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  1. NTU Theses and Dissertations Repository
  2. 工學院
  3. 應用力學研究所
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/31752
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor李雨
dc.contributor.authorYi-Sheng Chenen
dc.contributor.author陳意昇zh_TW
dc.date.accessioned2021-06-13T03:19:15Z-
dc.date.available2016-08-02
dc.date.copyright2011-08-02
dc.date.issued2011
dc.date.submitted2011-07-29
dc.identifier.citation[1] Akaydin, H.D., Elvin, N. and Andreopoulos, Y., “Energy Harvesting from Highly Unsteady Fluid Flows using Piezoelectric Materials”, Journal of Intelligent Material Systems and Structures, 21, 2010, 1263
[2] Ardakani, H.A. and Bridges T.J., “Dynamic Coupling between Shallow-Water Sloshing and Horizontal Vehicle Motion”, Journal of Applied Mathematics, 2010, vol. 21, pp. 479–517
[3] Currie, I. G., “Fundamental Mechanics of Fluids”, 1985
[4] Dodge, Franklin T., “The New Dynamic Behavior of Liquids in Moving Containers”, 2000
[5] Elvin, N. and Elvin, A., “A General Equivalent Circuit Model for Piezoelectric Generators”, Journal of Intelligent Material Systems and Structures, 20, 2009, pp.3-9.
[6] Faltinsen, O. M., “Sloshing”, Cambridge University Press, New York, 2009
[7] Guyomar, D., Badel, A., Lefeuvre, E., and Richard C., “Toward Energy Harvesting Using Active Materials and Conversion Improvement by Nonlinear Processing”, IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control, April 2005, vol. 52, No. 4
[8] Ibrahim, R.A., “Liquid Sloshing Dynamics”, Cambridge University Press, New York, 2005
[9] IEEE Standard on Piezoelectricity, 1988
[10] Kalechman, Misza, “Practical MATLAB Applications for Engineers”, ch5, 2009
[11] Leo, Donald J., “Engineering Analysis of Smart Material Systems”, 2007
[12] Mateu, L. and Moll, F., “Optimum Piezoelectric Bending Beam Structures for Energy Harvesting Using Shoe Inserts”, Journal of Intelligent Material Systems and Structures, 16(10), 2005, pp. 835-845.
[13] Moulson, A.J. and Herbert, J.M., “Electroceramics, Materials, Properties, and Applications”, Chapman and Hall, London, 1990
[14] Na Kong, Dong Sam Ha, Alper Erturk and Daniel J. Inman, “Resistive Impedance Matching Circuit for Piezoelectric Energy Harvesting”, Journal of Intelligent Material Systems and Structures, 2010, 21: 1293
[15] Rao, J.S., “Advanced Theory of Vibration”, 1992
[16] Rao, S.S., “ Mechanical Vibrations”, 1995
[17] Schmidt, V., “Theoretical Electrical Power Output per Unit Volume of PVF2 and Mechanical-To-Electrical Conversion Efficiency as Functions of Frequency,” in Proc. IEEE 6th Int. Symp. Applications of Ferroelectrics, Bethlehem, PA, June 8–11, 1986.
[18] Tabesh, Ahmadreza and Fréchette, Luc G, “An Improved Small-Deflection Electromechanical Model for Piezoelectric Bending Beam Actuators and Energy Harvesters” , Journal of Micromechanics and Microengineering, 18, 2008, 104009
[19] Taylor, G.W., Burns, J.R., Kammann, S.M., Powers W.B., and Welsh, T.R., “The Energy Harvesting Eel: A Small Subsurface Ocean/River Power Generator”, IEEE Journal of Oceanic Engineering, Vol. 26, No. 4, Octorber 2001
[20] Veletsos, A.S. and Shivakumar, P., “Sloshing Response of Layered Liquids in Rigid Tanks”, Earthquake Engineering and Structure Dynamics, vol.22, 1993, pp. 801-821
[21] Weigert, S., Dreier, M., Hegner, M., “Frequency Shifts of Cantilevers Vibrating in Various Media”, Applied Physics Letters, 11/4/96, Vol. 69, Issue 19, pp. 2834
[22] 周卓明, “壓電力學”,民92
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/31752-
dc.description.abstract本論文以理論分析進行擷取流體表面或界面波能量的研究。我們在長方形盒中裝載單層或雙層流體,將PVDF雙層壓電片置於流體間的界面或自由表面上;並假設流體界面或表面的垂直方向位移與壓電片於垂直方向的位移分量相等,我們計算出整個系統最後之瞬時最大發電功率。單層流的分析考慮盒子受到側向施力或小角度搖擺運動兩種驅動模式。雙層流之分析則只考慮盒子受到側向施力驅動狀况,但壓電片可置於雙層流之表面或兩液體之界面。
計算結果發現,若想在低頻引發固流共振則必須將壓電片置於雙層流之界面。然而,若想在較高頻的情況引發固流共振則必須將壓電片置於雙層流表面。此外,對於單層流而言,盒子受到側向施力或搖擺運動,搖擺運動所產生的發電功率較高。
zh_TW
dc.description.abstractIn this thesis, we perform a theoretical study on harvesting the surface or interface wave energy from layer(s) of liquid. Scavenging the vibration energy surrounding us is the core idea of this research. Such vibration energy is used as a source to exert force on a rectangular tank which is partial filled with liquid(s), and thus drives the wave motion. We consider two major cases; one is a tank containing a single-layer liquid exerted by either a lateral or pitching excitation. We harvest the surface wave energy at the free surface. The other is a tank consisting of the two layers of immiscible liquid exerted by a lateral excitation. There are two harvesting locations for the latter case, one at the free surface and one at the interface of the double-layer liquid.
