Research article Special Issues

Parameter estimation and fractional derivatives of dengue transmission model

  • In this paper, we propose a parameter estimation of dengue fever transmission model using a particle swarm optimization method. This method is applied to estimate the parameters of the host-vector and SIR type dengue transmission models by using cumulative data of dengue patient in East Java province, Indonesia. Based on the parameter values, the basic reproduction number of both models are greater than one and obtained their value for SIR is R0=1.4159 and for vector host is R0=1.1474. We then formulate the models in fractional Atangana-Baleanu derivative that possess the property of nonlocal and nonsingular kernel that has been remained effective to many real-life problems. A numerical procedure for the solution of the model SIR model is shown. Some specific numerical values are considered to obtain the graphical results for both the SIR and Vector Host model. We show that the model vector host provide good results for data fitting than that of the SIR model.

    Citation: Windarto, Muhammad Altaf Khan, Fatmawati. Parameter estimation and fractional derivatives of dengue transmission model[J]. AIMS Mathematics, 2020, 5(3): 2758-2779. doi: 10.3934/math.2020178

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  • In this paper, we propose a parameter estimation of dengue fever transmission model using a particle swarm optimization method. This method is applied to estimate the parameters of the host-vector and SIR type dengue transmission models by using cumulative data of dengue patient in East Java province, Indonesia. Based on the parameter values, the basic reproduction number of both models are greater than one and obtained their value for SIR is R0=1.4159 and for vector host is R0=1.1474. We then formulate the models in fractional Atangana-Baleanu derivative that possess the property of nonlocal and nonsingular kernel that has been remained effective to many real-life problems. A numerical procedure for the solution of the model SIR model is shown. Some specific numerical values are considered to obtain the graphical results for both the SIR and Vector Host model. We show that the model vector host provide good results for data fitting than that of the SIR model.


    In 1965, Zadeh [18] introduced the concept of fuzzy theory, which has since undergone extensive research and various applications, including Choquet integrals of set-valued functions [5,6,20,21,22], fuzzy set-valued measures [9,10,16], fuzzy random variable applications [1,4,17], theory for general quantum systems interacting with linear dissipative systems [3], and more. The relationship between fuzzy theory and probability theory has been a subject of much discussion [1,12,14], as both frameworks aim to capture the concept of uncertainty using membership functions and probability density functions (PDFs) whose values lie within the interval [0, 1].

    Fuzzy theory and probability theory are two distinct mathematical frameworks, each with their own approach to modeling uncertainty. Fuzzy theory represents imprecision and vagueness in human reasoning using fuzzy sets, which assign degrees of membership to elements of a universe of discourse. Probability theory deals with randomness and uncertainty using probability distributions, which assign probabilities to outcomes of a random event. Despite their differences, both frameworks allow the expression of uncertainty using values that lie within the range of [0, 1], and they provide a means for decision-making under uncertainty, incorporating expert knowledge and data.

    Research has explored the relationships between fuzzy theory and probability theory, revealing similarities in terms of mathematical structure and some analytical tools. For instance, fuzzy measures can be viewed as a generalization of probability measures, and Choquet integrals of set-valued functions are analogous to probability integrals. While the majority of fuzzy probability measure theories [7,13,15,19] have traditionally considered probability as the expected value of the membership function of fuzzy events, however, by using fuzzifying a PDF we define the fuzzifying probability of crisp events.

    In this study, we propose the concept of fuzzifying probability for continuous random variables in the context of crisp events, along with its properties and associations with conventional probability theories. Therefore, fuzzy theory can be seen as an extension or generalization of probability theory. The main objective of this study is to introduce fuzzifying probability density functions and to investigate related properties by applying the concepts of fuzzifying probability of crisp events. This approach enables investigation of the ambiguities of the PDF and their impact on probability theories. Relevant definitions in probability theory will be briefly recalled to facilitate this investigation.

    Definition 1.1. [8] Let S be a sample space and X be a real-valued continuous random variable on S. Then, a function fX:SR+ is a PDF of X if it satisfies the following criteria:

    (i) fX(x) is positive everywhere in the support S, i.e., fX(x)>0 for all xS, and

    (ii) SfX(x)dx=1.

    If fX(x) is a PDF of the random variable X, then the probability P that X belongs to an event E is defined as

    P(XE)=EfX(x)dx.

    Definition 1.2. [8] Let A be the σ-algebra of a sample space S. A real-valued function P on A is a probability if P satisfies the following properties:

    (i) P(E)0 for all EA,

    (ii) P(S)=1 and P()=0, and

    (iii) For any sequence of events {E1,E2,} with EiEj=(ij), it holds

    P(n=1En)=n=1P(En).

