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Scientific Reports logoLink to Scientific Reports
. 2025 Sep 30;15:34054. doi: 10.1038/s41598-025-14183-w

Modelling the dynamically consistent numerical methods for COVID-19 disease with cost effectiveness strategies

Shuo Li 1, Muhammad Amjad Abbas 2, Ihsan Ullah Khan 2, Ali Akgül 3,4,5,6,7, Ali G Alkhathami 8, Murad Khan Hassani 9,
PMCID: PMC12485142  PMID: 41028096

Abstract

COVID-19, a perilous disease triggered by the SARS-CoV-2 virus, exhibits an unusually high spread rate through both direct and indirect physical contact. There are many ways to inspect the possibility of COVID-19 which may include but not limited to shortness of breath, fatigue, strict headaches, tastelessness, continuous chest pain, diarrhea and vomiting. In the present paper, the COVID-19 deterministic mathematical model with cost effectiveness strategies is considered and examined. The threshold quantity, assisting in establishing the existence and stability characteristics of equilibria, is computed by employing the next-generation matrix. The main objective of the present work is to use conditionally stable Euler and Runge–Kutta of order 4 (RK-4) schemes with the collaboration of unconditionally stable non-standard finite difference (NSFD) scheme to show the changing behavior of consistent SEIHR epidemic model. The Euler and RK-4 schemes are unable to precisely focus on the important aspects of the continuous model, resulting in numerical solutions that are not entirely analogous to the original model. However, the NSFD scheme provides a straightforward approach that demonstrates how discrete and continuous models behave appropriately and yield mathematically precise results. The NSFD system is a useful tool for tracking the spread of COVID-19 disease. For the NSFD scheme, different criteria and theories are employed to discuss the local and global stability of disease-free and endemic equilibria. Numerical simulations are provided to verify the theoretical findings and validate the dynamical aspects of the aforementioned schemes.

Keywords: COVID-19 model, Reproduction number, Numerical schemes, Schur-Cohn criterion, Routh-Hurwitz criterion, Local and global stability

Subject terms: Applied mathematics, Scientific data

Introduction

The coronavirus, most commonly introduced as COVID-19 is a global catastrophe which has left millions of people in the lurch13. The virus was initially emerged in individuals who traveled to a market for seafood in Wuhan City, China, in December 20194. It had affected people badly from normal to the lethal level. The common symptoms of COVID-19 may include but not limited to cough, fatigue, fever, throat soreness and breathing problems57. COVID-19 urges the world to impose a health emergency and demanded a collective and fruitful efforts to curb this global menace. From the beginning, world health organization (WHO) mainly focused to analyze its symptoms and prepare the effective and accurate vaccines. For the perfect vaccination, WHO gathered the brilliant minds to achieve its landmark target of minimization of lethal impacts of the virus. Vaccination stands as the best effective means to avert and control the disease’s spread. At the end of 2020, The WHO has authorized numerous vaccines for use in emergencies8. Global efforts have been made to launch massive campaign of vaccination which brought down effective results in curbing and stopping the exacerbation of virus9. Some recent publications regarding the efficiency of vaccines can be perceived in1012.

The dynamics of real-world situations can be efficiently analyzed using mathematical models1316. Researchers from all over the world develop numerous mathematical models to comprehend the various kinds of diseases and their dynamical aspects. Fractional models offer a more adaptable and practical framework for comprehending and forecasting the evolution of infectious diseases. The transmission of various infectious illnesses has been examined and assessed in1726 using mathematical models of fractional order derivatives. The authors performed numerical simulations to validate the theoretical results in addition to analyzing the exact qualitative characteristics of the developed models. Many scholars have established a profound wide range of mathematical models to examine the effectiveness of the vaccines and transmission of COVID-192729. By applying these models, one can concentrate how an infectious disease extends amongst the masses. The models discussed in3032 may be materialized to amplify all of their sources and execute all control activities more effectively. In33, the authors considered and analyzed COVID-19 mathematical model cobbled with quarantine class and resistive compartment. Because of the quarantine and restive classes, the model is entirely changed from other models that have been developed in the existing works. Peter et al.34 estimated the COVID-19 model by concentrating on actual data that assesses the impacts of several controlling methodologies on the spread of COVID-19 in the human population. The novel COVID-19 has been widely inspected by scholars using mathematical methods from a variety of viewpoints3537. They concentrated on native and sophisticated dynamics, stability theory and numerical tools.

