FEATURES OF GROUND COILS FOR YAMANASI

MAGLEV TEST LINE

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Hiroshi SUWA

Director, Guideway Engineering Group, Maglev System

Development Division

Railway Technical Research Institute

2-8-38 Hikari-cho Kokubunji-city,185 Tokyo Japan

facsimile:+81-425-73-7370

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Hitoshi TURUGA

Deputy Director General, Linear Express Development Div.

Central Japan Railway Company

1-6-6 Yaesu Chuoh-Ku,103 Tokyo Japan

facsimile:+81-3-3274-9550

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Motohiro IGARASHI

Senior Engineer, Linear Express Development Div.

Central Japan Railway Company

1-6-6 Yaesu Chuoh-Ku,103 Tokyo Japan

facsimile:+81-3-3274-9550

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Abstract:

In Superconducting Maglev, ground coil is one of the most important equipment which determine the structure and characteristics of the Maglev system. At Yamanashi Test Line we adopted a null-flux levitation and double-layered propulsion coil system.As a result of study, it was decided to adopt a more efficient null-flux levitation system for Yamanashi Test Line. In this system, levitation coils are set over the propulsion coils on the side wall. To reduce the harmful vibration of superconducting magnets caused by magnetic fieldfs change from propulsion coils, a double-layered propulsion coil system is adopted for Yamanashi Test Line. The following describes the features of this new structure.

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Key Words : Maglev, Linear Motor, Ground Coils

1.Introduction

A U-shaped guideway is used in Superconducting Maglev. At Miyazaki Test Track, levitation coils are set on the floor to produce a repulsive levitation force. But as a result of study, it was decided to adopt a more efficient null-flux levitation system for Yamanashi Test Line. In this system, levitation coils are set over the propulsion coils on the side wall. To reduce the harmful vibration of superconducting magnets caused by magnetic fieldfs change from propulsion coils, a double-layered propulsion coil system is adopted for Yamanashi Test Line. These new systems have been preliminarily tested at Miyazaki Test Track.

Parallel to these tests in Miyazaki, we developed high voltage propulsion coils,whichbecame the basis of Yamanashifs propulsion coil.

This paper presents the electro-magnetic guideway structure of Yamanashi Test Line, outline of preliminary tests in Miyazaki Test Track, profile of coils for Yamanashi and the development of coil from now on.

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2.Structure of the electro-magnetic guideway on Yamanashi Test Line

At Miyazaki test track, originally, a repulsive levitation coil and a single-layered propulsion coil system were adopted. We have been using these coils for more than 18years, and there has been almost no trouble with these coils. But, on Yamanashi Test Line, we have decided to adopt a null-flux levitation and double-layered propulsion coil system. The following describes the features of this new structure.

2.2 Double-layered propulsion coil system

At Miyazaki test track, propulsion coils are single-layered and are installed every120electrical angle on the both side walls. This type is simple, but it is evident that a large harmonic magnetic field produced by these coils induces a considerable temperature rise inside the superconducting magnets. It does not matter for short run time operation like Miyazaki test vehicle, but for long revenue service line, the operation will be difficult if the heat generated inside the superconducting magnets is larger than the capacity of on-board refrigerators which must keep the superconducting coils at a very low temperature.

So, we have decided to improve the magnetic fields produced by propulsion coils, by using bigger coils and a double-layered installation. One coil covers 180electricalangle, and coils are installed at 120 pitch along the side wall. Fig.2 is an image of the composite magnetic field produced by those double-layered coils. The harmful change of magnetic field is reduced remarkably. As the distance from the superconducting magnet is different between the front coil and the back one, it is necessary to adjust the turn number of coils between them.

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3.Preliminary tests at Miyazaki Test Track

In order to check this new electro-magnetic guideway structure, we have remodeled Miyazaki Test Track. Repulsive levitation coils of about 2.0 km have been changed to null-flux type. There has not been observed any large difference between null-flux levitation and repulsive levitation concerning the vehiclefs levitating condition. On the contrary, we can observe a clear difference of drag force between the two systems .

As for propulsion coils, about 1 km of single-layered coils has been replaced by double-layered ones. Accordingly, at this section, triple-layered coils are installed along the both side walls, which are null-flux levitation coil and double-layered propulsion coils. Wefve confirmed the effect of propulsion coilfs new structure on the superconducting magnetsf vibration reduction .

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4.Coils for Yamanashi Test Line

5.Coil installation

To reduce the coilfs level adjustment work, we have developed gbeamh system. A beam is 12.6m long, and levitation coils and propulsion coils are set on one side of it. Instead of individual coilsf adjustment, beams are adjusted to arrange guideway. Also gpanelh system is adopted in some section, the aim of which is similar to the beam.

So there are three types of side walls in Yamanashi Test Line, that are beam, panel and ordinary side wall.

6.Study for cost down

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7.Conclusions

We have introduced a new electro-magnetic guideway structure and several ways of coil fixation for Yamanashi Test Line. The installation work of ground coils has already been finished. Through the running test and the bench tests, we will compare and assess the many types of coils. And besides, we will make efforts to reduce the coil cost. The development of the ground coil has been financially supported by the Ministry of Transport of Japan. Also, a part of this development was performed by Central Japan Railway Company.

References

1) gCharacteristics Of The Combined Levitation And Guidance System Using Ground Coils On The Side Wall Of The Guidewayh, Maglev e89, July 1989,pp.241-244 S.Fujiwara, T. Fujimoto

2) gDevelopment of the Ground Coil by RIM Methodh, QR of RTRI Vol.35, No.3, pp178-184, August 1984, M. Suzuki, T. Yoshikawa

3) gNew Structure of Electro-magnetic Guideway for Maglevh, MAGLEV e93, May 1993,

pp.60-63 , S. Fujiwara, K. Sawada, N. Uchiyama, Y. Saitou, Y. Kobayashi, S. Oohama

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