U.S. patent application number 11/157789 was filed with the patent office on 2005-11-17 for permanent magnet motor for driving a fan.
Invention is credited to Enomoto, Yuji, Ishii, Hitoshi, Kawashima, Katsuo, Sekiguchi, Osamu.
Application Number | 20050253471 11/157789 |
Document ID | / |
Family ID | 32844448 |
Filed Date | 2005-11-17 |
United States Patent
Application |
20050253471 |
Kind Code |
A1 |
Enomoto, Yuji ; et
al. |
November 17, 2005 |
Permanent magnet motor for driving a fan
Abstract
A permanent magnet motor for driving a fan is rotated while a
movement of the rotor in a direction of thrust of a rotary shaft
with a rotation of the fan is prevented by magnetic attraction
force of a permanent magnet and a stator core. A surface magnetic
flux density of the permanent magnet facing the stator core is
lower at an end portion than at a central portion of the permanent
magnet in the direction of thrust of the rotary shaft.
Inventors: |
Enomoto, Yuji; (Hitachi,
JP) ; Sekiguchi, Osamu; (Ryugasaki, JP) ;
Ishii, Hitoshi; (Aioi, JP) ; Kawashima, Katsuo;
(Aioi, JP) |
Correspondence
Address: |
DICKSTEIN SHAPIRO MORIN & OSHINSKY LLP
2101 L Street, NW
Washington
DC
20037
US
|
Family ID: |
32844448 |
Appl. No.: |
11/157789 |
Filed: |
June 22, 2005 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
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11157789 |
Jun 22, 2005 |
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10776262 |
Feb 12, 2004 |
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6943475 |
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Current U.S.
Class: |
310/90 |
Current CPC
Class: |
H02K 7/14 20130101; F04D
29/051 20130101; F04D 25/0606 20130101; F04D 25/06 20130101; H02K
7/09 20130101 |
Class at
Publication: |
310/090 |
International
Class: |
H02K 005/16; H02K
007/08 |
Foreign Application Data
Date |
Code |
Application Number |
Feb 17, 2003 |
JP |
2003-037766 |
Claims
1-4. (canceled)
5. A permanent magnet motor for driving a fan, comprising: a rotor
including a permanent magnet; a stator including a stator core
having a stator winding; a bearing for rotatably supporting a
rotary shaft of said rotor; and a fan arranged on said rotor;
wherein said fan is rotated while a movement of said rotor in a
direction of thrust of the rotary shaft with a rotation of said fan
is prevented by a magnetic attraction force of the permanent magnet
and the stator core; and wherein the permanent magnet has an
opposed portion in opposed relation with an end surface of the
stator core in a direction of thrust of the rotary shaft, and the
magnetic attraction force of the opposed portion and the stator
core prevents a movement of said rotor in the direction of thrust
of the rotary shaft.
6-9. (canceled)
10. A permanent magnet motor for driving a fan, comprising: a rotor
including a permanent magnet; a stator including a stator core
having a stator winding; a bearing for rotatably supporting a
rotary shaft of said rotor; and a fan arranged on said rotor;
wherein the fan is rotated while preventing, by a magnetic
attraction force of the permanent magnet and the stator core, said
rotor moving in a direction of thrust of the rotary shaft with a
rotation of said fan; and wherein a surface magnetic flux density
of the permanent magnet facing the stator core is lower at an end
portion than at a central portion of the permanent magnet along the
direction of thrust of the rotary shaft, and wherein a gap between
the rotor and the stator is constantly maintained at opposite
surfaces with a flux density of the gap being variable.
11. The permanent magnet motor recited in claim 10, wherein no
feedback control is provided which results in the elimination of
complicated control.
12. The permanent magnet motor recited in claim 11, wherein said no
feedback control further comprises winding current and voltage.
Description
BACKGROUND OF THE INVENTION
[0001] 1. Field of the Invention
[0002] This invention relates to a small fan motor such as an
ordinary fan motor and a disk drive motor.
