Loading [MathJax]/jax/output/SVG/jax.js
Research article Special Issues

Modeling and analysis of fractional order Zika model

  • Received: 26 September 2021 Accepted: 10 November 2021 Published: 10 December 2021
  • MSC : 37C75, 93B05, 65L07

  • We propose mathematical model for the transmission of the Zika virus for humans spread by mosquitoes. We construct a scheme for the Zika virus model with Atangna-Baleanue Caputo sense and fractal fractional operator by using generalized Mittag-Leffler kernel. The positivity and boundedness of the model are also calculated. The existence of uniquene solution is derived and stability analysis has been made for the model by using the fixed point theory. Numerical simulations are made by using the Atangana-Toufik scheme and fractal fractional operator with a different dimension of fractional values which support the theoretical outcome of the proposed system. Developed scheme including simulation will provide better understanding in future analysis and for control strategy regarding Zika virus.

    Citation: Muhammad Farman, Ali Akgül, Sameh Askar, Thongchai Botmart, Aqeel Ahmad, Hijaz Ahmad. Modeling and analysis of fractional order Zika model[J]. AIMS Mathematics, 2022, 7(3): 3912-3938. doi: 10.3934/math.2022216

    Related Papers:

    [1] Awatif J. Alqarni . Modeling and numerical simulation of Lumpy skin disease: Optimal control dynamics approach. AIMS Mathematics, 2025, 10(4): 10204-10227. doi: 10.3934/math.2025465
    [2] Ahmed Alshehri, Miled El Hajji . Mathematical study for Zika virus transmission with general incidence rate. AIMS Mathematics, 2022, 7(4): 7117-7142. doi: 10.3934/math.2022397
    [3] Youming Guo, Tingting Li . Dynamics and optimal control of an online game addiction model with considering family education. AIMS Mathematics, 2022, 7(3): 3745-3770. doi: 10.3934/math.2022208
    [4] Ahmed Alshehri, Saif Ullah . Optimal control analysis of Monkeypox disease with the impact of environmental transmission. AIMS Mathematics, 2023, 8(7): 16926-16960. doi: 10.3934/math.2023865
    [5] Puntipa Pongsumpun, Jiraporn Lamwong, I-Ming Tang, Puntani Pongsumpun . A modified optimal control for the mathematical model of dengue virus with vaccination. AIMS Mathematics, 2023, 8(11): 27460-27487. doi: 10.3934/math.20231405
    [6] Xinjie Zhu, Hua Liu, Xiaofen Lin, Qibin Zhang, Yumei Wei . Global stability and optimal vaccination control of SVIR models. AIMS Mathematics, 2024, 9(2): 3453-3482. doi: 10.3934/math.2024170
    [7] Shinta A. Rahmayani, Dipo Aldila, Bevina D. Handari . Cost-effectiveness analysis on measles transmission with vaccination and treatment intervention. AIMS Mathematics, 2021, 6(11): 12491-12527. doi: 10.3934/math.2021721
    [8] Turki D. Alharbi, Md Rifat Hasan . Global stability and sensitivity analysis of vector-host dengue mathematical model. AIMS Mathematics, 2024, 9(11): 32797-32818. doi: 10.3934/math.20241569
    [9] Suganya Govindaraj, Senthamarai Rathinam . Mathematical modeling and analysis of the effect of the rugose spiraling whitefly on coconut trees. AIMS Mathematics, 2022, 7(7): 13053-13073. doi: 10.3934/math.2022722
    [10] Salma M. Al-Tuwairqi, Asma A. Badrah . Modeling the dynamics of innate and adaptive immune response to Parkinson's disease with immunotherapy. AIMS Mathematics, 2023, 8(1): 1800-1832. doi: 10.3934/math.2023093
  • We propose mathematical model for the transmission of the Zika virus for humans spread by mosquitoes. We construct a scheme for the Zika virus model with Atangna-Baleanue Caputo sense and fractal fractional operator by using generalized Mittag-Leffler kernel. The positivity and boundedness of the model are also calculated. The existence of uniquene solution is derived and stability analysis has been made for the model by using the fixed point theory. Numerical simulations are made by using the Atangana-Toufik scheme and fractal fractional operator with a different dimension of fractional values which support the theoretical outcome of the proposed system. Developed scheme including simulation will provide better understanding in future analysis and for control strategy regarding Zika virus.



    Although the majority of human papillomavirus (HPV) infections are transient and thus are relatively harmless, persistent infection with certain high-risk HPV genotypes can cause cervical precursor lesions and cervical carcinoma [1,2]. Cervical cancer is the most common malignancy reported among women in developing countries and is a leading cause of cancer deaths worldwide, with an estimated 233,000 deaths in 2000 [3]. By 2002, the number of women dying from cervical cancer had risen to 274,000 [4,5,6]. Nearly, all cervical cancers are attributable to genital infection with HPV [7,8]. Up to 70% of women in the general population will acquire genital HPV infection during their lifetime [9]. Most HPV related infections are cleared by treatment or natural healing of the host, while some are persistent and may develop into cervical cancer [10,11]. The progression from persistent infection to cervical cancer typically needs a period of 20 years or longer [12,13]. Fortunately, therapeutic HPV vaccines have made progress in clinical trials after long-term exploration and development. These vaccines include DNA vaccines, RNA replicon vaccines, peptide vaccines, vector vaccines, cell vaccines, and protein vaccines [14,15].

    Mathematical models have been established to understand the dynamics of HPV related disease. In the modeling, some important variables specific for infectious disease are developed. For example, a variable representing how often an infectious individual contacts with a susceptible individual in a unit time is defined as the contact rate. The probability of each contact is set as β, indicating the ability of an infectious person to infect others (susceptible persons) in unit time. Considering that there are other members (e.g., immune persons R(t)), and that the number of members infected by one infected person in a unit time is limited, let N(t)=S(t)+I(t)+R(t), where the total population N(t) is divided into three epidemiological states: S(t) is size of the susceptible population at time t and I(t) is size of the infected population at time t. This generates a formula for the incidence rate: the standard incidence rate βS(t)I(t)N(t) represents the newly infected individuals infected by infectious individuals in unit time at time t. Based on these studies, A Omame et al [16] formulated a mathematical model to investigate the impact of treatment and vaccination on HPV transmission dynamics. Elamin H and Elbasha et al [17] developed a nonlinear, deterministic and age-structured mathematical model. In the same year, Elamin H and Elbasha [18] studied the dynamic behaviors of a two-sex, deterministic model for assessing the potential impact of a prophylactic HPV vaccine with several properties. Mo’tassem and S Robert [19] developed an age-dependent two-sex mathematical model to describe the HPV vaccination program for a vaccine targeting HPV types 16 and 18 in both childhood and adult stages.

