:pa2754-math-0151 increases, urn:x-wiley:14723891:media:pa2754:pa2754-math-0152 also increases simultaneously and become greater than unity after a certain value of urn:x-wiley:14723891:media:pa2754:pa2754-math-0153. Therefore, it is said that up to a certain value of urn:x-wiley:14723891:media:pa2754:pa2754-math-0154, the DFE point is stable (Theorem 3) and beyond that value of urn:x-wiley:14723891:media:pa2754:pa2754-math-0155, the endemic equilibrium point is stable (Theorem 6).

Details are in the caption following the image
Change of urn:x-wiley:14723891:media:pa2754:pa2754-math-0156 with respect to urn:x-wiley:14723891:media:pa2754:pa2754-math-0157
TABLE 1. Parameters with their real field value
Parameters Value Reference
urn:x-wiley:14723891:media:pa2754:pa2754-math-0158 urn:x-wiley:14723891:media:pa2754:pa2754-math-0159 Estimated
urn:x-wiley:14723891:media:pa2754:pa2754-math-0160 urn:x-wiley:14723891:media:pa2754:pa2754-math-0161 Estimated
urn:x-wiley:14723891:media:pa2754:pa2754-math-0162 urn:x-wiley:14723891:media:pa2754:pa2754-math-0163 Assumed
urn:x-wiley:14723891:media:pa2754:pa2754-math-0164 urn:x-wiley:14723891:media:pa2754:pa2754-math-0165 Estimated
urn:x-wiley:14723891:media:pa2754:pa2754-math-0166 urn:x-wiley:14723891:media:pa2754:pa2754-math-0167 Assumed
urn:x-wiley:14723891:media:pa2754:pa2754-math-0168 urn:x-wiley:14723891:media:pa2754:pa2754-math-0169 Estimated
urn:x-wiley:14723891:media:pa2754:pa2754-math-0170 urn:x-wiley:14723891:media:pa2754:pa2754-math-0171 Estimated
urn:x-wiley:14723891:media:pa2754:pa2754-math-0172 urn:x-wiley:14723891:media:pa2754:pa2754-math-0173 Estimated

4.2 Local stability of the DFE

This section will discuss the parameter restrictions of the local stability of DFE.

Theorem 3.The disease free equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0174 of the system (4) is locally asymptotically stable if urn:x-wiley:14723891:media:pa2754:pa2754-math-0175. Whereas, it is unstable if urn:x-wiley:14723891:media:pa2754:pa2754-math-0176.

Proof.The variational matrix of the system (4) at urn:x-wiley:14723891:media:pa2754:pa2754-math-0177 is given by

urn:x-wiley:14723891:media:pa2754:pa2754-math-0178(6)

The eigen values of the characteristic equation of urn:x-wiley:14723891:media:pa2754:pa2754-math-0179 are

urn:x-wiley:14723891:media:pa2754:pa2754-math-0180

For stability, all eigen values must be negative. So, urn:x-wiley:14723891:media:pa2754:pa2754-math-0181 gives

urn:x-wiley:14723891:media:pa2754:pa2754-math-0182

Hence, the DFE is locally asymptotically stable if urn:x-wiley:14723891:media:pa2754:pa2754-math-0183.■

4.3 Global stability of the DFE

In this section, we will discuss the parameter restrictions of the global stability of DFE.

Theorem 4.When urn:x-wiley:14723891:media:pa2754:pa2754-math-0184, the disease free equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0185 is globally asymptotically stable in urn:x-wiley:14723891:media:pa2754:pa2754-math-0186.

Proof.To prove the global stability of DFE urn:x-wiley:14723891:media:pa2754:pa2754-math-0187 when urn:x-wiley:14723891:media:pa2754:pa2754-math-0188, we choose a suitable Lyapunov function urn:x-wiley:14723891:media:pa2754:pa2754-math-0189. Differentiating urn:x-wiley:14723891:media:pa2754:pa2754-math-0190 along (4), we obtain that

urn:x-wiley:14723891:media:pa2754:pa2754-math-0191

We observe that urn:x-wiley:14723891:media:pa2754:pa2754-math-0192 = 0 if and only if urn:x-wiley:14723891:media:pa2754:pa2754-math-0193. Therefore, the maximum invariant set in urn:x-wiley:14723891:media:pa2754:pa2754-math-0194 is the singleton set urn:x-wiley:14723891:media:pa2754:pa2754-math-0195, when urn:x-wiley:14723891:media:pa2754:pa2754-math-0196. By using Lasalle's invariance principle (LaSalle, 1976), the DFE urn:x-wiley:14723891:media:pa2754:pa2754-math-0197 is globally asymptotically stable in urn:x-wiley:14723891:media:pa2754:pa2754-math-0198, when urn:x-wiley:14723891:media:pa2754:pa2754-math-0199.■

5 DISEASE PERSISTENCE

5.1 Uniformly persistence

In this subsection, an effort is made to understand the uniform persistence of the dynamical system (4) for the threshold parameter by applying the acyclicity theorem (Sun & Hsieh, 2010).

Definition 1.The system (4) is said to be uniformly persistent (Butler et al., 1986) if there exists a constant urn:x-wiley:14723891:media:pa2754:pa2754-math-0200 such that all solutions urn:x-wiley:14723891:media:pa2754:pa2754-math-0201 with positive initial urn:x-wiley:14723891:media:pa2754:pa2754-math-0202 satisfy the following inequality

urn:x-wiley:14723891:media:pa2754:pa2754-math-0203(7)

Let urn:x-wiley:14723891:media:pa2754:pa2754-math-0204 be a locally compact metric space with metric urn:x-wiley:14723891:media:pa2754:pa2754-math-0205, and let urn:x-wiley:14723891:media:pa2754:pa2754-math-0206 is a closed non-empty subset of urn:x-wiley:14723891:media:pa2754:pa2754-math-0207 with the boundary urn:x-wiley:14723891:media:pa2754:pa2754-math-0208 and interior urn:x-wiley:14723891:media:pa2754:pa2754-math-0209. Clearly, urn:x-wiley:14723891:media:pa2754:pa2754-math-0210 is a closed subset of urn:x-wiley:14723891:media:pa2754:pa2754-math-0211 and let urn:x-wiley:14723891:media:pa2754:pa2754-math-0212 be a dynamical system on urn:x-wiley:14723891:media:pa2754:pa2754-math-0213. Then set urn:x-wiley:14723891:media:pa2754:pa2754-math-0214 in urn:x-wiley:14723891:media:pa2754:pa2754-math-0215 is said to be invariant if urn:x-wiley:14723891:media:pa2754:pa2754-math-0216.

