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研究生: 鍾志韓
Chung, Chih-Han
論文名稱: 獨立雙開口式二氧化鈦奈米管陣列製備及應用於可見光下光還原二氧化碳
Preparation of Free-Standing Open-Ended TiO2 Nanotube Array and Application in Photoreduction of CO2 under Visible Light
指導教授: 凌永健
Ling, Yong-Chien
口試委員:
學位類別: 碩士
Master
系所名稱: 理學院 - 化學系
Department of Chemistry
論文出版年: 2010
畢業學年度: 98
語文別: 中文
論文頁數: 84
中文關鍵詞: 光觸媒二氧化鈦奈米管陣列二氧化碳光還原
相關次數: 點閱:3下載:0
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  • 人類對於石化能源過度使用的結果,已導致大氣中二氧化碳(CO2)的濃度劇烈增加,造成全球暖化現象愈來愈嚴重,嚴重地影響氣候變遷,導致海平面上升,危害到整個生態環境。因此,對於減少大氣二氧化碳含量已是刻不容緩的事。此外,將二氧化碳捕捉下來,利用光觸媒將其還原成碳氫化合物再利用,不僅能減少大氣中的二氧化碳含量,也能開發出新能源的來源。
    本研究透過陽極氧化法,並藉有改變電壓方式,來製備出獨立雙開口式二氧化鈦奈米管陣列(open-ended TiNT),相對於一端封閉的奈米管陣列結構(close-ended TiNT)而言,此流通式奈米管結構,使反應物能更容易進到管柱內部,增加反應物接觸面積。此外,藉有尿素於高溫下會熱裂解產生氨氣,來將氮摻雜到二氧化鈦晶格中(ON-TiNT),進而修飾觸媒能隙以增加對可見光能量的吸收。
    本研究以亞甲基藍光降解實驗,測試在紫外光燈照射下的觸媒降解效率,發現OA-TiNT約四小時即可將亞甲基藍完全分解,其光降解效率約為CA-TiNT的1.45倍。光還原二氧化碳效率,在模擬太陽燈照射下,OA-TiNT的甲醇產率約為CA-TiNT的1.7倍,ON-TiNT的產率約為CN-TiNT的1.6倍。顯示出將薄膜底部阻礙層移除後,能增加反應物與觸媒接觸的機會,推論為雙開口奈米管結構具有較好的光還原甲醇產率的原因。


    The excessive use of fossil fuels has dramatically increased the concentration of CO2 in the atmosphere. Global warming has become more serious and made a significant impact on the climate change and ecological environment. Therefore, the reduction of atmospheric CO2 is an urgent issue. The use of photocatalyst to convert CO2 into hydrocarbons can not only reduce atmospheric CO2 but also develop new energy sources.
    In this study, free-standing open-ended TiO2 nanotube array has been successfully fabricated by raising the voltage at the end of anodization process. Compared with the close-ended structure, the flow-through nanotube structure facilitate the reactants to flow into the inside of the tube. Moreover, in order to absorb more visible light, we doped nitrogen into TiO2 to modify the band gap by annealing under urea ambient (ON-TiNT).
    The degradation of TiNT catalyst was tested by the photodegradation of methylene blue solution under UV irradiation. The complete decoloration of methylene blue solution by the OA-TiNT was observed in 4 hours with a degradation efficiency about 1.45 times of the CA-TiNT. For CO2 photoreduction experiment, the methanol yield by OA-TiNT was 1.7 times of the CA-TiNT, whereas ON-TiNT was 1.6 times of the CN-TiNT under Xe lamp irradiation. Our results show that open-ednded TiNT provides the increase of the methanol yield which might be attributed to the increased reaction surface area after removing the bottom cap of close-ended TiNT.

