Beta: Difference between revisions
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(Created page with 'Plasma performance is often expressed in terms of beta (β), defined as: <ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 052…') |
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:<math>\frac{1}{\beta} = \frac{1}{\beta_p} + \frac{1}{\beta_t}</math> | :<math>\frac{1}{\beta} = \frac{1}{\beta_p} + \frac{1}{\beta_t}</math> | ||
== | == Normalized beta == | ||
The normalized beta is an operational parameter indicating how close the plasma is to reaching the [[Greenwald limit]]. Its definition is (for tokamaks): | |||
:<math>\beta_N = \beta \frac{a B}{I_p}</math> | |||
where ''B'' is in T, ''a'' in m, and ''I<sub>p</sub>'' in MA. | |||
== References == | == References == | ||
<references /> | <references /> |
Revision as of 11:58, 9 September 2009
Plasma performance is often expressed in terms of beta (β), defined as: [1]
i.e., the ratio of the plasma pressure to the magnetic pressure. Here, <p> is the mean plasma pressure, and B the mean total field strength. It is customary to introduce also the poloidal β (βp) and the toroidal β (βt), in which B is replaced by the poloidal and toroidal magnetic field component, respectively. One has:
Normalized beta
The normalized beta is an operational parameter indicating how close the plasma is to reaching the Greenwald limit. Its definition is (for tokamaks):
where B is in T, a in m, and Ip in MA.
References
- ↑ J.P. Freidberg, Plasma physics and fusion energy, Cambridge University Press (2007) ISBN 0521851076