    We next recall some basic fuzzy theory notions and definitions. Let U and V be two universal sets and g:UV be a crisp function between these sets. Then the fuzzifying function ˜g:UF(V) is a mapping from the same domain to a new range F(V) comprising the family of all fuzzy sets on V. The fuzzy set ˜AF(V) of V can be expressed as

    ˜A={(v,m˜A(v))|vV},

    where m˜A:V[0,1] is a membership function of ˜A (For more details see [2,11]). Recall that a fuzzy set ˜A is said to be normal if there exists v0V such that m˜A(v0)=1.

    Let I([0,1]) be the set of all intervals in [0,1] whose elements are described as

    I([0,1]):={[a,a+]|0aa+1}.

    In particular, we consider a=[a,a] for any a[0,1]. Then the interval operators in I([0,1]) are defined as follows.

    Definition 1.3. [5,6,12] For each ˉa=[a,a+],ˉb=[b,b+]I([0,1]), the arithmetic, comparison, and inclusion operators can be expressed as follows.

    (i) ˉa+ˉb=[a+b,a++b+],

    (ii) kˉa=[ka,ka+] for all k[0,1],

    (iii) ˉaˉb=[ab,a+b+],

    (iv) ˉaˉb=[ab,a+b+],

    (v) ˉaˉb=[ab,a+b+],

    (vi) ˉaˉb if and only if ab and a+b+,

    (vii) ˉa<ˉb if and only if ˉaˉb and ˉaˉb, and

    (viii) ˉaˉb if and only if ba and a+b+.

    Also, algebraic operations of fuzzy sets are defined as follows.

    Definition 1.4. [11] Let X be a nonempty set and ˜A and ˜B be fuzzy sets of X.

    (i) The α-cut ˜Aα of a fuzzy set ˜A is defined as

    ˜Aα={xX|m˜A(x)α}.

    (ii) The algebraic sum ˜A+˜B of two fuzzy sets ˜A and ˜B of X is defined as

    (˜A+˜B)α=˜Aα+˜Bα for all α[0,1],

    provided ˜Aα+˜Bα[0,1].

    (iii) The algebraic product ˜A˜B of two fuzzy sets ˜A and ˜B of X is defined as

    (˜A˜B)α=˜Aα˜Bα for all α[0,1].

    Let A be a measurable subset of U and f be an integrable function on U. If ˜f is a fuzzifying function, then the fuzzifying integral [11] of ˜f over A is defined as

    (F)A˜f(x)dx:={([Afα(x)dx,Af+α(x)dx],α)|α[0,1]}, (1.1)

    where fα and f+α are α-cut functions of ˜f(x), i.e.,

    (˜f(x))α=[fα(x),f+α(x)] for all xA.

    Let S be a sample space with continuous random variable X:SR and F(R+) be the family of all fuzzy sets on [0,). Using the concepts [2] of fuzzifying functions to a PDF fX:S[0,), we define a fuzzifying PDF ˜fX as follows. In order to facilitate theoretical development throughout the remainder of the paper, it is assumed that the fuzzifying PDF ˜fX is integrable for all α-cuts.

    Definition 2.1. Let X be a continuous random variable and fX be a PDF of X. Then we define the fuzzifying PDF ˜fX:SF(R+) by fuzzifying fX that satisfies the following conditions:

    (i) ˜fX(x)>0 for all xS, i.e.,

    m˜fX(x)>0 for all xS,

    where m˜fX(x)>0 means that there exists uR+ such that m˜fX(x)(u)>0.

    (ii) The fuzzifying integration (1.1) of ˜fX satisfies

    (F)S˜fX(x)dx=˜1,

    where ˜1 is a convex fuzzy set [11] of 1 with m˜1(1)=1.

    Note that from (1.1), the fuzzy set ˜1 in Definition 2.1 (ii) has its α-cuts

    (˜1)α={[SfXα(x)dx,Sf+Xα(x)dx] if 0α<1,SfX(x)dx=1 if α=1.

    If ˜fX is a fuzzifying PDF of X, then the fuzzifying probability ˜P that X belongs to some event E is given by the fuzzifying integral of ˜fX over E, i.e.,

    ˜P(XE)=(F)E˜fX(x)dx. (2.1)

    We consider the fuzzifying probability using the concept of fuzzifying functions in a similar way.

    Definition 2.2. Let A be a σ-algebra of a sample space S and P:A[0,1] be a probability. Then the fuzzifying function ˜P:AF([0,1]) is called the fuzzifying probability if the following conditions are satisfied:

    (i) 0˜P(E)1 for each event E of S.