Recently, Keno et al.38 developed and analyzed a deterministic mathematical model for COVID-19 epidemic disease with cost-effectiveness using real data from Ethiopia. The researchers investigated the local and global stability of endemic and disease-free equilibria for the continuous model considering several kinds of criteria. In the present work, three different schemes, which are Euler, RK-4, and NSFD schemes are developed for the original model in order to investigate ecological sustainability and different components of the model. The dynamics of the model are clarified by performing positivity and boundedness properties of solutions. It is revealed that two standard finite difference (SFD) schemes, such as Euler and RK-4 had limitations in capturing the model’s essential dynamics, whereas the third scheme NSFD yields exceptionally accurate and useful findings, and it is suitable for the continuous model. The advanced NSFD technique is being used to better understand the dynamics of COVID-19 transmission and evaluate possible health effects. The NSFD scheme was actually designed for making up over the deficiencies of the RK-4 scheme. The local and global stability of disease-free and endemic equilibria are discussed for the NSFD scheme by employing multiple number of criteria and theories. The results explain that NSFD scheme is unconditionally stable and viable for the continuous model which generates incredible effective results.

The paper is divided into the following categories. In Sect. 2 “SEIHR model”, the COVID-19 mathematical model is presented and its associated parameters are explored. Sect. 3 “COVID-19 model equilibria and basic reproductive number” includess the basic reproduction number and model equilibria. In Sect. 4 “SFD and NSFD numerical schemes”, the conditionally convergent Euler and RK-4 schemes, and unconditionally convergent NSFD scheme are built for the original model. The local and global stability of disease free and endemic equilibria are displayed in the same section for the NFSD scheme. Numerical simulations are given to support our theoretical results. Numerical and theoretical findings portray that the NSFD scheme dominates in every characteristic by controlling the flaws of the RK-4 and Euler schemes. In Sect. 5 “Conclusions”, the conclusions are given.

SEIHR model

Nonlinear mathematical models that describe the spread dynamics of the deadly COVID-19, are essential in the field of epidemiology. They provide critical insights for public health officials and policymakers. The whole population Inline graphic is separated into five different categories in this section: susceptible Inline graphic, exposed Inline graphic, infected Inline graphic, hospitalized Inline graphic, and recovered Inline graphic. Then, the nonlinear mathematical model for COVID-1938 is represented as follows.

graphic file with name 41598_2025_14183_Article_Equa.gif
graphic file with name 41598_2025_14183_Article_Equb.gif
graphic file with name 41598_2025_14183_Article_Equ1.gif 1
graphic file with name 41598_2025_14183_Article_Equc.gif
graphic file with name 41598_2025_14183_Article_Equd.gif

This division is portrayed by the system of ordinary differential equations (ODE’s) represented in Fig. 1. However, the explanation of the parameters is provided in Table 1.

Fig. 1.

Fig. 1

Flowchart for the SEIHR mathematical model, which demonstrates the variations among the model’s compartments.

Table 1.

The parameters and their description for the suggested SEIHR model (1).

Parameters Description
Inline graphic Rate at which individuals are recruited
Inline graphic Chances of contact rate of transmission
Inline graphic recovery rate for early mediation
Inline graphic Rate at which natural deaths occurs
Inline graphic Rate of recovered people fall into the susceptible class again
Inline graphic Rate at which an individual gets infected after being exposed
Inline graphic Rate of infected people that are hospitalized
Inline graphic Deaths rate due to COVID-19
Inline graphic Rate of hospitalized class who get recovered

In upcoming section, we illustrate the equilibria and basic reproduction number for mathematical model (1).

COVID-19 model equilibria and basic reproductive number

First, we find the equilibria for model (1) as follows.