    With the development of the mathematical model used to explain the spread of infectious diseases, optimization strategies are introduced into the model. Eihab B M et al [20] studied an optimal control model governed by a system of delay differential equations. The optimal vaccination strategy for a constrained time-varying SEIR (Susceptible, Exposed, Infected and Recovered) epidemic model was solved [21]. T K Kar and AshimBatabyal [22] formulated a nonlinear mathematical SIR epidemic model with a vaccination program. Yang and Tang et al [23] studied a mathematical model to explore the impact of vaccination and treatment on the transmission dynamics of tuberculosis (TB).

    The purpose of this study was to incorporate both therapeutic HPV vaccines and partial immunity compartments based on the present models to investigate how they influence dynamic behavior and to further examine the optimal treatment control measures to minimize the number of asymptomatic patients and treatment costs. We formulate a mathematical model for HPV transmission, and the existence and stability of the equilibria are discussed. In the next section, we present a sensitivity analysis of the model through Partial Rank Correlation Coefficients to identify the key factors in the model. After that, we use optimal control and theory to minimize the number of asymptomatic patients and treatment costs; we also carry out some numerical simulations to highlight the effect of optimal treatment control on the model. Finally, we give concluding remarks.

    Since persistent infection with high-risk HPV genotypes is the main cause of precursor cervical lesions and cervical carcinoma [24], we divided a cohort into three groups, namely, asymptomatic infectious individuals (E), symptomatic infectious females or males(I1), and individuals with persistent HPV infection (I2). The persistently infected individuals who have not been treated will develop cervical cancer (A) after a period of time. Moreover, we consider that E, I1, I2 can be cured and become recovered (R), thus gaining permanent or temporary immunity, which is less reported in previous studies (Table 1). Our assumptions for the dynamic transmission of HPV are demonstrated in Figure 1.

    Table 1.  Description of variables and parameters in the model.
    Variable Description
    S(t) Susceptible individuals
    E(t) Infectious individuals with no symptoms
    I1(t) Individuals with HPV symptoms
    I2(t) Individuals with persistent infection
    A(t) Cancer-infected individuals
    R(t) Recovered individuals
    Parameter Description
    Λ Rate of recruitment
    d Natural mortality rate
    δ1 Disease-induced mortality for individuals
    δ Rate at which recovered individuals become susceptible
    β1 Probability of infection in contact with no symptom persons
    β2 Probability of infection in contact with infectious individuals
    β3 Probability of infection in contact with persistent infections individuals
    α Rate of progression to symptomatic stage for individuals
    α1 Rate at which symptomatic individuals become persistent infections
    α2 Rate at persistent HPV infection develops cervical cancer
    α3 Rate from persistent infections to symptomatic stage
    α4 Rate from symptomatic stage to no symptom stage
    γ1 Rate of recovery from persistent infections
    γ2 Rate of recovery from no symptom stage

     | Show Table
    DownLoad: CSV
    Figure 1.  Flow chart of the HPV transmission.

    The total human population at time t, denoted by N(t), is subdivided into 6 mutually exclusive compartments of S, E, I1, I2, A, R. Thus

    N(t)=S(t)+E(t)+I1(t)+I2(t)+A(t)+R(t). (2.1)

    Combining all the aforementioned definitions and assumptions, it follows that the model for the transmission dynamics of HPV in a population is given by the following system of nonlinear differential equations:

    {dSdt=Λ+δR(t)λ(t)S(t)dS(t),dEdt=λ(t)S(t)+α4I1(t)(α+γ1+d)E(t),dI1dt=αE(t)+α3I2(t)(α1+α4+γ2+d)I1(t),dI2dt=α1I1(t)(α3+α2+d)I2(t),dAdt=α2I2(t)(δ1+d)A(t),dRdt=γ1E(t)+γ2I1(t)(δ+d)R(t), (2.2)

    where

    λ(t)=β1E(t)+β2I1(t)+β3I2(t)N(t). (2.3)

    Here, we shall show the positivity and boundedness of the population.

    Lemma 1. [25] Assume that x(t) satisfies x(0)>0 and a>0, b>0, dxdtbax, then

    limsuptx(t)ba

    .

    Theorem 1. Let S(0)0, E(0)0, I1(0)0, I2(0)0, A(0)0, R(0)0, then the solutions S(t), E(t), I1(t), I2(t), A(t), R(t) are positive for all t>0.

    Proof It follows from the first equation of the system (2.2) that

    dSdt=Λ+δR(t)λ(t)S(t)dS(t),

    which can be re-written as

    ddt{S(t)exp[t0λ(ρ)dρ+dt]}=(Λ+δR)exp[t0λ(ρ)dρ+dt],

    hence

    S(t)exp[t0λ(ρ)dρ+dt]S(0)=t0(Λ+δR)exp[θ0λ(θ)dθ+dθ]dθ,

    so that

    S(t)=S(0)exp[t0λ(ρ)dρ+dt]+t0(Λ+δR)exp[θ0λ(θ)dθ+dθ]dθ>0.

    Similarly, it can be shown that E(t)0, I1(t)0, I2(t)0, A(t)0, R(t)0.

    Theorem 2. The region Ω is positively invariant for model (2.2) with initial conditions in R6+.

    Proof Adding all the equations in the differential equation system (2.2) gives

    dNdtΛdN, (2.4)

    by using Lemma 1, one could easily obtain that

    N(t)Λd+N(0)exp(dt),

    when t, we have

    N(t)Λd.

    Let

    Ω={(S,E,I1,I2,A,R)R6+|S,E,I1,I2,A,R0,S+E+I1+I2+A+RΛd},

    the region Ω is positively invariant.

    In this region, the model can be considered as been epidemiologically and mathematically well-posed [26]. Thus, each solution of the basic model (2.2) with initial conditions in Ω remains in Ω for all t>0.

