دانشگاه تربیت دبیر شهید رجائی
انتشارات دانشگاه تربیت دبیر شهید رجائی

  اخبار و اعلانات

 آمار

تعداد نشریات11
تعداد شماره‌ها210
تعداد مقالات2,098
تعداد مشاهده مقاله2,877,503
تعداد دریافت فایل اصل مقاله2,085,310
Madani, Seyed Mostafa, Alinejad, Javad, Rostamiyan, Yasser, Fallah, Keivan. (1402). Lattice Boltzmann simulation inside a cavity: The effect of pipe profile on natural convection. فناوری آموزش, 13(1), 67-74. doi: 10.22061/jcarme.2023.9454.2270
Seyed Mostafa Moafi Madani; Javad Alinejad; Yasser Rostamiyan; Keivan Fallah. "Lattice Boltzmann simulation inside a cavity: The effect of pipe profile on natural convection". فناوری آموزش, 13, 1, 1402, 67-74. doi: 10.22061/jcarme.2023.9454.2270
Madani, Seyed Mostafa, Alinejad, Javad, Rostamiyan, Yasser, Fallah, Keivan. (1402). 'Lattice Boltzmann simulation inside a cavity: The effect of pipe profile on natural convection', فناوری آموزش, 13(1), pp. 67-74. doi: 10.22061/jcarme.2023.9454.2270
Madani, Seyed Mostafa, Alinejad, Javad, Rostamiyan, Yasser, Fallah, Keivan. Lattice Boltzmann simulation inside a cavity: The effect of pipe profile on natural convection. فناوری آموزش, 1402; 13(1): 67-74. doi: 10.22061/jcarme.2023.9454.2270

Lattice Boltzmann simulation inside a cavity: The effect of pipe profile on natural convection

Journal of Computational & Applied Research in Mechanical Engineering (JCARME)
مقاله 6، دوره 13، شماره 1 - شماره پیاپی 25، آذر 2023، صفحه 67-74    اصل مقاله (804.7 K)
نوع مقاله: Research Paper
شناسه دیجیتال (DOI): 10.22061/jcarme.2023.9454.2270
نویسندگان
Seyed Mostafa Moafi Madani؛ Javad Alinejad* ؛ Yasser Rostamiyan؛ Keivan Fallah
Department of Mechanical Engineering, Sari Branch, Islamic Azad University, Sari, Iran
تاریخ دریافت: 12 آذر 1401،  تاریخ بازنگری: 04 اردیبهشت 1402،  تاریخ پذیرش: 09 اردیبهشت 1402 
چکیده
In the present study, the effect of the heating pipe profile on natural convection in a two-phase fluid inside a cavity has been investigated. This geometry has been simulated with the LB Method based on the D2Q9 model for analyzing stream lines, dimensionless velocity field of fluid flow, solid particles volume fraction, temperature arrangement, and Nusselt number. These parameters have been studied in three different cases of the cavity. The results are signified by changing the geometry from a horizontal ellipse to a circular one and a vertical ellipse;the maximum particle volume fraction is decreased. Also, by changing the geometry from a horizontal ellipse to a circular and vertical ellipse, larger velocity vectors have been formed around the geometry. The Nusselt number variations of circular and  vertical ellipse geometries are from 90⁰ to 270⁰. The Nusselt number variation of horizontal ellipse geometry is negligible from 90⁰ to 270⁰.  Also, the Nusselt number of the circular geometry is larger than the other geometries from 270⁰ to 90⁰. The highest average Nusselt number belongs to circular, vertical and horizontal ellipse geometries, respectively.
کلیدواژه‌ها
Lattice Boltzmann model؛ Fuel heating؛ Particle Volume Fraction؛ two–phase fluid؛ natural convection
اصل مقاله

[1] J. Esfahani and J. Alinejad, "Lattice Boltzmann simulation of viscous-fluid flow and conjugate heat transfer in a rectangular cavity with a heated moving wall," Thermophysics and AeromechanicsVol. 20, No. 5, pp. 613-620, (2013).

[2] J. Esfahani and J. Alinejad, "Entropy Generation of Conjugate Natural Convection in Enclusures: The Lattice Boltzmann Method," J. Thermophys Heat Transfer, Vol. 27, pp. 498-505, 07/01 (2013).

[3] J. Alinejad and J. A. Esfahani, "Lattice Boltzmann simulation of forced convection over an electronic board with multiple obstacles," Heat Transfer Res., Vol. 45, No. 3, pp. 241-262, (2014).

[4] J. Alinejad and J. Abolfazli Esfahani, "Numerical Stabilization of Three-Dimensional Turbulent Natural Convection Around Isothermal Cylinder," J. Thermophys Heat Transfer, Vol. 30, No. 1, pp. 94-102, (2016).

[5] J. Alinejad and J. Esfahani, "Lattice Boltzmann simulation of EGM and solid particle trajectory due to conjugate natural convection," Aerospace Sci Technol; Vol. 4. No. 1, pp. 36–43. (2016).

[6] J. Alinejad and K. Fallah, "Taguchi Optimization Approach for Three-Dimensional Nanofluid Natural Convection in a Transformable Enclosure," J. Thermophys Heat Transfer, Vol. 31, No. 1,  pp. 1-7 (2016).

[7] J. Alinejad and J. A. Esfahani, "Taguchi design of three dimensional simulations for optimization of turbulent mixed convection in a cavity," Meccanica,Vol. 52, No. 4, pp. 925-938, (2017).

