[0001] This invention relates to permanent magnet alloys.
[0002] Permanent magnet alloys used in the production of permanent magnets for use in electric
motors, and particularly electric motors used in household appliances and the like,
are required to have good resistance to demagnetization at elevated temperatures for
efficient motor operation. The temperatures involved in these motor applications are
typically within the range of 125 to 150°C. To achieve high resistance to demagnetization
good remanence (B
r) and coercive force (H
ci) values are required within this temperature range. It is further desired in applications
such as permanent magnets used in electric motors for household appliance applications
that the alloy of the magnet be relatively low cost.
[0003] It is known that permanent magnet alloys of neodymium, iron, boron have remanence
values sufficiently high for the purpose and these are relatively inexpensive alloys;
however, at the typical service temperatures of 125 to 150°C magnets of these alloys
are characterized by a loss of coercive force to below the level suitable for the
purpose. Coercive force is known to be increased by increasing the crystal anisotropy
or the anisotropy field (
HA).
[0004] It is accordingly a primary object of the present invention to provide a low-cost
permanent magnet alloy that may be used in the manufacture of magnets having high
resistance to demagnetization at elevated temperatures within the range of 125 to
150°C.
[0005] A more specific object of the invention is to provide a permanent magnet alloy of
low cost having a good combination of both remanence and coercive force within the
temperature range of 125 to 150°C which increase in coercive force is achieved by
an improved crystal anisotropy without decreasing remanence to below acceptable levels.
[0006] The permanent magnet alloy of the invention consists of, in weight percent, 1 to
10 dysprosium, 20 to 37 neodymium, with the total dysprosium and neodymium content
being within the range of 30 to 38, 0.8 to 1.33 boron and balance iron and impurities
usual in metal alloys. Preferably the dysprosium content is from 2.5 to 6.5% and more
preferred from 3 to 6%.
[0007] The invention will be more particularly described with reference to the accompanying
drawing taken in conjunction with the following description and specific examples.
[0008] The single FIGURE of the drawing is a graph illustrating the effect of the dysprosium
content of a magnet alloy on the coercive force.
[0009] It is known generally that coercive force (H
ci)is increased by increases in the crystal anisotropy (H
A). It has been discovered, in accordance with the present invention, that generally
with magnet alloys of iron and boron with a neodymium content of approximately 33%
the H
A in kilo oersteds is 150; with similar alloys having dysprosium as the rare earth
element the H
A values in kilo oersteds are approximately 314. It may be seen, therefore, that by
the use of dysprosium in rare earth, iron, boron alloys the crystal anisotropy is
improved to in turn increase the coercive force. In addition, however, it has been
determined that the use of dysprosium in alloys of this type decreases remanence (B
r).
[0010] The following specific examples of the invention show with neodymium, iron, boron
magnets the temperature effect on loss of coercive force. Also, the examples demonstrate
that coercive force in magnet alloys of this type are increased by the addition of
dysprosium as a rare earth element. They also show that increased dysprosium above
the limits of the invention decreases remanence values to below acceptable levels.
Consequently, it is critical with regard to achieving a combination of good remanence
and coercive force within the required temperature range of 125 to 150°C to have the
rare earth element content of the alloy comprise a combination of dysprosium and neodymium.
[0011] An alloy of Nd (33%) B (1%) FE (66%) in weight percent was melted, crushed to about
1 to 10 micron particle size. The fine powder was oriented in a magnetic field and
pressed. The pressed part was sintered over a temperature range of 1000°C - 1100°C
and cooled. The sintered magnet had the intrinsic coercive force at the indicated
temperatures in Table I.

The remanence of the magnet varied from 12,100 Gauss to 10,738 Gauss from 20° to 145°C.
The loss of intrinsic coercive force to below 6,000 Oersted at 94°C makes this magnet
not applicable for motors.
[0013] As can be seen from Tables II and III and FIG.1 adding dysprosium increases the coercive
force rapidly at room temperature. The temperature dependence of the coercive force
of a 3% Dy containing alloy and 6% Dy containing alloy is given in Table IV.

[0014] As can be seen from Table IV, dysprosium addition in combination with neodymium permits
utilization of these magnets at elevated temperatures. Increasing the dysprosium further
results in a decrease in B
r which makes the magnets not have enough flux at the required temperature for the
intended applications. Table V shows the magnetic properties of a 10% Dy containing
magnet.

1. A permanent magnet alloy characterised in consisting of, in weight percent, 1 to
10 dysprosium, 20 to 37 neodymium, with the total dysprosium and neodymium content
being within the range of 30 to 38, 0.8 to 1.33 boron and balance iron and impurities
usual in metal alloys.
2. An alloy according to claim 1, wherein dysprosium is present in an amount of from
2.5 to 6.5%.
3. An alloy according to claim 1 or 2, wherein dysprosium is present in an amount
of from 3 to 6%.