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Research Article

On variable-order hybrid FracInt Covid-19 mathematical model: optimal control approach

, ORCID Icon, & ORCID Icon
Pages 368-377 | Received 12 Jan 2023, Accepted 22 May 2023, Published online: 28 Jun 2023

Abstract

An optimal control problem for the variable-order fractional-integer mathematical model of vaccination Covid 19 is presented in this research, where the order of the derivatives varies during the course of the time interval, becoming fractional or classical when it is more favourable. The variable-order derivatives are defined here using both the variable-order integral of Riemann–Liouville and the variable-order Caputo derivative. The existence, uniqueness, boundedness and positivity of the solutions are given. In order to test the rate for the detection of symptomatic infected people, two control variables are introduced. The optimality conditions are derived. The fractional-integer operator is approximated using Grünwald–Letnikov. Examples and comparative studies are presented to demonstrate the simplicity of the approximation approaches and the applicability of the utilized methods.

2010 MATHEMATICS SUBJECT CLASSIFICATION:

1. Introduction

Coronavirus has been designated by the world health organization (WHO) as a variant of serious concern. According to scientists, COVID-19 is more contagious compared to severe acute respiratory syndrome (SARS), because there are more routes of transmission and a large number of susceptible people. COVID-19 broke out worldwide at a rapid pace since the end of 2019, which had a tremendous impact on the lives of people around the world where it has claimed the lives of millions. Fighting the COVID-19 epidemic is difficult and expensive, and to control and prevent its spread of it, many governments have implemented very strict Epidemic prevention and control strategies, such as social distancing, self-isolation, medical quarantine, contact tracing, travel restrictions and city shutdown (WHO Int, Citation2020).

Fractional order mathematical models give more information about diseases (Ain, Anjum, & He, Citation2021; Ain et al., Citation2022; Ali, Alshammari, Islam, Khan, & Ullah, Citation2021; Anjum, He, & He, Citation2021; Arenas, Gonzàlez-Parra, & Chen-Charpentierc, Citation2016; Singh, Citation2020; Singh, Ganbari, Kumar, & Baleanu, Citation2021), the constant proportional Caputo fractional derivate (CPC) is proposed by Baleanu, Fernandez, and Akgül (Citation2020) and Sweilam, Al-Mekhlafi, and Baleanu (Citation2021). In epidemic applications constructed in terms of the variable order derivatives see the work by Samko, Kilbas, and Marichev (Citation1993), Samko and Ross (Citation1993), Sun, Chen, Wei, and Chen (Citation2011), Sweilam, Al‐Mekhlafi, and Shatta (Citation2020), Sweilam, Al-Mekhlafi, Mohammed, and Baleanu (Citation2020) and Sweilam and Al-Mekhlafi (Citation2016). Recently, Rosa and Torres (Citation2021) proposed a system of differential equations, the derivatives order varies along the interval of time, also, it is classical or fractional. This idea has many advantages. One such system, a variable order fractional system, is referred to herein as the FractInt system, which has been found to be useful in controlling the disease. Where the derivate order of the fractional-integer (FractInt) system varies accordingly (1) α(t)={0<α01, tt0,1, Tft>t.(1)

We paid special attention in this article to study the variable-order FracInt mathematical model of vaccination Covid-19 and their optimal control (Olivares and Staffetti, Citation2021). The variable-order derivatives are defined here using both the variable-order integral of Riemann–Liouville and the variable-order Caputo derivative. Moreover, the solution properties such as the existence, uniqueness, boundedness and positivity will be studied. We add two-control variables for the testing rate for detecting symptomatic infected individuals. The optimality conditions are derived. The FracInt operator is approximated using Caputo-proportional-constant Grünwald–Letnikov finite difference method (CPC-GLFDM).

To our knowledge, no numerical investigations of variable-order FracInt for COVID-19 vaccination mathematical model utilizing CPC-GLFDM have been conducted.

