Bootstrap current: Difference between revisions
Jump to navigation
Jump to search
(Created page with 'The bootstrap current is a Neoclassical toroidal current produced in the presence of a pressure gradient, associated with the existence of trapped (ban…') |
mNo edit summary |
||
Line 1: | Line 1: | ||
The bootstrap current is a [[Neoclassical transport|Neoclassical]] toroidal current produced in the presence of a pressure gradient, associated with the existence of trapped (banana) particles. | The bootstrap current is a [[Neoclassical transport|Neoclassical]] toroidal current produced in the presence of a pressure gradient, associated with the existence of trapped (banana) particles. | ||
These trapped particles must be able to complete their (banana) orbits, so a requirement for the existence of the bootstrap current is ν<sub>ei</sub> < ν<sub>b</sub> (the collision frequency is less than the banana | These trapped particles must be able to complete their (banana) orbits, so a requirement for the existence of the bootstrap current is ν<sub>ei</sub> < ν<sub>b</sub> (the collision frequency is less than the banana bounce frequency). | ||
The difference in particle density on banana orbits crossing a given radial position ''r'' then leads to a net toroidal current at ''r''. | The difference in particle density on banana orbits crossing a given radial position ''r'' then leads to a net toroidal current at ''r''. | ||
The bootstrap current is estimated (roughly) as | The bootstrap current is estimated (roughly) as |
Revision as of 08:48, 27 September 2009
The bootstrap current is a Neoclassical toroidal current produced in the presence of a pressure gradient, associated with the existence of trapped (banana) particles. These trapped particles must be able to complete their (banana) orbits, so a requirement for the existence of the bootstrap current is νei < νb (the collision frequency is less than the banana bounce frequency). The difference in particle density on banana orbits crossing a given radial position r then leads to a net toroidal current at r. The bootstrap current is estimated (roughly) as [1]
Here, ε is the inverse aspect ratio a/R, Bp the poloidal magnetic field, and p the pressure. More precise estimates can be made by simulating particle orbits.
References
- ↑ K. Miyamoto, Plasma physics and controlled nuclear fusion, Springer (2004) ISBN 3-540-24217-1