[0003] 2. Description of the Related Art
[0004] The fan motor is generally used for cooling or blowing
devices. The fan motor is required to be high in efficiency and
also low in vibration and noises. Normally, to reduce the vibration
and noises, a mold motor is employed for the purpose of increasing
the mechanical rigidity of the motor and reducing the transfer of
the electromagnetic vibration generated by the motor.
JP-A-2001-231192 discloses a mold motor in which the entire stator
core including the winding of the motor is molded so that resin is
filled between the stacked cores thereby to reduce the transfer of
the electromagnetic vibration generated by the stator core.
[0005] Another conventional method of reducing the vibration and
noises is disclosed in JP-A-8-70550. In this motor, the assembly
accuracy between the stator and the bearing unit and between the
shaft and the rotor, the accuracy and the assembly accuracy of the
parts are improved to suppress the vibration due to the wobbling
generated from the error thereby to reduce the vibration and noises
of the motor as a whole.
[0006] In the conventional motors described above, the unique
values of each motor can be changed by molding the motor and
increasing the mechanical rigidity of the whole motor. In these
conventional motors, however, the resonant point is simply
transferred to another frequency band, and the vibration source of
the motor is not affected. Therefore, the problem vibration and
noises are still generated as far as the relation with the housing
for mounting the motor is concerned. With regard to the improved
accuracy, on the other hand, the electro-magnetic vibration
generated by the motor itself remains equivalent. Therefore, the
problem vibration and noises are generated by the resonance
achieved in view of the fact that the electromagnetic vibration of
the stator has the natural frequency of the system according to the
manner in which the housing is mounted.
[0007] In recent years, a product set with a fan motor built
therein is required to have a highly efficient motor and a reduced
size to reduce the power consumption. For this purpose, the efforts
are made to improve the winding occupancy rate, reduce the size
using the optimum design technique and employ the highly efficient
design. An improved motor efficiency is accompanied by a higher
output such as a higher torque or a higher rotational speed under
the same input conditions. Therefore, the electromagnetic vibration
constituting the source of the vibration and noises is
correspondingly increased. On the other hand, the product set is
required to produce a smaller vibration and noises than the
predecessors, and therefore the electromagnetic vibration generated
from the motor is required to be reduced.
SUMMARY OF THE INVENTION
[0008] An object of this invention is to solve a problem described
above and to provide a fan motor high in efficiency and small in
electromagnetic vibration, in which the required output is secured
with a reduced vibration and noise according to the shape of the
rotor magnet of the fan motor.
[0009] In order to achieve the object described above, according to
this invention, taking note of the axial vibration of the fan
motor, there is provided a method of reducing the axial vibration
of rotation generated in the motor providing an axial vibration
source. The fan motor is rotated normally at high speed, and thus
has the function of generating the wind by rotating the fan (vane)
mounted on the shaft of the motor rotor. With the occurrence of the
wind, the vane receives the reaction of the wind generated and is
subjected to the thrust force in the direction opposite to the
direction of the wind. Due to this thrust force, the rotor loses
the balance thus far maintained at the magnetic center with the
stator. The rotor thus applies a force in the direction opposite to
the thrust force of the vane by the magnetic attraction force
between the rotor and the stator. This magnetic attraction force is
varied from one rotational portion of the rotor to another
according to the number of rotor poles and the stator slots. While
the rotor is in rotation, therefore, like the cogging torque of the
motor, as many amplitudes as the least common multiple of the
number of poles and the number of slots per rotation are repeated.
The axial vibration is generated from the relation between the
thrust force of the vane and the magnetic attraction force. This
vibration is not generated in the absence of displacement between
the stator and the rotor, and therefore a structure is conceivable
for fixing the position of the rotor in thrust direction. For an
increased mechanical friction, however, the mechanical loss is
increased for a lower motor efficiency. According to this
invention, therefore, the axial vibration is suppressed by changing
the structure of the rotor.
