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Grain Size Estimation in Anisotropic Materials

机译:各向异性材料中的粒度估计

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摘要

The estimators proportional to (N_A(x,y)N_A{x,z}N_A(y,z))~(1/2) and (N_L(x)N_L(y)N_L(z)) obtained by profile and intercept counts are recommended by ASTM Standards E 112 for 3D grain intensity lambda of anisotropic grain structures (N_A(centre dot) are estimated in three mutually perpendicular planes suitably oriented with respect to the prevailing anisotropy direction and N_L(centre dot ) are intercept intensities along three suitably selected mutually perpendicular directions). However, X is also related to the profile and intercept intensities X', X", namely X= c'(lambda')~(3/2)= c"(?v")3. The induced intensities are estimated by arithmetic means N_A = {N_A(x,y)+N_A(x,z)+N_A(y,z)y3, N_L = (N_L(x)+N_L(y)+N_L(z))/3. A simple model is developed, in which the role of geometric and arithmetic means of profile and intercept counts in the grain size estimation is elucidated. Its results are compared with computer simulated random tessellations with prevailing rod-like and plate-like cells and applied to anisotropic grain structures of pure Al produced by ECAP and to platinum based composite Pt - 0.5 Y2O3.
机译:通过简介和拦截获得的(n_a(x,y)n_a {x,z} n_a(y,z))〜(y,z))〜(y,z))〜(y,z)和(n_l(x)n_l(y)n_l(z))成比例由ASTM标准EACTM标准建议计数E112用于3D颗粒强度,各向异性晶粒结构的λ(N_A(中心点)估计在相对于主要各向异性方向的三个相互垂直的平面中,并且N_L(中心点)沿三个截取强度适当地选择相互垂直的方向)。然而,X也与轮廓和拦截强度x',x“,即x = c'(lambda')〜(3/2)= c”(Δv“)3。诱导强度估计算术表示n_a = {n_a(x,y)+ n_a(x,z)+ n_a(y,z)y3,n_l =(n_l(x)+ n_l(y)+ n_l(z))/ 3。一个简单的模型是开发的,其中阐明了几何和算术装置的角色和截取计数在晶粒尺寸估计中的作用。它的结果与计算机模拟随机曲线与普遍存在的棒状和板状细胞进行了比较并应用于各向异性晶粒结构由ECAP产生的纯Al和铂基复合PT - 0.5 Y2O3。

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