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請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/37711
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor林銘崇
dc.contributor.authorWei-Ping Hungen
dc.contributor.author洪維屏zh_TW
dc.date.accessioned2021-06-13T15:39:54Z-
dc.date.available2008-07-11
dc.date.copyright2008-07-11
dc.date.issued2008
dc.date.submitted2008-07-08
dc.identifier.citation1. Bill Cooper and Frank Beiboer(2002) “Potential Effects Of Offshore Wind Developments On Coastal Processes”
2. Boussinesq, J. (1872) “Theorie des ondes et remous qui se propagent le long d,un canal rectangularire horizontal, en communiquant au liquide contenu dansce canal des vitesses sensiblement pareilles de la surface au,” J. Math. Pure et. Appl., 2nd Series, Vol.17, pp. 55-108.
3. Burcharth, H.F. and Andersen, O.H. (1995) “On the One-Dimensional Steady and Unsteady Porous Flow Equation,” Coastal Eng., Vol. 24, pp.233-257.
4. Dalrymple, R.A., Losada, M.A. and Martin, P.A. (1991) “Reflection and Transmission from Porous Structures under Oblique Wave Attack,” J. Fluid Mech., Vol. 224, pp.625-644.
5. Danish Hydraulic Institute,2000“MIKE 21 Coastal Hydraulic and Oceanography,”User Guide-Hydrodynamic Module.
6. Gobbi, M.F. and Kirby, J.T. (1999) “Wave Evolution over Submerged Sills: Tests of A High-order Boussinesq Model,” Proc. 25th Int. Conf. on Coastal Eng., pp.1116-1129.
7. Gobbi, M.F., Kirby, J.T. and Wei, G. (2000), “A Fully Nonlinear Boussinesq Model for Surface Waves, Part 2. Extended to ,” J. Fluid Mech., Vol. 405, pp. 181-210.
8. Grilli, S. T., Ioualalen, M., Asavanant, J., Shi, F., Kirby, J. T. and Watts, P. (2007) “Source constraints and model simulation of the December 26, 2004 Indian Ocean tsunami,” J. Waterway, Port, Coast. and Ocean Engrng., 133, pp. 414-428.
9. Hoffman, J.D. (1992), “Numerical Methods for Engineers and Scientists,” McGraw-Hill, Inc., New York.
10. Lin, C.C. and Clark A. (1959), “On the theory of shallow water waves, ”Tsing Hua J. of Chinese Studies, Special l, pp. 54-62.
11. Longuet-Higgins&Cartwright (1957), “The amplitude of waves reflected from a vertical circular cylinder,”NIO Internal Report No A9.
12. Madsen, P.A., Murray, R. and. Sørensen, O.R (1991) “A New Form of Boussinesq Equations with Improved Linear Dispersion Characteristics,” Coastal Eng. Vol. 15, pp. 371-388.
13. Madsen, P.A. and Sørensen, O.R. (1992) “A New Form of Boussinesq Equations with Improved Linear Dispersion Characteristics Part2. A slowly-varying bathymetry,” Coastal Eng. Vol.18, pp. 183-204. Vol. 21, pp.199-208.
14. Madsen, P.A., Bingham, H.B. and Liu, H. (2002) “A New Boussinesq Method for Fully Nonlinear Waves from Shallow to Deep Water,” J. Fluid Mech., Vol. 462, pp. 1-30.
15. McCowan, A.D. (1985) “Equation Systems for Modeling Dispersive Flow in Shallow Water,” Proc. 21st IAHR Congress, Melbourne, pp. 51-57.
16. McCowan, A.D. (1987) “The Range of Application of Boussinesq Type Numerical Short Wave Models,” Proc. 22nd IAHR Congress, Laussane, pp. 378-384.
17. Nwogu, O. (1993) “An Alternative Form the Boussinesq Equation for Near Shore Wave Propagation,” J. Waterway, Port, Coast Ocean Eng. ASCE, Vol. 119(6), pp.618-638.
18. Peregrine, D.H. (1967) “Long Wave on a Beach,” J. Fluid Mech., vol.27, pp. 815-827.
19. Sarpkaya,T.and Isaacson,M.(1981)“Mechanics of Wave Force on Offshore Structures,” Van Nostrand Rheinhold.ISBN 0-442-25402-4.
20. Schäffer, H.A. and Madsen, P.A. (1995) “Further Enhancements of Boussinesq-type Equations,” Coastal Eng. Vol. 26, pp.1-14.
21. Watts, P , Grilli , S.T., Kirby , J.K., Fryer , G.J. and Tappin , D.R.(2003), “Landslide Tsunami Case Studies Using A Boussinesq Model and A Fully Nonlinear Tsunami Generation Model, ” Natural Hazards and Earth System Sciences,3,pp.391-402.
22. Wei, G., Kirby, J.T., Grilli, S.T. and Subramanya, R. (1995) “Time-dependent Numerical Code for Extended Boussinesq Equations,” J. Fluid Mech., Vol. 294, pp. 71-92.
23. Wei, G., Kirby, J.T. and Sinha, A. (1999), “Generation of Waves in Boussinesq Equation Models Using a Source Function Method,” Coastal Eng., Vol. 36, pp. 271-299.
24. Witting, J.M. (1984), “A Unified Model for the Evolution of Nonlinear Water Waves,” J. of Computational Physics, Vol. 56, pp. 203-236.