Theorem 5.Suppose the conditions urn:x-wiley:14723891:media:pa2754:pa2754-math-0217 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0218 holds true for the dynamical system urn:x-wiley:14723891:media:pa2754:pa2754-math-0219

H1:.The system urn:x-wiley:14723891:media:pa2754:pa2754-math-0220 has a global attractor.

H2:.If urn:x-wiley:14723891:media:pa2754:pa2754-math-0221, then there exists a set

urn:x-wiley:14723891:media:pa2754:pa2754-math-0222 of disjoint, compact and isolated invariant sets in urn:x-wiley:14723891:media:pa2754:pa2754-math-0223 such that

  1. There are no subsets of M which form a cycle on urn:x-wiley:14723891:media:pa2754:pa2754-math-0224;
  2. urn:x-wiley:14723891:media:pa2754:pa2754-math-0225, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0226 is the omega limit set of urn:x-wiley:14723891:media:pa2754:pa2754-math-0227
  3. Every set urn:x-wiley:14723891:media:pa2754:pa2754-math-0228 is isolated in urn:x-wiley:14723891:media:pa2754:pa2754-math-0229, 1 urn:x-wiley:14723891:media:pa2754:pa2754-math-0230 i urn:x-wiley:14723891:media:pa2754:pa2754-math-0231
  4. urn:x-wiley:14723891:media:pa2754:pa2754-math-0232 for urn:x-wiley:14723891:media:pa2754:pa2754-math-0233, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0234 is a stable manifold of urn:x-wiley:14723891:media:pa2754:pa2754-math-0235.

Then the dynamical system urn:x-wiley:14723891:media:pa2754:pa2754-math-0236 is uniformly persistent with respect to urn:x-wiley:14723891:media:pa2754:pa2754-math-0237.

Proof.For the modified COVID-19 system (4), we assume that

urn:x-wiley:14723891:media:pa2754:pa2754-math-0238 = urn:x-wiley:14723891:media:pa2754:pa2754-math-0239: urn:x-wiley:14723891:media:pa2754:pa2754-math-0240, urn:x-wiley:14723891:media:pa2754:pa2754-math-0241 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0242. Clearly, urn:x-wiley:14723891:media:pa2754:pa2754-math-0243. On urn:x-wiley:14723891:media:pa2754:pa2754-math-0244, the system (4) reduces to urn:x-wiley:14723891:media:pa2754:pa2754-math-0245, in which urn:x-wiley:14723891:media:pa2754:pa2754-math-0246 as urn:x-wiley:14723891:media:pa2754:pa2754-math-0247. So it is concluded that urn:x-wiley:14723891:media:pa2754:pa2754-math-0248 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0249 for all urn:x-wiley:14723891:media:pa2754:pa2754-math-0250 urn:x-wiley:14723891:media:pa2754:pa2754-math-0251 which proves (i) and (ii) of urn:x-wiley:14723891:media:pa2754:pa2754-math-0252. From Theorem 3 the DFE urn:x-wiley:14723891:media:pa2754:pa2754-math-0253 is unstable When urn:x-wiley:14723891:media:pa2754:pa2754-math-0254 and also urn:x-wiley:14723891:media:pa2754:pa2754-math-0255 which indicates that (iii) and (iv) of urn:x-wiley:14723891:media:pa2754:pa2754-math-0256 are satisfied. Since all system (4) solutions are uniformly bounded, a global attractor exists and hence urn:x-wiley:14723891:media:pa2754:pa2754-math-0257 holds true for the system (4). Hence the system (4) is uniformly persistent with respect to urn:x-wiley:14723891:media:pa2754:pa2754-math-0258, when urn:x-wiley:14723891:media:pa2754:pa2754-math-0259.■

6 ENDEMIC EQUILIBRIUM AND STABILITY ANALYSIS

From Theorem 4, it is already observed that DFE is globally asymptotically stable when urn:x-wiley:14723891:media:pa2754:pa2754-math-0260 which implies that there is no endemic equilibrium when urn:x-wiley:14723891:media:pa2754:pa2754-math-0261. To analyze the existence of nontrivial interior equilibrium of system (4), it should satisfy the following conditions:
urn:x-wiley:14723891:media:pa2754:pa2754-math-0262(8)
with urn:x-wiley:14723891:media:pa2754:pa2754-math-0263 and the above Equations (9) leads to the following solutions as urn:x-wiley:14723891:media:pa2754:pa2754-math-0264, urn:x-wiley:14723891:media:pa2754:pa2754-math-0265, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0266. Clearly urn:x-wiley:14723891:media:pa2754:pa2754-math-0267 but urn:x-wiley:14723891:media:pa2754:pa2754-math-0268 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0269 are positive if urn:x-wiley:14723891:media:pa2754:pa2754-math-0270. Hence the nontrivial interior equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0271 of system (4) exists if urn:x-wiley:14723891:media:pa2754:pa2754-math-0272.

6.1 Local stability analysis of the endemic equilibrium

Theorem 6.The endemic equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0273 of the system (4) is locally asymptotically stable in urn:x-wiley:14723891:media:pa2754:pa2754-math-0274 if urn:x-wiley:14723891:media:pa2754:pa2754-math-0275.

