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Research article

Epidemiological analysis of fractional order COVID-19 model with Mittag-Leffler kernel

  • Received: 08 August 2021 Accepted: 30 September 2021 Published: 15 October 2021
  • MSC : 37C75, 93B05, 93B07, 65L07

  • This paper derived fractional derivatives with Atangana-Baleanu, Atangana-Toufik scheme and fractal fractional Atangana-Baleanu sense for the COVID-19 model. These are advanced techniques that provide effective results to analyze the COVID-19 outbreak. Fixed point theory is used to derive the existence and uniqueness of the fractional-order model COVID-19 model. We also proved the property of boundedness and positivity for the fractional-order model. The Atangana-Baleanu technique and Fractal fractional operator are used with the Sumudu transform to find reliable results for fractional order COVID-19 Model. The generalized Mittag-Leffler law is also used to construct the solution with the different fractional operators. Numerical simulations are performed for the developed scheme in the range of fractional order values to explain the effects of COVID-19 at different fractional values and justify the theoretical outcomes, which will be helpful to understand the outbreak of COVID-19 and for control strategies.

    Citation: Muhammad Farman, Ali Akgül, Kottakkaran Sooppy Nisar, Dilshad Ahmad, Aqeel Ahmad, Sarfaraz Kamangar, C Ahamed Saleel. Epidemiological analysis of fractional order COVID-19 model with Mittag-Leffler kernel[J]. AIMS Mathematics, 2022, 7(1): 756-783. doi: 10.3934/math.2022046

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  • This paper derived fractional derivatives with Atangana-Baleanu, Atangana-Toufik scheme and fractal fractional Atangana-Baleanu sense for the COVID-19 model. These are advanced techniques that provide effective results to analyze the COVID-19 outbreak. Fixed point theory is used to derive the existence and uniqueness of the fractional-order model COVID-19 model. We also proved the property of boundedness and positivity for the fractional-order model. The Atangana-Baleanu technique and Fractal fractional operator are used with the Sumudu transform to find reliable results for fractional order COVID-19 Model. The generalized Mittag-Leffler law is also used to construct the solution with the different fractional operators. Numerical simulations are performed for the developed scheme in the range of fractional order values to explain the effects of COVID-19 at different fractional values and justify the theoretical outcomes, which will be helpful to understand the outbreak of COVID-19 and for control strategies.



    Coronavirus (COVID-19) is a new phenomenon in recent days, which indulged the whole world in an emergency situation. According to reports, it's originated from Wuhan city of China [1]. In December 2019, the first case of novel coronavirus was reported. The symptoms of coronavirus are dry cough, fever, fatigue, and severe cases of acute respiratory syndrome that appears in 2–10 days and further cause pneumonia, Kidney failure, and even death [2]. Between March and April, coronavirus became a global phenomenon, and the whole globe faced an emergency situation. Initial cases were reported in the wet seafood market in Wuhan, China [3]. That's why some researchers thought that it's transmitted in humans through animals. This virus is transmitted from one person to another through physical contact, droplets during sneezing and coughing [4]. Researchers of the field of epidemiology and other fields of biology are trying hard to develop the cure based on ongoing clinical trials, but different researching companies of different countries have developed the vaccine of COVID-19. If we mention here, then China, the USA, England and Russia have developed the vaccine. In most countries of the globe, people receiving doses of vaccines. According to WHO, at 4:53 pm CET, 18 March 2021, there were 120,915,219 confirmed cases reported globally, including 2,674,078 deaths and a total of 364,184,603 vaccine doses were administered [5]. Developed countries like the USA, UK, Italy, Spain, and many others are affected very badly; most of the global deaths are reported from these countries [6]. Some precautionary measures for COVID-19 are wearing a face mask, maintaining a 6feet distance, coughing and sneezing in the elbow, and washing your hands minimally 30 seconds. Almost all countries' governments have enforced non-medical interventions such as social distancing, self-quarantine, isolation, wearing a face mask, protecting gears for medical staff, and travel restrictions to control the spread of disease. Mathematical modelling is used to understand the dynamics and behaviour of disease and then develop the procedures for the treatment of disease. For this purpose, many researchers developed the COVID-19 models (see [7,8,9,10]). The reproductive number has a notable role in the analysis of mathematical models. Reproductive number explains the behaviour of the simulation of COVID-19.

    In Pakistan, 739,818 confirmed cases had been reported, including 15,872 deaths out of over 220 million population to date [11,12]. On 26 February 2020, the first case of COVID-19 was reported in Karachi, Pakistan's economic hub. Nowadays, Pakistan has been facing the third wave of COVID-19, which is at its peak. The government is not in the right of Strick lockdown because most of the people are a daily wager; that's why the government has been implementing smart lockdown. There are many mathematical models provided for more insight into how to control the spread of Covid-19 to health authorities [13,14,15]. In three highly affected countries, the transmission pattern of COVID-19 was studied by Fanelli and Piazza [16]. To explain the simulation of COVID-19 transmission [17,18] are used and explain the natural fact of fractional-order mathematical models in a systematic way as in [19,20]. The fractional-order models are more effective than classical integer models in analyzing the dynamics and behaviour of infectious diseases [21,22]. The fractional-order models give better results to the real data. Some fractional operators are given in [23,24], and applications of these fractional operators are given in [25,26]. The investigations of some other infectious disease mathematical models have been studied in [27,28,29,30,31]. Studied the outcome of an antiviral drug on the system to obstruct the contact between epithelial cells and SARS-CoV-2 to restrict the COVID-19 disease in [37,38]. Results have good accuracy, and the method is valid for the fuzzy system of fractional ODEs COVID-19. Also, the random COVID-19 model described by a system of random differential equations was presented in [39,40,41,42,43], and some application of fractional order for the real-life problem was also given in [44,45,46,47,48].

