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研究生: 王秉成
Wang, Ping-Chung
論文名稱: µ(I)-rheology流體在地形座標系統上之應用
An application of µ(I)-rheology flows in terrain-fitted coordinate system
指導教授: 戴義欽
Tai, Yih-Chin
學位類別: 碩士
Master
系所名稱: 工學院 - 水利及海洋工程學系
Department of Hydraulic & Ocean Engineering
論文出版年: 2015
畢業學年度: 103
語文別: 中文
論文頁數: 64
中文關鍵詞: rheology地形座標系統顆粒流
外文關鍵詞: rheology, terrain-fitted coordinate system, granular flow
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  • 近年來由於全球氣候異常的因素,導致降雨量的暴增,使得土石流、山崩
    等自然災害發生的頻率越來越高,直接的影響到人民的生命財產安全,為了有效的去預測這些自然災害的影響範圍以及危害程度,我們可以藉由研究顆粒體的運動行為,來推估其流動特性。傳統的做法是透過實驗方法來進行探討,不過近年來透過應用數值模擬的方法,來進行顆粒流之研究也漸日益蓬勃發展。
    本文的研究重點是著重在控制方程式中的摩擦項,以往在模擬顆粒的崩塌行為時,通常是採用庫倫摩擦力,本研究則是將Pouliquen & Forterre (2002)所提出的μ(I)-rheology 應用在摩擦項及對流項中,去探μ(I)-rheology 在變動地形上對流體行為的影響,包括土體厚度、土體滑移的距離等,且將控制方程式拓展至三維現地地形,並使用地形座標系(Tai and Kuo, 2008、Tai et al., 2012)將控制方程式建立在隨底床變動的座標軸上,以此來描述顆粒流的動態行為。

    In recent years, due to abnormal climate factors, result in a surge of rainfall, it may increase the frequency of debris flow or landslides occusrs. It also affect people's lives and properties. In order to effectively predict the range of these natural disasters, we can study particle behavior of movement to estimates its flow characteristics. The traditional approach is through experimental methods, but for the past few years, the application of numerical simulation methods to study the granular flows has developed gradually.
    In this paper, we focus on the friction term in the momentum equation.In the past, simulating the collapse behavior of particle usually used Coulomb friction, but we apply μ(I)-rheology to friction term and convection term to explore fluid behavior of the change in terrain, including thickness, run-out distance of granular flows. In addition, governing equation was extended to two-dimensional terrain, by using the terrain-fitted coordinate system to governing equation base on changes in the bed with the coordinate axes. To describe the dynamic behavior of granular flow.

    第一章 緒論 1 1.1 研究背景 1 1.2 研究動機與目的 5 1.3 研究方法 6 1.4 論文架構 7 第二章 文獻回顧 8 2.1 土石流研究之發展 8 第三章 地形座標系統及理論 12 3.1 地形座標系統(Terrain-fitted coordinate) 12 3.2 控制方程式 15 3.2.1 質量守恆 15 第四章 μ(I)-rheology 的應用與探討 21 4.1 μ(I)-rheology 之參數 21 4.2 μ(I)-rheology 於控制方程式之應用 25 4.3 在卡式座標系統下,μ(I)-rheology 應用於一維之控制方程式 28 4.4 在卡式座標系統下,μ(I)-rheology 應用於二維之控制方程式 29 4.5 μ(I)-rheology 之參數討論 31 4.5.1 不同的h/L,相同的β,μ-Fr 之關係圖 31 4.5.2 相同的 h/L,不同的β,μ-Fr 之關係圖 32 4.5.3 相同的β,不同的Fr,μ-h/L 之關係圖 34 4.5.4 不同的L/β,νF-θ 關係圖 35 4.6 在地形曲面座標系統下,μ(I)-rheology 應用於一維之控制方程式 37 4.7 在地形曲面座標系統下,μ(I)-rheology 應用於二維之控制方程式 38 第五章 數值方法 40 5.1 NOC scheme 40 第六章 結果與討論 44 6.1 μ(I)-rheology 於控制方程式之運用 44 6.1.1 μ(I)-rheology 與庫倫摩擦力對土體崩塌之一維模擬結果 45 6.1.2 μ(I)-rheology 裡不同參數值對土體崩塌之一維模擬結果 47 6.1.3 土體滑落過程中,μ 值隨位置的變化關係 49 6.1.4 摩擦項使用庫倫摩擦力,模擬二維之土石崩塌 52 6.1.5 摩擦項使用μ(I)-rheology,沒有考慮擴散項,模擬二維之土石崩塌 54 6.1.6 摩擦項使用μ(I)-rheology,模擬二維之土石崩塌 56 6.1.7 不同摩擦項的條件下,二維之土石崩塌的比較結果 58 第七章 結論與建議 60 參考文獻 62

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