![]() The material has no preferred direction of orientation and can therefore be magnetized in any direction ![]() A preferred magnetic axis has been induced during manufacture in order to obtain higher magnetic properties in that direction. Anisotropic magnets can only be magnetized in that direction ![]() The hysteresis loop in the second quadrant and used to define the main properties of permanent magnet materials. ![]() This is the flux density in the magnetic material at zero air gap (Field strength=0), which remains after magnetization to saturation and then removing the magnetizing field. Units: mT, T or G, kG. ![]() The demagnetizing field strength in order to bring the polarizing J to zero from saturation. Units: kA/m or Oe, kOe. ![]() The demagnetizing field strength in order to bring the polarization J to zero from saturation. Units: kA/m or Oe, kOe. ![]() The maximum product of B and H on the demagnetization curve. This is the highest energy produced by the magnet, the optimal working point. Units: kJ/m3 or MGOe. ![]() The point on the demagnetization curve where the value of B and H correspond to the actual working conditions. ![]() This indicates the reversible change in Br or Hc because of changes in temperature. This is normally shown as a percentage per degree C, starting at 20 degree C. ![]() This maximum temperature is very dependent of the working point of the magnet. ![]() Above this temperature the magnets will loose their magnetism permanently. |