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JPS6019646B2 - Electromagnetic mechanism for camera release - Google Patents
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JPS6019646B2 - Electromagnetic mechanism for camera release - Google Patents

Electromagnetic mechanism for camera release

Info

Publication number
JPS6019646B2
JPS6019646B2 JP4475277A JP4475277A JPS6019646B2 JP S6019646 B2 JPS6019646 B2 JP S6019646B2 JP 4475277 A JP4475277 A JP 4475277A JP 4475277 A JP4475277 A JP 4475277A JP S6019646 B2 JPS6019646 B2 JP S6019646B2
Authority
JP
Japan
Prior art keywords
magnetic
armature
permanent magnet
yoke
electromagnetic mechanism
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
JP4475277A
Other languages
Japanese (ja)
Other versions
JPS53129627A (en
Inventor
秀明 宮川
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP4475277A priority Critical patent/JPS6019646B2/en
Publication of JPS53129627A publication Critical patent/JPS53129627A/en
Publication of JPS6019646B2 publication Critical patent/JPS6019646B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Shutters For Cameras (AREA)
  • Shutter-Related Mechanisms (AREA)

Description

【発明の詳細な説明】 本発明はカメラのしリーズ動作駆動源として用いられる
電磁機構で永久磁石によるアーマチュアの吸着を励磁コ
イルにより発生する磁束で打消すことにより吸着解除し
てしリーズ動作を行なわせるレリーズ用電磁機構に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention is an electromagnetic mechanism used as a drive source for the shutter operation of a camera, and the armature is canceled by magnetic flux generated by an excitation coil to cancel the attraction of the armature by a permanent magnet, thereby performing the trigger operation. This invention relates to an electromagnetic mechanism for release.

電気制御方式のカメラにおけるレリーズ動作を行なわせ
るための電磁機構としては極めて小型に構成されかつ動
作の速いものが要求されており、しかも消費電力を極力
少なくする必要があり、各種形成のものが提案されてい
る。本発明の出願人は先に「特願昭49−14360」
(特関昭50一109723号公報参照)として永久磁
石の磁束を励磁コイルにより発生する磁束で打消してァ
ーマチュアの吸着解除を行なう方式のしリーズ用電磁機
構を提案した。この方式の電磁機構ではしりーズ動作を
行なうための励磁コイルに多量の電流をパルス的に流す
必要があり、これには電源電池で予め充電されているキ
ヤパシターの蓄積電荷を一時に励磁コイルに放電する回
路構成が用いられている。すなわち上記のような型式の
電磁機構はカメラ等に組込まれる小容量の電池、例えば
水銀電池、銀電池等では直接これを駆動することが困難
であるため、0予め充電されたキャパシターの電荷をパ
ルス的に励磁コイルに放電する方法を用いており、これ
にはキャパシター充電のためのある時間の遅れが供なう
ものである。このような電磁機構によりカメラのしリー
ズ動作を行なう場合、一般の撮影時に夕は何ら不都合は
起らないが、モータードライブ等を用いて高速連続撮影
を行なう場合にはキャパシターの充電が間に合わず不動
作を起すことがあり、これをカバーするために充電時間
が短くなるように電源電圧を高くすることが必要となり
、軍20源電池のスペースの関係、消費電力の増加等の
不都合が生じるものであった。本発明は上記の如き従来
の電磁機構の欠点を除いた構造のレリーズ用電磁機構を
提供するもので、その目的とするところは小容量電源に
より効25果的に作動可能であり、かつ高速連続撮影の
際のしリーズ動作にも充分応動し得る小型で消費電力の
少ない電磁機構を得ることである。
The electromagnetic mechanism for performing the release operation in electrically controlled cameras is required to be extremely compact and operate quickly, and it is also necessary to minimize power consumption, so various configurations have been proposed. has been done. The applicant of the present invention previously filed the "Patent Application No. 14360-1983"
(Refer to Special Publication No. 50-109723), we proposed an electromagnetic mechanism for electric wires in which the magnetic flux of a permanent magnet is canceled out by the magnetic flux generated by an excitation coil to release the armature from adsorption. In this type of electromagnetic mechanism, it is necessary to flow a large amount of current in pulses to the excitation coil to perform the shutter operation, and this requires the accumulated charge in the capacitor, which is pre-charged by the power battery, to be simultaneously transferred to the excitation coil. A discharging circuit configuration is used. In other words, the electromagnetic mechanism of the above type is difficult to directly drive with a small capacity battery built into a camera, etc., such as a mercury battery or a silver battery. A method of discharging the excitation coil is used, which is accompanied by a certain time delay for charging the capacitor. If the camera is operated by an electromagnetic mechanism like this, there will be no problem during normal shooting in the evening, but if you use a motor drive etc. for high-speed continuous shooting, the capacitor will not be charged in time and there will be a problem. In order to compensate for this, it is necessary to increase the power supply voltage to shorten the charging time, which causes inconveniences such as space constraints and increased power consumption for military 20 source batteries. there were. The present invention provides a release electromagnetic mechanism that eliminates the drawbacks of the conventional electromagnetic mechanisms as described above, and its purpose is to be able to operate effectively with a small capacity power source and to provide high-speed continuous operation. To obtain an electromagnetic mechanism that is small and consumes little power and can sufficiently respond to leakage operations during photographing.