    (ii) ˜P(S)=˜1, where ˜1 is a convex fuzzy set satisfying m˜1(1)=1.

    (iii) For any sequence of events {E1,E2,} with EiEj=(ij), it holds

    ˜P(n=1En)=n=1˜P(En).

    The following theorem follows from Definitions 2.1 and 2.2.

    Theorem 2.3. Let ˜fX be a fuzzifying PDF for a continuous random variable X and ˜P be the fuzzifying probability with the density function ˜fX given by (2.1). Then ˜P is a fuzzifying probability.

    Proof. We need only show that ˜P satisfies the three conditions in Definition 2.2.

    (i) Let E be an element of S. Then from (1.1) and (2.1),

    ˜P(XE)=(F)E˜fX(x)dx={([EfXα(x)dx,Ef+Xα(x)dx],α)|α[0,1]}.

    Since 0EfXα(x)dxEf+Xα(x)dx1 for all α[0,1], it implies 0˜P(XE)1. Thus the first condition holds.

    (ii) Since ˜fX1(x)=fX(x) for all xS, the α-cut of ˜P(XS) at α=1 can be expressed as

    (˜P(XS))1=[SfX1(x)dx,Sf+X1(x)dx]=[SfX(x)dx,SfX(x)dx]=1.

    Hence the second condition is satisfied.

    (iii) Let {E1,E2,} be a sequence of disjoint events. Then

    ˜P(Xn=1En)={([n=1EnfXα(x)dx,n=1Enf+Xα(x)dx],α)|α[0,1]}={([n=1(EnfXα(x)dx,Enf+Xα(x)dx]),α)|α[0,1]}=n=1{([EnfXα(x)dx,Enf+Xα(x)dx],α)|α[0,1]}=n=1˜P(XEn).

    Thus, third condition is satisfied, which completes the proof.

    Remark 2.4. Theorem 2.3 confirms the fuzzifying probability is a fuzzifying probability. Thus, we consider the fuzzifying probability to be ˜P(E)=˜P(XE).

    Recall the negative-scalar product [11]: for kR=(,0) and some interval [a,b] in R=(,) with ab, the product [a,b] by k can be expressed as

    k[a,b]=[kb,ka]. (2.2)

    Consider a fuzzy set ˜P(E) for ES whose α-cuts are defined by

    (˜P(E))α={[Ef+Xα(x)dx,EfXα(x)dx] if 0α<1,EfX(x)dx=P(E) if α=1. (2.3)

    Then the fuzzifying probability establishes the following property.

    Theorem 2.5. Let X be a continuous random variable on a sample space S and ˜P be a fuzzifying probability. Then

    (i) ˜P(Ec)=˜1˜P(E) for ES,

    (ii) ˜P()=0,

    (iii) If E1E2 in S, then ˜P(E1)˜P(E2).

    Proof. We need only show that ˜P satisfies the conditions.

    (i) From (2.2) with Ec=SE,

    ˜P(Ec)=(F)Ec˜fX(x)dx={([EcfXα(x)dx,Ecf+Xα(x)dx],α)|α[0,1]}={([SfXα(x)dxEfXα(x)dx,Sf+Xα(x)dxEf+Xα(x)dx],α)|α[0,1]}={([SfXα(x)dx,Sf+Xα(x)dx][Ef+Xα(x)dx,EfXα(x)dx],α)|α[0,1]}=˜1˜P(E),

    where the fuzzy set ˜P(E) is given by (2.3).

    (ii) The second condition is trivially satisfied by the definition

    ˜P()={([fXα(x)dx,f+Xα(x)dx],α)|α[0,1]}=0.

    (iii) Since E2fXα(x)dxE1fXα(x)dx and E1f+Xα(x)dxE2f+Xα(x)dx for all α[0,1],

    ˜P(E1)={([E1fXα(x)dx,E1f+Xα(x)dx],α)|α[0,1]}{([E2fXα(x)dx,E2f+Xα(x)dx],α)|α[0,1]}=˜P(E2).

    We present an example of the fuzzifying probability obtained from a fuzzifying PDF.

    Example 2.6. Let X be a continuous random variable with PDF fX(x)=3x2,0x1. Then, we consider the fuzzifying PDF ˜fX(x)=˜3x2,0x1 of fX, where a fuzzy set ˜3 of the constant 3 is given by

    m˜3(u)={u2 if 2u3,12u+52 if 3<u5.

