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Glossary

Magnetic Field

The invisible force that confines charged plasma particles along helical trajectories — the fundamental mechanism that makes magnetic confinement fusion possible.

Reviewed Last reviewed: 9 Aug 2026 · Category: Glossary

Role in Fusion

A fusion plasma at 100+ million degrees would instantly destroy any physical container. Magnetic confinement exploits the fact that charged particles — the ions and electrons that make up a plasma — spiral tightly around magnetic field lines due to the Lorentz force. By shaping these field lines into closed, nested surfaces inside a toroidal vessel, the plasma can be held away from material walls long enough for fusion reactions to occur.[1]

Toroidal and Poloidal Fields

In a tokamak, confinement requires two principal field components. The toroidal field (BT) runs the long way around the torus and is generated by external D-shaped or circular coils. The poloidal field (BP) runs the short way around the plasma cross-section and is produced primarily by the plasma current itself, with additional contributions from external shaping coils. The superposition of these two fields creates helical field lines that map out nested toroidal flux surfaces — the "magnetic bottles" that confine the plasma.[2]

Field Strength and Magnet Technology

Confinement quality improves with field strength: higher fields allow higher plasma pressure at a given plasma beta (the ratio of plasma pressure to magnetic pressure). Early tokamaks used copper electromagnets that consumed enormous electrical power. Modern devices increasingly employ superconducting magnets — low-temperature superconductors (LTS) such as Nb3Sn in ITER, or high-temperature superconductors (HTS) such as REBCO tape in next-generation compact tokamaks — that can sustain fields of 12–20+ tesla with far lower power consumption.[3]

The magnetic field inside ITER's toroidal field coils will reach 11.8 tesla — roughly 200,000 times stronger than Earth's magnetic field at the surface.

Magnetic Topology and Stability

The detailed shape and twist of the magnetic field determine plasma stability. Key parameters include the safety factor q (describing how tightly field lines wind), magnetic shear (the rate at which q changes across the plasma radius), and triangularity (the D-shaped distortion of flux surfaces). Careful optimization of these properties suppresses magnetohydrodynamic (MHD) instabilities such as kink modes, tearing modes, and edge-localized modes (ELMs) that would otherwise cause the plasma to lose confinement.[1]

Beyond Tokamaks

Magnetic fields are equally central to other confinement concepts. Stellarators use twisted external coils to generate the full rotational transform without relying on plasma current. Magnetic mirrors use open-ended field geometries with strong-field "plugs" at each end. In each case, the architecture of the magnetic field is the primary engineering and physics design variable.

Sources

  1. Freidberg, J.P., Plasma Physics and Fusion Energy, Cambridge University Press, 2007.
  2. Wesson, J., Tokamaks, 4th ed., Oxford University Press, 2011, Chapter 3.
  3. Whyte, D. et al., "Smaller and sooner: exploiting high magnetic fields from new superconducting technologies," Journal of Fusion Energy, vol. 35, pp. 41–53, 2016.

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