JP3572396B2 - Bar magnet - Google Patents

Bar magnet Download PDF

Info

Publication number
JP3572396B2
JP3572396B2 JP2000103793A JP2000103793A JP3572396B2 JP 3572396 B2 JP3572396 B2 JP 3572396B2 JP 2000103793 A JP2000103793 A JP 2000103793A JP 2000103793 A JP2000103793 A JP 2000103793A JP 3572396 B2 JP3572396 B2 JP 3572396B2
Authority
JP
Japan
Prior art keywords
bar
shaped magnet
rod
magnetic
magnet
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 - Fee Related
Application number
JP2000103793A
Other languages
Japanese (ja)
Other versions
JP2001291613A (en
Inventor
浩志 米田
正弘 栗田
康男 國府田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nissan Motor Co Ltd
Original Assignee
Nissan Motor Co Ltd
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 by Nissan Motor Co Ltd filed Critical Nissan Motor Co Ltd
Priority to JP2000103793A priority Critical patent/JP3572396B2/en
Publication of JP2001291613A publication Critical patent/JP2001291613A/en
Application granted granted Critical
Publication of JP3572396B2 publication Critical patent/JP3572396B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)
  • Valve Device For Special Equipments (AREA)
  • Magnetically Actuated Valves (AREA)
  • Electromagnets (AREA)

