JPS6349094Y2 - - Google Patents

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Publication number
JPS6349094Y2
JPS6349094Y2 JP12644583U JP12644583U JPS6349094Y2 JP S6349094 Y2 JPS6349094 Y2 JP S6349094Y2 JP 12644583 U JP12644583 U JP 12644583U JP 12644583 U JP12644583 U JP 12644583U JP S6349094 Y2 JPS6349094 Y2 JP S6349094Y2
Authority
JP
Japan
Prior art keywords
magnet
inclined groove
shaft
yoke
coil
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.)
Expired
Application number
JP12644583U
Other languages
Japanese (ja)
Other versions
JPS6034767U (en
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed filed Critical
Priority to JP12644583U priority Critical patent/JPS6034767U/en
Publication of JPS6034767U publication Critical patent/JPS6034767U/en
Application granted granted Critical
Publication of JPS6349094Y2 publication Critical patent/JPS6349094Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は自転車用発電ランプの負荷トルク調整
装置に関するものである。
[Detailed Description of the Invention] The present invention relates to a load torque adjusting device for a bicycle power generation lamp.

夜間での自転車の無灯火走行は危険防止のため
禁止されており、従来から自転車の車輪の回転に
よりタイヤと接触せしめた回転シヤフトのプーリ
ーによる発電ランプがある。しかし、従来の発電
ランプは自転車のスピードを上げていくと、初速
時が最大トルクで高速になるにつれ慣性により多
少は軽くなるが、発電ランプの負荷が増大し疲労
が増して無灯火になる。そして高速により高電流
がながれて電球が切れてしまうこととなる。すな
わち第7図に示すように、従来の自転車発電ラン
プ1はプーリー2に固着したシヤフト3を容器体
1内に軸受5を介して回動自在に挿入し、シヤフ
ト3の下端にマグネツト4をヨーク7の中央部に
位置させて固着して設けている。
Riding a bicycle without lights at night is prohibited to prevent danger, and conventionally there are power-generating lamps using a pulley on a rotating shaft that is brought into contact with the tire as the bicycle wheel rotates. However, as the speed of the bicycle increases, conventional power-generating lamps have maximum torque at initial speed, and as the speed increases, they become lighter due to inertia, but the load on the power-generating lamp increases and fatigue increases, causing it to go off. The high speed causes a high current to flow, causing the bulb to burn out. That is, as shown in FIG. 7, in the conventional bicycle power generation lamp 1, a shaft 3 fixed to a pulley 2 is rotatably inserted into the container body 1 via a bearing 5, and a magnet 4 is attached to the lower end of the shaft 3 by a yoke. It is located and fixed in the center of 7.

従つて、プーリー2が高速回転すると、それに
比例して高電流がながれ電球が切れる原因とな
る。なお6はコイル、8はターミナルである。
Therefore, when the pulley 2 rotates at high speed, a proportionally high current flows, causing the light bulb to burn out. Note that 6 is a coil and 8 is a terminal.

このためスポーツ用自転車の発電ランプにおい
ては、プーリーの外径を大きくするためのアタツ
チメントプーリーを付属し手動で作用させるのも
存するが、一般自転車用の発電ランプではアタツ
チメントプーリーを設けたものは見られない。
For this reason, some power-generating lamps for sports bicycles are equipped with an attachment pulley that is operated manually to increase the outside diameter of the pulley, but power-generating lamps for general bicycles are equipped with an attachment pulley. I can't see anything.

本考案は上記欠点を解消するためになされたも
ので、プーリーの径を変えることなく高速時にお
いても一定電流を確保することを目的としたもの
である。
The present invention was made to eliminate the above-mentioned drawbacks, and its purpose is to ensure a constant current even at high speeds without changing the diameter of the pulley.

