[go: up one dir, main page]

CN1740895A - Magnetic Aperture Adjuster - Google Patents

Magnetic Aperture Adjuster Download PDF

Info

Publication number
CN1740895A
CN1740895A CN200410068556.0A CN200410068556A CN1740895A CN 1740895 A CN1740895 A CN 1740895A CN 200410068556 A CN200410068556 A CN 200410068556A CN 1740895 A CN1740895 A CN 1740895A
Authority
CN
China
Prior art keywords
magnet
coil
magnetomotive
track
magnetic
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.)
Granted
Application number
CN200410068556.0A
Other languages
Chinese (zh)
Other versions
CN100419565C (en
Inventor
张起豪
张绍雄
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.)
Delta Electronics Inc
Original Assignee
Delta Electronics 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 Delta Electronics Inc filed Critical Delta Electronics Inc
Priority to CNB2004100685560A priority Critical patent/CN100419565C/en
Publication of CN1740895A publication Critical patent/CN1740895A/en
Application granted granted Critical
Publication of CN100419565C publication Critical patent/CN100419565C/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Diaphragms For Cameras (AREA)

Abstract

The invention relates to a magnetic diaphragm regulator, which comprises a yoke iron shaped like a Chinese character 'ri', a first magnet, a second magnet, a coil, a shaft hole rod with a shaft hole, a light screen and a magnetic induction component, wherein the yoke iron is provided with a magnetic pole; the first magnet and the second magnet are respectively positioned in the first through hole and the second through hole of the yoke, the first magnet and the second magnet are arranged in a mode that the same polarities are opposite, the coil is formed by surrounding the track of the yoke, and the magnetic induction component is positioned on the shaft hole rod; when current exists in the coil, the coil makes circular motion by taking the shaft hole as the center of a circle due to the magnetic field effect of the first magnet and the second magnet, and then the shading plate is driven to perform the action of adjusting the size of the aperture; when no current flows in the coil, the magnetic force generated by the magnetic induction component drives the shading plate to return to a preset position.

Description

磁动光圈调节器Magnetic Aperture Adjuster

技术领域technical field

本发明有关一种光圈调节器,特别是有关一种可以应用于一光学装置中,以磁力为动力且具有磁簧回复力功能的磁动光圈调节器。The present invention relates to an aperture adjuster, in particular to a magnetic aperture adjuster which can be applied to an optical device and is driven by magnetic force and has the function of restoring force of a magnetic spring.

背景技术Background technique

在一般的光学装置中,例如是光学投影机、背投式投影机或是照相机等,其中会有一个控制光线的装置,例如是光圈调节器,用来调节光学装置中光线射出的强弱,用以产生具有不同亮度的影像资料;其中,现有技术的光圈调节器大都以动力机构来驱动,而有的是以磁动力来驱动,但是,现有技术中若是希望光圈调节器在不使用时,其遮光板可以自动地回复至一预设位置,通常是借由弹簧来实现。In general optical devices, such as optical projectors, rear projection projectors or cameras, etc., there will be a device for controlling light, such as an aperture adjuster, which is used to adjust the intensity of light emitted from the optical device. It is used to generate image data with different brightness; among them, most of the aperture adjusters in the prior art are driven by power mechanisms, and some are driven by magnetic power. However, in the prior art, if the aperture adjuster is not in use, The visor can automatically return to a preset position, usually by means of a spring.

