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http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/17604Full metadata record
| ???org.dspace.app.webui.jsptag.ItemTag.dcfield??? | Value | Language |
|---|---|---|
| dc.contributor.advisor | 朱國瑞(Kwo-Ray Chu) | |
| dc.contributor.author | Kuan-Yu Lin | en |
| dc.contributor.author | 林冠宇 | zh_TW |
| dc.date.accessioned | 2021-06-08T00:24:43Z | - |
| dc.date.copyright | 2013-07-31 | |
| dc.date.issued | 2013 | |
| dc.date.submitted | 2013-07-15 | |
| dc.identifier.citation | 參考資料
[1] K.R. Chu, ” Time Domain Analysis of open cavities” , 1993 [2] K.R. Chu, Cs. Kou, JM. Chen, YC. Tasi, C. Cheng, S.S. Bor, and L.H. Chang, ”Spectral Domain Analysis of Open cavities,” Int. J. Infrared and Millimeter Wave vol. 13, PP.1571-1598, 1992. [3] K.R. Chu, ”Analysis of a Basis Electron Cyclotron Maser Model”, J. Chinese Institute of Engineers, vol.4, pp.85-90, 1981 [4] J.D. Jackson, “Classical Electrodynamics”, John Wiley & Son, the third edition, 2001 [5] K. R. Chu, Reviews of Modern Physics vol. 76, pp.490-540, 2004. [6] 洪健倫, “開口式共振腔及超高增益磁旋行波放大器研究”, 清華大學博士論文, 1998. [7] Jon Mathews and R.L. Walker, “Mathematical Method of Physics”, California Institute of Technology. | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/17604 | - |
| dc.description.abstract | 本文討論的低Q值的開口式共振腔常應用於磁旋振盪管(gyromonotron oscillator)及磁波調速管(gyroklystron)。
可以知道開口式共振腔不同於封閉式共振腔乃是因為缺乏一個明顯的邊界,為了對其基本性質深入瞭解,因此針對兩個開口式共振腔特性詳加闡述: 共振頻率 ƒ0 、品質因素 Q 。 內文將以兩種不同模型: (1)時域法 (2)頻域法,在第一種模型中會將主腔體長度改變、角度改變去討論Q值與頻率的影響,再討論不同場型的分佈影響;第二種模型將以最大場強法、總場能法與反射法去討論不同方法的異同,藉由模態疊加效應分清方法的差異,再跟第一種模型做理論推導與數值模擬,並針對其中的不同,加以探討與比較,然而可以經由理論推導,去做出總場能法與反射法的近似,以達到理論模理與實驗的結合。 | zh_TW |
| dc.description.abstract | For open-end cavities generally used in gyrotrons, the lack of a well-defined geometrical boundary gives rise to distinctive feature as well as physics that are basically different from the closed cavity.
We are concerning the consistency that time and frequency domain interpretations of the resonant frequency and quality factor . In the time domain, we change cavity size to discuss quality factor and resonant frequency. In the spectral domain, we can use different methods to get quality factor. The methods are maximum-field, the field energy, reflection spectrum. The field energy spectrum can be constructed from the power of the reflected waves, and compared time domain model to analyze some difference. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-08T00:24:43Z (GMT). No. of bitstreams: 1 ntu-102-R00222083-1.pdf: 4819587 bytes, checksum: b67c08fdb8d24f0e94169bbc851d8bbf (MD5) Previous issue date: 2013 | en |
| dc.description.tableofcontents | CONTENTS
口試委員會審定書 中文摘要 i ABSTRACT ii CONTENTS iii LIST OF FIGURES v LIST OF TABLES vi 第一章 緒論 1 1.1 微波管 2 1.2 研究動機 3 1.3 研究內容摘要 5 第二章 時域法模型 6 2.1 時域法模型 (time domain model) 理論 7 2.2 時域法模型之場分佈 13 2.3 共振腔特性與 Q 值 15 第三章 頻域法模型 (spectral domain model) 18 3.1 開口共振腔之模態疊加效應 18 3.2 理論推導和數值模擬 22 3.3 最大場強法 26 3.4 總場能法 30 3.5 反射法 32 3.6 總場能法與反射法的關係 33 第四章 結論 40 參考文獻 41 附錄A一維波動方程推導 42 附錄B波導中有歐姆損耗之色散關係 45 附錄C TEmn mode 在均勻波導中之歐姆損耗與場能 47 | |
| dc.language.iso | zh-TW | |
| dc.title | 開口式共振腔之時域與頻域分析 | zh_TW |
| dc.title | Time and Frequency Domain Analysis of Open Cavity | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 101-2 | |
| dc.description.degree | 碩士 | |
| dc.contributor.oralexamcommittee | 張存續,陳寬任,陳仕宏 | |
| dc.subject.keyword | 共振腔,共振頻率,品質因素,最大場強法,場能法, | zh_TW |
| dc.subject.keyword | open cavity,resonant frequency,quality factor,maximum-field,field energy, | en |
| dc.relation.page | 51 | |
| dc.rights.note | 未授權 | |
| dc.date.accepted | 2013-07-16 | |
| dc.contributor.author-college | 理學院 | zh_TW |
| dc.contributor.author-dept | 物理研究所 | zh_TW |
| Appears in Collections: | 物理學系 | |
Files in This Item:
| File | Size | Format | |
|---|---|---|---|
| ntu-102-1.pdf Restricted Access | 4.71 MB | Adobe PDF |
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