$ \alpha $ contours in a toroidal annulus

Figure 21 compares the $ \phi $ coordinate surface of $ (\psi , \theta , \phi )$ coordinates with the $ \alpha $ coordinate surface of $ (\psi , \theta , \alpha )$ coordinates.

Figure 21: Comparison between isosurface of $ \phi = 2 \pi / 8$ (projection of magnetic field lines onto $ \phi = 2 \pi / 8$ plane) and isosurface of $ \alpha = 2 \pi / 8$. The $ \alpha $ isosurface is made of a family of contours of $ \alpha = 2 \pi / 8$, which are all magnetic field lines. These field lines are traced by starting from a series of points on the low-field-side midplane $ (\theta = 0)$ at different radial locations and the field lines are followed by a complete poloidal loop. The radial range is given by $ \psi _N \in [0.4 : 0.5]$, where $ \psi _N$ is the normalized poloidal magnetic flux. Magnetic field from EAST discharge #59954@3.03s.
\resizebox{8cm}{!}{\includegraphics{/home/yj/project_new/fig_lorentz/fig3g/p.eps}} \resizebox{8cm}{!}{\includegraphics{/home/yj/project_new/fig_lorentz/fig3f/p.eps}}

Figure 22: The same plot as in Fig. 21 but with a larger radial range. $ \psi _N \in [0.4 : 0.7]$, where $ \psi _N$ is the normalized poloidal magnetic flux.
\resizebox{8cm}{!}{\includegraphics{/home/yj/project_new/fig_lorentz/fig3i/p.eps}} \resizebox{8cm}{!}{\includegraphics{/home/yj/project_new/fig_lorentz/fig3h/p.eps}}

yj 2018-03-09