    The model (2.2) has a disease-free equilibrium (DFE), given by

    x0=(S0,E0,I01,I02,A0,R0)=(Λd,0,0,0,0,0).

    Let X=(E,A,I2,I1,S,R), using the notation [27], the model consists of nonnegative initial conditions together with the following system of equations:

    dXdt=Φ(X)Γ(X),

    where

    Φ(X)=(β1SE+β2SI1+β3SI2N00000),Γ(X)=(α4I1+a1Eα2I2+a4Aα1I1+a3I2αEα3I2+a2I1Λ+β1SE+β2SI1+β3SI2NδR+dSγ1Eγ2I1+(δ+d)R),

    and a1=α+γ1+d, a2=α1+α4+γ2+d, a3=α3+α2+d, a4=δ1+d, a5=d+δ. It is obvious that

    DΦ(x0)=(F000),DΓ(x0)=(V0J3J4),

    the matrices F and V, for the new infection terms and the remaining transfer terms, are, respectively, given by

    F=(β1S0N0β3S0Nβ2S0N000000000000),V=(a100α40a4α2000a3α1α0α3a2), (2.5)

    and

    J3=(β1S0N0β3S0Nβ2S0Nγ100γ2),J4=(dδ0d+δ), (2.6)

    we can get

    R0=ρ(FV1)=β1(a2a3α1α3)+β3αα1+β2a3αa1a2a3a3αα4a1α1α3. (2.7)

    Consequently, we have the following conclusions

    Theorem 3. The DFE of the model (2.2) is globally asymptotically stable if R0<1.

    Proof Model (2.2) can be rewritten as

    (˙E˙A˙I2˙I1)=(FV)(EAI2I1)(1dΛS)F(EAI2I1), (2.8)

    where F and V is given by (2.6), and from [28], we have

    (˙E˙A˙I2˙I1)(FV)(EAI2I1), (2.9)

    when t, SΛd, (E,A,I2,I1)(0,0,0,0), that is, (S,R,E,A,I2,I1)x0 if t. Further, F is nonnegative, V is a nonsingular matrix and all eigenvalues of J4 have positive real part. According to [27], all eigenvalues of FV have negative real part. Therefore, the DFE of the model (2.2) is globally asymptotically stable if R0<1.

    Theorem 4. In the first quadrant, there is no limit cycle in system (2.2).

    Proof We consider the Dulac function as B(S,E)=1SE, now we have

    Θ=(BS)S+(BE)E+(BI1)I1+(BI2)I2+(BA)A+(BR)R=(ΛES2δRES2)+(β2I1Nβ3I2Nβ1E2β2I1Eβ3I2E(EN)2α4I1ES2)α1+α4+γ2+dSEα3+α2+dSEδ1+dSEδ+dSE<0,

    therefore, by the Dulac–Bendixson theorem [29], there is no periodic orbit for the system (2.2).

    The epidemiological implications of backward bifurcation are that the effective disease control is only feasible if the basic reproduction number is reduced to values below another subthreshold less than unity [28]. Compared with backward bifurcation, the epidemiological significance of forward bifurcation means that the disease will disappear as long as the basic reproduction number is less than unity. Clearly, this phenomenon has important public health implications. Next, we analyze the existence and properties of bifurcation of the model.

    Let

    D1=a2a3α1α3αα1>0, D2=a3α1, D3=α2a4, D4=γ1(a2a3α1α3)+γ2αa3αα1a5,

    D5=β1D1+β2D2+D3, D6=1+D1+D2+D3+D4,

    D7=(a1D1α4D2)D6D5+α4D2a1D=D6R01>0.

    Setting the right-hand sides of model (2.2) to zero (at steady state) give by E=(S,E,I1,I2,A,R), where

    S=ΛR0D7(R01)D5(R01)+dD6R0δR0(R01)D4, E=ΛR0D1(R01)D5(R01)+dD6R0δR0(R01)D4,

    I1=ΛR0D2(R01)D5(R01)+dD6R0δR0(R01)D4, I2=ΛR0(R01)D5(R01)+dD6R0δR0(R01)D4,

    A=ΛR0D3(R01)D5(R01)+dD6R0δR0(R01)D4, R=ΛR0D4(R01)D5(R01)+dD6R0δR0(R01)D4.

    It is instructive to characterize the type of bifurcation the model (2.2) may undergo, and we demonstrate the results in Appendix A. This phenomenon is illustrated by simulating model (2.2) with the set of parameter values listed in Table 2. The associated forward bifurcation diagram, depicted in Figure 2, shows that the model has a disease-free equilibrium (corresponding to R0<1) (Figure 3) and an endemic equilibria (corresponding to R0>1) (Figure 4).

    Table 2.  Values of the parameters.
    Parameter Value Reference
    Λ 28802 [30]
    d 0.0162 [30]
    δ1 0.001 [31]
    δ 0.5 [16]
    β1 variable Assumed
    β2 0.72 [31]
    β3 0.81 [31]
    α1 0.09 [16]
    α2 0.57 [16]
    α3 0.5 [33]
    α4 0.000019 [33]
    γ1 0.0099 [16]
    γ2 0.891 [16]
    α 0.5 [32]

     | Show Table
    DownLoad: CSV
    Figure 2.  Forward bifurcation diagram of model (2.2).
    Figure 3.  Changes of the every variable size over time, where β1=0.1, and R0=0.973.
    Figure 4.  Changes of the every variable size over time, where β1=0.16 and R0=1.0868.

    We used the parameter values given in Table 2 (unless otherwise stated) for our numerical simulations and changed the key parameter values to observe the corresponding effects on the disease outbreak.

    To investigate the effect of contact rate on disease infection, we varied β1, as shown in Figure 5. The figure shows that as the contact rate of E(t) with S(t) increases, the number of infected individuals increases, and consequently, the increased contact rate will result in an increase in the disease outbreak.

    Figure 5.  Variation in E(t), A(t) population with different parameters β1.

