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| ???org.dspace.app.webui.jsptag.ItemTag.dcfield??? | Value | Language |
|---|---|---|
| dc.contributor.advisor | 吳政忠 | |
| dc.contributor.author | Yi Chen | en |
| dc.contributor.author | 陳毅 | zh_TW |
| dc.date.accessioned | 2021-06-17T02:14:25Z | - |
| dc.date.available | 2020-01-04 | |
| dc.date.copyright | 2018-01-04 | |
| dc.date.issued | 2017 | |
| dc.date.submitted | 2017-11-13 | |
| dc.identifier.citation | [1] Y.-C. Shu and I. Lien, 'Efficiency of energy conversion for a piezoelectric power harvesting system,' Journal of micromechanics and microengineering, vol. 16, no. 11, p. 2429, 2006.
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| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/68190 | - |
| dc.description.abstract | 聲子晶體(Phononic crystals)是由一種或多種材料週期性排列的結構，其具有頻溝(band gap)的特性，可阻擋某頻段之彈性波傳遞。依據產生頻溝機制的不同可分為布拉格散射和局部共振型式，其中局部共振型式主要取決於共振子的結構與頻率，因此可實現以較小尺寸阻擋較大的波長。在完美週期的聲子晶體中，將其中一單胞移除會引致局部共振模態，本論文即利用此方法設計出聲子晶體共振腔。利用聲子晶體頻溝的特性使彈性波能量得以聚集，再透過壓電效應將振動能轉換為電能。並設計低頻風能轉換敲擊力的機制，以此激發出高頻聲波。
本論文使用有限元素法軟體(COMSOL)來模擬板波在聲子晶體樑結構中之行為，並透過幾何尺寸分析設計出具有低頻頻溝(7-11.5 kHz)之聲子晶體共振腔，在9.04 kHz有一共振模態。另外，模擬結果顯示當聲子晶體層數達到四層以上時有較佳的共振振幅。在壓電聲晶體的模擬中，可以發現壓電層厚度與共振腔底板比例為0.3、壓電層長度為8 mm時會有較佳的輸出電壓，故以此做為最終設計。 實驗的量測結果顯示，本研究之聲子晶體結構在5.9 kHz至9 kHz聲波會有較大的衰減，證明其阻擋波傳的能力。同時也對敲擊源的激發能量頻率進行量測與分析，以設計出最佳的敲擊源。在聲子晶體共振腔量測的部分，以螺絲配合AT-3黏膠製成的共振腔其共振頻率為8.28 kHz，加入壓電層後的共振頻率為7.25 kHz，平均功率為0.77 mW，最佳阻抗為8.27 kΩ。與無頻溝之對照組平板相比功率可達到7倍之多，證明聲子晶體對於能量擷取的效益。 最後配合電源管理模組與風力敲擊裝置進行實驗，將四個共振腔同時於風速 4 m/s下運作，平均每1.06秒可使設計電路中的電容充滿至標準電壓，並放電至後端負載，實踐壓電能量擷取裝置之研究。 | zh_TW |
| dc.description.abstract | Phononic crystals (PC) are composed of one or more materials which distributed periodically. One of the main properties of the phononic crystals is band gap which prevents the wave of a specific frequency range propagating. The band gap based on local resonant could get lower frequency band structures. A resonant cavity is formed by removing a unit from perfect PCs. And the energy of elastic wave at the resonant frequency can be trapped in the cavity. In this study, the piezo energy harvester is based on converting the acoustic energy into electric energy by putting a piezoelectric ceramics film. Besides, we design a mechanism to transforming low-frequency wind energy into impact, so we can get the high-frequency acoustic waves as source.
