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研究生: 黃詩惠
Huang, Shih-Hui
論文名稱: 氧化鋁/相變化奈米流體分流於同心雙圓管流道內管/外環之強制對流熱傳遞增益特性研究
On forced convection heat transfer enhancement efficacy of concurrent flows of Al2O3/PCM nanofluids through inner tube/outer annulus of a concentric double-tube duct
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: 2021
畢業學年度: 109
語文別: 中文
論文頁數: 193
中文關鍵詞: 同心雙圓管 、奈米流體 、奈米乳液 、相變化材料 、層流強制對流
外文關鍵詞: Concentric double tube, Alumina nanofluid, Nano-PCM emulsion, Phase change material, Laminar forced convection
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  • 本文採用數值模擬與實驗並行探討在等熱通量下流體通入同心雙圓管之強制對流層流中的熱傳遞現象與增益,在數值模擬的部分會先輸入入口溫度、總流量、流量比與加熱功率等參數後進行模擬並針對熱阻的結果進行分析,其中發現同心雙管的熱傳機制主要由外環流體帶走熱能,故設計以下實驗參數比較討論:改變加熱功率120W、160W和200W及總雷諾數800、1300和1700,並調控六個流量比為:0.1、0.286、0.454、1.0、1.6、2.38。此外,也藉由改變工作流體之熱物理性質,實現降低整體軸向與徑向熱阻值,進而增加熱傳增益,例如:外環以擁有高熱傳係數之 及 奈米流體代替純水,內管則以 奈米乳液代替純水,藉由其相變化過程增加熱散逸及降低壁溫。同心雙管之材料與尺寸如下:外管管材為無氧紅銅管,外管外徑為6mm,外管內徑為5.4mm,總長為1250mm;內管管材為不銹鋼管,內管外徑為4.6mm,內管內徑為4.2mm,總長為2060mm。
    在同心雙管實驗結果可得外環為 奈米流體內管為純水因熱物理性質與散熱機制的關係並無明顯的增益,但當外環奈米流體濃度提升至 後,其平均熱傳增益在總雷諾樹為1700、加熱功率為200W且流量比在2.38時有12.63%的增益,而外環為 奈米流體內管為 奈米乳液則因內管流體潛熱的發揮提升了整體熱傳對流效果使其擁有最大平均熱傳增益16.5%,且與單管比較也有最大熱傳增益27.7%,而在壓降增幅的結果來看不論是改變工作流體還是流道從單管轉變成同心雙管的架構所增加的壓降都過大,以至於效能指標都偏低,不過單從熱傳增益的部分機能性流體除了外環為 奈米流體內管為純水外,都有不錯的收穫。

    This paper uses numerical simulation and experiments to discuss the heat transfer phenomenon and enhance efficacy in forced convection laminar flow. The fluid passes through the concentric double circular tube under equal heat flux. In the part of numerical simulation, the results of thermal resistance are going to be analyzed after input the initial parameters, such as the inlet temperature, the total flow rate, the ratio of flow rate, and the heater power. It is found that the heat transfer mechanism of the concentric double-tube duct is mainly taken away by the fluid in outer tube. The following experimental conditions including the heater power (120W, 160W, 200W), the total Reynolds numbers( 800, 1300, and 1700), and the flow rate ratio of outer tube over inner tube (0.1, 0.286, 0.454, 1.0, 1.6, 2.38) are used to explore and discuss. In addition, improving the thermophysical properties of the working fluid not only reduces the overall axial and radial thermal resistance but also increases the heat transfer effect.
    Therefore, choosing nanofluid of volume concentration of 0.5 percent or 1.0 percent and a weight concentration of 4.63 percent nano-emulsion as working fluids can improve high heat transfer conductivity and the latent heat mechanism, thus increase the heat transfer effectivity. The heat exchanger was made of concentric tubes with the following dimensions: inner and outer diameters of stainless-steel tube were 4.2mm and 4.6mm, respectively; inner and outer diameters of the oxygen-free copper tube were 5.4mm and 6mm, respectively. The total length of the inner and outer tubes was 2060mm and 1250mm.
    Based on the experimental results, the working fluid combination of 0.5% nanofluid and the pure water in the outer annulus, as well as the inner tube, does not have a significant gain because of the thermophysical properties and the heat dissipation mechanism. For the specified condition of total Reynolds is 1700, the heating power is 200W, and the ratio of flow rate is 2.38, nanofluid of the concentration increases to 1.0 percent in the outer annulus, the average heat transfer has 12.63% improvement. Further, using 4.63% nano-emulsion to replace the pure water in the inner tube show that the maximum average heat transfer improvement compared with the pure water and the single pipe were 16.5% and 27.7%, respectively. However, the figure of merit (FOM) is low because the viscosity of the functional fluid and the flow channel structure cause the pressure drop dramatically increases as well as the increment of the heat transfer is relatively low. Although concentric double tube will cause a significant loss of pressure drop, using functional fluid or modifying the flow channel structure still has good harvests for heat transfer efficiency.

    摘要 III 英文摘要 IV 致謝 XXI 目錄 XXII 表目錄 XXV 圖目錄 XXVI 符號說明 XXXVIII 第一章 緒論 1 1-1前言 1 1-2文獻回顧 1 1-3研究動機 6 1-4 論文架構 6 第二章 物理模型與數值模擬方法 7 2-1物理模型 7 2-2數學模型 8 2-2-1統御方程式 8 2-2-2邊界條件 10 2-2-3無因次變數定義 12 2-2-4無因次統御方程式及邊界條件 13 表2-1計算Biot數之相關係數 15 2-2-5工作流體熱物理性質 16 2-3數值方法 19 2-3-1程式解題流程 20 2-3-2網格測試 21 2-4相關熱傳特性參數定義 22 第三章 實驗方法與數據處理 33 3-1實驗設計 33 表3-1 內外管不同工作流體之組合 33 3-2實驗迴路 34 3-3實驗步驟 37 3-4奈米流體和奈米乳液的調配與熱物性質量測 38 表3-2 奈米顆粒之物性表 38 3-4-1奈米流體的調配 38 3-4-2奈米相變化乳液的調配 39 3-4-3熱物理性質之量測 40 表3-3 不同溫度下純水與奈米流體之熱物性質表 52 3-5數據處理 53 3-6不準度分析 63 表3-4 實驗參數誤差分析表 64 表3-4 實驗誤差分析表(續) 65 第四章 同心雙圓管—使用機能性流體替代純水之效益評估66 4-1 數值模擬結果 66 4-2實驗結果 73 4-2-1無因次外環內壁壁溫分布 73 4-2-2 內管載熱比 74 4-2-3熱點壓抑增益 75 4-2-4加熱面均勻度指標 76 表4-1 實驗參數表(圖4-25) 96 4-2-5局部與平均熱傳增益 100 表4-2 實驗參數表 (圖4-41) 116 表4-3 實驗參數表(圖4-42) 117 4-2-6熱傳遞性能效益指標 118 4-3總結 119 第五章 比較同心雙管與單管間的熱傳效益 137 5-1雙管與單管之局部對流熱傳係數與熱傳增益 138 5-2雙管與單管之平均熱傳增益 139 5-3雙管與單管之壓降比 169 5-4局部熱傳遞性能效益指標 170 5-5總結 170 第六章 結論與未來發展 188 6-1結論 188 6-1-1 同心雙管 188 6-1-2 同心雙管與單管之比較 189 6-2未來研究方向與發展 190 參考文獻 191

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