KR100189078B1 - A single-phase brushless axial fan motor - Google Patents

Abstract

By inserting the single-phase coreless stator armature on the stator armature support without screwing it, the armature is held at the position and a certain quality is generated to generate a constant dead retraction torque for dead spot escape. DC single phase brushless axial fan motors are easily and cheaply obtained. Armature coil-mounted stator to obtain air gaps for disposing the drive circuit on the underside of the board. Four-point escape reluctance torque generation and single-phase coreless stator mounted on the head of the armature support arm. Engagement parts such as perforations formed on the substrate are inserted by means of insertion or the like. The armature coil on the armature coil-mounted substrate is arranged such that the magnetic protrusion is located within a angular range that is 1/2 the magnetic pole of the magnetic field magnet from the dead point position, and the magnetic field protrusion is constrained to the magnetic field magnet. A dead point escape reluctance torque is generated to prevent it from being prevented.

Description

DC Single Phase Brushless Axial Flow Fan Motor

1 is an exploded perspective view of an axial void type (disc) direct current single-phase brushless axial fan motor showing a first embodiment of the present invention.

2 is a longitudinal cross-sectional view of the fan motor of FIG.

3 is an enlarged perspective view of the motor excretion unit.

4 is a perspective view of a venturi case in which a single-phase coreless stator armature is disposed in the motor excretion unit of FIG. 3.

5 is an exploded view of the armature coil in the field magnet single phase arrangement.

6 is a schematic diagram illustrating the principle of a single-phase brushless motor.

7 is a longitudinal sectional view of a conventional direct current single phase brushless axial fan motor.

* Explanation of symbols for main parts of the drawings

1: Electronic torque curve 2: Synthetic torque curve

3-1,3-2: Dead point 4: Reluctance torque curve

5: field magnet 6,6 ': steak yoke

7,7 ': single-phase coreless stator armature

8,8 ': Axial airflow direct current single phase brushless axial fan motor

9-1,9-2: Armature coil 9a, 9b: Effective conductor part contributing to generated torque

9c, 9d: Conductor part not contributing to generated torque

10,10 ': Venturi case 11: Rotating fan

12: stay 13: motor excretion unit

14: impeller (rotary wing) 15: air flow through

16: bearing housing 17: ball bearing

18: sliding bearing 19: rotating shaft

20: Perforation 21: Printed (wiring) board

22: screw hole

23: Intellectual protrusion for positioning dead-point reluctance torque and single-phase coreless stator armature positioning (magnetic rod)

24: axial void 25: through hole

26: rotor yoke 27: magnetic screw

28: semiconductor stop value (drive circuit) 29: PNP type transistor

30: magnetoelectric conversion element 31: driver circuit (conduction control circuit) IC

32,32 ': Stator armature support holder 33: Air gap

34: NPN transistor 35: PNP transistor

36: NPN transistor 37: Positive (+) side power supply terminal

38: negative power terminal 39-1, 39-2 output terminal

41 hook 42: coupling recess

43: coupling protrusion 44,45: coupling groove

BACKGROUND OF THE INVENTION 1. Field of the Invention [0001] The present invention relates to a DC single-phase brushless axial fan motor, and to a DC single-phase brushless axial fan motor which is capable of self-driving with a simple configuration and suitable for a cooling fan motor such as a computer switching power supply. .

(DC) brushless motors are used for axial fan motors.

In general, brushless motors have been widely used in recent years because of their high reliability in addition to the characteristics of direct current motors such as high torque and good controllability. By the way, two phases and three phases are mainly used for the brushless motor, but as the constant of the motor increases, the Hall element used as the expensive driving circuit and the position detecting element by the number of the constants, A magnetoelectric conversion element such as a Hall IC (Integrated Circuit) is required. Therefore, in the DC brushless axial fan motor for the purpose of blowing air only for cooling, it is desirable to solve the driving circuit and the electromagnet conversion element as one and make it a cheap single-phase brushless motor type.

However, since the two-stage brushless motor has a part where the torque becomes zero (dead spot part), if the rotation stops at the dead point position occasionally, there is a drawback that self-automatic rotation is not possible. When the rotation is stopped at the dead point position, even when the armature coil is energized, it is not possible to generate a torque by the armature coil, and the magnetoelectric conversion element used as the position detecting element also has a field magnet ( Since the boundary line between the N pole and the S pole of the magnet) is detected, no output signal is output from the magnetoelectric conversion element, and the drive circuit is in a state in which the armature coil cannot be energized. The advantages will be further described below. Usually, when considering the constant of the motor, the energized state of the electromagnetic coil is considered without simply determining the placement of the armature coil.

In the single-phase brushless motor, the electromagnetic torque curve 1 obtained by the armature coil when energizing the armature coil is shown as shown in FIG. In FIG. 6, the rotation angle is taken on the horizontal side, and the torque intensity is taken on the vertical axis.

On the other hand, since the two-phase brushless motor has two-phase armature coils that are out of phase by an angle of π / 2 (π is 180 degrees in electrical angle), the two-phase armature coil is energized. The combined torque curve obtained by combining two electromagnetic torque curves obtained by each armature coil does not have a dead point position where torque is zero. Therefore, when this two-phase brushless motor is energized, the torque does not become zero at any position during rotation, and thus, the motor rotates automatically.