Proof.The variational matrix of the system (4) at urn:x-wiley:14723891:media:pa2754:pa2754-math-0276 is

urn:x-wiley:14723891:media:pa2754:pa2754-math-0277
where
urn:x-wiley:14723891:media:pa2754:pa2754-math-0278

The characteristic equation of urn:x-wiley:14723891:media:pa2754:pa2754-math-0279 is

urn:x-wiley:14723891:media:pa2754:pa2754-math-0280(9)
where urn:x-wiley:14723891:media:pa2754:pa2754-math-0281 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0282. One of the eigenvalues of urn:x-wiley:14723891:media:pa2754:pa2754-math-0283 from the Equation (10) is urn:x-wiley:14723891:media:pa2754:pa2754-math-0284 which is negative. The Routh–Hurwitz conditions state that the quadratic equation urn:x-wiley:14723891:media:pa2754:pa2754-math-0285 has negative roots or complex conjugates with negative real part if and only if urn:x-wiley:14723891:media:pa2754:pa2754-math-0286 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0287. But after simplification, we get
urn:x-wiley:14723891:media:pa2754:pa2754-math-0288

Obviously urn:x-wiley:14723891:media:pa2754:pa2754-math-0289 for urn:x-wiley:14723891:media:pa2754:pa2754-math-0290. Hence, the positive equilibrium point urn:x-wiley:14723891:media:pa2754:pa2754-math-0291 is locally asymptotically stable if urn:x-wiley:14723891:media:pa2754:pa2754-math-0292.■

6.2 Global stability analysis of the endemic equilibrium

To investigate the globally stability of the endemic equilibrium of system (4) when urn:x-wiley:14723891:media:pa2754:pa2754-math-0293, we apply here a geometric approach (Li & Muldowney, 1996). We begin the preliminary discussion on the geometric approach by formulating the local version of the urn:x-wiley:14723891:media:pa2754:pa2754-math-0294 closing lemma of Pugh (Hirsch, 1991). Consider the differential equation
urn:x-wiley:14723891:media:pa2754:pa2754-math-0295(10)
where urn:x-wiley:14723891:media:pa2754:pa2754-math-0296, urn:x-wiley:14723891:media:pa2754:pa2754-math-0297 open set, simply connected and urn:x-wiley:14723891:media:pa2754:pa2754-math-0298.

Let urn:x-wiley:14723891:media:pa2754:pa2754-math-0299 be an urn:x-wiley:14723891:media:pa2754:pa2754-math-0300 matrix valued function which is urn:x-wiley:14723891:media:pa2754:pa2754-math-0301 in urn:x-wiley:14723891:media:pa2754:pa2754-math-0302 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0303, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0304 is the matrix obtained by replacing each entry urn:x-wiley:14723891:media:pa2754:pa2754-math-0305 in urn:x-wiley:14723891:media:pa2754:pa2754-math-0306 by its directional derivative in the direction of urn:x-wiley:14723891:media:pa2754:pa2754-math-0307. Let urn:x-wiley:14723891:media:pa2754:pa2754-math-0308 be the second additive compound matrix of urn:x-wiley:14723891:media:pa2754:pa2754-math-0309 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0310 be the Lozinskii measure (Coppel, 1965) with respect to a vector norm urn:x-wiley:14723891:media:pa2754:pa2754-math-0311 on urn:x-wiley:14723891:media:pa2754:pa2754-math-0312 defined as urn:x-wiley:14723891:media:pa2754:pa2754-math-0313, I is the unit matrix.

The following quantity urn:x-wiley:14723891:media:pa2754:pa2754-math-0314 urn:x-wiley:14723891:media:pa2754:pa2754-math-0315 is well defined. If there exists a compact absorbing set urn:x-wiley:14723891:media:pa2754:pa2754-math-0316 and the system (11) has a unique equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0317 in urn:x-wiley:14723891:media:pa2754:pa2754-math-0318, then the unique equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0319 of (11) is globally asymptotically stable in urn:x-wiley:14723891:media:pa2754:pa2754-math-0320 if urn:x-wiley:14723891:media:pa2754:pa2754-math-0321.

Theorem 7.Assume that urn:x-wiley:14723891:media:pa2754:pa2754-math-0322. Then there exist urn:x-wiley:14723891:media:pa2754:pa2754-math-0323 such that the unique endemic equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0324 is globally asymptotically stable in the interior of urn:x-wiley:14723891:media:pa2754:pa2754-math-0325 when urn:x-wiley:14723891:media:pa2754:pa2754-math-0326.

Proof.To prove this result, we find the second additive compound matrix urn:x-wiley:14723891:media:pa2754:pa2754-math-0327 from the Jacobian matrix urn:x-wiley:14723891:media:pa2754:pa2754-math-0328 of (5) for the reduced system (4) at urn:x-wiley:14723891:media:pa2754:pa2754-math-0329 in the following form:

urn:x-wiley:14723891:media:pa2754:pa2754-math-0330(11)
where
urn:x-wiley:14723891:media:pa2754:pa2754-math-0331
and the matrix function urn:x-wiley:14723891:media:pa2754:pa2754-math-0332 is defined by urn:x-wiley:14723891:media:pa2754:pa2754-math-0333 with urn:x-wiley:14723891:media:pa2754:pa2754-math-0334. Then urn:x-wiley:14723891:media:pa2754:pa2754-math-0335. Therefore, the matrix urn:x-wiley:14723891:media:pa2754:pa2754-math-0336 can be written in the following block form as
urn:x-wiley:14723891:media:pa2754:pa2754-math-0337
where urn:x-wiley:14723891:media:pa2754:pa2754-math-0338, urn:x-wiley:14723891:media:pa2754:pa2754-math-0339, urn:x-wiley:14723891:media:pa2754:pa2754-math-0340 and
urn:x-wiley:14723891:media:pa2754:pa2754-math-0341