    In this paper, we proposed a fractional-order COVID-19 model with Atangana-Baleanu, Atangan-Tufik scheme and fractal fractional-order derivative. In Section 1, we construct the introduction with the literature review of COVID-19 and fractional calculus. Section 2 has some basic definitions which are helpful for analysis and simulation if the model. In Section 3, the mathematical model of COVID-19 is present with disuses the boundedness and positivity of the model. In Section 4, using fixed point theory and an iterative method, the existence and uniqueness of the system of solutions for the model have been made. In Sections 5 and 6, new numerical scheme and fractal fractional-order derivative construct with Atanga-Tufik method for real data of Wuhan China. In Section 7, we describe the numerical simulation of the proposed scheme with real data and best-fitted parameter substitution. We give the conclusions and perspectives in Section 8.

    Definition 2.1. For a function y(t)W12(0,1),b>aandΘ[0,1], the definition of Atangana-Baleanu derivative in the Caputo sense is given by

    ABC0DΘty(t)=AB(Θ)1Θt0ddτy(τ)MΘ[Θ1Θ(tτ)Θ]dτ,n1<Θ<n (1)

    where

    AB(Θ)=1Θ+ΘΓ(Θ).

    By using the Sumudu transform (ST) for (1), we obtain

    ST[ABC0DΘty(t)](s)=q(Θ)1Θ{ΘΓ(Θ+1)MΘ(11ΘVΘ)}×[ST(y(t))y(0)]. (2)

    Definition 2.2. The Laplace transform of the Caputo fractional derivative of a function y(t) of order Θ>0 is defined as

    L[0CDΘty(t)]=sΘy(s)n1Θ=0y(Θ)(0)sΘv1. (3)

    Definition 2.3. The Laplace transform of the function tΘ11EΘ,Θ1(±μtΘ) is defined as

    L[tΘ11EΘ,Θ1(±μtΘ)]=sΘΘ1sΘμ, (4)

    where EΘ,Θ1 is the two-parameter Mittag-Leffler function with Θ,Θ1>0. Further, the Mittag-Leffler function satisfies the following equation [32].

    EΘ,Θ1(f)=fEΘ,Θ+Θ1(f)+1Γ(Θ1). (5)

    Definition 2.4. Suppose that y(t) is continuous on an open interval (a,b), then the fractal-fractional integral of y(t) of order Θ having Mittag-Leffler type kernel and given by

    FFMJΘ,Θ10,t(y(t))=ΘΘ1AB(Θ)Γ(Θ)t0sΘ11y(s)(ts)Θds+Θ1(1Θ)tΘ11y(t)AB(Θ). (6)

    This section considers the novel coronavirus (COVID-19) disease model developed by Yang and Wang [33]. In this model total human population is divided into five classes, namely, susceptible individuals are represented by Sc, Ec represents exposed individuals, who are infected but not infectious as yet, Ic represents infected population, those individuals in which symptoms have shown strongly and can spread infection by contact with susceptible individuals, Rcrepresents the individuals who have no symptoms and they have recovered after receiving treatment and the concentration of virus is represented by Vc.

    dScdt=ΠcβEcScEcβIcScIcβVcScVcμcSc,
    dEcdt=βEcScEc+βIcScIc+βVcScVc(αc+μc)Ec,
    dIcdt=αcEc(ωc+γc+μc)Ic, (7)
    dRcdt=γcIcμcRc,
    dVcdt=ψ1cEc+ψ2cIcτcVc.

    In the above system parameters are defined as the influx of population is denoted by Πc, µc represents natural death rate, (αc)−1 represents quarantine period of the infected individuals, rate of recovery is denoted by γc, The exposed and infected people which contributing the coronavirus in the surrounding is represented by ψ1c, ψ2c respectively, disease induced death rate is represented by ωc and τc represents removal rate. βEc represents the rate of human to human transmission of virus between exposed and susceptible people, The rate of human to human transmission between infected and susceptible people are represented by βIc and βVc denotes the rate of transmission due to environmental contact to human. We suppose that given all functions βEc,βIcandβVc are non-negative and non-increasing. By applying Atangana-Baleanu fractional derivative (ABC) of order Θ and Θ(0,1], then the system (7) becomes

    ABC0DΘtSc=ΠcβEcScEcβIcScIcβVcScVcμcSc,
    ABC0DΘtEc=βEcScEc+βIcScIc+βVcScVc(αc+μc)Ec,
    ABC0DΘtIc=αcEc(ωc+γc+μc)Ic, (8)
    ABC0DΘtRc=γcIcμcRc,
    ABC0DΘtVc=ψ1cEc+ψ2cIcτcVc.

    Initial conditions are

    Sc(0)a1,Ec(0)a2,Ic(0)a3,Rc(0)a4andVc(0)a5. (9)

    Equilibrium points

    In this section, we will discuss the equilibrium points of the given COVID-19 model (8). Equilibrium points have two types, namely disease-free equilibrium and endemic equilibrium. We obtained these points by putting the Right-hand side of the system (7) is zero. We suppose that E0 represents disease free equilibrium and endemic equilibrium is represented by E, we have

    E0=(Sc(0),Ec(0),Ic(0),Rc(0),Vc(0))=(Πcμc,0,0,0,0)
    E=(Sc,Ec,Rc,Ic,Vc),where
    Sc=1μc(Πc(αc+μc)Ec),Ec=(ωc+γc+μc)Icαc,Rc=γcIcμc,Vc=ψ1c(ωc+γc+μc)+αcψ2cIc(d+μ+δ).

    We obtain the basic reproductive number R0 by [34], we have

    R0=βEcSc(0)(αc+μc)+αcβIcSc(0)(ωc+γc+μc)(αc+μc)+((ωc+γc+μc)ψ1c+αcψ2c)βVcSc(0)τc(ωc+γc+μc)(αc+μc)

    We consider the following parameters values and initial conditions [34] for our simulations:

    Πc=8859.23×104,βEc=6.11×108,βIc=2.62×108,βVc=3.03×108,μc=3.01×102,αc=0.143,ωc=0.01,γc=0.67,ψ1c=1.30,ψ2c=0.06,τc=2.0.

    Theorem 3.1. The solution of the proposed fractional-order model (8) along initial conditions (9) is unique and bounded in R5+.

    Proof.