This article is organized as follows: Some notations and definitions of variable order fractional derivatives are introduced in Section 2. In Section 3, the model with a hybrid variable-order FracInt with control variables is presented, moreover, the positivity, boundedness, existence, uniqueness of the solutions and the stability are discussed. The numerical method CPC-GLFDM are constructed, moreover, the stability analysis for the proposed method is studied in Section 4. In Section 5, numerical simulations are presented. The conclusions are ultimately outlined in Section 6.

2. Basic definitions

Definition 2.1.

Riemann–Liouville’s left and right (L-R) sides integral (Podlubny,Citation1999): (2) aItαf(t)=[atf(s)(ts)α1ds]1Γ(α),t>a,(2) (3) tIbαf(t)=[tb(ts)α1f(s)ds](Γ(α))1,t<b,(3) where <a<b<+, αC,R(α)>0, f(t) is a continuous function and 0<α<1.

Definition 2.2.

The right-side and the left-side Caputo’s derivatives of order α, for a function f(t), fACn[a,b] are defined, respectively by (Podlubny,Citation1999) (4) (CDbαf)(x)=(tCDbαf)(t)=(1)nΓ(nα)tbfn(s)(st)1n+αds,  t<b.(4) (5) (CDa+αf)(t)=(aCDtαf)(t)=1Γ(nα)atfn(s)(ts)1n+αds,t>a,(5) where n=[R(α)]+1, R(α)N0, <a<b<+, αC.

Moreover, if 0<α<1, (Almeida & Torres, Citation2011): abg(t)aCDtαf(t)dt=abf(t)tDbαg(t)dt+f(t)It1αg(t)|ab, abg(t)tCDbαf(t)dt=abf(t)aDtαg(t)dtf(t)It1αg(t)|ab.

Proposition 2.1

(Podlubny, Citation1999). Let L-R sides Caputo’s and Riemann–Liouville’s fractional derivatives of f(t), given respectively aCDtαf,tCDbαf, aDtαf,tDbαf then (6) aDtαf(t)=k=0n1(ta)(kα)Γ(kα+1)fk(a)+aCDtαf(t),(6) (7) tDbαf(t)=tCDbαf(t)+k=0n1(bt)(kα)Γ(kα+1)fk(b),(7) for n=[R(α)]+1, αN. We can prove that aDtαf(t)=aCDtαf(t), if f(s)=f(s)=f(s)==fn1(s)=0, where s = a or b, as in Definition 2.2.

Definition 2.3.

The variable order hybrid operator CPC (Baleanu et al., Citation2020): (8) 0CPCDtα(t)y(t)=(0t(ts)α(t)(y(s)G1(α(t))+y(s)G0(α(t)))ds)(Γ(1α(t)))1=G1(α(t))0RLIt1α(t)y(t)+G0(α(t))0CDtα(t)y(t),(8) where, G0=Q(α(t)+1)α(t), G1=(α(t)+1)Qα(t), Q is a constant.

On the other side, we can define (Baleanu et al., Citation2020): (9) 0CPCItα(t)y(t)=(0texp[G1(α(t))(G0(α(t)))1(ts)]0RLDt1α(t)y(s)ds)1G0(α(t)),(9) where, 0CPCItα(t)y(t) is the CPC inverse operator.

