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Research article

Limited impact of sulfate-driven chemistry on black carbon aerosol aging in power plant plumes

  • Received: 30 April 2018 Accepted: 18 June 2018 Published: 25 June 2018
  • The aging of refractory black carbon (rBC) aerosol by sulfate-driven chemistry has been constrained in coal-fired power-plant plumes using the NOAA WP-3D research aircraft during the Southern Nexus (SENEX) study, which took place in the Southeastern US in June and July of 2013. A Single Particle Soot Photometer (SP2) determined the microphysical properties of rBC-containing particles including single-particle rBC mass and the presence and amount of internally-mixed non-rBC material, hereafter referred to as “coatings”. Most power-plant influenced air was associated with very slightly increased amounts of non-refractory material, likely sulfate internally mixed with the rBC, however this increase was statistically insignificant even after semi-Lagrangian exposure for up to 5 h. On average, the increase in coating thickness was 2 ± 4 nm for particles containing 3–5 fg rBC. Similarly, the number fraction of rBC-containing particles that could be identified as internally mixed was increased by plume chemistry by only 1.3 ± 1.3%. These direct measurements of microphysical aging of rBC-containing aerosol by power plant emissions constrain the enhancement of sulfate chemistry on both rBC’s column-integrated absorption optical depth, and rBC-containing aerosol’s ability to act as cloud condensation nuclei. Appling Mie and k-Köhler theories to the SP2 observations, permits the resulting effect on rBC ambient light-absorption to be capped at the 2–6% level.

    Citation: Milos Z. Markovic, Anne E. Perring, Ru-Shan Gao, Jin Liao, Andre Welti, Nick L. Wagner, Ilana B. Pollack, Ann M. Middlebrook, Thomas B. Ryerson, Michael K. Trainer, Carsten Warneke, Joost A. de Gouw, David W. Fahey, Philip Stier, Joshua P. Schwarz. Limited impact of sulfate-driven chemistry on black carbon aerosol aging in power plant plumes[J]. AIMS Environmental Science, 2018, 5(3): 195-215. doi: 10.3934/environsci.2018.3.195

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  • The aging of refractory black carbon (rBC) aerosol by sulfate-driven chemistry has been constrained in coal-fired power-plant plumes using the NOAA WP-3D research aircraft during the Southern Nexus (SENEX) study, which took place in the Southeastern US in June and July of 2013. A Single Particle Soot Photometer (SP2) determined the microphysical properties of rBC-containing particles including single-particle rBC mass and the presence and amount of internally-mixed non-rBC material, hereafter referred to as “coatings”. Most power-plant influenced air was associated with very slightly increased amounts of non-refractory material, likely sulfate internally mixed with the rBC, however this increase was statistically insignificant even after semi-Lagrangian exposure for up to 5 h. On average, the increase in coating thickness was 2 ± 4 nm for particles containing 3–5 fg rBC. Similarly, the number fraction of rBC-containing particles that could be identified as internally mixed was increased by plume chemistry by only 1.3 ± 1.3%. These direct measurements of microphysical aging of rBC-containing aerosol by power plant emissions constrain the enhancement of sulfate chemistry on both rBC’s column-integrated absorption optical depth, and rBC-containing aerosol’s ability to act as cloud condensation nuclei. Appling Mie and k-Köhler theories to the SP2 observations, permits the resulting effect on rBC ambient light-absorption to be capped at the 2–6% level.


    As an extension of the current development and generalizations in the field of fractional calculus [1,2,3], the investigation of solution behaviors and qualitative properties of the solution in classical or fractional differential equations has become a matter of intense interest for researchers. This reflects the extent of its uses in several applied and engineering aspects. It draws amazing applications in nonlinear oscillations of seismic tremors, the detection of energy transport rate, and energy generation rate. The importance of fractional equations has been recognized in many physical phenomena, in addition to its importance in the mathematical modeling of diseases and viruses to limit and reduce their spread.

    The relaxation differential equation gives as u(ϰ)+u(ϰ)=f(t);u(0+)=u0, whose solution is

    u(ϰ)=u0exp(ϰ)+ϰ0f(tτ)exp(τ)dτ.

    Some recent contributions to the theory of FDEs can be seen in [4]. In [5], the authors studied the following problem

    Dκ0+u(ϰ)=f(ϰ,u(ϰ)),ϰ(0,1),u(0)=0,

    where 0<κ<1,f:[0,1]×R+R+ is continuous and f(ϰ,) is non-decreasing for ϰ[0,1], by lower and upper (LU) solution method. The existence and uniqueness of solutions of the FDE

    Dκ0+u(ϰ)=f(ϰ,u(ϰ)),(0<κ<1;ϰ>0), (1.1)
    Dκ10+u(0+)=u0, (1.2)

    were obtained in [1,2,6], by using the fixed point theorem (FPT) of Banach.

    In [7], the authors discussed the existence and uniqueness of solutions of the following FDE

    Dκ0+u(ϰ)=f(ϰ,u(ϰ)),ϰ(0,ϰ],ϰ1κu(ϰ)|ϰ=0=u0, (1.3)

    by using the LU solution method and its associated monotone iterative (MI) method. The problem (1.3) with non-monotone term has been studied by Bai et al. [8].

