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Stellarator/Helical Confinement

The stellarator is a magnetic confinement fusion device that confines plasma using only external magnetic coils. It was invented by Lyman Spitzer at Princeton University in 1951. The name combines “stellar” (relating to stars) and “generator.”

In Japan, a variant called the “helical device” has developed independently, with the Large Helical Device (LHD) leading the world.

While a tokamak generates the poloidal field through plasma current, a stellarator forms the complete magnetic configuration using only external coils.

FeatureTokamakStellarator
Poloidal fieldPlasma currentExternal coils
Plasma currentRequiredNot required
Operation modePulsed (in principle)Steady-state possible
DisruptionPossibleDoes not occur
Coil geometryRelatively simpleComplex

In stellarators, the geometric arrangement of coils generates a rotational transform ι\iota. The rotational transform represents the angle advanced in the poloidal direction while a field line goes once around toroidally:

ι=2πtoroidal turns/poloidal turn=1q\iota = \frac{2\pi}{\text{toroidal turns/poloidal turn}} = \frac{1}{q}

where qq is the safety factor.

The earliest design with a figure-8 twisted torus shape. No longer in use today.

A method using continuous helical coils. Japan’s Large Helical Device (LHD) uses this approach.

LHD employs helical coils with l = 2 and m = 10, where l is the poloidal period number and m is the toroidal period number.

A method using complex three-dimensional modular coils. Wendelstein 7-X is the prime example of this approach. It achieves a magnetic configuration designed through computer optimization.

Stellarator coils have complex three-dimensional shapes. Design requires optimization of:

  1. Maximizing particle confinement
  2. Ensuring MHD stability
  3. Minimizing heat and particle transport
  4. Manufacturability

In modern stellarator design, the concept of “quasi-symmetry” is important. While perfect axisymmetry is impossible, effective symmetry for particle orbits minimizes neoclassical transport.

Types of quasi-symmetry include:

  • Quasi-axisymmetry (QA)
  • Quasi-helical symmetry (QH)
  • Quasi-isodynamic (QI)

Wendelstein 7-X employs QI configuration, while HSX uses QH configuration.

The greatest advantage of stellarators is the inherent capability for steady-state operation.

In tokamaks, maintaining plasma current requires either:

  1. Changing magnetic flux of the central solenoid (finite time)
  2. External current drive (low efficiency)

This is a barrier to steady-state operation.

In stellarators:

  • No flux consumption since plasma current is not required
  • Bootstrap current does not affect confinement
  • Operation can continue with auxiliary heating alone

For power reactors, continuous operation offers significant advantages in terms of facility availability and economics.

Tokamak disruptions occur due to rapid collapse of plasma current. In stellarators, since plasma current is not essential for confinement:

  1. Current quench does not occur
  2. Large electromagnetic forces are not generated
  3. No runaway electron problem

This represents a major advantage in terms of safety and device lifetime.

The world’s largest stellarator, operated by the Max Planck Institute for Plasma Physics (IPP) in Germany.

ParameterValue
Major radius5.5 m
Minor radius0.53 m
Magnetic field3 T
Heating power10 MW
Number of coils50 (non-planar superconducting)

W7-X is a device to demonstrate the concept of optimized stellarators, and began operation in 2015. In 2022, it set a record for energy confinement time.

Major achievements:

  • High energy confinement (exceeding ISS04 scaling)
  • Multi-minute long-pulse discharges
  • Demonstration of as-designed magnetic configuration

The world’s largest helical device, operated by the National Institute for Fusion Science (NIFS) in Japan.

ParameterValue
Major radius3.9 m
Minor radius0.65 m
Magnetic field3 T (max 4 T)
Heating power23 MW

LHD features:

  • l = 2 helical configuration
  • High-density plasma confinement research
  • Long-pulse discharge (over 1 hour steady-state operation achieved)
  • Fusion reaction research with deuterium experiments

LHD started deuterium experiments in 2017 and has obtained important data in both plasma physics and fusion engineering.

A quasi-helical symmetric stellarator at the University of Wisconsin, USA. Though a small device, it plays an important role in experimentally verifying quasi-symmetry physics.

The three-dimensionally complex coil geometry presents challenges in both manufacturing cost and precision. For W7-X, the tolerance for coil position was set to sub-millimeter levels.

Historically, stellarator confinement performance has been inferior to tokamaks. However, this gap is narrowing with optimized designs.

The stellarator energy confinement time scaling is represented by the ISS04 scaling:

τEISS04=0.134a2.28R0.64P0.61nˉe0.54B0.84ι0.41\tau_E^{\text{ISS04}} = 0.134 \cdot a^{2.28} \cdot R^{0.64} \cdot P^{-0.61} \cdot \bar{n}_e^{0.54} \cdot B^{0.84} \cdot \iota^{0.41}

where aa is the minor radius, RR is the major radius, PP is the heating power, nˉe\bar{n}_e is the line-averaged electron density, BB is the magnetic field strength, and ι\iota is the rotational transform.

Stellarators are attractive as power reactors due to steady-state operation and absence of disruptions. However, further improvement in confinement performance and reduction in manufacturing costs are needed.

In Europe, a power reactor conceptual design HELIAS (Helical Advanced Stellarator) is being considered based on W7-X results.

With high-temperature superconductors and advanced manufacturing technologies, more compact stellarators are expected to become feasible.