Description

【0001】
【発明の属する技術分野】
本発明は、磁界形成用の棒状磁石に係り、特に、変位計測用に好適な磁界形成用の棒状磁石に関する。
【0002】
【従来の技術】
変位計測方法の一種に、両端を磁極とする棒状磁石とホール素子などの磁気検出素子を用い、棒状磁石による磁界の強度測定により、棒状磁石と磁気検出素子の相互位置変位を計測する方法があり、例えば特開平6−180242号公報では、流量計測装置に適用した例について開示している。
【0003】
ところで、近年、吸気弁と排気弁を電磁的に開閉制御する方式のエンジン、すなわち電子制御吸排気弁システムが実用化されているが、図3は、このようなシステムに使用される電磁式吸排気弁(吸気弁又は排気弁)駆動システムの一例で、この例は、図示のように、磁性材料で作られている可動子(アマチュア)1と、2個の電磁石2、3、それにスプリング4からなる電磁アクチュエータを用い、可動子1の駆動軸5に吸排気弁6を取付けてある。
【0004】
そして、吸排気弁6を図の上方に動かすとき、つまり閉弁させるときは電磁石2に通電して可動子1を吸引し、下方に動かすとき、つまり開弁させるときは電磁石3に通電して可動子1を吸引するのであり、このとき、スプリング4は、図示されていない他のスプリングと共に、電磁石2、3に通電されていないとき、可動子1を中立位置に保持する働きをするものである。
【0005】
この場合、運転中での開弁タイミングと閉弁タイミングの独立した制御と、さらにはリフト量の制御が可能になる点が特徴的であるが、このためには、可動子1の駆動位置を正確に制御する必要があり、このためには、変位した位置を正しく検出する必要がある。
そこで、この図3の例では、図示のように、棒状の永久磁石、つまり棒状磁石7とホール素子8からなる位置検出手段を設けてある。
【0006】
ここで棒状磁石7は、駆動軸5の吸排気弁6が取付けてある方とは反対側の、図では上側の端部に取付けられており、ホール素子8は、棒状磁石7に対峙するようにして本体に取付けてあり、従って、駆動軸5の変位に応じてホール素子8に対する棒状磁石7の位置が変化し、この結果、ホール素子8に検知される磁界の強さが変化するので、この磁界の強さに応じて棒状磁石7の位置、すなわち吸排気弁6の位置が検出でき、変位量を知ることができる。
【0007】
このとき、ホール素子8は可動子1の移動方向と平行に設置されると共に、可動子1が中立位置にあるとき、上下端を磁極とする棒状磁石7の長さ方向の中心とホール素子8の中心が一致するように、位置が調整されており、これにより、ホール素子8は棒状磁石7から半径方向に発生する磁界強度が測定でき、可動子1の位置が計測され、変位量を求めることができ。
【0008】
【発明が解決しようとする課題】
上記従来技術は、位置検出のための棒状磁石に存在する磁界の非対称性について配慮がされておらず、駆動軸の回動に伴って発生する位置検出誤差に問題があった。
電磁式吸排気弁駆動システムでは、上記したように、エンジンの様々な運転状況下において最適な吸排気タイミングに制御するためには、高速で往復移動する可動子1の位置を検出する必要がある。
【0009】
また、可動子1が上下の電磁石2、3と衝突する際に発生する騒音やショックを低減するためには衝突速度を遅くする速度制御、すなわちストローク中での速度可変制御も必要であり、可動子1が衝突直前になるストロークの上・下死点近傍での高精度な位置計測が不可欠な要素となる。
更に、衝突時の加速度は数千Gにまで及ぶため、高寿命化のためにも可動子1の速度制御が必要である。
【0010】
ところで、上記した電磁式吸排気弁駆動システムでは、動作中、可動子1は往復運動と同時に回転運動してしまうことがある。
この場合、棒状磁石7の磁軸が、この棒状磁石7の長さ方向の中心軸に正しく一致しているときは問題が無いが、磁軸に曲りがあり、磁界強度分布が棒状磁石7の長さ方向の中心軸に対して円対称になっていないときには、この棒状磁石7が回転運動することにより磁石周囲の磁界強度に変動が生じ、正確な変位量計測が行なえなくなる。
【0011】
つまり、棒状磁石の磁軸に曲りがあると、長さ方向の中心軸に対する磁界の対称性が崩れ、回転しただけで、長さ方向の位置が変わらなくても磁界が変化してしまうため、測定誤差が増大してしまうのである。
しかるに、従来技術では、その磁軸が曲りなく、長さ方向の中心軸に正確に一致している棒状磁石を得るのが困難であり、従って、検出精度の保持に問題が生じてしまうのである。
【0012】
本発明の目的は、磁軸の曲りによる中心軸とのずれが少なく、位置検出用に使用して充分な検出精度が容易に得られるようにした棒状磁石を提供することにある。
【0013】
【課題を解決するための手段】
上記目的は、永久磁石用磁性材料からなる棒状部材の両端が磁極になるように着磁した後、この着磁された棒状部材を長さ方向に2分割して第1と第2の部材とした上で、これら第1と第2の各部材の前記磁極になっていた方の端部を相互に接合させ、分割された方の端部で新たな磁極が形成されるようにして達成される。
【0014】
なお、本発明では、上記手段に想到する過程で、図2に示した棒状磁石についても検討がされており、これによっても、一応は目的が達成されることが確認されているので、ここで本発明の実施形態について説明する前に、参考例として、この図2の棒状磁石について説明する。
【0015】
この図2の参考例は、永久磁石材料からなる棒状部材の両端が磁極になるように着磁した後、前記棒状部材の一方と他方の端部を取り除いて現われた両端で新たな磁極が形成されるようにしたものであり、まず、図2(a)に示すように、永久磁石用磁性材料の棒材7Aを用意する。
【0016】
ここで、この永久磁石用磁性材料(永久磁石材)としては、タングステン鋼などで代表される各種の合金鋼や、バリウム系、ネオジウム系などの焼結材が使用され、最終的に必要とする長さL(後述)よりも所定の寸法だけ長い寸法L を有する棒材7Aとして成形されたものが用意される。
【0017】
次に、図2(b)に示すように、この棒材7Aに、その長手方向の磁界を掛けて着磁し、棒状磁石7Bとする。
しかし、このとき、たとえ棒材7Aの軸方向に正しく着磁したとしても、着磁により形成された磁軸Mには曲りが現れ、この結果、図示のように、着磁された棒状磁石7Bでは、その端面で中心軸Cからずれてしまうのが避けられない。
なお、これが従来技術での問題点であることは、上記した通りである。
【0018】
そこで、次に、図2(c)に示すように、この棒状磁石7Bの両方の端部7B1、7B2をそれぞれ切り離してやると、これらの端部7B1、7B2が切り離されて新たに端面になった部分がそれぞれ新たに磁極を形成し、図2(d)に示すように、長さLの棒状磁石7になる。なお、このときな長さLは、最終的に棒状磁石7に必要な寸法であることは、上記した通りである。
【0019】
ここで、磁軸Mについて見ると、図2(b)から明らかなように、これは曲ってはいるが、中心点Oでは中心軸Cに一致していて、端部に向かうにつれ離れてゆき、端部で一番離れている。
【0020】
そこで、図2(c)に示すように、この棒状磁石7Bの両方の端部7B1、7B2をそれぞれ切り離してやれば、図2(d)に示すように、棒状磁石7として新たに形成された端面による磁極N、Sでは、磁軸Mが中心軸Cから離れている割合は充分に小さくなる。
【0021】
従って、この参考例による棒状磁石7によっても、磁極N、Sでの磁軸の曲りを小さく抑えることができ、例えば図3で説明した電磁式吸排気弁駆動システムに適用して、高い精度での位置検出が可能な棒状磁石を得ることができる。
【0022】
【発明の実施の形態】
以下、本発明による棒状磁石について、図示の実施の形態により詳細に説明する。
図1は本発明による棒状磁石の一実施形態で、まず、図1(a)に示すように、永久磁石の母材となる磁性材料の棒材7Aを用意し、次いで、図1(b)に示すように、この棒材7Aに、その長さ方向に向かう磁界Hをかけて着磁し、棒状磁石7Bとする。
【0023】
ここで、この棒材7Aとなる磁性材料(永久磁石材)としては、例えば熱安定性や耐腐食性、それに高保磁力特性などの見地からサマリウム−コバルト系の永久磁石材が使用されるが、参考例で説明した各種の合金鋼や焼結材でも実施可能である。
【0024】
次に、図1(c)に示すように、棒状磁石7Bを、その長さ方向の中心で切り離し、長さL/2づづの2個の棒状磁石7L、7Rにする。
ここで、これらの棒状磁石7L、7Rにおいて、元の端面を夫々EL、ERとし、切断面を夫々CL、CRとする。
【0025】
次に、図1(d)に示すように、各棒状磁石7L、7Rを図において左右に入替え、元の端面EL、ER同士が向かい合うようにして、これらの端面EL、ERで接合する。
そうすると、各棒状磁石7L、7Rの切断面CL、CRが新たな磁極N、Sを形成し、長さLの棒状磁石7が得られる。
【0026】
このときの接合には、例えばエポキシ系の接着材やシアノアクリレート系の接着材を用いてやれば良い。但し、これら棒状磁石7L、7Rの元の端面EL、ER同士は、一方はN極で他方はS極になって相互に磁気的に吸引し合うので、適当な保持方法を採ってやれば、特に接着させる必要はない。
【0027】
この実施形態によれば、図1(d)から明らかなように、磁軸Mが中心線Cに一致している棒状磁石7Bの切断面CL、CRが新たな磁極N、Sになっているので、この磁極N、Sでは、磁軸Cはほとんど曲りがない状態になっている。
【0028】
従って、この実施形態によれば、磁極となっている端面での磁軸の曲りが極めて小さく、ほどんどゼロに近くでき、この結果、例えば図3で説明した電磁式吸排気弁駆動システムに適用して、充分に高い精度で位置検出が可能な棒状磁石7を容易に得ることができる。
【0029】
【発明の効果】
本発明によれば、磁軸の曲りが小さくて、ほとんどゼロに近い棒状磁石による高精度の位置検出が容易に得られるので、電磁式吸排気弁駆動システムなどに適用して、エンジンを高精度で制御することができる。
【図面の簡単な説明】
【図1】本発明による棒状磁石の一実施形態を示す説明図である。
【図2】本発明の参考例となる棒状磁石の説明図である。
【図3】本発明による棒状磁石が適用対象とする電磁式吸排気弁駆動システムの一例を示す断面図である。
【符号の説明】
