On Cattaneo-Chrystov heat flux model for nanofluid flow on Darcy–Forchheimer porous medium past unsteady stretching cylinder

被引:0
|
作者
Sobhanapuram, Sreedhar [1 ]
Devi, S.V.V Rama [2 ]
Ganteda, Charankumar [3 ]
Kottapalli, Rajyalakshmi [3 ]
Govindan, Vediyappan [4 ]
Byeon, Haewon [5 ]
Pimpunchat, Busayamas [6 ]
机构
[1] Department of Mathematics, GITAM School of Science, GITAM Deemed University, Andhra Pradesh, Visakhapatnam, India
[2] Department of Mathematics, Raghu Engineering College (A), Andhra Pradesh, Visakhapatnam, India
[3] Department of Mathematics Koneru Lakshmaiah Eduction Foundation(KLEF) Vaddeswaram, Andhra Pradesh, Guntur, India
[4] Department of Mathematics, Hindustan Institute of Technology and Science, Chennai, India
[5] Convergence Department, Korea University of Technology and Education, Cheonan, Korea, Republic of
[6] Department of Mathematics, School of Science, King Mongkut's Institute of Technology Ladkrabang (KMITL), Bangkok, 10520, Thailand
来源
基金
新加坡国家研究基金会;
关键词
Boundary layer flow - Convergence of numerical methods - Cylinders (shapes) - Heat convection - Runge Kutta methods - Temperature - Thermal conductivity of liquids - Unsteady flow;
D O I
10.1016/j.ijft.2025.101101
中图分类号
学科分类号
摘要
In a Darcy-Forchheimer porous medium with variable thermal conductivity, this work describes the convective transport mechanisms of Williamson nanofluid and nanofluid flow via an unstable stretched cylindrical sheet. The governing boundary evaluates issue of the flow regime is formulated utilizing the conservation laws of mass, momentum, energy. A couple of nonlinear partial differential constitutions are used to express the flow. A suitable similarity transformation along with certain approaches are applied to convert the pair of partial differential constitutions into an initial value problem system. In this analysis, the Cattaneo-Chrystov model is introduced. After that, the shooting strategy and the Runge-Kutta fourth order are used to numerically solve the system of initial value problems. Analysis is done on the effects of several factors on the nanofluid's temperature, velocity, and concentration contours. such as the thermal conductivity parameter, the concentration and temperature Biot numbers, the unsteady parameter, and others. Conversely, larger values of the unstable parameter result in significant wall friction that hinders the nanofluid'smobility. Furthermore, under widely accepted assumptions, the numerical approach found here shows great agreement with several previous efforts. An uplifting in the unsteady factor causes the nanofluid's temperature and concentration boundary layers to enlarge. When the corresponding Biot numbers (thermal and concentration) grow, the two boundary layers of the nanofluid expand, initiating the convective mass and heat transfers from the wall to the system. The rates of mass and heat transfers increase and decrease in tandem with increases in the thermal conductivity parameter and thermal Biot number, respectively; however, the transfers exhibit the opposite behavior for higher concentration Biot number values.Compared with the existing research, the outcomes demonstrate excellent congruence. © 2025 The Author(s)
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