Instrument for measuring the electric field vector of high-voltage equipment

1983 ◽  
Vol 26 (1) ◽  
pp. 49-50
Author(s):  
I. P. Klimashevskii ◽  
B. L. Kondrat'ev ◽  
V. A. Poletaev ◽  
V. M. Yurkevich
Keyword(s):  
Electric Field ◽  
High Voltage ◽  
Field Vector ◽  
Electric Field Vector

Spatio-temporal and vectorial analysis of the electric field vector with an optical sensor

2014 ◽  
Author(s):  
Gwenael Gaborit ◽  
Pierre Jarrige ◽  
Frederic Lecoche ◽  
Jean Dahdah ◽  
Lionel Duvillaret
Keyword(s):  
Electric Field ◽  
Optical Sensor ◽  
Field Vector ◽  
Electric Field Vector ◽  
Spatio Temporal

Study on the Electromagnetic Responses of Split Ring Resonator in THz Regions

2013 ◽  
Vol 760-762 ◽  
pp. 302-305
Author(s):  
Wei Kai Xu ◽  
Ying Chun Tang ◽  
Wei Wang
Keyword(s):  
Electric Field ◽  
Ring Resonator ◽  
Split Ring Resonator ◽  
Field Vector ◽  
Electric Response ◽  
Electric Field Vector ◽  
Split Ring ◽  
Response Characteristics ◽  
Terahertz Region ◽  
Simulation Techniques

By using the numerical simulation techniques, the response characteristics of single split-ring resonator (SRR) in a broadband terahertz region are analyzed. We examine the transmission and dispersion characteristics of the SRR and show that there are different resonances while changing the orientations of electric field vector relative to the gap-bearing sides. Two significant resonances corresponding to electric response and magnetic response will be observed while the electric field vector perpendicular to the gap-bearing side, and only one electric resonance occurs when the electric field vector parallel to the same side. This will be a reference to design the possible terahertz metamaterials.

scholarly journals Detailed study of transient anomalous electric field vector focused by parabolic mirror

2017 ◽  
Vol 19 (3) ◽  
pp. 035603 ◽  
Author(s):  
Kazunori Shibata ◽  
Mitsuharu Uemoto ◽  
Mayuko Takai ◽  
Shinichi Watanabe
Keyword(s):  
Electric Field ◽  
Field Vector ◽  
Electric Field Vector ◽  
Parabolic Mirror

scholarly journals 5 GHz EVN Polarization of 3C286

1996 ◽  
Vol 175 ◽  
pp. 85-87 ◽  
Author(s):  
D. Dallacasa ◽  
R.T. Schilizzi ◽  
H.S. Sanghera ◽  
D.R. Jiang ◽  
E. Lüdke ◽  
...  
Keyword(s):  
Electric Field ◽  
Radio Source ◽  
Field Vector ◽  
Central Component ◽  
Electric Field Vector ◽  
Powerful Radio ◽  
Line System ◽  
Rotation Measure ◽  
Polarized Emission ◽  
5 Ghz

3C286 (1328+307) is a powerful radio source identified with a quasar at z=0.849. There is a foreground galaxy responsible for an H I absorption line system at z=0.6922 (Brown & Roberts 1973), centered approximately 2.″5 to the southeast of 3C286. The radio source has a steep spectrum (α = −0.61, Sv ∝ vα between 1.4 and 15 GHz) which turns over at about 100 MHz. Subarcsecond resolution radio images show a misaligned triple structure, dominated by the central component (Spencer et al. 1989) which accounts for at least 95% of the total flux density at all frequencies. 3C286 is one of the strongest extragalactic sources in polarized emission (0.84 Jy at 5 GHz and 1.41 Jy at 1.4 GHz) and with a rotation measure close to 0 rad m–2 (Rudnick and Jones 1983). Hence the observed orientation of the electric field vector is essentially independent of frequency.

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