DSpace@Çankaya

Significance of chemical reaction with activation energy for Riga wedge flow of tangent hyperbolic nanofluid in existence of heat source

Basit öğe kaydını göster

dc.contributor.author Abdal, Sohaib
dc.contributor.author Siddique, Imran
dc.contributor.author Alshomrani, Ali Saleh
dc.contributor.author Jarad, Fahd
dc.contributor.author Ud Din, Irfan Saif
dc.contributor.author Afzal, Saima
dc.date.accessioned 2022-12-16T12:03:36Z
dc.date.available 2022-12-16T12:03:36Z
dc.date.issued 2021-12
dc.identifier.citation Abdal, Sohaib...at all (2021). "Significance of chemical reaction with activation energy for Riga wedge flow of tangent hyperbolic nanofluid in existence of heat source", Case Studies in Thermal Engineering, Vol. 28. tr_TR
dc.identifier.issn 2214-157X
dc.identifier.uri http://hdl.handle.net/20.500.12416/6008
dc.description.abstract This manuscript uncovers the heat and mass transfer of an unsteady tangent hyperbolic nanofluid flow across an extensible Riga wedge under the effects of stagnation point, heat source, and activation energy. The flow computations with modified Hartmann numbers are embedded in this investigation particularly in the unsteady tangent hyperbolic liquid stream scenario. The focus pertains to augment heat conduction in the bulk liquid as heat and mass transport media. The implications of controlling parameters on non-dimensional speed, temperature, as well as concentration profiles are visually portrayed. The governing partial differential equations are modified into non-dimensional forms by reducing the number of independent factors, which are then pursued numerically utilizing the Runge-Kutta method with the shooting tool. The velocity of Newtonian fluid improves as the magnitude of wedge angle parameter βw rises, although it is marginally lower than that of tangent hyperbolic fluid, the temperature of Newtonian fluid intensifies substantially faster than that of tangent hyperbolic fluid for higher values of βw. The skin friction factor increases with alterations to the Hartmann parameter, Weissenberg factor, wedge angle parameter as well as suction parameter. The percentage increase in skin friction factor is 13.3 and 21.93 when modified Hartmann number takes input in the range 0 ≤ Mh ≤ 0.2 and unsteady parameter 0.1 ≤ A ≤ 0.5. The Schmidt number, chemical change, and wedge angle parameters are all designed to boost the Sherwood number. tr_TR
dc.language.iso eng tr_TR
dc.relation.isversionof 10.1016/j.csite.2021.101542 tr_TR
dc.rights info:eu-repo/semantics/closedAccess tr_TR
dc.subject Magnetohydrodynamic tr_TR
dc.subject Riga Wedge tr_TR
dc.subject Runge-Kutta Method tr_TR
dc.subject Stagnation Point tr_TR
dc.subject Tangent Hyperbolic Fluid tr_TR
dc.title Significance of chemical reaction with activation energy for Riga wedge flow of tangent hyperbolic nanofluid in existence of heat source tr_TR
dc.type article tr_TR
dc.relation.journal Case Studies in Thermal Engineering tr_TR
dc.contributor.authorID 234808 tr_TR
dc.identifier.volume 28 tr_TR
dc.contributor.department Çankaya Üniversitesi, Fen - Edebiyat Fakültesi, Matematik Bölümü tr_TR


Bu öğenin dosyaları:

Dosyalar Boyut Biçim Göster

Bu öğe ile ilişkili dosya yok.

Bu öğe aşağıdaki koleksiyon(lar)da görünmektedir.

Basit öğe kaydını göster