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  1. NTU Theses and Dissertations Repository
  2. 工學院
  3. 土木工程學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/52363
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor黃燦輝(Tsan-Hwei Huang)
dc.contributor.authorChun-Jung Wuen
dc.contributor.author吳俊融zh_TW
dc.date.accessioned2021-06-15T16:12:51Z-
dc.date.available2015-08-20
dc.date.copyright2015-08-20
dc.date.issued2015
dc.date.submitted2015-08-18
dc.identifier.citation1.Barton N. (1973): Review of a new shear strength criterion for rock joints. Engineering Geology, 7: 287-332.
2.Barton N, Choubey V. (1977): The shear strength of rock joints in theory and practice. Rock Mech, 10: 1-54.
3.Bahaaddini M, Sharrock G, Hebblewhite B.K. (2013): Numerical direct shear tests to model the shear behaviour of rock joints. Computers and Geotechnics, 51: 101-115.
4.Cundall P.A. (2000): Numerical experiments on rough joints in shear using a bonded particle model. In: Lehner FK, Urai JL, editors. Aspects of tectonic faulting. Berlin: Springer; 1–9.
5.Chiu C.C, Wang T.T, Weng M.C, Huang T.H. (2013): Modeling the anisotropic behavior of jointed rock mass using a modified smooth-joint model. Int J Rock Mech Mining Sci., 62: 14-22.
6.Eberhardt E. (2003): Rock Slope Stability Analysis-Utilization of Advanced Numerical Techniques. Vancouver, Canada: Earth and Ocean Sciences, University of British Columbia.
7.Einstein H.H, Veneziano D, Baecher G.B, Oreilly K.J. (1983): The Effect of Discontinuity Persistence on Rock Slope Stability. Int J Rock Mech Mining Sci., 20: 227-236.
8.Grasselli G. (2001): Shear strength of rock joints based on quantified surface description. Ph.D. thesis, Swiss Federal Institute of Technology (EPFL), Lausanne, Switzerland.
9.Itasca Consulting Group Inc. (2008): PFC3D (particle flow code in 3 dimensions) version 4.0. Minneapolis: Itasca.
10.Ladanyi B, Archambault G. (1969): Simulation of Shear Behaviour of Jointed Rock Mass.Proc.11th Symposium on Rock Mechanics.(AIME), chapter 7, 105-125.
11.Lambert C, Coll C. (2014): Discrete modeling of rock joints with a smooth-joint contact model. journal of Rock Mechanics and Geotechnical Engineering, 6: 1-12.
12.Potyondy D.O, Cundall P.A. (2004): A bonded-particle model for rock. Int J Rock Mech Mining Sci., 41: 1329-1364.
13.Patton F.D. (1966): Multiple model of shear failure in rock. In: Proc. 1st Congr. Of ISRM, Libson, 509-513.
14.Park J.W, Song J.J. (2009): Numerical simulation of a direct shear test on a rock joint using a bonded-particle model. Int J Rock Mech Mining Sci., 46: 1315-1329.
15.Stead D, Eberhardt E, Coggan J.S. (2006): Developments in the characterization of complex rock slope deformation and failure using numerical modelling techniques. Engineering Geology, 83: 217-235.
16.Scholtès L, Donzé F.V. (2014): A DEM analysis of step-path failure in jointed rock slopes. Comptes Rendus Mecanique.