However, in the single-phase brushless motor, since the armature coil is in a single phase arrangement, the torque is zero at the energization switching point of the armature coil. There is a so-called "dead spot". In the case of a single-phase brushless motor, the armature coil is in a single phase arrangement. As shown in FIG. 6, the electromagnetic torque curve 1 obtained when the armature coil is energized is zero dead point at the energization switching point at an angle of 2π. (3-1), (3-2) and two places.

When the field magnet stops at such dead point (3-1) (3-2) and the position, if the magnetoelectric conversion element is stopped at the position opposite to the dead point (3-1) (3-2), If there is no output signal and the armature coil is not energized by the drive circuit, it is not possible to obtain the rotation torque even when the single-phase brushless motor is energized, and magnetic rotation is not possible.

In general, when the field magnet is stopped at the dead point position, the magnetoelectric conversion element also has the dead points (3-1) and (3-2) of the field magnets facing the boundary between the N pole and the S pole of the field magnet. Therefore, it is common that the output signal is not output from the magnetoelectric conversion element and the armature coil is configured so as not to energize.

In addition, the armature coil is also a position where no torque is generated even when the armature coil is energized.

In addition, in order to obtain an ideal torque rotation angle curve in a magnetically movable single-phase brushless motor, a synthetic torque curve 2 as shown in FIG. 6 in which the electromagnetic torque curve 1 and the reluctance torque curve 4 are synthesized is obtained. I need to get According to this reluctance curve 4, it turns out that an escape torque is obtained to the dead point 3-1, (3-2) position.

As can be seen from the electromagnetic torque curve 1 and the reluctance curve 4, the reluctance torque is preferably made to be one half the electromagnetic torque. In this way, a combined torque curve 2 of substantially constant rotational torque is obtained over the entire region of the rotational angle. The single-phase brushless motor having the combined torque curve 2 can smoothly operate and continuously rotate.

That is, in the case of the single-phase brushless motor in which the synthesized torque curve 2 is obtained, since there is no dead point where the torque becomes zero when the armature coil is energized even in the single-phase, that is, when the start-up, the magnetoelectric conversion element is the N pole of the field magnet. Alternatively, since the magnetic pole of any of the S poles is detected and there is an output signal from the magnetoelectric conversion element, when the armature coil is energized based on this signal, it is possible to obtain a rotational torque in a predetermined direction, and the magnet of the field in the predetermined direction. Self-driving by.

As described above, in addition to the electromagnetic torque obtained by the armature coil and the field magnet, a reluctance torque (cogging torque) is added at the dead spots (3-1) and (3-2) by the magnetic processing means. By doing so, the phenomenon in which the motor stops at the dead point position is eliminated, and the magnetic driving is possible. In this way, a combined torque curve with a substantially constant rotational torque is obtained over the entire region of the rotational angle.

As a specific direct current (DC) single phase brushless axial fan motor using such a single phase brushless motor which enables such a magnetic movement, there exists a coreless structure of the axial air gap type shown in FIG. Since the DC single-phase brushless axial fan motor 8 'must be formed at low cost, it must be made simple and can be easily assembled.

In this regard, the DC single-phase brushless axial fan motor 8 'shown in FIG. 7 has an advantageous structure.

The DC single-phase brushless axial fan motor 8 'has a field magnet 5 for the poles of the north pole and the south pole, where the pole is P (P is an integer of 1 or more, and now P = 2 and 4 poles). A rotating fan 11 having a rotor as a rotor, and n (n is one or more in the stator yoke (b ') surface facing the field magnet 5 through the axial gap 24) Integer, n = 2) Coreless (iron-free) armature coils 9-1 and 9-2 are arranged in single phase (the armature coils 9-1 and 9-2 are in phase with each other) And the single-phase coreless data armature 7 'formed to face each other.

One magnetoelectric conversion element 30 is disposed on the upper surface for detecting the field of the field magnet 5 and determining the energization direction of the armature coils 9-1 and 9-2 based on the detection signal. A printed (wiring) substrate 21 is disposed on the bottom surface of the stator yoke 6 ', and the rotating conversion element 30 is placed in a perforation formed in the stator yoke 6'. Doing. The stator yoke 6 'is made of an armature coil mounting substrate.

Since the stator armature 7 'forms a gap 33 for accommodating a drive circuit (drive IC 31 for driving) between the motor excretion portion 13 and the single-phase coreless stator armature 7', When integrally molded with a venturi case 10 'resin including the motor excretion unit 13, the motor excrement unit 13 is integrally formed with a resin and positioned at two positions in which the stator armature support column 32' is 180 ° symmetrical. Forming. A screw hole 22 is provided in the stator armature support column 32 '.

On the underside of the printed board 21, a drive circuit IC 34 electrically connected by an electrically conductive wiring pattern (not shown) formed on the printed board 21 and solder or the like is disposed, and the stator armature 7 'and The drive circuit IC 31 is accommodated in the supply section 33 between the motor accommodating sections 13.

The stator armature support column 32 'is formed through a hole formed in the stator yoke 6' and a hole formed in the annular printed circuit board 21 by forming a magnetic screw (e.g., iron screw) 27 as a magnetic material. The coreless stator armature of the single-phase arrangement in the magnetic field of the field magnet 5 by inserting a screw into the screw hole 22 of the screw and placing the stator armature 7 'on the stator armature support column 32'. (7 ') is arrange | positioned.