すなわち本発明の電磁機構はヨークの一部に配設せる永
久磁石よりの磁束でレリーズ作動用アーマチュアを吸肴
保持し、ヨークに配設せる励磁コイルへの通電により発
生する磁束で前記永久磁石による磁束を打消してアーマ
チュァの保持解除を行なう電磁機構において前記永久磁
石の両極間に半硬磁性材料よりなるバイパス磁路を設け
、このバイパス磁路に第2の励磁コイルを配設すると共
に、レリーズリセット時に前記半硬磁性材料の消磁を行
なう手段を備えたレリーズ用電磁機構である。以下図面
によって本発明を詳細に説明する。
That is, in the electromagnetic mechanism of the present invention, the armature for release operation is attracted and held by the magnetic flux from the permanent magnet disposed in a part of the yoke, and the magnetic flux generated by energizing the excitation coil disposed in the yoke is caused by the permanent magnet. In the electromagnetic mechanism that cancels the magnetic flux and releases the armature, a bypass magnetic path made of a semi-hard magnetic material is provided between the poles of the permanent magnet, a second excitation coil is disposed in this bypass magnetic path, and a release mechanism is provided. The release electromagnetic mechanism includes means for demagnetizing the semi-hard magnetic material at the time of reset. The present invention will be explained in detail below with reference to the drawings.

第1図は本発明によるしリーズ用電磁機構の一実施例を
示す構成図である。図において、1はアーマチュアで軟
磁性材料により構成し、その吸着解除動作で不図示のレ
リーズ機構を駆動する。2はヨークで軟磁性材料よりな
る。
FIG. 1 is a configuration diagram showing an embodiment of an electromagnetic mechanism for a leash according to the present invention. In the figure, reference numeral 1 denotes an armature made of a soft magnetic material, and its attraction/release operation drives a release mechanism (not shown). 2 is a yoke made of a soft magnetic material.

3はヨーク2の一部に固定された永久磁石、4は永久磁
石3の両極間に配設された半硬磁性材料よりなるバイパ
ス磁路で、2,3および4は一体として構成される。
3 is a permanent magnet fixed to a part of the yoke 2; 4 is a bypass magnetic path made of a semi-hard magnetic material disposed between both poles of the permanent magnet 3; 2, 3, and 4 are integrally constructed.

5はアーマチュア1の付勢バネで矢印方向に付勢されて
いる。
5 is biased by a biasing spring of armature 1 in the direction of the arrow.

6はヨーク2の一方のアーム(又は両方のアーム)上に
巻回された励磁コイル、7はバイパス滋路上に巻回され
た励磁コイルで、これらに電流を流して電磁的に起磁力
を得る。
6 is an excitation coil wound on one arm (or both arms) of the yoke 2, and 7 is an excitation coil wound on the bypass feeder, and a current is passed through these to obtain magnetomotive force electromagnetically. .

8および9は永久磁石で電磁機構のリセツト時に前記バ
イパス磁路の両端部に近接させて消滋作用を行なう。
Permanent magnets 8 and 9 are brought close to both ends of the bypass magnetic path to perform an extinguishing action when the electromagnetic mechanism is reset.

10は永久磁石8,9の保持部材で、8,9,10で構
成されるリセット用部材は矢印方向に移動し得るように
構成される。
10 is a holding member for permanent magnets 8 and 9, and a reset member composed of 8, 9, and 10 is configured to be movable in the direction of the arrow.

