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1)  lossy media
损耗媒质
1.
It is found that the ordinary boundary conditions of harmonic electromagetic fields at interface of lossy media may not be satisfied simultaneously,which is due to that the different damping terms between the two media may lead the flux at Gauss surface and circumfluence along close loop of electromagetic fields near interface to be no longer harmonic.
通常的谐变电磁场边界条件方程在损耗媒质界面往往不能同时成立,这是因为界面两边媒质不同的损耗,可导致界面处电磁场相关的通量和环量不再是谐变函数。
2)  loss-free medium
无损耗媒质
3)  lossy medium
有损耗媒质
4)  medium-loss fiber
媒质损耗光纤(光)
5)  inhomogeneous and low lossy media
非均匀低损耗媒质
6)  lossy medium
有耗媒质
1.
As the real part of the divergence of Poynting vector for lossy medium must be less than zero and the propagation condition must be satisfied, the sufficient and essential judgement criterions, which the sourceless lossy anisotropic medium parameters must satisfied, are obtained.
从Maxwell方程出发 ,导出了平面波入射到半无界均匀各向异性媒质时电磁场的相互关系 ,根据有耗媒质应满足波传播条件和玻印廷矢量散度的实部应小于零 ,推得了无源有耗各向异性材料参数应满足的条件 ,论述了该有耗判别准则的充要性 ,为任意吸波材料参数的反演研究打下了理论基
2.
Laplace transform and variable separation (the so called Harmuth’s technique) are two common methods in deriving the transient solutions of Maxwell’s equations in lossy medium.
在相同的初边值条件下 ,首先给出了有耗媒质中Maxwell方程组的拉普拉斯变换法解和分离变量法解 。
3.
This paper present the reflectance and index of refraction, on conditon that uniform or nonuniform electromagnetic planewave incident in oblique angle upon the surface of lossy medium.
本文给出了有耗媒质界面上均匀与非均匀平面电磁波斜入射时的反射系数、透射系数的计算公式,并进而计算出了单层平板媒质的屏蔽效能。
补充资料:介质损耗角正切试验(见电容率与损耗因数试验)


介质损耗角正切试验(见电容率与损耗因数试验)
dielectric loss tangent test

)!eZh.sunhooJ一002匕engq一e sh一yon介质损耗角正切试验(dieleetri。1055 tangenttest)见电容率与损耗因数试验。
说明:补充资料仅用于学习参考,请勿用于其它任何用途。
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