    To examine the effect of treatment rate on disease infection, we plotted Figure 6. It demonstrates that increasing the parameter γ1 and γ2 decreases the endemic levels of asymptomatic patients and cancer-infected individuals. In particular, if we increased treatment rate γ1 by 400%, the population of the asymptomatic patients and cancer-infected individuals would be decreased by 23%, and treatment rate γ2 would be increased by 68%. Finally, the endemic levels of the cancer-infected individuals population would be decreased by 58%. Moreover, increasing treatment rate γ2 by 81%would decrease the population of asymptomatic patients by 25%.

    Figure 6.  Variation in E(t), A(t) population with different parameters γ1, γ2.

    Latin hypercube sampling (LHS) is one of the Monte Carlo (MC) sampling methods that was first proposed by Mckay [34] in 1979. The advantage of LHS sampling is that the number of iterations is less than in other methods of random sampling, and the clustering phenomenon of sampling is avoided [35].

    Model (2.2) has 14 parameters. In order to identify the factors associated with a given intervention that most strongly affect the spread of a new infection, following [36] we performed Latin Hypercube Sampling on the parameters that appear in R0. For the parameters in Eq. (2.7), Partial Rank Correlation Coefficients (PRCC) were calculated, and a total of 1000 simulations per LHS run were carried out. We chose a uniform distribution as the prior distribution when performing parameter sampling; the parameters of the model were set as input variables, and R0 as the output variable. If the absolute value of the PRCC is larger, the influence of the parameter in R0 is greater. It is assumed that if the p value is greater than 0.05, the parameter is not significant for R0.

    Table 3 lists the PRCC values of the estimated parameters associated with R0. The values reflect the correlation between the parameters β1, γ2, d, α2, α1, α3, β3, α, β2, γ1, α4 and R0. From Table 3 and Figure 7, β1, α1, α3, β3, α, β2 are positively correlated with R0, while γ2, d, α2, γ1, α4 are negatively correlated with R0. Among the parameters, the positive influence of β1 and β2 on R0 is most obvious, that is, as β1 and β2 increase, the values of R0 increase rapidly, and more individuals will become infected. When symptomatic infectious individuals are continue to be infected and suffer from cancer, not only will the treatment be more difficult, the value of R0 will also increase. This indicates that the rate of progression to the symptomatic stage for individuals has a greater positive impact on R0. In addition, γ2 and γ1 have the greatest negative impact on R0, indicating that the value of R0 will decrease if the individuals with HPV symptoms or infectious individuals with no symptoms can be treated. Moreover, we can obtain that |PRCC(γ2)|>|PRCC(β1)|>|PRCC(γ1)|>|PRCC(β2)|>|PRCC(α)|, namely, γ2, β1, γ1, β2, α, play the most important roles in determining R0.

    Table 3.  The range and PRCC values of the estimated parameters with respect to R0.
    Input parameter Range PRCC values p-value
    β1 (0.01,0.5) 0.526755 3.36E-143
    γ2 (0.3,0.9) -0.55735 1.29E-163
    d (0.005,0.05) -0.02163 0.333642
    α2 (0.1,0.9) -0.09826 1.07E-05
    α1 (0.01,0.1) 0.034657 0.121282
    α3 (0.1,0.9) 0.039391 0.078208
    β3 (0.7,0.99) 0.035278 0.114748
    α (0.2,0.8) 0.301851 2.09E-43
    β2 (0.5,0.99) 0.33039 3.82E-52
    γ1 (0.4,0.9) -0.33434 1.98E-53
    α4 (0.001,0.01) -0.02826 0.206432

     | Show Table
    DownLoad: CSV
    Figure 7.  The sensitivity analysis of R0.

    Time-varying sensitivity explains the influence of parameters on state variables when they change with time [35], thereby evaluating the influence and dependence of parameters on state variables in dynamic models. Given the different outbreak time periods of various diseases, one should pay attention to the effect of time period. For example, after being infected with HPV, the clinical manifestations are diverse, and individuals can even be asymptomatic. Therefore, the entire time period of disease prevention, outbreak, infection, and treatment should be considered.

    Based on the pathogenesis of HPV, this section considers the sensitivity analysis of parameters in state variables from two aspects, namely, a continuous period of time and a single point in time.

    The sensitivity analysis of parameters in E(t) and A(t) in continuous time period is shown in Figure 8, we set parameters are input variables, E(t) and A(t) are output variables, the number of samples N=2000.

    Figure 8.  Sensitivity analysis of parameters in E(t) and A(t).

    In Figure 8, we show that the sensitivity of parameters in the early stages of disease outbreak changes significantly, especially before t=500. As can be seen from Figure 8(a), the influence of γ2, γ1, β1, β2, d and α has obvious changes, where the PRCC values of γ2 and γ1 decrease significantly with time, indicating that with the outbreak of disease, people have a certain understanding on the way of disease infection and have made great progress in the treatment. As the time increases, the treatment method quickly forms a treatment system, and it is difficult to progress within a short period of time, meaning that when t>500, the influence of γ2 and γ1 is lessened. The PRCC values of α have positive and negative fluctuations over time, indicating that in addition to the factors for abandoning treatment due to economic or social discrimination, it is also affected by the use of condoms and other protective measures. There are obvious changes illustrated in Figure 8(c), when t<500, the influence of the transmission coefficients and the disease-induced mortality δ1 gradually increase, while due to the improvement of medical intervention, the PRCC values of α3, α1 and α2 decrease.

    The influence of different parameters on state variables is also different at a certain time [37], so the influence of parameters on state variables at t=4000 is studied, and the numerical simulation results can be seen in Table 4, Table 5, Figure 9, Figure 10, and Figure 11.