1 可動子
2、3 電磁石
4 スプリング
5 駆動軸
6 吸排気弁
7 棒状磁石
7A 永久磁石用磁性材料の棒状部材
7B 着磁された棒状磁石7B
7L、7R 切断された棒状磁石
8 ホール素子
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a bar-shaped magnet for forming a magnetic field, and more particularly to a bar-shaped magnet for forming a magnetic field suitable for measuring displacement.
[0002]
[Prior art]
As one type of displacement measurement method, there is a method of measuring a mutual displacement between the rod-shaped magnet and the magnetic detection element by using a rod-shaped magnet having magnetic poles at both ends and a magnetic detection element such as a Hall element, and measuring a magnetic field strength by the rod-shaped magnet. For example, Japanese Patent Laying-Open No. 6-180242 discloses an example applied to a flow rate measuring device.
[0003]
By the way, in recent years, an engine of a type that electromagnetically controls the opening and closing of an intake valve and an exhaust valve, that is, an electronically controlled intake / exhaust valve system has been put into practical use. FIG. 3 shows an electromagnetic type intake / exhaust valve used in such a system. This is an example of an exhaust valve (intake valve or exhaust valve) drive system. This example shows a mover (amateur) 1 made of a magnetic material, two electromagnets 2, 3 and a spring 4 as shown in the figure. An intake / exhaust valve 6 is attached to the drive shaft 5 of the mover 1 using an electromagnetic actuator consisting of
[0004]
When the intake / exhaust valve 6 is moved upward in the figure, that is, when the valve is closed, the electromagnet 2 is energized to attract the mover 1, and when it is moved downward, that is, when the valve is opened, the electromagnet 3 is energized. At this time, the mover 1 is attracted. At this time, the spring 4 works together with other springs (not shown) to hold the mover 1 in the neutral position when the electromagnets 2 and 3 are not energized. is there.
[0005]
In this case, it is characteristic that independent control of the valve opening timing and the valve closing timing during operation and also the control of the lift amount are possible. For this purpose, the drive position of the mover 1 is changed. It is necessary to control accurately, and for this purpose, it is necessary to correctly detect the displaced position.
Therefore, in the example of FIG. 3, as shown, a rod-shaped permanent magnet, that is, a position detecting means including a rod-shaped magnet 7 and a Hall element 8 is provided.
[0006]
Here, the rod-shaped magnet 7 is attached to the upper end in the figure opposite to the side where the intake / exhaust valve 6 of the drive shaft 5 is attached, so that the Hall element 8 faces the rod-shaped magnet 7. Therefore, the position of the bar-shaped magnet 7 with respect to the Hall element 8 changes according to the displacement of the drive shaft 5, and as a result, the strength of the magnetic field detected by the Hall element 8 changes. The position of the bar-shaped magnet 7, that is, the position of the intake / exhaust valve 6, can be detected according to the strength of the magnetic field, and the displacement can be known.
[0007]
At this time, the Hall element 8 is installed in parallel with the moving direction of the mover 1, and when the mover 1 is in the neutral position, the center of the length direction of the bar-shaped magnet 7 whose upper and lower ends are magnetic poles and the Hall element 8 Are adjusted so that the centers of the movable elements 1 coincide with each other, whereby the Hall element 8 can measure the magnetic field intensity generated in the radial direction from the rod-shaped magnet 7, the position of the movable element 1 is measured, and the displacement amount is obtained. It is possible.
[0008]
[Problems to be solved by the invention]
The above prior art does not consider the asymmetry of the magnetic field existing in the bar-shaped magnet for position detection, and has a problem in a position detection error generated with the rotation of the drive shaft.
In the electromagnetic intake / exhaust valve drive system, as described above, it is necessary to detect the position of the movable element 1 that reciprocates at high speed in order to control the intake / exhaust timing to be optimal under various operating conditions of the engine. .
[0009]