第2図は本発明の電磁機構におけるバイパス磁路を構成
する半硬磁性材料の磁化特性の一例を示す曲線図である
。図において横軸(磁化力H)と曲線との交点日一日三
は保磁力を表わし、縦軸(磁束密度B)と曲線との交点
Br,一Brは残留磁気を表わす。第1図の構成におい
て、アーマチュア1がヨーク2から離れている時に永久
磁石3により半硬磁性材料よりなるバイパス磁路4に加
えられる磁界の強さは第2図のHBで示すように保磁力
日さよりも大であり、またアーマチュアがヨークに吸着
された状態の時にバイパス滋路に加えられる磁界の強さ
HAは保磁力HEよりも小さくなるよに設定される。す
なわちこの時はHA<日さくHB
‘11の条件が成り立っている。
FIG. 2 is a curve diagram showing an example of the magnetization characteristics of the semi-hard magnetic material constituting the bypass magnetic path in the electromagnetic mechanism of the present invention. In the figure, the intersection between the horizontal axis (magnetizing force H) and the curve represents the coercive force, and the intersection between the vertical axis (magnetic flux density B) and the curve Br, 1 Br represents the residual magnetism. In the configuration shown in FIG. 1, when the armature 1 is apart from the yoke 2, the strength of the magnetic field applied by the permanent magnet 3 to the bypass magnetic path 4 made of a semi-hard magnetic material is determined by the coercive force as shown by HB in FIG. The strength of the magnetic field HA applied to the bypass passage when the armature is attracted to the yoke is set to be smaller than the coercive force HE. In other words, at this time HA < Sunsaku HB
The conditions of '11 are satisfied.

またリセット時にリセット用部材の永久磁石8および9
が第1図示の位置に来た時は、これら8および9により
バイパス磁路4に加えられる磁界の強さHRが半硬磁性
材料の保持カー日三よりも大きく、一服よりも小さい値
になるように設定される。すなわちこの状態では−日さ
<HR<−日き 【2)の条件
が成り立つように構成される。
Also, when resetting, the permanent magnets 8 and 9 of the reset member
When the magnetic field reaches the position shown in the first diagram, the strength HR of the magnetic field applied to the bypass magnetic path 4 by these 8 and 9 becomes a value larger than the retention force of the semi-hard magnetic material and smaller than the magnetic field strength. It is set as follows. In other words, in this state, the following condition is established: -day<HR<-date [2].

本発明の電磁機構においては第1図の構成でアーマチュ
ア吸着時(リセット後)は{1}式が、またアーマチュ
アリセット時と半硬磁性材料の保持力の関係は‘2}式
が満足するような半硬磁性材料により図示の如きバイパ
ス磁路を構成することが必要である。つぎに本発明によ
るしリーズ用電磁機構の動作を説明する。第3図は本発
明の電磁機構のリセツト時(a図),レリーズ信号入力
時(b図)およびレリーズ時(c図)の状態並びにそれ
らの等価磁気回礎b′,b′,c′を示す図である。図
において第1図と同じ部分は同一符号で示してある。な
お等価回路におけるRaはアーマチュア1の等価磁気抵
抗、Ryはヨーク2の等価磁気抵抗であり、Rgはアー
マチュアとヨークとの吸着面ギャップの等価磁気抵抗で
あり、これらは互いに直列接続されている。Rm‘まヨ
ーク2の一部に配設された永久磁石3の等価磁気抵抗で
あり、Umは永久磁石の起磁力である。リセット時にア
ーマチュアーが第3図aに示すようにリセットされると
同時にリセツト用部材の永久磁石8,9がバイパス滋略
の両端に近接して半硬磁性材料に磁界を加えたのち、離
脱する。これにより永久磁石3と励磁コイル7で発生し
た磁界で半硬磁性材料に生じた磁気が打消されるので、
等価磁気回路は第3図a′に示すように互に逆犠牲に接
続された2個の定電圧ダイオード(ツェナーダイオード
)ZDで示されることになり、従ってリセット時の等価
磁気回路は第3図a′のようになる。図示のように永久
磁石3の起磁力Umにより生ずる磁束■m,はヨーク側
の分路にのみ流れバイパス磁路へは流れないことになり
、この時のアーマチユア1とヨーク2との間の吸着力F
.はF.E2券さ−f ■ で表わされる。
In the electromagnetic mechanism of the present invention, with the configuration shown in Fig. 1, formula {1} is satisfied when the armature is attracted (after reset), and formula '2} is satisfied when the armature is reset and the holding force of the semi-hard magnetic material. It is necessary to construct the bypass magnetic path as shown in the figure using a semi-hard magnetic material. Next, the operation of the electromagnetic mechanism for leasing according to the present invention will be explained. Figure 3 shows the states of the electromagnetic mechanism of the present invention at the time of reset (Figure a), at the time of inputting the release signal (Figure B), and at the time of release (Figure C), and their equivalent magnetic circuits b', b', and c'. FIG. In the figure, the same parts as in FIG. 1 are designated by the same reference numerals. In the equivalent circuit, Ra is the equivalent magnetic resistance of the armature 1, Ry is the equivalent magnetic resistance of the yoke 2, and Rg is the equivalent magnetic resistance of the attraction surface gap between the armature and the yoke, and these are connected in series with each other. Rm' is the equivalent magnetic resistance of the permanent magnet 3 disposed in a part of the yoke 2, and Um is the magnetomotive force of the permanent magnet. At the time of resetting, the armature is reset as shown in FIG. 3a, and at the same time, the permanent magnets 8, 9 of the resetting member come close to both ends of the bypass mechanism, apply a magnetic field to the semi-hard magnetic material, and then separate. As a result, the magnetic field generated by the permanent magnet 3 and excitation coil 7 cancels out the magnetism generated in the semi-hard magnetic material.
The equivalent magnetic circuit is shown by two constant voltage diodes (Zener diodes) ZD connected in a reverse sacrificial manner to each other as shown in Fig. 3 a'. Therefore, the equivalent magnetic circuit at the time of reset is shown in Fig. 3. It becomes like a'. As shown in the figure, the magnetic flux ■m generated by the magnetomotive force Um of the permanent magnet 3 flows only into the shunt on the yoke side and does not flow into the bypass magnetic path. Force F
.. is F. It is represented by E2 ticket sa-f ■.

