Abstract
The use of nanofluids as working fluid is one of the represented methods in efficiency enhancement of various systems. One of the most important subjects in nanofluid utilization is finding the optimal conditions. In this study, the efforts have been made to find optimal condition of forced convection nanofluid flow inside a circular tube. The flow is assumed turbulent, and optimization process is carried out for two metallic oxide nanoparticles (Al2O3, CuO) and one nonmetallic oxide nanoparticle (SiO2), dispersed in a 60:40% ethylene glycol/water base fluid. The optimization process has been performed based on the second law of thermodynamic and entropy generation minimization approach. The process has been focused on finding the optimal values for volume fraction, Reynolds number, diameter of particles and average flow temperature. Results show that two metallic oxide nanofluids generate less entropy compared with nonmetallic oxide nanofluid. In addition, comparing these two metallic oxide nanofluids, the maximum amount of total entropy generation is 20% lower when CuO nanoparticles added to the base fluid instead of Al2O3.
Similar content being viewed by others
Abbreviations
- \(A\) :
-
Cross-sectional area of the tube (m2)
- \(B\) :
-
Duty parameter
- \(Be\) :
-
Bejan number
- \(C_{\text{p}}\) :
-
Specific heat (J kg−1 K−1)
- \(D\) :
-
Inside diameter of the tube (m)
- \(d_{\text{p}}\) :
-
Nanoparticle diameter (nm)
- \(f\) :
-
Friction factor
- \(h\) :
-
Heat transfer coefficient (W m−2 K−1)
- \(k\) :
-
Thermal conductivity (W m−1 K−1)
- \(L\) :
-
Length of the tube (m)
- \(\dot{m}\) :
-
Mass flow rate (kg s−1)
- \(N_{\text{s}}\) :
-
Entropy generation number
- \(Nu\) :
-
Nusselt number
- \(Pr\) :
-
Prandtl number
- \(Q\) :
-
Dimensionless heat flux
- \(q\) :
-
Heat transfer per unit tube length (W m−1)
- \(q''\) :
-
Heat flux (W m−2)
- \(Re\) :
-
Reynolds number
- \(R^{2}\) :
-
Coefficient of determination
- \(\dot{S}_{g}^{\prime }\) :
-
Entropy generation rate per unit tube length (W m−1 K−1)
- \(S_{{{\text{g}},{\text{h}}}}\) :
-
Entropy generation due to the heat transfer (W K−1)
- \(S_{{{\text{g}},{\text{f}}}}\) :
-
Entropy generation due to the fluid friction (W K−1)
- \(S_{{{\text{g}},{\text{tot}}}}\) :
-
Total entropy generation (W K−1)
- \(St\) :
-
Stanton number
- \(T\) :
-
Average flow temperature (K)
- \(T_{0}\) :
-
Reference temperature, 273 K
- \(\kappa\) :
-
Boltzmann constant, 1.381 × 10−23 (J K−1)
- \(\mu\) :
-
Viscosity (Ns m−2)
- \(\rho\) :
-
Density (kg m−3)
- \(\varPhi\) :
-
Irreversibility distribution ratio
- \(\phi\) :
-
Particle volumetric concentration (%)
- B:
-
Brownian motion
- bf:
-
Base fluid
- nf:
-
Nanofluid
- opt:
-
Optimum
- p:
-
Particle
- s:
-
Static
References
Mwesigye A, Huan Z, Meyer JP. Thermodynamic optimisation of the performance of a parabolic trough receiver using synthetic oil-Al2O3 nanofluid. Appl Energy. 2015;156:398–412. https://doi.org/10.1016/j.apenergy.2015.07.035.
Okati V, Behzadmehr A, Farsad S. Analysis of a solar desalinator (humidification–dehumidification cycle) including a compound system consisting of a solar humidifier and subsurface condenser using DoE. Desalination. 2016;397:9–21.
Jamal-abadi MT, Zamzamian AH. Optimization of thermal conductivity of Al2O3 nanofluid by using ANN and GRG methods. Int J Nanosci Nanotechnol. 2013;9:177–84.
Minea AA, Lorenzini G. A numerical study on ZnO based nanofluids behavior on natural convection. Int J Heat Mass Transf. 2017;114:286–96. https://doi.org/10.1016/j.ijheatmasstransfer.2017.06.069.
Minea AA. Comparative study of turbulent heat transfer of nanofluids: effect of thermophysical properties on figure-of-merit ratio. J Therm Anal Calorim. 2016;124:407–16.
Ahmadi MH, Ahmadi MA, Nazari MA, Mahian O, Ghasempour R. A proposed model to predict thermal conductivity ratio of Al2O3/EG nanofluid by applying least squares support vector machine (LSSVM) and genetic algorithm as a connectionist approach. J Therm Anal Calorim. 2018;123456789:1–11. https://doi.org/10.1007/s10973-018-7035-z.
