Research article Special Issues

Analysis and modeling of fractional electro-osmotic ramped flow of chemically reactive and heat absorptive/generative Walters'B fluid with ramped heat and mass transfer rates

  • Received: 19 January 2021 Accepted: 08 March 2021 Published: 30 March 2021
  • MSC : 26A33, 35R11, 76D05

  • In this contemporary era, fractional derivatives are widely used for the development of mathematical models to precisely describe the dynamics of real-world physical processes. In the field of fluid mechanics, analysis of thermal performance and flow behavior of non-Newtonian fluids is a topic of interest for a variety of researchers due to their significant applications in several industries, engineering operations, devices, and thermal equipment. The primary focus of this article is to investigate the effectiveness of jointly imposed time-controlled (ramped) boundary conditions in the electro-osmotic flow of a chemically reactive and radiative Walters' B fluid along with concentration and energy distributions. In Particular, the concept of using piece-wise time-dependent mass, motion, and energy conditions simultaneously for any non-Newtonian fluid is extensively explored in this work. The flow is developed due to the motion of the bounding vertical wall, which is suspended in a porous material subject to heat injection/absorption and uniform magnetic influences. Atangana-Baleanu derivative of order $ \psi $ is incorporated to establish the fractional form of ordinary modeled equations. Laplace transform method is adapted in light of some unit-less quantities to procure the exact solutions of the under observation model. Several graphical delineations are produced to comprehensively analyze the key characteristics of many physical and thermal parameters. To highlight the significance of operating surface conditions, solutions are compared for time-dependent and constant boundary conditions in every graph. Furthermore, the role of the fractional parameter, time-dependent conditions, and different other involved parameters in heat transfer, mass transfer, and flow rates is characterized by determining the expressions for Nusselt and Sherwood number and coefficient of skin friction. The numerical outcomes are organized in several tables to deeply scrutinize the noteworthy variations in the behavior of the aforementioned physical quantities. The graphical study reveals that the parameter $ E_s $ accounting for electro-osmotic effects decelerates the flow of fluid. At the atomic level, such electro-osmotic flows are useful in the separation processes of the liquids. The fractional parameter $ \psi $ attenuates thicknesses of boundary layers for the evolution of time $ t $ but, it exhibits an opposite role for smaller values of $ t $. It is also noted that the direct correspondence between velocity and time at the boundary for time duration $ t < 1 $ plays a supportive part to effectively control the flow. The exercise tolerance level of cardiac patients is anticipated by following a ramped velocity based protocol. The fractional models are more effective than ordinary models for restricting the boundary shear stress. The occurrence of a chemical reaction leads to improving the mass transfer rate. Additionally, augmentation in heat transfer rate due to the ramped heating technique indicates the significance of this technique in cooling processes. The findings of this work are helpful for clear and comprehensive understanding of electro-osmotic flow of Walters' B fluid in a fractional framework together with chemically reacted mass transfer and thermally radiative heat transfer phenomena subject to wall ramping technique.