    Table 4.  The PRCC values of the estimated parameters with respect to E(t) at t=4000.
    Parameter PRCC values p-value
    Λ 0.3064 9.93E-45
    δ 0.1807 3.81E-16
    β1 0.5745 5.13E-176
    β2 0.4073 8.57E-81
    β3 0.0240 0.2831
    d -0.2801 2.19E-37
    α4 0.0080 0.7208
    α -0.0123 0.5810
    γ1 -0.6967 1.48E-290
    α3 0.0782 0.0005
    α1 -0.0745 0.0009
    γ2 -0.2450 9.96E-29
    α2 -0.0567 0.0112
    δ1 0.0240 0.2836

     | Show Table
    DownLoad: CSV
    Table 5.  The PRCC values of the estimated parameters with respect to A(t) at t=4000.
    Parameter PRCC values p-value
    Λ 0.23116 1.14E-25
    δ 0.16689 5.84E-14
    β1 0.53907 3.65E-151
    β2 0.42215 2.95E-87
    β3 0.087454 9.00E-05
    d -0.40263 8.11E-79
    α4 -0.08243 0.000224
    α 0.31927 1.26E-48
    γ1 -0.63554 9.74E-227
    α3 -0.14916 2.03E-11
    α1 0.24989 7.50E-30
    γ2 -0.44721 6.17E-99
    α2 0.14316 1.26E-10
    δ1 -0.14249 1.55E-10

     | Show Table
    DownLoad: CSV
    Figure 9.  Sensitivity analysis of parameters in E(t) and A(t) at t=4000.
    Figure 10.  Scatter diagram of variable E(t) with respect to parameter PRCC values at t=4000.
    Figure 11.  Scatter diagram of variable A(t) with respect to parameter PRCC values at t=4000.

    Figure 9 (a) and Table 4 shows thatβ1, β2 and E(t) are positively correlated, namely, the increase of β1, β2 will lead to the increase of E(t); while γ1, γ2 and E(t) have a significant negative correlation. Moreover, from Figure 10, we can get that the monotonicity of parameters γ2, β1, β2, Λ and d is most significant, in other words, E(t) is mainly affected by these parameters at this time.

    From Figure 11 and Table 5, the monotonicity of parameter β1, β2, γ1, γ2, d, α1 and α is obvious, from Figure 9 (b), β1, β2, α, α1 has a positive correlation with A(t), while γ1, γ2, d has a negative correlation with A(t), which means that at this time, with the increase of β1, β2, α, α1, the number of A(t) will increase, but when γ1, γ2, d increases, the number of A(t) will decrease.

    The spread of infectious diseases can be controlled through reasonable treatment [16]. In this section, the optimal treatment problem will be addressed within the framework of the optimal control problem for constraints [21].

    We recorded γ1 as u, and indicated the rate of people receiving treatment in E(t). Then an additional variable V(t) was introduced:

    ˙V=uE, (4.1)

    where the value of V(t) at the initial time was set to 0. According to the actual situation, the treatment capacity of a city or a country is limited, and the number of people who can be treated is limited as well [38], so the following formula can be established as

    u(t)E(t)<Ω1(t), (4.2)

    where Ω1(t) is the time-dependent upper limit of the number of people that can be treated at each time instant. In addition, state restrictions can be introduced to keep the asymptomatic patients population at a low level, according to [39] we proposed the following constraints

    E(t)<Emax, (4.3)

    where Emax is the upper limit of E(t).

    Let x=[S,E,I1,I2,A,R]T, and the treatment rate u(t), was taken as the control variable. As to the cost function, the state variables and control variables are quadratic functions, which consider both the treatment rate and the number of asymptomatic patients. Based on the above description, the optimal treatment strategy can be formulated as the following problems with inequality constraints and free terminal state:

    Problem (P) {minJ=tf0(A1E2+u2)dt,s.t.˙S=Λ+δR(t)λ(t)S(t)dS(t),˙E=λ(t)S(t)+α4I1(t)(α+u(t)+d)E(t),˙I1=αE(t)+α3I2(t)(α1+α4+γ2+d)I1(t),˙I2=α1I1(t)(α3+α2+d)I2(t),˙A=α2I2(t)(δ1+d)A(t),˙R=u(t)E(t)+γ2I1(t)(δ+d)R(t),S(0)=Ss,E(0)=Es,I1(0)=I1s,I2(0)=I2s,A(0)=As,R(0)=Rs,0uumax,EEmax,uEΩ1, (4.4)

    where tfR+ is the terminal time; A1R+ is the weight coefficient of E(t).

    The optimal control of the problem (P) is expressed as u. Next, we use the maximum principle of Pontryagin [21] to derive the optimal system for problem (P). Prior to this, we converted the inequality constraints in the problem (P) into equality constraints with some non-negative parameter parameters ηi(i=1,2,3,4):

    {u+η1=0,uumax+η2=0,EEmax+η3=0,uEΩ1+η4=0, (4.5)

    and we denoted η=[η1,η2,η3,η4]T. Therefore, the Hamilton function of the problem (P) was obtained as follows

    H=A1E2+u2+φS(Λ+δRλSdS)+φE[λS+α4I1(α+u(t)+d)E]+φI1[αEα3I2(α1+α4+γ2+d)I1]+φI2[α1I1(α3+α2+d)I2]+φA[α2I2(δ1+d)A]+φR[u(t)E+γ2I1(δ+d)R]+μ1(u+η1)+μ2(uumax+η2)+μ3(EEmax+η3)+μ4(uEΩ1+η4), (4.6)

    where φ=[φS,φE,φI,φI2,φA,φR]T are costate variables, μ=[μ1,μ2,μ3,μ4]T are non-negative penalty multipliers.

    By using Pontryagin’s maximum principle, the first-order necessary conditions can be obtained. The optimality conditions with respect to state, costate and parametric variables generate a two-point boundary value problem coupled with a nonlinear complementarity problem [21] as follow:

    ˙x=Hφ, (4.7)
    ˙φ=Hx, (4.8)

    and η0, μ0, ηTμ=0.

    Consider the optimality conditions with respect to the control variable

    Hu=0, (4.9)

    and from Eq. (4.8), the adjoint system can be derived as follow:

    {˙φS=(φSφE)[(β1E+β2I1+β3I2)(NS)N2]+φSd,˙φE=(φSφE)[β1SN(β1SE+β2SI1+β3SI2)N2]+φEa1φI1αφRuμ3μ4u2A1E,˙φI1=(φSφE)[β2SN(β1SE+β2SI1+β3SI2)N2]φEα4+φI1a2φI2α1φRγ2,˙φI2=(φSφE)[β3SN(β1SE+β2SI1+β3SI2)N2]φI1α3+φI2a3φAα2,˙φA=φAa4,˙φR=φRa5φSδ, (4.10)

    with the transversality conditions

    φS(tf)=φE(tf)=φI1(tf)=φI2(tf)=φA(tf)=φR(tf)=0.

    From (4.4) we had 0uumax and uΩ1E, in other words, 0u{umax,Ω1E} is required to be satisfied. Let umax=1 and Ω1<Emax. Hence, Ω1E<umax always establishes.

