Partial Slip Impact on Double Diffusive Convection Flow of Magneto-Carreau Nanofluid through Inclined Peristaltic Asymmetric Channel

Abstract

The significance of partial slip on double diffusive convection on magneto-Carreau nanofluid through inclined peristaltic asymmetric channel is examined in this paper. The two-dimensional and directional flow of a magneto-Carreau nanofluid is mathematically described in detail. Under the lubrication technique, the proposed model is simplified. The solutions of extremely nonlinear partial differential equations are calculated using a numerical technique. Graphical data are displayed using Mathematica software and Matlab to examine how temperature, pressure rise, concentration, pressure gradient, velocity profile, nanoparticle volume fraction, and stream functions behave on emerging parameters. It is noticed that as the velocity slip parameter is increased, the axial velocity at the channel’s center increases. Additionally, near the boundary, opposite behavior is observed. The temperature, concentration, and nanoparticle profile drops by increasing thermal slip, concentration slip, and nanoparticle slip parameter.

Peristaltic Transport of Carreau Coupled Stress Nanofluid with Cattaneo-Christov Heat Flux Model Inside a Symmetric Channel

“…Therefore, rising in 𝑊 𝑒 𝑐 deemed as reason for decaying in the viscosity of the fluid, which enlarges the axial velocity 𝑞 𝜁 correspondingly. This demeanor is totally consistent to the behavior that reported in [15], [32], and [35]. Figure 3 portrays the impact of the velocity slip parameter𝛽 1 𝑠 on the axial velocity 𝑞 𝜁 .…”

“…These fluids are mainly utilized to modulate thermal conductivity and heat transfer in such a way as to achieve the better. Given the importance of these several important applications, many researchers have paid considerable attention to the study of nanofluids [20][21][22][23][24][25][26][27][28][29][30][31][32].…”

Outcomes of Uniform as well as Non-Uniform Temperature Profiles on the Onset of Double Diffusive Magneto-Darcy-Rayleigh-Benard Convection in a Two Layer set up in the presence of Local Thermal Non-Equilibrium

“…The first order equations in a F 2 are: For fluid layer, ... (8) ... (9) ... (10) For porous layer, ... (11) ... (12) ... ( 13…”