Abstract
The present numerical study deals with the analysis of hydrodynamic and thermal characteristics of a shear-thinning Herschel–Bulkley fluid flow within a pipe of a circular cross section, maintained at a uniform wall temperature. The governing equations of the studied steady problem are solved using a homemade computer code based on the finite volume method. The paper is focused on the consequences of neglecting the temperature dependency of the fluid’s consistency and/or the viscous dissipation on both pressure drop and heat transfer. The results show, indeed, that neglecting the temperature dependency of the fluid’s viscosity leads to significantly undervalue these parameters, especially when viscous dissipation is also missed. Abacuses depicting the friction factor of Fanning and the Nusselt number variations according to both Brinkman number and dimensionless temperature coefficient are proposed to sum up the study.
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Abbreviations
- a :
-
Temperature coefficient (K−1)
- \(a^{*}\) :
-
Dimensionless temperature coefficient, = a ΔT
- Br :
-
Brinkman number, \({{K_{0} V_{0}^{2} } \mathord{\left/ {\vphantom {{K_{0} V_{0}^{2} } {k(T_{0} - T_{\text{w}} )}}} \right. \kern-0pt} {k(T_{0} - T_{\text{w}} )}}\)
- C p :
-
Specific heat at constant pressure (J kg−1 K−1)
- D :
-
Pipe diameter (m)
- f :
-
Friction factor
- f Re :
-
Friction factor of Fanning
- h :
-
Heat transfer coefficient (W m−2 K−1)
- HB :
-
Herschel–Bulkley number, \({{\tau_{0} D^{n} } \mathord{\left/ {\vphantom {{\tau_{0} D^{n} } {K_{0} V_{0}^{n} }}} \right. \kern-0pt} {K_{0} V_{0}^{n} }}\)
- k :
-
Fluid thermal conductivity (W m−1 K−1)
- K :
-
Fluid consistency (Pa sn)
- K 0 :
-
Fluid consistency at the reference temperature (Pa sn)
- \(K^{*}\) :
-
Dimensionless fluid consistency, K(T)/K 0
- L :
-
Pipe length (m)
- m :
-
Exponential growth parameter (s)
- M :
-
Dimensionless exponential growth parameter in Eq. (6), = m V 0/D
- n :
-
Flow index
- Na :
-
Nahme number, \(= {{a\,K_{0} V_{0}^{2} } \mathord{\left/ {\vphantom {{a\,K_{0} V_{0}^{2} } k}} \right. \kern-0pt} k}\)
- Nu :
-
Nusselt number, \(= \frac{hD}{k} = \frac{ - 1}{{\theta_{m} }}\left. {\frac{\partial \theta }{\partial R}} \right|_{R = 0.5}\)
- Pe :
-
Peclet number, = Re Pr
- Pr :
-
Prandtl number, \(= {{K_{0} C_{\text{p}} V_{0}^{n - 1} } \mathord{\left/ {\vphantom {{K_{0} C_{\text{p}} V_{0}^{n - 1} } {kD^{n - 1} }}} \right. \kern-0pt} {kD^{n - 1} }}\)
- \(P^{*}\) :
-
Dimensionless pressure, = \(p^{*}\)/ρ V 20
- \(p^{*}\) :
-
Pressure (Pa)
- r :
-
Radial coordinate (m)
- r p :
-
Plug size (m)
- \(r_{0}^{*}\) :
-
Dimensionless plug size according to [19]
- \(r_{0}^{{\prime }}\) :
-
Dimensionless plug size, r p/(D/2) = τ 0/τ w = \(r_{0}^{*} /2\)
- R :
-
Dimensionless radial coordinate, = r/D
- Re :
-
Reynolds number, \({{ = \rho V_{0}^{2 - n} D^{n} } \mathord{\left/ {\vphantom {{ = \rho V_{0}^{2 - n} D^{n} } {K_{0} }}} \right. \kern-0pt} {K_{0} }}\)
- T :
-
Temperature (K)
- T 0 :
-
Inlet temperature (K)
- T m :
-
Bulk temperature (K)
- T w :
-
Wall temperature (K)
- U :
-
Dimensionless x-component velocity, = Vx/V0
- V :
-
Dimensionless r-component velocity, = V r/V 0
- V 0 :
-
Mean velocity (m s−1)
- V x :
-
x-Component velocity (m s−1)
- V r :
-
r-Component velocity (m s−1)
- x :
-
Axial coordinate (m)
- X :
-
Dimensionless axial coordinate, = x/D
- \(\dot{\gamma }\) :
-
Rate of strain (s−1)
- \(\dot{\gamma }^{*}\) :
-
Dimensionless rate of strain
- ΔT :
-
Temperature difference, = T w − T 0 (K)
- Δp :
-
Pressure drop (Pa)
- η :
-
Effective viscosity of the Herschel–Bulkley fluid (Pa sn)
- η eff :
-
Dimensionless effective viscosity, = η/K 0
- θ :
-
Dimensionless temperature, = (T − T w)/(T 0 − T w)
- θ m :
-
Dimensionless mean temperature, (T m − T w)/(T 0 − T w)
- ρ :
-
Density of the fluid (kg m−3)
- τ :
-
Shear stress (Pa)
- τ 0 :
-
Yield stress (Pa)
- τ w :
-
Wall shear stress (Pa)
- asy:
-
Asymptotic
- av:
-
Average
- c:
-
Centreline
- x:
-
Local
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Labsi, N., Benkahla, Y.K. & Boutra, A. Temperature-dependent shear-thinning Herschel–Bulkley fluid flow by taking into account viscous dissipation. J Braz. Soc. Mech. Sci. Eng. 39, 267–277 (2017). https://doi.org/10.1007/s40430-016-0499-5
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DOI: https://doi.org/10.1007/s40430-016-0499-5