    In [9], a new appraoch of the maximum principle was presented by using the completely monotonicity of the Mittag-Leffler (ML) function.

    On the other hand, there are several definitions and generalizations of the fractional operators (FOs) that contributed a lot to the development of this field. The generalization of RL's FOs based on a local kernel containing a differentiable function was first introduced by Osler [3]. Next, Kilbas et al. [1] dealt with some of the properties of this operator. Then, the interesting properties for this operator have been discussed by Agarwal [10]. Recently, Jarad and Abdeljawad [11] achieved some properties in accordance with the generalized Laplace transform with respect to another function.

    In this regard, most of the results similar to our current work are covered under the generalized FOs of Caputo [12] and Hilfer [13], for instance, see [14,15,16,17,18,19], whereas, very few considered results related to the dependence on generalized RL's definition. The authors in [20,21], investigated the existence and uniqueness of positive solutions of the fractional Cauchy problem in the frame of generalized RL and Caputo, respectively.

    For this end, as an additional contribution and enrichment to this active field, we consider the following linear and nonlinear relaxation equations with non-monotone term under ψ-RL fractional derivatives (ψ -RLFD):

    Dκ;ψ0+u(ϰ)+λDδ;ψ0+u(ϰ)=f(ϰ),ϰ(0,h], (1.4)
    (ψ(ϰ)ψ(0))1κu(ϰ)|ϰ=0=u00, (1.5)

    where 0<h<+, 0<κ,δ<1,λ0,fC([0,h],R) and

    Dκ;ψ0+u(ϰ)+λu(ϰ)=f(ϰ,u(ϰ)),ϰ(0,h], (1.6)
    (ψ(ϰ)ψ(0))1κu(ϰ)|ϰ=0=u00, (1.7)

    where fC([0,h]×R, R), Dκ;ψ0+and Dδ;ψ0+ are RL fractional derivatives of order κ and δ, respectively, with respect to another function ψC1([0,h],R), which is increasing, and ψ(ϰ)0 for all [0,h]. The main contributions of this work stand out as follows:

    i) With a new version of Laplace transform, we obtain Hyers-Ulam (HU) and generalized Hyers-Ulam (GHU) stabilities on the finite time interval to check whether the approximate solution is near the exact solution for a ψ-RL linear FDEs (1.4) and (1.5).

    ii) We establish a condition to derive the existence and uniqueness of solutions for ψ-RL nonlinear FDEs (1.6) and (1.7), by using LU solution method along with the Banach contraction map (this generalizes the results in [7]).

    iii) We formulate a new condition on the nonlinear term to ensure the equivalence between the solution of the proposed problem and the corresponding fixed point. Then in light of that, we discuss the maximal and minimal solutions for (1.6) and (1.7).

    Remark 1.1.

    (1) Our results remain valid if λ=0 on problems (1.4)–(1.7), which reduce to

    Dκ;ψ0+u(ϰ)=f(ϰ),ϰ(0,h], (1.8)
    (ψ(ϰ)ψ(0))1κu(ϰ)|ϰ=0=u00. (1.9)

    and

    Dκ;ψ0+u(ϰ)=f(ϰ,u(ϰ)),ϰ(0,h], (1.10)
    (ψ(ϰ)ψ(0))1κu(ϰ)|ϰ=0=u00, (1.11)

    (2) If ψ(ϰ)=ϰ, the problems (1.10) and (1.11) reduces to problem (1.3) considered in [7].

    (3) The linear versions (1.4) and (1.5) generalizes that given in Theorem 5.1 by Jarad et al. [11].

    Observe that in the preceding works, the nonlinear term needs to fulfill the monotone or other control conditions. Indeed, the nonlinear FDE with a non-monotone term can respond better to generic regulation, so it is vital to debilitate the control states of the nonlinear term.

    This work is coordinated as follows. Section 2 provides some consepts of ψ -fractional calculus. Section 3 studies the stability results for the ψ -RL linear FDEs (1.4) and (1.5). In Section 4, we investigate of the the existence and uniqueness results for the ψ-RL nonlinear FDEs (1.6) and (1.7). Moreover, the existence of maximal and minimal solutions is also obtaind. At the end, we provide some examples in the last section.

    Given 0a<b<+ and s>0, and let ψs(ϰ,a):=(ψ(ϰ)ψ(a))s. Define a set

    Cs;ψ[a,b]={u:uC(a,b], ψs(ϰ,a)u(ϰ)C[a,b]}.

    Clearly, Cs;ψ[a,b] is a Banach space with the norm

    uCs;ψ= ψs(ϰ,a)u(ϰ)C=maxϰ[a,b] ψs(ϰ,a)|u(ϰ)|.

    Definition 2.1. [1] Let θ>0, and f:[a,b]R be an integrable function. Then the generalized RL fractional integral and derivative with respect to ψ is given by

    Iκ;ψa+f(ϰ)=1Γ(κ)ϰaψ(ζ)ψκ1(ϰ,s)f(ζ)dζ,

    and

    Dκ;ψa+f(ϰ)=[1ψ(ϰ)ddϰ]nInκ;ψa+f(ϰ),

    respectively, where n=[κ]+1, and ψ:[a,b]R is an increasing with ψ(ϰ)0, for all t[a,b].

