Integral inequalities play a key role in applied and theoretical mathematics. The purpose of inequalities is to develop mathematical techniques in analysis. The goal of this paper is to develop a fractional integral operator having a non-singular function (generalized multi-index Bessel function) as a kernel and then to obtain some significant inequalities like Hermit Hadamard Mercer inequality, exponentially (s−m)-preinvex inequalities, Pólya-Szegö and Chebyshev type integral inequalities with the newly developed fractional operator. These results describe in general behave and provide the extension of fractional operator theory (FOT) in inequalities.
Citation: Shahid Mubeen, Rana Safdar Ali, Iqra Nayab, Gauhar Rahman, Kottakkaran Sooppy Nisar, Dumitru Baleanu. Some generalized fractional integral inequalities with nonsingular function as a kernel[J]. AIMS Mathematics, 2021, 6(4): 3352-3377. doi: 10.3934/math.2021201
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Abstract
Integral inequalities play a key role in applied and theoretical mathematics. The purpose of inequalities is to develop mathematical techniques in analysis. The goal of this paper is to develop a fractional integral operator having a non-singular function (generalized multi-index Bessel function) as a kernel and then to obtain some significant inequalities like Hermit Hadamard Mercer inequality, exponentially (s−m)-preinvex inequalities, Pólya-Szegö and Chebyshev type integral inequalities with the newly developed fractional operator. These results describe in general behave and provide the extension of fractional operator theory (FOT) in inequalities.
Fluids can be categorized into Newtonian and non-Newtonian categories based on shear stress, according to the rheological behavior presented earlier [1]. The linear relationship between stress and strain identifies the Newtonian type. Physical problems involving Newtonian fluids have piqued the interest of scientists and engineers in recent years [2,3,4,5,6]. Unlike Newtonian fluids, the non-Newtonian fluid's viscosity does not remain constant with the shear rate and can be affected by a variety of factors. Slurries, foams, polymer melts, emulsions, and solutions are examples of non-Newtonian fluids. Non-Newtonian fluids have been extensively researched due of their numerous industrial applications. Furthermore, given the wide range of fluids of interest, heat transfer with non-Newtonian fluids is a vast topic that cannot be treated in its entirety in this study. Paint and adhesives industries, nuclear reactors, cooling systems, and drilling rigs are all examples of non-Newtonian fluid applications. To discover applications in new sectors, non-Newtonian fluid flows need a full investigation in terms of analytical, experimental, and numerical features. A variety of models have been used to explain non-Newtonian fluids in a number of works [7,8,9,10,11,12,13,14,15,16,17,18,19,20]. Non-Newtonian fluids were examined further by Megahed [7] and Ahmed and Iqba [8] for the power-law model; Cortell [9], Midya [10] and Megahed [11] for the viscoelastic model; Ibrahim and Hindebu [12], Bilal and Ashbar [13] and Abbas and Megahed [14] for the Powell-Eyring model; Pramanik [15], Rana et al. [16] and Alali and Megahed [17] for the Casson model; and Hayat et al. [18], Prasad et al. [19] and Megahed [20] for the Maxwell model. It is important to note that this study considers the viscous dissipation phenomenon. Only if the friction increases to the point where the fluid temperature field is noticeably warmed should this phenomenon be taken into account. There is a vast amount of information accessible on the viscous dissipation phenomenon and many fluid flow models [21,22,23].
The Cattaneo-Christov heat transfer model is a modified form of the Fourier law that is used to calculate the characteristics of a heat flux model while considering the relaxation time for heat flux dispersion across the physical model [24]. As a result, several researchers [25,26,27,28,29,30] have conducted more research on this model's most essential characteristics. In many industrial and technical sectors, including natural processes, biomedical engineering, chemical engineering and petroleum engineering, the Cattaneo-Christov heat transfer model makes the heat transfer mechanism and fluid flow in porous media crucially important [31]. So, the cooling process, which is one of the benefits, is one of the most important real life applications of our research, especially in light of the influence of the double diffusive Cattaneo-Christov model on the non-Newtonian Williamson model. Also, this benefit can lower the cost of the finished product and serve as the primary component in preventing product fault. In addition, the novelty of the current work is to examine how Cattaneo-Christov heat mass fluxes affect non-Newtonian dissipative Williamson fluids due to a slippery stretching sheet under the presence of thermal radiation, chemical reactions, and changing thermal characteristics.
