JPS6152181A - Fan motor - Google Patents
Fan motorInfo
- Publication number
- JPS6152181A JPS6152181A JP59172501A JP17250184A JPS6152181A JP S6152181 A JPS6152181 A JP S6152181A JP 59172501 A JP59172501 A JP 59172501A JP 17250184 A JP17250184 A JP 17250184A JP S6152181 A JPS6152181 A JP S6152181A
- Authority
- JP
- Japan
- Prior art keywords
- magnet
- fan
- yoke
- magnetic flux
- housing
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000004907 flux Effects 0.000 abstract description 9
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 description 7
- 238000010586 diagram Methods 0.000 description 4
- 230000003321 amplification Effects 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 210000004907 gland Anatomy 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 229920003002 synthetic resin Polymers 0.000 description 1
- 239000000057 synthetic resin Substances 0.000 description 1
Landscapes
- Structures Of Non-Positive Displacement Pumps (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Abstract
Description
【発明の詳細な説明】
例えば電子機器の冷却ファン等は極めて小型に形成しな
ければならない。しかし従来t!7アンとモータとを別
個に形成してそれらを直結するか、ある―は予め一体に
梠成した場合でも、ファンの内側にモータを配匝して勝
たから、モータのトルクを大きくするとその軸方向の長
さ・従って$1の厚みを極めて大きくしなければならな
かった。DETAILED DESCRIPTION OF THE INVENTION For example, cooling fans for electronic equipment must be made extremely small. However, conventionally t! 7. You can form the fan and the motor separately and connect them directly, or even if they are integrated in advance, it is possible to install the motor inside the fan, so if you increase the torque of the motor, the shaft The length in the direction and therefore the thickness of $1 had to be made extremely large.
このような装置を電子機器の筐体壁等に取付けると7ア
ンの周辺に利用されない大きな空間が形成される0従っ
て機器の実質的専有空間は1これをファンの装置Kよっ
て充分有効に縮小し得な一欠点があった0本発明はこの
ような欠点を除去して\特に電子機器の筐体壁等に取付
けた場合に1その周辺に利用し得ない熱井な空allを
生ずることなくファンの取付けによっ″′C機器の大き
さを有効に縮小することのできるファン、モータを提供
するものである。When such a device is attached to the wall of an electronic device's casing, a large unused space is created around the device. Therefore, the actual exclusive space of the device can be effectively reduced by the fan device K. The present invention eliminates these drawbacks, especially when it is attached to the wall of an electronic device's casing, etc. without creating an unusable empty space around it. To provide a fan and a motor that can effectively reduce the size of a device by installing a fan.
本発明は特許zn求のf@gVc記載したよう<% 7
アンの外周部に磁石を環状に取付けて〜その磁石の外側
血を周方向にお−て順次N極、S極、l(極・・・・・
となL〜この磁石の外側1c複数個の固定コイルを配列
すると共にコイルの外側Km状のヨークを設けである。The present invention is as described in patent zn f@gVc <% 7
Attach a magnet in a ring shape to the outer periphery of the magnet.The outer part of the magnet is connected in the circumferential direction to the N pole, S pole, L (pole...
A plurality of fixed coils are arranged on the outer side 1c of this magnet, and a Km-shaped yoke is provided on the outer side of the coil.
従って前記H,Eの6極からヨークに通ずる磁力線がそ
の間のコイルと交叉するから、該コイルlC電流を流す
ことによって磁石1すなわちその内側のファンに回転力
が発生する0かつこの回転力で磁石が移動して磁束の方
向が反転すると、これと同時にコイルの電流が逆向きに
切換えらnるから同一方向の回転力が打続して・ファン
に連続回転が生ずる。かつ放射状の翼からなるファンの
外側に磁石を環状に配列して、更にその外側に複数個の
固定コイルと環状のヨークとを同軸的に配直しであるか
ら、モータの借成に必要な容積を一定とすると、その周
方向の長さの増大により軸方向の長さか極めて小さくな
って、ファンとその駆動モータとを極めて薄い板状の一
体のyA儂として6成することができる0従ってそのフ
ァン・モータを例えば電子vA器の筐体壁等に取付ける
ときは、周辺に無用の空間が生ずることなく・装置肩ひ
めて小型に形成し得ると共に筐体の内部を有効に冷却す
ることができる。Therefore, the lines of magnetic force leading from the six poles H and E to the yoke intersect with the coils between them, so that by passing current through the coil IC, a rotational force is generated in the magnet 1, that is, the fan inside it. When the magnetic flux moves and the direction of the magnetic flux is reversed, the current in the coil is switched in the opposite direction at the same time, so the rotational force in the same direction continues, causing the fan to rotate continuously. In addition, magnets are arranged in a ring on the outside of the fan consisting of radial blades, and multiple fixed coils and an annular yoke are arranged coaxially on the outside, so the volume required for the motor is reduced. Assuming that is constant, as the length in the circumferential direction increases, the length in the axial direction becomes extremely small, and the fan and its drive motor can be constructed as an extremely thin plate-like integrated YA member. For example, when the fan motor is attached to the wall of the case of an electronic VA device, unnecessary space is not created around it, the device can be packed into a compact size, and the inside of the case can be effectively cooled. .
