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請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/52619
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor潘國隆
dc.contributor.authorChih-Wei Hsiehen
dc.contributor.author謝志偉zh_TW
dc.date.accessioned2021-06-15T16:20:38Z-
dc.date.available2018-09-17
dc.date.copyright2015-09-17
dc.date.issued2015
dc.date.submitted2015-08-17
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[59] 邱明峻, '生質柴油與柴油混合醇類於微重力場下燃燒研究,' 國立台灣大學機械工程學研究所碩士論文, 2010.
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[61] 張凱捷, “雙組份生質柴油、生質油料與柴油液滴燃燒行為之觀察” 國立台灣大學機械工程學研究所碩士論文, 2012.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/52619-
dc.description.abstract本研究以生質柴油預混醇類(甲醇、乙醇、異丙醇)液滴利用落塔(drop tower)的自由落體方式達到微重力燃燒,在此環境下浮力的影響可被忽略,液滴燃燒將呈現球對稱火焰。不同直徑大小液滴(0.38 mm、0.5 mm)透過液滴產生器產生並靜置在兩條陶瓷纖維線交叉的中心點,再置入燃燒室內以電熱絲點火進行實驗。液滴之後將經歷0.68秒的微重力過程,並在落下期間利用攝影機觀察其燃燒現象。除了落塔的實驗外,本實驗也透過數值計算的方式模擬雙組份生質柴油與異丙醇液滴的燃燒,希望藉此驗證實驗的燃燒結果。由於生質柴油與醇類的混合液滴點燃後會發生機率性的微爆(microexplosion),其燃燒趨勢將與不發生微爆的燃燒完全不同,而大部分的文獻都呈現微爆的結果。前人雖有完成不發生微爆的燃燒,但所呈現的燃燒趨勢並不明顯,且在混合液滴具有高重量百分比的醇類時(>45%)無法完成燃燒不具有微爆的結果,因此本文的重點為了解微爆現象發生的原因、解決微爆的問題以及研究非微爆的液滴燃燒。
實驗發現內部不均勻現象(nonhomogeneity)為導致微爆發生的原因,當其出現於液滴內部時,受熱後會被汽化膨脹,撐破液滴表面並直接導致微爆。內部不均勻物的發生與相對濕度並無明顯的關聯,而與醇類及生質柴油間互溶現象有關。微爆的發生為機率性,小尺寸液滴(0.38 mm)微爆機率較小,而大尺寸液滴(0.5 mm)發生微爆機率高,不過兩者皆在醇類與生質柴油組分比1:1的情況下機率最高。醇類加入生質柴油液滴有助於增加其燃燒速率,在不微爆時,混合液滴在醇類重量百分比25%時達到最高;在微爆狀況下,則在50%時因微爆最劇烈而使平均燃燒速率最高。整體而言,重量百分比25%的甲醇在所有的組份中具有最高的燃燒速率,但其燃燒速率在過了此組分之後會隨著甲醇組分比增加而劇烈下降,而異丙醇混合液滴燃燒速率下降的趨勢則相對最緩。
zh_TW
dc.description.abstractIn the present work, combustion of a multi-component droplet, blended with biodiesel and alcohol (methanol, ethanol and 2-propanol, respectively), was studied in a gravity-reduced environment. A “drop tower” facility was utilized to achieve the microgravity condition, and the falling time was about 0.68 s. Droplets of different sizes, i.e., 0.5 mm and 0.38 mm in diameter, respectively, were initially produced by a droplet generator. They were suspended at the crossing point of two ultra-thin fibers and ignited by a pair of electrical hot wires. The droplets then underwent a convection-free combustion, leading to formation of spherically symmetric flame. It was found that the existence of internal inhomogeneity directly contributed to occurrence of microexplosion. Via observation by using a CCD camera, explosion was yielded when a bubble was heated during the burning period to sufficiently high temperature. Furthermore, influence of different relative humidity of the environment was tested. The results revealed its little relevance to the formation of inhomogeneity in the droplet that was suspected to be caused by absorption of water on the surface. The stochastic nature of microexplosion was then found to correlate with the size of droplets, with a lower possibility of explosion in smaller ones. The maximum frequency occurred at 50% mass fraction of alcohol in all sizes of droplets, resulting in the corresponding highest averaged burning rate in the same proportion. In the meantime, the addition of alcohol into biodiesel showed significant enhancement of burning rate in the cases without explosion, with largest increment created when the mixture included 25% alcohol.en