    Citation: Asifa, Poom Kumam, Talha Anwar, Zahir Shah, Wiboonsak Watthayu. Analysis and modeling of fractional electro-osmotic ramped flow of chemically reactive and heat absorptive/generative Walters'B fluid with ramped heat and mass transfer rates[J]. AIMS Mathematics, 2021, 6(6): 5942-5976. doi: 10.3934/math.2021352

    Related Papers:

  • In this contemporary era, fractional derivatives are widely used for the development of mathematical models to precisely describe the dynamics of real-world physical processes. In the field of fluid mechanics, analysis of thermal performance and flow behavior of non-Newtonian fluids is a topic of interest for a variety of researchers due to their significant applications in several industries, engineering operations, devices, and thermal equipment. The primary focus of this article is to investigate the effectiveness of jointly imposed time-controlled (ramped) boundary conditions in the electro-osmotic flow of a chemically reactive and radiative Walters' B fluid along with concentration and energy distributions. In Particular, the concept of using piece-wise time-dependent mass, motion, and energy conditions simultaneously for any non-Newtonian fluid is extensively explored in this work. The flow is developed due to the motion of the bounding vertical wall, which is suspended in a porous material subject to heat injection/absorption and uniform magnetic influences. Atangana-Baleanu derivative of order $ \psi $ is incorporated to establish the fractional form of ordinary modeled equations. Laplace transform method is adapted in light of some unit-less quantities to procure the exact solutions of the under observation model. Several graphical delineations are produced to comprehensively analyze the key characteristics of many physical and thermal parameters. To highlight the significance of operating surface conditions, solutions are compared for time-dependent and constant boundary conditions in every graph. Furthermore, the role of the fractional parameter, time-dependent conditions, and different other involved parameters in heat transfer, mass transfer, and flow rates is characterized by determining the expressions for Nusselt and Sherwood number and coefficient of skin friction. The numerical outcomes are organized in several tables to deeply scrutinize the noteworthy variations in the behavior of the aforementioned physical quantities. The graphical study reveals that the parameter $ E_s $ accounting for electro-osmotic effects decelerates the flow of fluid. At the atomic level, such electro-osmotic flows are useful in the separation processes of the liquids. The fractional parameter $ \psi $ attenuates thicknesses of boundary layers for the evolution of time $ t $ but, it exhibits an opposite role for smaller values of $ t $. It is also noted that the direct correspondence between velocity and time at the boundary for time duration $ t < 1 $ plays a supportive part to effectively control the flow. The exercise tolerance level of cardiac patients is anticipated by following a ramped velocity based protocol. The fractional models are more effective than ordinary models for restricting the boundary shear stress. The occurrence of a chemical reaction leads to improving the mass transfer rate. Additionally, augmentation in heat transfer rate due to the ramped heating technique indicates the significance of this technique in cooling processes. The findings of this work are helpful for clear and comprehensive understanding of electro-osmotic flow of Walters' B fluid in a fractional framework together with chemically reacted mass transfer and thermally radiative heat transfer phenomena subject to wall ramping technique.



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    [1] F. F. Reuss, Charge-induced flow, Proc. Imp. Soc. Nat. Moscow, 3 (1809), 327–344.
    [2] G. Wiedemann, Ueber die Bewegung von Flüssigkeiten im Kreise der geschlossenen galvanischen Säule, Ann. Phys., 163 (1852), 321–352. doi: 10.1002/andp.18521631102
    [3] M. V. Smoluchowski, Elektrische endosmose und stromungsstrome, Handbuch del Elektrizitat und des Magnetismus, 2 (1921), 366.
    [4] D. H. Gray, Electrochemical hardening of clay soils, Geotechnique, 20 (1970), 81–93. doi: 10.1680/geot.1970.20.1.81
    [5] A. Asadi, B. B. Huat, H. Nahazanan, H. A. Keykhah, Theory of electroosmosis in soil, Int. J. Electrochem. Sci., 8 (2013), 1016–1025.
    [6] V. Chokkalingam, B. Weidenhof, M. Krämer, W. F. Maier, S. Herminghaus, R. Seemann, Optimized droplet-based microfluidics scheme for sol–gel reactions, Lab Chip, 10 (2010), 1700–1705. doi: 10.1039/b926976b
    [7] A. Manz, C. S. Effenhauser, N. Burggraf, D. J. Harrison, K. Seiler, K. Fluri, Electroosmotic pumping and electrophoretic separations for miniaturized chemical analysis systems, J. Micromech. Microeng., 4 (1994), 257. doi: 10.1088/0960-1317/4/4/010
    [8] S. Deng, The parametric study of electroosmotically driven flow of power-law fluid in a cylindrical microcapillary at high zeta potential, Micromachines, 8 (2017), 344. doi: 10.3390/mi8120344
    [9] S. Sarkar, P. M. Raj, S. Chakraborty, P. Dutta, Three-dimensional computational modeling of momentum, heat, and mass transfer in a laser surface alloying process, Numer. Heat Transfer A, 42 (2002), 307–326.
    [10] Y. Hu, C. Werner, D. Li, Electrokinetic transport through rough microchannels, Anal. Chem., 75 (2003), 5747–5758. doi: 10.1021/ac0347157
    [11] G. H. Tang, X. F. Li, Y. L. He, W. Q. Tao, Electroosmotic flow of non-Newtonian fluid in microchannels, J. non-Newton. Fluid Mech., 157 (2009), 133–137.
