博碩士論文 962202009 詳細資訊




以作者查詢圖書館館藏 以作者查詢臺灣博碩士 以作者查詢全國書目 勘誤回報 、線上人數:36 、訪客IP:18.219.22.169
姓名 黃冠華(Kuan-Hua Huang)  查詢紙本館藏   畢業系所 物理學系
論文名稱 剛體球在不對稱垂直震盪系統中的動力學行為
(Hard Spheres Dynamics in Asymmetrical Vertical Vibrating Systems)
相關論文
★ 庫倫作用粒子之動力學★ 帶電粒子在離子流中之交互作用
★ 肥皂膜上的能量耗散★ 紙片落下之行為研究
★ 外加場下肥皂膜的能量耗散★ 圓柱體在二維垂直肥皂膜之動力學
★ 螺旋狀物體在剪切流中的運動行為★ 二元高分子薄膜在平行電場下的相分離
★ 纖毛不對稱運動的模擬★ 肥皂膜流場中圓柱體之行為研究
★ 單向偶極子形成的柱狀結構與非均勻電解質的平均場理論★ 彈性懸掛棍在旋轉系統下之行為
★ 膠體球在電解質溶液中的擴散泳★ 細長彈性桿在旋轉下的非線性動力行為與動態穩定性分析
★ Thermophoresis and Diffusiophoresis in Brownian Simulation with Velocity Distribution Function★ Water Strider Locomotion
檔案 [Endnote RIS 格式]    [Bibtex 格式]    [相關文章]   [文章引用]   [完整記錄]   [館藏目錄]   [檢視]  [下載]
  1. 本電子論文使用權限為同意立即開放。
  2. 已達開放權限電子全文僅授權使用者為學術研究之目的,進行個人非營利性質之檢索、閱讀、列印。
  3. 請遵守中華民國著作權法之相關規定,切勿任意重製、散佈、改作、轉貼、播送,以免觸法。