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Previous issue date: 2015
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dc.description.tableofcontents目錄
誌謝 i
摘要 ii
Abstract iii
符號說明 iv
目錄 vii
圖目錄 xi
表目錄 xv
第一章 前言 - 1 -
1.1簡介 - 1 -
1.2文獻回顧 - 3 -
1.2.1 微重力下燃燒的方法 - 3 -
1.2.2 點火方式對燃燒影響 - 6 -
1.2.3 重力與微重力對於點火延遲的影響 - 6 -
1.2.4 懸掛線對於燃燒的影響 - 7 -
1.2.5 液滴大小與環境溫度的關係 - 7 -
1.2.6 碳微粒對於熱傳影響 - 8 -
1.2.7 醇類燃燒現象 - 9 -
1.2.8 多組分液滴燃燒現象 - 10 -
1.2.9微爆現象 - 12 -
1.3 研究動機 - 12 -
1.4 研究目的 - 13 -
第二章 基礎理論 - 14 -
2.1 球對稱燃燒理論 - 14 -
表2-1 d2-law基本假設 - 17 -
2.2 碳微粒(soot)形成 - 20 -
2.3 燃油分子於氣相中停留時間(residence time) - 22 -
2.4 點火延遲 - 23 -
2.5 多組份液滴燃燒現象 - 23 -
2.6 多組分液滴內部成核現象 - 27 -
2.7 生質柴油介紹 - 28 -
2.8 g-level評估 - 30 -
2.9 阻力箱與drop package之高度差 - 30 -
第三章 實驗方法 - 33 -
3.1 實驗設備 - 33 -
3.1.1 落塔 - 34 -
3.1.2 drop shield & drop package - 39 -
3.1.3 電子控制系統 - 46 -
3.1.4 電腦控制系統 - 48 -
3.1.5 影像處理系統 - 49 -
3.2 實驗儀器較正與分析 - 50 -
3.2.1 液滴產生器穩定性分析 - 50 -
表3-1 液滴產生器穩定性分析 - 51 -
3.2.2 電熱絲增溫對於液滴尺寸影響分析 - 51 -
3.2.3 於自由落體過程中時液滴穩定性分析 - 52 -
3.2.4 控制系統設定 - 52 -
3.2.5影像與實際尺寸校正 - 53 -
3.3 實驗步驟與流程 - 55 -
3.4 影像處理 - 56 -
3.5誤差分析 - 60 -
3.5.1 液滴直徑於重力與微重力環境下的誤差分析 - 60 -
3.5.2 不同組分液滴直徑誤差分析 - 61 -
表3-2 不同組分液滴直徑誤差分析 - 61 -
3.5.3 照片時間間距誤差 - 61 -
3.5.4 影像量測誤差 - 62 -
3.5.5 熱傳誤差 - 62 -
3.5.6 燃燒速率量測誤差 - 63 -
3.6 燃燒速率定義 - 63 -
3.7 實驗工作條件 - 65 -
3.8 計算模型方法(The computational model) - 66 -
3.8.1 計算理論 - 66 -
3.8.2 混合液滴性質 - 70 -
3.8.3 計算方法 - 70 -
3.8.4 實驗條件 - 71 -
第四章 結果與討論 - 72 -
I. 燃燒現象 - 72 -
4.1純油料燃燒現象觀察 - 72 -
4.1.1 生質柴油燃燒現象 - 72 -
4.1.2 醇類燃燒現象 - 74 -
4.2 純油料燃燒速率分析 - 76 -
4.3 雙組分液滴燃燒現象 - 79 -
II. 微爆現象 - 81 -
4.4 內部不均勻現象討論 - 81 -
4.4.1 不均勻物的形成過程 - 81 -
4.4.2 相對濕度對於不均勻物的影響 - 83 -
4.4.3 懸線大小與不均勻物的影響 - 84 -
4.4.4 雙組分液體間之互溶程度 - 85 -
4.4.5 液滴大小與不均勻物之關係 - 88 -
表4-1液滴透過0.13 mm及0.61 mm的噴嘴產生內部發生不均勻現象機率 - 91 -
4.5 微爆種類與燃燒速率量測 - 91 -
4.6微爆機率與液滴大小關係 - 94 -
III. 雙組分液滴燃燒速率分析 - 96 -
4.7雙組分混合液滴燃燒速率分析 - 96 -
4.8 前人比較 - 102 -
IV. 數值分析 - 105 -
4.9 計算結果 - 105 -
第五章 結論 - 108 -
5.1 結論 - 108 -
5.2 研究貢獻 - 110 -
5.3 未來展望與建議 - 110 -
參考文獻 - 111 -
附錄 - 116 -
附錄表一 陶瓷纖維性質表 - 116 -
附錄表二 生質柴油之特性表 - 116 -
dc.language.isozh-TW
dc.subject微爆zh_TW
dc.subject微重力zh_TW
dc.subject液滴燃燒zh_TW
dc.subject生質柴油zh_TW
dc.subject醇類zh_TW
dc.subjectmicrogravityen
dc.subjectmicroexplosionen
dc.subjectalcoholen
dc.subjectbiodieselen
dc.subjectdroplet combustionen
dc.title雙組份生質柴油與醇類液滴於微重力下燃燒與微爆現象之研究zh_TW
dc.titleOn the combustion and the microexplosion of biodiesel/alcohol droplet in microgravityen
dc.typeThesis
dc.date.schoolyear103-2
dc.description.degree碩士
dc.contributor.oralexamcommittee王興華,王安邦,林成原
dc.subject.keyword微重力,液滴燃燒,生質柴油,醇類,微爆,zh_TW
dc.subject.keywordmicrogravity,droplet combustion,biodiesel,alcohol,microexplosion,en
dc.relation.page117
dc.rights.note有償授權
dc.date.accepted2015-08-17
dc.contributor.author-college工學院zh_TW
dc.contributor.author-dept機械工程學研究所zh_TW
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