Maganti LS, Dhar P. Consequences of flow configuration and nanofluid transport on entropy generation in parallel microchannel cooling systems. Int J Heat Mass Transf. 2017;109:555–63. https://doi.org/10.1016/j.ijheatmasstransfer.2017.02.036.
Ibáñez G, López A, Pantoja J, Moreira J, Reyes JA. Optimum slip flow based on the minimization of entropy generation in parallel plate microchannels. Energy. 2013;50:143–9. https://doi.org/10.1016/j.energy.2012.11.036.
Arabpour A, Karimipour A, Toghraie D, Akbari OA. Investigation into the effects of slip boundary condition on nanofluid flow in a double-layer microchannel. Netherlands: J Therm Anal Calorim. Springer; 2017. p. 1–17.
Safi MA, Ghozatloo A, Hamidi AA, Shariaty-Niassar M. Calculation of heat transfer coefficient of MWCNT-TiO2 nanofluid in plate heat exchanger. Iran Nanotechnol Soc 2014;10:153–62. http://www.ijnnonline.net/article_9092_10.html.
Hosseinnezhad R, Akbari OA, Hassanzadeh Afrouzi H, Biglarian M, Koveiti A, Toghraie D. Numerical study of turbulent nanofluid heat transfer in a tubular heat exchanger with twin twisted-tape inserts. J Therm Anal Calorim. 2017. https://doi.org/10.1007/s10973-017-6900-5.
Esfahani JA, Akbarzadeh M, Rashidi S, Rosen MA, Ellahi R. Influences of wavy wall and nanoparticles on entropy generation over heat exchanger plat. Int J Heat Mass Transf. 2017;109:1162–71. https://doi.org/10.1016/j.ijheatmasstransfer.2017.03.006.
Bahiraei M, Berahmand M, Shahsavar A. Irreversibility analysis for flow of a non-Newtonian hybrid nanofluid containing coated CNT/Fe3O4 nanoparticles in a minichannel heat exchanger. Appl Therm Eng. 2017;125:1083–93. https://doi.org/10.1016/j.applthermaleng.2017.07.100.
Delfani S, Karami M, Akhavan Bahabadi MA. Experimental investigation on performance comparison of nanofluid-based direct absorption and flat plate solar collectors. Int J Nano Dimens. 2015;7:85–96. http://www.ijnd.ir/article_15588_2444.html.
Meibodi SS, Kianifar A, Mahian O, Wongwises S. Second law analysis of a nanofluid-based solar collector using experimental data. J Therm Anal Calorim. 2016;126:617–25.
Gong X, Wang F, Wang H, Tan J, Lai Q, Han H. Heat transfer enhancement analysis of tube receiver for parabolic trough solar collector with pin fin arrays inserting. Sol Energy. 2017;144:185–202. https://doi.org/10.1016/j.solener.2017.01.020.
MohammadZadeh P, Sokhansefat T, Kasaeian AB, Kowsary F, Akbarzadeh A. Hybrid optimization algorithm for thermal analysis in a solar parabolic trough collector based on nanofluid. Energy. 2015;82:857–64. https://doi.org/10.1016/j.energy.2015.01.096.
Mahian O, Kianifar A, Sahin AZ, Wongwises S. Entropy generation during Al2O3/water nanofluid flow in a solar collector: effects of tube roughness, nanoparticle size, and different thermophysical models. Int J Heat Mass Transf. 2014;78:64–75. https://doi.org/10.1016/j.ijheatmasstransfer.2014.06.051.
Liu ZH, Li YY. A new frontier of nanofluid research—application of nanofluids in heat pipes. Int J Heat Mass Transf. 2012;55:6786–97. https://doi.org/10.1016/j.ijheatmasstransfer.2012.06.086.
Farzaneh-Gord M, Ameri H, Arabkoohsar A. Tube-in-tube helical heat exchangers performance optimization by entropy generation minimization approach. Appl Therm Eng. 2016;108:1279–87. https://doi.org/10.1016/j.applthermaleng.2016.08.028.
Gutiérrez F, Méndez F. Entropy generation minimization for the thermal decomposition of methane gas in hydrogen using genetic algorithms. Energy Convers Manag. 2012;55:1–13.
Ellahi R, Hassan M, Zeeshan A, Khan AA. The shape effects of nanoparticles suspended in HFE-7100 over wedge with entropy generation and mixed convection. Appl Nanosci. 2015;6:1–11. https://doi.org/10.1007/s13204-015-0481-z.
Siavashi M, Jamali M. Heat transfer and entropy generation analysis of turbulent flow of TiO2-water nanofluid inside annuli with different radius ratios using two-phase mixture model. Appl Therm Eng. 2016;100:1149–60. https://doi.org/10.1016/j.applthermaleng.2016.02.093.
