Greenwald limit: Difference between revisions
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The Greenwald is an operational limit for the density in magnetic confinement devices: | The Greenwald limit is an operational limit for the density in magnetic confinement devices: | ||
<ref>[http://dx.doi.org/10.1088/0741-3335/44/8/201 M. Greenwald, ''Density limits in toroidal plasmas'', Plasma Phys. Control. Fusion '''44''' (2002) R27-R53]</ref> | <ref>[http://dx.doi.org/10.1088/0741-3335/44/8/201 M. Greenwald, ''Density limits in toroidal plasmas'', Plasma Phys. Control. Fusion '''44''' (2002) R27-R53]</ref> | ||
Revision as of 06:52, 7 September 2009
The Greenwald limit is an operational limit for the density in magnetic confinement devices: [1]
where nG is the density in 1020 m-3, Ip the plasma current in MA, and a the minor radius in m.
In tokamaks (and RFPs), exceeding the Greenwald limit typically leads to a disruption, although sometimes the limit can be crossed without deleterious effects (especially with peaked density profiles). Stellarators can typically exceed the Greenwald limit by factors of 2 to 5, or more (replacing Ip by an equivalent current corresponding to the magnetic field).
The mechanism behind this phenomenological limit is not understood, but probably associated with edge gradient limits.