The magnetic body for screwing to the stator armature support column 32 'for mounting and fixing the stator armature 7' inherently as a means for obtaining dead-point escape torque in the DC single-phase brushless axial fan motor 8 'of this embodiment. The screw 27 has a function as a magnetic copper processing means.

In the DC single-phase brushless axial fan motor 8 ', the magnetic coils 9-1 and 9-2 on the stator 6' need to be magnetically moved from the dead-point position of the magnetic screw 27. The field magnet 5 is disposed on the stator armature support column 32 ′ so as to be positioned at a position spaced apart by about a quarter of the magnetic pole width of the field magnet 5, by the magnetic screw 27. Dead-rejection reluctance stroke is generated to prevent constrained to the dead point position.

That is, about 4 of the field magnet 5 is directed from the conductor portion 9a which contributes to the generated torque of the armature coils 9-1 and 9-2 in the direction opposite to the rotation direction of the field magnet 5. The stator armature support column 32 'is formed in the motor excretion portion 13 and the screw hole 22 formed in the strut 32' at a position spaced by an angle of one magnetic pole, and the screw hole thereof. The magnetic screw 27 to be screwed into the 22 is also present at the position of the above conditions.

In order to attach the magnetic body 27 to the support 32 'existing at the position of the above condition, the magnetic field magnet 5 is the N pole or the S pole of the magnetic screw 27 and the magnetic field magnet 7 when it is not energized. Stop at the magnetically combined position with the central part of the magnetic pole.

Since the armature coils 9-1 and 9-2 are disposed at positions shifted in the circumferential direction by the angle of the quarter magnetic pole from the magnetic body screw 27, the armature coils 9-1 or The magnetoelectric conversion element 30 disposed at a position opposite to the effective conductor portion 9a (see FIG. 1) that contributes to the generated torque extending in the radial direction of (9-2) is secured to the field magnet 5. The magnetic pole of the N pole or the S pole can be detected. In addition, since the magnetoelectric conversion element 30 does not face dead centers 3-1 and 3-2, the armature coils 9-1 and 9-2 also exist at positions where torque can be generated. The output signal is obtained from the magnetoelectric conversion element 30. When the armature coils 9-1 and 9-2 are energized based on this signal, the armature coils 9-1 and 9-2 generate rotational torque in a predetermined direction, and the field magnet ( It is possible to automatically rotate 5) in that direction.

During rotation, the magnetic dead thread 27 generates the dead point escape reluctance torque as indicated by the reluctance torque curve 4 of FIG. 6 at the dead centers 3-1 and 3-2. The combined torque curve 2 obtained by combining the electromagnetic torque curve 1 by the armature coils 9-1 and 9-2 with the reluctance torque curve 4 is obtained, and the combined torque curve 2 is obtained. According to this, since dead spots 3-1 and 3-2 do not exist, the field magnet 5 rotates continuously.

[Problems with Prior Art]

The DC single-phase brushless axial fan motor 8 'is extremely useful because its structure is extremely simple and inexpensive to mass-produce.

In particular, the structure is extremely small and lightweight, having a small appearance, i.e., a length x width of 25 mm x 25 mm, 30 mm x 30 mm, 40 mm x 40 mm in a plane, and thicknesses of 6 mm and 10 mm. It is useful for DC single-phase brushless axial fan motors with size.

However, the DC single phase brushless axial fan motor 8 'may be extremely simple in structure, and is a means for positioning the single phase coreless stator armature 7'. That is, the single-hole brushless is made by combining the perforations formed in the stator yoke 6 'and the perforations formed in the printed board 21 with the screw holes 22 formed in the stator armature support 32' thereon. While holding the stator armature 7 'thereon, the magnetic body 27 is screwed into the two perforations and the screw holes 22 using the magnetic body 27, and the single-phase brushless stator armature 7' is inserted. It is necessary to fix on the stator armature support column 32 '. In the case where a slight error occurs in accordance with the positions of the two perforations and the screw holes 22, the magnetic screw 27 is screwed into the head of the head of the stator armature support 32 '. The stator armature support column 32 'having a small diameter formed of a resin may be damaged due to the fastening of the magnetic screw 27. FIG. In addition, when the fastening angles of the magnetic screw 27 are different, an error occurs in the magnitude of the generated reluctance stroke by the head of the magnetic screw 27. Therefore, a DC single-phase brushless axial fan motor 8 'of a certain quality is used. There is a fear that you will not get.

[Problem of invention]

In the DC single-phase brushless axial fan motor, the armature of the single-phase coreless stator armature is eliminated without the need for screwing a magnetic screw to generate a magnetic torque (for dead-spot escape) reluctance stroke at a dead point position. DC single phase brush of constant quality with small error by making it easy to determine the mounting position to the supporting support, and generating a certain amount of self-driving (for dead-spot escape) reluctance torque for reliably moving at dead-point position. An object of the present invention is to make a lease axial fan motor inexpensively and easily mass produced.

Another object of the present invention is to mount and couple the single-phase coreless stator armature on the stator armature supporter in one touch form without using a screw fixing means. The DC single-phase brushless axial fan motor can be mass produced easily.