    The existence and uniqueness of the solution of system (8) on the time interval (0,) can be obtained by the process discussed in the work of Lin [36]. Subsequently, we have to explain the non-negative region R5+ is positively invariant region. From model (8), we find

    OABCDΘtSc|Sc=0=Πc0
    OABCDΘtEc|Ec=0=βIcScIc+βVcScVc0
    OABCDΘtIc|Ic=0=αcEc0
    OABCDΘtRc|Rc=0=γcIc0
    OABCDΘtVc|Vc=0=ψ1cEc+ψ2cIc0.

    If (Sc(0),Ec(0),Ic(0),Rc(0),Vc(0))R5+, the solution [Sc(t),Ec(t),Ic(t),Rc(t),Vc(t)] cannot escape from the hyperplanes Sc=0,Ec=0,Ic=0,Rc=0andVc=0. Also, on each hyperplane bounding the non-negative orthant, the vector field points into R5+, i.e., the domain R5+ is a positively invariant set.

    In the next theorem, we will show the boundedness of the solution to the proposed model (8).

    Theorem 3.2. The region A={(Sc(t),Ec(t),Ic(t),Rc(t),Vc(t))R5+|0Sc(t)+Ec(t)+Ic(t)+Rc(t)+Vc(t)Πcμc} is a positive invariant set for system (8).

    Proof. For the proof of the theorem, we have from system (8)

    OABCDΘtNc(t)=Πc+ψ1cEc+ψ2cIcωcIcτcVcμcNc

    where

    Nc=Sc+Ec+Ic+Rc.

    Since ψ1cEc,ψ2cIc,ωcIc,τcVc are positive parameters, then

    OABCDΘtNc(t)ΠcμcNc.

    Applying the Laplace transform to above equation, we get

    sΘNc(s)sΘ1Nc(0)ΠcsμcNc(s),

    which further gives

    Nc(s)s1sΘ+μcΠc+sΘ1sΘ+μcNc(0).

    From Eqs (3) and (4) we infer that if(Sc0,Ec0,Ic0,Rc0,Vc0)R5+, then

    Nc(t)ΠctΘEΘ,Θ+1(μctΘ)+EΘ,1(μctΘ)
    (Ωδ)μc(μctΘEΘ,Θ+1(dtΘ))+EΘ,1(dtΘ)
    Πcμc1Γ(1)Πcμc.

    This shows that the total population N(t), i.e., the subpopulations S(t),H(t),I(t) and Q(t), are bounded. This proves the boundedness of the solution of system (8).

    By using the Sumudu transform on the system (8), we get

    q(Θ)ΘΓ(Θ+1)1ΘMΘ(11ΘVΘ)ST{Sc(t)Sc(0)}=ST[ΠcβEcScEcβIcScIcβVcScVcμcSc],
    q(Θ)ΘΓ(Θ+1)1ΘMΘ(11ΘVΘ)ST{Ec(t)Ec(0)}=ST[βEcScEc+βIcScIc+βVcScVc(αc+μc)Ec],
    q(Θ)ΘΓ(Θ+1)1ΘMΘ(11ΘVΘ)ST{Ic(t)Ic(0)}=ST[αcEc(ωc+γc+μc)Ic], (10)
    q(Θ)ΘΓ(Θ+1)1ΘMΘ(11ΘVΘ)ST{Rc(t)Rc(0)}=ST[γcIcμcRc],
    q(Θ)ΘΓ(Θ+1)1ΘMΘ(11ΘVΘ)ST{Vc(t)Vc(0)}=ST[ψ1cEc+ψ2cIcτcVc].

    Rearranging, we get

    ST(Sc(t))=Sc(0)+1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ΠcβEcScEcβIcScIcβVcScVcμcSc],
    ST(Ec(t))=Ec(0)+1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[βEcScEc+βIcScIc+βVcScVc(αc+μc)Ec],
    ST(Ic(t))=Ic(0)+1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[αcEc(ωc+γc+μc)Ic], (11)
    ST(Rc(t))=Rc(0)+1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[γcIcμcRc],
    ST(Vc(t))=Vc(0)+1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ψ1cEc+ψ2cIcτcVc].

    By using the inverse Sumudu transform of system (11), we have

    Sc(t)=Sc(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ΠcβEcScEcβIcScIcβVcScVcμcSc]],
    Ec(t)=Ec(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[βEcScEc+βIcScIc+βVcScVc(αc+μc)Ec]],
    Ic(t)=Ic(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[αcEc(ωc+γc+μc)Ic]], (12)
    Rc(t)=Rc(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[γcIcμcRc]],
    Vc(t)=Vc(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ψ1cEc+ψ2cIcτcVc]].

    Therefore the following recursive formula is obtained.

    Scn+1(t)=Scn(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ΠcβEcScnEcnβIcScnIcnβVcScnVcnμcScn]],
    Ecn+1(t)=Ecn(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[βEcScnEcn+βIcScnIcn+βVcScnVcn(αc+μc)Ecn]],
    Icn(t)=Icn(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[αcnEcn(ωc+γc+μc)Icn]], (13)
    Rcn+1(t)=Rcn(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[γcnIcnμcnRcn]],
    Vcn+1(t)=Vcn(0)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ψ1cEcn+ψ2cIcnτcVcn]].

    And the solution of (13) is provided by

    Sc(t)=limnScn(t),Ec(t)=limnEcn(t),Ic(t)=limnIcn(t),Rc(t)=limnRcn(t),
    Vc(t)=limnVcn(t).

    Stability analysis of model by using fixed-point theory

    Theorem 4.1. Suppose that (Y,|.|) as a Banach space and H a self-map of Y satisfying

    HyHrθYHy+θyr,

    y,rY, and 0θ<1. Assume that H is Picard H-Stable. Suppose that from system (10), we have

    1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ) (14)

    Equation (14) is a Lagrange multiplier.

