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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 地質科學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/32119
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor洪淑蕙
dc.contributor.authorCheng-Chien Pengen
dc.contributor.author彭振謙zh_TW
dc.date.accessioned2021-06-13T03:32:34Z-
dc.date.available2006-07-31
dc.date.copyright2006-07-31
dc.date.issued2006
dc.date.submitted2006-07-26
dc.identifier.citationBevis, M., The curvature of Wadati-Benioff zones and the torsional rigidity of subducting plates, Nature, 323, 52-53, 1986.
Bevis, M., Seismic slip and down-dip strain rates in Wadati-Banioff zones, Sciences, 240, 1317-1319, 1988.
Bondar, V. D., On the compatibility equations in terms of strains and stresses, J. Appl. Math. Mech., 33, 1058-1068, 1970.
Chiao, L.-Y., Membrane Deformation Rate and the Geometry of Subducting Slabs [Ph.D. thesis]: Seattle, University of Washington, 144 p, 1991.
Chiao, L.-Y., and K.C. Creager, Geometry and the membrane deformation rate of the subducting Cascadia slab, The Cascadia Subduction Zone and Related Subduction Systems-Seismic, Structure, Intraslab Earthquakes and Processes, and Earthquake Hazards, Kirby, S., K. Wang, and S. Dunlop eds., 169 p., U.S. Geological Survey Open-File Report 02-328, and Geological Survey of Canada OpenFile 4350.,2002.
Creager, K.C., and T.M. Boyd, The geometry of Aleutian subduction: Three-dimensional kinematic flow modeling, J. Geophys. Res., 96, 2293-2307, 1991.
Creager, K.C., L.-Y. Chiao, J.P. Winchester Jr., E.R. Engdahl, Membrane strain rates in the subducting plate beneath South America, Geophys. Res. Lett., 22, 2321-2324, 1995.
Cahill, T., and B,L. Isacks, Seismicity and shape of the subducted Nazca Plate., J. Geophys. Res., 97, 17503-17529, 1992.
Calladine, C, R., Theory of shell structures, Cambridge University Press, Cambridge, 763 p, 1988.
Chiu, J.-M., B.L. Isacks, R.K. Cardwell, 3-D configuration of subducted lithosphere in the western Pacific, Geophys. J. Int., 106, 99-111, 1991.
Danielson, D.A., Vectors and Tensors in Engineering and Physics: Redwood City, Addison-Wesley publishing company, 280 p, 1992.
Do Carmo, A. P., Differential Geometry of Curves and Surfaces: Prentice-Hall, 503p, 1976.
Dziewonski, A.M., and J.H. Woodhouse, An experiment in the systematic study of global seismicity: centroid-moment tensor for 201 moderate and large earthquakes of 1981, J. Geophys. Res., 88, 3247-3271, 1983.
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Gauss, Disquisitiones generales circa superficies curves, Gottingen Comm. Rec., t6, 1828.
Lancaster, P., and K. Salkauskas, Curve and Surface Fitting, Academic press, London, 280 pp, 1988.
Laravie, J. A. Geometry and lateral strain of subduction plates in island arcs, Geology, 3, 484-486, 1975.
Lisle, R.J., Detection of zones of abnormal strains in structures using Gaussian curvature analysis, Annual Association Petroleum Geology Bulletin, 78, 1811-1819, 1994.
Lundgren P.R. and D. Giardini, Lateral structure of the subducting Pacific Plate beneath the Hokkaido corner from intermediate and deep earthquakes, PAGEOPH, 134, 385-404, 1990.
Morgan, W. J., Rise, trench, great faults, and crustal blocks, J. Geophys. Res., 73, 1959-1982, 1968.
Nothard, S., D. Mckenzie, J. Haines, and J. Jackson, Gaussian curvature and the relationship between the shape and the deformation of the Toga slab, Geophys. J. Int., 127, 311-327, 1996.
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Rogers, G.C., Seismotectonics of British Columbia, Ph.D. thesis, Univ. British Columbia, Vancouver, 277pp., 1983.
