完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.author | 廖文紹 | en_US |
dc.contributor.author | Wen-shao Liao | en_US |
dc.contributor.author | 林健正 | en_US |
dc.contributor.author | Chien-Cheng Lin | en_US |
dc.date.accessioned | 2014-12-12T02:41:08Z | - |
dc.date.available | 2014-12-12T02:41:08Z | - |
dc.date.issued | 2004 | en_US |
dc.identifier.uri | http://140.113.39.130/cdrfb3/record/nctu/#GT009218511 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/74657 | - |
dc.description.abstract | 以熱壓法製備不同組成之Y2O3/ZrO2(Yttria/Zirconia)複合材料,與鈦(Titanium, Ti)在1atm 氬(Ar)氣氛下,進行1700°C/10min之擴散反應,利用X光繞射(x-ray diffraction, XRD)、掃描式電子顯微鏡(scanning electron microscopy/energy dispersive spectroscopy, SEM/EDS)、電子微探儀(electron probe microanalyzer, EPMA)與穿透式電子顯微鏡(transmission electron microscopy/energy dispersive spectroscopy, TEM/EDS),分析擴散反應後介面之微觀結構。結果顯示10 vol%Y2O3-ZrO2複合材料與鈦發生劇烈的擴散反應,鋯與氧大量固溶於鈦中,反應生成物從鈦側至陶瓷側依序為α-Ti(Zr, O)、β'-Ti(Zr, O)與針狀α-Ti二相區、以及大量的α-Zr。Y2O3體積含量大於30 vol%時,界面擴散反應明顯受到抑制,鈦液僅能沿晶界與孔隙滲入陶瓷側,冷卻後形成網狀分佈的α-Ti(Zr, O)與β'-Ti(Zr, O)二相區,同時鈦側β'-Ti(Zr, O)與陶瓷側α-Zr的生成量隨Y2O3含量的增加而減少。Y2O3體積含量大於70 vol%時,鈦液滲入陶瓷側的路徑大部分被阻斷,冷卻後形成塊狀分佈的α-Ti(Zr, O)與β'-Ti(Zr, O)二相區。Y2O3體積含量大於90 vol%時,鈦、鋯擴散反應幾乎完全被抑制,界面處無反應層出現。 | zh_TW |
dc.description.abstract | Hot pressed composites with various content of Y2O3 and ZrO2 were reacted with the titanium melt at 1700°C/10min in argon. The microstructure of the reaction interface were characterized using x-ray diffraction (XRD), scanning electron microscopy (SEM), electron probe microanalyzer (EPMA) and analytical transmission electron microscopy (TEM/EDS). The result showed that an obviously diffusive phenomenon occur in the 10vol% Y2O3-ZrO2 composite and titanium. The α-Ti(Zr, O) and β'-Ti(Zr, O) formed in the titanium side during cooling down to the room temperature. The β'-Ti(Zr, O) existed due to the dissolution of large amount of Zr which restrained β→α phase transformation. In the ceramic side, large amount of α-Zr was precipitate from ZrO2-x. When the Y2O3 content is greater then 30vol%, the diffusive phenomenon was restrained. The liquid titanium can only infiltrated into the ceramic mold through the open pores and grain boundary. The α-Ti(Zr, O) and β'-Ti(Zr, O) formed in the ceramic side in the form of network during cooling down to the room temperature. Precipitation of β'-Ti(Zr, O) in titanium side and α-Zr in ceramic side decrease as the Y2O3 content increase. When the Y2O3 content is greater then 70vol%, infiltration path of liquid titanium to ceramic side was mostly blocked. When the Y2O3 content is greater then 90vol%, there is no interfacial reaction zone between titanium and ceramic composite. | en_US |
dc.language.iso | zh_TW | en_US |
dc.subject | 氧化釔 | zh_TW |
dc.subject | 氧化鋯 | zh_TW |
dc.subject | 鈦 | zh_TW |
dc.subject | 擴散 | zh_TW |
dc.subject | Yttria | en_US |
dc.subject | Zirconia | en_US |
dc.subject | Titanium | en_US |
dc.subject | Diffusion | en_US |
dc.title | 氧化釔/氧化鋯複合材料與液態鈦金屬之介面反應 | zh_TW |
dc.title | Interfacial Phenomenon between Liquid Titanium and Yttria/Zirconia Composites | en_US |
dc.type | Thesis | en_US |
dc.contributor.department | 材料科學與工程學系 | zh_TW |
顯示於類別: | 畢業論文 |
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