完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.author | 陳筍陽 | en_US |
dc.contributor.author | Chen, Sun-Yang | en_US |
dc.contributor.author | 李遠鵬 | en_US |
dc.contributor.author | Lee, Yuan-Pern | en_US |
dc.date.accessioned | 2014-12-12T01:34:47Z | - |
dc.date.available | 2014-12-12T01:34:47Z | - |
dc.date.issued | 2009 | en_US |
dc.identifier.uri | http://140.113.39.130/cdrfb3/record/nctu/#GT079658513 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/43573 | - |
dc.description.abstract | 利用步進式掃描時間解析傅式轉換紅外光譜儀並搭配多重反射的White cell偵測CH3CO與O2反應生成的瞬態產物CH3C(O)OO與α-lactone的紅外光吸收光譜。吾人指派t,c-CH3C(O)OO在氣態的□3 (1851 cm-1)、□5 (1372 cm-1)、□6 (1169 cm-1)、□7 (1102 cm-1)與t,t-CH3C(O)OO在氣態的□3 (1862 cm-1)、□6 (1142 cm-1)、□7 (1078 cm-1)還有α-lactone在氣態的□□ (1960 cm-1)。基於理論計算B3LYP/aug-cc-pVDZ預測的振動基態與激發態轉動常數與偶極矩導數,可利用光譜模擬程式SpecView模擬出各個振動模的振轉動譜帶,其模擬光譜與實驗光譜相當吻合。這些振動模的氣態吸收波數除了t,t-CH3C(O)OO的□7振動模之外,其餘振動模的振動波數皆與Ne間質隔離光譜相差9 cm-1以內,亦與B3LYP/aug-cc-pVDZ的計算值相差2 %以內。依據譜帶的吸收面積與理論計算的紅外光吸收強度,吾人指出t,c-CH3C(O)OO較t,t-CH3C(O)OO穩定3.0 □ 0.6 kJ mol-1,以及CH3CO + O2 □ α-lactone + OH的分支比例(branch ratio)為0.04 □ 0.01。最後吾人利用簡單的動力學解釋CH3C(O)OO的消耗。 | zh_TW |
dc.language.iso | zh_TW | en_US |
dc.subject | CH3C(O)OO | zh_TW |
dc.subject | 紅外吸收光譜 | zh_TW |
dc.subject | 時間解析 | zh_TW |
dc.subject | CH3C(O)OO | en_US |
dc.subject | IR absorption | en_US |
dc.subject | time resolved | en_US |
dc.subject | lactone | en_US |
dc.title | 利用步進式掃描時間解析傅式轉換紅外光譜法研究CH3C(O)OO之紅外光吸收光譜 | zh_TW |
dc.title | Infrared absorption of CH3C(O)OO studied with step-scan time-resolved FT-IR | en_US |
dc.type | Thesis | en_US |
dc.contributor.department | 應用化學系分子科學碩博士班 | zh_TW |
顯示於類別: | 畢業論文 |