第1図、第2r2?Iは本発明の売蔵例で、第2図は縦
断面図、第1図は第2図のA−AUID図である。Figure 1, 2r2? I is a storage example of the present invention, FIG. 2 is a longitudinal sectional view, and FIG. 1 is an A-AUID diagram of FIG. 2.
このように中心に回転軸1を固定した合成何脂等の円筒
体2にΩ3,3.、、、、を放射状に取付けて、そる。In this way, a cylindrical body 2 made of synthetic resin or the like with the rotating shaft 1 fixed at the center is connected to a cylindrical body 2 of Ω3, 3. Attach , , , radially and warp.
磁石4の外側面は第1図に)rおよびSの記号で示した
ようK例えば60度間隔で交互にN極とS極とを形成し
である口また底面に複数個の窓5を形広した有底円筒状
の筐体6における側壁の内側に環状のヨーク7を取付け
て更にその内側に例えば4個の固定コイル8.8.、、
−、をその軸線が前記回転軸1と直交するように配列し
、筐体6の底面の中心に軸受?を設けである。更に一辺
の長さが筐体6の径と等しいほぼ正方形の基台10の中
心忙軸受11を取付けてその周辺1c複数個の窓12を
形広し、かつ四隅に取付用のボルト孔13を設けである
。すなわちこの基台10の軸受に前記沢3,3・・・・
・を有するファンの軸1を嵌合し、更にコイル8,8・
・・・・すを取付けた筐体6を嵌合してその軸受9に上
記軸1の他端を嵌合することにより一体に組立てたもの
で、ヨーク7の内研には適当な位置に磁束検出用のホー
ル素子14.および15を取付けである。The outer surface of the magnet 4 has N and S poles alternately formed at intervals of 60 degrees, for example, as shown by the symbols r and S in Fig. 1, and a plurality of windows 5 are formed on the opening and bottom surface. An annular yoke 7 is attached to the inside of the side wall of the wide bottomed cylindrical housing 6, and furthermore, for example, four fixed coils 8.8. ,,
- are arranged so that their axes are perpendicular to the rotating shaft 1, and the bearings are placed at the center of the bottom surface of the housing 6. This is provided. Furthermore, a center bearing 11 is attached to a substantially square base 10 whose length on one side is equal to the diameter of the housing 6, a plurality of windows 12 are widened around the base 10, and bolt holes 13 for mounting are provided at the four corners. It is a provision. That is, the bearings of this base 10 are provided with the grooves 3, 3, . . .
・Fit the fan shaft 1 with the coils 8, 8・
It is assembled into one piece by fitting the housing 6 with the yoke 7 attached, and fitting the other end of the shaft 1 into the bearing 9. Hall element 14 for magnetic flux detection. and 15 are installations.
第3図は第1図の一部を拡大した図で、固定コイル8の
1つに記号a、hで示したような極性の電流が流nSま
た環状の磁石番の外側面が図にN、Sで示したように磁
化されているものとすると1その磁石4しヨークマとを
介して矢印を附した細腺a、dで示したような磁束が発
生するから・回転自在に保持さi’tだ磁石4に矢印p
のような回転力が加わる。また第4図はホール素子14
によってその両側の2つのコイル8,8の電流の方向を
切換える回路の一例で、直流電源16に上記ホール素子
とスイッチングトランジスタ17m1[l、19+20
3dよび増幅用トランジスタ21.32 等を接続し、
かつコイル8には逆起電圧除去用のダイオード23を接
続しである。すなわち第3図のホール素子14には細線
eのような磁束が力Uわるから、出力端子りから例えば
正電圧の信号が送出されて1 トランジスタ21が遮断
し、22が導通する0従つ【トランジスタ18.I9が
導通、17#20が遮断してコイA/ a、a Kは矢
印!で示したような極性の電流が流れ、この電流で前述
のように磁石番に矢印pの方向の回転力が発生する。ま
たその回転力で磁石本が回転して第3図におけるN極の
位置かS極になったものとすると、ホール素子14)t
c加わる磁束の方向も反転して1端子りかも負の信鳴が
送出されるために・ トランジスタ21が導通、22が
遮断の状態となる0このためトランジスタ17および2
0が導通、1B、19が遮断となってニイル8,8には
矢印Iと逆向きの電流が流れるから、磁石4に加わる回
転力は矢印p方向を維持する。FIG. 3 is an enlarged view of a part of FIG. 1, in which a current with the polarity shown by symbols a and h flows through one of the fixed coils 8, and the outer surface of the annular magnet number is shown in the figure. , if it is magnetized as shown by S, magnetic flux as shown by the thin glands a and d with arrows will be generated through the magnet 4 and the yoke.・It is held rotatably. 't.Arrow p to magnet 4
A rotational force such as is applied. In addition, FIG. 4 shows the Hall element 14.