17.羅佳明等人(2011):國道3號七堵順向坡滑動過程之動態模擬,中華水土保持學報,42: 175-183。
18.許凱翔(2014):以數值模擬岩石節理面之剪力行為,國立中央大學土木工程學研究所碩士論文。
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/52363-
dc.description.abstract岩石邊坡常含有多組節理面,其為影響岩石邊坡穩定性的關鍵。目前分析節理岩坡穩定性的主要方式,多視其為連續體,並以極限平衡分析或連續體數值分析等方法進行探討,然而,對於分析節理岩坡中岩塊滑動破壞及塊體大量位移問題,節理面的力學行為具有極大的影響力,因此,透過能考慮分離塊體力學行為的離散元素法進行節理岩坡之穩定性分析,將可提供一更精確之預測。
本研究應用PFC3D軟體作為離散元素分析之工具,然而,因PFC在模擬節理面時過度簡化,無法合理反映具粗糙度節理面之力學行為,故本研究透過本團隊提出的修正平滑節理模式(Modified Smooth-Joint Model, 簡稱MSJ模式)模擬節理面力學特性。MSJ模式以Barton之剪力強度準則為基礎,由各項節理參數決定其力學特性。研究將先以數值直剪試驗驗證MSJ模式之準確性,接著建置簡易岩坡模型,探討其於極限平衡分析與節理參數之關係,然後再探討節理連續性之影響,並討論MSJ模式應用於岩坡破壞分析之可行性。
在驗證MSJ模式部分,研究首先由單軸壓縮試驗結果檢驗完整岩石微觀參數的正確性;接續以直剪試驗結果驗證節理面參數之合理性;最後檢驗直剪模擬結果與Barton之剪力強度模式是否相符,並與未修正之SJ模式互相對照。試驗結果經比較後,發現MSJ模式能合理表現出Barton模式中尖峰剪力強度隨正向應力變化之趨勢,而SJ模式在較粗糙的節理面則無法呈現出差異。
簡易岩坡分析部分,研究將以單一節理之梯形邊坡進行。首先依極限平衡理論,改變節理摩擦角參數設置,分析節理傾角與摩擦角關係;再來以改良的MSJ模式,探討節理面上摩擦角空間分佈差異,藉此瞭解節理面上正向應力作用的影響;最後將連續的節理面改為具岩橋之不連續節理,透過岩坡之變形及破壞分析,依序探討節理連續性、完整岩石強度與岩橋型式對岩坡穩定性造成的影響。
透過岩坡的各項數值模擬結果發現,在岩坡中,即使節理摩擦角小於傾角,坡體也未必發生滑動,此異於以往無限邊坡之極限平衡分析;節理面摩擦角會隨上部塊體重量分佈而改變,此特性反映出具粗糙度節理面力學行為受正向應力之影響;若節理面不連續,則節理破裂發展與岩橋長度與型式有關,且岩橋破壞將導致上部塊體滑動。未來可進一步模擬實際岩坡,以利於工程分析與設計之評估。
zh_TW
dc.description.abstractRock slope often contains discontinuities such as joints, which is the key factor of rock slope stability. Conventionally, the limit equilibrium analysis and continuum numerical analysis are most used method for stability of jointed rock slope. However, the mechanical behavior of joint surface influence the sliding failure of rock block and massive transfer of block in jointed rock slope extremely. Therefore, the discrete element analysis which can consider the mechanical behavior of discrete block is an effective way to investigate the stability of jointed rock slope.
In this study, PFC3D software is choose as the discrete element analysis tool, however, PFC is over-simplify in simulate joint surface behavior, thus it cannot react the mechanical behavior of roughness joint surface. Therefore, this study simulates the mechanical characteristic of joint surface through the improved method - Modified Smooth-Joint Model (MSJ model) which is developed by our research team. The MSJ model is based on Barton's shear strength criterion, the mechanical behaviors are determined by various joint parameters. This study first verify out the accuracy of MSJ model by numerical direct shear tests, then we construct a simple rock slope model to discuss the relationships between limit equilibrium analysis and joint parameters, and then the influence of joint continuity is investigated, finally discuss about the application of the MSJ model on rock slope failure analysis.
In the part of MSJ model verification, we first to examine the reliability of intact rock micro-parameters through the simulation data of uniaxial compress test; then the rationality of joint parameters are verified by the results of direct shear test; finally, the simulation results of direct shear test and Barton's shear strength model are compared to ensure that they are equal, and the SJ model is treated as the control group. The comparison shows MSJ model can reasonably represent the trend of Barton's model which shows friction angle is correlate with normal stress, while SJ model cannot point out this important characteristic in roughness joint.
In the section of simple rock slope analysis, trapezoid slope with single joint is used in the simulation. The first step is changing the joint friction angle parameters to analyze the relationship between the joint friction angle and dip angle according to the limit equilibrium theory; second, the revised MSJ model is used to investigate the spatial distribution of friction angle to recognize the influence of normal stress acted on joint surface; finally, the continuous joints are alter to discontinuous joints to simulate the effect of rock bridge, and then sequentially investigate the influence of joint persistence, intact rock strength and rock bridge type to the rock slope stability through failure analysis of rock slope.