[Means for achieving the task]

SUMMARY OF THE INVENTION An object of the present invention is to project a stator armature support by protruding in the direction of the field magnet to form a cavity for accommodating a drive circuit in the lower portion of the armature coil mounting substrate in the motor excretion portion provided in the central portion of the venturi case of the axial fan motor. And a magnetic phase projection for staging reluctance torque generation and a single-phase coreless stator armature positioning for the stator armature support head are formed by means of defecation, and the magnetic projection is formed on the armature coil mounting substrate. A single phase coreless stator armature is positioned and disposed on the stator armature support column by coupling to a coupling part such as a hole, and the like, and the armature coil on the armature coil mounting substrate is provided with the magnetic field projection from the dead point position. 1/2 stimulus spaced apart It was placed to be located at a position within the magnetic material above for the projections can be achieved by the field magnet to generate a reluctance torque for the dead point escape to avoid constraining the dead point position.

Another problem is that when the single-phase coreless stator armature is press-fitted from the upward direction to the motor excretion part and disposed on the stator armature support column, the armature coil mounting substrate is coupled against the elasticity. It is achievable by forming a hook and engaging the single-phase coreless stator armature on the stator armature support by the hook.

[Action]

Perforations 20 and printed circuit boards formed in the stator yoke 6 by positioning and mounting the single-phase coreless stator armature 7 on the stator armature support column 32 formed in the motor excretion unit 13 ( Magnetic rods (23) used as the magnetic projections for single-point coreless stator armature positioning and for the dead-point escape reluctance torque provided in the head of the stator armature support (32) formed in the perforations (25). ).

Since the single-phase coreless stator armature 7 is rotated and stopped by the magnetic rods 23 inserted into the through holes 20 and 25, the single-phase coreless stator armature 7 is positioned at a position determined by the magnetic rods 23, In addition, since there is an upper surface of the stator armature support column 32 at the lower position of the magnetic rod 23, the single-phase coreless stator armature 7 can be positioned and mounted on this upper surface.

At this time, since the hook 41 is formed in the outer peripheral part of the motor excretion part 13, when the single-phase coreless stator armature 7 is press-fitted toward the upper surface of the stator armature support column 32 from an upward direction, the said hook ( The engaging cutouts 44 and 45 formed in the stator yoke 6 and the printed circuit board 21 are lowered against the elasticity of the engaging projection 43 of the 41 and the hook 41 is lowered. Since the engaging recess 42 enters and engages, the single-phase coreless stator armature 7 can be held in a position positioned on the upper surface of the stator armature support column 32.

The armature coils 9-1 and 9-2 on the stator yoke 6 have the magnetic rod 23 from the dead centers 3-1 and 3-2, that is, the armature coils 9-1, Rotation direction of the field magnet 5 by the angle of about a quarter of the magnetic pole width of the field magnet 5 from the position of the effective conductor portion 9a contributing to the generation torque of (9-2) (arrow A in FIG. 1). Direction, which is located at a position spaced apart from the direction indicated by the direction of rotation, so that the magnetic field magnets 23 are not confined to the dead point position by the magnetic rod 23. It is possible to generate a torque torque (reluctance curve) 4 by the magnetic rod 32.

Therefore, at the time of non-energization, the field magnet 5 is attracted to the magnetic rod 23 magnetically and is stopped by a magnetically movable position. For this reason, since the magnetoelectric conversion element 30 detects the pole of the N pole or the S pole of the field magnet 5 at the time of energization to armature coils 9-1 and 9-2, for example, When the N pole is detected, a current in a predetermined direction flows through the armature coils 9-1 and 9-2 by the driving circuit (IC31 for the driving circuit), and therefore, in the predetermined direction (arrow A direction). The field magnet 5 is automatically rotated. If the field magnet 5 rotates in a predetermined direction, the armature coils 9-1 and 9-2 generate maximum starting torque, and further rotate in the same direction. When the field magnet 5 rotates and the rotation conversion element 30 detects the magnetic pole of the S pole of the field magnet 5, the armature coil 9-1 is driven by a drive circuit (drive IC IC 31). (9-2) flows in the reverse direction, and the magnet 5 is rotated by obtaining the rotational torque in the predetermined direction.

While repeating the above operation, the DC single-phase brushless axial fan motor 8 continuously rotates. Since the magnetic rod 23 is disposed at an angular position spaced apart from the armature coils 9-1 and 9-2 by about a quarter of the magnetic pole width of the field magnet 5, it is shown in FIG. As described above, since it is possible to obtain reluctance torque (reluctance torque curve 4) for dead center escape at the most preferable position, the combined torque curve 2 synthesized with the electromagnetic torque curve 1 is applied to the entire rotation angle region. Since it becomes a curve that slides almost constant over, that is, it is possible to obtain an ideal and surely self-directing DC single-phase brushless axial fan motor 8 which is capable of obtaining a rotation torque of almost constant intensity over the entire rotation angle region. .

In the above case, since there is a magnetic rod 23 which protrudes on the upper surface of the armature support column 32 and is embedded in advance, the single-phase coreless stator armature is mounted on the stator armature support column using a magnetic screw as in the prior art. Even without screwing, the single-phase coreless stator armature 7 can be mounted and fixed on the upper surface of the stator armature support column 32 very easily. In addition, since the magnetic rod 23 is projected on the upper surface of the stator armature support column 32 so as to have a predetermined height in advance, it is possible to always obtain a dead point escape reluctance torque of a constant size, and the occurrence of defective products It is possible to produce a low-cost, DC-phase single-phase brushless axial fan motor 8 of low quality and easily.