2.
Basic governing equations
Consider the flow of a non-Newtonian Williamson fluid with the Cattaneo-Christov phenomenon in two dimensions. It is assumed that the stretched sheet, which is embedded in a porous medium with permeability k, is what causes the fluid to flow. Likewise, it is considered that the fluid concentration along the sheet is Cw and that the sheet at y=0 is heated with temperature Tw. The fluid is flowing in a streamlined pattern, and its viscosity is low but not negligible. The modifying impact appears to be restricted within a narrow layer adjacent to the sheet surface; this is called the boundary layer region. Within such a layer, the fluid velocity rapidly changes from its starting value to its mainstream value. We chose this model because it can accurately describe a large number of non-Newtonian fluids, possibly the majority, over a vast scope of shear rates. The x-axis is chosen parallel to the surface of the sheet in the flow direction, with the origin at the sheet's leading edge, and the y-axis is perpendicular to it (Figure 1). Let T be the Williamson fluid temperature and u and v be the x-axial and perpendicular velocity components, respectively.
Figure 1.
A physical diagram of a boundary layer slip flow system.
The sheet on which the slip velocity phenomenon occurs is supposed to be rough and exposed to thermal radiation with a radiative heat flux of qr. The concept of the slip phenomenon was put forth by Mahmoud [32], who proved that it linearly depends on the shear stress τw at the surface, i.e.,
u−Uw=λ∗τw,
(2.1)
where τw=[μ∂u∂y+μΓ√2(∂u∂y)2]y=0 and Uw is the fluid velocity at the sheet. Also, chemical reactions and the viscous dissipation phenomenon are taken into consideration in this study. Similarly, the temperature Tw and concentration Cw are constant on the sheet. We continue to assume that the Williamson fluid thermal conductivity varies linearly with temperature κ=κ∞(1+εθ)[33], although its viscosity varies nonlinearly with temperature as μ=μ∞e−αθ[33], where μ∞ is the Williamson fluid's viscosity at ambient temperature, α is the viscosity parameter, κ∞ is the liquid thermal conductivity at ambient temperature, and ε is the thermal conductivity parameter. According to the aforementioned hypotheses, the fundamental equations governing the flow are
∇.U_=0,
(2.2)
ρ∞(U_.∇)U_=−∇p+∇.τ+r_,
(2.3)
ρ∞cp(U_.∇)T=−∇.q−∇.qr+Φ,
(2.4)
(U_.∇)C=−∇.j−k1(C−C∞),
(2.5)
where U_=(u,v,0), p is the pressure, r_=−μkU_ is the Darcy impedance for a Williamson fluid, Φ is the function of dissipation, q is the heat flux, and j is the mass flux. Also, the heat flux q and the mass flux j satisfy the following relations, respectively [34]:
q+γ1(U_.∇q−q.∇U_)=−κ∇T,
(2.6)
j+γ2(U_.∇j−j.∇U_)=−D∇C.
(2.7)
Then, using the conventional boundary layer approximation, we can show that the equations below control the flow and heat mass transfer in our physical description [35].
In addition, ρ∞ represents the ambient density, and μ represents the Williamson viscosity. Γ stands for a Williamson time constant, k is the permeability of the porous medium, cp signifies the specific heat at constant pressure, k1 is the reaction rate, D is the diffusion coefficient, γ1 is the time it takes for the heat flux to relax, γ2 is the time it takes for the mass flux to relax, and C∞ is the ambient fluid concentration. Now, we utilize suitable similarity transforms, such as [35]:
The relevant physical boundary conditions are also modified as a result of the invocation of the prior dimensionless transformations as
f=0,f′=1+λ(f″+We2f″2)e−αθ,θ=1,ϕ=1 at η=0,
(2.20)
f′→0,θ→0,ϕ→0 at η→∞.
