簡易檢索 / 詳目顯示

研究生: 張純
Jang, Chwen
論文名稱: 水平矩形容器內含相變化微粒懸浮液體 自然對流熱傳特性之探討
Natural Convection Heat Transfer Characteristics of Phase-Chang-Material Suspensions in a Horizontal Rectangular Enclosure
指導教授: 何清政
Ho, Ching-Jenq
學位類別: 碩士
Master
系所名稱: 工學院 - 機械工程學系
Department of Mechanical Engineering
論文出版年: 2002
畢業學年度: 90
語文別: 中文
論文頁數: 88
中文關鍵詞: 相變化自然對流
外文關鍵詞: natural convection, PCM
相關次數: 點閱:81下載:4
分享至:
查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報
  • 本文主要為藉由數值模擬的方法來探討水平矩形容器內含相變化微粒懸浮液體之二維自然對流熱傳特性,所探討之物理模型為一底部加熱及上部冷卻的水平矩形容器,且左右直立邊界為絕熱壁。數值模擬考慮之主要參數範圍為:萊利數 = 1000、2000、5000、7000、10000;史蒂芬數Ste = 0.01、0.05、0.005;次冷參數Sb = 0、0.5、1.0、10;初始濃度cm,i =0 %、3 %、5 %、10 %、20 %;PCM微粒無因次粒徑Dp = 5×10 -4,容器高寬比AR =1,普蘭特數Pr = 15,路易士數Le=3.2×10 5,過冷參數 ,PCM微粒時間延遲參數 ,質熱傳浮力比N=1。本文著重於萊利數、史蒂芬數、次冷參數及初始濃度對容器內添加PCM懸浮微粒自然對流熱傳遞影響。結果顯示出添加PCM微粒可以使得容器內產生自然對流之臨界萊利數大幅降低,尤其隨PCM微粒濃度之提高而下降。此外,本文結果顯示加入PCM懸浮微粒可以有效的提升水平矩形容器之自然對流熱傳率。隨著PCM微粒濃度的增加或史蒂芬數之降低,容器之熱傳率可較純流體顯著提升至67%。次冷參數主要是控制相變化區域的分佈以及PCM微粒融點等溫線的相對於冷壁之位置。

    This thesis is to investigate numerically natural convection heat transfer characteristics of phase-change-material suspensions in a two dimension horizontal rectangular enclosure. The horizontal rectangular enclosure is heated from the bottom and cooled from the top, while the vertical side walls are assumed adiabatic. The numerical simulations have been conducted for the dimensionless parameters in the following range : ( Rayleigh number) = 1000,2000,5000,7000,10000; Ste ( Stefan number) = 0.01,0.05,0.005; Sb ( Subcooling factor ) = 0,0.5,1.0,10; cm,i( initial concentration ) = 0 % , 3 % , 5 % , 10 % , 20 %. Dp ( dimensionless PCM particle diameter ) = 5×10 –4; AR =1; Pr( Prandtl number ) = 15;Le( Lewis number )=3.2×10 5; ;N( buoyancy ratio ) = 1. The numerical results are presented to emphasize the parameter effects of the Rayleigh number, thre Stefan number, the Subcooling factor and the initial concentration of PCM particles on heat transfer in a horizontal rectangular enclosure. The result show that critical Rayleigh numbers for the onset of natural convection of the PCM suspension in the enclosure are substantially lower then those for the pure fluid. Furthermore, the heat transfer rates of PCM suspension through the horizontal enclosure are found to be considerably enhanced in comparison with those of the pure fluid. Increase of the initial concentration on decrease of the Stefan number can lead to considerable enhancement in heat transfer rate ( about 20~170% ) through the PCM suspension in the enclosure.

