| 研究生: |
陳昭銓 Chen, Chao-Chuan |
|---|---|
| 論文名稱: |
邊界元素法分析二維局部無窮域異向性之熱傳問題 Boundary Element Analysis of 2D Anisotropic Heat Conduction Problem with Partially Infinite Domain |
| 指導教授: |
夏育群
Shiah, Yui-Chuin |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 航空太空工程學系 Department of Aeronautics & Astronautics |
| 論文出版年: | 2022 |
| 畢業學年度: | 110 |
| 語文別: | 中文 |
| 論文頁數: | 100 |
| 中文關鍵詞: | 邊界元素法 、二維異向熱傳問題 、無窮域 、局部無窮域 |
| 外文關鍵詞: | Boundary Element Method, 2D anisotropic heat conduction, Infinite plane, partially infinite plane |
| 相關次數: | 點閱:155 下載:0 |
| 分享至: |
| 查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報 |
本論文探討邊界元素法分析無窮域至局部無窮域的熱傳問題時的基本解。由於邊界元素法無需在內部作網格分割,因此其在無窮域分析上就有其優勢。對此有許多學者(如Wrobel【1】)有提出無窮域之基本解會有額外項,雖然提出的方法是用在等向性材料,不過利用映向點Shiah and Tan【9】可以將在無窮域平面的異向性材料扭曲成等向性材料藉此方便運算,在【1】提出半無窮等向性平面之基本解可以增加映向源點來求解,這個源點則是運用鏡射來找出。在本文中利用【9】的方法就能將異向材料轉成等效的等向性材料。再利用相同方法找四分之一無窮域,不過只能用在正交材料上,這是因為異向性材料的映射點扭曲後的四分之一域會變成非正交的楔形域,迫使為滿足邊界條件造成了額外的困難。
使用針對無窮域以及局部無窮域而修改的基本解,就不需要在無窮遠處或者局部無窮域的表面上畫網格,利用這一優勢,BEM在模擬無窮與局部無窮域熱傳問題上比起其他數值工具要來的更有效率。公式都在邊界元素法的程式碼中實現,為了驗證方法的準確性,最後給了數個範例。
關鍵字:邊界元素法、二維異向熱傳問題、無窮域、局部無窮域
This paper discusses the fundamental solutions of the boundary element method to analyze the heat conduction in an infinite/ partially infinite medium. Due to the distinctive feature of boundary discretization, the boundary element method is especially advantageous in modeling infinite domain. Many scholars (e.g Wrobel [1]) have proposed the fundamental solution of the infinite domain with an extra term. Although the proposed treatments are simply for isotropic media, the similar process can be applied to anisotropic cases when the anisotropic domain can be mapped to the equivalent “isotropic one” in infinite plane as proposed by Shiah and Tan [9]. It was proposed in [1] that the fundamental solutions to the half-infinite isotropic plane could be obtained by posing additional mapping point of the source point using the relation of mirror-mapping. In the thesis, this methodology is applied to the equivalent “isotropic” domain when the anisotropic medium is transformed by the formulations proposed in [9]. Also, the same treatment is applied to a quarter of the infinite domain; however, only orthotropic properties are allowed. This is because the mapping of anisotropy shall distort the quadrant domain into a non-orthogonal wedge-like domain, presenting extra difficulties to satisfy the boundary conditions.
By using the fundamental solutions modified for the infinite/partially infinite domain, no meshes are required to model the far-field and the partially infinite surfaces. Taking this advantage, the BEM is more efficient in modeling the heat conduction in the infinite/partially infinite plane as compared with other numerical tools. All formulations are implemented in an existing BEM code. For verifications of the veracity, several examples are studied in the end.
Keywords: Boundary Element Method, 2D anisotropic heat conduction, Infinite plane, partially infinite plane
[1]L. C. Wrobel, The boundary element method, volume 1: Applications in thermo-fluids and acoustics. John Wiley & Sons, 2002.
[2] G. E. Blandford, A. R. Ingraffea, and J. A. Liggett, "Two?dimensional stress intensity factor computations using the boundary element method," International Journal for Numerical Methods in Engineering, vol. 17, no. 3, pp. 387-404, 1981.
[3] J. DeSanto and P. Martin, "On the derivation of boundary integral equations for scattering by an infinite two-dimensional rough surface," Journal of Mathematical Physics, vol. 39, no. 2, pp. 894-912, 1998.
[4] E. Heymsfield, "Infinite domain correction for anti?plane shear waves in a two?dimensional boundary element analysis," International Journal for Numerical Methods in Engineering, vol. 40, no. 5, pp. 953-964, 1997.
[5] A. Houmat, "Mapped infinite p-element for two-dimensional problems of unbounded domains," Computers and Geotechnics, vol. 35, no. 4, pp. 608-615, 2008.
[6] B. Travis, P. Olson, and G. Schubert, "The transition from two-dimensional to three-dimensional planforms in infinite-Prandtl-number thermal convection," Journal of Fluid Mechanics, vol. 216, pp. 71-91, 1990.
[7] C. Wang, F. Wang, and Y. Gong, "Analysis of 2D heat conduction in nonlinear functionally graded materials using a local semi-analytical meshless method," Aims Math, vol. 6, no. 11, pp. 12599-12618, 2021.
[8] O. D. Kellogg, Foundations of potential theory. Courier Corporation, 1953.
[9] Y. Shiah and C. Tan, "BEM treatment of two-dimensional anisotropic field problems by direct domain mapping," Engineering Analysis with boundary elements, vol. 20, no. 4, pp. 347-351, 1997.
[10] M. Yang, K. Park, and P. Banerjee, "2D and 3D transient heat conduction analysis by BEM via particular integrals," Computer Methods in Applied Mechanics and Engineering, vol. 191, no. 15-16, pp. 1701-1722, 2002.
[11] M. Tanaka, T. Matsumoto, and Q. F. Yang, "Time-stepping boundary element method applied to 2-D transient heat conduction problems," Applied Mathematical Modelling, vol. 18, no. 10, pp. 569-576, 1994.
[12] C. Dong, "Shape optimizations of inhomogeneities of two dimensional (2D) and three dimensional (3D) steady state heat conduction problems by the boundary element method," Engineering Analysis with Boundary Elements, vol. 60, pp. 67-80, 2015.
[13] Y. Shiah and C.-L. Tan, "BEM treatment of three-dimensional anisotropic field problems by direct domain mapping," Engineering Analysis with boundary elements, vol. 28, no. 1, pp. 43-52, 2004.
[14] Y. Shiah and C. -L Tan, "BEM treatment of two-dimensional anisotropic field problems by direct domain mapping," Engineering Analysis with boundary elements, vol. 20, no. 4, pp. 347-351, 1997.
[15] Y. Shiah, R.-B. Yang, and P.-W. Hwang, "Heat conduction in dissimilar anisotropic media with bonding defects/interface cracks," Journal of Mechanics, vol. 21, no. 1, pp. 15-23, 2005.
[16] J. Luo, Y. Liu, and E. Berger, "Analysis of two-dimensional thin structures (from micro-to nano-scales) using the boundary element method," Computational Mechanics, vol. 22, no. 5, pp. 404-412, 1998.
校內:2027-09-21公開