4.3 Article

Oscillation Characteristics of HTS Maglev Under Strong Magnetic Field Fluctuations

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出版社

SPRINGER
DOI: 10.1007/s10948-021-06080-w

关键词

Type II superconductors; High-T-c superconducting maglev; Levitation; Nonlinear dynamics

资金

  1. Industrial Guidance (Key) Project of Fujian Science and Technology Department [2020H0013]
  2. Sichuan Applied Basic Research [2018JY0003]
  3. Open Project of the Key Laboratory of Maglev Train and Maglev Technology, Ministry of Education of China

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The stability and dynamic behavior of the magnetic levitation system are influenced by the amplitude of magnetic field fluctuations, leading to oscillation behavior that varies linearly with the magnetic fluctuation amplitude. The dynamical behavior is governed by two driving forces of different characteristic frequencies, which may result in periodical motion towards period-doubling bifurcation and eventually evolving into a chaotic state under certain conditions.
The high T-c-superconducting maglev system relies on the diamagnetic and magnetic flux pinning characteristics of the superconductor in a magnetic field; its performance is closely related to the uniformity of the magnetic field along the magnetic track. How the amplitude of magnetic field fluctuations on the stability and dynamic behavior of magnetic levitation is still an open issue so far. In this paper, a large magnetic field fluctuation ( increment B-z) with an adjustable fluctuation amplitude was generated by covering the silicon steel sheet on the magnetic track, which was superimposed on the original small fluctuating magnetic field (delta B-z) along the permanent magnetic track. Based on this platform, we have studied the combined influence of increment B-z and increment B-z on the dynamic characteristics of the magnetic levitation system. Very significant levitation oscillation behavior was found with its amplitude linearly varying with the magnetic fluctuation amplitude. However, the dynamical behavior of the levitation was governed by the cooperation of two driving forces of different characteristic frequencies, presenting a periodical motion to a period-doubling bifurcation, and finally evolving into a chaotic state under certain conditions.

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