    Proof. Suppose K as a self-map is given as

    K[Scn+1(t)]=Scn+1(t)=Scn(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ΠcβEcScnEcnβIcScnIcnβVcScnVcnμcScn]],
    K[Ecn+1(t)]=Ecn+1(t)=Ecn(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[βEcScnEcn+βIcScnIcn+βVcScnVcn(αc+μc)Ecn]],
    K[Icn+1(t)]=Icn+1(t)=Icn(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[αcnEcn(ωc+γc+μc)Icn]], (15)
    K[Rcn+1(t)]=Rcn+1(t)=Rcn(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[γcnIcnμcnRcn]],
    K[Vcn+1(t)]=Vcn+1(t)=Vcn(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST[ψ1cEcn+ψ2cIcnτcVcn]].

    By taking the norm and also using the triangular inequality, we obtain

    K[Scn(t)]K[Scm(t)]Scn(t)Scm(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST{ΠcβEcScnEcnScmEcmβIcScnIcnScmIcmβVcScnVcnScmVcmμcScnScm}],
    K[Ecn(t)]K[Ecm(t)]Ecn(t)Ecm(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST{βEcScnEcnScmEcm+βIcScnIcnScmIcm+βVcScnVcnScmVcm(αc+μc)EcnEcm}],
    K[Icn(t)]K[Icm(t)]Icn(t)Icm(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST{αcnEcnEcm(ωc+γc+μc)IcnIcm}], (16)
    K[Rcn(t)]K[Rcm(t)]Rcn(t)Rcm(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST{γcnIcnIcmμcnRcnRcm}],
    K[Vcn(t)]K[Vcm(t)]Vcn(t)Vcm(t)+ST1[1Θq(Θ)ΘΓ(Θ+1)MΘ(11ΘVΘ)×ST{ψ1cEcnEcm+ψ2cIcnIcmτcVcnVcm}].

    Hence K satisfied all the conditions of Theorem (4.1) while

    M=(0,0,0,0,0),M={Scn(t)Scm(t)×(Scn(t)+Scm(t))+ΠcβEcScnEcnScmEcmβIcScnIcnScmIcmβVcScnVcnScmVcmμcScnScm×Ecn(t)Ecm(t)×(Ecn(t)+Ecm(t))+βEcScnEcnScmEcm+βIcScnIcnScmIcm+βVcScnVcnScmVcm(αc+μc)EcnEcm×Icn(t)Icm(t)×(Icn(t)+Icm(t))+αcnEcnEcm(ωc+γc+μc)IcnIcm×Rcn(t)Rcm(t)×(Rcn(t)+Rcm(t))+γcnIcnIcmμcnRcnRcm×Vcn(t)Vcm(t)×(Vcn(t)+Vcm(t))+ψ1cEcnEcm+ψ2cIcnIcmτcVcnVcm

    This shows that K is Picard K-Stable.

    Theorem 4.2. Prove that system (8) has special unique solution.

    Proof. Let Hilbert space H=L2((a,b)×(0,T)) which is given as

    y:(a,b)×(0,T)R,ghdgdh<.

    Suppose that

    M(0,0,0,0,0),M={ΠcβEcScEcβIcScIcβVcScVcμcSc,βEcScEc+βIcScIc+βVcScVc(αc+μc)Ec,αcEc(ωc+γc+μc)Ic,γcIcμcRc,ψ1cEc+ψ2cIcτcVc.

    We show that

    P((Sc11Sc12,Ec21Ec22,Ic31Ic32,Rc41Rc42,Vc51Vc52),(W1,W2,W3,W4,W5)).

    Where (Sc11Sc12,Ec21Ec22,Ic31Ic32,Rc41Rc42,Vc51Vc52), represents the special solutions of system. We use the correspondence between norm and the inner product, we write the equation as

    {ΠcβEc(Sc11Sc12)(Ec21Ec22)βIc(Sc11Sc12)(Ic31Ic32)βVc(Sc11Sc12)(Vc51Vc52)μc(Sc11Sc12),W1}ΠcW1βEcSc11Sc12Ec21Ec22W1βIcSc11Sc12Ic31Ic32W1βVcSc11Sc12Vc51Vc52W1μcSc11Sc12W1
    {βEc(Sc11Sc12)(Ec21Ec22)+βIc(Sc11Sc12)(Ic31Ic32)+βVc(Sc11Sc12)(Vc51Vc52)(αc+μc)(Ec21Ec22),W2}βEcSc11Sc12Ec21Ec22W2+βIcSc11Sc12Ic31Ic32W2+βVcSc11Sc12Vc51Vc52W2(αc+μc)Ec21Ec22W2
    {αc(Ec21Ec22)(ωc+γc+μc)(Ic31Ic32),W3}αcEc21Ec22W3(ωc+γc+μc)Ic31Ic32W3
    {γc(Ic31Ic32)μc(Rc41Rc42),W4}γcIc31Ic32W4μcRc41Rc42W4
    {ψ1c(Ec21Ec22)+ψ2c(Ic31Ic32)τc(Vc51Vc52),W5}ψ1cEc21Ec22W5+ψ2cIc31Ic32W5τcVc51Vc52W5

    Due to large number of e1,e2,e3,e4ande5, both solutions converge to the exact solution. Applying the topological idea, we have the very small positive five parameters (χe1,χe2,χe3χe4andχe5).

    ScSc11,ScSc12χe1ϖ,EcEc21,EcEc22χe2ς,
    IcIc31,IcIc32χe3υ,RcRc41,RcRc42χe4κ,
    VcVc51,VcVc52χe5ζ.

