Motion of charged particles in a stepped magnetic field

Abstract We analyse the motion of a charged particle in a stepped magnetic field, in which two uniform regions are separated by a sharp interface. The trajectory consists of circular arcs of different radii joined at the boundary, and the mismatch of Larmor radii produces a drift along the interface. Four cases are distinguished: snake orbits for antiparallel fields and skipping orbits for parallel fields, each with two possible arc configurations. Using only elementary circular-motion geometry, we derive the drift velocity as a function of the crossing angle and the field ratio. For antiparallel fields, the drift velocity is independent of the field magnitudes; for parallel fields, it depends on their ratio and in one case has an intermediate maximum. The results can be written in a unified form. The model offers an intuitive introduction to gradient drift for advanced undergraduate students without requiring vector calculus.

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Publication Details

Journal
Physics Education
Published
2026-11-03
DOI
https://doi.org/10.1088/1361-6552/aeb849
Primary Topic
Quantum and Classical Electrodynamics
Type
article
Field-Weighted Citation Impact
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article

Motion of charged particles in a stepped magnetic field

Vladimir Valerievich Ivchenko
Physics Education
Quantum and Classical Electrodynamics
article

Motion of charged particles in a stepped magnetic field

Vladimir Valerievich Ivchenko
article en

Abstract

Abstract We analyse the motion of a charged particle in a stepped magnetic field, in which two uniform regions are separated by a sharp interface. The trajectory consists of circular arcs of different radii joined at the boundary, and the mismatch of Larmor radii produces a drift along the interface. Four cases are distinguished: snake orbits for antiparallel fields and skipping orbits for parallel fields, each with two possible arc configurations. Using only elementary circular-motion geometry, we derive the drift velocity as a function of the crossing angle and the field ratio. For antiparallel fields, the drift velocity is independent of the field magnitudes; for parallel fields, it depends on their ratio and in one case has an intermediate maximum. The results can be written in a unified form. The model offers an intuitive introduction to gradient drift for advanced undergraduate students without requiring vector calculus.

Physics EducationVol. 61(6)
Kherson National Technical University (UA)
Openalex Percentile: Top 22%
Quantum and Classical Electrodynamics
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