化学反应、Soret和Dufour参数对MHD耗散Williamson纳米流体在光滑拉伸片上通过多孔介质的影响

IF 3.1 Q1 ENGINEERING, MULTIDISCIPLINARY INTERNATIONAL JOURNAL OF MODELLING AND SIMULATION Pub Date : 2023-09-26 DOI:10.1080/02286203.2023.2261812
R. Madan Kumar, R. Srinivasa Raju, M. Anil Kumar
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The numerical computations were subsequently illustrated visually to demonstrate the influence of various physical factors on the plots of temperature, velocity, and concentration of the nanofluid. With the use of comparison with previously published data in a restricted sense, the veracity of computation results is evaluated. The tabular values illuminate that the local skin friction coefficient upsurge as the values of the magnetic parameter, porosity parameter, and Brownian motion parameter intensifies, whereas the opposite trend exists for other parameters. The local Nusselt number grows as the Schmidt number rises whereas the reverse trend was experienced for the freed-up parameters.KEYWORDS: Williamson nanofluid flowmagnetohydrodynamics (MHD)porous mediumslippery-stretching sheet Nomenclature C=concentration of the nanoparticles mol/LCw=surface nanoparticles concentration molL−1Kr=chemical reaction constant s−1a=Stretching velocit s−1T∞=free stream temperature KT=temperature of the nanofluidTm=mean nanofluid temperatureC∞=free nanoparticle concentration mol/LB0=Strength of the uniform magnetic field Tg=gravitational acceleration ms−2Dm=coefficient of mass diffusivitDB=Brownian diffusion coefficient m2s−1f=dimensionless stream functionk=permeability of porous medium m2kT=ratio of thermal diffusionk∗=mean absorption coefficient m−1cs=concentration susceptibilitycp=specific heat at constant pressure JKg−1K−1We=local Weissenberg numberPr=Prandtl numberQ0=heat generation (absorption) coefficient JK−1m−3s−1Q=heat generation parameterDu=Dufour (Diffusion- Thermo) parameterS=suction parameterSc=Schmidt numberSr=soret parameterK=porous parameterM=magnetic field parameterCf=skin friction coefficientCw=Surface nanoparticle concentration mol/LT=nanofluid temperature KR=radiation parameterTw=surface temperature KNb=Brownian motion parameter m−1Nt=thermophoresis parameterNux∼=local nusselt numberShux=local Sherwood parameteru=velocity on x-directionv=velocity on y-directionGreek symbols=θ=dimensionless temperaturev=kinematic viscosity m2s−1Γ=Williamson parameter sμ=CoefficientofviscosityKgm(−1s(−1))ρ=densityofthefluidKgm(−3)σ=electricalconductivitySm(−1)σ∗=Stefan−Boltzmannconstant\\breakWm(−2K(−4))κ=thermal conductivity Wm−1K−1ϕ=dimensionlessconcentrationSuperscripts=W=wall condition‘=differentiation with respect to η∞=free stream conditionDisclosure statementNo potential conflict of interest was reported by the author(s).Additional informationFundingThe authors received no financial support for the research, authorship, and publication of this article.Notes on contributorsR. Madan KumarR. Madan Kumar received his post-graduation degree in Pure Mathematics in 2008 and Master of Philosophy in Fluid Dynamics in 2012 from Sri Venkateswara University, Tirupati, Andhra Pradesh, India. He has been working as a Mathematics Mentor from 2008 to till date and worked as an E-Mathematics Content developer (2009 to 2014) at Rajiv Gandhi University of Knowledge Technologies, Idupulapaya, Andhra Pradesh, India. Currently, he is a researcher scholar, working in the area of Fluid Dynamics at GITAM School of Sciences (deemed to be a university), Hyderabad Campus, India. His main interest areas are Newtonian and Non-Newtonian fluids, the applications of nanofluids, Soret and Dufour effects, Heat and Mass Transfer, and Numerical Techniques.R. Srinivasa RajuDr. R. Srinivasa Raju is presently working as an Associate Professor at GITAM School of Science, GITAM (Deemed to be University), Hyderabad Campus, Rudraram, Hyderabad, Telangana state, India. He acquired his Doctorate in Applied Mathematics from Osmania University in 2012, and he also received his Master of Science in Applied Mathematics from Osmania University in 2005. He has over 115 publications in International and National reputed Journals. He also attended and paper presented in various National and International Conferences. He has published a book entitled Finite Element Technique on MHD Fluid Flow Problems by RIGI Publications. He serves as an editorial member for four international journals. He is a member of several National and International Mathematical Societies. He received the Srinivasa Ramanujan Life Time Achievement National Award in the year 2018. He has also received the Prestigious Award for Young Educator and Scholar Award from the National Foundation for Entrepreneurship Development (NFED) in the year 2018. He has produced 4 doctoral candidates. He is currently supervising 10 research scholars.M. Anil KumarDr. M. Anil kumar working as an Associate professor in the Department of Mathematics, at Anurag University. In the year 2020, he obtained his Doctorate from GITAM (Deemed to be University), Visakhapatnam, India, and in 2005, he received his Master of Science in Applied Mathematics from the National Institute of Technology Warangal. Dr. Anil kumar has over 18 years of teaching experience and over 8 years of research experience. He received the Best Teacher award from Anurag University for the academic year 2022-2023. He has 23 publications to his credit in reputed national and international journals. He received a SEED money project from Anurag University of Rs 2 lakhs for the Academic year 2021-22. He received the patent right in Micropolar fluids from Intellectual Property of India in 2022. He also presented papers at various National and International conferences. He is a member of several National and International Mathematical Societies. 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Under the influence of both magnetic field and thermal radiation, the significance of viscous dissipation and velocity slip boundary condition with heat generation have been explored. Similarity components were used to turn the nonlinear Partial Differential Equations (PDEs) into nonlinear Ordinary Differential Equations (ODEs), and they were solved using the fourth-order approach of the Runge–Kutta (R–K) method along with the shooting technique. The numerical computations were subsequently illustrated visually to demonstrate the influence of various physical factors on the plots of temperature, velocity, and concentration of the nanofluid. With the use of comparison with previously published data in a restricted sense, the veracity of computation results is evaluated. The tabular values illuminate that the local skin friction coefficient upsurge as the values of the magnetic parameter, porosity parameter, and Brownian motion parameter intensifies, whereas the opposite trend exists for other parameters. The local Nusselt number grows as the Schmidt number rises whereas the reverse trend was experienced for the freed-up parameters.KEYWORDS: Williamson nanofluid flowmagnetohydrodynamics (MHD)porous mediumslippery-stretching sheet Nomenclature C=concentration of the nanoparticles mol/LCw=surface nanoparticles concentration molL−1Kr=chemical reaction constant s−1a=Stretching velocit s−1T∞=free stream temperature KT=temperature of the nanofluidTm=mean nanofluid temperatureC∞=free nanoparticle concentration mol/LB0=Strength of the uniform magnetic field Tg=gravitational acceleration ms−2Dm=coefficient of mass diffusivitDB=Brownian diffusion coefficient m2s−1f=dimensionless stream functionk=permeability of porous medium m2kT=ratio of thermal diffusionk∗=mean absorption coefficient m−1cs=concentration susceptibilitycp=specific heat at constant pressure JKg−1K−1We=local Weissenberg numberPr=Prandtl numberQ0=heat generation (absorption) coefficient JK−1m−3s−1Q=heat generation parameterDu=Dufour (Diffusion- Thermo) parameterS=suction parameterSc=Schmidt numberSr=soret parameterK=porous parameterM=magnetic field parameterCf=skin friction coefficientCw=Surface nanoparticle concentration mol/LT=nanofluid temperature KR=radiation parameterTw=surface temperature KNb=Brownian motion parameter m−1Nt=thermophoresis parameterNux∼=local nusselt numberShux=local Sherwood parameteru=velocity on x-directionv=velocity on y-directionGreek symbols=θ=dimensionless temperaturev=kinematic viscosity m2s−1Γ=Williamson parameter sμ=CoefficientofviscosityKgm(−1s(−1))ρ=densityofthefluidKgm(−3)σ=electricalconductivitySm(−1)σ∗=Stefan−Boltzmannconstant\\\\breakWm(−2K(−4))κ=thermal conductivity Wm−1K−1ϕ=dimensionlessconcentrationSuperscripts=W=wall condition‘=differentiation with respect to η∞=free stream conditionDisclosure statementNo potential conflict of interest was reported by the author(s).Additional informationFundingThe authors received no financial support for the research, authorship, and publication of this article.Notes on contributorsR. Madan KumarR. Madan Kumar received his post-graduation degree in Pure Mathematics in 2008 and Master of Philosophy in Fluid Dynamics in 2012 from Sri Venkateswara University, Tirupati, Andhra Pradesh, India. He has been working as a Mathematics Mentor from 2008 to till date and worked as an E-Mathematics Content developer (2009 to 2014) at Rajiv Gandhi University of Knowledge Technologies, Idupulapaya, Andhra Pradesh, India. Currently, he is a researcher scholar, working in the area of Fluid Dynamics at GITAM School of Sciences (deemed to be a university), Hyderabad Campus, India. His main interest areas are Newtonian and Non-Newtonian fluids, the applications of nanofluids, Soret and Dufour effects, Heat and Mass Transfer, and Numerical Techniques.R. Srinivasa RajuDr. R. Srinivasa Raju is presently working as an Associate Professor at GITAM School of Science, GITAM (Deemed to be University), Hyderabad Campus, Rudraram, Hyderabad, Telangana state, India. He acquired his Doctorate in Applied Mathematics from Osmania University in 2012, and he also received his Master of Science in Applied Mathematics from Osmania University in 2005. He has over 115 publications in International and National reputed Journals. He also attended and paper presented in various National and International Conferences. He has published a book entitled Finite Element Technique on MHD Fluid Flow Problems by RIGI Publications. He serves as an editorial member for four international journals. He is a member of several National and International Mathematical Societies. He received the Srinivasa Ramanujan Life Time Achievement National Award in the year 2018. He has also received the Prestigious Award for Young Educator and Scholar Award from the National Foundation for Entrepreneurship Development (NFED) in the year 2018. He has produced 4 doctoral candidates. He is currently supervising 10 research scholars.M. Anil KumarDr. M. Anil kumar working as an Associate professor in the Department of Mathematics, at Anurag University. In the year 2020, he obtained his Doctorate from GITAM (Deemed to be University), Visakhapatnam, India, and in 2005, he received his Master of Science in Applied Mathematics from the National Institute of Technology Warangal. Dr. Anil kumar has over 18 years of teaching experience and over 8 years of research experience. He received the Best Teacher award from Anurag University for the academic year 2022-2023. He has 23 publications to his credit in reputed national and international journals. He received a SEED money project from Anurag University of Rs 2 lakhs for the Academic year 2021-22. He received the patent right in Micropolar fluids from Intellectual Property of India in 2022. He also presented papers at various National and International conferences. He is a member of several National and International Mathematical Societies. 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引用次数: 0

摘要

摘要本研究的目的是确定Soret, Dufour和化学反应参数对二维MHD Williamson纳米流体在浸入多孔介质中的滑张片上流动的影响。在磁场和热辐射的共同作用下,探讨了粘性耗散和速度滑移边界条件对热生成的意义。利用相似分量将非线性偏微分方程(PDEs)转化为非线性常微分方程(ode),并结合射击技术,采用龙格-库塔法(R-K)进行四阶求解。数值计算结果直观地展示了各种物理因素对纳米流体温度、速度和浓度的影响。通过与已有的有限数据进行比较,对计算结果的准确性进行了评价。由表值可知,局部表面摩擦系数随磁性参数、孔隙度参数和布朗运动参数的增大而增大,而其他参数则相反。局部努塞尔数随着施密特数的增加而增加,而释放参数则相反。关键词:命名法C=纳米颗粒浓度mol/LCw=表面纳米颗粒浓度molL−1Kr=化学反应常数s−1a=拉伸速度s−1T∞=自由流温度KT=纳米流体温度tm =纳米流体平均温度C∞=自由纳米颗粒浓度mol/LB0=均匀磁场强度Tg=重力加速度ms−2Dm=质量扩散系数vitdb =布朗系数扩散系数m2s−1f=无因次流函数k=多孔介质渗透率m2kT=热扩散比k∗=平均吸收系数m−1cs=浓度敏感性cp=恒压比热JKg−1K−1We=局部Weissenberg数pr =Prandtl数q0 =产热(吸收)系数JK−1m−3s−1Q=产热参数du =Dufour(扩散-热)参数=吸力参数sc =施密特数sr =soret参数k=多孔参数term =磁场参数cf =皮肤摩擦系数cw =表面纳米颗粒浓度mol/LT=纳米流体温度KR=辐射参数tw =表面温度KNb=布朗运动参数m - 1Nt=热游泳参数nux ~ =局部努塞尔数shux =局部舍伍德参数u= x方向上的速度v= y方向上的速度希腊符号=θ=无因次温度v=运动粘度m2s - 1Γ=威廉姆森参数μ=黏度系数kgm(−1s(−1))ρ=流体密度kgm(−3)σ=电导率σ m(−1)σ∗=Stefan−boltzmann常数\ breakn Wm(−2K(−4))κ=导热系数Wm−1K−1ϕ=无量次浓度上标=W=壁面条件' =微分η∞=自由流条件披露声明作者未报告潜在的利益冲突。作者在研究、撰写和发表这篇文章时没有得到任何经济支持。关于贡献者的说明。太太KumarR。Madan Kumar于2008年获得纯数学研究生学位,2012年获得印度安得拉邦蒂鲁帕蒂的Sri Venkateswara大学流体动力学哲学硕士学位。从2008年至今,他一直担任数学导师,并在印度安得拉邦伊杜普拉帕亚的拉吉夫甘地知识技术大学担任电子数学内容开发人员(2009年至2014年)。目前,他是一名研究学者,在印度海得拉巴校区GITAM科学学院(被认为是一所大学)流体动力学领域工作。他的主要兴趣领域是牛顿流体和非牛顿流体,纳米流体的应用,索雷特和杜福尔效应,传热传质和数值技术。Srinivasa RajuDr。R. Srinivasa Raju目前在印度特伦甘纳邦海得拉巴Rudraram海得拉巴校区GITAM科学学院(被视为大学)担任副教授。他于2012年获得Osmania大学应用数学博士学位,并于2005年获得Osmania大学应用数学硕士学位。他在国际和国内知名期刊上发表了115篇以上的文章。他还参加了各种国内和国际会议并发表论文。他出版了一本名为《MHD流体流动问题的有限元技术》的书,由RIGI出版。他是四家国际期刊的编辑。他是几个国家和国际数学学会的成员。2018年,他获得了斯里尼瓦萨·拉马努金终身成就奖。
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Effects of chemical reaction, Soret and Dufour parameters on MHD dissipative Williamson nanofluid flow over a slippery stretching sheet through a porous medium
ABSTRACTThe goal of this study is to determine the effects of Soret, Dufour, and chemical reaction parameters on 2-D MHD Williamson nanofluid flow over a slippery-stretching sheet immersed in a porous medium. Under the influence of both magnetic field and thermal radiation, the significance of viscous dissipation and velocity slip boundary condition with heat generation have been explored. Similarity components were used to turn the nonlinear Partial Differential Equations (PDEs) into nonlinear Ordinary Differential Equations (ODEs), and they were solved using the fourth-order approach of the Runge–Kutta (R–K) method along with the shooting technique. The numerical computations were subsequently illustrated visually to demonstrate the influence of various physical factors on the plots of temperature, velocity, and concentration of the nanofluid. With the use of comparison with previously published data in a restricted sense, the veracity of computation results is evaluated. The tabular values illuminate that the local skin friction coefficient upsurge as the values of the magnetic parameter, porosity parameter, and Brownian motion parameter intensifies, whereas the opposite trend exists for other parameters. The local Nusselt number grows as the Schmidt number rises whereas the reverse trend was experienced for the freed-up parameters.KEYWORDS: Williamson nanofluid flowmagnetohydrodynamics (MHD)porous mediumslippery-stretching sheet Nomenclature C=concentration of the nanoparticles mol/LCw=surface nanoparticles concentration molL−1Kr=chemical reaction constant s−1a=Stretching velocit s−1T∞=free stream temperature KT=temperature of the nanofluidTm=mean nanofluid temperatureC∞=free nanoparticle concentration mol/LB0=Strength of the uniform magnetic field Tg=gravitational acceleration ms−2Dm=coefficient of mass diffusivitDB=Brownian diffusion coefficient m2s−1f=dimensionless stream functionk=permeability of porous medium m2kT=ratio of thermal diffusionk∗=mean absorption coefficient m−1cs=concentration susceptibilitycp=specific heat at constant pressure JKg−1K−1We=local Weissenberg numberPr=Prandtl numberQ0=heat generation (absorption) coefficient JK−1m−3s−1Q=heat generation parameterDu=Dufour (Diffusion- Thermo) parameterS=suction parameterSc=Schmidt numberSr=soret parameterK=porous parameterM=magnetic field parameterCf=skin friction coefficientCw=Surface nanoparticle concentration mol/LT=nanofluid temperature KR=radiation parameterTw=surface temperature KNb=Brownian motion parameter m−1Nt=thermophoresis parameterNux∼=local nusselt numberShux=local Sherwood parameteru=velocity on x-directionv=velocity on y-directionGreek symbols=θ=dimensionless temperaturev=kinematic viscosity m2s−1Γ=Williamson parameter sμ=CoefficientofviscosityKgm(−1s(−1))ρ=densityofthefluidKgm(−3)σ=electricalconductivitySm(−1)σ∗=Stefan−Boltzmannconstant\breakWm(−2K(−4))κ=thermal conductivity Wm−1K−1ϕ=dimensionlessconcentrationSuperscripts=W=wall condition‘=differentiation with respect to η∞=free stream conditionDisclosure statementNo potential conflict of interest was reported by the author(s).Additional informationFundingThe authors received no financial support for the research, authorship, and publication of this article.Notes on contributorsR. Madan KumarR. Madan Kumar received his post-graduation degree in Pure Mathematics in 2008 and Master of Philosophy in Fluid Dynamics in 2012 from Sri Venkateswara University, Tirupati, Andhra Pradesh, India. He has been working as a Mathematics Mentor from 2008 to till date and worked as an E-Mathematics Content developer (2009 to 2014) at Rajiv Gandhi University of Knowledge Technologies, Idupulapaya, Andhra Pradesh, India. Currently, he is a researcher scholar, working in the area of Fluid Dynamics at GITAM School of Sciences (deemed to be a university), Hyderabad Campus, India. His main interest areas are Newtonian and Non-Newtonian fluids, the applications of nanofluids, Soret and Dufour effects, Heat and Mass Transfer, and Numerical Techniques.R. Srinivasa RajuDr. R. Srinivasa Raju is presently working as an Associate Professor at GITAM School of Science, GITAM (Deemed to be University), Hyderabad Campus, Rudraram, Hyderabad, Telangana state, India. He acquired his Doctorate in Applied Mathematics from Osmania University in 2012, and he also received his Master of Science in Applied Mathematics from Osmania University in 2005. He has over 115 publications in International and National reputed Journals. He also attended and paper presented in various National and International Conferences. He has published a book entitled Finite Element Technique on MHD Fluid Flow Problems by RIGI Publications. He serves as an editorial member for four international journals. He is a member of several National and International Mathematical Societies. He received the Srinivasa Ramanujan Life Time Achievement National Award in the year 2018. He has also received the Prestigious Award for Young Educator and Scholar Award from the National Foundation for Entrepreneurship Development (NFED) in the year 2018. He has produced 4 doctoral candidates. He is currently supervising 10 research scholars.M. Anil KumarDr. M. Anil kumar working as an Associate professor in the Department of Mathematics, at Anurag University. In the year 2020, he obtained his Doctorate from GITAM (Deemed to be University), Visakhapatnam, India, and in 2005, he received his Master of Science in Applied Mathematics from the National Institute of Technology Warangal. Dr. Anil kumar has over 18 years of teaching experience and over 8 years of research experience. He received the Best Teacher award from Anurag University for the academic year 2022-2023. He has 23 publications to his credit in reputed national and international journals. He received a SEED money project from Anurag University of Rs 2 lakhs for the Academic year 2021-22. He received the patent right in Micropolar fluids from Intellectual Property of India in 2022. He also presented papers at various National and International conferences. He is a member of several National and International Mathematical Societies. His research areas include Fluid mechanics, Heat, and Mass transfer. He is currently supervising one research scholar.
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来源期刊
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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