3. Mathematical model of FractInt variable order

FractInt variable order COVID-19 model (Olivares and Staffetti, Citation2021) is developed here. Also, two control variables v1 and v2 are added; v1 denotes the vaccination rate, ranging from 0 to v1u, where v1u is an upper bound to be provided by the designers of the optimal control model. Therefore, the vaccination policy is represented in the model by the term ϕv1uSt, where the parameter ϕ represents the vaccine efficacy level. v2 denotes the test rate for the detecting of asymptomatic infected people, which ranges from v2L to v2u, where v2L and v2u represent a lower and an upper bound, respectively, be provided by the designers of the optimal control model. A new parameter σ is presented in order to be consistent with the physical model problem. Moreover, we avoid dimensional mismatches by modifying the fractional model with an auxiliary parameter σ. As a result, the left side possesses the dimension day1 (Ullah & Baleanu, Citation2021). (10) σα(t)10CPCDtα(t)S=S(Iα+Dβ+Aγ+Rδ)+Hιv1ϕS,σα(t)10CPCDtα(t)I=S(γA+βD+αI+δR)(λ+v2+ζ)I,σα(t)10CPCDtα(t)D=v2I(η+ρ)D,σα(t)10CPCDtα(t)A=Iζ(μ+κ+θ+)A,σα(t)10CPCDtα(t)R=ηD+θA(Rν+ξ),σα(t)10CPCDtα(t)T=Aμ+νR(τ+σ)T,σα(t)10CPCDtα(t)H=Iλ+Dρ+Aκ+ξR+σTHι+v1ϕS,σα(t)10CPCDtα(t)E=Tτ,(10) subject to the following positive values: (11) S(0)=s0,I(0)=i0,D(0)=d0,A(0)=a0,R(0)=r0,T(0)=tu0,H(0)=h0,E(0)=e0.(11) for more details on the variables meaning of the proposed model see .

Table 1. All variables definitions of Eq. (Equation10).

By adding all equations of Equation(10), boundedness of the proposed model solution can be verified as follows: (12) 0CPCDtα(t)NH(t)=0, NH(0)=A0,(12) where, NH is the total population summation and A is a constant. The solution of EquationEq. (12) is given as follows: (13) NH(t)e(G1(α(t))G0(α(t)))tA0.(13)

At t, solutions of EquationEq. (10) are bounded.

Lemma 3.1.

All solutions of EquationEq. (10) are nonnegative under conditions Equation(11) for t0 (Lin Citation2007).

Proof.

Using EquationEq. (11), we have: (14) σα(t)10CPCDtα(t)S|S=0=ιH0,σα(t)10CPCDtα(t)I|I=0=S(βD+γA+δR)0,σα(t)10CPCDtα(t)D|D=0=v2I0,σα(t)10CPCDtα(t)A|A=0=ζI0,σα(t)10CPCDtα(t)R|R=0=ηD+θA0,σα(t)10CPCDtα(t)T|T=0=Aμ+Rν0,σα(t)10CPCDtα(t)H|H=0=Iλ+Dρ+Aκ+Rξ+TσιH+ϕv1S0,σα(t)10CPCDtα(t)E|E=0=τT0.(14)

3.1. Existence and uniqueness

System Equation(10) can be written as follows (15) 0CPCDtα(t)y(t)=ϱ(y(t),t), y0=y(0)0,(15) where, the state variables are (A,I,D,S,T,H,R,E)Tr=y(t), and ϱ is defined as follow

(cϱ1ϱ2ϱ3ϱ4ϱ5ϱ6ϱ7ϱ8)=(c(S(αI+βD+γA+δR)+ιHϕv1S)σ1α(t)(S(δR+βD+αI+γA)(λ+v2+ζ)I)σ1α(t)((ρ+η)D+v2I)σ1α(t)((κ+θ+μ)A+ζI)σ1α(t)(θA+ηD(ξ+Rν))σ1α(t)((τ+σ)T+νR+μA)σ1α(t)(ρD+ξR+λI+κA+σTιH+ϕv1S)σ1α(t)(τT)σ1α(t)), with an initial condition ϵ0. Furthermore, Lipschitz requirement holds (Bonyah, Sagoe, Kumar, & Deniz, Citation2021): (16) ||ϱ(ϵ1(t),t)ϱ(ϵ2(t),t)||G0||ϵ1(t)ϵ2(t)||.(16)

Theorem 3.2.

If the following condition holds, (17) (G0Amaxα(t)Xmaxα(t))(Γ(α(t)1)Q0(α(t)))1<1,(17) the hybrid model Equation(10) has a unique solution

Proof.