[Examples of the Invention]

1 is an exploded perspective view of an axial void type (disc) direct current brushless axial fan motor 8 showing an embodiment of the present invention, and FIG. 2 is a longitudinal sectional view of the fan motor 8 of FIG. 3 is an enlarged perspective view of the motor excretion portion, FIG. 4 is a perspective view of the venturi case in which the single phase coreless stator armature is disposed on the motor excretion portion, and FIG. 5 is an armature coil 5-1 and an armature coil 9-1 having a single phase arrangement, The developed view with 9-2) is shown.

Hereinafter, a DC single phase brushless axial fan motor 8 showing an embodiment of the present invention will be described with reference to FIGS.

A coreless structure supporting the venturi case 10, which is a stator, and the rotating fan 11, which is a rotor, is a rectangular DC axial air gap type single-phase brushless axial fan motor 8 having a thin axial thickness. It is an axial air-gap DC single-phase brushless axial fan motor. In this embodiment, the DC single-phase brushless axial fan motor 8 has a flat size of 40, 50, 60, 80, or 90 mm x 40, 50, 60, 80, or 90 mm in the size of the plane. It is a small and lightweight flat structure of extremely thin thickness having a thickness of 10 mm or 20 mm in the direction.

The fan motor 8 extends radially inward in the inner circumference of the venturi case 10 supporting the recessed portion thereof, and connects the motor excretion portion 13 connected to the stay 12 integrally formed. It is formed integrally with resin in the center part. Thereby, the wind blown by the impeller 14 of the rotating fan 11 to the outer periphery of the motor excretion part 13 of the bottom part of the venturi case 10 is made to pass downward in the axial direction. A wind through hole 15 is formed between the stays 12 and 12.

The rotating fan 11 has a field magnet 5 provided through an annular rotor yoke 26 so that the magnetic poles at the intersection N pole and the S pole are 90 degrees in mechanical angle so that adjacent magnetic poles become different poles. It is a 4-pole flat toroidal shape having a magnetizing width of.

An axial housing 16 extending in the axial direction is integrally formed with the motor excretion part 13 (venturi case 10) by resin at the center of the motor excretion part 13, and the bearing housing 16 is formed. Ball bearing 17 at the upper end of the shaft) and a sliding bearing 18 at the lower end thereof. The rotating shaft 19 fixed to the rotating fan 11 can be freely rotated to rotate the shaft. 11) is made rotatable.

The rotating fan 11 is formed of a single piece by resin other than the field magnet 5, the rotation shaft 19 and the rotor yoke 26, and the field magnet 5, the rotation shaft 19 and the rotor yoke 26 are It is integrated by resin.

On top of that, the rotary fan 11 is designed and arranged such that its center is located at the ball bearing 17 at the top of the bearing housing 16. Therefore, the ball bearing 17 is installed on the bearing housing 16 to support the center of the rotating fan 11 with the ball bearing 17, and the cheap sliding bearing 18 is located at the lower end of the bearing housing 16. ), And the sliding bearing 18 restricts the rotation shaft 19 from falling over a predetermined angle in the radial direction.

By doing in this way, it is sufficient not to use two expensive ball bearings 17 but only one use, and it is possible to respond to one of the expensive ball bearings 17 by the sliding bearings 18 of low price. Thus, the same life as in the case where two ball bearings 17 are used can be obtained.

The stator armature support column 32 is integrally formed in the motor excretion section 13 by extending upward in the axial direction at two positions of 180 ° symmetry. As described later, the stator armature support 32 is fixed on the stator armature supporter 32 by positioning the single-phase coreless stator armature 7 at a predetermined position and then excreted. On the upper surface of the motor), a hook 41 is formed to protrude and be formed at the same time by installing a magnetic rod 23, such as an iron rod, which is used as a magnetic material for positioning dead-reluctance torque generation and single-phase coreless stator armature positioning. It is formed in the outer peripheral part of 13).

The length of the magnetic rod 23 protruding from the upper surface of the stator armature support column 32 is longer than the thickness of the stator yoke 6 and the printed board 21 as shown in FIGS.

When the magnetic rod 23 is integrally molded with resin by the mold, the venturi case 10 (including the motor excrement part 13 and the stator armature support column 32) is mounted at a predetermined position of the mold, and the venturi is formed. When the case 10 is molded, it is preferable to integrate the upper surface of the stator armature support column 32 and to generate a magnetically-operated reluctance turnstock of a more uniform size. Although the height of the stator armature support column 32 is depicted long in the figure, it is in the air gap between the motor excretion part 13 and the printed board 21, or the bottom surface of the printed board 21 and the motor excretion part ( Since the drive circuit IC 31 needs to be extended between the bottom surfaces of 13) so that it can be accommodated, the height is 1 to several millimeters in length. The length of the magnetic rod 23 is also 1 to several millimeters in length.

Although the outer periphery of the motor excretion part 13 is formed slightly upward in the figure, the extension length is 1 to several millimeters, and the outer periphery of the motor excretion part 13 is located at two positions of 180 ° symmetry. The hook 41 is integrally formed with resin by extending upward in the axial direction. The hook 41 is formed at the outer circumferential position of the motor excretion portion 13 capable of pressing the stator yoke 6 or the like constituting the single-phase coreless stator armature 7. The hook 41 is integrally formed when the venturi case 10 is resin-molded, and as shown in the drawing, coupling cutouts 44 and 45 formed of the stator yoke 6 and the printed board 21. Coupling concave portion 42 of the base bite to fit snugly and the engaging projection 43 on the arc of the tip portion is formed. In order to heighten the elasticity of the hook 41, the groove | channel, such as a split, etc. may be formed in the motor excretion part of both sides of the hook 41, for example.

