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一种用于室温下圆柱形试样拉伸试验的新型应变硬化和软化流动模型。

A Novel Flow Model of Strain Hardening and Softening for Use in Tensile Testing of a Cylindrical Specimen at Room Temperature.

作者信息

Razali Mohd Kaswandee, Joun Man Soo, Chung Wan Jin

机构信息

Graduate School of Mechanical and Aerospace Engineering, Gyeongsang National University, Jinju 52828, Korea.

ERI, Graduate School of Mechanical and Aerospace Engineering, Gyeongsang National University, Jinju 52828, Korea.

出版信息

Materials (Basel). 2021 Aug 27;14(17):4876. doi: 10.3390/ma14174876.

Abstract

We develop a new flow model based on the Swift method, which is both versatile and accurate when used to describe flow stress in terms of strain hardening and damage softening. A practical issue associated with flow stress at room temperature is discussed in terms of tensile testing of a cylindrical specimen; we deal with both material identification and finite element predictions. The flow model has four major components, namely the stress before, at, and after the necking point and around fracture point. The Swift model has the drawback that not all major points of stress can be covered simultaneously. A term of strain to the third or fourth power (the "second strain hardening exponent"), multiplied and thus controlled by a second strain hardening parameter, can be neglected at small strains. Any effect of the second strain hardening exponent on the identification of the necking point is thus negligible. We use this term to enhance the flexibility and accuracy of our new flow model, which naturally couples flow stress with damage using the same hardening constant as a function of damage. The hardening constant becomes negative when damage exceeds a critical value that causes a drastic drop in flow stress.

摘要

我们基于斯威夫特方法开发了一种新的流动模型,该模型在用于从应变硬化和损伤软化方面描述流动应力时既通用又准确。结合圆柱形试样的拉伸试验讨论了与室温下流动应力相关的一个实际问题;我们同时处理材料识别和有限元预测。该流动模型有四个主要部分,即颈缩点之前、颈缩点处、颈缩点之后以及断裂点附近的应力。斯威夫特模型的缺点是不能同时涵盖应力的所有主要点。在小应变时,应变的三次方或四次方项(“第二应变硬化指数”)乘以并由第二个应变硬化参数控制,可以忽略不计。因此,第二应变硬化指数对颈缩点识别的任何影响都可以忽略不计。我们用这个项来提高我们新流动模型的灵活性和准确性,该模型自然地使用与损伤相关的相同硬化常数将流动应力与损伤耦合起来。当损伤超过导致流动应力急剧下降的临界值时,硬化常数变为负值。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9bf7/8432683/013493830384/materials-14-04876-g001.jpg

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