[8] M. M. Peiravi, J. Alinejad, D. Ganji, and S. Maddah, "Numerical study of fins arrangement and nanofluids effects on three-dimensional natural convection in the cubical enclosure," Challenges in Nano and Micro Scale Science and Technology, Vol. 7, No. 2, pp. 97-112, (2019).

[9] M. M. Peiravi and J. Alinejad, "Hybrid conduction, convection and radiation heat transfer simulation in a channel with rectangular cylinder," J. therm. anal. calorim,Vol. 140, No. 6, pp. 2733-2747, (2020).

[10] M. M. Peiravi, J. Alinejad, D. D. Ganji, and S. Maddah, "3D optimization of baffle arrangement in a multi-phase nanofluid natural convection based on numerical simulation," Int. j . Numer. Methods Heat  Fluid Flow, Vol. 30, No. 5, pp. 2583-2605, (2019).

[11] Y. Wang, Z. Yuan, Y. Liang, Y. Xie, X. Chen, and X. Li, "A review of experimental measurement and prediction models of crude oil fouling rate in crude refinery preheat trains," Asia‐Pac. J. Chem. Eng.,Vol. 10, No. 4, pp. 607-625, (2015).

[12] M. Haghshenasfard and K. Hooman, "CFD modeling of asphaltene deposition rate from crude oil," Journal of Petroleum Science and Engineering, Vol. 128, pp. 24-32, (2015).

[13] S. D. He and B. Wang, "Dispersion of particles in wall-bounded particle-laden turbulent flows with high wall permeability," Int. j. Multiph. Flow, Vol. 77, No. 4, pp. 104-119, (2015).

[14] P. Kor and R. Kharrat, "Modeling of asphaltene particle deposition from turbulent oil flow in tubing: Model validation and a parametric study," Petroleum, Vol. 2, No. 4, pp. 393-398, (2016).

[15] H. Seyyedbagheri and B. Mirzayi, "CFD modeling of high inertia asphaltene aggregates deposition in 3D turbulent oil production wells, Journal of Petroleum Science and Engineering",Vol. 150, pp. 257-264, (2017).

[16] S. Emani, M. Ramasamy, and K. Z. K. Shaari, "CFD modelling of shell-side asphaltenes deposition in a shell and tube heat exchanger," in AIP Conference Proceedings, Vol. 1859, No. 1: AIP Publishing LLC, p. 020118, (2017).

[17] M. M. Peiravi and J. Alinejad, "Nano particles distribution characteristics in multi-phase heat transfer between 3D cubical enclosures mounted obstacles," Alexandria eng. j., Vol. 60, No. 6, pp. 5025-5038, (2021).

[18] M. A. Abbassi, M. R. Safaei, R. Djebali, K. Guedri, B. Zeghmati, and A. A. Alrashed, "LBM simulation of free convection in a nanofluid filled incinerator containing a hot block," Int. J. Mech. Sci., Vol. 144, pp. 172-185, (2018).

[19] M. R. Safaei, A. Karimipour, A. Abdollahi, and T. K. Nguyen, "The investigation of thermal radiation and free convection heat transfer mechanisms of nanofluid inside a shallow cavity by lattice Boltzmann method," Physica A, Vol. 509, pp. 515-535, (2018).

[20] M. Goodarzi, A. D’Orazio, A. Keshavarzi, S. Mousavi, and A. Karimipour, "Develop the nano scale method of lattice Boltzmann to predict the fluid flow and heat transfer of air in the inclined lid driven cavity with a large heat source inside, Two case studies: Pure natural convection & mixed convection," Physica A, Vol. 509, pp. 210-233, (2018).

[21] X. Zhou, F. Chi, Y. Jiang, and Q. Chen, "Numerical investigation of thermocapillary convection instability for large Prandtl number nanofluid in rectangular cavity," Int. Commun. Heat Mass Transfer, Vol. 133, p. 105956, (2022).

[22] H. Shaker, M. Abbasalizadeh, S. Khalilarya, and S. Yekani Motlagh, "Two-phase modeling of the effect of non-uniform magnetic field on mixed convection of magnetic nanofluid inside an open cavity, " Int. J. Mech. Sci, (2021).

[23] X. Zhang, L. Wang, and D. Li, "Lattice Boltzmann simulation of natural convection melting in a cubic cavity with an internal cylindrical heat source," Int. J. Therm. Sci, vol. 165, p. 106917, (2021).

[24] M. Rajarathinam, N. Nithyadevi, and A. J. Chamkha, "Heat transfer enhancement of mixed convection in an inclined porous cavity using Cu-water nanofluid," Adv. Powder Technol., Vol. 29, No. 3, pp. 590-605, (2018).

[25] A. Alsabery, M. Sheremet, A. Chamkha, and I. Hashim, "Conjugate natural convection of Al2O3–water nanofluid in a square cavity with a concentric solid insert using Buongiorno’s two-phase model, " Int. J. Mech. Sci, Vol. 136, pp. 200-219, (2018).

[26] E. Jamesahar, M. Ghalambaz, and A. Chamkha, "Fluid–solid interaction in natural convection heat transfer in a square cavity with a perfectly thermal-conductive flexible diagonal partition," Int. J. Heat Mass Transfer,Vol. 100, pp. 303-319, (2016).

[27] M. Ahmed and M. Eslamian, "Natural convection in a differentially-heated square enclosure filled with a nanofluid: significance of the thermophoresis force and slip/drift velocity," Int. Commun. Heat Mass Transfer, Vol. 58, pp. 1-11, (2014).

آمار
تعداد مشاهده مقاله: 265
تعداد دریافت فایل اصل مقاله: 270


سامانه مدیریت نشریات علمی. طراحی و پیاده سازی از سیناوب