In addition, as shown in FIG. 1, the coupling recess grooves 44 and 45 are formed at the outer circumferences of the stator yoke 6 and the printed circuit board 21 to prevent rotation of the single-phase coreless stator armature 1 and the hook ( The single-phase coreless stator armature 7 with respect to 41 is facilitated.

In the present embodiment, the single-phase coreless stator armature 7 has two coreless armature coils 9-1 and 9-2 in phase on the stator yoke 6 whose surface is insulated ( Exposed in a single-phase arrangement so as to enable frostbite conduction.

The coreless armature coils 9-1 and 9-2 have an effect of contributing to the generated torque extending in the radial direction in order to form a highly efficient DC-axis air gap type single-phase brushless axial fan motor 8. The opening angle between the body parts 9a and 9b is equal to the opening width of the magnetic field magnet 5, i.e., π (π is an angle of 180 degrees in the electric angle. Since 4 poles are 4 poles, the machine angle in this case is of a concentric type formed with an opening width of 90 degrees). In addition, the armature coils 9-1 and 9-2 are formed on a double-sided adhesive tape or the like on the surface of the annular stator yoke 6, which is 180 degrees symmetrical in phase to form a single-phase coreless stator armature 7. It adheres by. Moreover, the conductor parts 9c and 9d in the circumferential direction of the armature coils 9-1 and 9-2 are conductor parts that contribute little to the generated torque.

Here, the coreless armature coil means not having an iron core (magnetic material) for winding the armature coils 9-1 and 9-2, that is, winding the conductor. In the core for winding the wire, the nonmagnetic material corresponds to the coreless armature coil referred to herein. That is, in this case, when the magnetic cores such as iron cores are energized by the armature coils 9-1 and 9-2, the magnetic cores have a function of acting as an N pole or an S pole, but they do not have such a function. Even if a simple magnetic body is not in the armature coils 9-1 and 9-2, such armature coils 9-1 and 9-2 belong to the coreless armature coil.

On the bottom surface of the stator yoke 6, an annular printed (wiring) substrate 21 is bonded with a double-sided adhesive tape or the like. On the bottom surface of the printed board 21, an IC 31 for a driving circuit (conduction control circuit) is disposed, and is electrically connected by a lead wiring pattern (not shown) formed on the printed board 21 and solder.

The magnetoelectric conversion element 30 such as a Hall element or a Hall IC used as the position detecting element is soldered to the upper surface of the printed circuit board 21 in the radial direction of the armature coil 9-1 or 9-2. The magnetoelectric conversion element 30 is housed and disposed in a perforation formed at a position of the stator yoke 6 facing the effective conductor portion 9a (or 9b) contributing to the generated generation torque.

When the annular printed circuit board 21 is bonded to the bottom surface of the stator yoke 6 with a double-sided adhesive tape or the like, the perforations 20 formed in the stator yoke 6 and the joining notches 44 and the printed board ( The through hole 25 and the engagement notch groove 45 formed in 21 are made to match.

Alternatively, after attaching the printed board 21 to the bottom surface of the stator yoke 6, the perforations 20 and 25 and the joining notches 44 and 45 are formed so as to be formed at the corresponding positions.

The single-phase coreless stator armature 7 formed as described above allows the perforations 20 and 25 to pass through the magnetic rod 23, and the stator armature is opposed to the elasticity of the engaging protrusion 43 of the hook 41. It press-fits into the upper surface of the support column 32, and fits in the engaging recess part 42 in the lower part of the hook 41 in the engaging notch grooves 44 and 45 formed in the stator yoke 6 and the printed board 21. As shown in FIG. The single-phase coreless stator armature 7 is coupled to and supported in the state positioned on the upper surface of the stator armature support column 32 to open the axial air gap 24 in which the single-phase coreless stator armature 7 extends in the radial direction. By rotating the surface magnet so as to face relative to the field magnet 5, the magnetoelectric conversion element 30 and the coreless stator armature 7 in the single phase arrangement are disposed in the field of the field magnet 5.

The magnetic rod 23 contributes to the generated torque of the armature coils 9-1 and 9-2 from the dead centers 3-1 and 3-2, for example, and is an arrow A from the effective conductor portion 9a. The stator armature is supported so as to be located in a position within a range of an angle (45 degrees) that is 1/2 the magnetic pole of the field magnet 5 in a direction opposite to the rotational direction of the field magnet 5 indicated by The support 32 is attached to the motor excretion unit 13.

The magnetic rod 23 obtains a reluctance torque for generating dead point escape torque for preventing the field magnet 5 from being confined to the dead spots 3-1 and 3-2.

In a preferred embodiment of the present invention, the magnetic rod 23 is provided from the effective conductor portion 9a which contributes to the generated torque of the armature coils 9-1 and 9-2 so as not to cancel the dead-point escape reluctance torque. Half arrow 180 ° to the motor excretion part 13, which is circumferentially displaced by an angle of about one quarter (22.5 degrees electrical angle (π / 4 = 46 degrees) in the machine angle) toward the A direction. In the upper surface of the stator armature support column 32 formed at two locations.

