1) inclined magnetic field
斜向磁场
2) oblique magnetic field
倾斜磁场
1.
1—10 Hz) from magnetosphere to the conductive ground is studied in the presence of oblique magnetic field and the analytical solution is obtained.
分析了倾斜磁场对电离层Alfven谐振器各种参数如反射系数、谐振频率、衰减率的影响。
3) Oblique magnetization
斜向磁化
4) longitudinal magnetic field
纵向磁场
1.
Effect of longitudinal magnetic field on microstructure and properties of MIG weld joint of mild steel;
纵向磁场对低碳钢MIG焊焊缝组织及性能的影响
2.
Effect of applied longitudinal magnetic field on the properties of overlaying weld metal;
外加纵向磁场对堆焊层金属性能的影响
3.
Effect of longitudinal magnetic field on splatter in CO_2 short-circuit transfer arc welding;
外加纵向磁场对CO_2焊短路过渡飞溅影响的研究
5) transverse magnetic field
横向磁场
1.
Mechanical Properties of Iron Based Surfacing Alloys Applied DC Transverse Magnetic Field;
直流横向磁场作用下铁基堆焊合金的力学性能
2.
In order to refine the structure of deposited metal and control the morphology and distribution of hard phases in surfacing deposited metal, DC transverse magnetic field was applied to the carbon arc surfacing of Cr-B-Ni-V iron based alloy system.
采用碳弧堆焊方法对Cr-B-Ni-V系铁基合金堆焊时加入直流横向磁场,来细化堆焊层金属的组织,控制硬质相的形态及分布。
3.
A one-di-mensional transverse magnetic field may cause an ecc.
一维横向磁场将使液池发生偏心喷溅，加剧了液滴的发射；二维横向磁场则可减轻液池的喷溅。
6) axial magnetic field
轴向磁场
1.
Effects of an axial magnetic field on silicon crystal Czochralski growth;
轴向磁场对硅单晶Czochralski生长过程的影响
2.
The theoretical models of Faraday nonreciprocal phase error which is generated by axial magnetic field in Single-Depo-I-FOG and Twin-Depo-I-FOG are founded respectively through using Jones Matrix.
运用琼斯矩阵,分别建立了轴向磁场作用下,单消偏陀螺系统和双消偏陀螺系统产生Faraday非互易相位差的理论模型。
3.
Based on monochromatic light,theory derivation and analysis of the single-mode fiber loop that is resulted from axial magnetic field is introduced.
去偏光纤陀螺的非理想单模光纤,在垂直于光纤环面的轴向磁场作用下,由于Faraday效应,在其中传播的正反两束光会产生一个与磁场有关的非互易相位差。
补充资料：各向异性第二临界磁场（anisotropicsecondcriticalmagneticfield）
各向异性第二临界磁场（anisotropicsecondcriticalmagneticfield）
在主轴坐标系中，设磁场平行于主轴Z，由各向异性GL方程给出的各向异性第二临界磁场为
Hc2∥(T)=`\frac{2|\alpha(T)|(m_1^\**m_2^\**)^{1/2}}{\mu_0\hbare^\**}`
$=sqrt{2K_1K_2}H_c(T)$
这里α(T)为GL自由能密度展式系数，mμ*和Kμ(μ=1,2,3)分别为库珀对有效质量和GL参量的μ分量，e*为库珀电子对电荷量，$hbar$是除以2π的普朗克常数，μ0是真空磁导率，Hc(T)为热力学临界磁场。对层状结构氧化物超导体，GL参量Ka≈Kb=Kab，并有
Hc2∥(T)=$sqrt2K_{ab}H_c(T)$
Hc2⊥(T)=$(2K_{ab}K_c)^{1/2}H_c(T)$
Hc2∥和Hc2⊥分别为磁场与主轴Z（或晶轴C）平行和垂直时的第二临界磁场，其物理性质含义参见“第二临界磁场”。
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