Disease absence equilibrium point (DAEP)

An equilibrium condition known as disease absence equilibrium point (DAEP) is attained when COVID-19 vanishes. By establishing the model’s (1) right-side equal to 0, it can be attained.

graphic file with name 41598_2025_14183_Article_Eque.gif
graphic file with name 41598_2025_14183_Article_Equf.gif
graphic file with name 41598_2025_14183_Article_Equ2.gif 2
graphic file with name 41598_2025_14183_Article_Equg.gif
graphic file with name 41598_2025_14183_Article_Equh.gif

In order to identify DAEP, we replace Inline graphic for each differential equation in the system (2) when Inline graphic. Then, we obtain

graphic file with name 41598_2025_14183_Article_Equi.gif

i.e.

graphic file with name 41598_2025_14183_Article_Equj.gif

Thus, if we represent DAEP by Inline graphic= Inline graphic, then it is simple to determine DAEP as Inline graphic.

Endemic equilibrium point (EEP)

The EEP illustrates a situation whereby the disease is persisted in the community rather than being completely eradicated. The quantities for Inline graphic must be non-zero at the equilibria if the disease present in the population, i.e. if Inline graphic is EEP, then Inline graphic. The model (2) yields Inline graphic, Inline graphic, Inline graphic, Inline graphic, Inline graphic

The basic reproduction number is provided in the following which is essential for the stability of model (1) equilibria.

Basic reproductive number Inline graphic

The basic reproduction number is the average number of secondary infections that one infectious individual causes in a group of people that are all completely susceptible. It gives an overall assessment of the possibility that an infection will spread throughout a community and is influenced by both the average length of infectiousness and the transmission coefficient. Though, a perfect assessment of secondary infections can’t be given, while studies of epidemiology may yield an average approximation, which is called the basic reproduction number3941. To find Inline graphic, we use the translation Inline graphic and transmission Inline graphic matrices, respectively. For model (1), these can be presented as follows.

graphic file with name 41598_2025_14183_Article_Equk.gif

Since Inline graphic is same as the spectral radius, which is determined from the matrix product as Inline graphic Therefore, we get.

graphic file with name 41598_2025_14183_Article_Equl.gif

The following section presents the NSFD scheme and two SFD schemes, namely Euler and RK-4, in order to better comprehend the model (1) dynamics.

SFD and NSFD numerical schemes

An approach for understanding and measuring the dynamics of disease spread is numerical modeling of infectious illnesses. In the current paper, a mathematical model for COVID-19 is proposed and investigated. The goal is to mathematically well understand the spread and behavior dynamics of the disease. To demonstrate the validity and biological animation of mathematical model of COVID-19, we develop two conditionally stable Euler and RK-4 SFD schemes as well as an unconditionally stable NSFD scheme. NSFD schemes are crucial to numerical analysis because they offer better accuracy and stability than standard finite difference techniques, especially for analyzing nonlinear differential equations. The NSFD numerical scheme constructed for model (1) is dynamically credible that retains the positive feature of the solutions. The NSFD scheme guarantees convergence to the model’s equilibria for all time step sizes, however aforementioned SFD schemes break down at large time steps. The findings presented in this research clarify that the previously discussed SFD and NSFD schemes give a clear and detailed picture of the continuous model.

In the following subsection, we first layout Euler scheme for system (1).

Euler scheme

This is one of the earliest and easiest ways to compute the numerical solutions of ODE’s. From model (1), we can write

graphic file with name 41598_2025_14183_Article_Equm.gif
graphic file with name 41598_2025_14183_Article_Equn.gif
graphic file with name 41598_2025_14183_Article_Equo.gif

On Similar basis

graphic file with name 41598_2025_14183_Article_Equp.gif
graphic file with name 41598_2025_14183_Article_Equq.gif
graphic file with name 41598_2025_14183_Article_Equr.gif

Similarly, as

graphic file with name 41598_2025_14183_Article_Equs.gif
graphic file with name 41598_2025_14183_Article_Equt.gif
graphic file with name 41598_2025_14183_Article_Equu.gif

In the same way

graphic file with name 41598_2025_14183_Article_Equv.gif
graphic file with name 41598_2025_14183_Article_Equw.gif
graphic file with name 41598_2025_14183_Article_Equx.gif

and

graphic file with name 41598_2025_14183_Article_Equy.gif
graphic file with name 41598_2025_14183_Article_Equz.gif
graphic file with name 41598_2025_14183_Article_Equaa.gif