25. Zheng, P. (1999) “A High-order Numerical Model for Waves and Curents Based on Boussinesq Equation,” Ph. D. dissertation of the University of Tokyo, Japan.
26. 林銘崇、丁肇隆、張國緯(2002)「應用Boussinesq方程式在一維波浪場上之數值計算」,海洋工程學刊,第2卷,第1期,15頁-31頁。
27. 許朝敏(2004)「波流場中波浪變形之研究」,博士論文,國立台灣大學。
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/37711-
dc.description.abstract本研究旨在運用Boussinesq equations,發展出一套數值模式,藉由此數值模式來模擬二維波浪通過圓形柱樁對波高變形之影響,理論模式方面,以Nwogu(1993)所推導以任意水深形式表示之二維布斯尼斯克方程式為基礎,數值模擬計算則採用Wei and Kirby (1995) 所提出之四階亞當斯-貝西福斯-摩頓之預測-修正法,配合造波函數及適當之消波邊界條件,來增加計算穩定性及節省計算時間。接著將所建立之數值模式與Sarpkaya and Isaacson(1981)及丹麥水利研究所之研究結果相互比較驗證後,模式的適用性相當良好。數值計算方面,首先於水深h=5m之等水深地形,分別給定T=3.5s、T=5s之規則波,探討波浪通過柱樁半徑R=3m之波高變形,由計算結果可知,設有雙根柱樁之計算領域,且此雙根柱樁位於同樣x座標,其柱樁前方因反射造成波高值約可達1.7倍入射波高,而設有四根柱樁之計算領域,最靠近造波邊界之柱樁,其前方波高值約可達1.8倍入射波高。此外,於變水深地形下,本模式也能模擬波浪通過群樁之波場變化,故本模式適用於模擬在等水深、變水深地形下,波浪通過圓形柱樁之波場變化。zh_TW
dc.description.abstractThe objective of the research is to apply Boussinesq equations to develop a series of numerical calculations to simulate the affaction of wavehight changes that because two dimensional wave passing through cylinders. This article is based on the concept of Nwogu (1993) that expressed by random depth and the fourth-order Adams-Bashforth-Moulton predictor-corrector scheme in coordination with source function and proper damping boundary conditions to increase the stability of calculation and to decrease the required processing time.The results are quite well in comparison with previous research. In the numerical calculation,first in the geography of 5 meters depth ,we think about that wave of the period is 3.5 seconds and 5 seconds pass through the cylinders of the radious is 3 meters and make waveheight changing.The two cases that one is setting two cylinders shows the wavehight that in the front of the cylinder is approximately 1.7 times the H0,and another is setting four cylinders shows the wavehight that in the front of the cylinder is approximately 1.8 times the H0. Additionally, the numerical calculation can to simulate that wave pass through a group of cylinders in different depth making wave transformations. So the numerical calculations apply to simulate wave pass through cylinders making wave transformations in constant depth、varying depth .en
dc.description.provenanceMade available in DSpace on 2021-06-13T15:39:54Z (GMT). No. of bitstreams: 1
ntu-97-R94525002-1.pdf: 5714869 bytes, checksum: 3340cf39dae76e624e0896ff980b9a2c (MD5)
Previous issue date: 2008
en
dc.description.tableofcontents目 錄
頁次
中文摘要 Ⅰ
英文摘要 Ⅱ
目 錄 Ⅲ
圖 目 錄 Ⅴ
符號說明 Ⅶ
第一章 緒論...... 1
1-1 研究目的...... 1
1-2 相關文獻回顧.. 2
1-3 本文組織...... 8
第二章 理論分析.. 10
2-1控制方程式及邊界條件.... 10
2-2無因次化方程式及其邊界條件....... 12
2-3波浪勢流函數之垂直向分佈函數..... 14
2-4微擾法(Perturbation Method).....16
第三章 數值方法.. 20
3-1基本方程式有限差分化.....21
3-1-1基本方程式.............21
3-1-2時間之離散式...........23
3-1-3空間之離散式...........25
3-2邊界條件.................28
3-2-1入射波邊界條件或造波邊界條件(Source function).....29
3-2-2完全反射邊界條件........30
3-2-3消波邊界條件 ........31
第四章 數值計算.. 33
4-1造波及消波邊界條件測試.. 33
4-2二維波浪傳遞數值模式驗證 ...36
4-2-1波浪通過防波堤之模擬....36
4-2-2波浪通過圓形柱樁之變形 .......38
4-3數值計算結果與討論..........42
4-3-1圓柱直徑與入射波長比值對波場之影響.....42
4-3-2波浪與圓柱在等水深地形下之交互作用.....48
4-3-3變水深地形群樁波場模擬 ............61
第五章 結論與建議.....64
5-1結論.....64
5-2建議.....65
參考文獻....66
dc.language.isozh-TW
dc.subject離岸風田zh_TW
dc.subjectOffshore Wind Farmen
dc.title離岸風田之波場分析zh_TW
dc.titleAnalysis of Wave Transformations around Offshore Wind Farmen
dc.typeThesis
dc.date.schoolyear96-2
dc.description.degree碩士
dc.contributor.oralexamcommittee陳陽益,丁肇隆,蕭松山,許朝敏
dc.subject.keyword離岸風田,zh_TW
dc.subject.keywordOffshore Wind Farm,en
dc.relation.page68
dc.rights.note有償授權
dc.date.accepted2008-07-08
dc.contributor.author-college工學院zh_TW
dc.contributor.author-dept工程科學及海洋工程學研究所zh_TW
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