    Note that the membership function of the fuzzifying function is given by

    m˜fX(x)(u)=m˜3x2(u)={(u2)x2 if 2u3,(12u+52)x2 if 3<u5.

    From Definition 2.1 (iii), the corresponding fuzzifying probability can be expressed as

    ˜P(0<X<13)=(F)130˜fX(x)dx={([130fXα(x)dx,130f+Xα(x)dx],α)|α[0,1]}, (2.4)

    where

    ˜fXα(x)=[fXα(x),f+Xα(x)]:=[(α+2)x2,(52α)x2] for all α[0,1].

    Thus, from (2.4),

    ˜P(0<X<13)={([130(α+2)x2dx,130(52α)x2dx],α)|α[0,1]}={([α+234,52α34],α)|α[0,1]}, (2.5)

    and hence,

    (˜P(0<X<13))α=[α+234,52α34].

    Therefore, the membership of the fuzzifying probability ˜P for 0<X<13 is given by

    m˜P(0<X<13)(u)={34u2 if 234u133,534u2 if 133u534.

    Note that the probability P over 0<X<13 is given by

    P(0<X<13)=1303x2dx=133.

    Therefore, as observed in the graph of the membership function m˜P(0<X<13) in Figure 2, we see that ˜P(0<X<13) establishes a normal fuzzy set of 133 since m˜P(0<X<13)(133)=1.

    Figure 1.  Membership function of a fuzzy set ˜3.
    Figure 2.  Membership function of fuzzifying probability ˜P(0<X<13).

    We define the fuzzifying expected value of a random variable X with the fuzzifying PDF ˜fX as

    ˜E(X)=(F)x˜fX(x)dx={([xfXα(x)dx,xf+Xα(x)dx],α)|α[0,1]}

    and the fuzzifying expected value for a measurable function g(X) of X for ˜fX as

    ˜E(g(X))=(F)g(x)˜fX(x)dx.

    Thus, we can derive the fuzzifying n-th moment of a random variable as follows.

    Theorem 3.1. Let X be a continuous random variable with PDF fX and μn=E(Xn) be the n-th moment about the origin for X. If ˜fX is a fuzzifying PDF, then ˜E(Xn)=˜μn is a fuzzy set of μn and (˜μn)1=μn for each nN.

    Proof. The definition of ˜E directly provides that

    ˜E(Xn)=(F)xn˜fX(x)dx={([xnfXα(x)dx,xnf+Xα(x)dx],α)|α[0,1]}, (3.1)

    hence ˜E(Xn)=˜μn is a fuzzy set of μn. The α-cut of ˜E(Xn) at α=1 in (3.1) can be expressed as

    (˜E(Xn))1=[xnfX1(x)dx,xnf+X1(x)dx]=[xnfX(x)dx,xnfX(x)dx]=E(Xn), (3.2)

    thus (˜μn)1=μn.

    We now proceed to introduce the concept of the fuzzifying variance of a random variable with a fuzzifying PDF, expressed in terms of the fuzzifying expected value.

    Theorem 3.2. If X is a random variable with a fuzzifying PDF fX and μ=E(X) is the expected value of X, then fuzzifying variance ~Var(X) of X can be expressed as

    ~Var(X)=˜E((Xμ)2)=˜E(X2)2μ˜μ+˜1μ2,

    where ˜μ=˜E(X) and ˜1={([fXα(x)dx,f+Xα(x)dx],α)|α[0,1]}.

    Proof. From the definition of the fuzzifying variance,

    ~Var(X)=˜E((Xμ)2)={([x2fXα(x)dx,x2f+Xα(x)dx],α)|α[0,1]}2μ{([xfXα(x)dx,xf+Xα(x)dx],α)|α[0,1]}+μ2{([fXα(x)dx,f+Xα(x)dx],α)|α[0,1]}=˜E(X2)2μ˜μ+˜1μ2.

    Remark 3.3. Theorem 3.2 shows the fuzzy set

    ˜1={([fXα(x)dx,f+Xα(x)dx],α)|α[0,1]}

    is a generalization of the constant 1. Since fX1=f+X1=fX when α=1, (˜1)1 is a PDF of X, hence

    (˜1)1=[fX1(x)dx,f+X1(x)dx]=[fX(x)dx,fX(x)dx]=fX(x)dx=1.

    We extend Example 2.6 to introduce the concept of fuzzifying expected value and fuzzifying variance, and establish their relationship with the corresponding crisp measures.