Using EquationEqs. (8) and Equation(15), we have (18) ϵ(t)=ϵ(t0)+1Q0(α(t))0texp(G1(α(t))G0(α(t))(ts))0RLDt1α(t)ϱ(ϵ(s),s)ds.(18)

Let B:C(Q,R8)C(Q,R8) and Q=(0,T) achieved that: (19) B[ϵ(t)]=ϵ(t0)+1G0(α(t))0texp(G1(α(t))G0(α(t))(ts))0RLDt1α(t)ϱ(ϵ(s),s)ds.(19)

We have: B[ϵ(t)]=ϵ(t).

The supremum norm on Q is represented by ||.||Q. Thus ||ϵ(t)||Q=suptQ||ϵ(t)||, ϵ(t)C(Q,R8).

Then, ||.||Q with C(Q,R8): Λ||φ(s,t)||Q||ϵ(s)||Q||0tϱ(s,t)ε(s)ds||, with ϱ(s,t)C(Q2,R9) ϵ(t)C(Q,R9), achieved that: supt,sQ|φ(s,t)|=||φ(s,t)||Q.

Also, relation Equation(19) can be written as (20) ||B[ϵ1(t)]B[ϵ2(t)]||Q||1G0(α(t))0texp(G1(α(t))G0(α(t))(ts))(0RLDt1α(t)ϱ(ϵ1(s),s)0RLDt1α(t)ϱ(ϵ2(s),s))ds||Q.Amaxα(t)(Γ(α(t)1)1)G0(α(t))||0t(ts)α(t)2(ϱ(ϵ1(s),s)ϱ(ϵ2(s),s))ds||Q,Amaxα(t)Xmaxα(t)(Γ(α(t)1)1)G0(α(t))||ϱ(ϵ1(t),t)ϱ(ϵ2(t),t)||Q,G0Amaxα(t)Xmaxα(t)(Γ(α(t)1)1)G0(α(t))||ϵ1(t)ϵ2(t)||Q.(20)

Then (21) ||B[ϵ1(t)]B[ϵ2(t)]||QL||ϵ1(t)ϵ2(t)||Q,(21) where L=G0Amaxα(t)Xmaxα(t)G0(α(t))Γ(α(t)1).

So EquationEq. (10) has a unique solution. □

4. The control problem

Let, the admissible control set Ω={(v1(.),v2(.))|v1,v2(.)  are  Lebsegue  measurable  on  [0,1], 0v1(.),v2(.)1,t[0,Tf]},

The objective functional: (22) J(v1,v2)=0Tf(C1(T(t)+E(t))+C2v12(t)+C3v22(t))dt,(22) C1, C2, and C3 are the weight constants. The control problem is find v1(t), v2(t) such that (23) J(v1,v2)=0Tfη(t,A,I,S,R,D,T,E,H,v1,v2)dt,(23) is minimum. It is subject to the constraints (24) aCPCDtα(t)Ψj=ξi.(24)

Where ξi=ξi(t,H,T,I,D,S,R,E,A,v1,v2),i,j=1,,8,Ψj={H,T,I,D,S,R,E,A,v1,v2}, Ψ1(0)=S0, Ψ2(0)=I0, Ψ3(0)=D0, Ψ4(0)=A0, Ψ5(0)=R0,

Ψ6(0)=T0, Ψ1(0)=H0, Ψ1(0)=E0,

In the following using (Agrawal, Citation2008; Sweilam, Al-Mekhlafi, Alshomrani, & Baleanu, Citation2020; Sweilam, Al-Mekhlafi, Mohammed, et al., Citation2020; Sweilam, Al-Mekhlafi, Albalawi, & Tenreiro Machado, Citation2021) we extend numerically optimality conditions

