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United States Patent 6025667 |
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Permanent magnet rotor type electric motor with different permanent magnet materials
US Patent Issued on February 15, 2000
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Inventor(s)
Assignee
Application
No. 159668 filed on 1998-09-24
Current US Class
310/156.53 Embedded in a core
Examiners
Attorney, Agent or Firm
Foreign Patent References
| 63-9102 JP Jan., 1988 |
| 4-225439 JP Sep., 1992 |
| 8-275419 JP Oct., 1996 |
| 9-205746 JP Aug., 1997 |
| 10-191585 JP Jul., 1998 |
| 11-113198 JP Apr., 1999 |
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Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates to an electric motor having a permanent magnet in a
rotor, such as Brushless DC motor or the like and, more specifically, to
an electric motor in which a magnetic flux density, a reluctance torque
and so on can be selectively established, appropriate as a driving source
of a compressor of an air conditioner, for example.
2. Description of the Related Art
In the electric motor of the type as described above, a permanent magnet is
embedded in a core of an inner rotor of the electric motor, an example
thereof being shown respectively in FIG. 8 and FIG. 9 each of which is a
plane view showing the inside of this electric motor from a plan
perpendicular to the axis of rotation.
In the example shown in FIG. 8 a rotor core 2 is disposed inside a stator
core 1, having 24 slots for example, in which a field magnet rotates. In
this case, the number of poles of the electric motor is four, therefore
four permanent magnets 3 are arranged in the rotor core 2.
Each permanent magnet 3 is formed to be a band plate shape with rectangular
cross-section, and each pair of the permanent magnets 3 is disposed to
face each other along a direction perpendicular to a diameter line of the
rotor core 2 in the vicinity of the outer circumference of the rotor core
2. Each permanent magnet 3 is embedded inside the rotor core 2 along a
direction perpendicular to paper of FIG. 8.
Between the adjacent permanent magnets 3, holes 4 as flux barrier for
preventing short-circuit and leak of magnetic flux between the adjacent
permanent magnets are formed. In this example, the holes 4 are represented
as triangle holes and disposed at both ends of the permanent magnet 3. In
the center of the rotor core 2, a center hole 5 is formed to allow a
rotating shaft (not shown) to pass therethrough.
In this structure, when the magnetic flux distribution in a gap portion
(between teeth of the stator core 1 and the permanent magnet 3) caused by
the permanent magnet 3 is in a sine wave state, torque T of the electric
motor is expressed by, T=Pn{.PHI.a.multidot.Ia.multidot.cos
β-0.5(Ld-Lq).multidot.I2 sin 2β}, where T is an output torque,
.PHI.a is an armature flux linkage caused by the permanent magnet 3 on the
coordinate axes d and q, Ld and Lq are the inductance on the axis d and
the inductance on the axis q respectively, Ia is amplitude of an armature
current on the coordinate axes d and q, β is a lead angle of the
armature current from the axis q on the coordinate axes d and q, and Pn is
a pole logarithm.
In the above expression, the first term expresses a magnet torque 15
generated by the permanent magnet 3, and the second term expresses a
reluctance torque generated by a difference between the inductance on the
axis d and the inductance on the axis q. Refer to a treatise published in
T. IEE Japan, Vol. 117-D, No. 8. 1997 for further detail.
In the rotor core 2 shown in FIG. 9 as another conventional example, a
permanent magnet 6 having arch-shaped cross-section is used, and the
torque T thereof is also found by the aforementioned operational
expression.
Typically, ferrite magnet and rare-earth magnet are used for the permanent
magnets 3 and 6 employed in the aforementioned type of the electric motor.
The ferrite magnet is less expensive and available for forming the
permanent magnet in various shapes due to easiness of forming thereof, but
the magnetic flux density is low, therefore hindering the reduction in
size of the rotor core.
On the other hand, the rare-earth magnet has a high magnetic flux density,
so that the reduction in size of the rotor core is easy, but the shape of
the permanent magnet is limited by difficulty of forming thereof. In
addition, the rare-earth magnet is more expensive than the ferrite magnet.
Since both the ferrite magnet and the rare earth magnet have merits and
demerits as explained above, conventionally for reasons of the use and/or
a cost of a motor, either the ferrite magnet or the rare-earth magnet is
chosen for all permanent magnets of magnetic poles. In this case, there
are disadvantages described below.
