Toroidal Approximate \( \vec{\nabla}\cdot \mathcal{K}_{\vec{\kappa}} \).
\( \vec{\hat{\nabla}}\cdot \mathcal{\hat{K}}_{\vec{\kappa}} = \frac{1}{R_0 I^2} \partial_{Z} I\)
- Note
- We implicitly assume the toroidal field line approximation, i.e. all curvature and other perpendicular terms assume that the perpendicular direction lies within the R-Z planes of a cylindrical grid (The plane \( \perp \hat{ e}_\varphi\) ). Additionally, in this version the magnetic field strength is simply the toroidal component of the magnetic field.