(2.21)
The dimensionless controlling factors that have emerged are the local Weissenberg number We=Γx√2a3ν∞, the porous parameter Δ=ν∞ak, the radiation parameter R=16σ∗T3∞3k∗κ∞, the slip velocity parameter λ=λ1√aν∞, the thermal Deborah number De1=γ1a, the Eckert number Ec=u2wcp(Tw−T∞), the Deborah number which related to the mass transfer field De2=γ2a, the chemical reaction parameter K=k1a and the Prandtl number Pr=μ∞cpκ∞. It is interesting to see that when We=0, the nature of the non-Newtonian Williamson fluid model transforms into a Newtonian fluid model.
Furthermore, the local Nusselt number Nux, the local Sherwood number Shx, and the drag force coefficient in terms of Cfx are determined by [37]:
Table 1 compares the values of the local skin-friction coefficient (CfxRe12) with those from Andersson's earlier work [38] to validate the current findings acquired by the shooting technique. This comparison is carried out for various slip velocity parameter values. We can confidently state that our results are in good accord with those references based on this comparison. Furthermore, the collected results show that the proposed strategy is both reliable and efficient.
Table 1.
Comparison of CfxRe12 with the results of Andersson [38] when We=α=Δ=0.
The simulation studies of a non-Newtonian Williamson fluid over a stretching surface are presented in this section. The momentum field considers the slip velocity phenomenon, the energy equation includes the viscous dissipation and thermal radiation effects, and the mass transport equation includes the chemical process. Via the shooting approach, the governing equations are numerically solved using supported dimensionless transformation. All the governing physical parameters are utilized in the following ranges: 0.0≤Δ≤0.5,0.0≤α≤0.5, 0.0≤λ≤0.4,0.0≤We≤0.5,0.0≤ε≤0.5,0.0≤De1≤0.4,0.0≤De2≤1.0,0.0≤K≤0.5 and 0.0≤Ec≤0.5. Thus, the values of the parameters with fixed values which are used for graphical display can be chosen as Δ=0.2,We=0.4,Sc=4.0, R=0.5,α=0.2,K=0.2,ε=0.2,λ=0.2,De1=0.2,Pr=7.0,De2=0.2 and Ec=0.2. This section discusses the graphical effects of physical dimensionless amounts on complicated profiles. The effect of porous parameter Δ on the Williamson fluid velocity is tested and introduced by means of Figure 2(a). When we assume Δ=0.0,0.2 and 0.5, both the velocity of the Williamson fluid and the thickness of the boundary layer are dramatically reduced. The porous parameter exhibits this behavior due to its direct presence in the velocity field. Figure 2(b) shows the impact of the porous parameter on both the fluid temperature and the fluid concentration. We discovered that the Williamson fluid temperature θ(η) rises as the porous parameter rises. Likewise, the Williamson fluid concentration ϕ(η) is subject to the same phenomenon. Physically, the porous parameter causes a restriction in the flow of the fluid, which reduces the fluid's velocity and raises the temperature and concentration distributions.
Figure 2.
(a) f′(η) for chosen Δ. (b) θ(η) and ϕ(η) for chosen Δ.
The velocity, temperature and concentration profiles for the viscosity parameter α are shown in Figure 3. It's worth noting that α has a greater impact on velocity profiles than on temperature or concentration profiles. Increases in the viscosity parameter α result in decreases in the velocity profile f′(η) and associated boundary layer thickness, whereas the temperature θ(η) and concentration ϕ(η) fields show the opposite tendency. Physically, a barrier type of force will be produced in the Williamson flow due to the fluid viscosity's reliance on temperature. The fluid velocity can be slowed down by this force. The fluid layers consequently acquire little thermal energy via the same force.
Figure 3.
