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  1. NTU Theses and Dissertations Repository
  2. 工學院
  3. 應用力學研究所
Please use this identifier to cite or link to this item: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/27994
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dc.contributor.advisor張正憲
dc.contributor.authorWai-Ping Linen
dc.contributor.author林偉平zh_TW
dc.date.accessioned2021-06-12T18:32:18Z-
dc.date.available2012-08-02
dc.date.copyright2007-08-02
dc.date.issued2007
dc.date.submitted2007-07-31
dc.identifier.citation1. H. Anderson, W. van der Wijngaart, P. Nilsson, P. Enoksson, and G. Stemme,“A valve-less diffuser micropump for microfluidic analytical systems”, Sensors and Actuators B., Vol. 72, pp.259-265, 2001.
2. B. Fan, G. Song and F. Hussain,“Simulation of a piezoelectrically actuated valveless micropump“, Smart Mater. Struct., Vol.14, pp.400-405, 2005.
3. Y. Feng, Z. Zhou and G. Wang,“A fluid-solid coupling modal analysis of piezoelectrically actuated microjet and the frequency design of nozzles layout”, SPIE, Vol. 5718, pp.243-253, 2005.
4. T. Gerlach, M. Schuenemann and H. Wurmus,“A new micropump principle of the reciprocating type using pryramidic micro flow channel as passive valves”, Journal of Micromechanics and Microengineering, Vol. 5, pp. 199-201, 1995.
5. Laser, D. J. and Santiago, J. G.,“A review of micropumps”, J. Micromech. Microeng., Vol. 14, pp. 35-64, 2004.
6. E. STEMME, G. STEMME, A. Olsson,“A valveless diffuser/nozzle-based fluid pump”, Sensors and actuators. A, Physical 39:22, 159-167, Elsevier Science, 1993.
7. A. Olsson, G. Stemme and E. Stemme,“A valve-less planar fluid pump with two pump chambers”, Sensor and Actuators, Vol. 46-47, pp.549-556, 1995.
8. A. Olsson, G. Stemme and E. Stemme, “A valves-less planar pump isotropically etched in silicon”, J. Micromech. Microeng., Vol. 46-47, pp.549-556, 1996.
9. A. Olsson, G. Stemme and E. Stemme,“Diffuser-element design investigation for valve-less pumps”, Sensor and Actuators A., Vol. 57, pp.137-143, 1996.
10. A. Olsson, G. Stemme and E. Stemme,“Numerical design study of the valveless diffuser pump using a lumped-mass model”, J. Micromech. Microeng., Vol. 9, pp. 34-44, 1999.
11. A. Olsson, G. Stemme and E. Stemme, “Numerical and experimental studies of flat-walled diffuser elements for valve-less micropumps”, Sensor and Actuators, Vol. 84, pp.165-175, 2000.
12. L. S. Pan, T. Y. Ng, X. H. Wu and H. P. Lee, “Analysis of valveless micropumps with inertial effects”, J. Micromech. Microeng., Vol. 13, pp.390-399, 2003.
13. E. Stemme and G. Stemme, “A valve-less diffuser/nozzle-based fluid pump”, Sensor and Actuators A., Vol. 39, pp. 159-167, 1993.
14. 楊政穎, 林俊達, 李雨, ”A valve-less micro-pump on asymmetric obstacles”, 第七屆奈米工程暨微系統技術研討會論文集, 330-333, 2003.
15. CFDRC V2004 User Manuals
16. 涂智凱, ”新式無閥門微型幫浦之開發”, 國立台灣大學應用力學所碩士論文,2004.
17. 羅卓錚, ”擋體式無閥門微幫浦之數值模擬”, 國立台灣大學應用力學所碩士論文,2004.
18. 吳咨亨, ”無閥門壓電微幫浦與為混合器之整合設計”, 國立台灣大學應 用力學所碩士論文,2005.
19. 田明偉, ”微流道中以不對稱擋體作為流場導向的研究”, 國立台灣大學 應用力學所碩士論文,2005.
20. C. J. Lee, Z. K. Tsu, U. Lei, C. J. Hsu, and H. J. Sheen,“ A Valveless Micropump with Asymmetric Obstacles” , The Sixteenth International Symposium on Transport Phenomena (ISTP-16), Prague, Czech, August 2005.