[0010] According to this invention, based on the various trials,
there is provided a permanent magnet motor for driving a fan, in
which even in the case where the rotor is displaced from the
magnetic center of the permanent magnetic thereof and the stator
core by the thrust force of the vane (fan), the amount of
magnetization at the end along the thrust direction of the rotary
shaft of the permanent magnet is reduced as compared with that at
the central portion in such a manner as to reduce the magnetic
attraction force, so that the magnetic force is reduced in the
presence of a minor displacement. In another method that can be
implemented, the diameter at the end of the magnet is reduced as
compared with that at the central portion, or the gap magnetic flux
density is reduced only at the axial end portion by changing the
shape by chamfer, rounding (curving), etc. of the corner. The
magnetic attraction force can be reduced in the presence of a minor
displacement by employing a material only at the end portion having
a different magnetic characteristic such as a small residual
magnetic flux density.
[0011] As described above, the vibration and noises along axial
direction can be reduced by reducing the magnetic attraction force
opposite to the thrust force generated by the fan (vane).
[0012] Other objects, features and advantages of the invention will
become apparent from the following description of the embodiments
of the invention taken in conjunction with the accompanying
drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
[0013] FIGS. 1A to 1D show the distribution of the magnetic flux
density of the permanent magnet of a permanent magnet motor for
driving a fan according to an embodiment of the invention.
[0014] FIG. 2 shows a structure of a permanent magnet motor for
driving a fan according to an embodiment of the invention.
[0015] FIGS. 3A and 3B are diagrams for explaining the balance
between the thrust force of the vane (fan) and the magnetic
attraction force of the permanent magnet and the stator core
according to an embodiment of the invention.
[0016] FIGS. 4A to 4C show a FEM mesh structure and other
conditions such as the distribution of the magnetic flux density of
the rotor magnet to analyze the electromagnetic phenomenon of the
permanent magnet motor for driving a fan according to an embodiment
of the invention.
[0017] FIG. 5 is a graph showing the result of determining the
stress exerted in an axial direction of the rotor by analyzing the
magnetic field using the conditions shown in FIG. 4 according to an
embodiment of the invention.
[0018] FIG. 6 shows the shape of the magnetizing yoke conforming
with the structure of the permanent magnet motor for driving a fan
according to an embodiment of the invention.
[0019] FIGS. 7A to 7D show examples of development of various
shapes conforming with the structure of the permanent magnet motor
for driving a fan according to the invention.
DESCRIPTION OF THE EMBODIMENTS
[0020] A motor according to embodiments of the invention is
described below with reference to the accompanying drawings.
[0021] FIG. 1 shows a structure of a permanent magnet used as a
rotor of a basic fan motor constituting a fan drive motor according
to an embodiment of the invention. In this embodiment, the
permanent magnet has four poles. The rotor 1 having the permanent
magnet includes a rotary shaft 2. The rotary shaft 2 is assembled
directly by the insert-molding means at the center of the rotor 1.
Nevertheless, the rotary shaft may alternatively be assembled using
the press fitting or bonding method.
[0022] FIG. 1A is a side view of the permanent magnet of the rotor
1. The greater part of the rotor 1 is formed of a permanent magnet
which in turn is molded by a die. As indicated by dotted lines, the
cross section of the permanent magnet of the rotor has the
thickness varied along the direction of thrust. As a result, the
magnetic flux density on the surface of the magnet is different at
points a, b and c.
[0023] This permanent magnet, as shown in FIG. 1B, has four poles
(two pairs of poles), and has the magnetic flux density
distribution of one period in the angular range of 0 to 180
degrees. The result of measuring the magnetic flux density
distribution along the axial direction is shown in FIG. 1C, and the
result of measuring the magnetic flux density distribution in the
rotational direction is shown in FIG. 1D. The magnetic flux density
distribution, as viewed in an axial direction, is such that
assuming that the magnetic flux density in the range X having the
axial center at position b is about 100%, the magnetic flux density
at positions a and c is as small as 80% or less. The magnetic flux
density distribution along the rotational direction, on the other
hand, indicates that as shown in FIG. 1D, the peak value at
position b is 100%, while the peak value at positions a and c is
not more than 80%. In this way, the distribution of the surface
magnetic flux density in an axial direction can be changed by
changing the thickness along the axial direction of the permanent
magnet.
