The Lateral Shift of Quasi-Total Reflection of Inhomogeneous Electromagnetic Wave when the Electric Field is Perpendicular to the Incident Plane

2005 ◽  
Vol 48 (4) ◽  
pp. 989-998 ◽  
Author(s):  
Fu-Ping LIU ◽  
Hong-Mei ZHANG ◽  
Chang-Chun YANG ◽  
Rui-Zhong LI ◽  
An-Ling WANG ◽  
...  
Keyword(s):  
Electromagnetic Wave ◽  
Electric Field ◽  
Total Reflection ◽  
Lateral Shift ◽  
Incident Plane ◽  
Inhomogeneous Electromagnetic Wave

The Lateral Shift of Reflected Inhomogeneous Electromagnetic Wave on the Interface of Conductive Media

2006 ◽  
Vol 49 (2) ◽  
pp. 474-482 ◽  
Author(s):  
Fu-Ping LIU ◽  
Rui-Zhong LI ◽  
Chang-Chun YANG ◽  
Hong-Mei ZHANG ◽  
Hui-Guo CHEN ◽  
...  
Keyword(s):  
Electromagnetic Wave ◽  
Lateral Shift ◽  
Inhomogeneous Electromagnetic Wave ◽  
Conductive Media

Emission Spectrum and Charged-Particle Trajectory in the Field of an Inhomogeneous Electromagnetic Wave

2019 ◽  
Vol 64 (10) ◽  
pp. 377-380
Author(s):  
V. B. Lapshin ◽  
A. A. Skubachevskiy ◽  
A. V. Belinsky ◽  
A. S. Bugaev
Keyword(s):  
Electromagnetic Wave ◽  
Charged Particle ◽  
Emission Spectrum ◽  
Particle Trajectory ◽  
Inhomogeneous Electromagnetic Wave

Electric-Field-Induced Reorientation of Liquid Crystalline p-Cyanophenyl-p-n-Alkylbenzoates: A Time-Resolved Study by Fourier Transform Infrared Transmission and Attenuated Total Reflection Spectroscopy

2003 ◽  
Vol 57 (5) ◽  
pp. 499-505 ◽  
Author(s):  
E. Klimov ◽  
M. Fuelleborn ◽  
H. W. Siesler
Keyword(s):  
Fourier Transform ◽  
Electric Field ◽  
Liquid Crystalline ◽  
External Perturbation ◽  
Fourier Transform Infrared ◽  
Surface Region ◽  
Total Reflection ◽  
Attenuated Total Reflection ◽  
Infrared Transmission ◽  
Time Resolved

Time-resolved polarization Fourier transform infrared (FT-IR) transmission and attenuated total reflection (ATR) spectroscopy were applied to investigate the reorientation phenomena of the three members of the homologous series of nematic liquid crystalline p-cyanophenyl-p-n-alkylbenzoates 6CPB, 7CPB, and 10CPB under the external perturbation of an electric field. In conjunction with a newly constructed measurement cell, this method allowed us to differentiate the response of the LC system in the surface layer and in the bulk of the cell at different temperatures and voltages. The relaxation time of the LC molecules close to the wall of the cell was found to be shorter than in the bulk. However, at a field strength of 7 V, the initial orientation in the bulk preceeds the analogous process in the surface region.

Topologic configuration of electron

2018 ◽  
Vol 33 (26) ◽  
pp. 1850163
Author(s):  
Qing Yang ◽  
J. D. Fan
Keyword(s):  
Magnetic Field ◽  
Electromagnetic Wave ◽  
Electric Field ◽  
Classical Mechanics ◽  
Three Dimensional ◽  
Möbius Strip ◽  
Left Hand ◽  
Topological Configuration ◽  
Microscopic World ◽  
Mobius Strip

Motion of an electron is much different from that of a kind of matter in classical mechanics. Although it is impossible to directly observe the configuration of a bare electron, it is never as simple as to treat it as a three-dimensional (3D) particle in the microscopic world because the electron itself certainly has its own topological configuration, so that it presents a field of a unit charge and a spin, etc. An electron produces a magnetic field in motion and also can radiate or absorb an electromagnetic field in its accelerating motions. Thus, the topological configuration of an electron must be related or similar to the configurations of the magnetic field and electromagnetic wave. Starting from the topological configuration of a single electromagnetic wave, it is possible to derive that an electron is a quantized left-hand Möbius strip, on the center of which there exists an anti-neutrino. The Möbius strip excites a [Formula: see text] circumference of a unit negative charge and a linear electric field of a [Formula: see text] torsion and can explain the wave feature of the electron and the essential cause of producing a magnetic field and radiating an electromagnetic wave as well as predict that the second-order tensor field among the three quarks in a proton has a topological configuration of right-hand three-leaf knot and can excite a [Formula: see text] circumference of a unit positive charge and a linear electric field of a [Formula: see text] torsion, which is just allelomorphic to an electron.

Dependent Scattering Properties of Woven Fibrous Insulations for Normal Incidence

1995 ◽  
Vol 117 (1) ◽  
pp. 160-166 ◽  
Author(s):  
Sunil Kumar ◽  
S. M. White
Keyword(s):  
Electromagnetic Wave ◽  
Plane Electromagnetic Wave ◽  
Normal Incidence ◽  
Woven Fabrics ◽  
Fibrous Materials ◽  
Parallel Fibers ◽  
Closed Form Solutions ◽  
Incident Plane ◽  
Additional Interaction ◽  
The Difference

The scattering properties of woven fibrous materials are examined in this paper and a simple model is presented to account for the interactions between the scattered radiation from different individual fibers. The case of a normally incident plane electromagnetic wave is considered. Fiber sizes in the Rayleigh regime are considered for developing closed-form solutions. Previous studies in the literature that have addressed the scattering properties of fibrous materials have mostly ignored the effect of constructive or destructive addition of scattered waves from individual fibers, the exception being the case of parallel fibers. The difference in the effects of interference on scattering properties of parallel fibers and of woven fabrics arises from the additional interaction of radiation scattered from mutually perpendicular fibers in the latter case, which further complicates the analysis.

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