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.
Basic Principles
Section titled “Basic Principles”Differences from Tokamak
Section titled “Differences from Tokamak”While a tokamak generates the poloidal field through plasma current, a stellarator forms the complete magnetic configuration using only external coils.
| Feature | Tokamak | Stellarator |
|---|---|---|
| Poloidal field | Plasma current | External coils |
| Plasma current | Required | Not required |
| Operation mode | Pulsed (in principle) | Steady-state possible |
| Disruption | Possible | Does not occur |
| Coil geometry | Relatively simple | Complex |
Rotational Transform
Section titled “Rotational Transform”In stellarators, the geometric arrangement of coils generates a rotational transform . The rotational transform represents the angle advanced in the poloidal direction while a field line goes once around toroidally:
where is the safety factor.
Types of Magnetic Configurations
Section titled “Types of Magnetic Configurations”Classical Stellarator
Section titled “Classical Stellarator”The earliest design with a figure-8 twisted torus shape. No longer in use today.
Heliotron/Helical
Section titled “Heliotron/Helical”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.
Modular Stellarator
Section titled “Modular Stellarator”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.
Confinement by External Coils
Section titled “Confinement by External Coils”Coil Design Optimization
Section titled “Coil Design Optimization”Stellarator coils have complex three-dimensional shapes. Design requires optimization of:
- Maximizing particle confinement
- Ensuring MHD stability
- Minimizing heat and particle transport
- Manufacturability
Quasi-symmetry
Section titled “Quasi-symmetry”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.
Advantages of Steady-State Operation
Section titled “Advantages of Steady-State Operation”The greatest advantage of stellarators is the inherent capability for steady-state operation.
Constraints of Tokamaks
Section titled “Constraints of Tokamaks”In tokamaks, maintaining plasma current requires either:
- Changing magnetic flux of the central solenoid (finite time)
- External current drive (low efficiency)
This is a barrier to steady-state operation.
Superiority of Stellarators
Section titled “Superiority of Stellarators”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.
Why No Disruptions
Section titled “Why No Disruptions”Tokamak disruptions occur due to rapid collapse of plasma current. In stellarators, since plasma current is not essential for confinement:
- Current quench does not occur
- Large electromagnetic forces are not generated
- No runaway electron problem
This represents a major advantage in terms of safety and device lifetime.
Representative Devices
Section titled “Representative Devices”Wendelstein 7-X (W7-X)
Section titled “Wendelstein 7-X (W7-X)”The world’s largest stellarator, operated by the Max Planck Institute for Plasma Physics (IPP) in Germany.
| Parameter | Value |
|---|---|
| Major radius | 5.5 m |
| Minor radius | 0.53 m |
| Magnetic field | 3 T |
| Heating power | 10 MW |
| Number of coils | 50 (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
Large Helical Device (LHD)
Section titled “Large Helical Device (LHD)”The world’s largest helical device, operated by the National Institute for Fusion Science (NIFS) in Japan.
| Parameter | Value |
|---|---|
| Major radius | 3.9 m |
| Minor radius | 0.65 m |
| Magnetic field | 3 T (max 4 T) |
| Heating power | 23 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.
HSX (Helically Symmetric Experiment)
Section titled “HSX (Helically Symmetric Experiment)”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.
Challenges and Current Status
Section titled “Challenges and Current Status”Manufacturing Complexity
Section titled “Manufacturing Complexity”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.
Confinement Performance
Section titled “Confinement Performance”Historically, stellarator confinement performance has been inferior to tokamaks. However, this gap is narrowing with optimized designs.
Scaling
Section titled “Scaling”The stellarator energy confinement time scaling is represented by the ISS04 scaling:
where is the minor radius, is the major radius, is the heating power, is the line-averaged electron density, is the magnetic field strength, and is the rotational transform.
Future Outlook
Section titled “Future Outlook”Potential as Power Reactor
Section titled “Potential as Power Reactor”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.
HELIAS
Section titled “HELIAS”In Europe, a power reactor conceptual design HELIAS (Helical Advanced Stellarator) is being considered based on W7-X results.
Compact Stellarators
Section titled “Compact Stellarators”With high-temperature superconductors and advanced manufacturing technologies, more compact stellarators are expected to become feasible.
Related Topics
Section titled “Related Topics”- Confinement Methods: Overview - Overview of confinement methods
- Tokamak Confinement - Alternative method using plasma current
- Glossary: Stellarator - Basic definition
- Glossary: Confinement - Concept of confinement