研究了不压缩的超弹性薄圆圆圆圆圆外的非线性反应,这些外具有几何缺陷
Morteza Shayan Arani1, Mehrdad Bakhtiari1, Mohammad Toorani1
1Mechanical Engineering Department, Polytechnique de Montréal, C.P. 6079, Succ. Centre-ville, Montréal, Québec, H3C 3A7, Canada.
Journal of the mechanical behavior of biomedical materials
|April 28, 2024
概括
超弹性中的初始几何不完美会增加自然频率. 不同的不完美类型和模型改变了这种效果,影响了外.
科学领域:
- 固体力学 固体力学是什么
- 非线性动力学是一种非线性动力学.
- 材料科学 材料科学 材料科学
背景情况:
- 超弹性薄圆柱形外在工程中至关重要.
- 最初的几何缺陷显著影响的行为.
- 了解非线性反应对于结构完整性至关重要.
研究的目的:
- 分析具有初始几何不完美的超弹性薄圆柱形外.
- 研究缺陷对自然频率和振幅响应的影响.
- 提供对非线性外动态的全面理解.
主要方法:
- 使用多内尔理论和拉格朗日方程,推导出非线性运动方程.
- 采用了Mooney-Rivlin模型来研究超弹性材料的行为.
- 用多个尺度方法分析解决合的非线性方程.
- 与混合有限元法和Abaqus软件对比,验证了模型准确性.
主要成果:
- 发现几何不完美增强了贝的自然频率.
- 不同的不完美模型导致了自然频率增强的各种趋势.
- 振幅响应表现出两个峰值,表明变软和变硬的行为.
- 显而易见的初始几何不完美被证明影响了这些双峰.
结论:
- 这项研究为分析不完美的超弹性外提供了经过验证的模型.
- 几何不完美在改变圆柱形外的动态特征方面发挥着至关重要的作用.
- 这些发现为这些结构的复杂非线性行为和稳定性提供了见解.
相关概念视频
Circular Shafts - Elastoplastic Materials
102
The study of solid circular shafts under stress shows that within the elastic limit, stress increases directly to the distance from the shaft's center. This relationship holds until the shaft reaches a critical point of stress, beyond which it begins to yield, marking the transition from elastic to plastic deformation. At this crucial juncture, the maximum torque the shaft can endure without permanent deformation is determined, signifying the limit of its elastic behavior.
As torque on the...
As torque on the...
102
Members Made of Elastoplastic Material
97
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...
97
Plastic Deformation in Circular Shafts
186
When materials are subjected to forces that surpass their yield strength, they undergo a process known as plastic deformation. This results in a permanent alteration or strain in their structure. This concept can be specifically applied to circular shafts, where the deformation leads to a change in its shape. The precise evaluation of this plastic deformation requires understanding the stress distribution within the circular shaft, which is achieved by calculating the maximum shearing stress in...
186
Thin-Walled Hollow Shafts
185
In analyzing a thin-walled hollow shaft subjected to torsional loading, a segment with width dx is isolated for examination. Despite its equilibrium state, this segment faces torsional shearing forces at its ends. These forces are quantitatively described by the product of the longitudinal shearing stress on the segment's minor surface and the area of this surface, leading to the concept of shear flow. This shear flow is consistent throughout the structure, indicating a uniform distribution...
185
Deformation in a Circular Shaft
286
One of the distinctive characteristics of circular shafts is their ability to maintain their cross-sectional integrity under torsion. In other words, each cross-section continues to exist as a flat, unaltered entity, simply rotating like a solid, rigid slab. To understand the distribution of shearing stress within such a shaft, consider a cylindrical section inside this circular shaft. This section has a length of L and a radius of R, with one end fixed. The radius of the cylindrical section is...
286
Relation between Poisson's ratio, Modulus of Elasticity and Modulus of Rigidity
264
Deformation occurs in axial and transverse directions when an axial load is applied to a slender bar. This deformation impacts the cubic element within the bar, transforming it into either a rectangular parallelepiped or a rhombus, contingent on its orientation. This transformation process induces shearing strain. Axial loading elicits both shearing and normal strains. Applying an axial load instigates equal normal and shearing stresses on elements oriented at a 45° angle to the load axis.
264