For example, in the case that the magnetic pole is formed of only the
ferrite magnet, the amount of the magnet should be increased to increase
the magnetic flux density. Therefore the polarized area becomes large, and
consequently, the magnet occupies the most of the rotor core. Accordingly,
the inductance on the axis q is small, so that the difference of the
inductance on the axis q and the inductance on the axis d (parameter of a
reluctance torque: refer to the aforementioned operational expression)
becomes small, with the result that a sufficient reluctance torque cannot
be attained.
In the case that the magnetic pole is formed of only the rare-earth magnet,
the magnetic flux density is high, so that the magnet does not occupy the
most of the rotor core as the ferrite magnet, but the magnetic flux
density is often excessively high, and additionally the rare-earth magnet
is expensive, therefore the motor is increased in cost.
As described hereinbefore, conventionally, a proper permanent magnet having
an intermediate state between the ferrite magnet and the rare-earth magnet
is troublesome to obtain, that is to say it is difficult to select the
required magnetic flux density and reluctance torque, with low cost.
SUMMARY OF THE INVENTION
The present invention has been made for resolving the aforementioned
disadvantages. It is an object of the present invention to provide a
permanent magnet rotor type electric motor capable of selectively
determining a magnet flux density and a reluctance torque and having a
reasonable cost.
According to the present invention, the object can be attained in a
permanent magnet rotor type electric motor in which a rotor core having
magnetic poles formed of the permanent magnets therein is disposed inside
a stator core generating a rotation magnetic field, wherein the magnetic
poles in a rotor core are formed of three or more permanent magnets, and
at least two kinds of magnetic materials are used for the permanent
magnets.
The two kinds of magnetic materials may be ferrite magnet and rare-earth
magnet, and by using the above magnetic materials together, the required
magnetic flux density is easily attained. In addition, in this case, the
occupying rate of the magnets in the core can be lowered and the
inductance on the axis q is larger than those in the case in which each
magnetic pole is formed of only the ferrite magnet having a low magnetic
flux density for example. Accordingly, a difference between the inductance
on the axis q and the inductance on the axis d can be large. As is
described above, according to the present invention, a selecting range for
a reluctance torque and a magnetic flux density can be enlarged, and a
reasonable cost corresponding to the quality can be attained.
To attain the above object, in the present invention a permanent magnet
rotor type electric motor has a rotor core having magnetic poles formed of
the permanent magnets therein, which is disposed inside a stator core
generating a rotation magnetic field. The rotor core has a first permanent
magnet disposed on a boundary line along a diametrical line of the rotor
core between the adjacent magnetic poles and a second permanent magnet
disposed in the vicinity of the outer circumference of the rotor core in
each magnetic pole, in which each magnetic pole is practically formed of
three permanent magnets such that the first permanent magnet as a magnet
is shared between the adjacent magnetic poles, and the first permanent
magnet and the second permanent magnet are made of different magnetic
materials.
In this case, the first permanent magnet is formed to be a band plate shape
with rectangular cross-section and polarized in a direction of the plate
width, and disposed in the rotor core to position the center line of the
plate width on the boundary line, so that one pole thereof serves as any
one of the adjacent magnetic poles and the other pole serves as the other
of the adjacent magnetic poles.
When the ferrite magnet is used for the first permanent magnet, the
rare-earth magnet is used for the second permanent magnet. Conversely,
when the rare-earth magnet is used for the first permanent magnet, the
ferrite magnet is used for the second permanent magnet.
In any way, the first permanent magnet is formed to be a band plate shape
with rectangular cross-section and polarized in a direction of the plate
width, and disposed in the rotor core to position the center line of the
plate width on the boundary line.
On the other hand, for the second permanent magnet, various shapes can be
available. For example, a band plate shape with rectangular cross-section,
arch-shaped cross-section, or trapezoid cross-section may be used. In the
case of a shape of rectangular cross-section, the second permanent magnet
is preferably disposed along a direction perpendicular to a diametrical
line of the rotor core. In the case of a shape of arch-shaped
cross-section, the second permanent magnet is preferably disposed in a
state that the convex face thereof is oriented toward the center of the
rotor core. Further, in the case of a shape of trapezoid cross-section,
the second permanent magnet is advisably disposed in a state that the
upside thereof is oriented toward the center of the rotor core.
