1)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。
英文短句/例句
1.circular transverse-field electromagnetic flowmeter圆形横向磁场电磁流量计
2.Research on Transverse Flux Permanent Magnet Machine and Its Control System;横向磁场永磁电机及其驱动系统研究
3.RESEARCH ON A NEW TRANSVERSE-FLUX SWITCHED RELUCTANCE MACHINE WITH PM SHIELDS横向磁场开关磁阻电机永磁屏蔽技术研究
4.The Determination of Critical Magnetic Field of Magnetoelastic Buckling of Cantilevered Ferromagnetic Plates with Finite Width in Transverse Magnetic Fleld;悬臂铁磁板在横向磁场中磁弹性屈曲的临界磁场判定
5.CALCULATE THE INDUCTION EMF OF A SUPERCONDUCTOR IN TRANSVERSE MAGNETIC FIELD横向磁场中超导体感应电动势的计算
6.The Strip Board Bifurcation and Chaos Movement in Transverse Magnetic Field横向磁场中条形板的分岔和混沌运动
7.Researches on a Transverse Flux Permanent Propulsion Motor Control System;横向磁场永磁推进电动机控制系统的研究
8.Study of Transverse Flux Permanent Magnet Linear Machine and Its Drive;横向磁场永磁直线电机及其驱动的研究
9.Studies on Novel Transverse Flux Permanent Magnetic Propulsive Motor;新型横向磁场永磁电力推进电动机的研究
10.Physically Nonlinear Chaotic Vibration of Soft Ferromagnetic Thin Plate in Transverse Magnetic Field横向磁场中软铁磁薄板的物理非线性混沌振动
11.Analysis of Planar Type TFPM Structure with 3D Finite Element Method平板式横向磁场永磁电动机三维有限元分析
12.A current is sent transversely through the liquid metal, in a direction at right angles to a transverse magnetic field.使电流横穿过液态金属，其方向又与横向磁场垂直。
13.Experimental and Theoretic Studies on Magnetoelastic Buckling of Cantilevered Ferromagnetic Plates in Transverse Magnetic Field;悬臂铁磁板在横向磁场中磁弹性失稳的实验及理论研究
14.Effects of Transverse Magnetic Heat Treatment on the Magnetic Propertiesof Fe-based Amorphous Alloy with High Saturation Magnetic Induction横向磁场热处理对高饱和磁感应强度Fe基非晶磁性能的影响
15.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
16.Effect of Transverse Magnetic Field Frequency on Microstructure and Properties of Fe5 Deposited Metal横向磁场频率对Fe5堆焊合金组织性能的影响
17.Subharmonic Resonances and Stability of Conductive Thin Shell in Transverse Magnetic Field横向磁场中导电壳体的亚谐波共振与稳定性
18.Design and Research on a Novel Transverse Flux Machine Based on Scalar Potential 3D FEM;基于标量磁位三维有限元法新型横向磁场电机设计与研究
相关短句/例句
Transverse flux横向磁场
1.Transverse flux permanent propulsive magnetic(TFPPM)motor has low speed,high torque density and is widely researched as propulsive motor.由于横向磁场永磁同步电动机具有低转速、高转矩密度的特点,在推进电机领域被广泛研究。
2.Based on the study of the torque and power factor equations, this paper proposed a new view on the characteristic of the transverse flux permanent machines.基于电机转矩和功率因数方程研究的基础,提出了一种依据电、磁负荷等参数解释横向磁场高转矩密度和低功率因数性能特点的新观点。
3.The operation principle of the transverse flux permanent motor, classification, characteristics and the developing situation have been introduced by the paper.文章详细介绍了横向磁场永磁电机的工作原理。
3)slot cross field槽横向磁场
4)cross-field正交场，横向磁场
5)magnetic athwartships deviation横向磁场航向差
6)transverse rotating magnetic field横向旋转磁场
1.This paper is dealt with the fluidizaion of cohesive particles under transverse rotating magnetic field.本文研究了横向旋转磁场作用下粘性颗粒的气固流态化。
2.A transverse rotating magnetic field generator is designed,in which the rotating speed and the maximum amplitude of magnetic flux density are separately controlled by frequency of carrier wave and duty cycle of modulated wave.设计了一种横向旋转磁场发生装置,通过调节低频载波的频率和高频调幅波的占空比来控制旋转磁场的旋转速度和磁感应强度的幅值。
延伸阅读
横向磁场中的空心超导圆柱体（hollowsuperconductingcylinderinatransversalmagneticfield）横向磁场中的空心超导圆柱体（hollowsuperconductingcylinderinatransversalmagneticfield）垂直于柱轴（横向）磁场H0中的空心超导长圆柱体就其磁性质讲是单连通超导体。徐龙道和Zharkov由GL理论给出中空部分的磁场强度H1和样品单位长度磁矩M的完整解式，而在`\zeta_1\gt\gt1`和$\Delta\gt\gt1$条件下为：$H_1=\frac{4H_0}{\zeta_1}sqrt{\frac{\zeta_2}{\zeta_1}}e^{-Delta}$$M=-\frac{H_0}{2}r_2^2(1-\frac{2}{\zeta_2})$这里r1和r2分别为空心柱体的内、外半径，d=r2-r1为柱壁厚度，ζ=r/δ(r1≤r≤r2)，Δ=d/δ，δ=δ0/ψ，δ0为大样品弱磁场穿透深度，ψ是有序参量。显然此时H1→0，M→-H0r22/2，样品可用作磁屏蔽体。当$\zeta_1\gt\gt1$，$\Delta\lt\lt1$时，则H1=H0/(1 ζ1Δ/2)，M=-H0r23[1-(1 ζ1Δ/2)-1]。若$\zeta_1\Delta\gt\gt1$，则$H_1\lt\ltH_0$或H1≈0。所以，虽然$d\lt\lt\delta$，但磁场几乎为薄壁所屏蔽而难于透入空心，称ζ1Δ/2为横向磁场中空心长圆柱体的屏蔽因子。当$\zeta_1\Delta\lt\lt1$时，则H1≈H0，磁场穿透薄壁而均进入空腔，失去屏蔽作用，此时M≈0。类似于实心小样品，由GL理论可求出薄壁样品的临界磁场HK1，HK，HK2和临界尺寸等。