Further, in order to reduce noise and shock generated when the mover 1 collides with the upper and lower electromagnets 2, 3, speed control for reducing the collision speed, that is, variable speed control during a stroke is necessary. High-precision position measurement near the top and bottom dead center of the stroke immediately before the child 1 collides is an essential element.
Furthermore, since the acceleration at the time of collision reaches several thousand G, it is necessary to control the speed of the mover 1 to extend the life.
[0010]
By the way, in the above-described electromagnetic intake / exhaust valve drive system, during operation, the mover 1 sometimes rotates at the same time as reciprocating motion.
In this case, there is no problem when the magnetic axis of the bar-shaped magnet 7 is correctly coincident with the central axis of the bar-shaped magnet 7 in the longitudinal direction. When the rod-shaped magnet 7 is not circularly symmetric with respect to the central axis in the longitudinal direction, the magnetic field strength around the magnet changes due to the rotational movement, so that accurate measurement of the displacement cannot be performed.
[0011]
In other words, if the magnetic axis of the rod-shaped magnet is bent, the symmetry of the magnetic field with respect to the central axis in the longitudinal direction is broken, and the magnetic field changes even if the position in the longitudinal direction does not change just by rotating, The measurement error increases.
However, in the prior art, it is difficult to obtain a bar-shaped magnet whose magnetic axis does not bend and is exactly coincident with the central axis in the longitudinal direction, and therefore, a problem occurs in maintaining the detection accuracy. .
[0012]
SUMMARY OF THE INVENTION An object of the present invention is to provide a rod-shaped magnet which is used for position detection and has sufficient detection accuracy easily with little deviation from a central axis due to bending of a magnetic axis.
[0013]
[Means for Solving the Problems]
The object is to magnetize a rod-shaped member made of a magnetic material for a permanent magnet so that both ends become magnetic poles, and then divide the magnetized rod-shaped member into two parts in a length direction to form a first member and a second member. Then, the ends of the first and second members, which have become the magnetic poles, are joined to each other so that a new magnetic pole is formed at the divided end. You.
[0014]
In the present invention, the rod-shaped magnet shown in FIG. 2 has also been studied in the process of arriving at the above means, and it has been confirmed that the object can be achieved to some extent. Before describing the embodiment of the present invention, the bar-shaped magnet of FIG. 2 will be described as a reference example.
[0015]
In the reference example of FIG. 2, after the both ends of the rod-shaped member made of a permanent magnet material are magnetized to be magnetic poles, one end and the other end of the rod-shaped member are removed, and new magnetic poles are formed at both ends that appear. First, as shown in FIG. 2A, a bar 7A made of a magnetic material for a permanent magnet is prepared.
[0016]
Here, as the magnetic material (permanent magnet material) for the permanent magnet, various alloy steels represented by tungsten steel and the like, and sintered materials such as barium-based and neodymium-based materials are used, and finally required. the length L (described later) that is formed is prepared as a rod 7A having a long dimension L 1 by a predetermined dimension than.
[0017]
Next, as shown in FIG. 2B, the bar 7A is magnetized by applying a magnetic field in its longitudinal direction to form a bar-shaped magnet 7B.
However, at this time, even if the bar 7A is correctly magnetized in the axial direction, the magnetic axis M formed by the magnetizing bends, and as a result, as shown, the magnetized bar-shaped magnet 7B Then, it is inevitable that the end face deviates from the center axis C.
It is to be noted that this is a problem in the prior art, as described above.
[0018]
Then, as shown in FIG. 2C, when both ends 7B1 and 7B2 of the bar-shaped magnet 7B are cut off, these ends 7B1 and 7B2 are cut off to form a new end face. The newly formed portions each newly form a magnetic pole, and become a bar-shaped magnet 7 having a length L as shown in FIG. It should be noted that the length L at this time is a dimension finally required for the bar-shaped magnet 7 as described above.
[0019]