21. 藍文彬, ”壓電驅動無伐門微幫浦固液耦合之模態分析”, 國立台灣大學 應用力學所碩士論文,2007.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/27994-
dc.description.abstract本文利用CFDRC 商業軟體作為數值分析的工具,模擬無閥門式微幫浦並進而修改,比較各種型式的無閥門式微幫浦在各個頻率的淨流量差異。由於單腔室的無閥門式微幫浦的淨流量有限,因此我們用兩個微幫浦做組合以提升微幫浦的效能,最常見的微幫浦組合有串聯以及併聯。其中併聯為了連通兩個微幫浦會產生多餘的流道,故體積比較大,雖然淨流量優異,但微小化不易,因此我們我們在微幫浦的組合的型式是以串聯為主,並藉由搭配不同的頻率組合來找出最適合微幫浦串聯的運作方式。將漸張/漸縮管式微幫浦串聯在一起,流體為水時,輸入波形為正弦波,給予固定電壓80伏特,兩個壓電片執行同頻率反相位角的作動,從數值計算的結果可以得知,於頻率4.8KHz時流量為134 uL/min,為單一腔室的1.64倍,而兩個壓電片執行倍頻模式,也就是其中一個壓電片給予f頻率、另一個壓電片給予2f的頻率並給予一個90度的相位角延遲,數值計算結果可以得知,在頻率f為3.4KHz時淨流量為244.49 uL/min,為單一腔室微幫浦的2.99倍,增幅效果極佳。zh_TW
dc.description.abstractWe use the software CFDRC to do the research about the valveless micropump which is driven by piezoelectrical materials. We also modify valveless micropump to other type valveless micropump and compare flow rate in each frequency. In order to increase the flow rate, we connect two valveless micropumps in serials and run in anti-phase mode and double frequency mode to obtain large flow rate. Double frequency mode is that one piezoelectrical material runs in f KHz and another runs in 2f KHz with phase angle different. The flow rate of anti-phase is 134 uL/min in 4.8 KHz, and flow rate of double frequency is 244 uL/min in f=3.4KHz . The efficiency of double frequency mode is higher than that of anti-phase mode.en
dc.description.provenanceMade available in DSpace on 2021-06-12T18:32:18Z (GMT). No. of bitstreams: 1
ntu-96-R93543055-1.pdf: 1803644 bytes, checksum: 58a493309b8ce6fb9003a5e1aaf34331 (MD5)
Previous issue date: 2007
en
dc.description.tableofcontents摘要 I
目錄 III
圖目錄 VI
表目錄 X
符號對照表 XI
第一章 導論 1
1.1前言 1
1.2文獻回顧 1
1.3研究動機 5
1.4本文研究方法與架構 6
第二章 理論基礎 7
2.1 無閥門微幫浦基本工作原理 7
2.2 基本假設 8
2.3 固體結構 9
2.3-1壓電結構物的統御方程式 9
2.3-2壓電結構物的本構方程式 9
2.4 流場內的統御方程式 10
2.5 邊界條件 12
2.6 倍頻模式輸入電壓 12
第三章 數值方法與結果討論 13
3.1 有限體積法 13
3.2 有限差分法 17
3.3 收斂標準 18
3.4 CFDRC軟體介紹 18
3.4-1 前言 18
3.4-2 建立格點 19
3.4-3 物理性質 20
3.4-4 邊界條件設定 21
3.5數值算例 22
3.5-1 檔體式無閥門微幫浦輸入波為方波與正弦波之 23
模擬分析
3.5-2 檔體式無閥門微幫浦流體為血漿與水之比較之 26
模擬分析
3.5-3 檔體式無閥門微幫浦修改為漸張/漸縮管式微幫 27
浦
3.5-4 漸張/漸縮管式微幫浦的模擬分析 28
3.5-5 倍頻雙腔室微幫浦 30
3.5-6 倍頻概念應用於漸張/漸縮管式微幫浦串聯與反 32
相同頻率的比較
第四章 結論與未來展望 34
4.1 結論 34
4.2 未來展望 35
參考文獻 38
附圖 40
附表 61
附錄 64
dc.language.isozh-TW
dc.subject無閥門zh_TW
dc.subject壓電材料zh_TW
dc.subject微幫浦zh_TW
dc.subjectvalvelessen
dc.subjectmicropumpen
dc.subjectpiezoelectricalen
dc.title壓電材料驅動無閥門式微幫浦之模擬分析zh_TW
dc.titleANALYSIS OF PIEZOELECTRICAL ACTUATED VALVELESS MICROPUMPen
dc.typeThesis
dc.date.schoolyear95-2
dc.description.degree碩士
dc.contributor.oralexamcommittee吳光鐘,沈弘俊,趙聖德
dc.subject.keyword無閥門,微幫浦,壓電材料,zh_TW
dc.subject.keywordpiezoelectrical,micropump,valveless,en
dc.relation.page39
dc.rights.note有償授權
dc.date.accepted2007-08-01
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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