ここでSはアーマチュア・ヨーク間ギャップの吸着面積
、ムoは真空中の透磁率、fはアーマチュアーを付勢し
ているバネの力である。すなわちリセット状態(第3図
a)ではアーマチュァ1はヨーク2に吸着された状態を
保持するに充分な磁束がアーマチュア・ヨーク側に流れ
ており外力fに抗してアーマチュアがヨークに吸着され
ている。第3図bはしりーズ信号が励磁コイル6および
7に入力された状態の図であり、第3図世′がこの状態
における等価磁気回路である。
Here, S is the attraction area of the gap between the armature and the yoke, M o is the magnetic permeability in vacuum, and f is the force of the spring biasing the armature. That is, in the reset state (Fig. 3a), sufficient magnetic flux flows toward the armature and yoke to maintain the state in which the armature 1 is attracted to the yoke 2, and the armature is attracted to the yoke against the external force f. . FIG. 3b shows a state in which the reset signal is input to the excitation coils 6 and 7, and FIG. 3' shows an equivalent magnetic circuit in this state.

この状態ではヨーク及びバイパス滋路に巻回されて励磁
コイル6および7に励磁電流が流れ、これにより第3図
Mこ示すようにヨーク、アーマチュア側に永久磁石3に
よる磁束■m,の他にこれと逆方向に磁束■Eが流れる
。またバイパス磁路には励磁コイル7による磁界が生じ
、これと永久磁石3による磁界と同一方向に生じて加算
されて磁束■Dが流れる。即ち半硬磁性材料の保持力日
三よりこの磁界が大きくなってバイパス磁路に磁束が流
れ始め、この回路が永久磁石のバイパス磁路として作動
する。従ってこの状態の等価磁気回路は第3図b′のよ
うに半硬質磁性材料は一方向に接続されたダイオードD
で表わされる。従って永久磁石3による磁束■m,はバ
イパス磁路に分流されると共に励磁コイル6によりじた
磁束■Eによって打消され、アーマチュア,ヨーク間の
吸着力F2はF2=2〔■m,一く■D+■E)〕2−
f 側2ム。
In this state, an excitation current flows through the excitation coils 6 and 7 wound around the yoke and the bypass supply path, and as a result, as shown in Fig. 3M, in addition to the magnetic flux m due to the permanent magnet 3 on the yoke and armature side. Magnetic flux ■E flows in the opposite direction. Further, a magnetic field generated by the excitation coil 7 is generated in the bypass magnetic path, and this and the magnetic field generated by the permanent magnet 3 are generated in the same direction and are added together, and a magnetic flux (D) flows. That is, as the coercive force of the semi-hard magnetic material increases, this magnetic field becomes larger and magnetic flux begins to flow through the bypass magnetic path, and this circuit operates as a bypass magnetic path for the permanent magnet. Therefore, the equivalent magnetic circuit in this state is as shown in Figure 3b', where the semi-hard magnetic material is a diode D connected in one direction.
It is expressed as Therefore, the magnetic flux ■m caused by the permanent magnet 3 is shunted to the bypass magnetic path and is canceled by the magnetic flux ■E deflected by the excitation coil 6, and the attractive force F2 between the armature and the yoke is F2=2 [■m, one D+■E)〕2-
f side 2mm.