Shalchi-Tabrizi A, Seyf HR. Analysis of entropy generation and convective heat transfer of Al2O3 nanofluid flow in a tangential micro heat sink. Int J Heat Mass Transf. 2012;55:4366–75. https://doi.org/10.1016/j.ijheatmasstransfer.2012.04.005.
Bianco V, Manca O, Nardini S. Performance analysis of turbulent convection heat transfer of Al2O3 water-nanofluid in circular tubes at constant wall temperature. Energy. 2014;77:403–13. https://doi.org/10.1016/j.energy.2014.09.025.
Singh PK, Anoop KB, Sundararajan T, Das SK. Entropy generation due to flow and heat transfer in nanofluids. Int J Heat Mass Transf. 2010;53:4757–67. https://doi.org/10.1016/j.ijheatmasstransfer.2010.06.016.
Torabi M, Torabi M, Ghiaasiaan SM, Peterson GP. The effect of Al2O3-water nanofluid on the heat transfer and entropy generation of laminar forced convection through isotropic porous media. Int J Heat Mass Transf. 2017;111:804–16. https://doi.org/10.1016/j.ijheatmasstransfer.2017.04.041.
Mwesigye A, Huan Z. Thermodynamic analysis and optimization of fully developed turbulent forced convection in a circular tube with water-Al2O3 nanofluid. Int J Heat Mass Transf. 2015;89:694–706. https://doi.org/10.1016/j.ijheatmasstransfer.2015.05.099.
Ghasemi SE, Ranjbar AA. Thermal performance analysis of solar parabolic trough collector using nanofluid as working fluid: a CFD modelling study. J Mol Liq. 2016;222:159–66. https://doi.org/10.1016/j.molliq.2016.06.091.
Oullette WR, Bejan A. Conservation of available work (exergy) by using promoters of swirl flow in forced convection heat transfer. Energy. 1980;5:587–96.
Paoletti S, Rispoli F, Sciubba E. Calculation of exergetic losses in compact heat exchanger passages. ASME AES. 1989;10:21–9.
Pascale S, Gregory JM, Ambaum M, Tailleux R. Climate entropy budget of the HadCM3 atmosphere–ocean general circulation model and of FAMOUS, its low-resolution. Clim Dyn. 2010;10:125–39.
Vajjha RS. Measurements of thermophysical properties of nanofluids and computation of heat transfer characteristics. University of Alaska Fairbanks; 2008.
Lajos K. International news No uvelles in terna tionales. 1979;56–7.
Al-Ansary H, Zeitoun O. Numerical study of conduction and convection heat losses from a half-insulated air-filled annulus of the receiver of a parabolic trough collector. Sol Energy. 2011;85:3036–45. https://doi.org/10.1016/j.solener.2011.09.002.
Bellos E, Tzivanidis C, Tsimpoukis D. Thermal enhancement of parabolic trough collector with internally finned absorbers. Sol Energy. 2017;157:514–31. https://doi.org/10.1016/j.solener.2017.08.067.
Vajjha RS, Das DK. Experimental determination of thermal conductivity of three nanofluids and development of new correlations. Int J Heat Mass Transf. 2009;52:4675–82. https://doi.org/10.1016/j.ijheatmasstransfer.2009.06.027.
Sahoo BC. Measurement of rheological and thermal properties and the freeze-thaw characteristics of nanofluids. University of Alaska Fairbanks; 2008.
Koo J, Kleinstreuer C. A new thermal conductivity model for nanofluids. J Nanoparticle Res. 2004;6:577–88.
Vajjha RS, Das DK, Kulkarni DP. Development of new correlations for convective heat transfer and friction factor in turbulent regime for nanofluids. Int J Heat Mass Transf. 2010;53:4607–18. https://doi.org/10.1016/j.ijheatmasstransfer.2010.06.032.
Mwesigye A, Meyer JP. Optimal thermal and thermodynamic performance of a solar parabolic trough receiver with different nanofluids and at different concentration ratios. Appl Energy. 2017;193:393–413. https://doi.org/10.1016/j.apenergy.2017.02.064.
Menbari A, Alemrajabi AA, Rezaei A. Heat transfer analysis and the effect of CuO/Water nanofluid on direct absorption concentrating solar collector. Appl Therm Eng. 2016;104:176–83. https://doi.org/10.1016/j.applthermaleng.2016.05.064.
Author information
Authors and Affiliations
Corresponding authors
Rights and permissions
About this article
Cite this article
Mohseni-Gharyehsafa, B., Ebrahimi-Moghadam, A., Okati, V. et al. Optimizing flow properties of the different nanofluids inside a circular tube by using entropy generation minimization approach. J Therm Anal Calorim 135, 801–811 (2019). https://doi.org/10.1007/s10973-018-7276-x
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s10973-018-7276-x