That is, the armature coils 9-1 and 9-2 are in the opposite direction to the rotation direction of the field magnet 5 from the position of the through hole 20 for passing through the magnetic rod 23 formed in the stator yoke 6. It is arranged in the single phase on the stator yoke 6 such that the effective conductor portion 9a or 9b is positioned at a position shifted radially by an angle of about one quarter of the width toward the direction A of the arrow.

The reason why the magnetic rod 23 is installed at 24 positions symmetrical by 180 degrees is that the magnetic field magnet 5 can be rotated automatically by only installing at one position, but the magnetic rod 23 and the magnetic field magnet are installed. This is to achieve stable balance (balance) with the magnetic attraction force according to (5), and to allow the field magnet 5 (rotating fan 11) to slip and rotate at the same time.

When the magnetic rod 23 is formed at the above position, as shown in the correspondence relationship between the field magnet 5 and the armature coils 9-1 and 9-2, which are indicated by dotted lines in FIG. The field magnet 5 stops at a position where the magnetic rod 23 is magnetically balanced with the magnetic pole center of the N pole or the S pole of the field magnet 5 in question.

Here, the effective conductor portion 9a or 9b of the armature coils 9-1 and 9-2 is positioned at a position shifted in the circumferential direction indicated by the arrow A direction by the angle of the quarter pole from the magnetic rod 23. Since it is arrange | positioned so that it may be located, the rotation conversion element 30 can detect the magnetic pole of the N pole or S pole of the field magnet 5 certainly. That is, since the magnetoelectric conversion element 30 does not oppose dead points 3-1 and 3-2, an output signal is obtained from the magnetoelectric conversion element 30. Based on this signal, when the armature coils 9-1 and 9-2 are energized in a predetermined direction by the driving circuit IC 31, the armature coils 9-1 and 9-2 are supplied. It is possible to obtain the rotation torque in the direction of arrow A, and it is possible to rotate the field magnet 5 in the direction of arrow A and to rotate continuously.

The position where the magnetic rod 23 is formed is an angle of one quarter magnetic pole from the position at which the maximum torque of the electromagnetic torque curve 2 is obtained so as to be clear from the curves 1, 2, and 4 of FIG. From the position spaced in the circumferential direction toward the direction of the half arrow A by (22.5 degrees at the machine angle), the reluctance torque for dead point escape by the magnetic rod 23 is generated, and is disposed at the position where the reluctance torque curve 4 is obtained. In this embodiment, the magnetic rod 23 is formed at a position that meets such conditions.

Moreover, the center part of the mountain of the electromagnetic torque curve 1 obtained by energizing the armature coils 9-1 and 9-2 is the position where the largest electromagnetic torque is obtained, and this part is the armature coil 9 -1) in the effective conductor portion 9a or 9b which contributes to the generated torque of (9-2).

When the reluctance torque for dead-spot escape is generated in this part 9a or 9b, in addition to the loss at the time of operation, it is also lost at the position extremely close to the dead centers (3-1) and (3-2) positions. There is a loss, the DC single-phase brushless axial fan motor 8 may not be self-moving, and the DC single-phase brushless axial fan motor 8 is inefficient. The rod 23 is formed.

5 is an exploded view of the field magnet 5 and the armature coils 9-1 and 9-2 in a single phase arrangement, and the armature coils 9-1 and 9-2 are conductor portions 9a which contribute to the generated torque. ) And (9b) are each formed in the angular width of the magnetic field magnet (5 degrees) (90 degrees for the mechanical angle, 180 degrees for the electrical angle) of the field magnet. It becomes clear that it is excreted.

The terminal of the conductor portion 9a, which contributes to one of the generated torques of the armature coil 9-1, is a semiconductor stop value (drive circuit, current device) constituted by two drive circuit ICs 31. 28) is electrically connected to the connection point of the collector circuit of the PNP-type transistor 29 and the collector circuit of the NPN-type transistor 34. The terminals of the effective conductor portion 9b contributing to the other generated torque of the armature coil 9-2 are the collector circuit of the PNP transistor 35 in the semiconductor rectifier 28 and the collector circuit of the NPN transistor 36. It is electrically connected to the connection point with.

The terminal of the effective conductor portion 9b that contributes to the other generated torque of the armature coil 9-1 and the terminal of the conductor portion 9a that contributes to one generated torque of the armature coil 9-2 are electrically connected. You are connected.

The emitter circuits of the transistors 29 and 35 are electrically connected to each other, and are electrically connected to the positive (+) side power supply terminal 37 side.

The emitter circuits of the transistors 34 and 36 are electrically connected to each other, and are electrically connected to the negative (-) side power supply terminal 38 side. The base circuits of the transistors 29 and 36 are electrically connected to each other, and electrically connected to one output terminal 39-1 side of the magnetoelectric conversion element (in this case, a four-stage Hall element). The base circuits of the transistors 34 and 35 are electrically connected to each other and electrically connected to the other output terminal 39-1 side of the magnetoelectric conversion element 30.

In FIG. 5, the field magnet 5 in the position indicated by the dotted line is stable by electrically attracting and combining the magnetic rod 23 and the field magnet 5 at the time of no energization, and the field magnet 5 is stopped. Indicates the state. Although the position of the field magnet 5 is clear from the development view of FIG. 5, since the magnetoelectric conversion element 30 is in a state of detecting the magnetic pole of the N pole or the S pole of the field magnet 5, it is certainly a DC single phase. It shows that the brushless axial fan motor 8 can be magnetically operated.