    Where

    ϖ=5(ΠcβEcSc11Sc12Ec21Ec22βIcSc11Sc12Ic31Ic32βVcSc11Sc12Vc51Vc52μcSc11Sc12)W1
    ς=5(βEcSc11Sc12Ec21Ec22+βIcSc11Sc12Ic31Ic32+βVcSc11Sc12Vc51Vc52(αc+μc)Ec21Ec22)W2
    υ=5(αcEc21Ec22(ωc+γc+μc)Ic31Ic32)W3
    κ=5(γcIc31Ic32μcRc41Rc42)W4
    ζ=5(ψ1cEc21Ec22+ψ2cIc31Ic32τcVc51Vc52)W5

    But, it is obvious that

    (ΠcβEcSc11Sc12Ec21Ec22βIcSc11Sc12Ic31Ic32βVcSc11Sc12Vc51Vc52μcSc11Sc12)0
    (βEcSc11Sc12Ec21Ec22+βIcSc11Sc12Ic31Ic32+βVcSc11Sc12Vc51Vc52(αc+μc)Ec21Ec22)0
    (αcEc21Ec22(ωc+γc+μc)Ic31Ic32)0
    (γcIc31Ic32μcRc41Rc42)0
    (ψ1cEc21Ec22+ψ2cIc31Ic32τcVc51Vc52)0

    Where W1,W2,W3,W4,W50

    Therefore, we have

    Sc11Sc12=0,Ec21Ec22=0,Ic31Ic32=0,Rc41Rc42=0,
    Vc51Vc52=0

    which yields that

    Sc11=Sc12,Ec21=Ec22,Ic31=Ic32,Rc41=Rc42,Vc51=Vc52.

    This shows that, the special solution is unique.

    We define the Atanagana-Tufik proposed scheme for fractional derivative model (8) for the COVID-19 epidemic [35]. For this purpose, we suppose that

    {ABC0Dx(t)=g(t,x(t)),x(0)=x0. (17)

    We express the Eq (17) in the form of fractional integral equation by applying fundamental theorem of fractional calculus.

    x(t)x(0)=(1Θ)ABC(Θ)g(t,x(t))+ΘΓ(Θ)×ABC(Θ)t0g(τ,x(τ))(tτ)Θ1dτ. (18)

    At a given point tn+1,n=0,1,2,3,, the above equation is reformulated as

    x(tn+1)x(0)=(1Θ)ABC(Θ)g(tn,x(tn))+ΘΓ(Θ)×ABC(Θ)tn+10g(τ,x(τ))(tn+1τ)Θ1dτ
    =(1Θ)ABC(Θ)g(tn,x(tn))+ΘΓ(Θ)×ABC(Θ)nj=0tj+1tjg(τ,x(τ))(tn+1τ)Θ1dτ. (19)

    Within the interval [tj,tj+1], the function g(τ,x(τ)), using the two-steps Lagrange polynomial interpolation, can be approximate as follows:

    Pj(τ)=τtj1tjtj1g(tj,x(tj))τtjtjtj1g(tj1,x(tj1))
    =g(tj,x(tj))h(τtj1)g(tj1,x(tj1))h(τtj)
    g(tj,xj)h(τtj1)g(tj1,xj1)h(τtj). (20)

    The above approximation can therefore be included in Eq (19) to produce

    xn+1=x0+(1Θ)ABC(Θ)g(tn,x(tn))+ΘΓ(Θ)×ABC(Θ)nj=0(g(tj,xj)htj+1tj(τtj1)(tn+1τ)Θ1dτg(tj1,xj1)htj+1tj(τtj)(tn+1τ)Θ1dτ). (21)

    For simplicity, we let

    Ya,j,1=tj+1tj(τtj1)(tn+1τ)Θ1dτ

    and also

    Ya,j,2=tj+1tj(τtj)(tn+1τ)Θ1dτ
    Ya,j,1=hΘ+1p1p2p3p4Θ(Θ+1) (22)
    Ya,j,2=hΘ+1p5p3p6Θ(Θ+1) (23)

    where

    p1=(m+1j)Θp2=(mj+2+Θ)p3=(mj)Θ
    p4=(mj+2+2Θ)p5=(m+1j)Θ+1p6=(mj+1+Θ).

    By using Eqs (22) and (23), we obtain

    xn+1=x0+(1Θ)ABC(Θ)g(tn,x(tn))+ΘABC(Θ)nj=0(hΘg(tj,xj)Γ(Θ+2)(p1p2p3p4)hΘg(tj1,xj1)Γ(Θ+2)(p5p3p6)).

    We obtain the following for model (8).

    Scn+1=Sc0+(1Θ)ABC(Θ)g(tn,Sc(tn))+ΘABC(Θ)nj=0(hΘf(tj,Scj)Γ(Θ+2)(p1p2p3p4)hΘg(tj1,Scj1)Γ(Θ+2)(p5p3p6))
    Ecn+1=Ec0+(1Θ)ABC(Θ)g(tn,Ec(tn))+ΘABC(Θ)nj=0(hΘg(tj,Ecj)Γ(Θ+2)(p1p2p3p4)hΘg(tj1,Ecj1)Γ(Θ+2)(p5p3p6))
    Icn+1=Ic0+(1Θ)ABC(Θ)g(tn,Ic(tn))+ΘABC(Θ)nj=0(hΘg(tj,Icj)Γ(Θ+2)(p1p2p3p4)hΘg(tj1,Icj1)Γ(Θ+2)(p5p3p6)) (25)
    Rcn+1=Rc0+(1Θ)ABC(Θ)g(tn,Rc(tn))+ΘABC(Θ)nj=0(hΘg(tj,Rcj)Γ(Θ+2)(p1p2p3p4)hΘg(tj1,Rcj1)Γ(Θ+2)(p5p3p6))
    Vcn+1=Vc0+(1Θ)ABC(Θ)g(tn,Vc(tn))+ΘABC(Θ)nj=0(hΘg(tj,Vcj)Γ(Θ+2)(p1p2p3p4)hΘg(tj1,Vcj1)Γ(Θ+2)(p5p3p6)).

    We present the COVID-19 model (7) using fractal-fractional Atangana-Baleanu derivative. We have the following model:

    FFDΘ,Θ10,tSc=ΠcβEcScEcβIcScIcβVcScVcμcSc,
    FFDΘ,Θ10,tEc=βEcScEc+βIcScIc+βVcScVc(αc+μc)Ec,
    FFDΘ,Θ10,tIc=αcEc(ωc+γc+μc)Ic, (26)
    FFDΘ,Θ10,tRc=γcIcμcRc,
    FFDΘ,Θ10,tVc=ψ1cEc+ψ2cIcτcVc.