[0024] The structure of an ordinary permanent magnet motor for
driving a fan is shown in FIG. 2. The ordinary permanent magnet
motor for driving a fan comprises a stator core 4 having a stator
winding 5. This stator core 4 is molded by synthetic resin thereby
to produce a resin-molded stator. The stator winding 5 and the
stator core 4 are covered with a resin mold portion 3. A rotatable
rotor 1 is arranged-on the inside of the stator. The rotor 1 has a
rotary shaft 2.
[0025] End brackets 15, 15 are arranged on both sides of the
stator. The end brackets 15, 15 are mounted to fit in the counter
lock of the stator.
[0026] The end brackets 15, 15 have bearing holding portions. A
bearing 6 is supported by the bearing holding portions. The bearing
6 is of ball type and rotated by the rolling of balls interposed
between the inner race and the outer race. The rotary shaft 2 is
fitted in the inner race of the bearing 6. The outer peripheral
side of the outer race of the bearing 6 is fitted on the bearing
holding portions, and held in such a manner as to slide along the
direction of thrust of the rotary shaft (longitudinal direction
along the rotary shaft).
[0027] An anti-detachment bank 16 is arranged at the outer end of
the bearing holding portions. In one of the bearing holding
portions (the upper bearing holding portion in the drawing), a
pressure spring 20 is interposed between the anti-detachment bank
16 and the bearing 6. This pressure spring 20 energizes and pushes
the bearing 6 along the direction of thrust of the rotary shaft 2.
Since the rotary shaft 2 is fitted in the inner race of the bearing
6, the rotor 1 is also energized and pushed along the direction of
thrust of the rotary shaft 2. In this way, the rotor 1 is movable
to some degree along the direction of thrust of the rotary shaft 2,
and kept pressed by the pressure spring 20 in one direction.
[0028] The stator 1 has a permanent magnet as described above with
reference to FIG. 1. This permanent magnet and the stator core 4 of
the stator are magnetically attracted with each other. The rotor
movable along the direction of thrust of the rotary shaft is held
at a predetermined position by this magnetic attraction force.
[0029] The blowing vane 7 (the fan for the axial flow) is mounted
at the forward end of the rotary shaft 2 of the rotor 1 and fixed
by a stop ring 8.
[0030] The greater part of the permanent magnet motor for driving a
fan shown in FIG. 3, except for the bearing, has the same
configuration as the permanent magnet motor for driving a fan shown
in FIG. 2.
[0031] The fan driving permanent magnet motor shown in FIG. 2 has a
ball bearing 6, while the fan driving permanent magnet motor shown
in FIG. 3 has a slide bearing 30.
[0032] The slide bearing 30 slidably and rotatably supports the
rotary shaft 2 on the inner peripheral portion thereof, and has the
outer peripheral portion thereof kept fitted in the bearing holding
portions of the end brackets 15, 15. The rotary shaft 2 is slidably
and rotatably supported on the inner peripheral portion of the
bearing 30, and therefore slidable also along the direction of
thrust of the rotary shaft 2. The rotor 1 is thus movable along the
direction of thrust of the rotary shaft 2.
[0033] Further, the balance between the thrust force of the vane 7
(fan for the axial flow) and the magnetic attraction force of the
permanent magnet and the stator core 4 is described below with
reference to FIG. 3.
[0034] FIG. 3A shows the state where the rotor 1 is stationary, and
FIG. 3B shows the state where the rotor 1 is in rotation.
[0035] As shown in FIG. 3B, when the rotor 1 rotates and the vane 7
(fan for axial flow) blows the air rearward, the forward thrust
force (the force for moving in the direction of thrust of the
rotary shaft) of the vane 7 (fan for the axial flow) acts on the
rotor 1.
[0036] The magnetic attraction force of the permanent magnet and
the stator core 4 is exerted against the force of the rotary shaft
to move in the direction of thrust, and balanced at a position
where both forces are in equilibrium so that the rotor 1 is held
stationary at the particular position.
[0037] The magnetic attraction force, however, works differently
depending on the rotational position of the rotor due to the
relation between the number of the stator slots and the number of
the poles of the magnet. Even in the case where a constant thrust
force of the wind is generated by the vane rotating at a constant
rotational speed, therefore, the attraction force acts in the
opposite direction repeatedly with an amplitude equivalent to the
least common multiple of the number of poles and the number of
slots of the stator and the rotor per rotation, thus generating an
oscillation in an axial direction. This oscillation causes the
unrequired vibration and noises by resonating with the natural
frequencies of the motor and the housing on which it is mounted.
