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Content available remote Parallel implementation of a PIC simulation algorithm using OpenMP
EN
Particle-in-cell (PIC) simulations are focusing on the individual trajectories of a very large number of particles in self-consistent and external electric and magnetic fields; they are widely used in the study of plasma jets, for example. The main disadvantage of PIC simulations is the large simulation runtime,which often requires a parallel implementation of the algorithm. The current paper focuses on a PIC1d3v simulation algorithm and describes the successful implementation of a parallel version of it on a multi-core architecture, using OpenMP, with very promising experimental and theoretical results.
PL
Doświadczalnie stwiedzono, że naniesienie powłok proszkowych PG-10N-01, PG-19N-01 i PGAN-33 metodą detonacji plazmowej z podwójną obróbką powierzchni powoduje powstawanie wielofazowych powłok. Stopienie powłok wiązką elektronów prowadzi do zmian rozkładupierwiastków. Powłoki posiadają mikrotwardość ok. 5 GPa. Metodą transmisyjnej mikroskopii elektronowej ustalono obecność faz amorficznej i krystalicznej.
EN
In the presented work it was empirically demonstrated that depositing PG-10N-01, PG-19N-01 and PGAN-33 (Russia Industrial Standard) powder coatings by plasma jets with the duplex surface treatment according to the parameters resulted in forming multi-phase dense coatings with intermetallic hardening compounds. The surface melting of coatings by electronic beam leads to redistribution of elements. The coatings have high microhardness of the same order of 5 GPŕ. TEM methods reveal that in coatings before irradiation form the amorphous and crystalline phases.
EN
The properties of an argon D.C. arc-jet thruster for space propulsion functioning at low electric power (around 10 kW) and low mass flow (0.5 g/s) are determined. The physical description of the arc and jet plasma takes into account non-equilibrium conditions for local kinetic temperatures and ionization effect. The plasma properties (velocity, pressure, electron and heavy particles temperatures and densities) are calculated by a Navier-Stokes modeling. The influence of different plasma source geometry such as angle and length of the nozzle divergent part and electric power on thrust, specific impulse and arc-jet efficiency are discussed.
EN
The aim of the present experiments was to reproduce and to study in laboratory quasi-perpendicular supercritical collisionless shocks similar to the Earth-Solar Wind shock, by using a plasma focus facility as the plasma source. The experiments were performed on the PF-3 facility (Filippov-type plasma focus) at a level of energy supply of about 1 MJ. Directed plasma jets are produced with axial velocities ~107 cm/s after compression of a plasma-current sheath in the initial stage of plasma focus formation. These jets then travel through an ambient plasma resulting in early gas ionization by X-ray radiation from the plasma focus, and at an angle of 90° to the 2500 G external magnetic field applied by a system based on rear-earth magnets. Our experimental conditions allowed us to reach a range MA ~ 5÷10.
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