摘要(中) 我們觀察鋼球在三種不同的不對稱且垂直震盪的環形容器中的行為。首先,這個環形的容器底部被刻鑿了放射狀的不對稱溝槽,使得球會往一個方向移動。我們測量了在不同的震盪振幅與頻率下的平均角速度。減掉平均速度之後的速度分佈符合Gaussian 分佈,而減掉平均速度之後的位置平方與時間的關係,使我們獲得了擴散係數。假設底板給球的推進力為Fd,而此力所建立的位能場為U=Fd Rθ當記錄球位置的分佈機率,再用Maxwell-Boltzmann 與它匹配,我們便可知道這個力的大小。搭配上之前求出的平均速度我們可以得到溫度與摩擦係數的比值。將這個比值與擴散係數做比較,可得知此實驗系統符合Einstein-Smoluchowski 理論。我們也將許多顆球放入系統中,用磁場改變球的密度,它們集體的行為,例如等效的溫度等,將會因為密度的不同而改變。在其他的實驗中,鋼球將被放入不對稱邊界的容器中,平均速度與震動振幅的關係將會被記錄下來。而當鋼球被放入有不對稱位能場的容器中時,它的動力學行為隨著振幅的增加有三個步驟,從被困住,前進,到隨機移動。移動的軌跡顯示,其主要的原因是磁場可以幫助改變方向,使它可以在容器中移動較長的距離,而這個機制在兩個方向是不對稱的,這使得球可以朝某個特定方向移動。在這三種不對稱的系統中,球的速度都不會因提高振動的振幅而無限量的增加。
摘要(英) We observe the dynamics of steel spheres in three kinds of asymmetric annular cells vibrated vertically. First, the annular cell is carved with asymmetric troughs in the bottom and the spheres are continuously driven to move in one direction. The average angular velocities of the spheres in different vibration frequencies and amplitudes are measured. The velocity distribution of the deviation from the average velocity is shown to follow the Gaussian distribution. According to the displacement deviation from the average velocity, the diffusion constant is obtained. When the spheres are confined in one region of the cell, we assume the potential isU=Fd Rθand fit the density distribution with Boltzmann distribution to get the driving force Fd. Using the driving force and the average velocity, we can get the ratio of the effective temperature and the drag coefficient. Comparing this ratio with the diffusion constant, the behavior fit Einstein-Smoluchowski theory. We put multiple spheres in the cell and add magnet under the cell to control the magnetic field which change the density distribution of the spheres. It is found that the collective behaviors like effective temperature change in different densities. The relation between the average angular velocity and the non-uniform density is also reported. In other experiments, the sphere is put in the asymmetrical boundary systems. The sphere transports. The relation of the vibrate amplitudes and the average velocity is brought up. When we add asymmetrical magnetic field on a symmetrical system. The behavior of the sphere change from trapped, transport, to moving randomly. The trajectories of the sphere show how the magnetic field change the sphere’s direction. This mechanism is asymmetrical in two direction which makes the sphere move in one direction. The transport velocity can’t increase infinite in these three methods.
關鍵字(中) ★ 複雜流體
★ 粒狀流體
★ 垂直震盪
★ 不對稱系統
關鍵字(英) ★ granular fluid
★ complex fluid
★ vertical vibrate
★ asymmetrical system
論文目次 1 Introduction 1
1.1 Maxwell-Boltzmann distribution. . . . . . . . . . . . . . . . . 3
1.2 Einstein-Smoluchowski theory . . . . . . . . . . . . . . . . . . 5
2 Apparatus and experiment 8
2.1 Whole apparatus . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.2 Composition of the cells . . . . . . . . . . . . . . . . . . . . . 8
2.3 The measurement of the experiment . . . . . . . . . . . . . . 13
2.3.1 In symmetric container . . . . . . . . . . . . . . . . . . 13
2.3.2 In asymmetric bottom container . . . . . . . . . . . . 13
2.3.3 Confined region in asymmetric bottom container . . . 15
2.3.4 Horizontal calibration . . . . . . . . . . . . . . . . . . 16
3 Result and Discussion 19
3.1 One sphere in the asymmetrical bottom system . . . . . . . . 19
3.2 Multiple spheres in the asymmetrical bottom system . . . . . 23
3.3 Multiple spheres in the asymmetrical bottom and potential
system . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26
3.4 The asymmetrical boundary system . . . . . . . . . . . . . . . 27
3.5 The asymmetrical potential system . . . . . . . . . . . . . . . 29
4 Conclusion 43
參考文獻 [1] H. M. Jaeger, S. R. Nagel, and R. P. Behringer, Rev. Mod. Phys. 68, 1259 (1996).
[2] Florence Rouyer and Narayanan Menon, Phys. Rev. Lett. 85, 3676–3679 (2000).
[3] T. P. C. van Noije and M. H. Ernst, Granular Matter 1, 57 (1998).
[4] J. J. Brey, D. Cubero, and M. J. Ruiz-Montero, Phys. Rev. E 59, 1256 (1999).
[5] V. Kumaran, Phys. Rev. E 59, 4188 (1999).
[6] G. W. Baxter and J. S. Olafsen, Nature 425, 680-680 (2003).
[7] J. S. van Zon and F.C. MacKintosh, Phys. Rev. Lett. 93, 038001 (2004).
[8] P. M. Reis, R. A. Ingale, and M. D. Shattuck, Phys. Rev. E 75, 051311 (2007).
[9] S. Bleil, P. Reimann, and C. Bechinger, Phys. Rev. E 75, 031117 (2007).
[10] W. Mu, Z. Liu, L. Luan, G. Wang, G. C. Spalding, and J. B. Ketterson, New Journal of Physics 11, 103017 (2009).
[11] Dirk Helbing, Reviews of Modern Physics 73, 1067 (2001).
[12] Yuki Sugiyama, Minoru Fukui, Macoto Kikuchi, Katsuya Hasebe, Akihiro Nakayama, Katsuhiro Nishinari, Shin-ichi Tadaki and Satoshi Yukawa, New journal of Physics 10, 033001 (2008).
指導教授 陳培亮(Peilong Chen) 審核日期 2010-8-5
推文 facebook   plurk   twitter   funp   google   live   udn   HD   myshare   reddit   netvibes   friend   youpush   delicious   baidu   
網路書籤 Google bookmarks   del.icio.us   hemidemi   myshare   

若有論文相關問題,請聯絡國立中央大學圖書館推廣服務組 TEL:(03)422-7151轉57407,或E-mail聯絡  - 隱私權政策聲明