    Lemma 2.1. ([11], Theorem 5.1) Let 0<κ<1,λR is a constant, and ϕL(0,h). Then the linear version

    {Dκ;ψa+u(ϰ)λu(ϰ)=ϕ(ϰ), ϰ>a,I1κ;ψa+ u(ϰ)|ϰ=a=cR, (2.1)

    has the following solution

    u(ϰ)=c ψκ1(ϰ,a)Eκ,κ(λψκ(ϰ,a))+ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λψκ(ϰ,ζ))ϕ(ζ)dζ.

    Lemma 2.2. [1] For 0<κ1, the ML function Eκ,κ(λ(ψ(ϰ)ψ(0))κ) satisfies

    0Eκ,κ(λ(ψ(ϰ)ψ(0))κ)1Γ(κ),ϰ[0,),λ0.

    Lemma 2.3. (see [11], Lemma 4.2) For Re(s)>|λ|1κδ, we have

    0es[ψ(ϰ)ψ(0)][ψ(ϰ)ψ(0)]β1Eα,β(λ[ψ(ϰ)ψ(0)]α)dϰ=sαβsα+λ.

    Lemma 2.4. [22] Assume that U is an ordered Banach space, u0,v0U, u0v0, D=[u0,v0], Q:DU is an increasing completely continuous map and u0Qu0,v0Qv0. Then, Q has u and v are minimal and maximal fixed point, respectively. If we set

    un=Qun1,vn=Qvn1,n=1,2,,

    then

    u0u1u2unvnv2v1v0,unu,vnv.

    Definition 2.2. We say that v(ϰ)C1κ;ψ[0,h] is a lower solution of (1.6) and (1.7), if it satisfies

    Dκ;ψ0+v(ϰ)+λv(ϰ)f(ϰ,v(ϰ)),ϰ(0,h), (2.2)
    ψ1κ(ϰ,0) v(ϰ)|ϰ=0u0. (2.3)

    Definition 2.3. We say that w(ϰ)C1κ;ψ[0,h] is an upper solution of (1.6) and (1.7), if it satisfies

    Dκ;ψ0+w(ϰ)+λw(ϰ)f(ϰ,w(ϰ)),ϰ(0,h), (2.4)
    ψ1κ(ϰ,0) w(ϰ)|ϰ=0u0. (2.5)

    Theorem 2.4. [11] Let 0<κ<1. Then, the generalized Laplace transform of ψ-RL fractional derivative is given by

    Lψ[Dκ;ψ0+u(ϰ)]=sκLψ[u(ϰ)]I1κ;ψ0+u(ϰ)|ϰ=0,

    where

    Lψ{f(t)}=aes[ψ(t)ψ(a)]ψ(t)f(t)dt.

    Here, we discuss the HU and GHU stability of ψ-RL linear problems (1.4) and (1.5), by using the ψ-Laplace transform. Before proceeding to prove the results, we will provide the following auxiliary lemmas:

    Lemma 3.1. Let 0<κ<1, and uC1κ;ψ[0,h]. If

    limϰ0+(ψ(ϰ)ψ(0))1κu(ϰ)=u0,u0R,

    then

    I1κ;ψ0+u(0+):=limϰ0+I1κ;ψ0+u(ϰ)=u0Γ(κ).

    Proof. The proof is obtained by the same technique presented in Lemma 3.2, see [1], taking into account the properties of the ψ function.

    Lemma 3.2. Let 0<κ,δ<1,λ0 is a constant, and f:[0,h]R is a continuous function. Then the linear problems (1.4) and (1.5) has the following solution

    u(ϰ)=[Γ(κ)+λΓ(δ)]u0ψκ1(ϰ,0)Eκδ,κ(λψκδ(ϰ,0))+ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκδ,κ(λψκδ(ϰ,ζ))f(ζ)dζ. (3.1)

    Proof. Taking the generalized Laplace transform of (1.4) as

    Lψ[Dκ;ψ0+u(ϰ)]+λLψ[Dδ;ψ0+u(ϰ)]=Lψ[f(ϰ)].

    Via Theorem 2.4, we have

    sκLψ[u(ϰ)]I1κ;ψ0+u(ϰ)|ϰ=0+λ[sδLψ[u(ϰ)]I1δ;ψ0+u(ϰ)|ϰ=0]=Lψ[f(ϰ)].

    From (1.5) and Lemma 3.1, we have I1κ;ψ0+u(ϰ)|ϰ=0=Γ(κ)u0. It follows that

    sκLψ[u(ϰ)]Γ(κ)u0+λ[sδLψ[u(ϰ)]Γ(δ)u0]=Lψ[f(ϰ)].

    One has,

    Lψ[u(ϰ)]=sδsκδ+λ[[Γ(κ)+λΓ(δ)]u0+Lψ[f(ϰ)]]. (3.2)

    Taking L1ψ to both sides of (3.2), it follow from Lemma 2.3 that

    u(ϰ)=[Γ(κ)+λΓ(δ)]u0ψκ1(ϰ,0)Eκδ,κ(λψκδ(ϰ,0))+ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκδ,κ(λψκδ(ϰ,ζ))f(ζ)dζ,

    which is (3.1).