Finally, Euler scheme for system (1) becomes

graphic file with name 41598_2025_14183_Article_Equab.gif
graphic file with name 41598_2025_14183_Article_Equac.gif
graphic file with name 41598_2025_14183_Article_Equ3.gif 3
graphic file with name 41598_2025_14183_Article_Equad.gif
graphic file with name 41598_2025_14183_Article_Equaa.gif

Figure 2 (a-d) provides a graphic depiction of the Euler scheme for various step sizes. The Euler scheme produces stable and positive solutions for smaller step sizes, as explained in Fig. 2 (a, b). However, Fig. 2 (c, d) shows the equilibrium point’s instability as the step size grows. This suggests that greater step sizes are not appropriate for Euler scheme.

Fig. 2.

Fig. 2

Graphical illustration of Euler scheme with Inline graphic Inline graphic.

The well-known RK-4 approach is used in the following subsection to solve system (1). The RK-4 scheme is extensively employed method to solve ODE systems. In numerous situations, the RK-4 scheme is frequently employed, unless specified otherwise.

RK-4 scheme

C. V. Runge (1856–1927) and M. W. Kutta (1867–1944), two famous German mathematicians introduced RK–4 method42. It is a commonly used strategy for solving problems and is applied in numerous situations. Let Inline graphic then for system (1) the RK-4 scheme can be signified as below.

Stage-1

graphic file with name 41598_2025_14183_Article_Equaf.gif
graphic file with name 41598_2025_14183_Article_Equag.gif
graphic file with name 41598_2025_14183_Article_Equah.gif
graphic file with name 41598_2025_14183_Article_Equai.gif
graphic file with name 41598_2025_14183_Article_Equaj.gif

Stage-2

graphic file with name 41598_2025_14183_Article_Equak.gif
graphic file with name 41598_2025_14183_Article_Equal.gif
graphic file with name 41598_2025_14183_Article_Equam.gif
graphic file with name 41598_2025_14183_Article_Equan.gif
graphic file with name 41598_2025_14183_Article_Equao.gif

Stage-3

graphic file with name 41598_2025_14183_Article_Equap.gif
graphic file with name 41598_2025_14183_Article_Equaq.gif
graphic file with name 41598_2025_14183_Article_Equar.gif
graphic file with name 41598_2025_14183_Article_Equas.gif
graphic file with name 41598_2025_14183_Article_Equat.gif

Stage-4

graphic file with name 41598_2025_14183_Article_Equau.gif
graphic file with name 41598_2025_14183_Article_Equav.gif
graphic file with name 41598_2025_14183_Article_Equaw.gif
graphic file with name 41598_2025_14183_Article_Equax.gif
graphic file with name 41598_2025_14183_Article_Equay.gif
graphic file with name 41598_2025_14183_Article_Equaz.gif
graphic file with name 41598_2025_14183_Article_Equba.gif
graphic file with name 41598_2025_14183_Article_Equbb.gif
graphic file with name 41598_2025_14183_Article_Equbc.gif
graphic file with name 41598_2025_14183_Article_Equbd.gif

Figure 3 (a-d) shows an example of RK-4 scheme containing different step sizes. The RK-4 method provides solutions that are positive and stable for lower step sizes, as revealed in Fig. 3 (a, b). However, Fig. 3 (c, d) shows the equilibrium point’s instability as the step size grows. This suggests that greater step sizes are not suitable for RK-4 scheme.

Fig. 3.

Fig. 3

Graphical illustration of RK-4 scheme withInline graphic. The values of fixed parameters are Inline graphicGenerally.

In the following, we build the NSFD scheme for model (1) which is independent of the step size, guaranteeing the boundedness of the solutions and provide better outcomes in all aspects.

