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:<math> | :<math> | ||
\sqrt{g_B} = \frac{V'}{4\pi^2}\frac{\langle B^2\rangle} {B^2} | \sqrt{g_B} = \frac{V'}{4\pi^2}\frac{\langle B^2\rangle} {B^2} | ||
</math> | |||
== Contravariant representation of the magnetic field in Boozer coordinates == | |||
In Boozer coordinates the angular covariant <math>B</math>-field components are flux functions | |||
:<math> | |||
\mathbf{B} = -\tilde\eta\nabla\psi + \frac{I_{tor}}{2\pi}\nabla\theta + \frac{I_{pol}^d}{2\pi}\nabla\phi~. | |||
</math> | </math> |
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