Abstract:A neutral particle analyzer is used to measure the time-resolved energy spectrum of neutral hydrogen leaving a spheromak plasma. A gas cell filled with 10-50 mTorr of helium is used to strip electrons from incoming neutral hydrogen, lowering the minimum detectable energy well below that obtained with thin foils. Effective neutral particle temperature is calculated by fitting a Maxwellian energy distribution to the measured energy spectrum above and below approximately 300 eV. A computational model with approxi… Show more
“…The recent addition of a Charge-exchange Neutral Particle Analyzer (CNPA) has allowed measurements of charge exchange power losses and given and estimate of the majority ion temperature [20]. Escaping neutrals are collimated and then stripped by passing through neutral hydrogen.…”
Section: F Charge-exchange Losses and Ion Heatingmentioning
The Sustained Spheromak Physics Experiment (SSPX) [E.B. Hooper, et. al., Nuclear Fusion, Vol. 39,No. 7] explores the physics of efficient magnetic field buildup and energy confinement,
“…The recent addition of a Charge-exchange Neutral Particle Analyzer (CNPA) has allowed measurements of charge exchange power losses and given and estimate of the majority ion temperature [20]. Escaping neutrals are collimated and then stripped by passing through neutral hydrogen.…”
Section: F Charge-exchange Losses and Ion Heatingmentioning
The Sustained Spheromak Physics Experiment (SSPX) [E.B. Hooper, et. al., Nuclear Fusion, Vol. 39,No. 7] explores the physics of efficient magnetic field buildup and energy confinement,
“…The flux of neutral atoms is proportional to the product of the probabilities that these events occur. We measure the energy of these charge exchange neutrals with a radially viewing 25-channel analyzer [27]. By using information known about the neutral density profile and the plasma parameters which determine the attenuation (n e , T e , and n i ), information about the ion energy distribution function can be extracted from the neutral spectrum.…”
Complementary measurements of ion energy distributions in a magnetically confined high-temperature plasma show that magnetic reconnection results in both anisotropic ion heating and the generation of suprathermal ions. The anisotropy, observed in the C(+6) impurity ions, is such that the temperature perpendicular to the magnetic field is larger than the temperature parallel to the magnetic field. The suprathermal tail appears in the majority ion distribution and is well described by a power law to energies 10 times the thermal energy. These observations may offer insight into the energization process.
“…In operational energy range of our work this paprameter is approximately constant (0.286) like Ref. [11]. In other tokamaks that use this system for ion temperature measurement resolution depond on particle energy [12].…”
In this paper the average ion temperature of the TVD tokamak plasma is determined by a low cost charge exchange analyzer. When the neutral beam energy was equal to 3 keV, the stripping efficiency was 0.065. Estimated average ion temperatures for cold and hot regions of the plasma were 100 and 650 eV, respectively. Unlike the cold region of the plasma in which ion temperature was not related to the time, ion temperature in the hot region was maximum when the plasma current reached its maximum value.Keywords Tokamak Á Total detection efficiency Á Average ion temperature Á Flux of neutral atoms Á Hot and cold region of the plasma
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