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/32119-
dc.description.abstractPlate kinematics on the surface of the Earth has been described successfully by the Eulerian rotation without intraplate deformation. It is, however, difficult to specify the kinematics of the lithosphere subduction. Connected with the surface plate velocity across the pivot axis, the trench, the velocity vector field of the subducted slab had been conventionally defined by simply rotating the surface Eulerian kinematics with respect to the local strike onto the slab surface. It usually results in unrealistic in-plane deformation rates within the slab surface. Alternatively, the flow field as well as the observed slab geometry can be shown to be natural consequences of attaining the kinematic field with the minimum dissipation power. The dependence of the deformation rates, associated with such flow field as defined following the minimization, upon the intrinsic geometry of the non-Euclidean surface is, however, implicit and opaque. We derive, in this study, the fundamental compatibility equation of the strain-rates tensor for the subduction flow field to highlight the fundamental dependency. There are two factors; one is associated with the variation of the Gaussian curvature along the stream lines. The other is the local compressibility amplified by the in situ Gaussian curvature. We discuss the implications of these factors and point out that to delineate the potential membrane deformation rates of the subducted slab, unambiguous information on the subduction kinematics is essential in addition to mapping the Gaussian curvature variation of the subducted slab.en
dc.description.provenanceMade available in DSpace on 2021-06-13T03:32:34Z (GMT). No. of bitstreams: 1
ntu-95-R93224209-1.pdf: 926300 bytes, checksum: 7261cbf7e55df586380e94e1a7de3d41 (MD5)
Previous issue date: 2006
en
dc.description.tableofcontents目錄 I
圖目錄 II
摘要 III
第一章 序論
1.1運動學與幾何空間 ……………………………………………………………1
1.2應變的相容方程式 ……………………………………………………………3
第二章 基本理論
2.1對於隱沒板塊的假設 …………...…………………………………………….7
2.2 薄板變形與撓曲變形 ……………...…………………………………………8
2.3 薄板變形率:順推問題 ……..……………………………………………….9
2.3.1 薄板變形率張量……………………………………………………………9
2.3.2 投影算符(Projection operator) ….…………………………………………10
2.3.3 將三維問題簡化至二維 …………………………………………………13
2.4 薄板變形率:逆推問題 ……….. …………………………………………..14
2.4.1 總應變率功率 ……………………………………………………………14
2.4.2逆推隱沒流場 …………………………………….………………………15
2.4.2.a牛頓流體的線性逆推問題 .…………………………………………...15
2.4.2.b 指數率流體的非線性逆推問題 ……………...………………………..15
第三章 西北太平洋實驗
3.1 西北太平洋地震活動與板塊幾何 …....…………………………………….17
3.2 前人實驗 …………………………………………………………………….18
3.3 西北太平洋實驗 …………………………………………………………….23
第四章 非歐空間中的應變率相容方程式
4.1 共變微分(Covariant derivative)與平行性(Parallelism) ………….....……….27
4.2高斯理論(Gauss theorem egregium) …….………………..………..…………29
4.3 應變相容方程式……......………………….…..…………………..………….29
4.4 應變相容方程式回顧 …………………………………………..……………30
4.5 非歐空間中的應變率相容方程式 …………………………..………………31
第五章 結論與討論 ……………………………………………..……………….33
參考資料 ………………………………………………………..………………...34
附錄一推導非歐空間中的應變相容方程式 ……………….……………………37
附錄二 推廣的應變相容方程式在橢圓面上的應用 …….….………………….39
dc.language.isozh-TW
dc.subject高斯曲率zh_TW
dc.subject隱沒板塊zh_TW
dc.subject應變相容方程式zh_TW
dc.subjectsubductionen
dc.subjectGaussian curvatureen
dc.subjectcompatibility equationsen
dc.title隱沒板塊運動應變相容方程式之探討zh_TW
dc.titleCapatibility Conditions for the Kinematics of Subductionen
dc.typeThesis
dc.date.schoolyear94-2
dc.description.degree碩士
dc.contributor.coadvisor喬凌雲
dc.contributor.oralexamcommittee龔源成,郭本垣
dc.subject.keyword隱沒板塊,應變相容方程式,高斯曲率,zh_TW
dc.subject.keywordsubduction,compatibility equations,Gaussian curvature,en
dc.relation.page40
dc.rights.note有償授權
dc.date.accepted2006-07-28
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept地質科學研究所zh_TW
顯示於系所單位:地質科學系

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