Furthermore, a hole for flux barrier is formed between the first permanent
magnets in the vicinity of the inner circumference of the rotor core,
thereby preventing short-circuit and leak of the magnetic flux in between
the adjacent permanent magnets. According to the preferable embodiment,
holes for the flux barrier are also formed at both ends of the second
permanent magnet.
In the present invention it is preferable that the rotor core is formed of
a laminated body made of a magnetic steel plate which is stamped out
through a pressing process. In this case, it is desirable in terms of
manufacturing that holes for inserting the permanent magnets are opened in
the laminated body of the magnetic steel plate during the pressing process
so that the first permanent magnet and the second permanent magnet are
embedded to be polarized. Thereby, a conventional producing processes can
be continuously employed, so that the production cost is not increased.
The present invention is appropriate for a brushless DC motor used for
driving a compressor in an air conditioner, whereby the performance of the
air conditioner can be improved.
BRIEF DESCRIPTION OF THE DRAWINGS
The present invention will be described further hereinafter, by way of
example only, with reference to the accompanying drawings in which:
FIG. 1 is a diagrammatic plan view showing a structure of a permanent
magnet rotor type electric motor as an embodiment according to the present
invention from a plane perpendicular to the axis of rotation thereof;
FIG. 2 is diagrammatic vertical sectional view along the axis d of a rotor
core shown in the above embodiment;
FIG. 3 is an enlarged plan view of the rotor core shown in the above
embodiment;
FIG. 4 to FIG. 7 are diagrammatic plan views showing modifications of the
above rotor core;
FIG. 8 is a diagrammatic plan view showing a structure of a permanent
magnet rotor type electric motor as a first conventional example, which is
similar to FIG. 1; and
FIG. 9 is a diagrammatic plan view showing a structure of a permanent
magnet rotor type electric motor as a second conventional example.
DETAILED DESCRIPTION OF PREFERRED EMBODIMENT(S)
In the present invention, a magnetic flux density and a reluctance torque
can be established in required values by forming each magnetic pole in a
rotor core of a plurality of permanent magnets and making the permanent
magnets of different magnetic materials. Therefore, as shown in FIG. 1 and
FIG. 3, each magnetic pole in a rotor core 10 is formed of a first
permanent magnet 11 of ferrite magnet and a second permanent magnet 12 of
rare-earth magnet, and the permanent magnet 11 is shared between the
adjacent magnetic poles in this embodiment.
Incidentally, the rotor core 10 is made of a magnetic steel plate and
disposed inside a stator core 16 generating a rotation magnetic field. The
explanation of the stator core 16 will be omitted since, in the
performance of the present invention, the stator core 16 may be similar to
the stator core 1 shown in FIG. 8 which is explained hereinbefore.
The first permanent magnet 11 made of the ferrite magnet is formed to be a
band plate shape which is slightly thick having rectangular cross-section
and polarized in a direction of the plate width. In FIG. 1, one axis q and
the other axis perpendicular thereto are magnetic-pole boundary lines
between the adjacent magnetic poles, which pass through the center of the
rotor core 10. When each of the boundary lines is B, each first permanent
magnet 11 is disposed between the adjacent magnetic poles so that the
center line of the plate width thereof is positioned on a boundary line B.
That is to say each first permanent magnet 11 is imaginary divided by a
boundary line B into a magnet portion 111 on the north pole side and a
magnet portion 112 on the south pole side.
In this embodiment, the second permanent magnet 12 made of the rare-earth
magnet has rectangular cross-section similar to the first permanent magnet
11 but is formed to be a band plate shape which is slightly thin. The
second permanent magnet 12 is disposed along a direction perpendicular to
a diametrical line of the rotor core 10 in the vicinity of the outer
circumference of the rotor core 10 in each magnetic pole. Accordingly, in
each magnetic pole, the north pole is formed of three magnets which are
two magnet portions 111 and 111 of the adjacent first permanent magnets 11
and 11 and the second permanent magnet 12 in the north pole, and the south
pole is also formed of three magnets which are two magnet portions 112 and
112 of the adjacent first permanent magnets 11 and 11 and the second
permanent magnet 12 in the south pole.