    In order to present the numerical algorithm for the fractal-fractional COVID-19 model (26), we first describe the general system and present the steps by considering the Cauchy problem below:

    0FFMDΘ,Θ1tx(t)=Φ(t,x(t)). (27)

    The following is obtained by integrating the above equation:

    x(t)x(0)=(1Θ)C(Θ)Θ1tΘ11Φ(t,x(t))+ΘΘ1C(Θ)Γ(Θ)t0τΘ11Φ(τ,x(τ))(tτ)Θ1dτ, (30)

    Let k(t,x(t))=Θ1tΘ11Φ(t,x(t)), then system (26) becomes

    x(t)x(0)=(1Θ)C(Θ)k(t,x(t))+ΘC(Θ)Γ(Θ)t0k(τ,x(τ))(tτ)Θ1dτ, (28)

    At tn+1=(n+1)t, we have

    x(tn+1)x(0)=(1Θ)C(Θ)k(tn,x(tn))+ΘC(Θ)Γ(Θ)tn+10k(τ,x(τ))(tn+1τ)Θ1dτ, (29)

    Also, we have

    x(tn+1)=x(0)+(1Θ)C(Θ)k(tn,x(tn))+ΘC(Θ)Γ(Θ)nj=2tj+1tjk(τ,x(τ))(tn+1τ)Θ1dτ. (30)

    Approximating the function k(t,x(t)), using the Newton polynomial, we have

    Pn(τ)=k(tn2,x(tn2))+k(tn1,x(tn1))k(tn2,x(tn2))t(τtn2)+k(tn,x(tn))2k(tn1,x(tn1))+k(tn2,x(tn2))2(t)2(τtn2)(τtn1) (31)

    Using Eq (31) into system (30), we have

    xn+1=x0+(1Θ)C(Θ)k(tn,x(tn))+ΘC(Θ)Γ(Θ)nj=2tj+1tj{k(tn2,x(tn2))+k(tn1,x(tn1))k(tn2,x(tn2))t(τtn2)+k(tn,x(tn))2k(tn1,x(tn1))+k(tn2,x(tn2))2(t)2(τtn2)(τtn1)}(tn+1τ)Θ1dτ. (32)

    Rearranging the above system, we have

    xn+1=x0+(1Θ)C(Θ)k(tn,x(tn))+ΘC(Θ)Γ(Θ)nj=2k(tj2,xj2)tj+1tj(tn+1τ)Θ1dτ+ΘC(Θ)Γ(Θ)nj=2k(tj1,xj1)k(tj2,xj2)ttj+1tj(τtj2)(tn+1τ)Θ1dτ+ΘC(Θ)Γ(Θ)nj=2k(tj,xj)2k(tj1,xj1)+k(tj2,xj2)2(t)2tj+1tj(τtj2)(τtj1)(tn+1τ)Θ1dτ. (33)

    Now, calculating the integrals in system (33), we get

    tj+1tj(tn+1τ)Θ1dτ=(t)ΘΘ[(mj+1)Θ(mj)Θ],
    tj+1tj(τtj2)(tn+1τ)Θ1dτ=(t)Θ+1Θ(Θ+1)[(mj+1)Θ(mj+3+2Θ)(mj+1)Θ(mj+3+3Θ)],
    tj+1tj(τtj2)(τtj1)(tn+1τ)Θ1dτ=(t)Θ+2Θ(Θ+1)(Θ+2)[(mj+1)Θ{2(mj)2+(3Θ+10)(mj)+2Θ2+9Θ+12}(mj)Θ{2(mj)2+(5Θ+10)(mj)+6Θ2+18Θ+12}].

    Inserting them into system (33), we get

    xn+1=x0+(1Θ)C(Θ)k(tn,x(tn))+Θ(t)ΘC(Θ)Γ(Θ+1)nj=2k(tj2,xj2)[(mj+1)Θ(mj)Θ]+Θ(t)ΘC(Θ)Γ(Θ+2)nj=2[k(tj1,xj1)k(tj2,xj2)][(mj+1)Θ(mj+3+2Θ)(mj+1)Θ(mj+3+3Θ)]+Θ(t)ΘC(Θ)Γ(Θ+3)nj=2[k(tj,xj)2k(tj1,xj1)+k(tj2,xj2)][(mj+1)Θ{2(mj)2+(3Θ+10)(mj)+2Θ2+9Θ+12}(mj)Θ{2(mj)2+(5Θ+10)(mj)+6Θ2+18Θ+12}]. (34)

    Finally, we have the following approximation:

    xn+1=x0+(1Θ)C(Θ)Θ1tΘ11nΦ(tn,x(tn))+ΘΘ1(t)ΘC(Θ)Γ(Θ+1)nj=2tΘ11j2Φ(tj2,xj2)[(mj+1)Θ(mj)Θ]+ΘΘ1(t)ΘC(Θ)Γ(Θ+2)nj=2[tΘ11j1Φ(tj1,xj1)tΘ11j2Φ(tj2,xj2)][(mj+1)Θ(mj+3+2Θ)(mj+1)Θ(mj+3+3Θ)]+ΘΘ1(t)ΘC(Θ)Γ(Θ+3)nj=2[tΘ11jΦ(tj,xj)2tΘ11j1Φ(tj1,xj1)+tΘ11j2Φ(tj2,xj2)][(mj+1)Θ{2(mj)2+(3Θ+10)(mj)+2Θ2+9Θ+12}(mj)Θ{2(mj)2+(5Θ+10)(mj)+6Θ2+18Θ+12}]. (35)

    We obtain the following for system \left(26\right)