(a) f′(η) for chosen α. (b) θ(η) and ϕ(η) for chosen α.
Figure 4 shows the velocity, temperature, and concentration for the slip velocity parameter λ. When the slip velocity parameter is increased, both the temperature θ(η) and concentration ϕ(η) profiles increase, and as a result, the thermal boundary layer thickness increases. With the same parameter, however, the reverse tendency is observed for both the velocity distribution f′(η) and the sheet velocity f′(0). In terms of physics, the existence of the slip phenomenon produces a resistance force between the fluid layers, which in turn reduces the fluid's velocity and enhances the fluid temperature.
Figure 4.
(a) f′(η) for chosen λ. (b) θ(η) and ϕ(η) for chosen λ.
The influence of the local Weissenberg number We on Williamson fluid velocity, Williamson fluid temperature, and Williamson fluid concentration is depicted in Figure 5. The graph illustrates that raising the local Weissenberg number We causes temperature and concentration distributions to rise, whereas the same value of We causes fluid velocity to decrease. Physically, a high local Weissenberg number increases the viscous forces that hold the Williamson fluid layers together, which lowers the fluid's velocity and improves the fluid's heat distribution through the boundary layer.
Figure 5.
(a) f′(η) for chosen We. (b) θ(η) and ϕ(η) for chosen We.
The impact of the thermal conductivity parameter ε has been depicted in Figure 6. The larger values of ε correspond to a broader temperature distribution θ(η) and a marginal increase in the concentration field ϕ(η), but an increase in the same parameter results in a slight decrease in the velocity graphs f′(η). Physically, higher values of the thermal conductivity characteristic indicate a fluid's ability to gain higher temperatures, which may cause the fluid's temperature to rise through the thermal layer.
Figure 6.
(a) f′(η) and ϕ(η) for chosen ε. (b) θ(η) for chosen ε.
The effect of the thermal Deborah number De1 on velocity distribution, temperature distribution and concentration distribution is depicted in Figure 7. The Deborah number is a rheological term that describes the fluidity of materials under specified flow circumstances. Low-relaxation-time materials flow freely and exhibit quick stress decay as a result. The fluid motion f′(η) scarcely improves with the bigger De1 parameter, but the concentration profiles ϕ(η) are slightly reduced. Furthermore, extended values of the thermal Deborah number De1 reduce both the thickness of the thermal region and the profiles of temperature θ(η).
Figure 7.
(a) f′(η) and ϕ(η) for chosen De1. (b) θ(η) for chosen De1.
Figure 8 depicts the dimensionless velocity, dimensionless concentration, and thermal profiles for different Eckert number Ec estimates. It is evident that as the Eckert number is increased, the dimensionless velocities f′(η) diminish modestly, while the dimensionless concentration ϕ(η) increases slightly. Furthermore, the increase in Eckert number Ec obviously increases both the temperature profile and the thickness of the thermal region. Physically, the Williamson fluid moves quickly, causing some kinetic energy to be transformed into thermal energy as a result of the viscous dissipation phenomenon. This promotes the fluid distributing heat more through the thermal layer.
Figure 8.
(a) f′(η) and ϕ(η) for chosen Ec. (b) θ(η) for chosen Ec.
Figure 9 shows the effects of the Deborah number De2, which is related to mass transfer, and the chemical reaction parameter K on Williamson fluid concentration. Because both the concentration characteristics ϕ(η) and the concentration boundary thickness of the Williamson fluid decrease when both the chemical reaction parameter and the Deborah number increase, the mass transfer rate increases as well.
Figure 9.
(a) ϕ(η) for chosen De2. (b) ϕ(η) for chosen K.
From an engineering standpoint, we now concentrate on the fluctuations of physical quantities of interest. For all regulating factors of our model, the local skin-friction Cfx(Rex)12, the local Nusselt number NuxRe−12x1+R, and the local Sherwood number ShxRe−12x are introduced in Table 2. Skin friction coefficient values decrease when the viscosity parameter, slip velocity parameter, and local Weissenberg number increase, lowering both the local Nusselt number and the local Sherwood number. The skin friction coefficient and the local Nusselt number, respectively, grow and shrink uniformly with the thermal Deborah number and the Eckert number. Furthermore, increasing the chemical reaction parameter or the Deborah number increases the rate of mass transfer, while increasing the thermal conductivity parameter reduces it significantly.
