electron component
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Author(s):  
Г.С. Курскиев ◽  
Н.С. Жильцов ◽  
А.Н. Коваль ◽  
А.Ф. Корнев ◽  
А.М. Макаров ◽  
...  

Diagnostics of the plasma electron component by the method of Thomson scattering (TS) of laser radiation makes it possible to reliably measure the spatial distributions of the electron temperature and density. One of the obstacles to the implementation of TS diagnostics in thermonuclear reactors is the distortion of the spectral characteristics of the optical system due to radiation-induced absorption and contamination of optical elements with erosion products of the first wall. As a consequence, the reliability of measurements by the TS method will decrease over time. The paper describes the method of multi-laser Thomson scattering, which will solve this problem. The results of the first experiments on the Globus-M2 tokamak are also presented.


2020 ◽  
Author(s):  
Mika Holmberg ◽  
Fabrice Cipriani ◽  
Grégoire Déprez ◽  
Christian Imhof ◽  
Olivier Witasse ◽  
...  

<div class="x_gmail-co_mto_htmlabstract-content x_gmail-mt-3"> <p>We use Spacecraft Plasma Interaction Software (SPIS) simulations of the surface charging of the Jupiter Icy Moons Explorer (JUICE) spacecraft to study how the variable magnetospheric environment of Jupiter will impact the future JUICE particle and electric field measurements.</p> <p>The study has been limited to the magnetospheric region relevant for JUICE, that is, the environments of the inner and middle magnetosphere of Jupiter. The closest approach of Jupiter will be at 9.3 R<sub>J</sub>. In the inner magnetosphere the spacecraft will charge a few volts negative for the typical plasma sheet environment, where n<sub>e,cold</sub> ≈ 50 cm<sup>-3</sup> and T<sub>e,cold</sub> ≈ 20 eV. However, Galileo detected plasma densities of up to 600 cm<sup>-3</sup> in the region around 9.4 R<sub>J</sub> (Kurth et al., 2001). These densities could be due to activity on Europa, such as plumes, or a local disturbance of cold and dense iogenic plasma (Bagenal et al., 2015). Such high densities could result in surface potentials of tens of volts, when assuming T<sub>e,cold</sub> ≈ 5 eV, which would inhibit cold electron measurements performed by the electron spectrometer of JUICE, since the electrons would be repelled before reaching the detector. In addition, the large differential charging of tens of volts, due to the dielectric surfaces, would disturb electric field measurements. However, the cold electron temperature is not well constrained for this particular disturbance and a lower plasma temperatures would decrease the magnitude of the surface potential.</p> <p>Our SPIS simulations show surface potentials of a few volts positive for typical magnetospheric environments in the plasma sheet between 15 and 26 R<sub>J</sub>, where n<sub>e,cold</sub> > 20 n<sub>e,hot</sub> and the hot electron component range from 1-5 keV. However, Galileo measurements occasionally show hot electron densities equal to or slightly larger than the typical cold electron densities (Futaana et al., 2018). Simulated surface potentials, using n<sub>e,cold</sub> ≈ n<sub>e,hot</sub>, show no significant difference compared to the typical environment since the increase in hot electrons is counterbalanced by the increase in the production of secondary electrons. In this particular environment, higher electron densities will charge the spacecraft more negative while higher secondary electron production will charge the spacecraft more positive. Assuming Maxwellian distributions, we obtain that an unusually dense hot, 1-5 keV, electron component, like the one measured by Galileo, would not disturb the particle measurements of JUICE.</p> <p>Our study shows that the absolute charging of the spacecraft strongly depends on the cold electron density and temperature, and, for certain environments, on the spacecraft orientation relative to the plasma flow and the solar radiation. An unusually dense and hot, 1-5 keV, electron plasma component will not have a substantial impact on the charging, in the studied region. We are investigating whether different energy distributons will change this conclusion. The SPIS JUICE surface charging simulation results show that only minor perturbations will be obtained in typical Jovian magnetospheric environments, while substantial perturbations will occasionally occur in the disturbed magnetosphere.</p> </div>


2019 ◽  
Vol 1394 ◽  
pp. 012002
Author(s):  
L.V Shibkova ◽  
V.M Shibkov ◽  
A.A Logunov ◽  
A.A Andrienko ◽  
K.N Kornev ◽  
...  

2019 ◽  
Vol 83 (8) ◽  
pp. 991-994
Author(s):  
A. A. Lagutin ◽  
N. V. Volkov ◽  
A. I. Goncharov ◽  
T. L. Serebryakova ◽  
R. I. Raikin

Author(s):  
Е.А. Генрих ◽  
М.А. Боронина

Представлена гибридная математическая модель осесимметричной плазменной ловушки, основанная на кинетическом описании для ионной компоненты плазмы и приближении МГД для электронной компоненты. На основе гибридной модели разработан двумерный алгоритм для изучения динамики разлета инжектируемых частиц в поле ловушки. Движение ионной компоненты рассчитывается по методу частиц в ячейках, для расчета магнитного поля и электронной компоненты плазмы используются конечно-разностные схемы. На основе разработанного алгоритма создан комплекс программ для исследования механизмов формирования самосогласованной структуры магнитного поля ловушки. A hybrid mathematical model of an axisymmetric plasma trap based on the kinetic description for the ion component of the plasma and the MHD approximation for the electronic component is presented. On the basis of the hybrid model, a two-dimensional algorithm is developed to study the dynamics of injected particles in the trap field. The motion of the ion component is calculated by the particle-in-cell method. Finite-difference schemes are used to calculate the magnetic field and the electron component of the plasma. On the basis of the developed algorithm, a program code is created to study the mechanisms of the self-consistent magnetic field structure formation.


2016 ◽  
Vol 23 (6) ◽  
pp. 062302 ◽  
Author(s):  
L. N. Mbuli ◽  
S. K. Maharaj ◽  
R. Bharuthram ◽  
S. V. Singh ◽  
G. S. Lakhina

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