The vector norm urn:x-wiley:14723891:media:pa2754:pa2754-math-0342 of the vector urn:x-wiley:14723891:media:pa2754:pa2754-math-0343 in urn:x-wiley:14723891:media:pa2754:pa2754-math-0344 can be defined as urn:x-wiley:14723891:media:pa2754:pa2754-math-0345. Suppose urn:x-wiley:14723891:media:pa2754:pa2754-math-0346 be the Lozinskii measure with the above defined norm, so as described in (Martin, 1974) and it follows the condition as urn:x-wiley:14723891:media:pa2754:pa2754-math-0347, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0348, urn:x-wiley:14723891:media:pa2754:pa2754-math-0349, urn:x-wiley:14723891:media:pa2754:pa2754-math-0350, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0351 are the matrix norm with respect to the urn:x-wiley:14723891:media:pa2754:pa2754-math-0352 vector norm. If urn:x-wiley:14723891:media:pa2754:pa2754-math-0353 denotes the Lozinskii measure with respect to urn:x-wiley:14723891:media:pa2754:pa2754-math-0354 norm. Using the second equation of system (4), we have

urn:x-wiley:14723891:media:pa2754:pa2754-math-0359

Using the third equation of system (4), we have

urn:x-wiley:14723891:media:pa2754:pa2754-math-0360

Since system (4) is uniformly persistent when urn:x-wiley:14723891:media:pa2754:pa2754-math-0361, there exist urn:x-wiley:14723891:media:pa2754:pa2754-math-0362 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0363 such that urn:x-wiley:14723891:media:pa2754:pa2754-math-0364 implies urn:x-wiley:14723891:media:pa2754:pa2754-math-0365, urn:x-wiley:14723891:media:pa2754:pa2754-math-0366, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0367 for all urn:x-wiley:14723891:media:pa2754:pa2754-math-0368. If urn:x-wiley:14723891:media:pa2754:pa2754-math-0369, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0370, then urn:x-wiley:14723891:media:pa2754:pa2754-math-0371. Therefore, we get urn:x-wiley:14723891:media:pa2754:pa2754-math-0372. Hence,

urn:x-wiley:14723891:media:pa2754:pa2754-math-0373
which implies that urn:x-wiley:14723891:media:pa2754:pa2754-math-0374. Thus, the endemic equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0375 of the reduced system (4) is globally asymptotically stable, when urn:x-wiley:14723891:media:pa2754:pa2754-math-0376.■

7 DISCUSSION AND SIMULATIONS

In this section, firstly we consider the case when the BRN urn:x-wiley:14723891:media:pa2754:pa2754-math-0377 by utilizing the parameter values as in Table 1. For different initial conditions, the dynamics of the system (4) is represented in Figure 3. These figures illustrate that the susceptible population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0378) persists and tends to urn:x-wiley:14723891:media:pa2754:pa2754-math-0379 as urn:x-wiley:14723891:media:pa2754:pa2754-math-0380 and the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0381) and the known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0382) tends to zero as urn:x-wiley:14723891:media:pa2754:pa2754-math-0383, that is, the system (4) approaches the DFE urn:x-wiley:14723891:media:pa2754:pa2754-math-0384. This numerical simulation supports the result stated in Theorem 4. Next, we consider the case when urn:x-wiley:14723891:media:pa2754:pa2754-math-0385 by utilizing the values of parameter from Table 1 with urn:x-wiley:14723891:media:pa2754:pa2754-math-0386. For various initial conditions, the dynamics of the system (4) is represented in Figure 4. These figures illustrate that the susceptible population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0387), the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0388) and the known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0389) all persist, that is, the system (4) tends to endemic equilibrium urn:x-wiley:14723891:media:pa2754:pa2754-math-0390.

Details are in the caption following the image
Time series plot of urn:x-wiley:14723891:media:pa2754:pa2754-math-0391 (a), urn:x-wiley:14723891:media:pa2754:pa2754-math-0392 (b), urn:x-wiley:14723891:media:pa2754:pa2754-math-0393 (c) when urn:x-wiley:14723891:media:pa2754:pa2754-math-0394 for different initial conditions using parameter values from Table 1
Details are in the caption following the image
Time series plot of urn:x-wiley:14723891:media:pa2754:pa2754-math-0395 (a), urn:x-wiley:14723891:media:pa2754:pa2754-math-0396 (b), urn:x-wiley:14723891:media:pa2754:pa2754-math-0397 (c) when urn:x-wiley:14723891:media:pa2754:pa2754-math-0398 for different initial conditions with parameter values from Table 1 with urn:x-wiley:14723891:media:pa2754:pa2754-math-0399

To determine the outbreak of infected individuals of COVID-19 disease in the Indian population, we present the numerical simulation of the proposed dynamical system (1), using MATLAB for simulation experiments, based on the SARS-CoV-2 virus-infected cases in the time frame in India. Here, we employ the nonlinear least-squares curve fitting method with the help of “fminsearch” function from the MATLAB Optimization Toolbox to obtain the best-fit parameters for INDIA. The procedure looks for the set of initial guesses and pre-estimated parameters for the model whose solutions best fit or pass through all the data points by reducing the sum of the square difference between the observed data and the model solution, that is, If a theoretical model urn:x-wiley:14723891:media:pa2754:pa2754-math-0400 is attained and depend on a few unknown parameters urn:x-wiley:14723891:media:pa2754:pa2754-math-0401 and a sequence of actual data points urn:x-wiley:14723891:media:pa2754:pa2754-math-0402 is also at hand then the aim is to obtain values of the parameters so that the error urn:x-wiley:14723891:media:pa2754:pa2754-math-0403 calculated can attain a minimum, where urn:x-wiley:14723891:media:pa2754:pa2754-math-0404.

For simulation, we assume the initial values are urn:x-wiley:14723891:media:pa2754:pa2754-math-0405, urn:x-wiley:14723891:media:pa2754:pa2754-math-0406, urn:x-wiley:14723891:media:pa2754:pa2754-math-0407 from March 25 to April 14, 2020 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0408, urn:x-wiley:14723891:media:pa2754:pa2754-math-0409, urn:x-wiley:14723891:media:pa2754:pa2754-math-0410 from April 15 to April 20, 2020.