The NSFD scheme

The primary goal of this section is to develop a discrete, smoothly changing NSFD scheme for model (1). The Mickens43,44 approach is remarkable for producing a discrete model that has similarities to the continuous model. For both partial and ordinary differential equations, the NSFD scheme provides a flexible way for discrete model creation and numerical solution findings. According to Shokri et al.45, discretizing the derivative and accurately estimating nonlinear terms are the two key components that make the NSFD scheme effective. Inline graphic is written as Inline graphic, where Inline graphic represents the step size. Mickens specified that, this term can be written as Inline graphic, where Inline graphic is a rising denominator function. For model (1), Inline graphic are the numerical estimates of Inline graphic,Inline graphic,Inline graphic, Inline graphic at Inline graphic, where Inline graphic denotes the step size and Inline graphic is a nonnegative integer. Therefore, from model (1) we can express

graphic file with name 41598_2025_14183_Article_Eqube.gif
graphic file with name 41598_2025_14183_Article_Equbf.gif
graphic file with name 41598_2025_14183_Article_Equ4.gif 4
graphic file with name 41598_2025_14183_Article_Equbg.gif
graphic file with name 41598_2025_14183_Article_Equbh.gif

After simplifying, the explicit form of NSFD scheme (4) can be given as

graphic file with name 41598_2025_14183_Article_Equbi.gif
graphic file with name 41598_2025_14183_Article_Equbj.gif
graphic file with name 41598_2025_14183_Article_Equ5.gif 5
graphic file with name 41598_2025_14183_Article_Equbk.gif
graphic file with name 41598_2025_14183_Article_Equbl.gif

The numerical solutions of epidemic models must persist positive in order to guarantee validity and applicability. However, it is crucial to make sure that the total population is never greater than the sum of the populations in each compartment. The positivity and boundedness are successfully addressed in the subsection that follows.

The NSFD scheme’s positivity and boundedness

Let the starting values of scheme (5) are positive, i.e. Inline graphic. Due to the expectancies, the predicted outcomes for these variables are also nonnegative., i.e. Inline graphic. Hence, the NSFD scheme (5) is positive, i.e. Inline graphic. To find the boundedness of solutions for NSFD system (5), we write Inline graphic. Then

graphic file with name 41598_2025_14183_Article_Equ6.gif 6

From (6), we can write.

graphic file with name 41598_2025_14183_Article_Equbm.gif

I.e.

graphic file with name 41598_2025_14183_Article_Equbn.gif
graphic file with name 41598_2025_14183_Article_Equbo.gif

If Inline graphic, then Gronwall’s inequality permits us to establish

graphic file with name 41598_2025_14183_Article_Equbp.gif

As Inline graphic, therefore we acquire Inline graphic whenever Inline graphic This shows that the system (5)’s solutions are bounded, and the reasonable region turns into

graphic file with name 41598_2025_14183_Article_Equbq.gif

The following subsection discusses the local stability of DAEP and EEP for NSFD scheme (5).

Local stability of equilibria

For local asymptotic stability (LAS) of equilibria, assume

graphic file with name 41598_2025_14183_Article_Equbr.gif
graphic file with name 41598_2025_14183_Article_Equbs.gif
graphic file with name 41598_2025_14183_Article_Equ7.gif 7
graphic file with name 41598_2025_14183_Article_Equbt.gif
graphic file with name 41598_2025_14183_Article_Equbu.gif

We will implement the Schur-Cohn criterion46,47 as stipulated in the subsequent Lemma 1 to establish that DAEP is LAS.

Lemma 1

The solutions to Inline graphic ensure that Inline graphic Inline graphic the prerequisites are met.

  1. Inline graphic 

  2. Inline graphic 

  3. Inline graphic 

where Inline graphic concerns to the J-matrix’s determinant and Inline graphic specifies the trace.

