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Synthesis of Grain Size Distribution Functions Determined by the Coulter Counter Method

机译:库尔特计数器法确定的粒度分布函数综合

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There are many measuring methods of grain sizes. Taking into consideration the fine grained materials, one of the existing techniques is measurement of grain size by the Coulter Counter method. This method is based on the measuring the changes of electrolyte resistance during grains flow through the calibrated diaphragm. This method is relatively simple to apply, significantly precise and the results are given quickly. However, the problem is that the measurements are limited by the size of diaphragm. Because of this situation,measurement of grain sizes by this instrument is possible in range from 10% to 60% of diaphragm diameter. This limitation causes the necessity of replacing diaphragm in case when the measured grain size distribution concerns the material of large size range. In purpose of determining the total grain size distribution, the synthesis of some partial distributions, given for individual grain fractions (with different diaphragm applied), is required.This is possible to do by calculating the mixture of distribution functions, created from the partial distribution functions.Two materials were selected to research: quartzite and glass, which were comminuted in cylindrical crusher, additionally grinded, screened and then analyzed by Coulter Counter for five grain fractions: 0~125 μm, 0~80 μm, 0~56 μm, 0~40 μm and 0~25 μm. For each fraction, five different partial distributions were given (in case of glass four), which are the basis for the creating the joined grain composition. To assure the adequacy of the given distribution function, it is necessary to obtain the possibly best approximation of partial distributions. In the work, both the parametric and non-parametric methods of density approximations of investigated random variable. For each grain fraction the approximations were done by three traditional distribution functions: RRB, GSA and log-norm distribution functions and three methods of non-parametric approximation: Gauss kernel, Epanechnikov kernel and orthogonal Fourier series method. As the criterion of the certain distribution function acceptance, the value of the residual deviation was assumed, given by the formulae:where F(di) is the value of the theoretical distribution function and F0(d1) is the value of the empirical distribution, k is number of fractions.
机译:晶粒度的测量方法很多。考虑到细粒材料,现有技术之一是通过库尔特计数法测量晶粒尺寸。该方法基于测量谷物流经校准膜片时电解质电阻的变化。该方法应用相对简单,非常精确,并且可以快速给出结果。然而,问题在于测量结果受到隔膜尺寸的限制。由于这种情况,可以用此仪器在隔膜直径的10%至60%范围内进行晶粒尺寸的测量。当测量的粒度分布涉及大尺寸范围的材料时,此限制导致必须更换隔膜。为了确定总晶粒尺寸分布,需要综合一些针对个别晶粒分数(使用不同隔膜)的部分分布,这可以通过计算由部分分布创建的分布函数的混合来实现选择了两种材料进行研究:石英岩和玻璃,然后在圆柱形破碎机中进行粉碎,再进行研磨,筛分,然后用库尔特计数器对五个颗粒进行分析:0〜125μm,0〜80μm,0〜56μm, 0〜40μm和0〜25μm。对于每个部分,给出了五种不同的部分分布(在使用四块玻璃的情况下),这是创建结合的晶粒成分的基础。为了确保给定分布函数的充分性,有必要获得偏分布的可能最好的近似值。在工作中,研究随机变量的密度逼近的参数方法和非参数方法均如此。对于每个颗粒分数,通过三种传统的分布函数:RRB,GSA和对数范数分布函数以及三种非参数近似的方法进行近似:高斯核,Epanechnikov核和正交傅里叶级数法。作为确定一定分布函数的标准,假设残差的值由以下公式给出:其中,F(di)是理论分布函数的值,F0(d1)是经验分布的值, k是分数的数量。

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