Impact of velocity slip and heat source on tangent hyperbolic nanofluid flow over an electromagnetic surface with Soret effect and variable suction/injection

Abstract

The applicability and significance of tangent hyperbolic fluid in several engineering fields are encouraging, and the examination of the Soret effect phenomena on non-Newtonian fluids with thermal transport mechanisms is becoming more widely accepted. The effect of velocity slip on electromagnetohydrodynamic (EMHD) of tangent hyperbolic flow through a Riga plate with a heat source, suction/injection, and reactive energy, on the other hand, is unknown. The current research configuration model investigates the impact of Soret, suction/injection, activation energy, and heat source on the EMHD flow of hyperbolic tangent nanofluid via a stretched sheet. The governing equations of PDEs are transmuted into nonlinear ODEs with adequate similarity variables. The numerical output of the resulting Ordinary differential equations is performed using the MATLAB bvp4c built-in. The implication of rising attributes on temperature, velocity, concentration shapes, drag force coefficient, Sherwood number, and Nusselt number is graphically and numerically depicted. As a result, the derived findings are validated by comparing them to previous output. Remarkably, the increase in temperature of the hyperbolic tangential nanofluid flow is caused by a rise in slip velocity and Weissenberg numbers, which has a reverse effect on Suction. The EMHD parameter, on the other hand, enhances the velocity distribution, which impacts the slip velocity parameter.

Analysis on Rheology of Unsteady Casson Fluid Flow through an Atherosclerotic Lesion

“…With the use of predefined parameters and MATLAB (R2022b), numerical computations of these quantities for their primary physiological importance have been carried out. The results of axial velocity (u c ), plug core velocity (u p ), plug core radius (R c ), flow rate (Q), wall shear stress (τ wa ) and effective viscosity (μ e ) are obtained and computed for the fixed values of F = 0.2, n = 0.95, m = 2, φ = 0.2, τ c = 0.1, ω = 1 [25][26][27]. Figure 2 depicts the variation of Reynolds number (α) on axial velocity (u c ) with axial distance (r) for different fixed parameters F = 0.2, ϕ = 0.2, e = 1, ω = 1, t = 1, δ c = 0.1, u s = 0.02.…”

Numerical Analysis Study of Chemically Radiative MHD Williamson Nanofluid Flow over an Inclined Surface with Heat Source

“…Numerous researchers investigated numerous facets of Newtonian fluid under diverse conditions as can be observed in Ref. [34][35][36][37][38][39][40][41][42][43][44][45].…”

Comprehensive analysis of radiation impact on the transfer of heat and mass micropolar MHD free convective fluid flow across a stretching permeability sheet with suction/injection

“…Reddy and Goud 28 studied the stagnation point of the flow of nanofluids using a stretched sheet and the impact of thermal radiation on the underlying MHD heat and mass transfer. The stretched sheet, boundary layer flow, suction/injection, porosity, and many other flow configurations have all been the subject of much research 11,29–45 …”

“…The stretched sheet, boundary layer flow, suction/injection, porosity, and many other flow configurations have all been the subject of much research. 11,[29][30][31][32][33][34][35][36][37][38][39][40][41][42][43][44][45] The reason for carrying out this task is to examine the impact of radiation on the transmission of heat and mass using micropolar free convective MHD fluid flow over a stretching permeable sheet with suction and injection. In an effort to turn the governing boundary layer equations into ordinary differential equations (ODEs), similarity changes are put to use.…”