    Theorem 3.1. Let 0<κ,δ<1, λ0, and f:[0,h]R is a continuous function. If uC1κ;ψ[0,h] satisfies the inequality

    |Dκ;ψ0+u(ϰ)+λDδ;ψ0+u(ϰ)f(ϰ)|ϵ, (3.3)

    for each ϰ(0,h] and ϵ>0, then there exists a solution uaC1κ;ψ[0,h] of (1.4) such that

    |u(ϰ)ua(ϰ)|ψκ(h,0)Γ(κ+1)ϵ.

    Proof. Let

    Υ(ϰ):=Dκ;ψ0+u(ϰ)+λDδ;ψ0+u(ϰ)f(ϰ),ϰ(0,h]. (3.4)

    As per (3.3), |Υ(ϰ)|ϵ. Taking the ψ-Laplace transform of (3.4) via Theorem 2.4, we have

    Lψ[Υ(ϰ)]=Lψ[Dκ;ψ0+u(ϰ)]+λLψ[Dδ;ψ0+u(ϰ)]Lψ[f(ϰ)]=sκLψ[u(ϰ)]I1κ;ψ0+u(ϰ)|ϰ=0+λ[sδLψ[u(ϰ)]I1δ;ψ0+u(ϰ)|ϰ=0]Lψ[f(ϰ)].

    From (1.5) and Lemma 3.1, I1κ;ψ0+u(ϰ)|ϰ=0=Γ(κ)u0. It follows that

    Lψ[Υ(ϰ)]=sκLψ[u(ϰ)]Γ(κ)u0+λsδLψ[u(ϰ)]λΓ(δ)u0Lψ[f(ϰ)].

    One has,

    Lψ[u(ϰ)]=sδsκδ+λ[[Γ(κ)+λΓ(δ)]u0+Lψ[Υ(ϰ)]+Lψ[f(ϰ)]]. (3.5)

    Set

    ua(ϰ)=[Γ(κ)+λΓ(δ)]u0ψκ1(ϰ,0)Eκδ,κ(λψκδ(ϰ,0))+ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκδ,κ(λψκδ(ϰ,ζ))f(ζ)dζ. (3.6)

    Taking the Laplace transform of (3.6), It follow from Lemma 2.3 that

    Lψ[ua(ϰ)]=sδsκδ+λ[[Γ(κ)+λΓ(δ)]u0+Lψ[f(ϰ)]]. (3.7)

    Note that

    Lψ[Dκ;ψ0+ua(ϰ)]+λLψ[Dδ;ψ0+ua(ϰ)]=Lψ[Υ(ϰ)]+Lψ[f(ϰ)]=sκLψ[ua(ϰ)]Γ(κ)u0+λsδLψ[ua(ϰ)]λΓ(δ)u0=(sκ+λsδ)Lψ[ua(ϰ)](Γ(κ)+λΓ(δ))u0. (3.8)

    Substituting (3.7) into (3.8), we get

    Lψ[Dκ;ψ0+ua(ϰ)]+λLψ[Dδ;ψ0+ua(ϰ)]=Lψ[f(ϰ)],

    which implies that ua(ϰ) is a solution of (1.4) and (1.5) due to Lψ is one-to-one. It follow from (3.5) and (3.7) that

    Lψ[u(ϰ)ua(ϰ)](s)=sδsκδ+λLψ[Υ(ϰ)],

    which implies

    u(ϰ)ua(ϰ)=Lψ{ψκ1(ϰ,0)Eκδ,κ(λψκδ(ϰ,0))}Lψ[Υ(ϰ)]={ψκ1(ϰ,0)Eκδ,κ(λψκδ(ϰ,0))}ψΥ(ϰ).

    Thus, from (Definition 2.6, [21]) and Lemma 2.2, we obtain

    |u(ϰ)ua(ϰ)|=|{ψκ1(ϰ,0)Eκδ,κ(λψκδ(ϰ,0))}ψΥ(ϰ)|ϰ0ψ(ζ)ψκ1(ϰ,ζ)|Eκδ,κ(λψκδ(ϰ,ζ))||Υ(ζ)|dζϵϰ0ψ(ζ)ψκ1(ϰ,ζ)|Eκδ,κ(λψκδ(ϰ,ζ))|dζϵΓ(κ)ϰ0ψ(τ)ψκ1(ϰ,ζ)dζψκ(h,0)Γ(κ+1)ϵ.

    Remark 3.1. If h<, then (1.4) is HU stable with the constant K:=ψκ(h,0)Γ(κ+1).

    Corollary 3.1. On Theorem 3.1, let φ:[0,)[0,) is continuous function. If we set φ(ϵ)=ψκ(h,0)Γ(κ+1)ϵ, which satisfies φ(0)=0, then (1.4) is GHU stable.