This is an example of a circuit that switches the direction of the current in the two coils 8, 8 on both sides of the coil.
Connect 3d and amplification transistors 21, 32, etc.
Further, a diode 23 for removing back electromotive force is connected to the coil 8. In other words, since a magnetic flux such as the thin wire e acts on the Hall element 14 in FIG. Transistor 18. I9 conducts, 17#20 cuts off, and Koi A/ a, a K is an arrow! A current with the polarity shown flows, and this current generates a rotational force in the direction of the arrow p in the magnet number as described above. Also, assuming that the magnet book rotates due to the rotational force and becomes the north pole position in FIG. 3 or the south pole position, the Hall element 14) t
Since the direction of the applied magnetic flux is also reversed and a negative signal is sent from one terminal, transistor 21 becomes conductive and transistor 22 is cut off. Therefore, transistors 17 and 2
0 is conductive, 1B and 19 are disconnected, and current flows in the direction opposite to arrow I through the coils 8 and 8, so the rotational force applied to magnet 4 maintains the direction of arrow P.
また第5図は上記実flIi例の各回転位IVtにおい
て各部に発生する回転力とその方向を示した図である・
すなわち円環状の永久磁石4がコイル8,8.。Furthermore, FIG. 5 is a diagram showing the rotational force generated in each part and its direction at each rotational position IVt of the above-mentioned actual flIi example.
That is, the annular permanent magnet 4 connects the coils 8, 8 . .
・・およびホール素子14.15に対して(αンのよう
を位置にあるものとすると、この磁石4の各部にはそれ
ぞれ矢印で示したような方向および大きさの回転力が発
生する。すなわち磁石4には大きな右回転トルクが発生
して(りの位置へ移動するがこの位置にお(ρてもは4
丁同程度の右回J広トルクが発生して(りの位置へ移動
する。この位置では磁石の一部に左回転トルクが発生し
て、右回転トルクの一部は相殺されるが、′fxお歿り
の右回転トルクによって回転なり続する。しかしくりの
位置を通遇する。とホール素子14.15に加わる磁束
の方向が反転するために、前記第4図のような回路によ
ってコイル8,8.、、、、の電流の極性も反転してC
d)の状態となる。従って磁石の各部には矢印で示した
ようなトルクが発生して−これを綜合すると右回転トル
クが残留するから、磁石+1−2.(”)(1)のよう
に右回転を継続する。このように第1図、第2図の実施
例は60度回転する毎にその間で1個所だけ右回転トル
クの消滅する吋間が存在する口しかし大部分の範囲では
ほぼ一定の大金な右回転トルクが発生して回転なIf続
する0また上述のようにトルクが0となる位置で回転が
停止した場合は、つぎの起動がIII難になる口しかし
ファン・モータは起動に必要なトルクが極めて小さ−と
共にトルクが零となる範囲が第5図につ−て説明したよ
うに極めて狭(へために僅かの振動等で容易に起動する
。...and the Hall elements 14, 15 (assuming that they are in the position α), a rotational force is generated in each part of the magnet 4 in the directions and magnitudes shown by the arrows. That is, A large clockwise rotation torque is generated in the magnet 4, and it moves to the position (ri), but at this position (ρ is no longer 4).
A clockwise rotation torque of the same degree as d is generated and the magnet moves to position ri. At this position, counterclockwise rotation torque is generated on a part of the magnet, and part of the clockwise rotation torque is canceled out, but fx continues to rotate due to the clockwise rotation torque.However, when the position of the hole is changed, the direction of the magnetic flux applied to the Hall elements 14 and 15 is reversed, so the coil is rotated by the circuit shown in FIG. The polarity of the current of 8, 8., , , is also reversed and C
The state d) is reached. Therefore, torques as shown by the arrows are generated in each part of the magnet, and when these are combined, a clockwise rotation torque remains, so the magnet +1-2. ('') Continuing clockwise rotation as shown in (1).In this way, in the embodiments shown in Figures 1 and 2, there is only one gap in between where the clockwise rotation torque disappears every 60 degrees of rotation. However, in most of the range, a large amount of clockwise rotation torque is generated that is almost constant and the rotation continues to 0.Also, as mentioned above, if the rotation stops at the position where the torque becomes 0, the next startup will be However, the torque required to start a fan motor is extremely small, and the range in which the torque reaches zero is extremely narrow (as explained in Figure 5). to start.
