Entropy analysis and unsteady MHD mixed convection stagnation-point flow of Casson nanofluid around a rotating sphere

被引:43
|
作者
Mahdy, A. [1 ]
Chamkha, Ali J. [2 ]
Nabwey, Hossam A. [3 ,4 ]
机构
[1] South Valley Univ, Fac Sci, Math Dept, Qena, Egypt
[2] Prince Mohammad Bin Fahd Univ, Mech Engn Dept, Prince Sultan Endowment Energy & Environm, Al Khobar 31952, Saudi Arabia
[3] Prince Sattam Bin Abdulaziz Univ, Coll Sci & Humanities Al Kharj, Dept Math, Al Kharj 11942, Saudi Arabia
[4] Menoufia Univ, Fac Engn, Dept Basic Engn Sci, Shibin Al Kawm 32511, Egypt
关键词
Two-phase nanofluid; Entropy generation; Biot number; Non-Newtonian; Mixed; Sphere; NON-NEWTONIAN NANOFLUID; HEAT-TRANSFER; FLUID-FLOW; GENERATION MINIMIZATION; STRETCHING SHEET; MASS-TRANSFER; MAGNETOHYDRODYNAMICS; RADIATION;
D O I
10.1016/j.aej.2020.04.028
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The current perusal introduces a numerical analysis to point out the flow of MHD conjugate forced and free convection with entropy generation analysis due to non-Newtonian Casson-nanofluid around a rotating sphere with convective boundary conditions. Two-phase flow of nanofluid model is employed for the problem under consideration. Both the velocity of free stream and the sphere rotates with angular velocity changed continuously with time. The highly nonlinear partial differential Structures which describe the case study are mutated into a nonlinear ordinary differential structures via utilizing appropriate dimensionless quantities. The numerical solutions of ordinary differential structures have been acquired by applying the fourth order Runge-Kutta-Fehlberg technique with shooting scheme via MATLAB. Aspects of such controlled physical parameters have been clarified and discussed in details using some charts and tables. Comparison with previous literature results is also done and is found to be very good agreement with those published earlier. (C) 2020 The Authors. Published by Elsevier B.V. on behalf of Faculty of Engineering, Alexandria University.
引用
收藏
页码:1693 / 1703
页数:11
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