    {{S}_{c}}^{n+1} = {{S}_{c}}^{0}+\frac{\left(1-\varTheta \right)}{\mathrm{C}\left(\varTheta \right)}{\varTheta }_{1}{t}_{n}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{n}, {S}_{c}\left({t}_{n}\right)\right)+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +1\right)}\sum _{j = 2}^{n}{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{S}_{c}}^{j-2}\right)\left[{\left(m-j+1\right)}^{\varTheta }-\\{\left(m-j\right)}^{\varTheta }\right]+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +2\right)}\sum _{j = 2}^{n}\left[{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{S}_{c}}^{j-1}\right)-{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{S}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta }\left(m-j+\\3+2\varTheta \right)-{\left(m-j+1\right)}^{\varTheta }\left(m-j+3+3\varTheta \right)\right]+ \\ \frac{\varTheta {{\varTheta }_{1}\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +3\right)}\sum _{j = 2}^{n}\left[{t}_{j}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j}, {{S}_{c}}^{j}\right)-2{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{S}_{c}}^{j-1}\right)+{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{S}_{c}}^{j-2}\right)\right]\\ \left[{\left(m-j+1\right)}^{\varTheta }\left\{2{\left(m-j\right)}^{2}+\left(3\varTheta +10\right)\left(m-j\right)+2{\varTheta }^{2}+9\varTheta +12\right\}-{\left(m-j\right)}^{\varTheta }\left\{2{\left(m-j\right)}^{2}+\left(5\varTheta +10\right)\left(m-\\j\right)+6{\varTheta }^{2}+18\varTheta +12\right\}\right],
    {{E}_{c}}^{n+1} = {{E}_{c}}^{0}+\frac{\left(1-\varTheta \right)}{\mathrm{C}\left(\varTheta \right)}{\varTheta }_{1}{t}_{n}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{n}, {E}_{c}\left({t}_{n}\right)\right)+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +1\right)}\sum _{j = 2}^{n}{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{E}_{c}}^{j-2}\right)\left[{\left(m-j+1\right)}^{\varTheta }-\\{\left(m-j\right)}^{\varTheta }\right]+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +2\right)}\sum _{j = 2}^{n}\left[{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{E}_{c}}^{j-1}\right)-{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{E}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta }\left(m-j+\\3+2\varTheta \right)-{\left(m-j+1\right)}^{\varTheta }\left(m-j+3+3\varTheta \right)\right]+ \\ \frac{\varTheta {{\varTheta }_{1}\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +3\right)}\sum _{j = 2}^{n}\left[{t}_{j}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j}, {{E}_{c}}^{j}\right)-2{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{E}_{c}}^{j-1}\right)+{\mathrm{\Phi }}_{j-2}^{{\varTheta }_{1}-1}g\left({t}_{j-2}, {{E}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta } \\ \left\{2{\left(m-j\right)}^{2}+\left(3\varTheta +10\right)\left(m-j\right)+2{\varTheta }^{2}+9\varTheta +12\right\}-{\left(m-j\right)}^{\varTheta }\left\{2{\left(m-j\right)}^{2}\\+\left(5\varTheta +10\right)\left(m-j\right)+6{\varTheta }^{2}+18\varTheta +12\right\}\right],
    {{I}_{c}}^{n+1} = {{I}_{c}}^{0}+\frac{\left(1-\varTheta \right)}{\mathrm{C}\left(\varTheta \right)}{\varTheta }_{1}{t}_{n}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{n}, {I}_{c}\left({t}_{n}\right)\right)+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +1\right)}\sum _{j = 2}^{n}{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{I}_{c}}^{j-2}\right)\left[{\left(m-j+1\right)}^{\varTheta }-\\{\left(m-j\right)}^{\varTheta }\right]+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +2\right)}\sum _{j = 2}^{n}\left[{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{I}_{c}}^{j-1}\right)-{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{I}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta }\left(m-j+\\3+2\varTheta \right)-{\left(m-j+1\right)}^{\varTheta }\left(m-j+3+3\varTheta \right)\right]+ \\ \frac{\varTheta {{\varTheta }_{1}\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +3\right)}\sum _{j = 2}^{n}\left[{t}_{j}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j}, {{I}_{c}}^{j}\right)-2{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{I}_{c}}^{j-1}\right)+{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{I}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta }\\ \left\{2{\left(m-j\right)}^{2}+\left(3\varTheta +10\right)\left(m-j\right)+2{\varTheta }^{2}+9\varTheta +12\right\}-{\left(m-j\right)}^{\varTheta }\left\{2{\left(m-j\right)}^{2}+\left(5\varTheta +10\right)\left(m-\\j\right)+6{\varTheta }^{2}+18\varTheta +12\right\}\right], (36)
    {{R}_{c}}^{n+1} = {{R}_{c}}^{0}+\frac{\left(1-\varTheta \right)}{\mathrm{C}\left(\varTheta \right)}{\varTheta }_{1}{t}_{n}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{n}, {R}_{c}\left({t}_{n}\right)\right)+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +1\right)}\sum _{j = 2}^{n}{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{R}_{c}}^{j-2}\right)\left[{\left(m-j+1\right)}^{\varTheta }-\\{\left(m-j\right)}^{\varTheta }\right]+\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +2\right)}\sum _{j = 2}^{n}\left[{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{R}_{c}}^{j-1}\right)-{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{R}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta }\left(m-j+\\3+2\varTheta \right)-{\left(m-j+1\right)}^{\varTheta }\left(m-j+3+3\varTheta \right)\right]+ \\ \frac{\varTheta {{\varTheta }_{1}\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +3\right)}\sum _{j = 2}^{n}\left[{t}_{j}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j}, {{R}_{c}}^{j}\right)-2{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{R}_{c}}^{j-1}\right)+{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{R}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta } \\ \left\{2{\left(m-j\right)}^{2}+\left(3\varTheta +10\right)\left(m-j\right)+2{\varTheta }^{2}+9\varTheta +12\right\}-{\left(m-j\right)}^{\varTheta }\left\{2{\left(m-j\right)}^{2}\\+\left(5\varTheta +10\right)\left(m-j\right)+6{\varTheta }^{2}+18\varTheta +12\right\}\right],
    {{V}_{c}}^{n+1} = {{V}_{c}}^{0}+\frac{\left(1-\varTheta \right)}{\mathrm{C}\left(\varTheta \right)}{\varTheta }_{1}{t}_{n}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{n}, {V}_{c}\left({t}_{n}\right)\right)\\ +\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +1\right)}\sum\limits_{j = 2}^{n}{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{V}_{c}}^{j-2}\right)\left[{\left(m-j+1\right)}^{\varTheta }-{\left(m-j\right)}^{\varTheta }\right] \\ +\frac{\varTheta {\varTheta }_{1}{\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +2\right)}\sum\limits_{j = 2}^{n}\left[{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{V}_{c}}^{j-1}\right)\\-{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{V}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta }\left(m-j+3+2\varTheta \right)\\-{\left(m-j+1\right)}^{\varTheta }\left(m-j+3+3\varTheta \right)\right]\\+\frac{\varTheta {{\varTheta }_{1}\left(∆t\right)}^{\varTheta }}{\mathrm{C}\left(\varTheta \right)\mathrm{\Gamma }\left(\varTheta +3\right)}\sum\limits_{j = 2}^{n}\left[{t}_{j}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j}, {{V}_{c}}^{j}\right)-2{t}_{j-1}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-1}, {{V}_{c}}^{j-1}\right)\\+{t}_{j-2}^{{\varTheta }_{1}-1}\mathrm{\Phi }\left({t}_{j-2}, {{V}_{c}}^{j-2}\right)\right]\left[{\left(m-j+1\right)}^{\varTheta }\left\{2{\left(m-j\right)}^{2}+\left(3\varTheta +10\right)\left(m-j\right)+2{\varTheta }^{2}+9\varTheta \\+12\right\}-{\left(m-j\right)}^{\varTheta }\left\{2{\left(m-j\right)}^{2}+\left(5\varTheta +10\right)\left(m-j\right)+6{\varTheta }^{2}+18\varTheta +12\right\}\right].