Figures 5-8 are drawn based on the parameter values (shown in Table 1). The values of the parameters are fixed based on the following real-time data of India, as shown in Table 2, the spread of the COVID-19 disease during the lockdown period is recorded as follows (MoHFW, 2021)

Details are in the caption following the image
Time history of the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0411) and known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0412) for urn:x-wiley:14723891:media:pa2754:pa2754-math-0413 urn:x-wiley:14723891:media:pa2754:pa2754-math-0414, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0415
Details are in the caption following the image
Time history of the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0416) and known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0417) for urn:x-wiley:14723891:media:pa2754:pa2754-math-0418 urn:x-wiley:14723891:media:pa2754:pa2754-math-0419, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0420
Details are in the caption following the image
Time history of the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0421) and known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0422) for urn:x-wiley:14723891:media:pa2754:pa2754-math-0423 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0424
Details are in the caption following the image
Long run prediction of the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0425) and known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0426) for urn:x-wiley:14723891:media:pa2754:pa2754-math-0427 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0428
TABLE 2. COVID-19 active cases in India from 25th March to 20th April, 2020
Date urn:x-wiley:14723891:media:pa2754:pa2754-math-0429 urn:x-wiley:14723891:media:pa2754:pa2754-math-0430 urn:x-wiley:14723891:media:pa2754:pa2754-math-0431 urn:x-wiley:14723891:media:pa2754:pa2754-math-0432 urn:x-wiley:14723891:media:pa2754:pa2754-math-0433 urn:x-wiley:14723891:media:pa2754:pa2754-math-0434 urn:x-wiley:14723891:media:pa2754:pa2754-math-0435 urn:x-wiley:14723891:media:pa2754:pa2754-math-0436 urn:x-wiley:14723891:media:pa2754:pa2754-math-0437
Active cases urn:x-wiley:14723891:media:pa2754:pa2754-math-0438 urn:x-wiley:14723891:media:pa2754:pa2754-math-0439 urn:x-wiley:14723891:media:pa2754:pa2754-math-0440 urn:x-wiley:14723891:media:pa2754:pa2754-math-0441 urn:x-wiley:14723891:media:pa2754:pa2754-math-0442 urn:x-wiley:14723891:media:pa2754:pa2754-math-0443 urn:x-wiley:14723891:media:pa2754:pa2754-math-0444 urn:x-wiley:14723891:media:pa2754:pa2754-math-0445 urn:x-wiley:14723891:media:pa2754:pa2754-math-0446
Date urn:x-wiley:14723891:media:pa2754:pa2754-math-0447 urn:x-wiley:14723891:media:pa2754:pa2754-math-0448 urn:x-wiley:14723891:media:pa2754:pa2754-math-0449 urn:x-wiley:14723891:media:pa2754:pa2754-math-0450 urn:x-wiley:14723891:media:pa2754:pa2754-math-0451 urn:x-wiley:14723891:media:pa2754:pa2754-math-0452 urn:x-wiley:14723891:media:pa2754:pa2754-math-0453 urn:x-wiley:14723891:media:pa2754:pa2754-math-0454 urn:x-wiley:14723891:media:pa2754:pa2754-math-0455
Active cases urn:x-wiley:14723891:media:pa2754:pa2754-math-0456 urn:x-wiley:14723891:media:pa2754:pa2754-math-0457 urn:x-wiley:14723891:media:pa2754:pa2754-math-0458 urn:x-wiley:14723891:media:pa2754:pa2754-math-0459 urn:x-wiley:14723891:media:pa2754:pa2754-math-0460 urn:x-wiley:14723891:media:pa2754:pa2754-math-0461 urn:x-wiley:14723891:media:pa2754:pa2754-math-0462 urn:x-wiley:14723891:media:pa2754:pa2754-math-0463 urn:x-wiley:14723891:media:pa2754:pa2754-math-0464
Date urn:x-wiley:14723891:media:pa2754:pa2754-math-0465 urn:x-wiley:14723891:media:pa2754:pa2754-math-0466 urn:x-wiley:14723891:media:pa2754:pa2754-math-0467 urn:x-wiley:14723891:media:pa2754:pa2754-math-0468 urn:x-wiley:14723891:media:pa2754:pa2754-math-0469 urn:x-wiley:14723891:media:pa2754:pa2754-math-0470 urn:x-wiley:14723891:media:pa2754:pa2754-math-0471 urn:x-wiley:14723891:media:pa2754:pa2754-math-0472 urn:x-wiley:14723891:media:pa2754:pa2754-math-0473
Active cases urn:x-wiley:14723891:media:pa2754:pa2754-math-0474 urn:x-wiley:14723891:media:pa2754:pa2754-math-0475 urn:x-wiley:14723891:media:pa2754:pa2754-math-0476 urn:x-wiley:14723891:media:pa2754:pa2754-math-0477 urn:x-wiley:14723891:media:pa2754:pa2754-math-0478 urn:x-wiley:14723891:media:pa2754:pa2754-math-0479 urn:x-wiley:14723891:media:pa2754:pa2754-math-0480 urn:x-wiley:14723891:media:pa2754:pa2754-math-0481 urn:x-wiley:14723891:media:pa2754:pa2754-math-0482

Figure 5 has been drawn for the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0483) and known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0484) for urn:x-wiley:14723891:media:pa2754:pa2754-math-0485 urn:x-wiley:14723891:media:pa2754:pa2754-math-0486, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0487 for the specified period from March 25 to April 14, 2020 during the first lockdown. This figure is fascinating because it is observed that for urn:x-wiley:14723891:media:pa2754:pa2754-math-0488, the known infected population curve of our proposed system fits to the curve of the real confirmed infected individuals in India during the above said period.

Figure 6 shows the time history of the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0489) and known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0490) for urn:x-wiley:14723891:media:pa2754:pa2754-math-0491 urn:x-wiley:14723891:media:pa2754:pa2754-math-0492, and urn:x-wiley:14723891:media:pa2754:pa2754-math-0493 for the period from April 15 to April 20, 2020 during the second lockdown situation. Figure 10 is very interesting because it is observed that for urn:x-wiley:14723891:media:pa2754:pa2754-math-0494, the known infected population curve of our proposed COVID-19 system fits to the curve of the real confirmed infected individuals in India during the above said period.

