弹性幂律应变硬化材料尖锐压痕的硬度方程

M. Mata, M. Anglada, J. Alcalá
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引用次数: 30

摘要

本研究基于Mata等人对应变硬化材料接触变形机制的研究。结果使我们可以推导出弹幂律塑性材料尖锐压痕的一般硬度方程。发现公式H/σr = 1.440 + 0.264 ln(E/σr)提供了大范围弹塑性响应的硬度H估计,只要接触变形处于弹塑性过渡状态。该公式是对以前的公式的修改,该公式适用于不表现应变硬化的固体;式中E为杨氏模量,屈服强度σys替换为σr,表示特征应变ϵr为0.1时单轴应力-应变曲线中的应力水平。径向流型的发展被认为是上述方程成立的必要条件。随着压头下方的变形演变为不包含模式,具有弹塑性转变特征的径向流动模式越来越被破坏,以至于非径向流动导致接触边界处材料堆积。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A hardness equation for sharp indentation of elastic-power-law strain-hardening materials
Abstract This investigation is predicated upon work by Mata et al. on the contact deformation regimes for strain-hardening materials. The results allow us to derive a general hardness equation for sharp indentation of elastic-power-law plastic materials. The formula H/σr = 1.440 + 0.264 ln(E/σr) is found to provide estimates of hardness H for a wide range of elastoplastic responses as long as the contact deformation regime lies within the elastic-plastic transition. This formulation is a modification to previous formulae derived for solids that do not exhibit strain hardening; where E is Young's modulus and the yield strength σys has been replaced by σr, the stress level in the uniaxial stress-strain curve at a characteristic strain ϵr of 0.1. The development of radial flow patterns is regarded as a necessary condition to the validity of the above equation. As the deformation underneath the indenter evolves to an uncontained mode, the radial flow patterns that are characteristic of the elastic-plastic transition are increasingly disrupted to a point where non-radial flow leads to piling-up of material at the contact boundary.
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