    In this section, we prove the existence and uniqueness results for ψ -RL nonlinear FDEs (1.6) and (1.7), by using the LU solution method and the Banach contraction mapping. Moreover, we discuss the maximal and minimal solutions for the problem at hand. The following hypotheses will be used in our forthcoming analysis:

    (A1) There exist constants A,B0 and 0<s11<s2<1/(1κ) such that for ϰ[0,h],

    |f(ϰ,u)f(ϰ,v)|A|uv|s1+B|uv|s2,u,vR. (4.1)

    (A2) f:[0,h]×RR satisfies

    f(ϰ,u)f(ϰ,v)+λ(uv)0,for ˆuvu˜u,

    where λ0 is a constant and ˆu,˜u are lower and upper solutions of problems (1.6) and (1.7) respectively.

    (A3) There exist constant >0 such that

    |f(ϰ,u)f(ϰ,v)||uv|,ϰ[0,h],u,vR.

    Remark 4.1. Suppose that f(ϰ,u)=a(ϰ)g(u) with g is a Hölder continuous and a(ϰ) is bounded, then (4.1) holds.

    Theorem 4.1. Suppose (A1) holds. The function u solves problems (1.6) and (1.7) iff it is a fixed-point of the operator Q:C1κ;ψ[0,h]C1κ;ψ[0,h] defined by

    (Qu)(ϰ)=Γ(κ)u0ψκ1(ϰ,0)Eκ,κ(λψκ(ϰ,0))+ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))f(ζ,u(ζ))dζ. (4.2)

    Proof. At first, we show that the operator Q is well defined. Indeed, for every uC1κ;ψ[0,h] and ϰ>0, the integral

    ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))f(ζ,u(ζ))dζ,

    belongs to C1κ;ψ[0,h], due to

    ψ1κ(ϰ,0)f(ζ,u(ζ))C[0,h], and ψ1κ(ϰ,0)u(ζ)C[0,h],

    bearing in mind that

    Φ(ϰ):=ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))=m=0ψ(ζ)(λ)m ψ(2κ1)(m+1)(ϰ,ζ)Γ(κ(m+1))

    is continuous on [0,h].

    By the condition (4.1), we have

    |f(ϰ,u)|A|u|s1+B|u|s2+C, (4.3)

    where C=maxϰ[0,h]f(ϰ,0).

    By Lemma 2.2, for u(ϰ)C1κ;ψ[0,h], we have

    |ψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))f(ζ,u(ζ))dζ|ψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))|f(ζ,u(ζ))|dζψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))(A|u|s1+B|u|s2+C)dζψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ)){Aψ(κ1)s1(ζ,0)[ψ1κ(ζ,0)|u(ζ)|]s1+Bψ(κ1)s2(ζ,0)[ψ1κ(ζ,0)|u(ζ)|]s2+C}dζA(uC1κ;ψ)s1 ψ1κ(ϰ,0)Γ(κ)ϰ0ψ(ζ)ψκ1(ϰ,ζ)ψ(κ1)s1(ζ,0)dζ+B(uC1κ;ψ)s2 ψ1κ(ϰ,0)Γ(κ)ϰ0ψ(ζ)ψκ1(ϰ,ζ)ψ(κ1)s2(ζ,0)dζ+CΓ(κ+1)ψ1(ϰ,0)A(uC1κ;ψ)s1 Γ((κ1)s1+1)Γ((κ1)s1+κ+1)ψ(κ1)s1+κ+1κ(ϰ,0)+B(uC1κ;ψ)s2 Γ((κ1)s2+1)Γ((κ1)s2+κ+1)ψ(κ1)s2+κ+1κ(ϰ,0)+CΓ(κ+1)ψ1(ϰ,0)Γ[(κ1)s1+1]Aψ(κ1)s1+1(h,0)Γ[(κ1)s1+κ+1](uC1κ;ψ)s1+Γ[(κ1)s2+1]Bψ(κ1)s2+1(h,0)Γ[(κ1)s2+κ+1](uC1κ;ψ)s2+CΓ(κ+1)ψ1(h,0).

    Thus, the integral exists and belongs to C1κ;ψ[0,h].

    The previous inequality and the hypothesis 0<s11<s2<1/(1κ) imply that

    limϰ0+ψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))f(ζ,u(ζ))dζ=0.

    Since limϰ0+Eκ,κ(λψκ(ϰ,0))=Eκ,κ(0)=1/Γ(κ) it follows that

    limϰ0+ψ1κ(ϰ,0)(Qu)(ϰ)=u0.

    .

    The above arguments concerted along with Lemma 2.1 yields that the fixed-point of Q solves (1.6) and (1.7). And the vice versa. The proof is complete.

    Next, we consider the compactness of Cs;ψ[0,h]. Let FCs;ψ[0,h] and X={g(ϰ)=ψs(ϰ,0)h(ϰ)h(ϰ)F}, then XC[0,h]. It is obvious that F is a bounded set of Cs;ψ[0,h] iff X is a bounded set of C[0,h].

    Thus, to prove that FCs;ψ[0,h] is a compact set, it is sufficient to show that XC[0,h] is a bounded and equicontinuous set.

    Theorem 4.2. Let f:[0,h]×RR is a continuous and (A1) holds. Then Q is a completely continuous.