    To identify the potential effectiveness of Coronavirus disease transmission in the Community, the COVID-19 fractional-order model in the case of Wuhan, China, is presented to analyze with simulations. That's why; we have used Atangana-Baleanu in Caputo sense with Mittag-Leffler law, new Atangana Toufik scheme and fractal fractional derivative model of the COVID-19 in the case of Wuhan China with the initial conditions are provided. Details of the parameters of real data are Πc = 8859.23 × 104, βEc = 6.11 × 10−8, βIc = 2.62 × 10−8, βVc = 3.03 × 10−8, µc = 3.01 × 10−2, αc = 0.143, ωc = 0.01, γc = 0.67, ψ1c = 0.06, τc = 2.0. The various numerical methods identify the mechanical features of the fractional-order model with the time-fractional parameters. The dynamics of the model has changed, and simulations have been divulged. The results of the nonlinear system memory were also detected with the help of fractional values. Figures 15 represents the simulations obtained by ABC method and Figures 610 is obtained with fractal fractional derivative. It is easily observed that in Figures 15, all compartments starts increasing by decreasing the fractional values which converge to steady state. Similar behavior can be seen in Figures 610 but converge rapidly. In Figures 1 and 3, we will see that the concentration of virus and infection rate is directly proportional to each other in Figures 6 and 8. In Figures 1 and 5, we will see that the concentration of the virus and the rate of susceptibility are inversely proportional to each other. It has been shown that physical processes are better explained using the fractional-order derivatives, which are the most notable and reliable component compared to the classical-order case. Existing non-integer-order models are less profitable compared to those operators. The behaviors of the dynamics found in the various fractional orders are shown in the form of numerical results that have been reported.

    Figure 1.  Simulation of {S}_{c}\left(t\right) with ABC fractional derivative.
    Figure 2.  Simulation of Ec(t) with ABC fractional derivative.
    Figure 3.  Simulation of {\mathrm{I}}_{\mathrm{c}}\left(\mathrm{t}\right) with ABC fractional derivative.
    Figure 4.  Simulation of {\mathrm{R}}_{\mathrm{c}}\left(\mathrm{t}\right) with ABC fractional derivative.
    Figure 5.  Simulation of {\mathrm{V}}_{\mathrm{c}}\left(\mathrm{t}\right) with ABC fractional derivative.
    Figure 6.  Simulation of Sc(t) with fractal fractional derivative.
    Figure 7.  Simulation of {\mathrm{E}}_{\mathrm{c}}\left(\mathrm{t}\right) with fractal fractional derivative.
    Figure 8.  Simulation of Ic(t) with fractal fractional derivative.
    Figure 9.  Simulation of {\mathrm{R}}_{\mathrm{c}}\left(\mathrm{t}\right) with fractal fractional derivative.
    Figure 10.  Simulation of {\mathrm{V}}_{\mathrm{c}}\left(\mathrm{t}\right) with fractal fractional derivative.

    In this paper, Atangana-Baleanu in Caputo sense, Atangana-Toufik and Fractal fractional Atangana-Baleanu differential equation model for COVID-19 disease in case of Wuhan China has been investigated. The uniqueness and stability results of the COVID-19 model are investigated by applying the fixed point theory and the iterative method. The boundedness and positivity of the given model also have been investigated. The arbitrary derivative of fractional order has been taken in the Atangana-Baleanu Caputo sense and Fractal fractional Atangana-Baleanu with Mittag-Leffler kernel. Non-linear fractional differential equations were raised from the derivative with the help of a non-singular and non-local kernel within the fractional derivative framework. Atangana-Baleanu with Smudu transform, Atangana-Toufik and Fractal fractional Atangana-Baleanu is used to obtain the derived fraction order COVID-19 model results. Comparison has been made between Atangana-Toufik and Fractal fractional Atangana-Baleanu to verify the efficiency of results. Some theoretical results are also discussed for the fractional-order model. Simulations are carried out to check the actual behaviour of COVID-19 in society. We observe that obtained results are effective for the proposed fractional-order model, which will be helpful in future to analyze the COVID-19 and for control strategies. To control the transmission of COVID-19, stay at home and putting COVID-19 positive individuals into quarantine.

    The authors are thankful to the Institute of Research and Consulting Studies at King Khalid University for supporting this research through grant number # 35-69-S-2020.

    The authors declare no conflict of interest.



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