Figure 7 shows that the time history of the unknown infected (urn:x-wiley:14723891:media:pa2754:pa2754-math-0495) and known infected (urn:x-wiley:14723891:media:pa2754:pa2754-math-0496) populations of the proposed system corresponding to urn:x-wiley:14723891:media:pa2754:pa2754-math-0497 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0498 fits to the curve of the real confirmed infected individuals in India during the lockdown period from March 25 to April 20, 2020.

It is also clear that urn:x-wiley:14723891:media:pa2754:pa2754-math-0499 as a representative of lack of following the good practices such as proper hand wash, sanitizing the places, nasal, and oral covering with a mask, social distancing has an effect in the proposed coronavirus model and an increase in urn:x-wiley:14723891:media:pa2754:pa2754-math-0500 means many individuals are not following the good practices as said above and as a result, many individuals gets infected and move to the unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0501). Long run prediction of the time history of the known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0502) for urn:x-wiley:14723891:media:pa2754:pa2754-math-0503 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0504 is drawn in Figure 8, which shows that the disease gets diminished may be due to the availability of a Vaccine.

From Figure 8, it is observed that the active cases will decrease and the COVID-19 disease will persist in the society for a long period. Furthermore, it is noticed that the COVID-19 disease diminishes after a long period if people do not strictly follow the government guidelines and vaccination is not found at the earliest as we have considered that geographical and climatic factors do not have any impact on this virus infection.

From Figure 9, it is noticed that if urn:x-wiley:14723891:media:pa2754:pa2754-math-0505 increases, which is a representative of the identification process of the infected individuals, then the unknown infected population reduces and hence we can identify the individuals for quarantine. Thus, the lockdown period can be reduced and people can come back to a normal situation.

Details are in the caption following the image
Unknown infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0506) with time for corresponding the value of urn:x-wiley:14723891:media:pa2754:pa2754-math-0507 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0508

Figure 10 shows that if the recovery rate urn:x-wiley:14723891:media:pa2754:pa2754-math-0509 increases, which representing the quality of treatment and cooperation of the patient to the treatment, then the known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0510) tends to zero in the long run. Hence, the rapid spread of COVID-19 disease is reduced drastically.

Details are in the caption following the image
Known infected population (urn:x-wiley:14723891:media:pa2754:pa2754-math-0511) with time with the recovery rate urn:x-wiley:14723891:media:pa2754:pa2754-math-0512 and urn:x-wiley:14723891:media:pa2754:pa2754-math-0513

Figure 11 represents the graphical representation of the day-wise increase of infected, recovered, and deceased population from March 1 to March 20, 2020 in India (COVID19 tracker, 2021). It is observed that active infected cases start to increase from the third week of March because many have already been infected, failed to be in isolation, not strictly adhering to the rules imposed by the Government and ICMR at the time of the second week of March, and hence the active cases increases but in control during the first lock downstage. It is also observed that the day-wise recovered cases are also increasing and day-wise deceased cases are very low. From the above discussions, it can be said that SARS-COV-2 is threatening to the society, but not deadly dangerous until now in Indian perspective.

Details are in the caption following the image
Day wise infected, recovered, and deceased population from 1st to 20th March 2020 in India

8 CONCLUSION

The proposed model has determined the outbreak of COVID-19 disease in the Indian population. The BRN urn:x-wiley:14723891:media:pa2754:pa2754-math-0514 is the threshold limit that determines the dynamical proliferation. The reproduction number urn:x-wiley:14723891:media:pa2754:pa2754-math-0515 decreases if the transmission coefficient urn:x-wiley:14723891:media:pa2754:pa2754-math-0516 decreases. If urn:x-wiley:14723891:media:pa2754:pa2754-math-0517 increases, then the transmission of COVID-19 disease increases and is very harmful to society. The system has a unique DFE urn:x-wiley:14723891:media:pa2754:pa2754-math-0518, which is globally stable if urn:x-wiley:14723891:media:pa2754:pa2754-math-0519 which symbolizes that the disease diminishes eventually. When urn:x-wiley:14723891:media:pa2754:pa2754-math-0520, the system is uniformly persistent under some conditions, a unique endemic equilibrium is globally stable. The study shows that the infected population who incubate the illness of our proposed system fits well to the real confirmed infected individuals in India during the lockdown period.

By observing the time graph of the known infected class (urn:x-wiley:14723891:media:pa2754:pa2754-math-0521) for various values of urn:x-wiley:14723891:media:pa2754:pa2754-math-0522, we conclude that if people do not strictly follow the guidelines and lockdown measures imposed by the Government of India to prevent the rapid spread of the infection, the situation will be out of control.

ACKNOWLEDGMENTS

We are grateful to the editor and anonymous referees for their careful reading, valuable comments, and helpful suggestions which have helped us to improve the presentation of this work significantly.

    CONFLICT OF INTEREST

    The authors declare no conflicts of interest.

    AUTHOR CONTRIBUTIONS

    Analysis and draft the paper: R. Prem Kumar and Sanjoy Basu. Collected the data, conceived and designed the analysis, perform the analysis tool for the paper: D. Ghosh and P. K. Santra. Supervised, designed the analysis and wrote the paper: G. S. Mahapatra.

    CONSENT TO PARTICIPATE

    This article does not contain any studies involving animals or human participants performed by any authors. Anyone can read material published in the Journal.

    CONSENT FOR PUBLICATION

    We, the undersigned, give our consent for the publication of identifiable details, which can include figures and details within the text (“Material”) to be published in the above Journal and Article. Therefore, anyone can read material published in the Journal.