本考案は発電用の容器体1の軸受5に、傾斜溝
12を周面に有する回転シヤフト3を回動自在に
軸受けせしめ、容器体1の内部に設けているコイ
ル6とヨーク7内方には、内部に設けた傾斜溝1
3を前記シヤフト3の傾斜溝12と互いにはめあ
うようにしたマグネツト14と、該マグネツト1
4に一定の付勢力を与えるスプリングとを設け、
前記マグネツト4は回転時に生じる回転シヤフト
3と平行な推力により前記ヨーク7との位置関係
を変更させ、コイル6への鎖交磁束数を変化させ
るようになしたことを特徴とする自転車用発電ラ
ンプの負荷トルク調整装置である。
In the present invention, a rotating shaft 3 having an inclined groove 12 on the circumferential surface is rotatably supported on a bearing 5 of a power generation container 1, and a coil 6 and a yoke 7 provided inside the container 1 are connected inwardly. is the inclined groove 1 provided inside.
a magnet 14 which is adapted to fit into the inclined groove 12 of the shaft 3, and the magnet 1;
4 is provided with a spring that applies a constant urging force,
A power generation lamp for a bicycle, characterized in that the magnet 4 changes its positional relationship with the yoke 7 by a thrust parallel to the rotating shaft 3 generated during rotation, and changes the number of interlinked magnetic fluxes to the coil 6. This is a load torque adjustment device.

以下に本考案の実施例を図面に基づいて説明す
る。
Embodiments of the present invention will be described below based on the drawings.

本考案は第3図において、発電用の容器体1
(従来例と同符号で示す。以下主構成部について
も同様とする。)の筒部aに設けた軸受5にプー
リー2を圧着又はナツト(図示せず。)で固着し
たシヤフト3を支承して回動自在に設け、このシ
ヤフト3には傾斜溝12を設ける。他方マグネツ
ト4には前記傾斜溝12と対応する内周傾斜溝1
3を設けて、このマグネツト4をシヤフト3に遊
嵌する。そしてマグネツト4をヨーク7の中央部
に位置させて(図中A点)、マグネツト4の下面
とシヤフト3の下端部17との間にシヤフト3で
ガイドされた下部スプリング9を設け、さらにマ
グネツト4の上面とシヤフト3の傾斜溝12に嵌
合して設けたストツパ11との間に上部スプリン
グ10を設けて、マグネツト4の上面及び下面を
上下のスプリング9,10で挟持する。6はコイ
ルで第5図に示すように容器体1の内法両側に設
ける。8はターミナルで、容器体1の外部に絶縁
固定されている。
The present invention is shown in Fig. 3.
(Denoted with the same reference numerals as the conventional example. The same applies to the main components hereinafter.) A shaft 3 is supported, with a pulley 2 crimped or fixed with a nut (not shown) on a bearing 5 provided in a cylindrical portion a. The shaft 3 is provided with an inclined groove 12 so as to be rotatable. On the other hand, the magnet 4 has an inner circumferential inclined groove 1 corresponding to the inclined groove 12.
3 is provided, and the magnet 4 is loosely fitted onto the shaft 3. Then, the magnet 4 is located at the center of the yoke 7 (point A in the figure), and a lower spring 9 guided by the shaft 3 is provided between the lower surface of the magnet 4 and the lower end 17 of the shaft 3. An upper spring 10 is provided between the upper surface and a stopper 11 fitted into the inclined groove 12 of the shaft 3, and the upper and lower surfaces of the magnet 4 are held between the upper and lower springs 9 and 10. Coils 6 are provided on both sides of the inner diameter of the container body 1, as shown in FIG. A terminal 8 is insulated and fixed to the outside of the container body 1.

なお、マグネツト4は後述する磁束量の変化割
合を更に強くするように第6図に示す円錐台形に
形成してもよい。また、傾斜溝の材質は摩擦抵抗
を減らす効果を出すため樹脂材を使用してもよ
い。
The magnet 4 may be formed into a truncated cone shape as shown in FIG. 6 so as to further increase the rate of change in the amount of magnetic flux, which will be described later. Further, the material of the inclined groove may be a resin material in order to reduce frictional resistance.

次に本考案の作用及び効果について説明する。 Next, the functions and effects of the present invention will be explained.

