Numerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluid

This article concentrates on the characteristics of heat transfer in oblique stagnation point flow of Jeffrey fluid deformed by a linear stretchable surface. The surface temperature is higher than that of the ambient fluid. Appropriate transformations are implemented to produce a system of dimension...

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Main Authors: Ambreen Arshad, M. Sajid, M. A. Rana, K. Mahmood
Format: Article
Language:English
Published: AIP Publishing LLC 2018-10-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5038810
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spelling doaj-55355a47f57a4c2db9d16168af6f69162020-11-25T02:27:32ZengAIP Publishing LLCAIP Advances2158-32262018-10-01810105111105111-1310.1063/1.5038810041809ADVNumerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluidAmbreen Arshad0M. Sajid1M. A. Rana2K. Mahmood3Department of Mathematics and Statistics, Riphah International University, Islamabad 44000, PakistanDepartment of Mathematics and Statistics, International Islamic University, Islamabad 44000, PakistanDepartment of Mathematics and Statistics, Riphah International University, Islamabad 44000, PakistanDepartment of Mathematics and Statistics, International Islamic University, Islamabad 44000, PakistanThis article concentrates on the characteristics of heat transfer in oblique stagnation point flow of Jeffrey fluid deformed by a linear stretchable surface. The surface temperature is higher than that of the ambient fluid. Appropriate transformations are implemented to produce a system of dimensionless equations. Numerical solutions are computed via Keller-Box scheme. Graphical behaviors of numerous physical parameters are illustrated corresponding to velocity and temperature distributions. Numerical data is computed for skin friction coefficient and heat transfer rate corresponding to various pertinent parameters. Location of the stagnation point is also computed through graphical analysis. Velocity and temperature distributions decay for higher values of ratio parameter of relaxation to retardation times and Prandtl number respectively.http://dx.doi.org/10.1063/1.5038810
collection DOAJ
language English
format Article
sources DOAJ
author Ambreen Arshad
M. Sajid
M. A. Rana
K. Mahmood
spellingShingle Ambreen Arshad
M. Sajid
M. A. Rana
K. Mahmood
Numerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluid
AIP Advances
author_facet Ambreen Arshad
M. Sajid
M. A. Rana
K. Mahmood
author_sort Ambreen Arshad
title Numerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluid
title_short Numerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluid
title_full Numerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluid
title_fullStr Numerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluid
title_full_unstemmed Numerical simulation of heat transfer features in oblique stagnation-point flow of Jeffrey fluid
title_sort numerical simulation of heat transfer features in oblique stagnation-point flow of jeffrey fluid
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2018-10-01
description This article concentrates on the characteristics of heat transfer in oblique stagnation point flow of Jeffrey fluid deformed by a linear stretchable surface. The surface temperature is higher than that of the ambient fluid. Appropriate transformations are implemented to produce a system of dimensionless equations. Numerical solutions are computed via Keller-Box scheme. Graphical behaviors of numerous physical parameters are illustrated corresponding to velocity and temperature distributions. Numerical data is computed for skin friction coefficient and heat transfer rate corresponding to various pertinent parameters. Location of the stagnation point is also computed through graphical analysis. Velocity and temperature distributions decay for higher values of ratio parameter of relaxation to retardation times and Prandtl number respectively.
url http://dx.doi.org/10.1063/1.5038810
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