Numerical study of transient chemical reactive magnetized Casson fluid flow in the presence of Newtonian heating

IF 3.1 Q1 ENGINEERING, MULTIDISCIPLINARY INTERNATIONAL JOURNAL OF MODELLING AND SIMULATION Pub Date : 2023-09-12 DOI:10.1080/02286203.2023.2249641
Gollapalli Shankar, Siva Reddy Sheri, Sabir Ali Shehzad
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It has been observed that the velocity profiles step up with the increment in various parameters. Comparisons are made with the available results in the open literature. These results are in good agreement with the previously published reports.KEYWORDS: transient flowMHDCasson fluidSoret-Dufour effectsFinite element method Nomenclature τ=ShearStressτ0=CassonyieldStressα∗=Shearrateμβ=PlasticdynamicviscosityNsm−1Py=Yieldstressfluideij= i.jthcomponentofdeformationrateu ′=Velocitythefluidms−1k=ThermalconductivityofthefluidWm−1K−1k∗=Absorptioncoefficientcp=Specificheattransferflow\\breakatconstantpressureJkg−1K−1cs=ConcentrationsusceptibilityF=QuadraticdragcoeficientT ′=FluidtemperatureKT∞′=TemperaturefarawayfromtheplateKC′=Speciesconcentrationmolm−3C∞′=Speciesconcentrationfaraway\\breakfromtheplatemolm−3Q0=Volumetricrateofheat\\breakgenerationorabsorptiong=GravitationalaccelerationB0=MagitudeofmagneticfieldU=Wallvelocityofthefluidms−1hs=Heattransfercoefficientqr′=RadiativeheatfluxD=Massdiffusivitym2s−1DCT=SoretdiffusivityPr=PrandtlnumberGr=ThermalGrashofnumberGm=MassGrashofnumberM=MagneticfieldK=Permeabilityparameterk ′=PermeabilityofporousmediumR=RadiationParameterEc=ViscousdissipationQ=HeatabsorptionSc=Schmidtnumberkr=ChemicalreactioncoefficientKr=ChemicalreactionparameterGreek symbols=ρ=Fluiddensitykgm−3βT=Volumeexpansionfactor\\breakforheattransportationβC=Volumeexpansionfactor\\breakformasstransportationμ=Dynamicviscositykgm−1s−1Cf=Skinfrictionα=Cassonparameterγ=ConjugateparameterΓ=Forchheimernumberω=Frequencyparameterθ=DimensionlesstemperatureC=Dimensionless\\,concentrationσ=Magneticpermeabilityofthefluidv=KinematiccoefficientofviscositySubscripts=w=Wallcondition∞=FreestreamconditionDisclosure statementNo potential conflict of interest was reported by the authors.Additional informationNotes on contributorsGollapalli ShankarMr. Gollapalli Shankar is an Assistant Professor in the Department of Mathematics, B V Raju Institute of Technology, Narsapur, Medak, Hyderabad, Telangana, India. He submitted his Ph.D. in Mathematics from GITAM University, Hyderabad Campus, Hyderabad, India. He has more than 11 years of teaching experience and 4 years of research. His current research studies include Fluid dynamics, Magnetohydrodynamics, Heat and Mass Transfer, and FEM. He has published 3 research papers in National/International journals.Siva Reddy SheriDr. Siva Reddy Sheri is an Associate Professor in the Department of Mathematics, GITAM School of Science, Hyderabad Campus, Hyderabad, Telangana, India. He received his Ph.D. in the Mathematics from Osmania University, Hyderabad, India. He has more than 20 years of experience of teaching and research. His current area of research studies includes Fluid dynamics, Magnetohydrodynamics, Heat and Mass Transfer and FEM. He completed one major Research Project from Univerty Grants Commission (UGC) [F.No:42-22/2013 (SR) letter dated 12-03-2013]. 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Abstract