In this study, we numerically calculate the dispersion of lamb wave in phononic crystals strip by finite element method (FEM). The PC resonator with a band gap at 7-11 kHz and resonant frequency at 9.04 kHz was formed. Moreover, the simulated results show that more than 4 rows of PC grating can get larger resonant amplitude. And the maximum voltage output occurs at the ratio of thickness of piezoelectric ceramics film and PC plate in 0.3. The length of piezoelectric ceramics film is 8mm. In the experiment, the acoustic wave attenuated at 5.9-9 kHz in a PC strip. And we design impact source by analyzing different materials contact with thin plate. The piezo energy harvester with resonant frequency at 7.25 kHz could get a maximum power 0.77 mW under a load resistance 3.9 kΩ. Compared with the control group, the output power is 7 times lager. It shows that PC is helpful to trapping energy. Finally, we connect the output voltage to power-management circuit to observe capacitance discharging. When four PC resonators work at the same time, the average time of capacitance discharging is 1.06 seconds with the wind velocity of 4 m/s. It validates that the piezoelectric energy harvester could generate electric power from wind energy. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-17T02:14:25Z (GMT). No. of bitstreams: 1 ntu-106-R04543054-1.pdf: 4133204 bytes, checksum: 79330906183355444626a0d48a51ab8b (MD5) Previous issue date: 2017 | en |
| dc.description.tableofcontents | 致謝 I
中文摘要 II ABSTRACT III 目錄 V 表目錄 VII 圖目錄 VIII 符號對照表 XII 第一章 研究介紹 1 1.1 研究動機 1 1.2 文獻回顧 2 1.3 章節介紹 4 第二章 聲子晶體樑共振腔設計 7 2.1 聲子晶體波傳理論 7 2.2 聲子晶體結構設計 10 2.2.1 板波於聲子晶體樑之頻散與振動模態 10 2.2.2 幾何尺寸設計 11 2.2.3 穿射率分析 13 2.3 聲子晶體樑共振腔設計 14 2.3.1 共振模態設計 14 2.3.2 聲子晶體層數分析 15 第三章 壓電能量擷取裝置之設計 29 3.1 壓電效應 29 3.2 壓電材料之特性與相關參數 30 3.2.1 壓電材料組成律 30 3.2.2 壓電材料極化處理 31 3.2.3 壓電操作模式 32 3.2.4 機電耦合係數( Electro-Mechanical Coupling Factor ) 32 3.2.5 機械品質因子( Mechanical Quality Factor ) 33 3.3 壓電聲子晶體樑共振腔功率分析 33 3.3.1 壓電材料選用 34 3.3.2 壓電陶瓷片尺寸設計 34 3.4 等效電路模型與電源管理模組 37 3.4.1 等效電路模型 37 3.4.2 電源管理電路設計 38 3.5 風能擷取機構 39 3.5.1 低頻能量轉換高頻機制 39 3.5.2 壓電能量擷取裝置機構設計 41 第四章 聲子晶體樑共振腔之壓電能量擷取 54 4.1 聲子晶體頻溝量測 54 4.2 敲擊源訊號分析 55 4.3 壓電聲子晶體樑共振腔之特性量測 57 4.3.1 不同製作方式之共振腔比較 57 4.3.2 壓電共振腔訊號量測 58 4.3.3 聲子晶體層數對共振腔之影響 58 4.4 輸出功率量測 59 4.4.1 外接電阻與輸出功率之量測 59 4.4.2 聲子晶體對輸出電壓與功率之影響 60 4.4.3 不同敲擊源之輸出功率比較 61 4.5 壓電能量擷取電路實驗 62 第五章 結果討論與未來展望 86 5.1 結論 86 5.2 未來展望 87 參考文獻 88 | |
| dc.language.iso | zh-TW | |
| dc.subject | 聲子晶體共振腔 | zh_TW |
| dc.subject | 風力敲擊裝置 | zh_TW |
| dc.subject | 聲子晶體樑 | zh_TW |
| dc.subject | 蘭姆波 | zh_TW |
| dc.subject | 壓電能量擷取 | zh_TW |
| dc.subject | Piezo energy harvesting | en |
| dc.subject | Phononic crystal resonator | en |
| dc.subject | Wind-induced impact | en |
| dc.subject | Phononic crystal strip | en |
| dc.subject | Lamb wave | en |
| dc.title | 結合聲子晶體樑共振腔之壓電能量擷取裝置研製 | zh_TW |
| dc.title | Piezo Energy Harvester Using Resonant Cavity in Phononic Crystal Strip | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 106-1 | |
| dc.description.degree | 碩士 | |
| dc.contributor.oralexamcommittee | 陳永裕,孫嘉宏,陳蓉珊,鮑世勇 | |
| dc.subject.keyword | 聲子晶體樑,聲子晶體共振腔,壓電能量擷取,蘭姆波,風力敲擊裝置, | zh_TW |
| dc.subject.keyword | Phononic crystal strip,Phononic crystal resonator,Piezo energy harvesting,Lamb wave,Wind-induced impact, | en |
| dc.relation.page | 91 | |
| dc.identifier.doi | 10.6342/NTU201704366 | |
| dc.rights.note | 有償授權 | |
| dc.date.accepted | 2017-11-14 | |
| dc.contributor.author-college | 工學院 | zh_TW |
| dc.contributor.author-dept | 應用力學研究所 | zh_TW |
| Appears in Collections: | 應用力學研究所 | |
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| ntu-106-1.pdf Restricted Access | 4.04 MB | Adobe PDF |
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