1) 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。
2) potential field distribution
势能场分布
3) distribu tion of gases in potential field
势场中气体分布
4) distribution trend
分布走势
1.
Meanwhile,distribution trend of polymer AY in the process of liquid-so.
同时,考察了聚合物AY在熟料溶出过程中液固分离时的分布走势,结果表明,用含有80mg。
5) potential distribution
势分布
1.
On the basis of superposition principle and mirror image principle of potential,and considering borehole pressure drop,the computing model of 3-D potential distribution for inclined well reservoir is estabilished by using mathematical method.
根据势的迭加原理及镜像反映原理 ,考虑井筒压降 ,应用数学方法 ,建立了油藏斜井三维空间势分布计算模型 ,研究了油藏斜井三维势分布规律 ,并讨论了影响因素。
6) potential distribution
电势分布
1.
Relationship between reference point potential and potential distribution of normal electrocardial field on the thoracic surface of healthy individuals;
正常人胸表心电位场电势分布与导联参比点的关系
2.
Electromagnetic tomography of two-phase flow is forward simulated by finite element method(FEM) to model potential distribution in different flow types and measuring combinations,meantime,influences of amount and size of electrodes to the potential distribution are sought simply,then 6 kinds of typical sensitive fields are simulated.
应用有限元方法对两相流动电磁成像测量进行正演仿真,模拟不同测量组合下各种流型的电势分布,并简单考察了电极数目和电极尺寸对电势分布的影响,然后模拟6种典型测量敏感场。
3.
The factors effecton the potential distribution in the electrode are described theo- retically.
建立了不同操作模式下普遍化的固定床电化学反应器模型 ,联用正交配置法和中心差分法对复杂模型方程进行了求解 ,从理论上分析了影响床层内电势分布的因素 ,为固定床电化学反应器的开发、放大及操作优化奠定了理论基
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。
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参考词条