Theorem 1

For all Inline graphic, the DAEP of the NSFD scheme (5) for model (1) is LAS whenever Inline graphic

Proof

The above-mentioned data can be employed to get the J-matrix as follows.

graphic file with name 41598_2025_14183_Article_Equ8.gif 8

where Inline graphic and Inline graphic are provided in (7). The list of derivatives involved in (8) can be found as follows.

graphic file with name 41598_2025_14183_Article_Equbv.gif

By inserting all of the aforementioned derivatives in (8), we obtain

graphic file with name 41598_2025_14183_Article_Equ9.gif 9

At DAEP Inline graphic, the matrix (9) becomes.

graphic file with name 41598_2025_14183_Article_Equbw.gif

To find the eigenvalues, we adopt.

graphic file with name 41598_2025_14183_Article_Equbx.gif

I.e.

graphic file with name 41598_2025_14183_Article_Equby.gif

Easy calculations produce outcomes

graphic file with name 41598_2025_14183_Article_Equ10.gif 10

The Eq. (10) provides Inline graphic and Inline graphic.To look for remaining eigenvalues, we use.

graphic file with name 41598_2025_14183_Article_Equbz.gif

I.e.

graphic file with name 41598_2025_14183_Article_Equ11.gif 11

Comparing Eq. (11) with Inline graphic, we get.

graphic file with name 41598_2025_14183_Article_Equca.gif
  1. Inline graphic 

  2. Inline graphic 

  3. Inline graphic 

Therefore, the Schur-Cohn condition met whenever Inline graphic. The DAEP Inline graphic of the discrete NSFD scheme (5) then turn LAS when Inline graphic.

To discuss LAS of EEP, substitute Inline graphic by Inline graphic in Eq. (4). The system (4) will be reduced to

graphic file with name 41598_2025_14183_Article_Equcb.gif
graphic file with name 41598_2025_14183_Article_Equbf.gif
graphic file with name 41598_2025_14183_Article_Equ4.gif
graphic file with name 41598_2025_14183_Article_Equce.gif

Now the above system becomes

graphic file with name 41598_2025_14183_Article_Equcf.gif
graphic file with name 41598_2025_14183_Article_Equ12.gif 12
graphic file with name 41598_2025_14183_Article_Equcg.gif
graphic file with name 41598_2025_14183_Article_Equch.gif

Let

graphic file with name 41598_2025_14183_Article_Equci.gif
graphic file with name 41598_2025_14183_Article_Equcj.gif
graphic file with name 41598_2025_14183_Article_Equ13.gif 13
graphic file with name 41598_2025_14183_Article_Equck.gif
Theorem 2

For all Inline graphic, the EEP of the NSFD scheme (12) for model (1) is LAS whenever Inline graphic.

Proof

We find the derivatives of (13) as follows.

graphic file with name 41598_2025_14183_Article_Equcl.gif
graphic file with name 41598_2025_14183_Article_Equcm.gif

By putting EEP Inline graphic in above derivatives, we get

graphic file with name 41598_2025_14183_Article_Equcn.gif
graphic file with name 41598_2025_14183_Article_Equco.gif

Let

graphic file with name 41598_2025_14183_Article_Equcp.gif
graphic file with name 41598_2025_14183_Article_Equcq.gif

Following the same steps as in Theorem 1, the J-matrix can be described as.

graphic file with name 41598_2025_14183_Article_Equcr.gif

For eigenvalues, we study

graphic file with name 41598_2025_14183_Article_Equcs.gif

i.e.

graphic file with name 41598_2025_14183_Article_Equ14.gif 14

The Eq. (14) gives the characteristic equation as follows.

graphic file with name 41598_2025_14183_Article_Equct.gif

Where.

graphic file with name 41598_2025_14183_Article_Equcu.gif
graphic file with name 41598_2025_14183_Article_Equcv.gif
graphic file with name 41598_2025_14183_Article_Equcw.gif
graphic file with name 41598_2025_14183_Article_Equcx.gif
graphic file with name 41598_2025_14183_Article_Equcy.gif

By employing Routh–Hurwitz criteria48,49, the EEP Inline graphic of system (12) is LAS if Inline graphic for Inline graphic and Inline graphic Inline graphic2+Inline graphic2 Inline graphic. Therefore, whenever Inline graphic, the EEP for the discrete NSFD scheme (12) is LAS. Consequently, the EEP Inline graphic of the discrete NSFD scheme (5) is LAS.

The following subsection examines DAEP and EEP global asymptotic stability (GAS) for NSFD scheme (5).

Global stability of equilibria

Theorem 3

For all Inline graphic, the DAEP of the NSFD scheme (5) for the model (1) is GAS whenever Inline graphic and the EEP is GAS whenever Inline graphic.

