Actuators for Active Magnetic Bearings

The literature of active magnetic bearing (AMB) technology dates back to at least 1937 when the earliest work that clearly describes an active magnetic bearing system was published by Jesse Beams [1]. Progress on the technology was modest until the late 1970s, when commercial development began to emerge as, for instance, described by Haberman and Liard in 1977 [2]. The state of the art in 1988 is well-represented by the many technical papers compiled in the Proceedings of the First International Symposium on Magnetic Bearings [3]. In 1988, active magnetic bearings were still largely a novelty, and the literature of that time reflects this. Applications were relatively few, and producers of rotating machinery generally regarded the technology as a scientific curiosity. Most papers considered variations on the same theme: eight pole or “E”-core radial stators and single slot thrust stators with some form of transconductance control of the currents. Touch-down bearings were viewed as a necessity but were also feared as a likely source of failure: contacting a TDB seemed likely to mean a failure only narrowly short of catastrophic. Control was nearly always decentralized Proportional-Integral-Derivative (PID) and high-fidelity modeling of the combination of AMBs with a realistic, flexible rotor was at best in its infancy. It is immensely gratifying to see this technology blossom from this beginning into a successful and mature technology with wide industrial acceptance and use. This special issue includes eleven contributions covering a wide range of topics related to the actuators of AMB systems as well as their control. Reflecting the maturity of the technology, these papers are generally concerned with practical refinements rather than the fundamentals of the technology. The conventional concept of a radial magnetic bearing actuator is a sequence of coil-driven electromagnets arranged with alternating polarity around a rotor. Significant energy savings may be realized along with some simplification of the coil drive if the magnet array incorporates permanent magnets to provide biasing flux and arranges the poles in multiple planes so that the field does not alternate in the circumferential direction but, instead, in the axial direction. Such an arrangement is referred to as a homopolar structure. Filatov et al. [4] have provided an interesting and comprehensive view of the experience and design considerations that have led to the modern industrial implementation of homopolar magnetic bearings. Further departures from the conventional four-quadrant magnet scheme are explored in [5,6]. Meeker [5] considers control of general n-pole radial magnetic structures without biasing. Unbiased control is of interest because of potential reductions in power consumption. Further, as discussed in [5], there are some radial magnet configurations which fundamentally cannot be bias linearized but can still be acceptably controlled with a generalized quadratic method. David et al. [6] consider the special case of controlling the currents in a four-pole radial magnetic stator, of particular interest in small AMB applications. Continuing in the vein of using permanent magnets to reduce power consumption, Ishibashi et al. [7] explore the use of a mechanically actuated flux return path in an actuator energized only by a permanent magnet. Such an arrangement achieves magnetic suspension and control without the high coil currents required in a conventional electromagnet-based scheme. The authors propose