John Bryan Taylor (26 December 1928 – 14 May 2026) was a British physicist known for his contributions to plasma physics and their application in the field of fusion energy. Notable among these is the development of the "Taylor state", describing a minimum-energy configuration that conserves magnetic helicity.[1][2] Another development was his work on the ballooning transformation, which describes the motion of plasma in toroidal (donut) configurations, which are used in the fusion field.[3][4] Taylor has also made contributions to the theory of the Earth's Dynamo, including the Taylor constraint.[5]
He initiated the study of chaos in magnetic surfaces, developing several contributions to chaos theory and introducing the "standard map" (or Chirikov–Taylor map).[13][14] He studied 2D-plasmas, demonstrating the inherent Bohm diffusion which had been noticed in magnetic bottles since the 1950s.[15][16] He then played a major part in developing the "ballooning transformation" for toroidal plasmas, along with Jack Connor and Jim Hastie, which won him the 2004 Hannes Alfvén Prize.[17]
References
↑Hart, G. W.; Janos, A.; Meyerhofer, D. D.; Yamada, M. (1986). "Verification of the Taylor (minimum energy) state in a spheromak". The Physics of Fluids. 29 (6): 1994–1997. Bibcode:1986PhFl...29.1994H. doi:10.1063/1.865627. ISSN0031-9171.
↑Rechester, A. B.; Rosenbluth, M. N.; White, R. B. (1981). "Fourier-space paths applied to the calculation of diffusion for the Chirikov-Taylor model". Physical Review A. 23 (5): 2664–2672. Bibcode:1981PhRvA..23.2664R. doi:10.1103/PhysRevA.23.2664.
↑Lister, Dr Jo (2004). "Award of the 2004 Hannes Alfvén Prize of the European Physical Society to J W Connor, R J Hastie and J B Taylor". Plasma Physics and Controlled Fusion. 46 (12B). doi:10.1088/0741-3335/46/12B/E02. ISSN0741-3335. S2CID250876267.