According to the simulation results of simple rock slope, there are some conclusions and suggestions of the MSJ model. The simulation results show that even joint friction angle is lower to dip angle, the slope is not necessarily to slip in numerical rock slope. We suggest that three-dimensional limit equilibrium analysis can be adapted in future to correct the settings of numerical model; joint friction angles is vary with the distribution of upper block weight, this feature shows the mechanical behavior of roughness joint is influence by normal stress; if joint surface is discontinuous, the crack distribution are correlate to the length and type of rock bridges, and the failure of rock bridge will cause upper block to slide. We recommended that MSJ model can be used to simulate real rock slope in the future, and exploring the complex mechanism of jointed rock slope failure to evaluate the analysis and design of geo-engineering.
en
dc.description.provenanceMade available in DSpace on 2021-06-15T16:12:51Z (GMT). No. of bitstreams: 1
ntu-104-R02521109-1.pdf: 17695032 bytes, checksum: 6530e400acc27400fcf1f9af1c7ef0fe (MD5)
Previous issue date: 2015
en
dc.description.tableofcontents誌謝 I
摘要 II
ABSTRACT III
目錄 V
表目錄 VIII
圖目錄 IX
第一章 緒論 1
1.1 研究動機與目的 1
1.2 研究流程與方法 2
1.3 論文架構 3
第二章 文獻回顧 4
2.1 節理面剪力強度模式 4
2.1.1 Patton's Bilinear model(1966) 4
2.1.2 Ladanyi與Archambault(1970) 5
2.1.3 Barton's model(1973) 5
2.2 PFC中節理面的模擬方法 6
2.2.1 鍵結消除法 6
2.2.2 平滑節理模式 8
2.2.3 修正平滑節理模式 8
2.3 直接剪力試驗之數值模擬 9
2.3.1 Park與Song(2009) 9
2.3.2 Bahaaddini,Sharrock與Hebblewhite(2013) 11
2.3.3 Lambert與Coll(2014) 13
2.4 MSJ模式模擬節理岩體破壞行為 14
2.5 節理岩坡數值分析研究 15
2.5.1 Stead等人(2006) 15
2.5.2 Scholtès與Donzé(2014) 16
2.5.3 羅佳明等人(2011) 18
第三章 數值模型方法 20
3.1 PFC3D模擬原理與架構 20
3.1.1 PFC3D軟體簡介 20
3.1.2 顆粒接觸模式 21
3.1.3 FISH程式語言 26
3.2 MSJ模式之理論與驗證 27
3.2.1 基本理論 27
3.2.2 直剪模擬之完整岩石參數設置 29
3.2.3 節理面參數設置 30
3.2.4 直接剪力試驗模擬流程 31
第四章 數值模型驗證 35
4.1 直接剪力試驗參數驗證 35
4.1.1 模擬顆粒尺寸之影響 35
4.1.2 岩石材料之參數分析 36
4.1.3 節理面參數 38
4.2 MSJ模式之驗證 40
4.2.1 尖峰剪力強度 40
4.2.2 尖峰膨脹角 43
第五章 節理岩坡數值分析 46
5.1 岩坡數值模型建置與假設 46
5.1.1 簡易邊坡模型建置 46
5.1.2 簡易邊坡模型基本假設 47
5.1.3 顆粒單位重修正 49
5.2 極限平衡分析結果之探討 49
5.2.1 極限平衡理論 50
5.2.2 破壞發生之臨界摩擦角分析 50
5.3 節理參數分析 54
5.3.1 MSJ數值模型修正 54
5.3.2 節理面摩擦角分析 55
5.4 節理連續性分析 61
5.4.1 參數選擇與模型假設 61
5.4.2 模型參數驗證 62
5.4.3 岩橋面積分析 64
5.4.4 鍵結強度參數分析 66
5.4.5 岩橋型式分析 69
5.4.6 節理面強度參數分析 74
第六章 結論與建議 78
6.1 結論 78
6.2 建議 78
參考文獻 80
附錄 論文口試-問題與答覆 82
dc.language.isozh-TW
dc.subject離散元素分析zh_TW
dc.subjectPFCzh_TW
dc.subject節理岩坡zh_TW
dc.subjectMSJ模式zh_TW
dc.subjectjointed rock slopeen
dc.subjectdiscrete element analysisen
dc.subjectPFCen
dc.subjectMSJ modelen
dc.title修正平滑節理模式於節理岩坡之破壞分析zh_TW
dc.titleFailure Analysis of Jointed Rock Slopes Based on a Modified Smooth-Joint Modelen
dc.typeThesis
dc.date.schoolyear103-2
dc.description.degree碩士
dc.contributor.coadvisor翁孟嘉(Meng-Chia Weng)
dc.contributor.oralexamcommittee王泰典,李宏輝
dc.subject.keyword節理岩坡,離散元素分析,PFC,MSJ模式,zh_TW
dc.subject.keywordjointed rock slope,discrete element analysis,PFC,MSJ model,en
dc.relation.page84
dc.rights.note有償授權
dc.date.accepted2015-08-18
dc.contributor.author-college工學院zh_TW
dc.contributor.author-dept土木工程學研究所zh_TW
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