The experimental dusty plasma device consists of a horizontal plasma chamber and a vertical dust dropping unit. The horizontal plasma chamber is a stainless steel cylindrical chamber of length 100 cm and having a diameter of 30 cm. The chamber is evacuated up to a pressure of 〖10〗^(-6) mbar with the help of a diffusion pump backed by a rotary pump. Plasma is produced by a hot cathode filamentary discharge technique. Multiple viewing ports are available in the chamber. Multi-cusp magnetic confinement system is used for confining the plasma. The vertical dust dropping unit is placed above the horizontal chamber having a height of 72 cm and 15 cm in diameter.
Recent Research Outcomes
br>
Effect of dust particle and magnetic field on EEPF and plasma oscillation
The significance of dust particles for the electron energy probability function (EEPF) and plasma oscillations is studied under varying magnetic field strength in a filamentary discharge hydrogen plasma. The experimental result shows that with an increase in dust density, the electron density decreases as a result of the charging of dust grains in the plasma background. We have observed that the increase in magnetic field decreases the lower energy electron population. From the study of plasma oscillation, it is observed that the dominant frequency associated with the plasma oscillation is matched with the ion cyclotron frequency. The amplitude of the ion cyclotron frequency reduces with the increase of dust density which might be due to the decrease of plasma density
|
Figure 1. EEPFs for different magnetic field strengths with different dust densities (black line = no dust; red line=〖1×10〗^11 m^(-3) ; blue line=〖3×10〗^11 m^(-3), pink line=〖5×10〗^11 m^(-3); green line = 〖7×10〗^11 m^(-3)).
|
|
Figure 2. Low energy electron density versus magnetic field strengths for different dust densities.
|
|
Figure 3. Ion cyclotron frequency versus magnetic field strength in absence/presence of dust.
|
Novel technique of producing negative hydrogen ions
H− ion based neutral beam injector is a critical heating and current drive system in a fusion reactor. However, the present H− ion source configuration has limitations in terms of production, extraction, cesium (Cs) inventory and management. To overcome these limitations, a proof-of-principle experiment based on a novel concept regarding surface assisted volume H− ions production by sprinkling Cs coated tungsten (W) dust grains (low work function surface) into a hydrogen plasma is carried out. Four different diagnostics have been used to validate the concept. The H− ion fraction is estimated from (a) Langmuir probe diagnostic, (b) phase velocity of ion acoustic waves, (c) dust current and confirmed by the measurement of (d) Balmer line ratio. The measured H− ion fraction with respect to the plasma density for different discharge conditions varies from ~0.2 to 0.3 in presence of Cs coated W dust particles.
|
Figure 4. I-V characteristics of a Langmuir probe at different experimental conditions.
|
|
Figure 5. H_x^+ ion density and electron temperature at different discharge conditions.
|
Ongoing experiments
Controlled production of two-electron temperature plasma and related experiments
In low pressure filament discharge plasmas, three groups of electrons are observed, ionising electrons, hot electrons and cold electrons. The ionising electrons are emitted from the filaments, which are accelerated by the discharge voltage towards the chamber walls. The hot electrons are those ionising electrons who lose energy due to collisions with the background gas, and the cold electrons are formed due to ionisation of neutral gas species. At high neutral pressure, the ionising electrons become identical to the hot electrons due to an increase in inelastic collisions with the neutrals and consequently a bi-Maxwellian electron distribution is achieved. The ongoing experiment focuses on developing a controllable production technique of two electron plasma in the dusty plasma experimental chamber. The study aims at establishing a handy mechanism for the production of two electron groups and later on the effect of hot electrons on dust charging mechanism along with wave propagation will be investigated.
|
Figure 6. Schematic diagram of two-electron temperature plasma related experimental set-up.
|