Here, looking at the magnetic axis M, as is apparent from FIG. 2B, it is bent, but coincides with the central axis C at the center point O, and moves away toward the end. Farthest at the end.
[0020]
Therefore, as shown in FIG. 2C, if both ends 7B1 and 7B2 of the bar-shaped magnet 7B are cut off, a new bar-shaped magnet 7 is formed as shown in FIG. 2D. In the magnetic poles N and S formed by the end faces, the ratio of the magnetic axis M separated from the central axis C is sufficiently small.
[0021]
Therefore, the bending of the magnetic axis at the magnetic poles N and S can be suppressed to be small by the rod-shaped magnet 7 according to this reference example. For example, the rod-shaped magnet 7 can be applied to the electromagnetic intake / exhaust valve drive system described with reference to FIG. Can be obtained.
[0022]
BEST MODE FOR CARRYING OUT THE INVENTION
Hereinafter, a bar-shaped magnet according to the present invention will be described in detail with reference to the illustrated embodiments.
FIG. 1 shows an embodiment of a bar-shaped magnet according to the present invention. First, as shown in FIG. 1A, a bar 7A of a magnetic material serving as a base material of a permanent magnet is prepared, and then, FIG. As shown in Fig. 7, a magnetic field H is applied to the bar 7A in the length direction thereof to magnetize the bar 7A to obtain a bar-shaped magnet 7B.
[0023]
Here, as the magnetic material (permanent magnet material) to be the bar 7A, a samarium-cobalt permanent magnet material is used from the viewpoints of, for example, thermal stability, corrosion resistance, and high coercive force characteristics. Various alloy steels and sintered materials described in the reference example can be used.
[0024]
Next, as shown in FIG. 1 (c), the bar-shaped magnet 7B is cut off at the center in the length direction to form two bar-shaped magnets 7L and 7R each having a length of L / 2.
Here, in these rod-shaped magnets 7L and 7R, the original end faces are designated as EL and ER, respectively, and the cut faces are designated as CL and CR, respectively.
[0025]
Next, as shown in FIG. 1D, the bar-shaped magnets 7L and 7R are switched to the right and left in the figure, and the original end faces EL and ER are joined so as to face each other.
Then, the cut surfaces CL and CR of the bar magnets 7L and 7R form new magnetic poles N and S, and the bar magnet 7 having the length L is obtained.
[0026]
The bonding at this time may be performed using, for example, an epoxy-based adhesive or a cyanoacrylate-based adhesive. However, the original end faces EL and ER of these rod-shaped magnets 7L and 7R are magnetically attracted to each other with one being an N pole and the other being an S pole, so that if an appropriate holding method is adopted, There is no particular need for bonding.
[0027]
According to this embodiment, as is clear from FIG. 1D, the cut surfaces CL and CR of the bar-shaped magnet 7B whose magnetic axis M coincides with the center line C are new magnetic poles N and S. Therefore, at these magnetic poles N and S, the magnetic axis C is hardly bent.
[0028]
Therefore, according to this embodiment, the bending of the magnetic axis at the end face serving as the magnetic pole is extremely small and can be almost close to zero. As a result, for example, the present invention is applied to the electromagnetic intake / exhaust valve drive system described with reference to FIG. Thus, it is possible to easily obtain the bar-shaped magnet 7 capable of detecting the position with sufficiently high accuracy.
[0029]
【The invention's effect】
According to the present invention, the bending of the magnetic axis is small, and high-precision position detection can be easily obtained by a rod magnet that is almost zero. Can be controlled by
[Brief description of the drawings]
FIG. 1 is an explanatory view showing one embodiment of a bar-shaped magnet according to the present invention.
FIG. 2 is an explanatory view of a bar-shaped magnet serving as a reference example of the present invention.
FIG. 3 is a sectional view showing an example of an electromagnetic intake / exhaust valve drive system to which the bar-shaped magnet according to the present invention is applied.
[Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 Mover 2, 3 Electromagnet 4 Spring 5 Drive shaft 6 Intake / exhaust valve 7 Bar-shaped magnet 7A Bar-shaped member 7B of magnetic material for permanent magnets Magnetized bar-shaped magnet 7B
7L, 7R Cut rod magnet 8 Hall element