    [12] Q. Liu, Y. Jian, L. Yang, Alternating current electroosmotic flow of the Jeffreys fluids through a slit microchannel, Phys. Fluids, 23 (2011), 102001. doi: 10.1063/1.3640082
    [13] C. Zhao, E. Zholkovskij, J. H. Masliyah, C. Yang, Analysis of electroosmotic flow of power-law fluids in a slit microchannel, J. Colloid Interf. Sci., 326 (2008), 503–510. doi: 10.1016/j.jcis.2008.06.028
    [14] Q. S. Liu, Y. J. Jian, L. G. Yang, Time periodic electroosmotic flow of the generalized Maxwell fluids between two micro-parallel plates, J non-Newton. Fluid Mech., 166 (2011), 478–486.
    [15] C. Zhao, C. Yang, Joule heating induced heat transfer for electroosmotic flow of power-law fluids in a microcapillary, Int. J. Heat Mass Tran., 55 (2012), 2044–2051. doi: 10.1016/j.ijheatmasstransfer.2011.12.005
    [16] A. Bandopadhyay, D. Tripathi, S. Chakraborty, Electroosmosis-modulated peristaltic transport in microfluidic channels, Phys. Fluids, 28 (2016), 052002. doi: 10.1063/1.4947115
    [17] S. S. Hsieh, H. C. Lin, C. Y. Lin, Electroosmotic flow velocity measurements in a square microchannel, Colloid Polym. Sci., 284 (2006), 1275–1286. doi: 10.1007/s00396-006-1508-5
    [18] S. Hadian, S. Movahed, N. Mokhtarian, Analytical study of temperature distribution of the electroosmotic flow in slit microchannels, World Appl. Sci. J., 17 (2012), 666–671.
    [19] M. Dejam, Derivation of dispersion coefficient in an electro-osmotic flow of a viscoelastic fluid through a porous-walled microchannel, Chem. Eng. Sci., 204 (2019), 298–309. doi: 10.1016/j.ces.2019.04.027
    [20] J. C. Misra, A. Sinha, Electro-osmotic flow and heat transfer of a non-Newtonian fluid in a hydrophobic microchannel with Navier slip, J. Hydrodynam. Ser. B, 27 (2015), 647–657. doi: 10.1016/S1001-6058(15)60527-3
    [21] R. Ponalagusamy, R. Manchi, Particle-fluid two phase modeling of electro-magneto hydrodynamic pulsatile flow of Jeffrey fluid in a constricted tube under periodic body acceleration, Eur. J. Mech. B Fluid., 81 (2020), 76–92. doi: 10.1016/j.euromechflu.2020.01.007
    [22] M. Azari, A. Sadeghi, S. Chakraborty, Electroosmotic flow and heat transfer in a heterogeneous circular microchannel, Appl. Math. Model., 87 (2020), 640–654. doi: 10.1016/j.apm.2020.06.022
    [23] M. Dejam, Hydrodynamic dispersion due to a variety of flow velocity profiles in a porous-walled microfluidic channel, Int. J. Heat Mass Tran., 136 (2019), 87–98. doi: 10.1016/j.ijheatmasstransfer.2019.02.081
    [24] A. J. Moghadam, Heat transfer in electrokinetic micro-pumps under the influence of various oscillatory excitations, Eur. J. Mech. B Fluid., 85 (2020), 158–168.