    中文摘要 ………………………………………….. I 英文摘要 ………………………………………….. II 誌謝 ………………………………………….. III 總目錄 ………………………………………….. IV 圖目錄 ………………………………………….. VII 表目錄 ………………………………………….. XII 符號說明 ………………………………………….. XIV 第一章 緒 論 ………………………………………….. 1 1-1 研究動機 ………………………………………….. 1 1-2 文獻回顧 ………………………………………….. 2 1-3 本文架構 ………………………………………….. 3 第二章 理論分析與數值方法 ………………………………………….. 4 2-1 物理模型 ………………………………………….. 4 2-2 數學模式 ………………………………………….. 5 2-3紐賽數定義 ………………………………………….. 11 2-4 數值方法 ………………………………………….. 12 2-4-1 網格系統 ………………………………………….. 12 2-4-2 方程式之離散 ………………………………………….. 13 2-4-3 解題步驟 ………………………………………….. 16 2-5 數值方法之驗證 ………………………………………….. 19 2-6 收斂測試 ………………………………………….. 20 2-6-1 網格收斂測試 ………………………………………….. 20 2-6-2 時間前進步伐測試 ………………………………………….. 23 第三章 結果與討論 ………………………………………….. 26 3-1臨界萊利數之探討 ………………………………………….. 27 3-2暫態自然對流現象之演變 ………………………………………….. 31 3-3各參數對穩態自然對流之影響 ………………………………...……. 37 3-3-1萊利數對穩態自然對流之影響………………….……………….. 37 3-3-2初始濃度對穩態自然對流之影響……………….……………….. 40 3-3-3次冷參數對穩態自然對流之影響………………….……….….. 45 3-3-4史蒂芬數數對穩態自然對流之影響………………….……….….. 48 3-4震盪自然對流 ………………………………...……. 56 3-5高潛熱效應及高萊利數下之震盪流場 ……………………………….. 72 3-6 穩態自然對流與震盪自然對流之剖析 ………………………………... 66 3-7 熱傳結果 ………………………………………….. 68 3-7-1初始濃度對熱傳率之影響…………………………………….. 68 3-7-2次冷參數對熱傳率之影響………………………………………….. 71 3-5-3史蒂芬數對熱傳現象之影響……………………………………… 73 第四章 結論與建議 ……………………………….. 76 4-1 結論 ……………………………….. 76 4-2 對未來研究之建議 ……………………………….. 78 參考文獻 ……………………………….. 79 附錄 ……………………………….. 81 自述 ……………………………….. 87

    【1】 Kasza, K. E. and Chen, M. M., “Improvement of the Performance of Solar Energy or Waste Heat Utilization Systems by Using Phase-Chang Slurry as an Enhanced Heat –Transfer Storage Fluid ”, ASME J. Solar Energy Engineering, Vol. 107, pp. 229-236, 1985.
    【2】 Katz, L.,”Natural Convection Heat Transfer with Fluids Using Suspended Particles which Undergo Phase Change”, Ph.D. Dissertation, Massachusetts Institute of Technology, Cambridge, Massachusetts, 1967.
    【3】 Datta, P., Sengupta, S. and Roy, S. K., “Natural Convection Heat Transfer in an Enclosure with Suspensions of Microencapsulated Phase Change Materials”, ASME, HTD, Vol.204, pp. 100-116, 1992.
    【4】 Harhira, M., Roy, S. K. and Sengupta, S., “Natural Convection Heat Transfer from a Vertical Flat Plate with Phase Change Material Suspensions”, Enhan. Heat Transfer, Vol. 4, pp. 17-34, 1996.
    【5】 黃朝揚, “矩形容器內含懸浮相變化微粒之自然對流研究”,國立成功大學機械工程研究所碩士論文,2001。
    【6】 Tannehill, J. C. and Anderson D.A, and Pletcher, R. H., “Computation Fluid Mechanics And Heat Transfer”, Taylor & Francis, 1978
    【7】 Soong, C. Y. and Tzeng, P. Y., “Numerical Study on Model-Transition of Natural Convection in Differentially Heated Inclined Enclosures”, Int. J. Heat Mass Transfer, Vol. 39, pp. 2869-2882.
    【8】 Tzeng, P. Y., Soong, C. Y., and Sheu, T. S. “Numerical Investigation of Transient Flow-Mode Transition of Laminar Natural Convection in an Inclined Enclosure”, Numerical Heat Transfer, Part A, Vol. 31, pp. 193-206, 1997.
    【9】 夏志豪, “矩形容器內含懸浮相變化微粒之自然對流熱傳之數值模擬”,國立成功大學機械工程研究所碩士論文,2000。
    【10】 何泰安, “矩形容器內含懸浮相變化微粒之自然對流熱傳特性實驗研究”,國立成功大學機械工程研究所碩士論文,1999。
    【11】 Soong, C. Y., Tzeng, P. Y., and Hsieh, C.D. “Numerical Study of Bottom-Wall Temperature Modulation Effect on Thermal Instability and Oscillatory Cellular Convection in a Rectangular Enclosure”, Int. J. Heat and Mass Transfer, Vol. 44, pp. 3855-3868, 2001.

    下載圖示 校內:立即公開
    校外:2002-07-25公開
    QR CODE