Proof

Let Inline graphic denote the bounded sequence provided by the NFSD scheme (5). Our goal is to show that Inline graphic as Inline graphic where Inline graphic is either DAEP or EEP. Since, the sequence Inline graphic is bounded, the Bolzano-Weierstrass theorem ensures the existence of a convergent subsequence Inline graphic such that Inline graphic as Inline graphic.

Due to the structure of NSFD scheme (5) and assumption made above, the limit point Inline graphic must coincide with Inline graphic, which is either DAEP or EEP. It is already proved in Theorem 1 and 2 that both the equilibria are LAS. Thus, there exists Inline graphic such that for an initial condition Inline graphic satisfies

graphic file with name 41598_2025_14183_Article_Equ15.gif 15

Suppose Inline graphic be any arbitrary initial value. For instance Inline graphic, it follows that there exists an integer Inline graphic for which.

graphic file with name 41598_2025_14183_Article_Equ16.gif 16

From (15) and (16), we conclude that.

graphic file with name 41598_2025_14183_Article_Equ17.gif 17

This completes the proof that Inline graphic is GAS.

An illustration of NSFD scheme with various step sizes can be found in Fig. 4 (a–d) and Fig. 5 (a–d). The numerical assessment offered in Fig. 4 (a-d) displays that NSFD scheme (5) is convergent to DAEP, however Fig. 5 (a-d) shows that NSFD scheme (5) is convergent to EEP for all step sizes.

Fig. 4.

Fig. 4

Graphical illustration of NSFD scheme with Inline graphic. The values of fixed parameters are Inline graphic.

Fig. 5.

Fig. 5

Graphical illustration of NSFD scheme with Inline graphic. The values of fixed parameters are Inline graphic.

Conclusions

This paper develops and investigates a mathematical model for COVID-19. The intent is to study mechanisms of COVID-19 disease and reducing or preventing its transmission amongst people. The basic reproduction number is calculated which serves as essential tool in analyzing the local and global stability of both DAEP and EEP. Two different approaches, such as SFD which include Euler as well as RK-4 and NSFD schemes, are used to discuss the dynamical properties of the model. Conditional convergence and step-size dependency were both validated by the RK-4 and Euler systems, which means that when the step size increases, they diverge. In addition, to produce exact results that are both mathematically and biologically consistent with the corresponding continuous model, the discrete NSFD scheme is designed for the model which is unconditionally convergent. The aim of developing NSFD scheme for system is to ensure its dynamical reliability. The NSFD scheme is a useful method for confirming that outputs from discrete and continuous models act similarly and are mathematically steady. The local and global stability of both the equilibria for NSFD scheme are determined using multiple theories and criteria. Numerical solutions are applied to ensure the accuracy of all theoretical conclusions. The results indicate that the COVID-19 epidemic disease transmission can be effectively monitored using NSFD scheme. The evidences provided in this study are beneficial to both humanity and the field of health sciences. The outcomes provided in the current work can also be employed as a suitable tool to estimate the development of the COVID-19 epidemic disease.

In our future work, we will explore various comprehensive epidemic models with properties analogous to the one being measured in order to get an enhanced understanding of the dynamics of disease spread. We will examine the fluctuating behavior of the epidemic models employing the Euler, RK-4, and NSFD numerical approaches.

Acknowledgements

The authors extend their appreciation to the Deanship of Research and Graduate Studies at King Khalid University, KSA for funding this work through Large Research Project under grant number RGP.2/567/45. This work is also supported by the Natural Science Foundation of Xinjiang, China (2021D01C003).

Author contributions

S.L perform basic mathematical results, validate all the results with care, and formal analysis. M.A.A. and I.U.K. conceptualized the main problem, wrote the original manuscript, and performed theoretical and simulation results. A.A reviewed the entire mathematical results and Wrote the manuscript. A.G.A. and M.K.H reviewed and restructured the manuscript. All authors are agreed on the final draft of the submission file.

Data availability

The data used to support the findings of this study are included within the article.

Declarations

Competing interests

The authors declare no competing interests.

Footnotes

Publisher’s note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

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Data Availability Statement

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