    Proof. Given unuC1κ;ψ[0,h], with the definition of Q and condition (A1), we get

    QunQuC1κ;ψ=ψ1κ(ϰ,0)(QunQu)=max0ϰh|ψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))[f(ζ,un)f(ζ,u)]dζ|1Γ(κ)max0ϰhψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)[A|unu|s1+B|unu|s2]dζ1Γ(κ)[Amax0ϰhψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)ψs1(1κ)(ζ,0) ψs1(1κ)(ζ,0)|unu|s1dζ+Bmax0ϰhψ1κ(ϰ,0)ϰ0ϰ0ψ(ζ)ψκ1(ϰ,ζ)ψs2(1κ)(ζ,0) ψs2(1κ)(ζ,0)|unu|s2dζ]1Γ(κ)[A(unuC1κ;ψ)s1 max0ϰhψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)ψs1(1κ)(ζ,0)dζ+B(unuC1κ;ψ)s2 max0ϰhψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)ψs2(1κ)(ζ,0)dζ]A(unuC1κ;ψ)s1Γ[1s1(1κ)]Γ[1s1(1κ)+κ]ψ1s1(1κ)(h,0)+B(unuC1κ;ψ)s1Γ[1s2(1κ)]Γ[1s2(1κ)+κ] ψ1s2(1κ)(h,0)0,(n).

    Thus, Q is continuous.

    Assume that FC1κ;ψ[0,h] is a bounded set. Theorem 4.1 shows that Q(F)C1κ;ψ[0,h] is bounded.

    Finally, we show the equicontinuity of Q(F). Given ϵ>0, for every uF and ϰ1,ϰ2[0,h],ϰ1ϰ2,

    |[ψ1κ(ϰ,0)(Qu)(ϰ)]ϰ=ϰ2[ψ1κ(ϰ,0)(Qu)(ϰ)]ϰ=ϰ1|[Γ(κ)u0Eκ,κ(λψκ(ϰ,0))]ϰ2ϰ1+[ψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)×Eκ,κ(λψκ(ϰ,ζ))f(ζ,u(ζ))dζ]ϰ2ϰ1[Γ(κ)u0Eκ,κ(λψκ(ϰ,0))]ϰ2ϰ1+ψ1κ(ϰ2,0)Γ(κ)ϰ2ϰ1ψ(ζ)ψκ1(ϰ2,ζ)|f(ζ,u(ζ))|dζ+ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)ϰ10ψ(ζ)[ψκ1(ϰ2,ζ)ψκ1(ϰ1,ζ)]|f(ζ,u(ζ))|dζ:=[Γ(κ)u0Eκ,κ(λψκ(ϰ,0))]ϰ2ϰ1+I1+I2.

    As Eκ,κ(λψκ(ϰ,0)) is uniformly continuous on [0,h]. Thus

    [Γ(κ)u0Eκ,κ(λψκ(ϰ,0))]ϰ2ϰ10; as ϰ2ϰ1,
    I1:=ψ1κ(ϰ2,0)Γ(κ)ϰ2ϰ1ψ(ζ)ψκ1(ϰ2,ζ)|f(ζ,u(ζ))|dζψ1κ(ϰ2,0)Γ(κ)ϰ2ϰ1ψ(ζ)ψκ1(ϰ2,ζ)(A|u|s1+B|u|s2+C)dζp1A(uC1κ;ψ)s1Γ(p1+κ)ψ1κ(ϰ2,0)ψp1(ϰ2,ϰ1)+p2B(uC1κ;ψ)s2Γ(p2+κ)ψ1κ(ϰ2,0)ψp2(ϰ2,ϰ1)+CΓ(κ+1)ψ1(ϰ2,ϰ1)ψ1κ(ϰ2,0)0, as ϰ2ϰ1,

    where p1=(κ1)s1+1 and p2=(κ1)s2+1,

    I2:=ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)ϰ10ψ(ζ)[ψκ1(ϰ2,ζ)ψκ1(ϰ1,ζ)]|f(ζ,u(ζ))|dζψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)ϰ10ψ(ζ)[ψκ1(ϰ2,ζ)ψκ1(ϰ1,ζ)]×(A|u|s1+B|u|s2+C)dζ:=J1+J2+J3J4J5J60,

    where

    J1ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)A(uC1κ;ψ)s1ϰ10ψ(ζ)ψκ1(ϰ2,ζ)ψp1(ζ,0)dζ0
    J2ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)B(uC1κ;ψ)s2ϰ10ψ(ζ)ψκ1(ϰ2,ζ)ψp2(ζ,0)dζ0
    J3ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)Cϰ10ψ(ζ)ψκ1(ϰ2,ζ)dζ0
    J4ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)A(uC1κ;ψ)s1ϰ10ψ(ζ)ψκ1(ϰ1,ζ)ψp1(ζ,0)dζ0
    J5ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)B(uC1κ;ψ)s2ϰ10ψ(ζ)ψκ1(ϰ1,ζ)ψp2(ζ,0)dζ0
    J6ψ1κ(ϰ2,0)ψ1κ(ϰ1,0)Γ(κ)Cϰ10ψ(ζ)ψκ1(ϰ1,ζ)dζ0

    as ϰ2ϰ1 along with the continuity of ψ. To summarise,

    |[ψ1κ(ϰ,0)(Qu)(ϰ)]ϰ=ϰ2[ψ1κ(ϰ,0)(Qu)(ϰ)]ϰ=ϰ1|0, as ϰ2ϰ1.