Table 2.
Values for Cfx(Rex)12, NuxRe−12x1+R and ShxRe−12x for various values of Δ, α, λ,ε,We,De1,Ec,De2 and K with Pr=7.0, Sc=4.0 and R=0.5.
A description of the heat and mass transport features of a viscous non-Newtonian Williamson fluid across a stretching sheet that is embedded in a porous medium was attempted here. Heat and mass transfer in the Williamson fluid in the presence of thermal radiation, slip velocity, variable thermal characteristics, Cattaneo-Christov heat mass fluxes, chemical reaction and viscous dissipation are all investigated in this study. The governing equations have been converted via dimensionless transformations into a set of coupled nonlinear ordinary differential equations, which are then numerically solved using the shooting technique. The following are the major characteristics of the current work.
1) A concentration field grows as the viscosity and slip parameters increase, but as the chemical reactions and Deborah number increase, the concentration field decreases.
2) The Sherwood number decreases as the Eckert number rises, whereas the Deborah number and chemical parameter increase it.
3) The velocity profile is reduced by the viscosity and slip velocity parameters, whereas a minor increase in velocity profile occurs due to the Deborah number being increased.
4) The Deborah number has a lower temperature profile than the thermal conductivity parameter and the Eckert number.
5) The heat transfer rate is reduced by both the thermal conductivity parameter and the viscous dissipation phenomenon.
6) Skin-friction coefficient values increase with the porous parameter, but they decrease with an increase in either the slip velocity or the viscosity parameter.
7) When the local Weissenberg number is higher, both the skin-friction coefficient and the local Nusselt number's magnitude fall.
Acknowledgments
The authors are thankful to the honorable editor and anonymous reviewers for their useful suggestions and comments which improved the quality of this paper.
Conflict of interest
The authors declare that they have no competing interests.
References
[1]
S. M. Aslani, M. R. Delavar, S. M. Vaezpour, Inequalities of Fejer Type Related to Generalized Convex Functions, Int. J. Anal. Appl., 16 (2018), 38–49.
[2]
U. N. Katugampola, New approach to a generalized fractional integral, Appl. Math. Comput., 218 (2011), 860–865.
[3]
Y. Zhang, T. S. Du, H. Wang, Y. J. Shen, A. Kashuri, Extensions of different type parameterized inequalities for generalized (m, h) (m,h)-preinvex mappings via k-fractional integrals, J. Inequalities Appl., 2018 (2018), 1–30. doi: 10.1186/s13660-017-1594-6
[4]
B. Y. Xi, F. Qi, Some integral inequalities of Hermite-Hadamard type for convex functions with applications to means, J. Funct. Spaces Appl., 2012 (2012), 980438.
[5]
A. Kashuri, M. A. Ali, M. Abbas, H. Budak, New inequalities for generalized m-convex functions via generalized fractional integral operators and their applications, Int. J. Nonlinear Anal. Appl., 10 (2019), 275–299.
[6]
M. R. Delavar, M. De La Sen, Some generalizations of Hermiteâ€"Hadamard type inequalities, SpringerPlus, 5 (2016), 1661. doi: 10.1186/s40064-016-3301-3
[7]
T. Du, M. U. Awan, A. Kashuri, S. Zhao, Some k-fractional extensions of the trapezium inequalities through generalized relative semi-(m,h)-preinvexity, Appl. Anal., (2019), 1–21.
[8]
S. Mubeen, S. Iqbal, M. Tomar, On Hermite-Hadamard type inequalities via fractional integrals of a function with respect to another function and k-parameter, J. Inequal. Math. Appl., 1 (2016), 1–9.
