Beta: Difference between revisions

158 bytes added ,  13 April 2015
m
converted all html to math tags and added some minor information
No edit summary
m (converted all html to math tags and added some minor information)
Line 1: Line 1:
Plasma performance is often expressed in terms of beta (β), defined as:
Plasma performance is often expressed in terms of beta (<math>\beta</math>), defined as:
<ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 0521851076</ref>
<ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 0521851076</ref>


Line 5: Line 5:


i.e., the ratio of the plasma pressure to the magnetic pressure.
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.
Here, <math>\left \langle p \right \rangle </math> is the mean plasma pressure, and <math>B</math> the mean total field strength.
It is customary to introduce also the ''poloidal'' &beta; (&beta;<sub>p</sub>) and the ''toroidal'' &beta; (&beta;<sub>t</sub>), in which ''B'' is replaced by the poloidal and toroidal magnetic field component, respectively. One has:
It is customary to introduce also the ''poloidal'' beta <math>\beta_p</math> and the ''toroidal'' beta <math>\beta_t</math>, in which <math>B</math> is replaced by the poloidal and toroidal magnetic field component, respectively. One has:


:<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>
Line 15: Line 15:
<ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref>
<ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref>


:<math>\beta_N = \beta \frac{a B}{I_p}</math>
:<math>\beta_N = \beta_t \frac{a B_0}{I_p}</math>


where ''B'' is in T, ''a'' in m, and ''I<sub>p</sub>'' in MA.  
where <math>B_0</math> is the external magnetic field in T, <math>a</math> is the minor radius in m, and <math>I_p</math> is the plasma current in MA.  
Typically, the maximum value of &beta;<sub>N</sub> before the onset of deleterious instability is 3.5, although significantly higher values have been achieved.
Typically, the maximum value of <math>\beta_N</math> before the onset of deleterious instability is 3.5, although significantly higher values have been achieved.
<ref>[http://dx.doi.org/10.1088/0029-5515/46/5/014 S.A. Sabbagh et al, ''Resistive wall stabilized operation in rotating high beta NSTX plasmas'', Nucl. Fusion '''46''' (2006) 635-644]</ref>
<ref>[http://dx.doi.org/10.1088/0029-5515/46/5/014 S.A. Sabbagh et al, ''Resistive wall stabilized operation in rotating high beta NSTX plasmas'', Nucl. Fusion '''46''' (2006) 635-644]</ref>


3

edits