We define the Hamiltonian: (25) H(t,D,A,I,S,R,T,E,H,v1,v2λi)=η(t,D,S,I,A,T,R,E,H,v1,v2,λi)+i=17λiξi(t,D,A,I,S,R,T,E,H,v1,v2).(25)

The necessary conditions of optimal control as in (Agrawal, Citation2008; Sweilam, Al-Mekhlafi, Alshomrani et al., Citation2020; Sweilam, Al-Mekhlafi, Mohammed et al., Citation2020; Sweilam et al., Citation2021) are (26) tCPCDtfα(t)λι=Hϑι, ι=1,,8,(26) where, ϑι={t,S,I,D,A,R,T,H,E,v1,v2,ι=1,,8}, (27) 0=Hus, s=1,2,(27) (28) 0CPCDtα(t)ϑι=Hλι, ι=1,,8,(28) (29) λι(Tf)=0, ι=1,2,,8.(29)

Now, there exists v1, v2, that minimizes J(v1,v2) over Ω with I, E, D, A, S, R, T, H. Furthermore, there exists adjoint variables λi, i=1,2,3,,8, satisfy the following

  1. Adjoint equations:

σα(t)1tCPCDtfα(t)λ1=(λ1αIλ1βDλ1γAλ1δRλ1ϕv1+λ2αI+λ1βD+λ2γA+λ2δR+λ7ϕv1,),σα(t)1tCPCDtfα(t)λ2=(λ1αS+λ2αSλ2(v2+ζ+λ)+λ3v2+λ4ζ+λ7λ),σα(t)1tCPCDtfα(t)λ3=(λ1βS+λ2βSλ3(η+ρ)+λ5η+λ7ρ),σα(t)1tCPCDtfα(t)λ4=(λ1γS+λ2γS(θ+μ+κ)λ4+θλ5+μλ6+κλ7),(30) σα(t)1tCPCDtfα(t)λ5=(λ1δS+λ2δSλ5(ν+ξ)+λ6ν+λ6ξ),(30) σα(t)1tCPCDtfα(t)λ6=(c1λ6(σ+τ)+λ7(σ)+λ8(τ)),σα(t)1tCPCDtfα(t)λ7=(ιλ1ιλ7),σα(t)1tCPCDtfα(t)λ8=(c1),(31) λι(Tf)=0, ι=1,2,,8,(31)

i.e., this is transversality conditions.

  • Optimality conditions: (32) H(t,D,R,I,H,S,E,A,T,v1,v2,λ)=min0u1,u21H(t,D,R,I,H,S,E,A,T,v1,v2,λ).(32)

Moreover: (33) v1=min{1,max{0,ϕS(λ1λ7)2C2}},(33) (34) v2=min{1,max{0,I(λ2λ3)2C3}},(34)

EquationEquations (30) can be obtained from EquationEq. (26), where (35) H=λ1CPC0Dtα(t)S+λ2CPC0Dtα(t)I+λ3CPC0Dtα(t)D+λ4CPC0Dtα(t)A+λ5CPC0Dtα(t)R+λ6CPC0Dtα(t)T+λ7CPC0Dtα(t)H+λ8CPC0Dtα(t)E+(C1(T(t)+E(t))+C2v12(t)+C3v22(t)),(35)

is the Hamiltonian. λs(Tf)=0, s=1,,8. We can obtain EquationEqs. (33) and Equation(34) from EquationEq. (32).

