Usage of three Sample Clauses

Usage of three halfturn antenna at the Uragan-3M device. Three-halfturn (THT) antenna is regularly used at Uragan-3M device for Alvén plasma heating, while initial plasma is created with loop antenna which pulse precedes THT antenna impulse. The characteristic feature of this THT antenna regime is a possibility of operation at low initial neutral gas pressure ~3-5∙10-6 Torr. Plasma density increases gradually during impulse and can approach 1013 cm-3. Mainly plasma electrons are heated up to the temperature about 100 eV. RF power was supplied to antenna in a programmable way (by three-step increase) to the Uragan-3M plasma with the aim of keeping minimal start-up time of discharge and minimizing the antenna voltage. However, the programmable steps don’t guarantee reproducible plasma generation (no gas breakdown occurs with probability of 3%). Moreover, the discharge start-up time ∆t randomly deviates within the margins of 3-7 ms, that doesn’t allow maintaining stationary regime in reproducible way. THT antenna doesn’t create dense plasma in standard regime of Uragam-3M (toroidal magnetic field ≈0.72 T, RF heating frequency 8.6MHz), but low density plasma ≈1010 cm-3 is created sufficiently stably. This effect can be explained by slow wave generation that is excited by THT antenna via electrostatic mechanism. Experiments show that such plasma is quite suitable as initial for further stable production of dense plasma with the help of loop antenna. Decrease of magnetic field decreases a critical density value, starting from which Alvén resonances appear in plasma column. As soon as this value gets less than the plasma density created with the slow wave, plasma production becomes possible in the relay-race mode regime. It’s experimentally shown that THT antenna impulse creates high temperature dense plasma at magnetic field less than 0.7 T without pre-ionization, and plasma creation delay time decreases with magnetic field. Simultaneous work of loop and THT antennas provided high temperature dense plasma during whole impulse at magnetic field 0.68 T. The role of THT antenna was to create target plasma and to maintain plasma parameters both simultaneously with loop antenna and after loop antenna switch-off. (V.E. Moiseenko, V.V. Chechkin and others)
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