Sとなる。It becomes S.

‘4ー式における吸着力F2が(一)になった時、ァー
マチュアはヨークから吸着解除され、これによってレリ
ーズ動作が行なわれる。第3図Cはしりーズ後の状態を
示す図でアーマチュアーがバネ5の力でヨーク2から離
脱される。
When the attraction force F2 in the '4-type becomes (1), the armature is released from attraction from the yoke, thereby performing a release operation. FIG. 3C is a diagram showing the state after the release, in which the armature is separated from the yoke 2 by the force of the spring 5.

第3図に′はこの時の等価磁気回路でありヨークとァ−
マチュアの吸着面の等価抵抗Rg′は前記第3図a,b
の場合のRgよりも高い値になる。従って永久磁石3に
よる磁束はその大部分が半硬磁性材料よりなるバイパス
滋略4を流れることになり、半硬磁性材料は永久磁石と
して作用する。第3図C′におけるRm′はこの半硬磁
性材料の等価磁気抵抗である。Um′は起磁力である。
この状態における半硬磁性材料の動作点は第2図に日B
で示した点になる。そこでリセット用永久磁石8,9を
バイパス磁路の両端に近接させて半硬磁性材料の磁界を
打消してやるとヨーク,アーマチュア側の磁界が強くな
りァーマチュアのIJセットにより吸着面の磁気抵抗が
RgからRgに低下するので永久磁石3からの磁束が再
びヨーク,アーマチュアの磁路に流れてアーマチュアの
リセットが行なわれる。この際半硬磁性材料に印加され
る磁界の強さHRは、第2図示のように一日三<HR<
一日葦にしてやればよい。以上により電磁機構は第3図
aの状態に戻り、バイパス回路の等価磁気回路も第3図
a′のようにッェナーダィオードZ。で表わされる状態
に戻る。なお第1図、第3図の実施例ではリセット用部
材として永久磁石による磁界を用いているが、この他に
励磁コイル7に逆方向の電流を短時間流して電気的にバ
イパス磁路の消滋をしてもよいことは伝うまでもない。
以上の如く本発明によるレリーズ用電磁機構においては
、ヨークの一部に設けた永久磁石の両端に半硬磁性材料
よりなるバイパス磁路を設けることにより、励磁コイル
に流すレリーズ用電流が少なくてすみ、これによりしリ
ーズ時の電力消費が少なくなし得るものであり、高速連
続撮影の際のカメラレリーズ動作も適確に行ない得るも
のとなし得る。従ってカメラ等のしリーズ用電磁機構と
してすぐれた効果が得られる装置をなし得るものでその
効果は大なるものである。
In Figure 3, '' is the equivalent magnetic circuit at this time, and the yoke and the
The equivalent resistance Rg' of the suction surface of the mature is shown in Figure 3 a and b above.
The value is higher than Rg in the case of . Therefore, most of the magnetic flux generated by the permanent magnet 3 flows through the bypass 4 made of a semi-hard magnetic material, and the semi-hard magnetic material acts as a permanent magnet. Rm' in FIG. 3C' is the equivalent magnetic resistance of this semi-hard magnetic material. Um' is the magnetomotive force.
The operating point of the semi-hard magnetic material in this state is shown in Figure 2.
This will be the point shown in . Therefore, if the reset permanent magnets 8 and 9 are brought close to both ends of the bypass magnetic path to cancel out the magnetic field of the semi-hard magnetic material, the magnetic field on the yoke and armature sides will become stronger, and the magnetic resistance of the attraction surface will change from Rg due to the IJ setting of the armature. Since the magnetic flux decreases to Rg, the magnetic flux from the permanent magnet 3 flows again into the magnetic path between the yoke and the armature, and the armature is reset. At this time, the strength HR of the magnetic field applied to the semi-hard magnetic material is 3<HR<
All you have to do is turn it into a reed for a day. As a result of the above, the electromagnetic mechanism returns to the state shown in FIG. 3a, and the equivalent magnetic circuit of the bypass circuit also becomes a Zener diode Z as shown in FIG. 3a'. Return to the state expressed by . In the embodiments shown in FIGS. 1 and 3, a magnetic field from a permanent magnet is used as the reset member, but in addition to this, the bypass magnetic path can be electrically extinguished by passing a current in the opposite direction through the excitation coil 7 for a short time. It goes without saying that it's okay to be kind.
As described above, in the release electromagnetic mechanism according to the present invention, by providing a bypass magnetic path made of a semi-hard magnetic material at both ends of the permanent magnet provided in a part of the yoke, the release current flowing through the excitation coil can be reduced. This makes it possible to reduce power consumption when the camera is in use, and to perform the camera release operation accurately during high-speed continuous shooting. Therefore, it is possible to create a device that provides excellent effects as an electromagnetic mechanism for cameras and the like, and the effects are great.

