1) potential field distribution
势能场分布
2) field-potential distribution
场势分布
1.
Through building the elementary model of Boltzmann distribution of electrostatic dust the author calculates the field-potential distribution of electrostatic dust, discusses the empirical formula of dust concentration in the condition of disruption and verifies the effect of the previous conclusion through the issued experiment report.
通过建立静电粉尘的Ｂｏｌｔｚｍａｎｎ分布初等模型计算静电粉尘的场势分布，讨论了击穿条件下粉尘浓度的经验公式，并通过已发表的实验报告证实了上述结论的有效性。
3) distribu tion of gases in potential field
势场中气体分布
4) energy distribution characteristic
势能分布特征
1.
A three-dimensional molecular dynamics simulation method and Finnis-Sinclair embedded atom potential were utilized to study the potential energy distribution characteristic of an fcc Ag nanowires at room temperature and its changes during heating,by which we get the ratio and function of the potential energy distribution of Ag nanowires at different temperatures.
采用三维分子动力学模拟方法,以面心立方金属银为研究对象,基于Finnis-Sinclair型嵌入原子法(EAM)多体势,模拟研究了纳米线势能分布特征在常温下及其在不同温度直到熔化过程中的变化,给出了常温及不同温度银纳米线势能分布比例和势能分布函数。
5) field emission energy distribution
场发射能量分布
1.
This paper summarizes the results about emission mechanisms of CNTs during the past 10 years, including issues of field emission energy distribution (FEED), work function, emission models and emission stability.
较全面地介绍了碳纳米管场发射研究10年来在发射机理方面的研究结果,包括场发射能量分布、逸出功、发射模型以及发射稳定性和失效等问题,并介绍了相关方面的研究结果。
6) Energy distribution in wave field
波场能量分布
补充资料：开关场分布
分子式：
CAS号：
性质：在饱和磁滞回线的微分曲线上，峰值一半处两点之间的宽度称半峰宽ΔH(见图)，半峰宽与内禀矫顽力之比称为开关场分布，其表达式为SFD=ΔH/MHc。该值描述磁滞回线在矫顽力附近的陡峭程度。对磁记录材料而言，其值越小，磁滞回线在Hc附近越陡峭，录放信号的灵敏度越高。
CAS号：
性质：在饱和磁滞回线的微分曲线上，峰值一半处两点之间的宽度称半峰宽ΔH(见图)，半峰宽与内禀矫顽力之比称为开关场分布，其表达式为SFD=ΔH/MHc。该值描述磁滞回线在矫顽力附近的陡峭程度。对磁记录材料而言，其值越小，磁滞回线在Hc附近越陡峭，录放信号的灵敏度越高。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条