プーリー2は第1図に示すように自転車のタイ
ヤ16に当接せしめタイヤの回転に伴つて回転す
る。
As shown in FIG. 1, the pulley 2 is brought into contact with a bicycle tire 16 and rotates as the tire rotates.

第3図において低負荷トルク時のマグネツト4
は負荷トルクによる推力Fが少ないので自重及び
上部スプリング10の反力によりヨーク7の中央
部に位置するため(第3図A点)、マグネツト4
の磁束はヨーク7へ最大に流れ易くなり、従つて
磁束は最大に得られる。そして発生電圧は回転数
が低いながら得られるので、低速でも充分な照度
を確保することができる(第5図参照)。第6図
中14はランプ、15は導線である。
In Figure 3, magnet 4 at low load torque
Since the thrust force F caused by the load torque is small, the magnet 4 is located at the center of the yoke 7 due to its own weight and the reaction force of the upper spring 10 (point A in Fig. 3).
The magnetic flux easily flows to the yoke 7, and therefore the maximum magnetic flux can be obtained. Since the generated voltage can be obtained even at a low rotational speed, sufficient illuminance can be ensured even at low speeds (see FIG. 5). In FIG. 6, 14 is a lamp and 15 is a conductor.

第3図の状態で、シヤフト3が高回転で回転を
始めると、シヤフト3とマグネツト4との間に相
対的な回転が生じ、この回転によつて回転シヤフ
ト3と平行に生じる推力Fが増加し、これがマグ
ネツト4に加わる。そしてこの増加した推力Fが
自重及び上部スプリング10の反力に打ち勝ち、
マグネツト4は傾斜溝12及び傾斜溝13を介し
て、第3図A点から第2図B点へと移動する。
When the shaft 3 starts rotating at a high speed in the state shown in Fig. 3, a relative rotation occurs between the shaft 3 and the magnet 4, and this rotation increases the thrust force F generated parallel to the rotating shaft 3. And this will be added to magnet 4. This increased thrust F overcomes the own weight and the reaction force of the upper spring 10,
The magnet 4 moves from point A in FIG. 3 to point B in FIG. 2 via the inclined grooves 12 and 13.

この時マグネツト4から発する磁束とコイル6
との鎖交数は、マグネツト4が上方に移動するほ
ど減少し、シヤフト3の回転数が高まつても、発
生電圧は上がらない。
At this time, the magnetic flux emitted from the magnet 4 and the coil 6
The number of linkages with the magnet 4 decreases as the magnet 4 moves upward, and even if the rotational speed of the shaft 3 increases, the generated voltage does not increase.

次ぎに高速回転から低速回転に移行した場合に
は、マグネツト4の自重及び上部スプリング10
の反力が打ち勝ち、マグネツト4は傾斜溝12及
び傾斜溝13を介して下方に移動し、回転速度の
減少分を鎖交磁束数の増加により発電量を上昇さ
せる。従つて高回転時と、低回転時との発電量の
釣り合いをマグネツト4の移動により行わしめる
ように作用させている。
Next, when the rotation changes from high speed to low speed, the weight of the magnet 4 and the upper spring 10
The reaction force is overcome, and the magnet 4 moves downward through the inclined grooves 12 and 13, increasing the amount of power generated by increasing the number of interlinked magnetic fluxes to compensate for the decrease in rotational speed. Therefore, the movement of the magnet 4 acts to balance the amount of power generated during high rotation and low rotation.

上述のように本考案によれば、負荷トルクがシ
ヤフトとマグネツトとの間に生じた場合、このト
ルクの一部が推力となりマグネツトとヨークとの
位置関係を決めることによりヨークへの磁束量に
変化を与え、これが負荷トルクの調整作用をな
し、従来のように高速走行中に電球が切れるとい
うことはないのみならず、自転車走行用の労力も
軽減され無灯火乗車のおそれもなく夜間の安全乗
車を行なうことが出来る。また構造も簡単で安価
に製作出来る等の効果を有する。
As mentioned above, according to the present invention, when load torque is generated between the shaft and the magnet, a part of this torque becomes thrust and changes the amount of magnetic flux to the yoke by determining the positional relationship between the magnet and the yoke. This adjusts the load torque, which not only prevents the bulb from burning out while riding at high speeds like in the past, but also reduces the effort required to ride the bicycle and allows for safe riding at night without the risk of riding without a light. can be done. Further, the structure is simple and can be manufactured at low cost.