We rewrite EquationEq. (10) using EquationEqs. (33) and Equation(34) (36) 1σ1α(t)0CPCDtα(t)S=(Iα+Dβ+Aγ+Rδ)S+ιHϕv1S,1σ1α(t)0CPCDtα(t)I=S(Iα+Dβ+Aγ+Rδ)(v2+ζ+λ)I,1σ1α(t)0CPCDtα(t)D=Iv2(ρ+η)D,1σ1α(t)0CPCDtα(t)A=IζA(θ+κ+μ),1σ1α(t)0CPCDtα(t)R=Dη+Aθ(Rν+ξ),1σ1α(t)0CPCDtα(t)T=Aμ+Rν(τ+σ)T,1σ1α(t)0CPCDtα(t)H=Iλ+Dρ+Aκ+Rξ+TσιH+ϕv1S,1σ1α(t)0CPCDtα(t)E=τT.(36)

5. Numerical method for solving FracInt optimality systems

5.1. CPC-GLFDM

Let 1α(t)>0, (37) 0CPCDtα(t)y(t)=ξ(t,y(t)), y0=y(0).(37)

Using EquationEq. (8) we have: (38) 0CPCDtα(t)y(t)=1Γ(1α(t))0t(ts)α(t)(y(s)G1+y(s)G0)ds,=G1(α)0RLIt1α(t)y(t)+G0(α(t))0CDtα(t)y(t),=G1(α)0RLDtα(t)1y(t)+G0(α(t))0CDtα(t)y(t).(38)

Now by using GL-approximation, we have: (39) 0CPCDtα(t)y(t)|t=tn=G1(α(tn))τα(tn)1(yn+1+i=1n+1ωiyn+1i)+G0(α(tn))ταn(yn+1i=1n+1μiyn+1iqn+1y0),(39) (40) G1(α(tn))τα(tn)1(yn+1+i=1n+1ωiyn+1i)+G0(α(tn))τα(tn)(yn+1i=1n+1μiy1i+ny0qn+1)=ξ(y(tn),tn),(40) ω0=1, ωi=(1α(tn)i)ωi1, tn=nτ,  τ=TfNn,Nn is a natural number. qi=iα(tn)Γ(1α(tn)) i=1,2,,n+1, μi=(iα(tn))(1)i1, μ1=α(tn), Also, let us assume that (Scherer, Kalla, Tang, & Huang, Citation2011): 0<μi+1<μi<<μ1=α(tn)<1, 0<qi+1<qi<<q1=1Γ(α(tn)+1).

EquationEquation (40) is used to solve EquationEq. (30). Moreover, using the same technique with backward in time, EquationEq. (36) with transitivity condition can be discretized.

Remark 1.

If G0(α(t))=1 and G1(α(t))=0 in Equation(40), this is the disceritization of Caputo opretor using finite differance method (C-GLFDM).

5.2. CPC-GLFDM stability analysis

Consider the following test problem: (41) (0CPCDtα(t))y(t)=Ay(t), 0<α(t)1, t>0, A<0.(41)

Thanks to EquationEq. (38) then, EquationEq. (41) can be discretized as follows: (42) G1(α(tn))τα(tn)1(yn+1+i=1n+1ωiyn+1i)+G0(α(tn))τα(tn)(yn+1i=1n+1μiyn+1iqn+1y0)=Ayn,(42) put C=G1(α(tn))τα(tn)1, B=G0(α(tn))τα(tn). Then from boundness theorem (Arenas et al., Citation2016) we have: (43) yn+1=1C+B(AynCi=1n+1ωiyn+1i+B(i=1n+1μiyn+1i+qn+1y0))yn,(43) then we have: y1<y0 and y0y1yn1ynyn+1.

Now by discretize EquationEq. (38): (44) 0CPCDtα(t)y(t)|t=tn=G1(α(tn))τα(tn)1(yn+1+i=1n+1ωiyi+n+1)+ταnG0(α(tn))(yn+1i=1n+1μiyn+1iqn+1y0),(44) (45) G1(α(tn))τα(tn)1(yn+1+i=1n+1ωiyn+1i)+G0(α(tn))τα(tn)(yn+1i=1n+1μiyn+1iqn+1y0)ξ(y(tn),tn)=TRn,(45) where, TRn<M, M=Cmax0in+1|yi+1|, C=(τα(ti)1+τα(ti)).

The proposed method is convergent because it is consistent and stable (Yuste & Quintana-Murillo, Citation2012).