Claims (2)

永久磁石用磁性材料からなる棒状部材の両端が磁極になるように着磁した後、この着磁された棒状部材を長さ方向に2分割して第1と第2の部材とした上で、これら第1と第2の各部材の前記磁極になっていた方の端部を相互に接合させ、分割された方の端部で新たな磁極が形成されていることを特徴とする棒状磁石。After magnetizing so that both ends of the bar-shaped member made of a magnetic material for a permanent magnet become magnetic poles, the magnetized bar-shaped member is divided into two in the length direction to form first and second members. A rod-shaped magnet, wherein the ends of the first and second members which have become the magnetic poles are joined to each other, and a new magnetic pole is formed at the divided end. 請求項1に記載の発明において、
前記第1と第2の部材が、前記着磁された棒状部材の長手方向の中央で2分割されていることを特徴とする棒状磁石。
In the invention according to claim 1,
A rod-shaped magnet, wherein the first and second members are divided into two parts at the longitudinal center of the magnetized rod-shaped member.
JP2000103793A 2000-04-05 2000-04-05 Bar magnet Expired - Fee Related JP3572396B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000103793A JP3572396B2 (en) 2000-04-05 2000-04-05 Bar magnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000103793A JP3572396B2 (en) 2000-04-05 2000-04-05 Bar magnet

