在软组织中模拟疲劳失败,使用具有不连续损伤的粘性-超弹性模型
Bradley S Henderson1, Katelyn F Cudworth1, Estefanía Peña2
1Department of Mechanical & Biomedical Engineering, Boise State University, Boise, ID, USA.
概括
一种新的粘性-超弹性损伤模型成功地模拟了软纤维组织的疲劳失败. 这个框架预测了组织破裂,并可能统一对静态和疲劳失败的建模.
科学领域:
- 生物力学 生物力学
- 材料科学 材料科学 材料科学
- 组织工程是组织工程.
背景情况:
- 软组织易受单次高冲击负荷和重复低冲击疲劳负荷造成的伤害.
- 现有的模型有效模拟静态失效,但缺乏软组织疲劳失效的强大框架.
研究的目的:
- 评估粘性-超弹性损伤模型的可行性,用于模拟软纤维组织中疲劳失败的不连续损伤.
- 建立一个统一的构成式,能够模拟静态和疲劳失败行为.
主要方法:
- 使用一种粘性-超弹性损伤模型,并以应变能量为基础的损伤标准.
- 校准了样本特定的材料参数,使用来自人类中介阴囊的单轴拉力疲劳实验的循环爬行数据.
- 通过使用来自疲劳实验的参数,验证了模型模拟静态故障的能力.
主要成果:
- 该模型准确地模拟了循环爬行的三个特征阶段,并预测了组织破裂周期.
- 证明在循环应力下损伤的传播是由时间依赖的伸展和应变能量的粘弹性增加驱动的.
- 展示了模型复制静态失效应力-应变曲线的能力.
结论:
- 一个粘性-超弹性不连续损伤框架可以有效地建模周期性爬行,并预测软组织的破裂.
- 固体的粘弹性是调节疲劳失败的关键因素,较慢的应力放松时间赋予了更大的阻力.
- 这种统一模型提供了一种可靠的方法来模拟软组织中的疲劳和静态失效.
相关概念视频
Fatigue
213
Fatigue occurs when materials rupture under repeated or fluctuating loads, even at stress levels far below their static breaking strength. It typically results in brittle failure, even for ductile materials. It is a critical consideration in designing machines and structural components subjected to repetitive or varying loads. The nature of these loadings can range from fluctuating loads like unbalanced pump impellers causing vibrations to repeatedly bending a thin steel rod wire back and forth...
213
Deformation of Member under Multiple Loadings
192
When a rod is made of different materials or has various cross-sections, it must be divided into parts that meet the necessary conditions for determining the deformation. These parts are each characterized by their internal force, cross-sectional area, length, and modulus of elasticity. These parameters are then used to compute the deformation of the entire rod.
In the case of a member with a variable cross-section, the strain is not constant but depends on the position. The deformation of an...
In the case of a member with a variable cross-section, the strain is not constant but depends on the position. The deformation of an...
192
Plastic Behavior
230
A material's elastic behavior is characterized by the disappearance of stress once the load is removed, allowing the material to return to its original state. However, when stress surpasses the yield point, yielding commences, marking the onset of plastic deformation or permanent set. This change from elastic to plastic behavior is influenced by the peak stress value and the duration before the load is removed. An intriguing observation occurs when a specimen is loaded, unloaded, and...
230
Members Made of Elastoplastic Material
125
The behavior of elastoplastic materials under bending stresses, particularly in structural members with rectangular cross-sections, is crucial for predicting material responses and understanding failure modes. Initially, when a bending moment is applied, the stress distribution across the section follows Hooke's Law and is linear and elastic. This distribution means the stress increases from the neutral axis to the maximum at the outer fibers, up to the elastic limit.
As the bending moment...
As the bending moment...
125
Residual Stresses in Bending
211
In the study of elastoplastic members subjected to bending moments, understanding the loading and unloading phases is crucial for assessing material behavior and structural integrity. During the loading phase, as the bending moment increases, the material initially responds elastically, adhering to Hooke's Law, where stress is directly proportional to strain. When the load exceeds the yield strength, plastic deformation occurs, resulting in permanent strain and deformation that remains even...
211
Generalized Hooke's Law
1.1K
The generalized Hooke's Law is a broadened version of Hooke's Law, which extends to all types of stress and in every direction. Consider an isotropic material shaped into a cube subjected to multiaxial loading. In this scenario, normal stresses are exerted along the three coordinate axes. As a result of these stresses, the cubic shape deforms into a rectangular parallelepiped. Despite this deformation, the new shape maintains equal sides, and there is a normal strain in the direction of the...
1.1K