ABSTRACTThe numerical results of transient magnetohydrodynamic (MHD) Casson fluid flow under Soret-Dufour aspects are illustrated in this research. The governing dimensional equations of considered Casson fluids are first converted into dimensionless partial differential equations (PDEs) by utilizing the proper similar variables. The obtained system is then computed through the finite element method (FEM). The impact of dimensionless parameters is visualized on fluid velocity, skin friction, temperature, Nusselt number, concentration, and Sherwood number through the curves and tables. Both the temperature and velocity are risen against the higher Dufour number. It has been observed that the velocity profiles step up with the increment in various parameters. Comparisons are made with the available results in the open literature. These results are in good agreement with the previously published reports.KEYWORDS: transient flowMHDCasson fluidSoret-Dufour effectsFinite element method Nomenclature τ=ShearStressτ0=CassonyieldStressα∗=Shearrateμβ=PlasticdynamicviscosityNsm−1Py=Yieldstressfluideij= i.jthcomponentofdeformationrateu ′=Velocitythefluidms−1k=ThermalconductivityofthefluidWm−1K−1k∗=Absorptioncoefficientcp=Specificheattransferflow\breakatconstantpressureJkg−1K−1cs=ConcentrationsusceptibilityF=QuadraticdragcoeficientT ′=FluidtemperatureKT∞′=TemperaturefarawayfromtheplateKC′=Speciesconcentrationmolm−3C∞′=Speciesconcentrationfaraway\breakfromtheplatemolm−3Q0=Volumetricrateofheat\breakgenerationorabsorptiong=GravitationalaccelerationB0=MagitudeofmagneticfieldU=Wallvelocityofthefluidms−1hs=Heattransfercoefficientqr′=RadiativeheatfluxD=Massdiffusivitym2s−1DCT=SoretdiffusivityPr=PrandtlnumberGr=ThermalGrashofnumberGm=MassGrashofnumberM=MagneticfieldK=Permeabilityparameterk ′=PermeabilityofporousmediumR=RadiationParameterEc=ViscousdissipationQ=HeatabsorptionSc=Schmidtnumberkr=ChemicalreactioncoefficientKr=ChemicalreactionparameterGreek symbols=ρ=Fluiddensitykgm−3βT=Volumeexpansionfactor\breakforheattransportationβC=Volumeexpansionfactor\breakformasstransportationμ=Dynamicviscositykgm−1s−1Cf=Skinfrictionα=Cassonparameterγ=ConjugateparameterΓ=Forchheimernumberω=Frequencyparameterθ=DimensionlesstemperatureC=Dimensionless\,concentrationσ=Magneticpermeabilityofthefluidv=KinematiccoefficientofviscositySubscripts=w=Wallcondition∞=FreestreamconditionDisclosure statementNo potential conflict of interest was reported by the authors.Additional informationNotes on contributorsGollapalli ShankarMr. Gollapalli Shankar is an Assistant Professor in the Department of Mathematics, B V Raju Institute of Technology, Narsapur, Medak, Hyderabad, Telangana, India. He submitted his Ph.D. in Mathematics from GITAM University, Hyderabad Campus, Hyderabad, India. He has more than 11 years of teaching experience and 4 years of research. His current research studies include Fluid dynamics, Magnetohydrodynamics, Heat and Mass Transfer, and FEM. He has published 3 research papers in National/International journals.Siva Reddy SheriDr. Siva Reddy Sheri is an Associate Professor in the Department of Mathematics, GITAM School of Science, Hyderabad Campus, Hyderabad, Telangana, India. He received his Ph.D. in the Mathematics from Osmania University, Hyderabad, India. He has more than 20 years of experience of teaching and research. His current area of research studies includes Fluid dynamics, Magnetohydrodynamics, Heat and Mass Transfer and FEM. He completed one major Research Project from Univerty Grants Commission (UGC) [F.No:42-22/2013 (SR) letter dated 12-03-2013]. He has published more than 80 research papers in National/International journals.Sabir Ali ShehzadDr. Sabir Ali Shehzad is an Associate Professor at COMSATS University Islamabad, Sahiwal. He received his Ph.D. in the Mathematics from Quaid-i-Azam University, Islamabad. He has more than 12 years of experience of teaching and research. His current area of research studies includes Fluid dynamics, Magnetohydrodynamics, Heat and Mass Transfer.
