磁流的英文

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"磁流"怎么读用"磁流"造句

英文翻译手机版

ferrofluid
hydromagnetics
magnetic current
magnetic fluid
magnetic flux
magneticfluid

"磁"英文翻译 squeak; chirp; peep
"磁流波" 英文翻译 : hydromagnetic waver; hydromagnetic waves
"磁流管" 英文翻译 : flux tube
"磁流量" 英文翻译 : magnetic flow
"磁流体" 英文翻译 : hydromagnetic fluid; magnetic fluids; magnetofluid; magnetohydro
"磁通,磁流" 英文翻译 : magnetic flux
"电磁流" 英文翻译 : electromagnetic current
"隐磁流" 英文翻译 : hidden magnetic flux
"磁流波磁流体动力波" 英文翻译 : hydromagneticwave
"磁流包层" 英文翻译 : magnetic current sheath
"磁流测量计" 英文翻译 : magnetic flowmeter
"磁流单元" 英文翻译 : magnetic current element
"磁流电路" 英文翻译 : magnet current circuit
"磁流放大器" 英文翻译 : magnet current amplifier
"磁流力学" 英文翻译 : magnetofluidmechamics
"磁流量计" 英文翻译 : magnetic flow meter; magnetic induction flowmeter
"磁流哨声" 英文翻译 : hydromagnetic whistler
"磁流试验" 英文翻译 : magnaflux test; magnetic-flux test
"磁流速计" 英文翻译 : magnetic tachometer
"磁流体波" 英文翻译 : hydromagnetic wave
"磁流体的" 英文翻译 : hydromagnetic
"磁流体发电" 英文翻译 : magnetohydrodynamic generation
"磁流体发射" 英文翻译 : hydromagnetic emissions
"磁流体理论" 英文翻译 : hydromagnetic theory
"磁流体力" 英文翻译 : mhd force

例句与用法

Flux - tube dynamics
磁流管动力学
The expressions of external and internal coupling were derived from the reciprocity theorem by analysing slot voltage distribution in this paper , which invoked magnetic current to slots
缝隙之间的内(外)部互耦是从缝隙的口径电压出发、将缝隙等效为磁流源、通过互易原理而获得。
3 . a ~ vaveguide h - t coupler with a large aperture and an inductive post is analyzed where the magnetic current distribution is assumed on the aperture and the current on the surface of the post
将窗口等效为等效磁流源，而把匹配圆棒等效为电流源来处理，分析计算了这种耦合器的耦合特性。
Abstract : the general magnetic fluid grinding methods and magnetic fluids used home and abroad have been reviewed . the current research work and development prospect are also exposed
文摘:回顾了国内外常用的磁流研磨方法和采用的研磨流体，简述了磁流研磨领域的国内外研究概况及其发展前景。
In this part we start form the magnetic field integral equations ( mfie ) and then establish the matrix equations for the unknown magnetic currents on the surface of slot aperture . to solve this problem , piece - wise sinusoidal basis and galerkin ' s method are used
首先，利用理想缝隙假设建立关于缝隙内外口面磁流密度的磁场积分方程，然后采用分段正弦基galerkin方法将积分方程离散为关于展开系数的矩阵方程。
This method utilizes near - field data to determined an equivalent magnetic current source over a fictitious surface which encompass the em radiation source . this magnetic current , once determined , can be used to ascertain the near and the far field
将近场的测量数据用来确定一个等效磁流源，该等效磁流源位于包含电磁源辐射口面的假设平面上，当确定了这个等效磁流源以后，利用它计算出辐射源的近区场和远区场。
In the case of thin slot , taking the effect of wall thickness into account , the coupler is analyzed with the slots replaced by equivalence magnetic current using the equivalence principle . the integral equation system is fonned and calculated by the moment method
对于细长缝隙的情况，考虑了波导壁厚，利用等效原理将缝隙等效为磁流源在主波导和耦合波导中的作用，根据电磁场连续性条件建立积分方程，并用矩量法求解，进而求出耦合器的散射参数。
Due to the importance of the accuracy of the time - domain impedance matrix elements , the techniques by which treating of the singular integrals and near singular integrals arose from the tdie - mom solving process are analyzed in detail , and these techniques are utilized to solve the tdie . in the end , using triangle patches discretizing arbitrarily 3 - d dielectric objects and metal - nonmetal composite objects surface and utilizing spatial rwg and temporal triangular bases , the tdie are solved by mot algorithm
最后,分别对三维介质目标、金属非金属组合目标散射体表面用三角贴片离散,并在空间上采用rwg基函数,在时间上采用三角型时间基函数、利用阻抗元素的精确算法计算出阻抗矩阵,再运用mot法分别求解了介质体目标,金属非金属组合目标的时域积分方程,并分析了金属非金属组合目标分界面上的等效电流与等效磁流的特性。
Two cases are analyzedxonducting target with coat and dielectric target with coat . for the conducting target with coat , triangular patches are used to model the surfaces of the coat and the conducting object . now there have equivalent electric current and magnetic current on the surface of the coat , but only has equivalent electric current on the surface of the conducting object . the rwg vector base functions are used to denote equivalent electric currents and magnetic current . three integral equations should be built to obtain the unknown current coefficients ; for the dielectric object with coat , triangular patches are used to model the surfaces of the coat and the dielectric object . now there have equivalent electric current and magnetic current not only on the surface of the coat but also on the surface of the dielectric object . this time four integral equations should be built to obtain the unknown current coefficients
对于涂层导体目标，将涂层外表面和导体外表面进行三角形面元剖分，在涂层外表面有等效电磁流，导体外表面仅有等效电流(无等效磁流) 。将这些等效电磁流用rwg矢量基函数表示，需建立三个积分方程来求解未知的电磁流系数；对于涂层介质目标，将涂层外表面和内层介质外表面进行三角形面元剖分，在涂层外表面有等效电磁流，内层介质外表面也有等效电磁流，这时需建立四个积分方程来求解未知的电磁流系数。
Beginning with the equivalence principal , two types of near - field to far - field ( nfff ) transformation s are discussed systematically , i . e . frequency - domain nfff ( fd - nfff ) and time - domain nfff ( td - nfff ) . in td - nfff transformation , the concurrent - processing approach is used , where the contributions to far - field from the tangential electric current and magnetic current on the equivalence surface are calculated " on - the - fly " in step with the fdtd simulation . as a result , it is not necessary to store the tangential current components for every equivalence surface at every time step , and therefore reduce considerably computer storage required for the td - nfff transformation
在理论部分，本文从电磁场的等效原理出发，系统、详尽地论述了频域和时域近远场变换的基本思想，在时域近远场变换中采用实时的变换方法，即每进行一个时间步的迭代，就计算一次等效面上该时间步的切向电流和切向磁流对远场各方向的贡献，这样就使时域近远场变换不需要储存等效面上每一个时间步的切向电流和切向磁流，大大减小由于近远场变换而增加的计算机内存需要量。