机械工程学报
機械工程學報
궤계공정학보
CHINESE JOURNAL OF MECHANICAL ENGINEERING
2014年
17期
107-123
,共17页
田红亮%钟先友%赵春华%赵新泽%方子帆%刘芙蓉%朱大林%林卫共%晏红
田紅亮%鐘先友%趙春華%趙新澤%方子帆%劉芙蓉%硃大林%林衛共%晏紅
전홍량%종선우%조춘화%조신택%방자범%류부용%주대림%림위공%안홍
微动结合面%法向接触载荷%法向接触刚度%弹性变形%塑性变形
微動結閤麵%法嚮接觸載荷%法嚮接觸剛度%彈性變形%塑性變形
미동결합면%법향접촉재하%법향접촉강도%탄성변형%소성변형
fretting joint interfaue%normal contact load%normal contact stiffness%elastic deformation%plastic deformation
基于Hertz弹性理论及分形几何学理论,以粗糙表面突峰变形特征、表面突峰承受法向接触载荷的光滑性和连续性为基础以及严格区分弹性变形和塑性变形,构架微动结合面的一种法向接触校对分形模型。导出表面突峰法向弹性接触载荷和表面突峰法向变形量之间的幂函数方程,提出微动结合面2个突峰之间互相作用的法向接触刚度的求导函数而非偏导函数求解准则。数值仿真曲线揭示:对于给定的法向接触载荷,随着分形维数的增加,实际接触面积首先增加然后降低;增加法向接触载荷或降低表面粗糙度都将增大实际接触面积;微动结合面法向接触刚度随着实际接触面积、法向接触载荷、相关因子或材料性能参数的增大而增大,而随着分形粗糙度的加大而降低;分形维数在较小范围内,微动结合面法向接触刚度随着分形维数从1变大而增强;但分形维数在较大范围内,微动结合面法向接触刚度时常随着分形维数的加大接近于2而降低。微动结合面法向接触校对分形模型的构思,能深入研究微动两粗糙表面之间的实际接触状态。
基于Hertz彈性理論及分形幾何學理論,以粗糙錶麵突峰變形特徵、錶麵突峰承受法嚮接觸載荷的光滑性和連續性為基礎以及嚴格區分彈性變形和塑性變形,構架微動結閤麵的一種法嚮接觸校對分形模型。導齣錶麵突峰法嚮彈性接觸載荷和錶麵突峰法嚮變形量之間的冪函數方程,提齣微動結閤麵2箇突峰之間互相作用的法嚮接觸剛度的求導函數而非偏導函數求解準則。數值倣真麯線揭示:對于給定的法嚮接觸載荷,隨著分形維數的增加,實際接觸麵積首先增加然後降低;增加法嚮接觸載荷或降低錶麵粗糙度都將增大實際接觸麵積;微動結閤麵法嚮接觸剛度隨著實際接觸麵積、法嚮接觸載荷、相關因子或材料性能參數的增大而增大,而隨著分形粗糙度的加大而降低;分形維數在較小範圍內,微動結閤麵法嚮接觸剛度隨著分形維數從1變大而增彊;但分形維數在較大範圍內,微動結閤麵法嚮接觸剛度時常隨著分形維數的加大接近于2而降低。微動結閤麵法嚮接觸校對分形模型的構思,能深入研究微動兩粗糙錶麵之間的實際接觸狀態。
기우Hertz탄성이론급분형궤하학이론,이조조표면돌봉변형특정、표면돌봉승수법향접촉재하적광활성화련속성위기출이급엄격구분탄성변형화소성변형,구가미동결합면적일충법향접촉교대분형모형。도출표면돌봉법향탄성접촉재하화표면돌봉법향변형량지간적멱함수방정,제출미동결합면2개돌봉지간호상작용적법향접촉강도적구도함수이비편도함수구해준칙。수치방진곡선게시:대우급정적법향접촉재하,수착분형유수적증가,실제접촉면적수선증가연후강저;증가법향접촉재하혹강저표면조조도도장증대실제접촉면적;미동결합면법향접촉강도수착실제접촉면적、법향접촉재하、상관인자혹재료성능삼수적증대이증대,이수착분형조조도적가대이강저;분형유수재교소범위내,미동결합면법향접촉강도수착분형유수종1변대이증강;단분형유수재교대범위내,미동결합면법향접촉강도시상수착분형유수적가대접근우2이강저。미동결합면법향접촉교대분형모형적구사,능심입연구미동량조조표면지간적실제접촉상태。
On the basis of Hertz elastic theory and fractal geometry theory, one normal contact modification fractal model of fretting joint interface, following the character of the harsh surface bulge’s deflection, smoothness and continuity of normal contact load exerting surface asperity as well as differentiating severely elastic deformation and plastic deflection, is proposed. The power function equation between surface summit’s normal elastic contact load and its normal deformation is presented. Furthermore, the solving rule of differential function not partial differential function to attain fretting joint interface two bulges’ interacting normal contact stiffness is addressed. The digital simulation curves reveal that real contact area firstly increases and afterwards decreases with the augment of fractal dimension at the given normal contact load. Real contact area may outright add by increasing normal contact load or reducing surface roughness. Fretting joint interface normal contact stiffness enhances as the increase of real contact area, normal contact load, relating factor or material property parameter, yet an increase in fractal roughness causes a decrease in fretting joint interface normal contact stiffness. Fretting joint interface normal contact stiffness increases when fractal dimension increases from 1 in the smaller range of fractal dimension;nevertheless, fretting joint interface normal contact stiffness sometimes shrinks when fractal dimension increases close to 2 in the larger range of fractal dimension. Conceiving normal contact amendment fractal model of fretting joint interface investigates deeply the practicable contact states between fretting two coarse surfaces.