    總目錄 圖目錄 III 表目錄 VI 第一章 緒論 1 1-1 前言 1 1-2 研究動機與目的 2 第二章 文獻回顧 3 2-1 光觸媒起源 3 2-2 光觸媒原理與特性 4 2-3 二氧化鈦光觸媒 6 2-3-1 基本性質 6 2-3-2 晶格結構 6 2-3-3 吸收可見光之改質二氧化鈦 7 2-4 二氧化鈦光催化還原二氧化碳 9 2-5 二氧化鈦奈米管陣列 12 2-5-1 二氧化鈦奈米管陣列起源 12 2-5-2 陽極氧化法反應機制 13 2-5-3 獨立封閉式二氧化鈦奈米管陣列 15 2-5-4 獨立雙開口式二氧化鈦奈米管陣列 16 第三章 實驗方法 19 3-1 實驗藥品與儀器設備 19 3-1-1 實驗藥品 19 3-1-2 儀器設備 20 3-2 獨立雙開口式二氧化鈦奈米管陣列製備 21 3-3 材料特性分析 25 3-3-1 高解析度場發射掃描電子顯微鏡 25 3-3-2 X射線粉末繞射光譜儀 25 3-3-3 高解析電子能譜儀 27 3-3-4 紫外光-可見光分光光譜儀 29 3-4 光降解亞甲基藍反應 30 3-4-1 光降解反應系統 30 3-4-2 光降解效率分析 34 3-5 光還原二氧化碳反應 36 3-5-1 光還原反應系統 36 3-5-2 光還原產物分析 40 第四章 結果與討論 42 4-1 材料特性鑑定 42 4-1-1 SEM分析 42 4-1-2 PXRD分析 55 4-1-3 XPS分析 57 4-1-4 UV-Vis分析 63 4-2 光催化活性分析 64 4-2-1 光降解亞甲基藍反應 64 4-2-2 光還原二氧化碳反應 69 4-3 光觸媒活性比較 73 第五章 結論與建議 76 5-1 獨立雙開口式二氧化鈦奈米管陣列製備 76 5-2 光催化氧化還原反應 77 第六章 參考文獻 78 圖目錄 圖2-1、本田-藤島效應(Honda-Fujishima effect) 3 圖2-2、光激發產生之電子電洞對可能進行的途徑 5 圖2-3、常見的半導體光觸媒材料能隙位置與大小 5 圖2-4、陽極氧化反應之電流與時間關係圖 14 圖2-5、二氧化鈦奈米管陣列生長機制 14 圖2-6、電壓過渡期間底部管壁變化圖 18 圖2-7、離子移動方向與開口形狀 18 圖3-1、陽極氧化法實驗儀器架設圖 23 圖3-2、三階段程序升溫 23 圖3-3、獨立雙開口式二氧化鈦奈米管陣列製備流程圖 24 圖3-4、JCPDS圖譜(21-1272) - 銳鈦礦anatase 26 圖3-5、JCPDS圖譜(21-1276) - 金紅石rutile 27 圖3-6、亞甲基藍結構式 30 圖3-7、光降解反應系統示意圖 32 圖3-8、紫外光燈管波長分佈圖 32 圖3-9、光降解反應實驗流程圖 33 圖3-10、亞甲基藍標準液之全波長吸收圖譜 35 圖3-11、亞甲基藍標準液之檢量線 35 圖3-12、圓形PET材質反應器 37 圖3-13、光還原反應系統架設圖 37 圖3-14、太陽模擬燈波長分佈圖 38 圖3-15、光還原反應實驗流程圖 39 圖3-16、甲醇標準液之層析圖譜 41 圖3-17、甲醇標準液之檢量線 41 圖4-1、二氧化鈦奈米管陣列表面覆蓋物(Debris) 45 圖4-2、二氧化鈦奈米管陣列表面開口 46 圖4-3、二氧化鈦奈米管陣列表面側面圖 47 圖4-4、二氧化鈦奈米管陣列底部封閉(close-ended) 47 圖4-5、二氧化鈦奈米管陣列幾何結構圖 48 圖4-6、陽極氧化反應之電流密度與時間關係圖 48 圖4-7、二氧化鈦奈米管陣列底部- 120 V,7 min 49 圖4-8、二氧化鈦奈米管陣列底部開口- 120 V,10 min 50 圖4-9、二氧化鈦奈米管陣列底部側面圖 51 圖4-10、二氧化鈦奈米管陣列長度 51 圖4-11、二氧化鈦奈米管陣列表面開口-鍛燒後 52 圖4-12、二氧化鈦奈米管陣列底部開口-鍛燒後 53 圖4-13、各觸媒PXRD繞射圖譜 56 圖4-14、各觸媒Ti之XPS能譜圖 59 圖4-15、各觸媒O之XPS能譜圖 60 圖4-16、觸媒(a) ON-TiNT,(b) CN-TiNT 中N之XPS能譜圖 61 圖4-17、各觸媒C之XPS能譜圖 62 圖4-18、各觸媒UV-Vis吸收光譜圖 63 圖4-19、氮摻雜二氧化鈦能階示意圖 64 圖4-20、亞甲基藍直接照光實驗(未加觸媒) 66 圖4-21、亞甲基藍吸附平衡實驗(未照光) 66 圖4-22、不同照光時間後,亞甲基藍UV-Vis圖- CA-TiNT 67 圖4-23、不同照光時間後,亞甲基藍UV-Vis圖- OA-TiNT 67 圖4-24、光降解亞甲基藍反應- C/Co對時間圖 68 圖4-25、光降解亞甲基藍反應- ln(C/Co)對時間圖 68 圖4-26、各觸媒光還原二氧化碳產率 71 圖4-27、觸媒使用次數與產率 71 圖4-28、二氧化鈦觸媒結構示意圖 72 圖4-29、反應物進入管柱內部路徑圖 72   表目錄 表2-1、銳鈦礦和金紅石物理化學特性 7 表2-2、二氧化碳還原反應之標準還原電位(SHE) 9 表3-1、二氧化鈦光觸媒命名表 22 表3-2、本電子能譜儀不同元素之感應因子(S) 28 表3-3、紫外光燈所測得之光強度 32 表3-4、二氧化碳溶於水中以及其碳酸根離子之pKa值 37 表3-5、太陽模擬燈所測得之光強度 38 表3-6、氣相層析儀(GC-FID) 設定參數 40 表4-1、獨立雙開口式二氧化鈦奈米管結構特性 54 表4-2、各觸媒Ti之XPS特徵峰 59 表4-3、各觸媒O之XPS特徵峰 60 表4-4、觸媒ON-TiNT和CN-TiNT中N之XPS特徵峰 62 表4-5、觸媒ON-TiNT和CN-TiNT的N/O比例 62 表4-6、各觸媒估算之能隙 64 表4-7、亞甲基藍降解時間與速率常數k 68 表4-8、各研究光觸媒之甲醇產率與量子效率比較 75

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