6. Numerical experiments

This section examines the simulations of optimality systems EquationEqs. (30) and Equation(36). The parameter values in are used with the following initial conditions: I(0)=0.0008, S(0)=0.8474, D(0)=0.0008, A(0)=, R(0)=0.00017, H(0)=0.1489, E(0)=0.0017, T(0)=0.00003, A(0)=0.0002, and transversality conditions λi(Tf)=0,i=1,2,,8. CPC-GLNFDM Equation(40) are presented to study EquationEqs. (30) with Equation(31). EquationEquation (36) will be discretized using the same technique and backward in time, then we solve algebraic system of equations. The numerical results of the optimality systems Equation(30) and Equation(36) are shown graphically at different values of 0<α01 if 0tt, and α1=1 if t<tTf in . shows the behavior of the solution of the proposed model before and after the optimal control when α0=0.97, if 0t10, α1=1 if 10<t350. We found that, in the controlled case, the detected infected people with life-threatening symptoms is lower. Also, the number of deceased people are less in the controlled case. This has enabled us to reduce the number of confirmed infections with life-threatening symptoms and the number of deaths. Our results in show that controlling Covid-19 infection through optimal control is effective and that the FracInt model is the best one. shows the behavior of the control variables at variable-order FracInt α(t) when α0=0.98, if 0t10, α1=1 if 10<t350 and classical order when α=1 and α=0.98. Also, we noted the variable-order FracInt model is the best one. and show how the behavior of the solutions in controlled case varies with the values of α(t) where 0<α01 if 0t10, α1=1 if 10<t150. and show the objective functional values in FracInt case and the classical case. Clear that values of objective functional 22 in case of the variable-order FracInt are better than the classical one.

Figure 1. Comparison of the solutions behivor with and without control using CPC-GLFDM.

Figure 1. Comparison of the solutions behivor with and without control using CPC-GLFDM.

Figure 2. CPC-GLFDM simulations at different α(t) in controlled case.

Figure 2. CPC-GLFDM simulations at different α(t) in controlled case.

Figure 3. Approximations of v1,v2 using the method CPC-GLFDM.

Figure 3. Approximations of v1,v2 using the method CPC-GLFDM.

Figure 4. Controlled soluations behivors at different α(t) of the proposed model by CPC-GLFDM.

Figure 4. Controlled soluations behivors at different α(t) of the proposed model by CPC-GLFDM.

Figure 5. Approximations of v1,v2 using the method CPC-GLFDM.

Figure 5. Approximations of v1,v2 using the method CPC-GLFDM.

Table 2. System (Equation10) parameters.

Table 3. Comparison between the J values and Tf=350, r1=0.5.

Table 4. Comparison between the values of J, Tf=350, r1=0.5 using different methods.

7. Conclusions

In the present article, we paid special attention to study the hybrid variable-order FracInt mathematical model of vaccination Covid-19 and their optimal control. The variable-order derivative is defined using both the variable-order integral of Riemann–Liouville and the variable-order Caputo derivative. It is more general than Caputo fractional operator. The stability analysis of the proposed model was discussed, as well as the existence of equilibrium points. In this model, boundedness, positivity and stability are proved. σ is introduced to make the model compatible with the physical problem. The optimality conditions are numerically derived. CPC-GLNFDM is developed to study the optimality system. Generally, the numerical results show that the proposed FracInt system is effective in controlling the disease. Generally, the numerical findings demonstrate that the FOC system performs better only during a portion of the time period. In order to combat infection, we therefore suggest a system in which the derivative order changes over the course of the time interval, becoming fractional or integer as appropriate. This FracInt-named variable-order fractional model appears to be the most successful at controlling the illness. In the future, the present study can be extended to FracInt delay optimal control.

Disclosure statement

The authors have declared no conflict of interest.

Correction Statement

This article has been corrected with minor changes. These changes do not impact the academic content of the article.

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