    Example 3.4. Consider ˜fX(x)=˜3x2 in Example 2.6. Then, the fuzzifying expected value of X when n=1 in Theorem 3.1 is

    ˜E(X)={([xfXα(x)dx,xf+Xα(x)dx],α)|α[0,1]}, (3.3)

    where ˜fXα(x)=(α+2)x2 and ˜f+Xα(x)=(52α)x2 for all α[0,1].

    Therefore,

    ˜E(X)={([x3(α+2)dx,x3(52α)dx],α)|α[0,1]}={([α+24,52α4],α)|α[0,1]}. (3.4)

    Thus, (˜E(X))α=[α+24,52α4], and hence

    m˜E(X)(u)={4u2 if 12u34,54u2 if 34u54. (3.5)

    Since E(X)=10x3dx=34, ˜E(X) can be represented by a fuzzy set ~34 (see Figure 3).

    Figure 3.  Membership function of fuzzifying expected value ˜E(X).

    We can express ˜E(X2) and E(X2) as

    ˜E(X2)={([x4(α+2)dx,x4(52α)dx],α)|α[0,1]}={([α+25,52α5],α)|α[0,1]}, (3.6)

    hence (˜E(X))α=[α+25,52α5] for all α[0,1] and E(X2)=103x4dx=35. Thus ˜E(X2) comprises a fuzzy set ~35 (Figure 3). From Theorem 3.2,

    ~Var(X)=˜E(X2)2˜μ+˜1μ2,

    where ˜1 satisfies

    ˜1={([10x2(α+2)dx,10x2(52α)dx],α)|α[0,1]}={([α+23,52α3],α)|α[0,1]},

    and hence the membership function of ˜1 is

    m˜1(u)={3u2 if 23u1,53u2 if 1u53.

    From (2.2),

    (~Var(X))α=(˜E(X2))α2μ(˜μ)α+μ2(˜1)α=[α+280,52α80]

    for each α[0,1]. Thus, the fuzzifying variance ~Var(X) is

    ~Var(X)={([α+280,52α80],α)|α[0,1]},

    and the membership function of the fuzzifying variance is

    m~Var(X)(u)={80u2 if 140u380,580u2 if 380u580.

    Since Var(X)=E(X2)(E(X))2=35(34)2=380, ~Var(X) is a fuzzy set of 380 (see Figure 4).

    Figure 4.  Membership function of fuzzifying variance ~Var(X).

    In conclusion, the expression for the linearity of expectations for a random variable with a fuzzifying PDF is as follows.

    Theorem 3.5. Let gj be integrable functions of a random variable X and kj be positive integers for j=1,2,,m. Then,

    ˜E(mj=1kjgj(X))=mj=1kj˜E(gj(X)).

    Proof. Since gj(X)˜fX(x)=gj(X)[fXα(x),f+Xα(x)]=[gj(X)fXα(x),gj(X)f+Xα(x)] for all x,

    ˜E(mj=1kjgj(X))=(F)mj=1kjgj(X)˜fX(x)dx={([mj=1kjgj(X)fXα(x)dx,mj=1kjgj(X)f+Xα(x)dx],α)|α[0,1]}={([mj=1kjgj(X)fXα(x)dx,mj=1kjgj(X)f+Xα(x)dx],α)|α[0,1]}={mj=1kj([gj(X)fXα(x)dx,gj(X)f+Xα(x)dx],α)|α[0,1]}=mj=1kj((F)gj(X)˜fX(x)dx),

    which confirms linearity of fuzzifying expectations ˜E(gj(X)).

    In this study, the concept of fuzzifying functions has been introduced to probability theory as a means of developing a fuzzifying PDF and a fuzzifying probability. Through this approach, we aim to investigate the ambiguities inherent in probability theories that are affected by uncertainties in the PDF. The validity of the fuzzifying probability was established through Theorem 2.3, while Theorems 3.1 and 3.2 provided the fuzzifying n-th moment about the origin of a random variable and the fuzzifying variance, respectively. To demonstrate the utility of our approach, we presented modeled examples in which the fuzzifying functions were shown to generalize crisp functions in probability theory. Examples 2.6 and 3.4 illustrated the fuzzifying probability and the fuzzifying expected value, respectively. Furthermore, we extended the concept of fuzzifying functions to Bernoulli, Poisson, and geometric random variables, among others, thus enabling us to investigate the uncertainties in probability theories arising from the ambiguities in PDFs. In summary, our approach of employing fuzzifying functions allows for the investigation of the impact of uncertainties in PDFs on probability theories, and our findings suggest that the concept of fuzzifying functions has the potential to enhance our understanding of probability theory.

    The authors received no financial support for the research, authorship, and/or publication of this article.

    The authors declare no conflict of interest.



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