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Investigation of modeling on single grit grinding for martensitic stainless steel

马氏体不锈钢单磨粒磨削过程的建模研究

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Abstract

Single grit grinding is the simplified model to abstract the macro scale grinding. Finite element analysis is a strong tool to study the physical fields during a single grit grinding process, compared to experimental research. Based on the dynamic mechanical behavior of 2Cr12Ni4Mo3VNbN steel and the mathematical statistics of abrasive grit, modeling of the single grit grinding process was conducted by using commercial software AdvantEdge. The validation experiment was designed to validate the correctness of the FEA model by contrast with grinding force. The validation result shows that the FEA model can well describe the single grit grinding process. Then the grinding force and multi-physics fields were studied by experimental and simulation results. It was found that both the normal and tangential grinding forces were linearly related to the cutting speed and cutting depth. The maximum temperature is located in the subsurface of the workpiece in front of the grit, while the maximum stress and strain are located under the grit tip. The strain rate can reach as high as about 106 s−1 during the single grit grinding,which is larger than other traditional machining operations.

摘要

单磨粒磨削是宏观尺度磨削的简化模型。相比于传统实验研究,有限元分析是一种强有力的研 究工具,可以计算得到单磨粒磨削过程的多物理场分布。本文基于2Cr12Ni4Mo3VNbN 不锈钢的动态 力学模型和磨粒的数学统计模型,使用AdvantEdge 软件对单磨粒的磨削过程进行了有限元建模,计 算得到了磨削温度场、应力应变场、磨削力等物理量。搭建了单磨粒磨削试验平台,测量了不同工艺 参数下的磨削力变化。通过对比磨削力的实验值和计算值,结果表明有限元模型可以较好地描述单磨 粒磨削过程。试验和仿真数据一致表明,法向磨削力和切向磨削力均与磨粒的切速、切深成正比;工 件的最大磨削温度位于磨粒前刃面的下方,而应力应变最大值则位于磨粒尖端的下方。单磨粒磨削过 程的应变变形率高达106 s−1,远超其他常规切削方式的应变变形率。

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Correspondence to Gang Wang  (王罡).

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Foundation item: Projects(U1537202, 51575305) supported by the National Natural Science Foundation of China; Project(61328302) supported by National Security Major Basic Research Program of China

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Nie, Zg., Wang, G., Jiang, F. et al. Investigation of modeling on single grit grinding for martensitic stainless steel. J. Cent. South Univ. 25, 1862–1869 (2018). https://doi.org/10.1007/s11771-018-3875-8

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  • DOI: https://doi.org/10.1007/s11771-018-3875-8

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