    NOMENCLATURE

  1. urn:x-wiley:14723891:media:pa2754:pa2754-math-0523
  2. urn:x-wiley:14723891:media:pa2754:pa2754-math-0524 is the set on which the dynamical system is defined
  3. urn:x-wiley:14723891:media:pa2754:pa2754-math-0525
  4. 4-dimensional positive real space
  5. urn:x-wiley:14723891:media:pa2754:pa2754-math-0526
  6. the set of all real numbers
  7. urn:x-wiley:14723891:media:pa2754:pa2754-math-0527
  8. the total number of population at time t
  9. urn:x-wiley:14723891:media:pa2754:pa2754-math-0528
  10. urn:x-wiley:14723891:media:pa2754:pa2754-math-0529 is the non-monotonic incidence function
  11. urn:x-wiley:14723891:media:pa2754:pa2754-math-0530
  12. urn:x-wiley:14723891:media:pa2754:pa2754-math-0531 used for simplifying big expressions in Theorem 1
  13. urn:x-wiley:14723891:media:pa2754:pa2754-math-0532
  14. urn:x-wiley:14723891:media:pa2754:pa2754-math-0533 used for simplifying big expressions in Theorem 1
  15. urn:x-wiley:14723891:media:pa2754:pa2754-math-0534
  16. urn:x-wiley:14723891:media:pa2754:pa2754-math-0535 which is positively invariant region in urn:x-wiley:14723891:media:pa2754:pa2754-math-0536 for the system (1)
  17. urn:x-wiley:14723891:media:pa2754:pa2754-math-0537
  18. urn:x-wiley:14723891:media:pa2754:pa2754-math-0538 urn:x-wiley:14723891:media:pa2754:pa2754-math-0539
  19. urn:x-wiley:14723891:media:pa2754:pa2754-math-0540
  20. urn:x-wiley:14723891:media:pa2754:pa2754-math-0541 which is positively invariant region in urn:x-wiley:14723891:media:pa2754:pa2754-math-0542 for the reduced system (4)
  21. urn:x-wiley:14723891:media:pa2754:pa2754-math-0543
  22. the disease free equilibrium of the reduced system (4)
  23. urn:x-wiley:14723891:media:pa2754:pa2754-math-0544
  24. the endemic equilibrium of the reduced system (4)
  25. urn:x-wiley:14723891:media:pa2754:pa2754-math-0545, urn:x-wiley:14723891:media:pa2754:pa2754-math-0546, urn:x-wiley:14723891:media:pa2754:pa2754-math-0547
  26. the coordinates of the endemic equilibrium point urn:x-wiley:14723891:media:pa2754:pa2754-math-0548 of the reduced system (4)
  27. urn:x-wiley:14723891:media:pa2754:pa2754-math-0549
  28. the Jacobian or variational matrix of the system (4) evaluated at the disease free equilibrium point urn:x-wiley:14723891:media:pa2754:pa2754-math-0550
  29. urn:x-wiley:14723891:media:pa2754:pa2754-math-0551
  30. the Jacobian or variational matrix of the system (4) evaluated at the endemic equilibrium point urn:x-wiley:14723891:media:pa2754:pa2754-math-0552
  31. urn:x-wiley:14723891:media:pa2754:pa2754-math-0553
  32. basic reproduction number
  33. urn:x-wiley:14723891:media:pa2754:pa2754-math-0554
  34. these standard symbols are used in the calculation of the basic reproduction number urn:x-wiley:14723891:media:pa2754:pa2754-math-0555 as per the cited reference used for calculation
  35. urn:x-wiley:14723891:media:pa2754:pa2754-math-0556
  36. the eigen values of the characteristic equation of urn:x-wiley:14723891:media:pa2754:pa2754-math-0557
  37. urn:x-wiley:14723891:media:pa2754:pa2754-math-0558
  38. Lyapunov function chosen to prove the global stability of the disease free equilibrium
  39. urn:x-wiley:14723891:media:pa2754:pa2754-math-0559
  40. the positive constant in Lyapunov function urn:x-wiley:14723891:media:pa2754:pa2754-math-0560
  41. urn:x-wiley:14723891:media:pa2754:pa2754-math-0561
  42. the initial conditions for the reduced system (4)
  43. urn:x-wiley:14723891:media:pa2754:pa2754-math-0562
  44. locally compact metric space used in the introduction of the uniform persistence theorem
  45. urn:x-wiley:14723891:media:pa2754:pa2754-math-0563
  46. the metric for the metric space X
  47. urn:x-wiley:14723891:media:pa2754:pa2754-math-0564
  48. a closed non-empty subset of urn:x-wiley:14723891:media:pa2754:pa2754-math-0565 used in the introduction of the uniform persistence theorem
  49. urn:x-wiley:14723891:media:pa2754:pa2754-math-0566
  50. the boundary of urn:x-wiley:14723891:media:pa2754:pa2754-math-0567
  51. urn:x-wiley:14723891:media:pa2754:pa2754-math-0568
  52. the interior of urn:x-wiley:14723891:media:pa2754:pa2754-math-0569
  53. urn:x-wiley:14723891:media:pa2754:pa2754-math-0570
  54. it is a dynamical system
  55. urn:x-wiley:14723891:media:pa2754:pa2754-math-0571
  56. urn:x-wiley:14723891:media:pa2754:pa2754-math-0572
  57. urn:x-wiley:14723891:media:pa2754:pa2754-math-0573
  58. the solution space of the dynamical system urn:x-wiley:14723891:media:pa2754:pa2754-math-0574
  59. urn:x-wiley:14723891:media:pa2754:pa2754-math-0575
  60. urn:x-wiley:14723891:media:pa2754:pa2754-math-0576: urn:x-wiley:14723891:media:pa2754:pa2754-math-0577, urn:x-wiley:14723891:media:pa2754:pa2754-math-0578 t urn:x-wiley:14723891:media:pa2754:pa2754-math-0579}
  61. urn:x-wiley:14723891:media:pa2754:pa2754-math-0580
  62. urn:x-wiley:14723891:media:pa2754:pa2754-math-0581 is compact, pairwise disjoint, isolated invariant subsets in urn:x-wiley:14723891:media:pa2754:pa2754-math-0582
  63. urn:x-wiley:14723891:media:pa2754:pa2754-math-0583
  64. the stable manifold of urn:x-wiley:14723891:media:pa2754:pa2754-math-0584
  65. urn:x-wiley:14723891:media:pa2754:pa2754-math-0585
  66. the class urn:x-wiley:14723891:media:pa2754:pa2754-math-0586 consists of all differentiable functions whose derivative is continuous. Those functions are called continuously differentiable functions
  67. urn:x-wiley:14723891:media:pa2754:pa2754-math-0587
  68. the dynamical system used in the introduction of the geometric approach method used to investigate the global stability of the endemic equilibrium
  69. urn:x-wiley:14723891:media:pa2754:pa2754-math-0588
  70. urn:x-wiley:14723891:media:pa2754:pa2754-math-0589 is the domain of urn:x-wiley:14723891:media:pa2754:pa2754-math-0590 used in the introduction of the geometric approach method used to investigate the global stability of the endemic equilibrium
  71. urn:x-wiley:14723891:media:pa2754:pa2754-math-0591
  72. urn:x-wiley:14723891:media:pa2754:pa2754-math-0592 matrix valued function which is urn:x-wiley:14723891:media:pa2754:pa2754-math-0593 in urn:x-wiley:14723891:media:pa2754:pa2754-math-0594
  73. urn:x-wiley:14723891:media:pa2754:pa2754-math-0595
  74. urn:x-wiley:14723891:media:pa2754:pa2754-math-0596, which is used in accordance with the geometric approach method to investigate the global stability of the endemic equilibrium
  75. urn:x-wiley:14723891:media:pa2754:pa2754-math-0597
  76. urn:x-wiley:14723891:media:pa2754:pa2754-math-0598 is the matrix obtained by replacing each entry of the matrix urn:x-wiley:14723891:media:pa2754:pa2754-math-0599 by its directional derivative in the direction of urn:x-wiley:14723891:media:pa2754:pa2754-math-0600
  77. urn:x-wiley:14723891:media:pa2754:pa2754-math-0601
  78. the second additive compound matrix obtained from the jacobian matrix urn:x-wiley:14723891:media:pa2754:pa2754-math-0602
  79. urn:x-wiley:14723891:media:pa2754:pa2754-math-0603
  80. the Lozinskii measure with respect to urn:x-wiley:14723891:media:pa2754:pa2754-math-0604 norm
  81. urn:x-wiley:14723891:media:pa2754:pa2754-math-0605
  82. Lozinskii measure of the matrix urn:x-wiley:14723891:media:pa2754:pa2754-math-0606 which is given by urn:x-wiley:14723891:media:pa2754:pa2754-math-0607, I is the unit matrix
  83. urn:x-wiley:14723891:media:pa2754:pa2754-math-0608
  84. urn:x-wiley:14723891:media:pa2754:pa2754-math-0609 urn:x-wiley:14723891:media:pa2754:pa2754-math-0610. This quantity is defined as per the Geometric approach method to investigate the global stability of the endemic equilibrium
  85. urn:x-wiley:14723891:media:pa2754:pa2754-math-0611
  86. it is a compact absorbing set in the interior of urn:x-wiley:14723891:media:pa2754:pa2754-math-0612 which is absorbing for the reduced system (4)
  87. urn:x-wiley:14723891:media:pa2754:pa2754-math-0613
  88. urn:x-wiley:14723891:media:pa2754:pa2754-math-0614 is an open and simply connected set used in the introduction of Geometric approach method
  89. urn:x-wiley:14723891:media:pa2754:pa2754-math-0615
  90. the unique endemic equilibrium in G of the dynamical system urn:x-wiley:14723891:media:pa2754:pa2754-math-0616 used in the introduction of the Geometric approach to investigate the global stability of the endemic equilibrium
  91. urn:x-wiley:14723891:media:pa2754:pa2754-math-0617
  92. these symbols are used as per the Geometric approach to investigate the global stability of the endemic equilibrium
  93. urn:x-wiley:14723891:media:pa2754:pa2754-math-0618
  94. used in the definition of uniform persistence
  95. Biographies