    By solving (4.9), we got

    u=φEE+μ1φREμ2μ4E2. (4.11)

    We considered the case of Ω1E>umax, under this assumption, u<Ω1E always establishes, therefore, μ4=0. Next, to determine the explicit expression of optimal control without μ1 and μ2, we considered the following three assumptions:

    (1) On the set {t|0<u<umax}, we had μ1=μ2=0, hence, u=(φEφR)E2.

    (2) On the set {t|u=0}, we had μ2=0, therefore, 0=u=(φEφR)E+μ12, and μ10, it is determined that (φEφR)E0.

    (3) On the set {t|u=umax}, we had μ1=0, hence, u=umax=(φEφR)Eμ22, and μ20, it is determined that (φEφR)E2umax.

    Combining the above three cases, the optimal control u is characterized as

    u=max{0,min{(φEφR)E2,umax}}.

    Using the similar arguments, we can characterize the optimal control u under the condition where Ω1Eumax as

    u=max{0,min{(φEφR)E2,Ω1E}},

    from the above discussions, an analytical expression of the optimal treatment rate is derived

    u=max{0,min{(φEφR)E2,umax,Ω1E}}. (4.12)

    In this section, the symplectic pseudospectral method (SPM) developed in [40,41] is used to conduct numerical simulation. It owns structure-preserving property since the inherent Hamiltonian structure of optimal control problems is utilized. The local pseudospectral discretization scheme and the successive convexification technique are incorporated to make the algorithm fast and accurate. On one hand, the SPM can precisely quantify the energy variation for mechanical systems in optimal control and is thus widely used in vehicle trajectory planning [42,43,44]. On the other hand, it has sound stability for optimal control problems with long time span, which makes it an attractive method to solve policy-making problems for biological system [21].

    When using the SPM in this section, the whole time span is divided into 10 regular sub-intervals and a 10-order approximation polynomial is used in each sub-interval. The parameters for the optimal control problem is set as Table 2 (unless otherwise stated in Table 6).

    Table 6.  Parameters and their values used in the simulation.
    Parameter Parameter description Value
    β1 - 0.025
    β2 - 0.072
    β3 - 0.081
    Ω1 Maximum treatment supply at each time instant 2000
    Emax Maximum exposed population 2800
    umax Maximum treatment rate 1
    tf Number of years 40
    A1 Weight on the asymptomatic patients population 0.002

     | Show Table
    DownLoad: CSV

    The controlled solution is shown in Figure 12 along with the uncontrolled solution. It can be seen that the treatment strategy is effective, I1 and A decreases rapidly and almost reaches zero at t=40, and the values of E and I2 are also significantly reduced compared to before the addition of the treatment strategy. In addition, the values of S and R increased at the initial stage, and the effect before adding the treatment strategy is very obvious compared with the effect after the addition.

    Figure 12.  Optimal state trajectories, including (1) the susceptible population, (2) the asymptomatic patient population, (3) the infectious population, (4) the persistent infectious population, (5) the cancer population, (6) the recovered population, (7) Optimal treatment rate and (8) the treated population.

    In the controlled case, the control variable u(t) is continuously reduced and reaches zero at the terminal. It can be seen from Figure 12(7) that the numerical solution of the control variable is in good agreement with the analytical solution given in (4.12), which verifies the characteristics of the optimal control.

    For humans and some social animals, the standard incidence rate is more realistic than the bilinear incidence rate, so we used the standard incidence rate to indicate the ability of an infected person to infect others. Moreover, we assumed that the patients with persistent infection of HPV could be controlled and that mild infection could be cured, thus, those who are cured or have self-healed will gain immunity. Next, we established the model and analyzed its properties. It can be seen from the analysis results that controlling the value of the parameter in R0, making R0 less than 1, the disease will be die out, and when R0 greater than 1, the infection will experience an outbreak and form an endemic disease. The sensitivity analysis of the parameters in R0 and state variables illustrates that the value of R0 can be reduced or increased more efficiently, and the results can be used to control the spread of HPV. In the last section, the treatment rate is selected as the control variable, and the optimal treatment strategy is analyzed theoretically and simulated numerically. The results show that the appropriate treatment strategy can efficiently reduce the spread of the disease.

    This work was supported by the Fundamental Research Funds for the Central Universities (31920200037; 31920200070), the National Natural Science Foundation of China (31560127), the Program for Yong Talent of State Ethnic Affairs Commission of China (No. [2014]121), and Gansu Provincial First-class Discipline Program of Northwest Minzu University (No. 11080305).

    The authors declare that no conflict of interest.



