摘要: number of 2 X 10 18 and 1 1018 for the 1st 2nd plasmoid, respectively, is obtained. In Fig. 5, resulting energy balance presented as a function U. The effective ionization .EJion.eff was calculated using Eq. (2). Discussion This investigation did not serve so much to study acceleration plasma, but rather get information on continuously working plasma source with well-defined initial velocity v. It can be seen from that v varies slowly As known earlier investigations, oscillating frequency / has strong influence will investigated by further measurements. 3 shows an increase Eiot up factor larger than two yields only in Epi about 40%, because cti decreases increasing main portion Ep\ (Fig. 5) needed E-10n,en (more 90%), whereas E^n ^therm attain small values. 5), Ei0n,eff per particle ten times theoretical value which 4 10~18 //particle. Because technical physical reasons, realizable range flux N accelerators 1020 — 21 particles/sec. Thus, necessary power requirement Pp\ such estimated approximately PPi ~ (particles/s)-#ion,eff(//particles) Therefore, Ppi 5 kw < 50 kw. efficiency transfer rjeft (Eq. 7) 60-90% pulsed accelerator, assuming similar values continuous accelerator must divided corresponding rjett.