    • Mr. R. Prem Kumar is an Assistant Professor of Mathematics at Avvaiyar Government College for Women, Karaikal-609602 in the Union Territory of Puducherry. He is pursuing his Ph.D at National Institute of Technology Puducherry, Karaikal-609609.

    • Dr. Sanjoy Basu is an Assistant Professor of Mathematics at Arignar Anna Government Arts and Science College, Karaikal, Puducherry, India. He obtained M.Sc. and Ph.D. in Mathematics from Jadavpur University, Kolkata, India. Dr. Basu has been involved in teaching and research for more than twelve years and has published more than seven research articles in various International, National journals and proceedings to his credit. His fields of interest in research work are Solid Mechanics, Soft Computing, and Mathematical Biology.

    • Dipankar Ghosh holds the dual degrees of M.Sc. in Applied Mathematics and M.Sc. in Statistics from the University of Burdwan, Burdwan, India, and Ph.D. persuing from National Institute of Technology, Puducherry, India. Mr. Ghosh has been involved in research for more than four and half years and has published more than five research articles in various international journals and proceedings to his credit. His research interest field is Mathematical Biology.

    • Prasun Kumar Santra holds the degrees of M.Sc. in Applied Mathematics from Bengal Engineering and Science University, Shibpur, presently IIEST Shibpur, India, and Ph.D. from Maulana Abul Kalam Azad University of Technology, West Bengal, India. Dr. Santra has been involved in research for more than five years and has published more than twelve research articles in various international journals and proceedings to his credit. His research interest field is Mathematical Biology.

    • Dr. G. S. Mahapatra is an Associate Professor at National Institute of Technology Puducherry, India. He obtained M.Sc. and Ph.D. in Applied Mathematics from Bengal Engineering and Science University, Shibpur, presently IIEST Shibpur, India. Dr. Mahapatra has been involved in teaching and research for more than seventeen years and has published more than ninety research articles in various International, National journals and proceedings to his credit. His fields of interest in research work are Inventory Management, Reliability, Optimization, Fuzzy Set theory, Soft Computing, and Mathematical Biology.

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