    [1] V. Sikka, V. K. Chattu, R. K. Popli, S. C. Galwankar, D. Kelkar, S. G. Sawicki, et al., The emergence of Zika virus as a global health security threat: A review and a consensus statement of the INDUSEM Joint Working Group (JWG), J. Glob. Infect. Dis., 8 (2016), 3-15. doi: 10.4103/0974-777X.176140. doi: 10.4103/0974-777X.176140
    [2] M. Z. Mehrjardi, Is Zika virus an Emerging TORCH agent? An invited commentary, Virology: Res. Treat., 8 (2017), 1-3. doi: 10.1177/1178122X17708993. doi: 10.1177/1178122X17708993
    [3] D. M. Knipe, P. M. Howley, Fields virology, 5 Eds., Lippincott Williams & Wilkins, 1156 (2017), 1199.
    [4] E. B. Hayes, Zika virus outside Africa, Emerg. Infect. Dis., 15 (2009), 1347-1350. doi: 10.3201/eid1509.090442. doi: 10.3201/eid1509.090442
    [5] D. Baleanu, A. Mousalou, S. Rezapour, On the existence of solutions for some infinite coefficient-symmetric Caputo-Fabrizio fractional integro-differential equations, Bound. Value Probl., 145 (2017). doi: 10.1186/s13661-017-0867-9. doi: 10.1186/s13661-017-0867-9
    [6] D. Baleanu, S. Etemad, S. Rezapour, On a fractional hybrid integro-differential equation with mixed hybrid integral boundary value conditions by using three operators, Alex. Eng. J., 59 (2020), 3019-3027. doi: 10.1016/j.aej.2020.04.053. doi: 10.1016/j.aej.2020.04.053
    [7] D. Baleanu, Z. Nazemi, S. Rezapour, Attractivity for a k-dimensional system of fractional functional differential equations and global attractively for a k-dimensional system of nonlinear fractional differential equations, J. Inequal. Appl., 31 (2014). doi: 10.1186/1029-242X-2014-31. doi: 10.1186/1029-242X-2014-31
    [8] F. Mainardi, Fractional calculus: Theory and applications, Mathematics, 6 (2018), 145. doi: 10.3390/math6090145. doi: 10.3390/math6090145
    [9] M. A. C. Pinto, J. A. T. Machado, Fractional dynamics of computer virus propagation, Math. Probl. Eng., 2014 (2014). doi: 10.1155/2014/476502. doi: 10.1155/2014/476502
    [10] E. K. Akgul, Solutions of the linear and nonlinear differential equations within the generalized fractional derivatives, Chaos, 29 (2019), 023108. doi: 10.1063/1.5084035. doi: 10.1063/1.5084035
    [11] R. Hilfer, Applications of fractional calculus in physics, World Scientific, USA, 2001.
    [12] A. A. Kilbas, H. M. Srivastava, J. J. Trujillo, Theory and applications of fractional differential equations, Elsevier, Amsterdam, 2006.
    [13] H. Bulut, H. M. Baskonus, F. B. M. Belgacem, The analytical solutions of some fractional ordinary differential equations by sumudu transform method, Abst. Appl. Anal., 2013 (2013). doi: 10.1155/2013/203875. doi: 10.1155/2013/203875
    [14] A. Atangana, B. T. Alkahtani, Analysis of the Keller-Segel model with a fractional derivative without singular kernel, Entropy, 17 (2015), 4439-4453. doi: 10.3390/e17064439. doi: 10.3390/e17064439
    [15] A. Atangana, B. T. Alkahtani, Analysis of non-homogenous heat model with new trend of derivative with fractional order, Chaos Soliton. Fract., 89 (2016), 566-571. doi: 10.1016/j.chaos.2016.03.027. doi: 10.1016/j.chaos.2016.03.027
    [16] A. Atangana, A. Akgul, Can transfer function and Bode diagram be obtained from Sumudu transform, Alex. Eng. J., 59 (2020), 1971-1984. doi: 10.1016/j.aej.2019.12.028. doi: 10.1016/j.aej.2019.12.028
    [17] D. Kumar, J. Singh, D. Baleanu, A hybrid computational approach for Klein-Gordon equations on Cantor sets, Nonlinear Dyn., 87 (2017), 511-517. doi: 10.1007/s11071-016-3057-x. doi: 10.1007/s11071-016-3057-x
    [18] M. Farman, A. Ahmad, A. Akgul, M. U. Saleem, M. Naeem, D. Baleanue, Epidemiological analysis of the coronavirus disease outbreak with random effects, CMC-Comput. Mater. Con., 67 (2021), 3215-3227.
    [19] H. Ahmad, N. Alam, M. Omri, New computational results for a prototype of an excitable system, Results Phys., 28 (2021). doi: 10.1016/j.rinp.2021.104666. doi: 10.1016/j.rinp.2021.104666
    [20] M. Caputo, M. Fabrizio, A new definition of fractional derivative without singular kernel, Prog. Fract. Differ. Appl., 1 (2015), 1-13.
    [21] S. Javeed, S. Anjum, K. S. Alimgeer, M. Atif, S. W. Yao, W. A. Farooq, et al., A novel mathematical model for COVID-19 with remedial strategies, Results Phys., 27 (2021). doi: 10.1016/j.rinp.2021.104248. doi: 10.1016/j.rinp.2021.104248
    [22] M. Farman, A. Ahmad, A. Akgul, M. U. Saleem, M. Rizwan, M. O Ahmad, A mathematical analysis and simulation for Zika virus model with time fractional derivative, Math. Method. Appl. Sci., 2020 (2020), 1-12. doi: 10.1002/mma.6891. doi: 10.1002/mma.6891
    [23] I. E. Kibona, C. H. Yang, SIR model of spread of Zika virus infections: Zikv linked to microcephaly simulations, Health, 9 (2017), 1190-1210. doi: 10.4236/health.2017.98086. doi: 10.4236/health.2017.98086
    [24] A. Maysaroh, S. B. Waluya, W. Wuryanto, Analysis and simulation model mathematical model of Zika disease with one serotype virus Zika, Unnes J. Math., 8 (2019), 56-71. doi: 10.15294/ujm.v8i1.23297. doi: 10.15294/ujm.v8i1.23297
    [25] B. S. T. Alkahtani, A. Atangana, I. Koca, Novel analysis of the fractional Zika model using the Adams typepredictor-corrector rule for non-singular and non-local fractional operators, J. Nonlinear Sci. Appl., 10 (2017), 3191-3200. doi: 10.22436/jnsa.010.06.32. doi: 10.22436/jnsa.010.06.32
    [26] S. Rezapour, H. Mohammadi, A. Jajarmi, A new mathematical model for Zika virus transmission, Adv. Differ. Equ., 589 (2020). doi: 10.1186/s13662-020-03044-7. doi: 10.1186/s13662-020-03044-7
    [27] M. Toufik, A. Atangana, New numerical approximation of fractional derivative with non-local and non-singular kernel: Application to chaotic models, Eur. Phys. J. Plus, 132 (2017), 444. doi: 10.1140/epjp/i2017-11717-0. doi: 10.1140/epjp/i2017-11717-0
    [28] M. Higazy, F. M. Allehiany, E. E. Mahmoud, Numerical study of fractional order COVID-19 pandemic transmission model in context of ABO blood group, Results Phys., 22 (2021), 103852. doi: 10.1016/j.rinp.2021.103852. doi: 10.1016/j.rinp.2021.103852
    [29] M. Higazy, E. E. Mahmoud, E. M. Khalil, S. Abdel-Khalek, S. M. Abo-Dahab, H. Alotaibi, Dynamics and robust control of a new realizable chaotic nonlinear model, Complexity, 17 (2021). doi: 10.1155/2021/6692369. doi: 10.1155/2021/6692369
    [30] A. M. S. Mahdy, M. S. Mohamed, K. A. Gepreel, A. AL-Amiri, M. Higazy, Dynamical characteristics and signal flow graph of nonlinear fractional smoking mathematical model, Chaos Soliton. Fract., 141 (2020), 110308. doi: 10.1016/j.chaos.2020.110308. doi: 10.1016/j.chaos.2020.110308
    [31] E. E. Mahmoud, M. Higazy, O. A. Althagafi, A novel strategy for complete and phase robust synchronizations of chaotic nonlinear systems, Symmetry, 12 (2020), 1765. doi: 10.3390/sym12111765. doi: 10.3390/sym12111765
    [32] K. A. Gepreel, M. Higazy, A. M. S. Mahdy, Optimal control, signal flow graph, and system electronic circuit realization for nonlinear Anopheles mosquito model, Int. J. Mod. Phys. C, 31 (2020), 2050130. doi: 10.1142/S0129183120501302. doi: 10.1142/S0129183120501302
    [33] M. Higazy, M. A. Alyami, New Caputo-Fabrizio fractional order SEIASqEqHR model for COVID-19 epidemic transmission with genetic algorithm based control strategy, Alex. Eng. J., 59 (2020), 4719-4736. doi: 10.1016/j.aej.2020.08.034. doi: 10.1016/j.aej.2020.08.034
    [34] M. Higazy, Novel fractional order SIDARTHE mathematical model of COVID-19 pandemic, Chaos Soliton. Fract., 138 (2020), 110007. doi: 10.1016/j.chaos.2020.110007. doi: 10.1016/j.chaos.2020.110007
    [35] A. Mahdy, M. Higazy, Numerical different methods for solving the nonlinear biochemical reaction model, Int. J. Appl. Comput. Math., 5 (2019), 148. doi: 10.1007/s40819-019-0740-x. doi: 10.1007/s40819-019-0740-x
    [36] E. E Mahmoud, M. Higazy, T. M. Al-Harthi, A new nine-dimensional chaotic Lorenz system with quaternion variables: Complicated dynamics, electronic circuit design, anti-anticipating synchronization, and chaotic masking communication application, Mathematics, 7 (2019), 877. doi: 10.3390/math7100877. doi: 10.3390/math7100877
    [37] E. E. Mahmoud, M. Higazy, A. Hammad, S. M. Abo-Dahab, S. Abdel-Khalek, E. M. Khalil, Quaternion anti-synchronization of a novel realizable fractional chaotic model, Chaos Soliton. Fract., 144 (2021), 110715. doi: 10.1016/j.chaos.2021.110715. doi: 10.1016/j.chaos.2021.110715
    [38] Z. Memon, S. Qureshi, B. R. Memon, Assessing the role of quarantine and isolation as control strategies for COVID-19 outbreak: A case study, Chaos Soliton. Fract., 144 (2021), 110655. doi: 10.1016/j.chaos.2021.110655. doi: 10.1016/j.chaos.2021.110655
    [39] S. Qureshi, M. M. Chang, A. A. Shaikh, Analysis of series RL and RC circuits with time-invariant source using truncated M, atangana beta and conformable derivatives, J. Ocean Eng. Sci., 6 (2021), 217-227. doi: 10.1016/j.joes.2020.11.006. doi: 10.1016/j.joes.2020.11.006
    [40] S. Qureshi, R. Jan, Modeling of measles epidemic with optimized fractional order under Caputo differential operator, Chaos Soliton. Fract., 145 (2021), 110766. doi: 10.1016/j.chaos.2021.110766. doi: 10.1016/j.chaos.2021.110766
  • This article has been cited by:

    1. R. Musa, R. Willie, N. Parumasur, Behavior Change in a Virus-Resistance HIV-1 Mathematical Model, 2022, 15, 1995-4239, 138, 10.1134/S1995423922020069
    2. Oluwatayo Michael Ogunmiloro, Kayode James Adebayo, Multiple control strategies against human papilloma virus spread: A mathematical model, 2023, 34, 0129-1831, 10.1142/S0129183123500080
    3. Zhenzhen Lu, YangQuan Chen, Yongguang Yu, Guojian Ren, Conghui Xu, Weiyuan Ma, Xiangyun Meng, The effect mitigation measures for COVID-19 by a fractional-order SEIHRDP model with individuals migration, 2023, 132, 00190578, 582, 10.1016/j.isatra.2022.12.006
    4. Xiaotao Han, Hua Liu, Xiaofen Lin, Yumei Wei, Ma Ming, Yao Zhong Zhang, Dynamic Analysis of a VSEIR Model with Vaccination Efficacy and Immune Decline, 2022, 2022, 1687-9139, 1, 10.1155/2022/7596164
    5. Hua Liu, Xiaofen Lin, Xinjie Zhu, Qibin Zhang, Yumei Wei, Gang Ma, Modeling and analysis of a human papilloma virus transmission model with impact of media, 2024, 375, 00255564, 109247, 10.1016/j.mbs.2024.109247
    6. 丽娜 王, Dynamic Analysis of a Kind of HPV Transmission Model Incorporating Media Impact and Early Screening, 2024, 13, 2324-7991, 3845, 10.12677/aam.2024.138366
    7. Veronicah Nyokabi Njenga, Cyrus Gitonga Ngari, Winifred Mutuku Nduku, Livingstone Serwadda Luboobi, Nian-Sheng Tang, Modelling the Impact of Hygiene and Treatment on the Dynamics of Childhood Diarrhea in Nairobi County, Kenya, 2024, 2024, 0161-1712, 10.1155/2024/3336826
    8. M. Arunkumar, Praveen Kumar Rajan, K. Murugesan, Mathematical Analysis of an Optimal Control Problem for Mitigating HPV Transmission and Cervical Cancer Progression through Educational Campaigns, 2025, 2731-8095, 10.1007/s40995-025-01804-2
    9. Hua Liu, Xinjie Zhu, Xiaofen Lin, Qibin Zhang, Yumei Wei, Stability analysis and optimal control of a SVICR HPV model with vaccination and cancerous delay, 2025, 1598-5865, 10.1007/s12190-024-02335-6
  • Reader Comments
  • © 2022 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(2648) PDF downloads(156) Cited by(4)

Figures and Tables

Figures(12)

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog