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Front. Phys., 05 July 2019 |

Optimal Control Problem of a Non-integer Order Waterborne Pathogen Model in Case of Environmental Stressors

  • Department of Logistics Management, University of Turkish Aeronautical Association, Ankara, Turkey

In this work, we extend a mathematical model, which has been proposed for susceptible and infected compartments together with pathogen population, by including recovered subgroup. It is known that environmental pollution, such as contaminated drinking water and lack of an ordinary toilet, affects individuals and such negative impacts can be defined as “stressors.” In order to include the influence of such stressors, susceptible subpopulation has been divided into two groups as the one affected by stress or not. Thus, spread of the disease is expressed in terms of a five-dimensional system. Moreover, we extend this model with the use of a time fractional derivative due to non-local effects of water pollution and we prove that the solution is non-negative and bounded from above. Then, we perform stability analysis for the disease-free equilibrium point. Afterward, the next step is to apply optimal control theory to optimize the decay rate of pathogens and the stress related parameters so that the number of infected individuals and the pathogen population can be minimized. Finally, we present some numerical results to find out the most appropriate control policy and the effect of the fractional order.

1. Introduction

Water is one of the most required natural resources for life and it is not only vital for drinking but also needed for other daily uses. Every individual deserves safe water; but, unfortunately it has been estimated that at least 2 billion people have to use contaminated drinking water [1]. According to “Water for health: taking charge” report of WHO, about 3.4 million people died due to water related illnesses [2]. Specifically, almost 6,000 children die every day due to lack of clean water and hygienic conditions [3]. On the other hand, 35% of health care facilities in low and middle-income countries do not have water and soap, and half of the world's population is predicted to live in water-stressed zones by 2025 [3].

Mathematical models offer new ways to investigate the population dynamics in case of pollution related diseases. With the use of such models, strategic decisions can be tested beforehand, and we can reduce cost and save time. For example, in 2003, influence of stress to spread of infectious diseases is investigated [4]. In 2010, a SIR model is extended by including the pathogen population and, person–person and person–water–person interactions are modeled. On the other hand, spread of cholera due to unclean water is discussed for a delayed differential equation (DE) together with stability analysis [5]. The effect of heterogeneity by neglecting person-to-person transmission is studied [6]. On the other hand, the spread of virus/worm in computer networks have been modeled with DEs and optimal attack strategies have been decided [7] and the result can be useful to set network security protocols up. Another model including the influence of socioeconomic classes is constructed for multi patches [8]. As a different way to model waterborne diseases, networks are incorporated to express both indirect environment-to-human and direct human-to-human transmission routes [9]. As a two-dimensional model, we can mention the study on a system of reaction-diffusion equations published in 2018 [10].

Fractional differentiation and integration operators can be defined as the generalizations of their integer counterparts, where we use the fractional order to replace with the integer order [1113]. A review including a systematic classification and applications can be found in the studies [14, 15]. Indeed, the integer-order model is a special case of the generalized fractional order model where the solution of the fractional order model must converge to the solution of the integer order model as the order approaches one. On the other hand, fractional DEs are suitable to express the real world phenomena which are influenced by hereditary and memory properties that cannot be expressed with integer order models [16]. Some application areas can be noted as physics [17], viscoelasticity [18], control systems [19], economics [20], finance [21], biology [22, 23], and bioengineering [24]. Specifically, anomalous dispersion is modeled with Riemann–Liouville derivative in space [25]. A pn semiconductor diode is described under sinusoidal operational conditions with the use of fractional calculus and some experimental results are compared with the model [26]. Viscoelastic materials are modeled with a variable order DE [27] and Caputo-Fabrizio derivative [28]. Three different fractional operators are used to investigate the properties of blood ethanol concentration [29]. Coexistence of tuberculosis and diabetes mellitus has been examined [30], while a honeybee population growth model is presented [31]. On the other hand, the construction of diffusion equation is obtained with the Atangana–Baleanu fractional integral [32]. Existence and uniqueness of Caputo time fractional Navier-Stokes equation is proven [33], whereas flow characteristics of gas and oil are discussed for a heterogeneous media [34].

For some real world phenomena, data is available and it is quite straightforward to test contribution of fractional derivative. For example, Diethelm has compared the numerical solution of the integer order and fractional order models with the data and he has revealed that the fractional order model fits the data better [35]. Then, this study has been extended with the use of other fractional derivatives [36]. As another epidemic disease, namely Ebola, has been modeled with a Caputo fractional derivative and the numerical results agree well with the data [37]. On the other hand, economic growth of the Group of Seven (G7) in 1973–2016 period has been modeled with fractional order derivative and it has been underlined by comparison with the data that the fractional model gives better results than the integer order model due to memory effect [38]. In addition, the data of varicella disease outbreak in Shenzhen city of China in 2015 has been used to compare the numerical solution of the fractional order model and success of the fractional derivatives in modeling such epidemiological phenomena has been exemplified [29].

The topic of fractional optimal control problems (FOCPs) has started to gain interest. The number of studies on FOCPs is quite less when compared to the studies on the fractional DEs; but, it has been an emerging research field for a while. For example, we suggest the studies on optimization of biological reactive systems [39, 40], where construction of a model and derivation of its numerical solution have been discussed. Furthermore, we can mention some studies on tumor dynamics [41], trajectory tracking [42], fractional–order sliding mode controller [43], virus infection [44], an HIV/AIDS epidemic model [45], dynamics of Human African trypanosomiasis [46], the light tracking systems [47], and human respiratory syncytial virus infection [44].

In 2019, transmission of waterborne diseases is expressed for susceptible compartment, susceptible stressed compartment and infected compartment with the inclusion of pathogen population and stress related negative effects [48]. Motivated by this recent work, a new non-integer order model is constructed with the addition of recovered subgroup in this current study. For the new model, we prove that the solution is non-negative and bounded from above. Then, local stability of the disease free equilibrium point has been analyzed with the use of the reproduction number. On account of unfortunate facts reported by WHO [1, 3], it is inevitable to figure some strategies out to stop any harm of water pollution. Thus, we apply optimal control theory to decide the optimal intervention strategies to minimize the number of infected individuals and to reduce the pathogen population. We believe that this study can be a nice start to optimize stress related models to found healthier generations of all creatures. The rest of this study is organized as follows: In section 2, we construct a non-integer order model with constant controls. Then, we prove that the solution is bounded and we present stability analysis for the disease free equilibrium point. In section 3, we construct an OCP and we derive the optimality conditions. Section 4 is devoted to some illustrative examples for testing purposes. Then, we conclude the study.

2. Model formulation

In this section, we derive a non-integer order waterborne pathogen model which is an extended version of the one in the study [48] with the inclusion of recovered compartment. Environmental pollution is created in several years due to accumulated causes. Here, we use time fractional derivative to express temporal change both in the host and pathogen population.

We define the (left) generalized derivative with Caputo fractional derivative for t > a as Podlubny [12]

Dtqag(t)={1Γ(1q)atg(s)(ts)q ds,      0<q<1,g(t),    q=1,    (2.1)

where the Gamma function Γ :(0, ∞) → ℝ is defined as Γ(t)=0e-uut-1du. The corresponding right differentiation operator is defined as

Dbqtg(t)={1Γ(1q)tbg(s)(st)q ds,     0<q<1,g(t),                      q=1.    (2.2)

We mention the generalized right Riemann-Liouville (RL) derivative as

 tRDtfqg(t)={1Γ(1q)ddttbg(s)(st)q ds,             0<q<1,g(t),q=1.    (2.3)

Before presenting the model, we note a relation between the generalized Caputo and RL derivatives as

 tRDtfqg(t)= tDtfqg(t)+g(tf)Γ(1q)(tft)q.    (2.4)

The model is constructed by dividing the total population N(t) into four compartments, namely, susceptible population S1(t), susceptible population influenced by environmental stressors S2(t), infected population I(t), and recovered population R(t). To discuss the contribution of pollution to infection, pathogen pollution (Cells/liter) is included and it is denoted by P(t). The birth rate of susceptible individuals is fixed as Λ. A proportion (1 − p) of newborns joins S1 class, whereas the rest contributes to S2 class. Due to stressors, susceptible individuals enter stressors group at a rate of θ. The natural mortality rate and disease induced death rate are given by μ and α, respectively. Infectious individuals join recovered subgroup at a rate of ϕ. People are recovered at a rate of γ and a proportion r of them enters into susceptible class, while the rest joins stressors compartment. On the other hand, the disease is transmitted at a rate of β and transmission is affected due to stress related parameters, namely level of pollution affecting transmission ω and effect of pollution ρ. Moreover, the pathogen population grows at a rate of ξ and it decays at a rate of η. In Table 1, we present the description, units and values of the parameters.


Table 1. Parameter values.

Then, we reach the following model:

Dtq0S1(t)=(1p)ΛqθqS1(t)βqS1(t)P(t)                      μqS1(t)+rγqR(t),    (2.5a)
Dtq0S2(t)=pΛq+θqS1(t)βq(1+ωρ(1u1))S2(t)P(t)                     μqS2(t)+(1r)γqR(t),    (2.5b)
Dtq0I(t)=βqS1(t)P(t)+βq(1+ωρ(1u1))S2(t)P(t)                   (ϕq+αq+μq)I(t),    (2.5c)
Dtα0R(t)=ϕqI(t)(γq+μq)R(t),    (2.5d)
Dtα0P(t)=ξqI(t)ηq(1+u2)P(t),    (2.5e)
S1(0)=S1,0, S2(0)=S2,0, I(0)=I0, R(0)=R0, P(0)=P0,

where u1 and u2 stand for the fixed control terms. We note that the model is expressed for a generalized derivative. Indeed, it is possible to investigate the model for both classical and fractional order derivative. The reason of using fractional derivative is its success in a good fit to available data as discussed in the literature.

Remark 2.1. We note that it is possible to obtain analytical solution of some epidemiological model (such as SIS models) via a Lie algebra methodology. Due to lack of symmetry in more complicated models, this method is not widely used in biological or social systems. For the readers interested in this technique, we can suggest some studies as Shang [49, 50].

2.1. Basic Properties

To prove the non-negative solution of the model, we need the generalized mean value theorem and the corollary.

Lemma 2.2. Odibat and Shawagfeh [51] Let g(x) ∈ C[a, b] and aCDtqg(t)C(a,b] for 0 < q ≤ 1. Then, for asb andx ∈ (a, b], the following estimate holds:

g(x)=g(a)+1Γ(q)(aCDtqg)(s)(xa)q.    (2.6)

Corollary 2.3. Let g(x) ∈ C[a, b] and aCDtqg(t)C(a,b] for 0 < q ≤ 1. If aCDtqg(t) is non-negativex ∈ (a, b), then g(x) is non-decreasing for each x ∈ [a, b]. If aCDtqg(t) is non-positivex ∈ (a, b), then g(x) is non-increasing for each x ∈ [a, b].

To show that the solution is bounded from above, we use the Laplace transform. The Laplace transform of the (left) Caputo derivative is obtained as

L{aCDtqg(t)}=sqG(s)g(0)sq1.    (2.7)

Moreover, the Laplace transform of the Mittag-Leffler function is given by

L{tp-1Eq,p(-atq)}=sq-psq+a,    (2.8)

where Eq,p(z)=i=0ziΓ(qi+p) and Eq,p(z)=zEq,q+p(z)+1Γ(p).

Theorem 2.4. Let X(t)=(S1(t),S2(t),I(t),R(t),P(t)) be the unique solution of the model (2.5) for t ≥ 0. Then, the solution X(t) remains in +5.

Proof: By the study [52, Thm. 3.1, Remark 3.2], the solution to the model (2.5) is unique for t > 0. On the other hand, we observe that

Dtq0S1|S1=0=(1p)Λq+rγqR(t)0    (2.9a)
Dtq0S2|S2=0=pΛq+θqS1(t)+(1r)γqR(t)0,    (2.9b)
Dtq0I|I=0=βqS1(t)P(t)+βq(1+ωρ(1u1))S2(t)P(t)0,    (2.9c)
Dtq0R|R=0=ϕqI(t)0,    (2.9d)
Dtq0P|P=0=ξqI(t)0.    (2.9e)

It means that the vector field points to +5 and the solution lies in +5 for a non-negative initial condition [51].

Theorem 2.5. Let X(t)=(S1(t),S2(t),I(t),R(t),P(t)) be the solution of the model (2.5) for t > 0. Then, the solution X(t) is bounded from above.

Proof: We add the Equations (2.5a)-(2.5d) to reach

Dtq0N(t)=ΛqμqN(t)αqI(t)ΛqμqN(t).    (2.10)

Using the Laplace transform (2.7), we obtain

sqL(N(t))-sq-1N(0)Λqs-μqL(N(t)).    (2.11)

Arranging, we get

L(N(t))Λqs-1sq+μq+N(0)sq-1sq+μq=Λqsq-(1+q)sq+μq+N(0)sq-1sq+μq.    (2.12)

Applying inverse Laplace transform to (2.12), we obtain

N(t)L-1{Λqsq-(1+q)sq+μq}+L-1{N(0)sq-1sq+μq}       (2.8)ΛqtqEq,q+1(-μtq)+N(0)Eq,1(-μtq)       ΛqμqμqtqEq,q+1(-μtq)+N(0)Eq,1(-μtq)       max{Λqμq,N(0)}(μqtqEq,q+1(-μtq)+Eq,1(-μtq))       =CΓ(1)=C,    (2.13)

where C=max{Λqμq,N(0)}. Thus, N(t) is bounded from above which means that the solutions S1(t), S2(t), I(t) and R(t) are bounded from above.

We proceed with the equation for pathogen population (2.5e), which is written as

Dtq0P(t)=ξqI(t)ηq(1+u2)P(t)(2.13)ξqCηqP(t).    (2.14)

Then, the similar technique is applied to show that the pathogen pollution P(t) is bounded from above.

2.2. Stability Analysis of the Disease Free Equilibrium Point

The disease free equilibrium (DFE) point E0=(S10,S20,0,0,0) is obtained by equating the right-hand side of the Equations (2.5a)–(2.5b) to zero. Then, we obtain

S10=(1-p)Λθ+μ,S20=Λ(pμ+θ)μ(θ+μ).    (2.15)

To discuss the local stability of the DFE point E0, we need to obtain the basic reproduction number, namely a parameter measuring the contribution of a single infection to secondary infections [53]. We define the matrices for the new infections and the other terms for the Equations (2.5c)–(2.5e) as

F=(βS1P+βq(1+ωρ(1-u1))S2P0),V=((γq+αq+μq)I-ξqI+ηq(1+u2)P).    (2.16)

We note that the contribution of the recovered compartment does not appear here, since recovered individuals do not directly join the infected subgroup. Then, partial derivatives of these matrices with respect to I and P are obtained and then they are evaluated at the DFE point to obtain

F=(0βS10+βq(1+ωρ)S2000),V=((γq+αq+μq)0-ξqηq).    (2.17)

We reach the next generation matrix FV−1 and its spectral radius is given by Sharma and Kumari [48]

R0=ξqβqΛq(μq+θq(1+ωρ(1-u1)))+(1-u1)ωρpμq(1+u2)ηqμq(θq+μq)(γq+αq+μq).    (2.18)

We mention a result to derive stability analysis [54].

Lemma 2.6. The DFE point E0 is locally asymptotically stable if all eigenvalues λi of the linearization matrix of the model (2.5) satisfy |arg(λi)|>qπ2.

Now, we prove the following result for the DFE point.

Theorem 2.7. The DFE point E0 of the model (2.5) is locally asymptotically stable if R0<1 and unstable if R0>1.

Proof: The Jacobian matrix associated with the model (2.5) is obtained as

J(E0)=(-(θq+μq)00rγq-βS10θq-μq0(1-r)γq-βq(1+ωρ(1-u1))S2000-(ϕq+αq+μq)0βq(1+ωρ(1-u1))S2000ϕq-(γq+μq)000ξq0-ηq(1+u2)).    (2.19)

The characteristic equation of this matrix is given by p(λ) = (λ + μq)(λ + θq + μq)(λ + γq + dq)f(λ) and three eigenvalues are found as −μq, −(θq + μq) and −(γq + μq), which satisfy Lemma 2.6. Moreover, the quadratic part is written as f(λ)=λ2+c1λ+c0, where c1=ηq(1+u2)+ϕq+αq+μq, c0=ηq(1+u2)(ϕq+αq+μq)(1-R0). By Routh-Hurwitz criterion, we check that c1 > 0 and c0 > 0 with R0<1, which shows that the roots of f(λ) are negative. Then, we prove the desired result.

3. Optimal control problem

We investigate some suitable policies to reduce the reproduction number associated with the model. Specifically, we optimize the decay rate of pathogens and the stress related parameters with the aim of minimizing the number of infected individuals and reducing the pathogen population in size with the use of non-constant controls u1(t) and u2(t), respectively. Therefore, we determine their optimal values with the following cost functional:

min(u1,u2)Uad J(u1,u2)=I(tf)+P(tf)         +0tf(ω1I(t)+ω2P(t)+ω32u12(t)+ω42u22(t))dt,    (3.1)

subject to the system

Dtq0S1(t)=(1p)ΛqθqS1(t)βqS1(t)P(t)μqS1(t)                      +rγqR(t),    (3.2a)
Dtq0S2(t)=pΛq+θqS1(t)βq(1+ωρ(1u1(t)))S2(t)P(t)                     μqS2(t)+(1r)γqR(t),    (3.2b)
Dtq0I(t)=βqS1(t)P(t)+βq(1+ωρ(1u1(t)))S2(t)P(t)                  (ϕq+αq+μq)I(t),    (3.2c)
Dtα0R(t)=ϕqI(t)(γq+μq)R(t),    (3.2d)
Dtα0P(t)=ξqI(t)ηq(1+u2(t))P(t),    (3.2e)
S1(0)=S1,0, S2(0)=S2,0, I(0)=I0, R(0)=R0, P(0)=P0,

where the admissible space of controls is given by

Uad={(u1(t),u2(t)) | (u1(t),u2(t)) is measurable with    0.05u1(t)0.95, 0u2(t)1  for all t[0,tf]}.

Thus, the optimal control u*(t)=(u1*(t),u2*(t))Uad is required so that J(u*)=min(u1(t),u2(t))UadJ(u1(t),u2(t)) is reached. We observe that R0u1<0 and R0u2<0. Then, we can determine the optimal values of u1 and u2 to make R0<1.

3.1. Optimality System

We use Pontryagin's maximum principle [5557] to obtain the necessary optimality conditions where the adjoint (costate) functions attach the state equation to the cost functional J. Indeed, this technique allows us to express the control in terms of the state and the adjoint functions. Moreover, Pontryagin's maximum principle interprets the constraint minimization problem (3.1)-(3.2) as another minimization problem (Hamiltonian) with respect to the controls. Therefore, we construct the Hamiltonian as

H(X,U,P)=(ω1I(t)+ω2P(t)+ω32u12(t)+ω42u22(t))                    +λ1T((1p)ΛqθqS1(t)βqS1(t)P(t)                    μqS1(t)+rγqR(t))                    +λ2T(pΛq+θqS1(t)βq(1+ωρ(1u1))S2(t)P(t)                    μqS2(t)+(1r)γqR(t))                    +λ3T(βqS1(t)P(t)+βq(1+ωρ(1u1))S2(t)P(t)                    (ϕq+αq+μq)I(t))                    +λ4T(ϕqI(t)(γq+μq)R(t))                    +λ5T(ξqI(t)ηq(1+u2)P(t)),    (3.3)

where λi(t)s denote the adjoint variables associated with their corresponding states. The first part of the Hamiltonian H is related to the integrand in (3.1) and its second part is constructed by multiplying each adjoint function λi(t)s with the corresponding right-hand side of the model (3.2). Then, Pontryagin's maximum principle leads to the following optimality system.

Theorem 3.1. Given an optimal control u*(t)=(u1*(t),u2*(t))Uad and the state solution X*(t)=(S1*(t),S1*(t),I*(t),R*(t),P*(t)) corresponding to (3.2) that minimize J(u1, u2) in (3.1), there exists adjoint variable P(t)=(λ1(t),λ2(t),λ3(t),λ4(t),λ5(t)) satisfying

 tRDtfqλ1(t)=(θq+βqP(t)+μq)λ1(t)+rγqλ4(t)βqX1λ5(t),    (3.4a)
 tRDtfαλ2(t)=θqλ1(t)(βq(1+ωρ(1u1(t))P(t)+μq)λ2(t)                      +(1r)γqλ4(t)βq(1+ωρ(1u1(t)))X2(t)λ5(t),    (3.4b)
 tRDtfαλ3(t)=βqP(t)λ1(t)+βq(1+ωρ(1u1(t)))P(t)λ2(t)                      (ϕq+αq+μq)λ3(t),                      +(βqX1(t)+βq(1+ωρ(1u1(t))X2(t))λ5(t)+ω1,    (3.4c)
 tRDtfαλ4(t)=ϕqλ3(t)(γq+μq)λ4,    (3.4d)
 tRDtfαλ5(t)=ξqλ3(t)ηq(1+u2(t))λ5+ω2,    (3.4e)

with the transversality conditions

λ1(tf)=λ2(tf)=λ4(tf)=0,λ3(tf)=λ5(tf)=1.    (3.5)

Furthermore, the pair of optimal controls is given by

u1*=min(max((λ3-λ2)βq(1+ωρ)X2(t)P(t)ω3,0.05),0.95),    (3.6a)
u2*=min(max(λ5ηP(t)ω4,0),1).    (3.6b)

Proof: The existence of an optimal control u*(t)=(u1*(t),u2*(t)) and the associated state solution X*(t)=(S1*(t),S1*(t),I*(t),R*(t),P*(t)) comes from the convexity of J(u1, u2) with respect to ui's and the Lipschitz continuous constraint [58], Theorem 5. 1. On the other hand, differentiation of Hamiltonian H with respect to the state variable gives the adjoint system (3.4) as

 tRDtfqλ1(t)=HS1,tRDtfqλ2(t)=HS2,tRDtfqλ3(t)=HI,   tRDtfqλ4(t)=HR,tRDtfqλ5(t)=HP,

with λ1(tf) = λ2(tf) = λ4(tf) = 0, λ3(tf) = λ5(tf) = 1 due to the definition of the cost functional. The optimality conditions is obtained by differentiating Hamiltonian H with respect to the control variables u1 and u2 and then we project the resulting equations onto Uad to reach (3.6).

4. Numerical results

In this section, we present some numerical results to test the contribution of optimal control theory. As the optimization algorithm, forward-backward sweep method is applied [59], Chap. 5 [60] and the OCP is discretized with L1-method with Δt = 0.02, which is a variant of implicit Euler method [61]. We solve the OCP for 100 days and we choose ω1 = 100 and ω2 = 1000, since it is more important to reduce the pathogen pollution, which is the main source of infection, than the number of infected individuals. Moreover, we balance the weight constants ω3 and ω4 according to the cost of the corresponding strategy. Here, we assume that the cost of controlling the decay rate of pathogens is higher than the cost of reducing the stress related parameters, since stress acts on a smaller population than pollution (including children). Thus, we fix ω3 < ω4. To guarantee the reduction in I(t) and P(t) at the final time, we add the term I(tf) + P(tf) to the cost functional. On the other hand, to optimize the values of the stress related parameters, we set the bounds for u1(t) as [0.5, 0.95], since neither it is possible to eliminate stress totally nor it is a force acting fully all the time. We set the bounds for u2(t) as [0, 1] to be more strict. We fix the initial subpopulations as S1, 0 = 100, S2, 0 = 250, I0 = 50, R0 = 5, and P0 = 90, which are taken close to the equilibrium components in (Sec.10, [48]), section 10, except for R0. Here, we set up a scenario where the number of susceptible stressed individuals is greater than the susceptible compartment and the number of recovered individuals is quite small, since our goal is to test the strength of optimal control theory. We discuss two different control strategies and both of them have different costs and contribution. In addition to applying them simultaneously, single control will be tested, too.

With the parameters in Table 1, the reproduction number is calculated as


for q ∈ {0.7, 0.8, 0.9, 1}, respectively. As q increases, the disease becomes more endemic. Our goal is to find optimal values of the controls so that R0<1 can be reached.

Before discussing the optimal control strategy, we present the numerical solutions of I(t) and P(t) with u1 = u2 = 0 in Figure 1, which can be called the uncontrolled problem. We observe that I(t) and P(t) increase for q = {0.9, 1}, while they decrease for q = {0.7, 0.8} as time passes. It is quite vital to apply optimal control for q = {0.9, 1} to eliminate the spread of the disease. Here, the order q may represent the severity of pollution. As q increases, the pollution becomes more dominant and it leads to a rapid increase in the number of infected people.


Figure 1. (A,B) I(t) and P(t) with u1(t) = u2(t) = 0.

We start with the single control u1(t) and present the results in Figure 2. We immediately observe that there is not an obvious difference between the results associated with the uncontrolled problem and the current case. Therefore, trying to decrease the stress related parameters is not a successful action to reduce the number of infected individuals and pathogen population in size, although we apply the full control for almost 100 days.


Figure 2. (A,B) I(t) and P(t) with single optimal control u1(t) (C).

We proceed with the control u2(t) and the corresponding figures are depicted in Figure 3. The single control u2(t) is more powerful than the control u1(t) due to rapid decrease in both I(t) and P(t). Here, we can catch the impact of the fractional order to the choice of the control strategies. As we increase q, control must acts less. The decay rate of pathogen must be controlled strictly almost until the 60th day for q = 1. Then, as we decrease the order q, the control must be applied more strictly. Thus, q can be associated with awareness or reception toward some policies to eliminate pollution.


Figure 3. (A,B) I(t) and P(t) with single optimal control u2(t) (C).

Now, we proceed with the last case, namely the combination of controls u1(t) and u2(t). From the Figure 4, we observe success of the optimal control. The contribution of u1(t) is almost the same when we compare the numerical solutions in Figures 3, 4. Controlling the stress related parameters has a positive effect on the control of decay rate of pathogen. Due to this contribution, u2(t) acts fully not until the 60th day. Indeed, it starts to decrease earlier with the impact of the control u1(t). Moreover, for the model with a lower order of differentiation, u1(t) and u2(t) must act more strictly.


Figure 4. (A,B) I(t) and P(t) with optimal controls u1(t), u2(t) (C,D).

We revealed the success of the OCP in the figures above. Now, we examine the results in detail and show some values of the FOCP with respect to the order of differentiation in Table 2. We firstly observe that the reduction in the cost functional is the smallest one for u1(t). For the control u2(t) and the combined control, the reduction is almost the same; but, the combined control improves the result a little bit more. For the control u2(t) and the pair of controls, as we increase the order, the value of the cost functional decreases and the reduction increases. We remember that the number of infected individuals and the pathogen population decrease in size for q∈{0.7, 0.8} as t approaches 100 days in case of no controls (see Figure 2). Despite of this decrease, the optimal control theory is more powerful for higher values of the fractional order.


Table 2. Values of the cost functional J and reduction in J.

5. Summary and conclusion

We extend a non-integer order model for waterborne diseases motivated by the recent work [48]. The solution is proven to be bounded. On the other hand, we find the reproduction number R0 and we show that the DFE point is locally asymptotically stable if R0<1. Then, we construct an OCP to minimize the number of infected individuals and the pathogen pollution where the controls are used to optimize the stress related parameters and the decay rate of pathogen. We observe that optimizing only stress related parameters is not a successful strategy. Indeed, the value of the decay rate of pathogen is more critical to achieve the goal of this study. For the combined control, the best results are achieved; but, it is not more different than the ones obtained with the control u2(t). Therefore, we deduce that more attention must be paid to control the decay rate of pathogen within a polluted habitat and optimizing the values of the stress related parameters can be a supportive strategy. In addition, we note that as the order q is increased, the disease becomes more endemic. Here, the order q may represent the severity of pollution. As q increases, the pollution affects the population worse and it leads to a rapid increase in the number of infected people. On the other hand, control acts fully for shorter time as we increase q. Thus, q can be associated with awareness or reception toward some policies to eliminate pollution. As a future work, comparison of our numerical results with the field data (if available) can be mentioned. Moreover, the use of other types of fractional derivatives can be investigated for a better data fit and for more accurate control policies.

Data Availability

All datasets generated for this study are included in the manuscript and/or the supplementary files.

Author Contributions

The author confirms being the sole contributor of this work and has approved it for publication.

Conflict of Interest Statement

The author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.


The author is grateful to three referees for their valuable comments and helpful suggestions, which have helped to improve the presentation of this work significantly. Moreover, the author thanks the publisher for the full waiver.


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Keywords: optimal control, waterborne pathogen model, stability, stress, time fractional derivative

2010 Mathematics Subject Classification: 49K99, 34A08, 92B05

Citation: Akman Yıldız T (2019) Optimal Control Problem of a Non-integer Order Waterborne Pathogen Model in Case of Environmental Stressors. Front. Phys. 7:95. doi: 10.3389/fphy.2019.00095

Received: 17 February 2019; Accepted: 19 June 2019;
Published: 05 July 2019.

Edited by:

Amar Debbouche, 8 May 1945 University of Guelma, Algeria

Reviewed by:

Yilun Shang, Northumbria University, United Kingdom
HongGuang Sun, Hohai University, China
JinRong Wang, Guizhou University, China

Copyright © 2019 Akman Yıldız. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Tuğba Akman Yıldız,