    [25] T. Alqahtani, S, Mellouli, A. Bamasag, F. Askri, P. E. Phelan, Thermal performance analysis of a metal hydride reactor encircled by a phase change material sandwich bed, Int. J. Hydrog. Energy, 45 (2020), 23076–23092. doi: 10.1016/j.ijhydene.2020.06.126
    [26] U. Khan, A. Zaib, D. Baleanu, M. Sheikholeslami, A. Wakif, Exploration of dual solutions for an enhanced cross liquid flow past a moving wedge under the significant impacts of activation energy and chemical reaction, Heliyon, 6 (2020), e04565. doi: 10.1016/j.heliyon.2020.e04565
    [27] H. R. Kataria, H. R. Patel, Effects of chemical reaction and heat generation/absorption on magnetohydrodynamic (MHD) casson fluid flow over an exponentially accelerated vertical plate embedded in porous medium with ramped wall temperature and ramped surface concentration, Propuls. Power Res., 8 (2019), 35–46. doi: 10.1016/j.jppr.2018.12.001
    [28] J. Zhao, Thermophoresis and Brownian motion effects on natural convection heat and mass transfer of fractional Oldroyd-B nanofluid, Int. J. Fluid Mech. Res., 47 (2020), 357–370. doi: 10.1615/InterJFluidMechRes.2020030598
    [29] P. K. Gaur, R. P. Sharma, A. K. Jha, Transient free convective radiative flow between vertical parallel plates heated/cooled asymmetrically with heat generation and slip condition, Int. J. Appl. Mech. Eng., 23 (2018), 365–384. doi: 10.2478/ijame-2018-0021
    [30] L. Wang, D. W. Sun, Recent developments in numerical modelling of heating and cooling processes in the food industry–a review, Trends Food Sci. Tech., 14 (2003), 408–423. doi: 10.1016/S0924-2244(03)00151-1
    [31] S. Islam, A. Khan, P. Kumam, H. Alrabaiah, Z. Shah, W. Khan, et al., Radiative mixed convection flow of Maxwell nanofluid over a stretching cylinder with Joule heating and heat source/sink effects, Sci. Rep., 10 (2020), 17823. doi: 10.1038/s41598-020-59925-0
    [32] A. Baslem, G. Sowmya, B. J. Gireesha, B. C. Prasannakumara, M. R. Gorji, N. M. Hoang, Analysis of thermal behavior of a porous fin fully wetted with nanofluids: convection and radiation, J. Mol. Liq., 307 (2020), 112920. doi: 10.1016/j.molliq.2020.112920
    [33] T. Hayat, M. W. A. Khan, M. I. Khan, A. Alsaedi, Nonlinear radiative heat flux and heat source/sink on entropy generation minimization rate, Physica B, 538 (2018), 95–103. doi: 10.1016/j.physb.2018.01.054
    [34] C. Sulochana, G. P. Ashwinkumar, N. Sandeep, Effect of frictional heating on mixed convection flow of chemically reacting radiative Casson nanofluid over an inclined porous plate, Alex. Eng. J., 57 (2018), 2573–2584. doi: 10.1016/j.aej.2017.08.006
    [35] K. S. Miller, B. Ross, An introduction to the fractional calculus and fractional differential equations, Wiley, 1993.
    [36] S. Das, T. Das, S. Chakraborty, Analytical solutions for the rate of DNA hybridization in a microchannel in the presence of pressure-driven and electroosmotic flows, Sensors Actuat. B Chem., 114 (2006), 957–963. doi: 10.1016/j.snb.2005.08.012
    [37] S. Das, S. Chakraborty, Transverse electrodes for improved DNA hybridization in microchannels, AIChE J., 53 (2007), 1086–1099.
    [38] D. Kumar, J. Singh, M. A. Qurashi, D. Baleanu, A new fractional SIRS-SI malaria disease model with application of vaccines, antimalarial drugs, and spraying, Adv. Differ. Equ., 2019 (2019), 278. doi: 10.1186/s13662-019-2199-9
    [39] I. Ahmed, I. A. Baba, A. Yusuf, P. Kumam, W. Kumam, Analysis of Caputo fractional-order model for COVID-19 with lockdown, Adv. Differ. Equ., 2020 (2020), 1–14. doi: 10.1186/s13662-019-2438-0
    [40] S. Ullah, M. A. Khan, J. F. G. Aguilar, Mathematical formulation of hepatitis B virus with optimal control analysis, Optim. Contr. Appl. Meth., 40 (2019), 529–544. doi: 10.1002/oca.2493
    [41] B. Acay, E. Bas, T. Abdeljawad, Fractional economic models based on market equilibrium in the frame of different type kernels, Chaos Soliton. Fract., 130 (2020), 109438. doi: 10.1016/j.chaos.2019.109438
    [42] A. Kilbas, H. Srivastava, J. Trujillo, Theory and applications of fractional differential equations, Elsevier, 2006.