【図面の簡単な説明】[Brief explanation of the drawing]

図面は本考案の実施例を示すもので、第1図は
発電機の取付状態を示す正面図、第2図は高負荷
トルク時における本考案の断面図、第3図は低負
荷トルク時における同上の断面図、第4図は第3
図の横断面図、第5図は回路図、第6図はマグネ
ツトの他の実施例を示す断面図、第7図は従来品
の断面図である。 1は発電用の容器体、2はプーリー、3はシヤ
フト、4はマグネツト、5は軸受、6はコイル、
7はヨーク、8はターミナル、9は下部スプリン
グ、10は上部スプリング、11はストツパ、1
2は傾斜溝、13は内側傾斜溝、14はランプ、
15は導線、16はタイヤ、17は下端部、aは
筒部、Fは推力。
The drawings show an embodiment of the present invention. Fig. 1 is a front view showing the installed state of the generator, Fig. 2 is a sectional view of the invention at high load torque, and Fig. 3 is a cross-sectional view of the invention at low load torque. The sectional view of the same as above, Fig. 4 is the 3rd
5 is a circuit diagram, FIG. 6 is a sectional view showing another embodiment of the magnet, and FIG. 7 is a sectional view of a conventional product. 1 is a power generation container body, 2 is a pulley, 3 is a shaft, 4 is a magnet, 5 is a bearing, 6 is a coil,
7 is a yoke, 8 is a terminal, 9 is a lower spring, 10 is an upper spring, 11 is a stopper, 1
2 is an inclined groove, 13 is an inner inclined groove, 14 is a lamp,
15 is a conductor, 16 is a tire, 17 is a lower end, a is a cylinder, and F is a thrust force.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 発電用の容器体の軸受に、傾斜溝を周面に有す
る回転シヤフトを回動自在に軸受けせしめ、容器
体の内部に設けているコイルとヨーク内方には、
内部に設けた傾斜溝を前記シヤフトの傾斜溝と互
いにはめあうようにしたマグネツトと、該マグネ
ツトに一定の付勢力を与えるスプリングとを設
け、前記マグネツトは回転時に生じる回転シヤフ
トと平行な推力により前記ヨークとの位置関係を
変更させ、コイルへの鎖交磁束数を変化させるよ
うになしたことを特徴とする自転車用発電ランプ
の負荷トルク調整装置。
A rotating shaft having an inclined groove on the circumferential surface is rotatably supported on the bearing of the power generation container body, and a coil and a yoke provided inside the container body include:
A magnet is provided with an internally provided inclined groove that fits into the inclined groove of the shaft, and a spring that applies a constant biasing force to the magnet. A load torque adjusting device for a bicycle power generation lamp, characterized in that the positional relationship with the yoke is changed to change the number of magnetic flux linkages to the coil.
JP12644583U 1983-08-17 1983-08-17 Bicycle power generation lamp load torque adjustment device Granted JPS6034767U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12644583U JPS6034767U (en) 1983-08-17 1983-08-17 Bicycle power generation lamp load torque adjustment device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12644583U JPS6034767U (en) 1983-08-17 1983-08-17 Bicycle power generation lamp load torque adjustment device

Publications (2)

Publication Number Publication Date
JPS6034767U JPS6034767U (en) 1985-03-09
JPS6349094Y2 true JPS6349094Y2 (en) 1988-12-16

Family

ID=30287519

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12644583U Granted JPS6034767U (en) 1983-08-17 1983-08-17 Bicycle power generation lamp load torque adjustment device

Country Status (1)

Country Link
JP (1) JPS6034767U (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2005008865A1 (en) * 2003-07-18 2006-11-02 ヤマハ発動機株式会社 Rotating electric machine and electric vehicle including the rotating electric machine

Also Published As

Publication number Publication date
JPS6034767U (en) 1985-03-09

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