Abstract

We investigated the shear banding phenomena in the non-isothermal simple-shear flow of a viscoelastic-fluid-based nanofluid (VFBN) subject to exothermic reactions. The polymeric (viscoelastic) behavior of the VFBN was modeled via the Giesekus constitutive equation, with appropriate adjustments to incorporate both the non-isothermal and nanoparticle effects. Nahme-type laws were employed to describe the temperature dependence of the VFBN viscosities and relaxation times. The Arrhenius theory was used for the modeling and incorporation of exothermic reactions. The VFBN was modeled as a single-phase homogeneous-mixture and, hence, the effects of the nanoparticles were based on the volume fraction parameter. Efficient numerical schemes based on semi-implicit finite-difference-methods were employed in MATLAB for the computational solution of the governing systems of partial differential equations. The fundamental fluid-dynamical and thermodynamical phenomena, such as shear banding, thermal runaway, and heat transfer rate (HTR) enhancement, were explored under relevant conditions. Important novel results of industrial significance were observed and demonstrated. Firstly, under shear banding conditions of the Giesekus-type VFBN model, we observed remarkable HTR and Therm-C enhancement in the VFBN as compared to, say, NFBN. Specifically, the results demonstrate that the VFBN are less susceptible to thermal runaway than are NFBN. Additionally, the results illustrate that the reduced susceptibility of the Giesekus-type VFBN to the thermal runaway phenomena is further enhanced under shear banding conditions, in particular when the nanofluid becomes increasingly polymeric. Increased polymer viscosity is used as the most direct proxy for measuring the increase in the polymeric nature of the fluid.

Highlights

  • The evidence of the efficacy of nanofluids in heat transfer rate (HTR) and thermal conductivity (Therm-C) enhancement is widespread and commonly accepted; such nanofluids are extensively used for these purposes

  • This allows us to focus our attention on the primary effects of shear banding on HTR and Therm-C enhancement without the complications of 2D

  • P is the pressure field; ε is the Giesekus non-linear parameter; σ is the total stress tensor; S is the rate of deformation tensor; τ is the polymer stress tensor;n f is the solvent viscosity for the nanofluid; (η p )n f is the polymer viscosity for the nanofluid; ηn f is the total viscosity for the nanofluid; κn f is the thermal conductivity for the nanofluid; α is the activation energy parameter; β is the polymer to total viscosity ratio; Br is the Brinkman number; δ1 is σ = τ +n f S, S=

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Summary

Introduction

Fluid viscoelasticity has received wide attention in this regard, for the improvement of certain industrial, domestic, and medical applications. Such widespread viscoelastic (polymeric)fluids, fluids,for forthe theimprovement improvementand and enenhancement of,of, say, HTR and. Shear-banding phenomena of viscoelastic fluids represents physical discontinuities shear rateprofiles profilesofofthe theflow-velocity flow velocityand andfinds findswide wide ininandand physical discontinuities in in thethe shear-rate dustrial and domestic application, say, in emulsion polymerization and drop break-up [34]. Shear banding phenomena and Rolie-Poly viscoelastic constitutive models.

Problem Formulation
Model assumptions
Dimensionless Governing Equations
Numerical and Computational Algorithms
Time Development of Steady Smooth Solutions
Mesh-Size and Time-Step and Convergence
Development of Shear Banding
Thermal Runway
Parameter Dependence of Solutions under Shear Banding Conditions
Concluding Remarks
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