    [43] I. Podlubny, Fractional differential equations: An introduction to fractional derivatives, fractional differential equations, to methods of their solution and some of their applications, Amsterdam, The Netherlands: Elsevier, 1998.
    [44] M. Caputo, M. Fabrizio, A new definition of fractional derivative without singular kernel, Progr. Fract. Differ. Appl., 1 (2015), 1–13.
    [45] A. Atangana, D. Baleanu, New fractional derivatives with nonlocal and non-singular kernel: Theory and application to heat transfer model, Therm. Sci., 4 (2016), 763–769.
    [46] A. Gemant, XLV. On fractional differentials, The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, 25 (1938), 540–549.
    [47] S. Aman, Q. A. Mdallal, I. Khan, Heat transfer and second order slip effect on MHD flow of fractional Maxwell fluid in a porous medium, J. King Saud Univ. Sci., 32 (2020), 450–458. doi: 10.1016/j.jksus.2018.07.007
    [48] A. Awan, M. D. Hisham, N. Raza, The effect of slip on electro-osmotic flow of a second-grade fluid between two plates with Caputo-Fabrizio time fractional derivatives, Can. J. Phys., 97 (2019), 509–516. doi: 10.1139/cjp-2018-0406
    [49] Y. Jiang, H. Qi, H. Xu, X. Jiang, Transient electroosmotic slip flow of fractional Oldroyd-B fluids, Microfluid. Nanofluid., 21 (2017), 7. doi: 10.1007/s10404-016-1843-x
    [50] M. I. Asjad, M. Aleem, A. Ahmadian, S. Salahshour, M. Ferrara, New trends of fractional modeling and heat and mass transfer investigation of (SWCNTs and MWCNTs)-CMC based nanofluids flow over inclined plate with generalized boundary conditions, Chin. J. Phys., 66 (2020), 497–516. doi: 10.1016/j.cjph.2020.05.026
    [51] C. Bardos, F. Golse, B. Perthame, The Rosseland approximation for the radiative transfer equations, Commun. Pure Appl. Math., 40 (1987), 691–721. doi: 10.1002/cpa.3160400603
    [52] L. M. Ottosen, A. J. Pedersen, I. R. Dalgaard, Salt-related problems in brick masonry and electrokinetic removal of salts, J. Building Appraisal, 3 (2007), 181–194. doi: 10.1057/palgrave.jba.2950074
    [53] S. Chakraborty, Towards a generalized representation of surface effects on pressure-driven liquid flow in microchannels, Appl. Phys. Lett., 90 (2007), 034108. doi: 10.1063/1.2433037
    [54] H. M. Park, W. M. Lee, Effect of viscoelasticity on the flow pattern and the volumetric flow rate in electroosmotic flows through a microchannel, Lab Chip, 8 (2008), 1163–1170. doi: 10.1039/b800185e
    [55] K. R. Rajagopal, M. Ruzicka, A. R. Srinivasa, On the Oberbeck-Boussinesq approximation, Math. Mod. Meth. Appl. Sci., 6 (1996), 1157–1167. doi: 10.1142/S0218202596000481
    [56] I. Khan, F. Ali, N. A. Shah, Interaction of magnetic field with heat and mass transfer in free convection flow of a Walters'-B fluid, Eur. Phys. J. Plus, 131 (2016), 77. doi: 10.1140/epjp/i2016-16077-7
    [57] F. Ali, M. Iftikhar, I. Khan, N. A. Sheikh, Aamina, K. S. Nisar, Time fractional analysis of electro-osmotic flow of Walters's-B fluid with time-dependent temperature and concentration, Alex. Eng. J., 59 (2020), 25–38. doi: 10.1016/j.aej.2019.11.020
    [58] F. Ali, M. Saqib, I. Khan, N. A. Sheikh, Application of Caputo-Fabrizio derivatives to MHD free convection flow of generalized Walters'-B fluid model, Eur. Phys. J. Plus, 131 (2016), 377. doi: 10.1140/epjp/i2016-16377-x
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