Differently from the above embodiment, two permanent magnets corresponding
to each of magnet portions 111 and 112 may be disposed in parallel to each
other along a boundary line B. In this embodiment, the second permanent
magnet 12 has a sectional rectangular shape, but the second permanent
magnet 12 may have a sectional arch-shape and be disposed to orient the
convex face thereof toward the center of the rotor core 10.
At the end of each first permanent magnet 11 in the vicinity of the inner
circumference of the core and between the adjacent first permanent magnets
11 and 11, a hole 13 for the flux barrier is formed to prevent
short-circuit and leak of the magnetic flux, occurring between the first
permanent magnets 11. And also, at both ends of second permanent magnet
12, holes 14 and 14 for flux barriers are respectively formed because of
the same reason as above. Incidentally, a center hole 15 for passing a
rotating shaft (not shown) is formed on the axis line of the rotor core
10.
Next, a magnetic flux density and a reluctance torque of the rotor core 10
will be explained with reference to FIG. 3. In the drawing, a curve line
of a broken line with arrows shows the magnetic flux and a curve line of a
solid line with arrows shows a magnetic circuit.
According to the present invention, the first permanent magnet 11 made of
the ferrite magnet is shared between the adjacent magnetic poles and the
second permanent magnet 12 made of the rare-earth magnet is disposed in
each magnetic pole, so that, as compared with the using of the ferrite
magnet only, the magnetic flux density can be increased further, and
additionally, the distance between the first permanent magnet 11 and the
second permanent magnet 12 can be longer.
Additionally, the occupying rate of the ferrite magnet in the core is
controlled, therefore, as compared with the case that each magnetic pole
is formed of the ferrite magnet only for example, the magnetic resistance
of the magnetic circuit becomes low. That is to say, when each magnetic
pole is formed of only the ferrite magnet, the most of the rotor core 10
is occupied with the ferrite magnet to attain the same magnetic flux
density as that in this embodiment, so that the magnetic resistance of the
magnetic circuit becomes high naturally.
As described thus far, in the embodiment, the magnetic resistance of the
magnetic circuit can be low by decreasing the occupying rate of the
permanent magnet and increasing the occupying rate of a magnetic steel
plate which is the body of the rotor core 10, thereby the inductance on
the axis q can be large. Therefore, a difference between the inductance on
the axis q and the inductance on the axis d becomes large, which means the
reluctance torque can be increased.
According to the embodiment, the required magnetic flux density can be
attained by controlling the used amount of the ferrite magnet as the first
permanent magnet 11 and the rare-earth magnet as the second permanent
magnet 12. For example, a lower magnetic flux density can be attained
comparing to the case that all the magnetic poles are formed of the
rare-earth magnet.
On the other hand, in a case where the ferrite magnets are used for all the
magnetic poles to attain the magnetic flux density to be needed, the
thickness of the permanent magnet (polarized area) often exceeds the limit
in the manufacturing. However, the magnetic flux density can be
appropriately controlled by using the ferrite magnet and the rare-earth
magnet together. Therefore, the required magnetic flux density is easily
attained without making the polarized area large.
Further, short-circuit and leak of the magnetic flux can be prevented by
the hole 13 for the flux barrier which is formed between the first
permanent magnets 11 and the holes 14 for the flux barrier which are
formed at both ends of the second permanent magnet 12, so that the
magnetic flux error by the first and the second permanent magnets 11 and
12 is small and the required magnetic flux density can be further easily
attained.
Furthermore, the additional using of the less expensive ferrite magnet
controls the amount of the rare-earth magnet used, thereby attaining a
lower cost comparing to the case in which all the magnetic poles are
formed of the rare-earth magnet.
As shown in FIG. 2, the rotor core 10 is produced through processes in
which magnetic steel plates are mechanically laminated inside a die (not
shown) after being stamped out in the same shape by pressing. Preferably,
concurrently with the pressing process, spaces (holes) accommodating the
permanent magnets 11 and 12 are opened in all the magnetic steel plates,
and all the permanent magnets 11 and 12 are embedded inside the spaces to
be polarized. It is advisable that the holes 13 and 14 for the flux
barrier are opened during the above process. The permanent magnets 11 and
12 are inserted into the rotor core 10 in the lateral direction in FIG. 2.