We place a PVDF bimorph on the interface between two liquids or on the free surface of the liquid. Under the assumption that the displacement of the PVDF bimorph along the gravitational direction is equal to the sloshing height of liquid at the interface or at the free surface, we calculated the power harvested in the PVDF bimorph. We found that if we want to resonate at a lower frequency, we have to place the PVDF bimorph at the interface of the liquid layers. However, if we intend to resonate at a higher frequency, putting the PVDF bimorph at the free surface can harvest more electric power. Moreover, the power output for the single-layer liquid is greater when it is under the pitching excitation case compared with the lateral excitation case.
en
dc.description.provenanceMade available in DSpace on 2021-06-13T03:19:15Z (GMT). No. of bitstreams: 1
ntu-100-R98543027-1.pdf: 1582842 bytes, checksum: 41a7ade62432211f5b99e55bafd71f25 (MD5)
Previous issue date: 2011
en
dc.description.tableofcontentsAcknowledgements I
Abstract II
論文摘要 III
Contents IV
List of Figures VI
List of Tables XII
Nomenclature XIV
Chapter 1 Introduction 1
1-1 Research Background and Motivation 1
1-2 Literature Review 2
1-3 Work and Objective 4
1-4 Thesis Organization 4
Chapter 2 Wave Motion of Liquid Layers 6
2-1 Review of the Wave Motion in an Infinite Liquid Layer 6
2-2 Wave Motion of a Liquid Layer in a Rectangular Vessel 12
2-2.1 Lateral Excitation 12
2-2.2 Pitching Excitation 19
2-3 Sloshing of a Double-Layer Liquid in a Rectangular Vessel 24
Chapter 3 Energy Harvesting from PVDF Film 35
3-1 Mechanics of PVDF( Polyvinylidene Fluoride, PVF2) Film 35
3-2 Theory of Euler-Bernoulli Beams 42
3-3 Lateral Vibration of Beams 42
3-4 Charges Accumulation and Charges Conservation 48
3-5 Estimation of Electric Energy 49
3-5.1 Beam at the Interface of the Double-Layer Liquid 50
3-5.2 Beam at the Free Surface of the Double-Layer Liquid 53
3-5.3 Lateral Excitation of a Single-Layer Liquid 55
3-5.4 Pitching Excitation of a Single-Layer Liquid 56
Chapter 4 Conclusions and Future Work 58
4-1 Research Summary 58
4-2 Future Prospects 61
References 62
Figures 64
Tables 96
Appendix A. Solution of a Second Order Ordinary Differential Equation 103
Appendix B. Leibnitz’s Rule 104
Appendix C. Properties of a PVDF Film 105
dc.language.isoen
dc.subject搖擺與側向平移受力潑濺zh_TW
dc.subject能量擷取zh_TW
dc.subjectPVDF壓電薄膜zh_TW
dc.subject表面及界面波zh_TW
dc.subject雙層流潑濺zh_TW
dc.subjectSurface and interface waveen
dc.subjectPitching and lateral translating excitationen
dc.subjectDouble-layer sloshingen
dc.subjectEnergy harvestingen
dc.subjectPVDF piezoelectric filmen
dc.title擷取水波能量的理論分析zh_TW
dc.titleTheoretical Analysis of Harvesting Energy from Water Wavesen
dc.typeThesis
dc.date.schoolyear99-2
dc.description.degree碩士
dc.contributor.oralexamcommittee胡文聰,楊政穎
dc.subject.keyword能量擷取,PVDF壓電薄膜,表面及界面波,雙層流潑濺,搖擺與側向平移受力潑濺,zh_TW
dc.subject.keywordEnergy harvesting,PVDF piezoelectric film,Surface and interface wave,Double-layer sloshing,Pitching and lateral translating excitation,en
dc.relation.page105
dc.rights.note有償授權
dc.date.accepted2011-07-29
dc.contributor.author-college工學院zh_TW
dc.contributor.author-dept應用力學研究所zh_TW
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