Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane

碩士 === 國立中興大學 === 機械工程學系 === 85 === In the present paper, the topography of rough surface is simulated by using thefractal geometry. The mathematically created rough surface is brought in contact with a flat surface under a normal loading. the relationshi...

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Main Authors: Shyy, Jaan Horng, 史展宏
Other Authors: You H. I.
Format: Others
Language:zh-TW
Published: 1997
Online Access:http://ndltd.ncl.edu.tw/handle/66498905238345447590
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spelling ndltd-TW-085NCHU04890132015-10-13T12:15:17Z http://ndltd.ncl.edu.tw/handle/66498905238345447590 Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane 以Fractal模擬之粗糙面與平板間之實際接觸面積及負荷之分析 Shyy, Jaan Horng 史展宏 碩士 國立中興大學 機械工程學系 85 In the present paper, the topography of rough surface is simulated by using thefractal geometry. The mathematically created rough surface is brought in contact with a flat surface under a normal loading. the relationship of real contact area versus the contact loading was then investigated.In general, the governing parameters of the fractal geometry,i.e., D1,A1 and Wcare obained from the power spectrum of the rough surface being simulated. Thereal contact area and contact loading are calculated by virtue of the Hertziantheory. The criterion for the contact asperity being elastic or plastic is provided.It is found that the height distribution of the rough surface created by thefractal geometry has a random nature which satisfiesthe normal distribution. Variation in the parameter D1 is the primary role to simulate the rough surface. Due to plastic deformation, the rough surface creates rapidly the conatct area under loading. Constant real contact pressure, which is larger fora rough surface, is obained for every contact surfaces. You H. I. 游憲一 1997 學位論文 ; thesis 66 zh-TW
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description 碩士 === 國立中興大學 === 機械工程學系 === 85 === In the present paper, the topography of rough surface is simulated by using thefractal geometry. The mathematically created rough surface is brought in contact with a flat surface under a normal loading. the relationship of real contact area versus the contact loading was then investigated.In general, the governing parameters of the fractal geometry,i.e., D1,A1 and Wcare obained from the power spectrum of the rough surface being simulated. Thereal contact area and contact loading are calculated by virtue of the Hertziantheory. The criterion for the contact asperity being elastic or plastic is provided.It is found that the height distribution of the rough surface created by thefractal geometry has a random nature which satisfiesthe normal distribution. Variation in the parameter D1 is the primary role to simulate the rough surface. Due to plastic deformation, the rough surface creates rapidly the conatct area under loading. Constant real contact pressure, which is larger fora rough surface, is obained for every contact surfaces.
author2 You H. I.
author_facet You H. I.
Shyy, Jaan Horng
史展宏
author Shyy, Jaan Horng
史展宏
spellingShingle Shyy, Jaan Horng
史展宏
Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane
author_sort Shyy, Jaan Horng
title Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane
title_short Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane
title_full Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane
title_fullStr Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane
title_full_unstemmed Analysis of Real Contact Area and Contact Loading between a Fractal Rough Surface and a Flat Plane
title_sort analysis of real contact area and contact loading between a fractal rough surface and a flat plane
publishDate 1997
url http://ndltd.ncl.edu.tw/handle/66498905238345447590
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