Abstract
The impact and capability of Cu–Al\(_2\)O\(_3\)/water nanoliquid as the heat transfer fluid are numerically investigated along a moving surface with melting heat transfer. The reduced differential equations are solved and presented in the figures and tables. The percent error between present and previous numerical values is 0% which supports the model validation. The volumetric concentration of both Al\(_2\)O\(_3\) and Cu nanoparticles is chosen at most 4% to avoid the instability of the nanofluid. The dual solutions are only seen when the external flow and solid surface move in an opposite direction. Remarkably, the use of hybrid nanofluid assists the boundary layer separation in the presence of melting heat transfer. However, the heat transfer rate of Cu–Al\(_2\)O\(_3\)/water is inevitably greater than the pure water and Cu–water. An increase in melting parameter reduces the heat transfer rate and accelerates the separation of boundary layer. The stability analysis supports the initial hypothesis from the graphical results that the second solution is unstable.
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Abbreviations
- A :
-
Surface area of the heat transfer (\(\text {m}^{2}\))
- \(f(\eta )\) :
-
Dimensionless stream function
- h :
-
Heat transfer coefficient (\(\text {W}\,\text{m}^{-2}\,\text {K}^{-1}\))
- k :
-
Fluid thermal conductivity (\(\text {W}\,\text{m}^{-1}\,\text {K}^{-1}\))
- \(q_{\text{w}}\) :
-
Surface heat flux (\(\text {W}\,\text{m}^{-2}\))
- \(s_1\) :
-
First solid nanoparticle (Alumina/Al\(_2\)O\(_3\))
- \(s_2\) :
-
Second solid nanoparticle (Copper/Cu)
- t :
-
Time (s)
- u, v :
-
Velocity components along the x, y directions, respectively (\(\text {m}\,\text{s}^{-1}\))
- x, y :
-
Cartesian coordinates
- \(C_{\text{f}}\) :
-
Skin friction coefficient
- \(C_{\text{p}}\) :
-
Specific heat at constant temperature (\(\text {J}\,\text{kg}^{-1}\,\text {K}^{-1}\))
- \(\left( \rho C_{\text{p}}\right)\) :
-
Heat capacity of the fluid (\(\text {J}\,\text{K}^{-1}\,\text {m}^{-3}\))
- Me:
-
Melting parameter
- Nb:
-
Brownian motion parameter
- Nt:
-
Thermophoresis parameter
- \(Nu_{\text{x}}\) :
-
Local Nusselt number
- \(\text {Pr}\) :
-
Prandtl number
- \({\text{Re}}_{\text{x}}\) :
-
Local Reynolds number
- T :
-
Fluid temperature (K)
- \(T_{0}\) :
-
Temperature of the solid surface (K)
- \(T_{\text{m}}\) :
-
Melting surface temperature (K)
- \(T_{\infty }\) :
-
Ambient temperature (K)
- \(U_{\text{w}}\) :
-
Velocity of the moving surface (\(\text {m}\,\text{s}^{-1}\))
- \(U_\infty\) :
-
Free stream velocity (\(\text {m}\,\text{s}^{-1}\))
- \(\lambda\) :
-
Moving parameter
- \(\eta\) :
-
Similarity variable
- \(\psi\) :
-
Stream function
- \(\theta\) :
-
Dimensionless temperature
- \(\mu\) :
-
Dynamic viscosity (\(\text {kg}\,\text{m}^{-1}\,\text {s}^{-1}\))
- \(\nu\) :
-
Kinematic viscosity (\(\text {m}^2\,{\text {s}^{-1} }\))
- \(\rho\) :
-
Fluid density (\(\text {kg}\,{\text {m}^{-3} }\))
- \(\gamma\) :
-
Eigenvalue
- \(\gamma _1\) :
-
Smallest eigenvalue
- \(\tau\) :
-
Dimensionless time variable
- \(\tau _{\text{w}}\) :
-
Wall shear stress (\(\text {kg}\,\text{m}^{-1}\,\text {s}^{-2}\))
- \(\phi _1,\phi _2\) :
-
Volumetric concentration for first nanoparticle and second nanoparticle, respectively
- f:
-
Base fluid
- nf:
-
Nanofluid
- hnf:
-
Hybrid nanofluid
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Acknowledgements
The financial support from Ministry of Higher Education (Malaysia) through the Fundamental Research Grant Scheme (FRGS5540309) is deeply appreciated including the facilities from Universiti Putra Malaysia and Universiti Teknikal Malaysia Melaka. The authors also appreciate the good comments from the competent reviewers which surely improve the quality of this work.
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Khashi’ie, N.S., Md Arifin, N., Pop, I. et al. Melting heat transfer in hybrid nanofluid flow along a moving surface. J Therm Anal Calorim 147, 567–578 (2022). https://doi.org/10.1007/s10973-020-10238-4
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DOI: https://doi.org/10.1007/s10973-020-10238-4