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IEEE Transactions on Plasma Science | 1994

Discharge features in a steady-state nitrogen arcjet engine with an expansion nozzle

Hirokazu Tahara; Nobuki Uda; Ken-Ichi Onoe; Yasuji Tsubakishita; Takao Yoshikawa

Nitrogen discharges in a 10-kW-class water-cooled arcjet engine were studied by means of spectroscopic diagnostics. The atomic excitation temperature and electron density in the constrictor increased from 15,000 to 18,000 K and from 1/spl times/10/sup 15/ to 2/spl times/10/sup 16/ cm/sup /spl minus/3/, respectively, with input power levels of 7-11 kW. An increase in the mass flow rate raised the electron density because of enhanced thermal pinch effect of the arc column. In the expansion nozzle, the pressure and electron density decreased drastically downstream, and therefore the plasma was expected to be in high non-equilibrium. The N/sub 2//sup +/ vibrational temperature reached about 6,000 K at the nozzle exit, and the N/sub 2//sup +/ rotational temperature decreased gradually resulting in a range of 1,000-2,500 K. >


Japanese Journal of Applied Physics | 1993

Plasma Generation by Resonant-Cavity Microwave Discharge and Its Applications for Material Processing

Hirokazu Tahara; Ken-ichiro Minami; Toshiaki Yasui; Ken-Ichi Onoe; Yasuji Tsubakishita; Takao Yoshikawa

A 2.45-GHz-microwave plasma source with a resonant cavity was studied for material processing under medium to atmospheric pressures. Stable plasmas, with electron temperature and density of 1 to 5 eV and beyond the plasma cutoff density, respectively, were efficiently sustained in an ambient pressure of 10-2-10 kPa with hydrogen, helium, nitrogen, argon and a mixture of H2+2H2 (vol. rate). The operational characteristics of coupling efficiency and cavity length depended on gas species. From electric fields measured on the cavity inner wall, the electromagnetic field pattern of TM011 resonance mode was expected to be excited in the cavity over a wide range of operational conditions. In addition, operation of a plasmajet generator, into which the plasma source was modified, diamond film synthesis and surface modification due to atomic oxygen were demonstrated.


Japanese Journal of Applied Physics | 1993

Microwave Ion Source Using Resonant Cavity

Hirokazu Tahara; Toshiaki Yasui; Ken-Ichi Onoe; Yasuji Tsubakishita; Takao Yoshikawa

Ring-cusped magnetic-field ion sources using 2.45-GHz-microwave resonant cavities were studied to develop high-performance compact ion sources for economically assisting material processings. The minimum flow rate required to sustain discharge was 10 sccm for weak-B-field off-resonance discharge in the TM011-mode-excitation cylindrical cavity, 6 sccm for weak-B-field discharge in the reentrant coaxial cavity, in which a stronger electric field was generated compared with that in the cylindrical cavity, and 3 sccm for electron cyclotron resonance (ECR) discharge in the cylindrical cavity. As a result of ion beam extraction, the highest mass utilization efficiency of 18.7% was achieved for ECR discharge.


Review of Scientific Instruments | 1994

Long plasma generation using microwave slot antennas on a rectangular waveguide

Hirokazu Tahara; Jiro Kitayama; Toshiaki Yasui; Ken-Ichi Onoe; Yasuji Tsubakishita; Takao Yoshikawa

30‐cm‐class long plasmas were generated using 2.45‐GHz microwave slot antennas on a rectangular waveguide with a T‐shaped ridge for the development of high performance ion sources or for plasma reactors for large‐area material processing. The microwave coupling efficiencies above 85% were achieved for Ar, N2, and O2 over large flow rate ranges. From the electric fields on the inner wall E side of the waveguide, standing waves with the maximum electric field strength of about 30 kV/m were expected to be excited in the waveguide, depending on the location of the T‐shaped ridge. The plasma density for Ar was in the order of 1017 m−3 and for N2 and O2 1016 m−3 in a discharge chamber in front of the slot antennas. The electron temperature for Ar ranged from 3 to 4 eV and for N2 and O2 from 3 to 8 eV. The spatial profiles of the ion saturation current for Ar were almost flat in the discharge chamber although the profiles for N2 and O2, with large flow rates or near the antennas, were slightly rough.


