DocumentCode :
2880285
Title :
Plasma cloud generation with intense electric fields inside a porous spherical cavity resonator excited by an external plane wave
Author :
Bernhardt, P.A. ; Fernsler, Richard F. ; Fliflet, Arne W.
Author_Institution :
Plasma Phys. Div., Naval Res. Lab., Washington, DC, USA
fYear :
2011
fDate :
26-30 June 2011
Firstpage :
1
Lastpage :
1
Abstract :
Summary form only given. A porous spherical cavity resonator (PSCR) may be used to greatly increase the electric fields of a high power radio beam in order to produce isolated plasma clouds by neutral gas breakdown. The PSCR is a spherical polyhedron constructed from open surface polygons. The high-Q wave resonator can be excited at specific resonant frequencies by an external plane wave incident on the sphere. The resonant frequencies of the porous sphere are determined by the radius of the sphere and by the area of the openings in the surface of the sphere. The strength of the internal electric fields is influenced by the width of the conducting edges that comprise the polyhedron frame. The surface of the sphere contains polygons with dimensions much smaller than a wavelength. The transmission through the surface of the sphere decreases with the open area of the polygons. The optimum edge width is found where the external EM wave field excites the strongest internal field amplitudes by both letting the excitation field inside the sphere and keeping the internal fields contained. The WIPL-D EM simulation model is used to determine the optimum porous resonator for polyhedrons with 960 vertices (V960). All of the cavity modes for a solid spherical cavity resonator can be excited in the porous spherical cavity resonator (PSCR). With a high resonator Q, an EM plane-wave of 1 V/m can excite an internal electric field of over 1000 V/m. The spherical cavity modes are simulated to provide a variety of electric field distributions at the interior of the PSCR. The theory predicts that a wide variety of plasma clouds may be generated inside the sphere using selected resonant modes. This technique will be tested at NRL using a powerful (6 kW) plasma source operating at 2.54 GHz to illuminate a V960 ball fabricated out of stainless steel using stereo lithography processes.
Keywords :
cavity resonators; plasma electromagnetic wave propagation; plasma simulation; plasma sources; EM plane-wave; WIPL-D EM simulation model; cavity modes; conducting edge width; electric field distributions; excitation field; external EM wave field; external plane wave incident; frequency 2.54 GHz; high power radio beam; high-Q wave resonator; intense electric fields; internal electric field strength; internal field amplitudes; isolated plasma clouds; neutral gas breakdown; open surface polygons; opening area; optimum edge width; optimum porous resonator; plasma cloud generation; plasma source; polygon open area; polyhedron frame; porous sphere; porous spherical cavity resonator; power 6 kW; resonant frequencies; resonant modes; solid spherical cavity resonator; sphere radius; sphere surface; spherical polyhedron; stainless steel; stereolithography processes; Plasmas;
fLanguage :
English
Publisher :
ieee
Conference_Titel :
Plasma Science (ICOPS), 2011 Abstracts IEEE International Conference on
Conference_Location :
Chicago, IL
ISSN :
0730-9244
Print_ISBN :
978-1-61284-330-8
Electronic_ISBN :
0730-9244
Type :
conf
DOI :
10.1109/PLASMA.2011.5992982
Filename :
5992982
Link To Document :
بازگشت