[9]
A. Kashuri, R. Liko, Some new hermite-hadamard type inequalities and their applications, Studia Scientiarum Mathematicarum Hungarica, 56 (2019), 103–142. doi: 10.1556/012.2019.56.1.1418
[10]
M. Z. Sarikaya, On the Ostrowski type integral inequality, Acta Math. Univ. Comenianae, 79 (2010), 129–134.
[11]
T. Abdeljawad, On conformable fractional calculus, J. Comput. Appl. Math., 279 (2015), 57–66. doi: 10.1016/j.cam.2014.10.016
[12]
T. Abdeljawad, D. Baleanu, Monotonicity results for fractional difference operators with discrete exponential kernels, Adv. Differ. Equations, 2017 (2017), 78. doi: 10.1186/s13662-017-1126-1
[13]
P. L. Chebyshev, Sur les expressions approximatives des integrales definies par les autres prises entre les m˜Ames limites, In Proc. Math. Soc. Charkov, 2 (1882), 93–98.
[14]
M. A. Khan, N. Mohammad, E. R. Nwaeze, Y. M. Chu, Quantum Hermite-Hadamard inequality by means of a Green function, Adv. Differ. Equations, 2020 (2020), 1–20. doi: 10.1186/s13662-019-2438-0
[15]
S. Khan, M. A. Khan, Y. M. Chu, New converses of Jensen inequality via Green functions with applications, RACSAM, 114 (2020).
[16]
M. Niezgoda, A generalization of Mercer's result on convex functions, Nonlinear Anal.: Theory Methods Appl., 71 (2009), 2771–2779. doi: 10.1016/j.na.2009.01.120
[17]
P. O. Mohammed, T. Abdeljawad, Modification of certain fractional integral inequalities for convex functions, Adv. Differ. Equations, 2020 (2020), 1–22. doi: 10.1186/s13662-019-2438-0
[18]
A. Fernandez, P. Mohammed, Hermite-Hadamard inequalities in fractional calculus defined using Mittag-Leffler kernels, Math. Methods Appl. Sci., 2020 (2020), 1–18.
[19]
P. O. Mohammed, T. Abdeljawad, Integral inequalities for a fractional operator of a function with respect to another function with nonsingular kernel, Adv. Differ. Equations, 2020 (2020), 1–19. doi: 10.1186/s13662-019-2438-0
[20]
P. O. Mohammed, I. Brevik, A new version of the Hermite-Hadamard inequality for Riemann-Liouville fractional integrals, Symmetry, 12 (2020), 610. doi: 10.3390/sym12040610
[21]
E. Set, M. Tomar, M. Z. Sarikaya, On generalized Grüss type inequalities for k-fractional integrals, Appl. Math. Comput., 269 (2015), 29–34.
[22]
K. S. Nisar, G. Rahman, A. Khan, A. Tassaddiq, M. S. Abouzaid, Certain generalized fractional integral inequalities, AIMS Math., 5 (2020), 1588–1602. doi: 10.3934/math.2020108
[23]
F. Jarad, E. Ugurlu, T. Abdeljawad, D. Baleanu, On a new class of fractional operators, Adv. Differ. Equations, 2017 (2017), 247. doi: 10.1186/s13662-017-1306-z
[24]
F. Jarad, T. Abdeljawad, J. Alzabut, Generalized fractional derivatives generated by a class of local proportional derivatives, Eur. Phys. J. Spec. Top., 226 (2017), 3457–3471. doi: 10.1140/epjst/e2018-00021-7
[25]
C. J. Huang, G. Rahman, K. S. Nisar, A. Ghaffar, F. Qi, Some Inequalities of Hermite-Hadamard type for k-fractional conformable integrals, AJMAA, 16 (2019), 1–9.