Laser and Ion Beam Modification of Materials#R##N#Proceedings of the Symposium U: Material Synthesis and Modification by Ion Beams and Laser Beams of the 3rd IUMRS International Conference on Advanced Materials, Sunshine City, Ikebukuro, Tokyo, Japan, August 31–September 4, 1993 | 1994

DEVELOPMENT OF A REENTRANT-CAVITY-TYPE ELECTRON CYCLOTRON RESONANCE (ECR) ION SOURCE AND ITS APPLICATIONS FOR MATERIAL PROCESSING

Toshiaki Yasui; Miki Hiramatsu; Hirokazu Tahara; Ken-Ichi Onoe; Yasuji Tsubakishita; Takao Yoshikawa

An Electron Cyclotron Resonance (ECR) ion source using a reentrant coaxial cavity was newly developed. The reentrant coaxial cavity forces microwaves to propagate into plasmas from an annular window of a discharge chamber side wall. Uniform plasmas were obtained above 10 sccm of a mass flow rate for Ar. On the axis of the discharge chamber, the plasma density was higher than the cutoff density for Ar, although lower for O 2 and N 2 . The maximum ion beam current of 63.5 mA was obtained at a forward power of 304 W for Ar.


Laser and Ion Beam Modification of Materials#R##N#Proceedings of the Symposium U: Material Synthesis and Modification by Ion Beams and Laser Beams of the 3rd IUMRS International Conference on Advanced Materials, Sunshine City, Ikebukuro, Tokyo, Japan, August 31–September 4, 1993 | 1994

Performance characteristics of a sheet-shaped microwave ion source using slot antennas on a rectangular waveguide

Jiro Kitayama; Toshiaki Yasui; Hirokazu Tahara; Ken-Ichi Onoe; Yasuji Tsubakishita; Takao Yoshikawa

A 30-cm-class sheet-shaped 2.45-GHz-microwave ion source using slot antennas on a rectangular waveguide with a T-shaped ridge was newly developed. The microwave coupling efficiencies above 85% were achieved for Ar, N 2 and O 2 over large flow rate ranges. The plasma density for Ar was in an order of 10 17 m -3 and for N 2 and O 2 of 10 16 m -3 . The electron temperature for Ar ranged from 3 to 4 eV and for N 2 and O 2 from 3 to 8 eV. The spatial profiles of the ion saturation current for Ar were almost flat in the discharge chamber although the profiles for N 2 and O 2 , with large flow rates or near the slot antennas, were slightly rough. As a result, the maximum ion current of 60 mA with a beam size 70 × 280 mm for Ar was achieved at a beam voltage of 400 V.


Archive | 1992

Flowfield analysis of an arcjet thruster

Nobuki Uda; Hirokazu Tahara; Ken-Ichi Onoe; Takao Yoshikawa


Vacuum | 2002

Plasma plume characteristics of supersonic ammonia and nitrogen/hydrogen-mixture DC plasma jets for nitriding under low-pressure environment

Hirokazu Tahara; Yasutaka Ando; Ken-Ichi Onoe; Takao Yoshikawa


30th Plasmadynamic and Lasers Conference | 1999

dc arcjet plasma characteristics using ammonia and mixture of nitrogen and hydrogen

Hirokazu Tahara; Tomoki Taniguchi; Ken-Ichi Onoe; Takao Yoshikawa


Electrical Engineering in Japan | 1989

Fundamental operational characteristics of a microwave-heating-type plasmajet using a resonant cavity for space propulsion

Hirokazu Tahara; Yoshimasa Tanaka; Masao Abuku; Toshiaki Yasui; Ken-Ichi Onoe; Takao Yoshikawa

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Toshiaki Yasui

Toyohashi University of Technology

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