    Thus, Q(F) is equicontinuous. The proof is complete.

    Theorem 4.3. Let f:[0,h]×RR is a continuous, (A1) and (A2) hold, and v,wC1κ;ψ[0,h] are lower and upper solutions of (1.6) and (1.7), respectively, such that

    v(ϰ)w(ϰ),0ϰh. (4.4)

    Then, the problems (1.6) and (1.7) has x and y as minimal and maximal solution, respectively, such that

    x=limnQnv,y=limnQnw.

    Proof. Obviously, if functions v,w are lower and upper solutions of problems (1.6) and (1.7), then there are vQv, and wQw. Indeed, by the definition of the lower solution, there exist q_(ϰ)0 and ϵ0 such that

    Dκ;ψ0+v(ϰ)+λv(ζ)=f(ϰ,v(ϰ))q_(ϰ),ϰ(0,h),ψ1κ(ϰ,0)v(ϰ)=u0ϵ.

    Using Theorem 4.1 and Lemma 2.2, we obtain

    v(ϰ)=Γ(κ)(u0ϵ)ψκ1(ϰ,0)Eκ,κ(λψκ(ϰ,0))+ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λψκ(ϰ,ζ))[f(ζ,v(ζ))q_(ζ)]dζ(Qv)(ϰ).

    By the definition of the upper solution, there exist ¯q(ϰ)0 such that

    Dκ;ψ0+w(ϰ)+λw(ζ)=f(ϰ,w(ϰ))+¯q(ϰ),ϰ(0,h),ψ1κ(ϰ,0)w(ϰ)=u0+ϵ.

    Similarly, there is wQw.

    By Theorem 4.2, Q:C1κ;ψ[0,h]C1κ;ψ[0,h] is increasing and completely continuous. Setting D:=[v,w], by the use of Lemma 2.4, the existence of x,y is gotten. The proof is complete.

    Theorem 4.4. Let f:[0,h]×RR is a continuous and (A3) hold. Then problems (1.6) and (1.7) has a unique solution ˜u in the sector [v0,w0] on [0,h], provided

    Γ(κ+1)ψκ(h,0)<1, (4.5)

    where v0,w0 are lower and upper solutions, respectively, of (1.6) and (1.7) , and v0(ϰ)w0(ϰ).

    Proof. Let ˜u is a solution of (1.6) and (1.7). Then v0˜uw0. Consider the operator Q:C1κ;ψ[0,h]C1κ;ψ[0,h] defined by (4.2). For any u1,u2C1κ;ψ[0,h], we have

    Qu1Qu2C1κ;ψ=ψ1κ(ϰ,0)(Qu1Qu2)×max0ϰh|ψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)Eκ,κ(λ(ψκ(ϰ,ζ))×[f(ζ,u1)f(ζ,u2)]dζ|1Γ(κ)max0ϰhψ1κ(ϰ,0)ϰ0ψ(ζ)ψκ1(ϰ,ζ)|u1u2|dζmax0ϰhΓ(κ)ϰ0ψ(ζ)ψκ1(ϰ,ζ) u1u2C1κ;ψdζ Γ(κ+1)ψκ(h,0)u1u2C1κ;ψ.

    From (4.5), we obtain

    Qu1Qu2C1κ;ψ<u1u2C1κ;ψ.

    According to Banach's contraction mapping [23], Q has a unique fixed point, which is unique solution.

    In this part, we provide two examples to illustrate main results.

    Example 5.1. Consider the following problem

    Dκ;ψ0+u(ϰ)+110u(ϰ)=1+ϰκΓ(1κ)+sinπϰΓ(1κ)π(|u(ϰ)|0.5+|u(ϰ)|1.5),ψ1κ(ϰ,0)u(ϰ)|ϰ=0=120.

    Here ϰ(0,1], λ=110,Dκ;ψ0+ is the ψ-RL fractional derivative of order 0<κ<1. Obviously,

    f(ϰ,u)=1+ϰκΓ(1κ)+sinπϰΓ(1κ)π(|u|0.5+|u|1.5),

    and for ϰ[0,1],u,˜u[0,), we have

    |f(ϰ,u)f(ϰ,˜u)||sinπϰ|Γ(1κ)π[|u|0.5+|u|1.5|˜u|0.5|˜u|1.5]1Γ(1κ)π[|u|0.5|˜u|0.5+|u|1.5|˜u|1.5]1Γ(1κ)π[|u˜u|0.5+|u˜u|1.5]=A|u˜u|0.5+B|u˜u|1.5,

    for 0<s1=0.5<s2=1.5<1/(1κ)=2, for κ=12, here A=B=1Γ(1κ)π. Moreover, we have

    |f(ϰ,u)||sinπϰ|Γ(1κ)π[|u|0.5+|u|1.5]1Γ(1κ)π[1+|u|0.5+|u|1.5]=A|u|0.5+B|u|1.5+C,

    where C=maxϰ[0,1]f(ϰ,0)=1Γ(1κ)π. Also, for ϰ[0,1],u,˜u[0,], we have

    f(ϰ,u)f(ϰ,˜u)=sinπϰΓ(1κ)π(|u|0.5|˜u|0.5+|u|1.5|˜u|1.5)sinπϰΓ(1κ)π(|u|1.5|˜u|1.5)1Γ(1κ)π|u˜u|,

    where λ=1Γ(1κ)π>0. From the foregoing, we conclude that (A1), (A2) and (4.3) are satisfied. Hence, problem (3.4) has a solution on [0,1].