[26]
F. Qi, G. Rahman, S. M. Hussain, W. S. Du, K. S. Nisar, Some inequalities of Čebyšev type for conformable k-fractional integral operators, Symmetry, 10 (2018), 614. doi: 10.3390/sym10110614
[27]
K. S. Nisar, G. Rahman, K. Mehrez, Chebyshev type inequalities via generalized fractional conformable integrals, J. Inequal. Appl., 2019 (2019), 245. doi: 10.1186/s13660-019-2197-1
[28]
K. S. Niasr, A. Tassadiq, G. Rahman, A. Khan, Some inequalities via fractional conformable integral operators, J. Inequal. Appl., 2019 (2019), 217. doi: 10.1186/s13660-019-2170-z
[29]
G. Rahman, K. S. Nisar, F. Qi, Some new inequalities of the Gruss type for conformable fractional integrals, AIMS Math., 3 (2018), 575–583. doi: 10.3934/Math.2018.4.575
[30]
K. S. Nisar, G. Rahman, A. Khan, Some new inequalities for generalized fractional conformable integral operators, Adv. Differ. Equations, 2019 (2019), 427. doi: 10.1186/s13662-019-2362-3
[31]
G. Rahman, K. S. Nisar, A. Ghaffar, F. Qi, Some inequalities of the Grüss type for conformable k-fractional integral operators, RACSAM, 114 (2020), 9. doi: 10.1007/s13398-019-00731-3
[32]
G. Rahman, Z. Ullah, A. Khan, E. Set, K. S. Nisar, Certain Chebyshev type inequalities involving fractional conformable integral operators, Mathematics, 7 (2019), 364. doi: 10.3390/math7040364
[33]
G. Rahmnan, T. Abdeljawad, F. Jarad, K. S. Nisar, Bounds of Generalized Proportional Fractional Integrals in General Form via Convex Functions and their Applications, Mathematics, 8 (2020), 113. doi: 10.3390/math8010113
[34]
G. Rahman, K. S. Nisar, T. Abdeljawad, S. Ullah, Certain Fractional Proportional Integral Inequalities via Convex Functions, Mathematics, 8 (2020), 222. doi: 10.3390/math8020222
[35]
G. Rahman, T. Abdeljawad, F. Jarad, A. Khan, K. S. Nisar, Certain inequalities via generalized proportional Hadamard fractional integral operators, Adv. Differ. Equations, 2019 (2019), 454. doi: 10.1186/s13662-019-2381-0
[36]
G. Rahman, T. Abdeljawad, A. Khan, K. S. Nisar, Some fractional proportional integral inequalities, J. Inequal. Appl., 2019 (2019), 244. doi: 10.1186/s13660-019-2199-z
[37]
G. Rahman, A. Khan, T. Abdeljawad, K. S. Nisar, The Minkowski inequalities via generalized proportional fractional integral operators, Adv. Differ. Equations, 2019 (2019), 287. doi: 10.1186/s13662-019-2229-7
[38]
G. Rahman, K. S. Nisar, T. Abdeljawad, Certain Hadamard Proportional Fractional Integral Inequalities, Mathematics, 8 (2020), 504. doi: 10.3390/math8040504
[39]
G. Rahman, K. S. Nisar, S. Rashid, T. Abdeljawad, Certain Grüss-type inequalities via tempered fractional integrals concerning another, J. Inequal. Appl., 2020 (2020), 147. doi: 10.1186/s13660-020-02420-x
[40]
G. Rahman, K. S. Nisar, T. Abdeljawad, Tempered Fractional Integral Inequalities for Convex Functions, Mathematics, 8 (2020), 500. doi: 10.3390/math8040500
[41]
Q. Xiaoli, G. Farid, J. Pecaric, S. B. Akbar, Generalized fractional integral inequalities for exponentially (s, m) (s,m)-convex functions, J. Inequalities Appl., 2020 (2020), 1–13. doi: 10.1186/s13660-019-2265-6
[42]
K. S. Nisar, G. Rahman, D. Baleanu, M. Samraiz, S. Iqbal, On the weighted fractional Pólya–Szegö and Chebyshev-types integral inequalities concerning another function, Adv. Differ. Equations, 2020 (2020), 1–18. doi: 10.1186/s13662-019-2438-0
[43]
P. Agarwal, J. E. Restrepo, An extension by means of ω-weighted classes of the generalized Riemann-Liouville k-fractional integral inequalities, J. Math. Inequalities, 14 (2020), 35–46.
