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  2. Magnetic mirror - Wikipedia

    en.wikipedia.org/wiki/Magnetic_mirror

    A magnetic mirror, also known as a magnetic trap or sometimes as a pyrotron, is a type of magnetic confinement fusion device used in fusion power to trap high temperature plasma using magnetic fields. The mirror was one of the earliest major approaches to fusion power, along with the stellarator and z-pinch machines. In a classic magnetic ...

  3. Bumpy torus - Wikipedia

    en.wikipedia.org/wiki/Bumpy_torus

    The magnetic mirror is among the simplest magnetic fusion energy machines in terms of physical complexity. It consists largely of a cylinder with powerful magnets at each end, although in practice the cylindrical part (technically, a solenoid) is lined with less powerful magnets to better shape the field. The resulting magnetic field has a ...

  4. Guiding center - Wikipedia

    en.wikipedia.org/wiki/Guiding_center

    If the field has a parallel gradient, a particle with a finite Larmor radius will also experience a force in the direction away from the larger magnetic field. This effect is known as the magnetic mirror. While it is closely related to guiding center drifts in its physics and mathematics, it is nevertheless considered to be distinct from them.

  5. Pitch angle (particle motion) - Wikipedia

    en.wikipedia.org/wiki/Pitch_angle_(particle_motion)

    The pitch angle of a charged particle is the angle between the particle's velocity vector and the local magnetic field. This is a common measurement and topic when studying the magnetosphere, magnetic mirrors, biconic cusps and polywells. See Aurora and Ring current

  6. Category:Magnetic mirrors - Wikipedia

    en.wikipedia.org/wiki/Category:Magnetic_mirrors

    Download as PDF; Printable version; In other projects ... Pages in category "Magnetic mirrors" ... Magnetic mirror; M. Mirror Fusion Test Facility; T. Tandem Mirror ...

  7. Gas Dynamic Trap - Wikipedia

    en.wikipedia.org/wiki/Gas_Dynamic_Trap

    The magnetic field varies along this tube. In the center the field is low; reaching (at most) 0.35 Teslas. The field rises to as high as 15 Teslas at the ends. [1] This change in the strength is needed to reflect the particles and get them internally trapped (see: the magnetic mirror effect).