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牛顿加热作用下瞬态化学反应磁化卡森流体流动的数值研究
摘要本文给出了瞬态磁流体动力学(MHD)卡森流体在Soret-Dufour方面的数值结果。首先利用适当的相似变量将所考虑的卡森流体的控制量纲方程转换为无因次偏微分方程。然后用有限元法对得到的系统进行计算。通过曲线和表格可视化了无量纲参数对流体速度、表面摩擦、温度、努塞尔数、浓度和舍伍德数的影响。温度和速度都随着杜福尔数的升高而升高。观察到,随着各参数的增加,速度分布逐渐增大。与公开文献中的现有结果进行了比较。这些结果与以前发表的报告很好地吻合。关键词:瞬态流动mhdcasson流体soret - dufour效应有限元法术语τ=剪切应力τ0=CassonyieldStressα∗=剪切速率μβ=塑性动态粘度ynsm−1Py=屈服应力fluideij= i.jthcomponentofdeformationrate ' =速度流体- 1k=导热系数wm−1k−1k∗=吸收系数entcp=特定传热flow\breakatconstant tpressurejkg−1k−1cs=浓度敏感性f =二次阻力系数' = FluidtemperatureKT∞' = TemperaturefarawayfromtheplateKC ' = Speciesconcentrationmolm−3 c”∞= Speciesconcentrationfaraway \ breakfromtheplatemolm−3 q0 = Volumetricrateofheat \ breakgenerationorabsorptiong = GravitationalaccelerationB0 = MagitudeofmagneticfieldU = Wallvelocityofthefluidms−1 hs = Heattransfercoefficientqr ' = RadiativeheatfluxD = Massdiffusivitym2s−1 dct = SoretdiffusivityPr = PrandtlnumberGr = ThermalGrashofnumberGm = MassGrashofnumberM = MagneticfieldK = Permeabilityparameterk' = PermeabilityofporousmediumR = RadiationParameterEc = ViscousdissipationQ = HeatabsorptionSc = Schmidtnumberkr = ChemicalreactioncoefficientKr = ChemicalreactionparameterGreek符号=ρ= Fluiddensitykgm−3βT = Volumeexpansionfactor \ breakforheattransportationβC = Volumeexpansionfactor \ breakformasstransportationμ= Dynamicviscositykgm−1−1 cf = Skinfrictionα= Cassonparameterγ= ConjugateparameterΓ= Forchheimernumberω= Frequencyparameterθ= DimensionlesstemperatureC =无量纲\,浓度σ= Magneticpermeabilityofthefluidv = KinematiccoefficientofviscositySubscripts = w = Wallcondition∞= FreestreamconditionDisclosure statementNo潜在的利益冲突是报告的作者。其他资料投稿人备注gollapalli ShankarMr。Gollapalli Shankar是印度特伦甘纳邦海得拉巴纳尔萨普尔的B V Raju理工学院数学系助理教授。他在印度海得拉巴的GITAM大学海得拉巴校区获得数学博士学位。他有超过11年的教学经验和4年的研究经验。他目前的研究方向包括流体力学、磁流体力学、传热传质和有限元。在国内外期刊上发表研究论文3篇。Siva Reddy SheriDr。Siva Reddy Sheri是印度特伦加纳邦海得拉巴海得拉巴校区GITAM科学学院数学系副教授。他获得印度海得拉巴奥斯马尼亚大学数学博士学位。他有20多年的教学和研究经验。他目前的研究领域包括流体动力学、磁流体动力学、传热传质和有限元。他完成了一项由大学教育资助委员会(教资会)资助的主要研究项目[F]。编号:42-22/2013 (SR)函,日期:2013年3月12日)。在国内外期刊上发表研究论文80余篇。Sabir Ali ShehzadDr。Sabir Ali Shehzad是伊斯兰堡COMSATS大学的副教授。他在伊斯兰堡Quaid-i-Azam大学获得数学博士学位。他有超过12年的教学和研究经验。他目前的研究领域包括流体动力学、磁流体动力学、传热传质。
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INTERNATIONAL JOURNAL OF MODELLING AND SIMULATION
INTERNATIONAL JOURNAL OF MODELLING AND SIMULATION Engineering-Industrial and Manufacturing Engineering
CiteScore
6.10
自引率
32.30%
发文量
66
期刊介绍: This journal was first published in 1981 and covers languages, hardware, software, methodology, identification, numerical methods, graphical methods, VLSI, microcomputers in simulation, and applications in all fields. It appears quarterly.
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