[44]
S. Rashid, I. Iscan, D. Baleanu, Y. M. Chu, Generation of new fractional inequalities via n polynomials s-type convexity with applications. Adv. Differ. Equations, 2020 (2020), 1–20.
[45]
M. A. Noor, K. I. Noor, S. Rashid, Some new classes of preinvex functions and inequalities, Mathematics, 7 (2019), 29.
[46]
M. A. Noor, K. I. Noor, New classes of strongly exponentially preinvex functions, AIMS Math., 4 (2019), 1554–1568. doi: 10.3934/math.2019.6.1554
[47]
A. Rehman, G. Farid, S. Bibi, C. Y. Jung, S. M. Kang, k-fractional integral inequalities of Hadamard type for exponentially (s,m)-convex functions, AIMS Math., 6 (2020), 882.
[48]
S. Rashid, M. A. Latif, Z. Hammouch, Y. M. Chu, Fractional integral inequalities for strongly h-preinvex functions for a kth order differentiable functions, Symmetry, 11 (2019), 1448. doi: 10.3390/sym11121448
[49]
M. U. Awan, S. Talib, A. Kashuri, M. A. Noor, K. I. Noor, Y. M. Chu, A new q-integral identity and estimation of its bounds involving generalized exponentially µ-preinvex functions. Adv. Differ. Equations, 2020 (2020), 1–12.
[50]
G. Grüss, Über das Maximum des absoluten Betrages von, Mathematische Zeitschrift, 39 (1935), 215–226. doi: 10.1007/BF01201355
[51]
G. Pólya, G. Szegö, Aufgaben und Lehrsätze aus der Analysis, Julius Springer, 1925.
[52]
S. S. Dragomir, N. T. Diamond, Integral inequalities of Grüss type via Pólya-Szegö and Shisha-Mond results, RGMIA Res. Rep. Collect., 5 (2002).
[53]
J. Hadamard, Étude sur les propriétés des fonctions entiéres et en particulier dune fonction considerée par Riemann, J. de mathématiques pures et appliquées, (1893), 171–216.
[54]
A. M. Mercer, A variant of Jensen's inequality, J. Ineq. Pure Appl. Math., 4 (2003).
[55]
M. U. Awan, M. A. Noor, K. I. Noor, Hermite-Hadamard inequalities for exponentially convex functions, Appl. Math. Inf. Sci., 12 (2018), 405–409. doi: 10.18576/amis/120215
[56]
S. Mititelu, Invex sets, Stud. Cerc. Mat., 46 (1994), 529–532.
[57]
T. Weir, B. Mond, Pre-invex functions in multiple objective optimization, J. Math. Anal. Appl., 136 (1988), 29–38. doi: 10.1016/0022-247X(88)90113-8
[58]
J. Choi, P. Agarwal, A note on fractional integral operator associated with multiindex Mittag-Leffler functions, Filomat, 30 (2016), 1931–1939. doi: 10.2298/FIL1607931C
[59]
T. N. Srivastava, Y. P. Singh, On Maitland's Generalised Bessel Function. Can. Math. Bull., 11 (1968), 739–741.
[60]
H. M. Srivastava, ˇZ. Tomovski, Fractional calculus with an integral operator containing a generalized Mittag -Leffler function in the kernel, Appl. Math. Comput., 211 (2009), 198–210.
[61]
R. S. Ali, S. Mubeen, I. Nayab, S. Araci, G. Rahman, K. S. Nisar, Some Fractional Operators with the Generalized Bessel-Maitland Function, Discrete Dyn. Nat. Soc., 2020 (2020), 1378457.
[62]
T. R. Prabhakar, A singular integral equation with a generalized Mittag Leffler function in the kernel, Yokhama Math. J., 19 (1971), 7–15.
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