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

第1図は本発明によるしリーズ用電磁機構の一実施例を
示す構成図、第2図は半硬磁性材料の磁化特性の一例を
示す曲線図、第3図は本発明の電磁機構の動作説明のた
めの構成図並びに等価磁気回路図である。 1……アーマチュア、2……ヨーク、3……永久磁石、
4…・・・半硬磁性材料よりなるバイパス磁路、5・・
・・・・バネ、6,7・・・・・・励磁コイル、8,9
・・・・・・リセツト用永久磁石、10・・・・・・リ
セット用磁石支持部村。 第1図 第2図 繁る図
Fig. 1 is a configuration diagram showing an example of an electromagnetic mechanism for magnetic wires according to the present invention, Fig. 2 is a curve diagram showing an example of magnetization characteristics of a semi-hard magnetic material, and Fig. 3 is an operation of the electromagnetic mechanism of the present invention. They are a configuration diagram and an equivalent magnetic circuit diagram for explanation. 1... Armature, 2... Yoke, 3... Permanent magnet,
4... Bypass magnetic path made of semi-hard magnetic material, 5...
... Spring, 6, 7 ... Excitation coil, 8, 9
...Reset permanent magnet, 10... Reset magnet support village. Figure 1 Figure 2 Crowded diagram

Claims (1)

【特許請求の範囲】[Claims] 1 アーマチユアの吸着面を有しかつ一部を永久磁石を
配設するヨークの少なくとも一方の磁路に巻回せる第1
の励磁コイルに励磁電流を流して前記永久磁石による磁
束を打消すことによりアーマチユアのレリーズ動作を行
なわせる電磁機構において、前記永久磁石の両極間に配
設せる半硬磁性材料よりなるバイパス磁路と、該バイパ
ス磁路に巻回せる第2の励磁コイルとを設け、該第2の
励磁コイルに前記第1の励磁コイルと同期した励磁電流
を流して前記アーマチユアのレリーズ動作を行なわせる
と共に、アーマチユアのリセツト時に前記バイパス磁路
に流れる磁束を打消すための磁界を発生するリセツト機
構を備えることを特徴とするカメラのレリーズ用電磁機
構。
1. A first yoke which has an armature attraction surface and which can be wound around at least one magnetic path of a yoke in which a part of a permanent magnet is disposed.
An electromagnetic mechanism that performs a release operation of an armature by flowing an excitation current through an excitation coil to cancel the magnetic flux caused by the permanent magnet, comprising: a bypass magnetic path made of a semi-hard magnetic material disposed between both poles of the permanent magnet; and a second excitation coil that can be wound around the bypass magnetic path, and an excitation current that is synchronized with the first excitation coil is caused to flow through the second excitation coil to perform a release operation of the armature. An electromagnetic mechanism for releasing a camera, comprising a reset mechanism that generates a magnetic field for canceling the magnetic flux flowing through the bypass magnetic path at the time of reset.
JP4475277A 1977-04-19 1977-04-19 Electromagnetic mechanism for camera release Expired JPS6019646B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4475277A JPS6019646B2 (en) 1977-04-19 1977-04-19 Electromagnetic mechanism for camera release

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4475277A JPS6019646B2 (en) 1977-04-19 1977-04-19 Electromagnetic mechanism for camera release

Publications (2)

Publication Number Publication Date
JPS53129627A JPS53129627A (en) 1978-11-11
JPS6019646B2 true JPS6019646B2 (en) 1985-05-17

Family

ID=12700167

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4475277A Expired JPS6019646B2 (en) 1977-04-19 1977-04-19 Electromagnetic mechanism for camera release

Country Status (1)

Country Link
JP (1) JPS6019646B2 (en)

Also Published As

Publication number Publication date
JPS53129627A (en) 1978-11-11

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