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Electromagnet - Force on ferromagnetic materials |  | Electromagnet - Force on ferromagnetic materials: Encyclopedia II - Electromagnet - Force on ferromagnetic materials |  | Computing the force on ferromagnetic materials is, in general, quite complex. This is due to fringing field lines and complex geometries. It can be simulated using finite element analysis. However, it is possible to estimate the maximum force under specific conditions. If the magnetic field is confined within a high permeability material, such as certain steel alloys, the maximum force is given by:
Where:
F is the force in newtons
B is the magnetic field in teslas
A is the area of the pole faces in square ...
See also:Electromagnet, Electromagnet - Introduction, Electromagnet - Electromagnets and permanent magnets, Electromagnet - Devices that use electromagnets, Electromagnet - Force on ferromagnetic materials |  | | Electromagnet, Electromagnet - Devices that use electromagnets, Electromagnet - Electromagnets and permanent magnets, Electromagnet - Force on ferromagnetic materials, Electromagnet - Introduction, Dipole magnet Electro magnet used in Particle accelerators, Electromagnetism, Quadrupole magnet Electro magnet used in Particle accelerators |  | |
|  |  | Electromagnet: Encyclopedia II - Electromagnet - Force on ferromagnetic materials
Electromagnet - Force on ferromagnetic materials
Computing the force on ferromagnetic materials is, in general, quite complex. This is due to fringing field lines and complex geometries. It can be simulated using finite element analysis. However, it is possible to estimate the maximum force under specific conditions. If the magnetic field is confined within a high permeability material, such as certain steel alloys, the maximum force is given by:
Where:
- F is the force in newtons
- B is the magnetic field in teslas
- A is the area of the pole faces in square meters
- μ is the permeability of free space
See energy in a magnetic field for more details on the derivation.
In the case of free space (air), , the force per unit area (pressure) is:
or @ B = 1 tesla
or @ B = 2 teslas
In a closed magnetic circuit:
Where:
- N is the number of turns of wire around the electromagnet
- I is the current in amperes
- L is the length of the magnetic circuit
Substituting above,
In order to build a strong electromagnet, a short magnetic circuit, with large area is preferred. Note that most ferromagnetic materials saturate around 1 to 2 teslas. This occurs at a field intensity of:
or
For this reason, there is no point in building an electromagnet with a higher field intensity. Industrial lifting electromagnets, like the one pictured above, are designed with both pole faces at one side (the bottom). This confines the field lines to maximize the magnetic field. It's like a cylinder within a cylinder. Many speaker magnets use a similar geometry, although the field lines are radial from the inner cylinder rather than perpendicular to the face. Notice the large surface area compared with the height. With pole faces of one square foot or more, thousands of pounds can be lifted with drive currents of just a few amperes or less.
Other related archivesDipole magnet, Doorbells, Electromagnetism, Image:Quadrupole magnet.gif, Magnetic levitation trains, Magnets, Quadrupole magnet, actuators, bell, cathode ray tube, charged particle beams, coiled, core, corkscrew, current, electric motor, electrical power, energy in a magnetic field, ferromagnetic, finite element analysis, forces, hysteresis, iron, linear motor, locks, magnet, magnetic circuit, magnetic field, mass spectrometer, paramagnetic, permanent magnet, relays, right-hand rule, solenoid, solenoid valves, toroid, wire
 Adapted from the Wikipedia article "Force on ferromagnetic materials", under the G.N U Free Docmentation License. Please also see http://en.wikipedia.org/wiki |
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