核石墨中的动态变形及其潜在机制
Melonie Thomas1, Hajin Oh1, Ryan Schoell2
1Department of Mechanical Engineering, The Pennsylvania State University, University Park, PA 16802, USA.
Materials (Basel, Switzerland)
|September 28, 2024
概括
核石墨 (IG-110) 中先前存在的缺陷显著影响辐射诱导的变形. 莫佐夫斯基裂促进局部可塑性,而辐射类型影响爬行行为和脆化.
科学领域:
- 材料科学 材料科学 材料科学
- 核工程 核工程是指核工程.
- 固体力学 固体力学是什么
背景情况:
- 核石墨的性能对于反应堆的性能和安全至关重要.
- 辐射引起的缺陷和先前存在的缺陷,如Mrozowski裂,会影响石墨的机械行为.
- 了解在辐射下依赖时间的变形对于核应用至关重要.
研究的目的:
- 为了研究核石墨 (IG-110) 辐射下先前存在的缺陷 (点缺陷集群,Mrozowski裂) 的作用.
- 分析不同类型的离子 (Au2+和C2+) 和辐射条件对石墨机械反应的影响.
- 阐明核石墨中辐射诱导的变形和脆化的机制.
主要方法:
- 在特定的度下,用2.8 MeV Au2+和8 MeV C2+光束对IG-110石墨进行辐射.
- 在传输电子显微镜 (TEM) 内的微观标本的现场机械加载.
- 现场基于痕的爬行载荷实验.
主要成果:
- 在现场的TEM揭示了Mrozowski裂周围的局部塑性,形成滑动或波动带.
- 只有在非常高的压力下,在没有缺陷的区域附近才观察到滑带.
- 现场自我离子辐射导致了脆化和减少爬行,而重离子辐射显示了相反的效果.
- 假设大金离子诱导胀和缺陷移动通道.
结论:
- 预先存在的缺陷在辐射期间核石墨的动态应力放松中发挥着关键作用.
- 照射的类型显著改变了机械反应,包括脆化和爬行.
- 需要进一步的研究才能充分理解辐射环境和石墨的机械特性之间的复杂相互作用.
相关概念视频
Temperature Dependent Deformation
142
In a nonhomogeneous rod made up of steel and brass, restrained at both ends and subjected to a temperature change, several steps are involved in calculating the stress and compressive load. Due to the problem's static indeterminacy, one end support is disconnected, allowing the rod to experience the temperature change freely. Next, an unknown force is applied at the free end, triggering deformations in the rod's steel and brass portions. These deformations are then calculated and added...
142
Deformation of Member under Multiple Loadings
159
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...
159
Atomic Nuclei: Nuclear Relaxation Processes
632
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
632
Stress-Strain Diagram - Ductile Materials
646
The stress-strain relationship in ductile materials such as structural steel or aluminium is intricate and progresses through several stages. When a specimen is loaded, it initially exhibits a linear length increase, depicted by a steep straight line on the stress-strain diagram. It indicates the material is elastically deforming and will return to its original shape once unloaded. However, when a critical stress value is reached, plastic deformation begins. This stage sees substantial...
646
Nuclear Stability
18.6K
Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
To hold positively charged protons together...
To hold positively charged protons together...
18.6K
Deformation in a Circular Shaft
271
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...
271


