Eddy current brake
It has been suggested that this article be merged with track brake and talk:eddy current brake. (Discuss) Proposed since August 2007. |
An eddy current brake, like a conventional friction brake, is responsible for slowing an object, such as a train or a roller coaster. Unlike friction brakes, which apply pressure on two separate objects, eddy current brakes slow an object by creating eddy currents through electromagnetic induction which create resistance, and in turn either heat or electricity.
Construction and operation
Circular eddy current brake
Electromagnetic brakes are similar to electrical motors; non-ferromagnetic metal discs (rotors) are connected to a rotating coil, and a magnetic field between the rotor and the coil creates a resistance used to generate electricity or heat. When electromagnets are used, control of the braking action is made possible by varying the strength of the magnetic field. A braking force is possible when electric current is passed through the electromagnets. The movement of the metal through the magnetic field of the electromagnets creates eddy currents in the discs. These eddy currents generate an opposing magnetic field, which then resists the rotation of the discs, providing braking force. The net result is to convert the motion of the rotors into heat in the rotors.
Linear eddy current brake
The principle of the linear eddy current brake has been described by the French physicist Foucault, that's why in French the eddy current brake is called the "frein à courants de Foucault".
The linear eddy current brake consists of a magnetic yoke with electrical coils positioned along the rail, which are being magnetized alternating as south and north magnetic poles. This magnet does not touch the rail, as with the magnetic brake, but is held at a definite small distance from the rail (approximately 7 millimeters). It does not move along the rail, it exerts only a vertical pull on the rail. Let us call that magnetic force F.
When the magnet is moved along the rail, it generates in non-stationary magnetic field in the head of the rail, which then generates electrical tension (Faraday's induction law), and that causes eddy currents. These disturb the magnetic field in such a way that the magnetic force F, mentioned above, is diverted to the opposite of the direction of the movement, thus creating a parallelogram of forces consisting of the remaining vertical force FV and the horizontal force FH, which works against the movement of the magnet.
The braking energy of the vehicle is converted in eddy current losses which lead to a warming of the rail.
The regular magnetic brake which is in wide use in railways, exerts its braking force by friction with the rail, which also creates heat.
The eddy current brake does not have any mechanical contact with the rail, and thus no wear and tear of it, and creates no noise or odor. The eddy current brake is, as should be clear from the above explanation, unusable at low speeds, but can be used at high speeds both for emergency braking as well as regular and regulated braking.[1]
The TSI (Technical Specifications for Interoperability) of the EU for trans-European high speed rail recommends that all newly built high speed lines should make the eddy current brake possible.
The first train in commercial circulation to use such a braking is the ICE 3.
Modern roller coasters use this type of braking, but utilize permanent magnets instead of electromagnets. These brakes require no electricity. However, their braking strength cannot be adjusted.
See also
- Regenerative braking generates electricity rather than heat and hence is usually more energy efficient
- Electromagnetic brakes work differently, by using the magnetic force to press the brake on the rail.
- [1] Article on ICE's experience of eddy braking.
References
- Sears, Francis Weston (1955). University Physics (2nd ed.). Reading, MA: Addison-Wesley.
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- ^ "Wirbelstrombremse im ICE 3 als Betriebsbremssystem hoher Leistung" ("Eddy-current brake in the ICE 3 as high-efficiency service brake system", by Jürgen Prem, Stefan Haas, Klaus Heckmann, in "electrische bahnen" Vol 102 (2004), No. 7, pages 283ff