    Example 5.2. Consider the following problem

    {Dκ;ψ0+u(ϰ)+110u(ϰ)=12ϰ3(ϰu(ϰ))314ϰ4,ψ1κ(ϰ,0)u(ϰ)|ϰ=0=10. (5.1)

    Here ϰ(0,1], λ=110,Dκ;ψ0+ is the ψ-RL fractional derivative of order 0<κ<1. Obviously,

    f(ϰ,u)=12ϰ3(ϰu)314ϰ4,

    and for ϰ[0,1],u,˜u[0,),we have

    |f(ϰ,u)f(ϰ,˜u)|12ϰ3|(ϰu)3(ϰ˜u)3|12ϰ3|(u3˜u3)3ϰ(˜u2u2)+3ϰ2(˜uu)|32ϰ5|u˜u|32|u˜u|=B|u˜u|1.5,

    for s2=1.5<1/(1κ)=2, for κ=12, here A=0,B=32. Take v0(ϰ)=0, w0(ϰ)=ψ2(ϰ,0)=[ψ(ϰ)ψ(0)]2, it is not difficult to verify that v0(ϰ), w0(ϰ) be lower and upper solutions, respectively, of (5.1), and v0(ϰ)w0(ϰ). Then for ϰ[0,1],

    Dκ;ψ0+v0(ϰ)+110v0(ϰ)=012ϰ614ϰ4=f(ϰ,v0(ϰ))Dκ;ψ0+w0(ϰ)+110w0(ϰ)=Dκ;ψ0+[ψ(ϰ)ψ(0)]2+110[ψ(ϰ)ψ(0)]2=Γ(3)Γ(3κ)[ψ(ϰ)ψ(0)]2κ+110[ψ(ϰ)ψ(0)]2=83πϰ32+110ϰ212ϰ6(1ϰ)314ϰ4=f(ϰ,w0(ϰ)),

    where we used ψ(ϰ)=ϰ. In addition, let ϵ>0, q_(ϰ)=ϰ2, and ¯q(ϰ)=ϰ2, and consider

    {Dκ;ψ0+v(ϰ)+110v(ϰ)=12ϰ614ϰ4q_(ϰ),ϰ(0,h),ψ1κ(ϰ,0)v(ϰ)=u0ϵ. (5.2)

    and

    {Dκ;ψ0+w(ϰ)+110w(ϰ)=12ϰ6(1ϰ)314ϰ4+¯q(ϰ),ϰ(0,h),ψ1κ(ϰ,0)w(ϰ)=u0+ϵ. (5.3)

    By Lemma 4.1, we have

    v(ϰ)=Γ(12)(u0ϵ)1ϰEκ,κ(ϰ10)+ϰ01(ϰζ)E12,12((ϰζ10)(ζ62ζ44ζ2)dζ,

    and

    w(ϰ)=Γ(12)(u0+ϵ)1ϰEκ,κ(ϰ10)+ϰ01(ϰζ)E12,12(110(ϰζ)(ζ6(1ζ)32ζ44ζ210)dζ.

    Thus, all assumptions of Theorem 4.2 are fulfilled. As per Theorem 4.3, problem (5.1) has minimal and maximal solutions u[v0,w0], ˜u[v0,w0], which can be obtained by

    u=limn vn,˜u=limnwn, 

    where

    vn(ϰ)=Γ(12)u01ϰE12,12(ϰ10)+ϰ01(ϰζ)E12,12((ϰζ10)(12ζ3(ζvn1(ζ))314ζ4)dζ, n1

    and

    wn(ϰ)=Γ(12)u01ϰE12,12(ϰ10)+ϰ01(ϰζ)E12,12((ϰζ10)(12ζ3(ζwn1(ζ))314ζ4)dζ, n1.

    In the current work, we have investigated two classes of fractional relaxation equations. Our results were based on generalized Laplace transform, fixed point theorem due to lower and upper solutions method, and functional analysis approaches. The psi- RL fractional operator, which is connected with numerous well-known fractional operators, has been used in our study. Ulam-Hyer's stability of solutions for the linear version has been shown by the generalized Laplace transform approach. Then by establishing the method of lower and upper solutions along with Banach's fixed point technique, we have investigated the existence and uniqueness of iterative solutions for the nonlinear version with the non-monotone term f(ϰ,u(ϰ)), which permits the nonlinearity f to manage the condition (A1) to |f(ϰ,u)|A|u|s1+B|u|s2+C. Besides, we have also discussed the maximal and minimal solutions to the nonlinear version. Then, some known results in the literature have been extended. Finally, two examples to illustrate the obtained results have been provided.

    This work was supported by the Deanship of Scientific Research, Vice Presidency for Graduate Studies and Scientific Research, King Faisal University, Saudi Arabia [Grant No. 757].

    No conflicts of interest are related to this work.

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