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Electric current dynamics in the stellarator coil winding surface model

Wadim Gerner, Anouk Nicolopoulos-Salle, Diego Pereira Botelho

Abstract

In stellarator design, the coil winding surfaces $Σ\subset\mathbb R^3$ support current distributions $j$ that shape the magnetic field. This work provides a theoretical framework explaining the emergence of centre and saddle point regions, a key feature in coil optimisation. For coil winding surfaces with a toroidal shape, we prove a dichotomy principle: the current distribution has both centre and saddle point regions or is no-where vanishing. For coil winding surfaces that consist of piecewise cylinders, we show that if $j$ is oppositely oriented on the two boundary circles, centre and saddle points appear, and all but finitely many field lines of $j$ are periodic. When $j$ admits a harmonic potential, all field lines are closed poloidal orbits. These results offer insights into current patterns on winding surfaces, with implications for coil design strategies and their simplification.

Electric current dynamics in the stellarator coil winding surface model

Abstract

In stellarator design, the coil winding surfaces support current distributions that shape the magnetic field. This work provides a theoretical framework explaining the emergence of centre and saddle point regions, a key feature in coil optimisation. For coil winding surfaces with a toroidal shape, we prove a dichotomy principle: the current distribution has both centre and saddle point regions or is no-where vanishing. For coil winding surfaces that consist of piecewise cylinders, we show that if is oppositely oriented on the two boundary circles, centre and saddle points appear, and all but finitely many field lines of are periodic. When admits a harmonic potential, all field lines are closed poloidal orbits. These results offer insights into current patterns on winding surfaces, with implications for coil design strategies and their simplification.
Paper Structure (17 sections, 17 theorems, 44 equations, 10 figures)

This paper contains 17 sections, 17 theorems, 44 equations, 10 figures.

Key Result

Theorem 1.1

Let $T^2\cong\Sigma\subset\mathbb{R}^3$ be a smooth toroidal surface and let $j$ be a "generic" smooth, divergence-free current on $\Sigma$. Then we have the following dichotomy:

Figures (10)

  • Figure 1: Left side: A centre region, the field lines wrap around in circles around a singularity of the field (red dot). Right side: A saddle region, around the red dot.
  • Figure 2: Left: A toroidal coil winding surface. Right side: A coil winding surface made of cylindrical structures.
  • Figure 3: Left: A toroidal coil winding surface with coils depicted by red strips. Right: A piecewise cylindrical coil winding surface with coils depicted by red strips.
  • Figure 4: Two oppositely oriented boundary circles. Directions indicated by the arrows on a standard cylindrical surface.
  • Figure 5: The (toroidal) coil winding surface is depicted by the blue surface. Two coil boundaries corresponding to $\partial\widetilde{\Sigma}$ are depicted by the black circles. The connecting curve $\ell$ (the circular arc) is depicted in green with a tangent vector depicted in red. The corresponding normal $n$ which is tangent to $\widetilde{\Sigma}$ and normal to $\ell$ corresponds to the blue upward pointing arrow. The remaining black arrow depicts the normal $\mathcal{N}$ which corresponds to an (outward) unit normal of the coil winding surface $\Sigma$.
  • ...and 5 more figures

Theorems & Definitions (40)

  • Theorem 1.1: Generic behaviour of toroidal currents, informal version
  • Remark 1.2
  • Theorem 1.3: Generic behaviour of cylindrical currents, informal version
  • Theorem 1.4: Behaviour of physical currents, informal version
  • Theorem 1.5: Recurrent dynamics-Poincaré recurrence, GoHe49
  • Theorem 1.6: Almost all orbits are periodic, informal version
  • Remark 1.7
  • Definition 3.1: Centre regions
  • Definition 3.2: Saddle region
  • Remark 3.3
  • ...and 30 more