How to reduce the oscillation of the magnetic attraction force,
therefore, is crucial to reduce the vibration and noises of the
motor.
[0038] FIGS. 4A to 4C show the conditions for analyzing the force
in an axial direction by the magnetic field analysis method (FEM).
FIG. 4A shows the mesh division of the rotor and the stator of the
motor for FEM analysis. The analysis conditions include the
following two cases:
[0039] Rotor A: Conditions for securing a predetermined magnetic
flux density at points a, b, c in FIG. 1
[0040] Rotor B: Conditions for securing a larger magnetic flux
density at point 1 than at points a and c in the structure shown in
FIG. 1.
[0041] As shown in FIGS. 4B and 4C, the surface magnetic flux
density of the rotor A is uniform in an axial direction, and the
surface magnetic flux density of the rotor B is set high at the
central portion in an axial direction. Also, as viewed in the
direction of rotation, the rotor A has the same magnetic flux
density distribution at all of the positions a, b and c, while the
rotor B has a high magnetic flux density at the central portion
thereof. Thus, the peak value is set higher for the rotor B. This
is in order to secure the same torque even in the case where the
magnetic flux density is low at the ends.
[0042] FIG. 5 shows the result of FEM analysis. The force exerted
along the axial direction of the rotor is generated from neither
the rotor A nor the rotor B as long as the rotor position is not
displaced from the position magnetically balanced with the
stator.
[0043] In the case where the rotors A and B are displaced by 50
.mu.m, on the other hand, both generate the magnetic attraction
force thereby to generate an oscillation equivalent to the least
common multiple of the number of poles and slots of the stator and
the rotor. The level of this vibration is larger for the rotor A by
about forty percent. Incidentally, the rotational speed output from
the motor and the torque thereof are the same. This result shows
that the vibration level due to the magnetic attraction force can
be reduced more with the configuration of the rotor B for reducing
the magnetic attraction force.
[0044] FIG. 6 shows a structure of the magnetization yoke for
reducing the magnetic flux density in an axial direction of the
magnet rotor only at the end portion thereof. The thickness in an
axial direction of the magnetization yoke is reduced, so that the
magnetic fluxes are concentrated at the central portion.
[0045] FIGS. 7A to 7D show a method of implementing the axial
magnetic flux density distribution with various structures of the
rotor magnet.
[0046] FIG. 7A shows a structure intended to realize the magnetic
flux density distribution of FIG. 1 by employing a plurality of
types of magnet materials including a material 1a high in residual
magnetic flux density and a material 1b low in residual magnetic
flux density which are used differently in an axial direction.
[0047] FIG. 7B shows a structure in which the outer diameter of the
axial end portion is rendered smaller by chamfering than the outer
diameter of the central portion so that the gap between the stator
and the rotor is widened to secure a sufficient magnetic attraction
force. This method is implemented also by reducing the diameter of
the end portion by machining or rounding.
[0048] FIG. 7C shows a structure in which the axial thickness of
the stator and the rotor are changed in such a manner that the
stator is thicker than the rotor to prevent the attraction force
from being generated even in the case where the rotor moves in an
axial direction under the thrust force.
[0049] FIG. 7D shows a structure in which a portion in opposed
relation to the thrust surface of the stator is formed at the axial
end of the rotor magnet, so that the stator and the rotor are kept
attracted by the magnetic attraction force along the direction of
thrust, thereby preventing the vibration from being caused by the
thrust force of the vane.
[0050] According to this invention, an inexpensive fan motor very
small in vibration and noise and having a high strength, high
accuracy and high reliability is obtained without adversely
affecting the motor performance.
[0051] It should be further understood by those skilled in the art
that although the foregoing description has been made on
embodiments of the invention, the invention is not limited thereto
and various changes and modifications may be made without departing
from the spirit of the invention and the scope of the appended
claims.
* * * * *