Abstract
The method for accelerating ions and electrons in the field-reversed configuration using odd-parity rotating magnetic fields (RMFs) in the ion-cyclotron range-of-frequencies (ICRF) is studied. The approach is based on long, accurate numerical integration of Hamilton's equations for single-particle orbits. Rapid ion heating to thermonuclear conditions occurs in <0.1 ms in a modest-sized FRC. Strong variation of the magnetic-field strength over the confinement region prevents a true cyclotron resonance, resulting in stochastic though effective heating. Lyapunov exponents are computed to demonstrate chaotic orbits. Electrons are also effectively heated in this frequency range, primarily by a mechanism involving trapping in the wells of the azimuthal electric field. Odd-parity RMF promotes oppositely directed ion and electron motion near the minor axis, appropriate for supporting the plasma current.
| Original language | English (US) |
|---|---|
| Pages (from-to) | 2093-2102 |
| Number of pages | 10 |
| Journal | Physics of Plasmas |
| Volume | 9 |
| Issue number | 5 |
| DOIs | |
| State | Published - May 2002 |
All Science Journal Classification (ASJC) codes
- Condensed Matter Physics