また必要に応じては弱い永久磁石等を用いてモータの停
と位置を規定することにより、次の起動を常に確実に行
わせることもできる。なお五記実施例はコイル、NFJ
に対して磁極の数を6としたものことができる。Further, if necessary, by using a weak permanent magnet or the like to define the stop and position of the motor, the next start can always be performed reliably. In addition, the five embodiments are coils and NFJs.
In contrast, the number of magnetic poles can be set to six.
図面は本発明の一実施例で、第1図は第2図の人−A断
面図、第2図は縦断面図、第3図は第1図の7部を拡大
した図、第4図ii電気回路の一部を示した図、第5図
は各回転角位置において磁石の各部に発生するトルクを
示した図である口なおF?[お−て、lは回転軸、3は
翼、4は永久磁石〜7はヨーク、8はコイル、14.1
5はホール素子である。 ゛
イ、5′″MThe drawings show one embodiment of the present invention; FIG. 1 is a sectional view taken along the line A in FIG. 2, FIG. 2 is a vertical sectional view, FIG. 3 is an enlarged view of part 7 of FIG. 1, and FIG. ii. A diagram showing a part of the electric circuit. Figure 5 is a diagram showing the torque generated in each part of the magnet at each rotation angle position. [Here, l is the rotating shaft, 3 is the blade, 4 is the permanent magnet ~ 7 is the yoke, 8 is the coil, 14.1
5 is a Hall element.゛I, 5′″M
Claims (1)
上記翼の外周部に、外側面の周方向にN極とS極とを交
互に形成した環状の磁石を固定して、前記回転軸と直角
な方向の軸線を有する複数個の固定コイルを上記環状磁
石の外側へ環状に配列し、かつその外側に環状のヨーク
を配置すると共に上記各コイルとその電源との間に前記
フアンの回転に伴つてこのフアンに常に同一方向の回転
力が加わるようにコイル電流を切換える回路を設けたこ
とを特徴とするフアン・モータAn annular magnet having N poles and S poles alternately formed in the circumferential direction of the outer surface is fixed to the outer periphery of the wing of a fan having radial wings formed around the rotating shaft, and the magnet is perpendicular to the rotating shaft. A plurality of fixed coils having axes in the same direction are arranged in a ring on the outside of the annular magnet, and an annular yoke is arranged on the outside of the magnet. A fan motor characterized by being equipped with a circuit that switches the coil current so that a rotational force is always applied in the same direction to the lever fan.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59172501A JPS6152181A (en) | 1984-08-21 | 1984-08-21 | Fan motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59172501A JPS6152181A (en) | 1984-08-21 | 1984-08-21 | Fan motor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6152181A true JPS6152181A (en) | 1986-03-14 |
Family
ID=15943139
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59172501A Pending JPS6152181A (en) | 1984-08-21 | 1984-08-21 | Fan motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6152181A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000022716A1 (en) * | 1998-10-14 | 2000-04-20 | Air Concepts, Inc. | Fan |
US6249071B1 (en) * | 1998-10-14 | 2001-06-19 | Advanced Rotary Systems Llc | Rotor drive motor with u-shaped stator cores |
JP2007127013A (en) * | 2005-11-02 | 2007-05-24 | Denso Corp | Fuel pump |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59139848A (en) * | 1983-01-31 | 1984-08-10 | Takahashi Yoshiteru | Dc motor with double armature coils formed with armature of reduced thickness |
-
1984
- 1984-08-21 JP JP59172501A patent/JPS6152181A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59139848A (en) * | 1983-01-31 | 1984-08-10 | Takahashi Yoshiteru | Dc motor with double armature coils formed with armature of reduced thickness |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2000022716A1 (en) * | 1998-10-14 | 2000-04-20 | Air Concepts, Inc. | Fan |
US6249071B1 (en) * | 1998-10-14 | 2001-06-19 | Advanced Rotary Systems Llc | Rotor drive motor with u-shaped stator cores |
JP2007127013A (en) * | 2005-11-02 | 2007-05-24 | Denso Corp | Fuel pump |
JP4696855B2 (en) * | 2005-11-02 | 2011-06-08 | 株式会社デンソー | Fuel pump |
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