正方形环形/圆形纳米板的非线性热/机械曲与非局部应变梯度模型
Mostafa Sadeghian1, Arvydas Palevicius1, Giedrius Janusas1
1Faculty of Mechanical Engineering and Design, Kaunas University of Technology, Studentu 56, 51424 Kaunas, Lithuania.
Micromachines
|September 28, 2023
概括
这项研究研究了纳米板在热和机械负荷下的曲,考虑非局部和应变梯度效应. 一个新的方程将热和机械曲负荷与增强分析相关联.
科学领域:
- 固体力学 固体力学是什么
- 纳米技术 纳米技术
- 材料科学 材料科学 材料科学
背景情况:
- 研究了正轨环形/圆形纳米板的非线性曲折行为.
- 在弹性基础上考虑单层和双层结构 (帕斯特纳克和温克勒).
- 采用非局部应变梯度理论来捕捉小规模的影响.
研究的目的:
- 进行热和机械曲的非线性调查.
- 使用高阶剪切变形理论 (HSDT) 和第一阶剪切变形理论 (FSDT) 分析纳米板的稳定性.
- 开发一个统一的方程,从机械曲折结果中预测热曲折,反之亦然.
主要方法:
- 使用非线性·卡曼菌株推导稳定性方程.
- 高阶剪切变形理论 (HSDT) 和第一阶剪切变形理论 (FSDT) 的应用.
- 使用微分方程 (DQM) 解决稳定性方程.
主要成果:
- 分析了应变梯度系数,非局部参数,边界条件,弹性基础和几何学对曲负荷的影响.
- 通过提供更合适的剪切应力分布,HSDT表现出比FSDT更高的精度.
- 提出了一种新的方程来相互关联热和机械曲折负荷.
结论:
- 该研究提供了一个全面的了解在各种条件下纳米板的曲现象.
- 拟议的统一方程为预测曲行为提供了一种简化方法.
- 这些发现对于纳米结构在先进工程领域的设计和应用至关重要.
更多相关视频
相关概念视频
Plastic Deformations
101
It is essential to understand how structural members behave under plastic deformation when the bending stress exceeds the material's yield strength. This state of deformation permanently alters the shape of the member, in contrast to the linear elastic behavior observed before yielding. The strain at any point in the member is expressed in terms of maximum strain. Notably, the neutral axis, which coincides with the centroid during elastic bending, shifts away from the centroid under plastic...
101
Three-Dimensional Analysis of Strain
237
Three-dimensional strain analysis is crucial for understanding how materials deform under stress, particularly in elastic, homogeneous materials. This method employs principal stress axes to simplify complex stress states into more understandable forms. Subjected to stress, a small cubic element within a material either expands or contracts along these axes, transforming into a rectangular parallelepiped. This transformation effectively illustrates the material's deformation. The principal...
237
Relation between Poisson's ratio, Modulus of Elasticity and Modulus of Rigidity
284
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.
284
Plastic Deformations of Members with a Single Plane of Symmetry
103
When a structural member undergoes plastic deformation due to bending, it is crucial to understand the position of the neutral axis and the stress distribution. This member, characterized by a single plane of symmetry, exhibits a uniform stress distribution, with negative stress above the neutral axis and positive stress below. Notably, the neutral axis does not align with the centroid of the cross-section. This misalignment is typical in cases where the cross-section is not rectangular or...
103
Residual Stresses in Bending
192
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...
192
Members Made of Elastoplastic Material
114
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...
114


