Formation of Crater on Cathode Surface in Vacuum Metal Vapor Arc
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Formation of Crater on Cathode Surface in Vacuum Metal Vapor Arc
Vol. 46, Issue 3, Pages: 843-851(2020)
作者机构:
沈阳工业大学特种电机与高压电器教育部重点实验室
作者简介:
基金信息:
DOI:
CLC:
Published Online:31 March 2020,
Published:2020
稿件说明:
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FU Si, CAO Yundong, LI Jing, et al. Formation of Crater on Cathode Surface in Vacuum Metal Vapor Arc[J]. 2020, 46(3): 843-851.
DOI:
FU Si, CAO Yundong, LI Jing, et al. Formation of Crater on Cathode Surface in Vacuum Metal Vapor Arc[J]. 2020, 46(3): 843-851.DOI:
Formation of Crater on Cathode Surface in Vacuum Metal Vapor Arc
摘要
真空金属蒸气电弧作用下阴极表面热流密度和压力的不同时空分布情况
影响阴极表面蚀坑形成过程。结合阴极表面蚀坑形成过程中表面张力和马朗戈尼效应共同影响
建立考虑固、液、气态相变过程的二维轴对称流体动力学瞬态模型
描述阴极表面"火山口"形成的热力学行为
获得阴极最初喷射蒸气的表面结构和时间。阴极熔池相变过程中
熔融金属熔池中心形变和温度梯度较大
熔池流动由表面张力和马朗戈尼效应共同驱动
将熔坑中心热量转移至边缘
在蚀坑边缘
表面张力为熔池流动的主要驱动力。温度上升至临界温度
出现新的喷射爆炸点
"火山口"表面形成金属蒸气密度为10
25
m
-3
的覆盖层
密度分布与阴极蚀坑形状有关;增加热流密度、减小外部压力或增大作用半径
阴极表面覆盖层出现时间提前来到
蚀坑形状各异;当作用半径过小时
注入能量低
阴极斑点形成过程中蚀坑底部厚
半径小
蚀坑附近未产生金属蒸气覆盖层。
Abstract
The formation process of surface crater is affected by the different time and space distribution of the thermal flux and pressure on the cathode in the action of vacuum metal vapor arc. After taking the influence of surface tension and Marangoni into account
a transient 2 D axially symmetric melting model has been developed to describe the thermodynamic behavior of molten metal on cathode surface and the formation of a crater. Moreover
the surface structure and initial time of metal vapor injection from the crater are obtained. In the process of metal phase transition
the deformation and temperature gradient in the center of molten metal pool are remarkable. Due to the Marangoni effect and the surface tension
the energy from the center of the molten metal on the cathode surface
is transferred to the edge of the crater. At the edge of crater
the surface tension of the driving force is significant. As the temperature increases to the critical temperature
the new jet explosion point appears. The overburden layer of metal vapor density of 10
25
m
-3
on the surface of the crater is formed
in which distribution is related to the shape of the crater. By increasing the heat flux
reducing the external pressure and increasing the specified radius
the covering layer on the crater appears in advance. When the energy injected to the cathode is excessively low
the bottom of the crater is thick and the radius of the crater is small. Therefore
a dense metal vapor layer cannot be generated near the crater.