According to the above description, since the rotor core 10 is produced
through the conventional press processes, the production-efficiency is not
reduced, and also the production cost is not increased.
Those skilled in the art will determine positions of attaining sufficient
strength for enduring centrifugal force during the rotation of the rotor
core 10, in regard to the position of each end of the permanent magnets 11
and 12, specifically each position thereof in the vicinity of the outer
circumference of the rotor core 10, and each position for forming the
holes 13 and 14 for the flux barrier. Additionally, the hole for
accommodating (embedding) the second permanent magnet 12 and the holes 14
for the flux barrier, formed at both ends of the second permanent magnet
12, may be integrally formed, namely, formed as a linked hole.
A "Brushless" DC motor having the rotor core 10 is suitable for driving a
compressor of an air conditioner, and the performance of the air
conditioner can be improved (enhancement of the operating efficiency,
reduction in noise or vibrations) without increasing in cost by the
blushless DC motor.
Next, a modification of the rotor core 10 shown in FIG. 4 will be described
below. In the modification, a first permanent magnet 17 made of the
rare-earth magnet is disposed on a boundary line B between the adjacent
magnetic poles, and a second permanent magnet 18 made of the ferrite
magnet is disposed in the vicinity of the outer circumference of the rotor
core 10 in each magnetic pole. That is to say, the ferrite magnet and the
rare-earth magnet are disposed in converse with the aforementioned
embodiment.
The first permanent magnet 17 made of the rare-earth magnet is formed to be
a slightly thin band-plate shape having rectangular cross-section and
disposed so that the center line of the plate width lies upon a boundary
line between the magnetic poles, therefore the first permanent magnet 17,
as the first permanent magnet 11 of the aforementioned embodiment, is
shared between the adjacent magnetic poles.
On the other hand, the second permanent magnet 18 made of the ferrite
magnet has a trapezoid shape in section and disposed so that the upside
thereof which is shorter side is oriented toward the center of the rotor
core 10 in the vicinity of the outer circumference in each magnetic pole.
Further, a hole 19 for the flux barrier is formed at the end of the first
permanent magnet 17 in the vicinity of the inner circumference of the
core, and between the adjacent first permanent magnets 17 and 17, to
prevent short-circuit and leak of the magnetic flux. In the modification,
each hole 19 for the flux barrier is individually formed in an arch-shape
around the center hole 15.
According to the modification, the first permanent magnet 17 is made of the
rare-earth magnet and the magnetic flux density is high, therefore the
polarized area is smaller than the first permanent magnet 11 of the
aforementioned embodiment (refer to FIG. 3). On the other hand, the second
permanent magnet 18 is made of the ferrite magnet and the magnetic flux
density is low, therefore the polarized area is larger than the second
permanent magnet 12 of the aforementioned embodiment (refer to FIG. 3).
As to the magnetic flux density, there is no big difference from the
aforementioned embodiment. The occupying rate of the second permanent
magnet 18 in the core becomes high, but the occupying rate of the first
permanent magnet 17 in the core becomes low, thus the magnetic resistance
of the magnetic circuit remains low as in the case the aforementioned
embodiment. Accordingly, a difference between the inductance on the axis q
and the inductance on the axis d becomes large, so that the reluctance
torque can be increased.
Furthermore, as necessary in designing, the second permanent magnet 18 may
be formed to be a band plate with rectangular cross-section and disposed
along a direction perpendicular to a diametrical line of the rotor core 10
as shown in FIG. 6. Alternatively, the second permanent magnet 18 may be
formed to be a band plate with arch-shaped cross-section and disposed to
orient the convex face thereof toward the center of the rotor core 10
shown in FIG. 7.
In any modification, by various combinations of the ferrite magnet and the
rare-earth magnet, the reluctance torque and the magnetic flux density can
be selected from various values, that is to say the degree of selection
thereof can be enlarged.
Although the present invention has been shown and described with respect to
a best mode embodiment thereof, those skilled in the art understanding the
subject-matter of the present invention should readily think out other
changes, variations, and equivalents thereof, so that the scope of the
present invention should be within the scope of the accompanying claims
and the equivalencies thereof.
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Today In History
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Patent No. 5
August 17, 1993
Thomas Welsh was issued a patent for a platform steerable skateboard.
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