Publications (2)

Publication Number Publication Date
JP2001291613A JP2001291613A (en) 2001-10-19
JP3572396B2 true JP3572396B2 (en) 2004-09-29

Family

ID=18617435

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2000103793A Expired - Fee Related JP3572396B2 (en) 2000-04-05 2000-04-05 Bar magnet

Country Status (1)

Country Link
JP (1) JP3572396B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE10308958A1 (en) * 2003-02-28 2004-09-09 Siemens Ag Magnetically passive position sensor, method for manufacturing the magnetically passive position sensor
JP4831839B2 (en) * 2008-03-27 2011-12-07 三菱重工業株式会社 Engine valve actuator and internal combustion engine
DK200800779A (en) * 2008-06-05 2009-12-06 Alfa Laval Kolding As Sensing and control device

Also Published As

Publication number Publication date
JP2001291613A (en) 2001-10-19

Similar Documents

Publication Publication Date Title
JP3629362B2 (en) Driving method of electromagnetic valve for driving engine valve
US6819208B1 (en) Electromagnetic linear actuator with position sensor
US6160395A (en) Non-contact position sensor
ATE95278T1 (en) ELECTROMAGNETIC ACTUATOR.
US6313553B1 (en) Rotating electromagnetic actuator comprising at least one magnet embedded in ferromagnetic material
US7800470B2 (en) Method and system for a linear actuator with stationary vertical magnets and coils
US3694782A (en) Rotary actuator
JP3572396B2 (en) Bar magnet
JPH10220622A (en) Electromagnetic actuator with narrow structure
US20090114863A1 (en) Electromagnetically driven valve
US6916005B2 (en) Displacement sensor and solenoid valve driver
US6870285B2 (en) Long stroke linear voice coil actuator with the proportional solenoid type characteristic
JPH09320841A (en) Controller for electromagnetic actuator
EP1752626B1 (en) Electromagnetically driven valve
JP2001194182A (en) Magnetic sensor
US6543477B2 (en) Electromechanical actuator
JP2001126918A (en) Electromagnetic actuator
CA2408257A1 (en) Stud welding head
JP2001303915A (en) Valve system for internal combustion engine
CN204179915U (en) Controlled displacement feeding drive system
JP2007032436A (en) Solenoid drive valve
JP4779690B2 (en) Actuator
CN215369975U (en) Electromagnetic actuator and camshaft phase adjusting device
JP2011103493A (en) Actuator
JPS5852536Y2 (en) Movable iron piece type instrument

Legal Events

Date Code Title Description
A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20040506

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20040525

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20040607

R150 Certificate of patent or registration of utility model

Free format text: JAPANESE INTERMEDIATE CODE: R150

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20080709

Year of fee payment: 4

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20090709

Year of fee payment: 5

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20100709

Year of fee payment: 6

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20110709

Year of fee payment: 7

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20120709

Year of fee payment: 8

LAPS Cancellation because of no payment of annual fees