Therefore, referring to FIG. 5, since the magnetoelectric conversion element 30 detects the magnetic pole of the N pole of the field magnet 5 indicated by the dotted line, the transistor 29 is connected through one output terminal 39-1. And 36, conducting the current in the direction of the arrow through the armature coils 9-1 and 9-2 to obtain the rotational torque in the direction of the arrow A, and rotating the field magnet 5 (rotating fan 11). Rotate in the direction of arrow A. When the field magnet 5 (rotating fan 11) rotates in the direction of arrow A by a quarter of the magnetic poles, the field magnets 9-1 and 9-2 are represented by solid lines in FIG. The maximum starting torque is generated opposite to (5). If the maximum starting torque is generated from the beginning, the efficiency will actually be poor due to the loss during starting.However, if the maximum magnetizing torque is generated after the field magnet 5 rotates by a quarter stimulus angle, It is possible to obtain an efficient DC brushless axial fan motor 8 without loss of time.

After the maximum starting torque is obtained, the magnetic field magnet 5 rotates, and this time, the magnetoelectric conversion element 30 detects the S-pole of the field magnet 5 and transmits the transistor through the other output terminal 39-2. When the electrical conduction of the 34 and 36 conducts, rotational torque in the direction of the arrow A is obtained when the reverse current flows through the armature coils 9-1 and 9-2. Therefore, the field magnet 5 (rotation fan 11 )] Rotates in the direction of arrow A. By repeating the above operation, the direct current single-phase brushless axial fan motor 8 rotates continuously by the electromagnetic torque and the reluctance torque for time escape.

Other Examples

In the above embodiment, an example in which two armature coils are used has been shown. However, if the single phase coreless stator armature can be formed, the number may be one or three or more. For example, in the case where the four-pole magnetic field magnet 5 is used, up to four armature coils 9 can be disposed in the in-phase position without overlapping each other.

In this case, the armature coil 9 may be formed in a shape such that the opening angle of each of the outer peripheral portions of the effective conductor portions 9a and 9b is set in the middle of the magnetic pole width of the magnetic field.

In addition, although the field magnet used four poles, two poles or six or more poles may be used. However, in the case of a small direct current brushless axial fan motor, the use of a two-pole field magnet makes it impossible to form an armature coil in an optimal shape, or to provide a small number of field magnets, or to use an eight-pole or more field magnet. Although a large number of armature coils can be provided, it is cumbersome to manufacture an armature coil when the motor diameter is small. Therefore, as in the above embodiment, it is preferable to use four-pole magnets.

Moreover, in the case of the small one-DC single-phase brushless axial fan motor, since the rotating fan is also small, sufficient torque can be obtained only by using two electric coils.

In addition, the hook supporting the single-phase coreless stator armature may be in the interior, not in the outer periphery of the motor excretion section, and in this case, a coupling part such as a perforation or a cut groove may be provided at the position where the hook is coupled to the stator yoke and the printed board. Further, the hook is not limited to the shape shown above, and the design is appropriately changed to the optimum shape according to the design specification.

The stator yoke may be abolished, or a single phase coreless stator armature using an iron (magnetic) substrate in which the stator yoke and the printed board are integrally formed.

According to the present invention, a single phase brushless axial fan motor can be used for self-driving by simply pressing the single-phase coreless stator armature on the upper surface of the stator armature supporter. Since it generates a reluctance torque, it is possible to easily and inexpensively mass-produce a DC-phase single-phase brushless axial fan motor with a small variation.

In addition, since it is possible to fix the single-phase coreless stator armature to the stator armature supporter with a stator armature holder at a fixed position very simply without the hassle, mass production is good, there are few defective products, and a certain quality DC single phase brush The lease axial fan motor can be produced easily and inexpensively.

Claims (2)

A magnetic field magnet having a pole (N is an integer of 1 or more) with a pole of the N pole and the S pole is installed in a rotating fan having an impeller that blows wind in the axial direction, and the field magnet and the axial gap are interposed. Protruding in the field magnet direction for forming a cavity for accommodating the drive circuit in the lower part of the armature coil mounting substrate, in the motor excretion portion provided in the center portion of the venturi case of the DC single-phase brushless axial fan motor made of opposing resin. In the DC single-phase brushless axial fan motor fixed to form a stator armature support column and mounted on n (n is an integer of 1 or more) ironless armature support column on the armature coil mounting substrate surface, the head of the stator armature support column Such as excretion of magnetic material projection for positioning single phase coreless stator armature positioning for reluctance torque generation for dead center escape By means of insertion or the like by coupling the magnetic body projection to a coupling part such as a hole formed in the armature coil mounting substrate, and positioning and disposing the single-phase coreless stator armature on the stator armature support column. The armature coil on the coil-mounted substrate is disposed so that the magnetic projection is located at a position within an angular range in which one-half magnetic pole of the field magnet is spaced from the dead point position so that the magnetic field projection is not constrained by the magnetic projection. DC single-phase brushless axial fan motor, characterized in that for generating a dead point escape reluctance torque. The armature coil mounting apparatus according to claim 1, wherein the single-phase coreless stator armature is pushed from the top into the motor excretion part to be disposed on the stator armature supporter when the single-phase coreless stator armature is disposed on the motor excrement part. And a single phase coreless stator armature coupled to the stator armature support column by the hook.