举例来说,一种现有技术的具备弹性回复力的磁动光圈调节器如图1A至图1E所示,一磁动光圈调节器1包含一轭铁10、一第一磁铁11、一第二磁铁12、一线圈15、一遮光板16、一轴孔杆17以及一弹簧18,其中轭铁10是为一个具有一穿孔107的矩型体,以此现有技术为例,轭铁10是由两个「U」形轭铁块双双以开口端相对所组合而成,而第一磁铁11与第二磁铁12则是位于轭铁10的穿孔107中,且分别贴合于穿孔107内的相对侧,第一磁铁11与第二磁铁12的极性分别位于其较长边的两端且分别交错设置,以本例而言,第一磁铁11与第二磁铁12的极性位置如同图1C所示,第一磁铁11的N极是位于面对线圈15的左侧,而其S极则是位于面对线圈15的右侧,第二磁铁12的的极性位置恰与第一磁铁11相反,其N极是位于面对线圈15的右侧,而其S极则是位于面对线圈15的左侧,如此造成面对线圈15右侧产生一个方向向上的磁场,而面对线圈15左侧产生一个方向向下的磁场,线圈15是由一电线环绕而成,并位于第一磁铁11与第二磁铁12之间,其一侧延伸出一轴孔杆17,轴孔杆17上包含一轴孔170,轴孔170则是枢接于一轴(图中未显示)上,遮光板16则是连接于线圈15的相对于轴孔杆17的另一侧,通常设置于光学装置的光线路径上并与光线路径相互垂直,用以遮蔽光线前进,轴孔杆17上设一弹簧18,弹簧18的两端分别固设于轴孔杆17上以及轭铁10上的任意位置。For example, a prior art magnetic aperture adjuster with elastic restoring force is shown in Figure 1A to Figure 1E, a magnetic aperture adjuster 1 includes a yoke 10, a first magnet 11, a first Two magnets 12, a coil 15, a light-shielding plate 16, a shaft hole rod 17 and a spring 18, wherein the yoke 10 is a rectangular body with a perforation 107, taking this prior art as an example, the yoke 10 It is composed of two "U"-shaped yoke iron blocks with their open ends facing each other, and the first magnet 11 and the second magnet 12 are located in the through hole 107 of the yoke iron 10, and are respectively fitted in the through hole 107 On the opposite side, the polarities of the first magnet 11 and the second magnet 12 are located at the two ends of the longer side respectively and are respectively staggered. In this example, the polar positions of the first magnet 11 and the second magnet 12 are as follows As shown in Figure 1C, the N pole of the first magnet 11 is located on the left side facing the coil 15, and its S pole is located on the right side facing the coil 15, and the polarity position of the second magnet 12 is just the same as that of the first magnet 12. Magnet 11 is opposite, and its N pole is positioned at the right side facing coil 15, and its S pole then is positioned at the left side facing coil 15, causes like this to face the magnetic field that the right side of coil 15 produces a direction upwards, and faces The left side of the coil 15 produces a magnetic field in a downward direction. The coil 15 is surrounded by an electric wire and is located between the first magnet 11 and the second magnet 12. A shaft hole rod 17 extends from one side of the coil. The shaft hole rod 17 includes a shaft hole 170, and the shaft hole 170 is pivotally connected to a shaft (not shown in the figure), and the light shield 16 is connected to the other side of the coil 15 relative to the shaft hole rod 17, and is usually arranged on On the light path of the optical device and perpendicular to the light path, in order to shield the light from advancing, a spring 18 is arranged on the shaft hole rod 17, and the two ends of the spring 18 are respectively fixed on any of the shaft hole rod 17 and the yoke 10. Location.

为了更进一步解说现有技术的磁动光圈调节器1的结构与作动方式,请同时参照图1C至图1E,当线圈15中有电流流过时,其电流方向如图1D中的粗黑箭头所示,以图1D中线圈15的上方侧边为例,由于电流是自右侧流向左侧,而磁场是自下方垂直向上射出纸面,根据右手安培定律,线圈15会产生一个向上的力,由于线圈15的一侧连接于轴孔杆17,而其轴孔170枢接于一轴(图中未显示)上,使得线圈15整体被迫使以轴孔170为圆心沿着A-A′剖面作逆时针圆周运动,其逆时针圆周运动方向如图1D中的空心箭头所示;再以图1D中线圈15的下方侧边为例,由于电流是自左侧流向右侧,而磁场是自上方垂直向下射入纸面,根据右手安培定律,线圈15也会产生一个向上的力,由于其轴孔170的关系,亦使得线圈15整体被迫使以轴孔170为圆心沿着A-A′剖面作逆时针圆周运动,其逆时针圆周运动方向同样如图1D中的空心箭头所示,如此一来,线圈15同时将带动遮光板16以轴孔170为圆心沿着A-A′剖面作逆时针圆周运动,请参照图1E所示,若是准确调整线圈15中的电流量,便可以控制线圈15作圆周运动的角度,进而使遮光板16可以进行调节光圈大小的动作。In order to further explain the structure and operation mode of the magnetic aperture adjuster 1 in the prior art, please refer to FIG. 1C to FIG. 1E at the same time. When a current flows in the coil 15, its current direction is as shown in the thick black arrow in FIG. 1D As shown, taking the upper side of the coil 15 in FIG. 1D as an example, since the current flows from the right to the left, and the magnetic field shoots out of the paper from the bottom vertically, according to the right-hand Ampere’s law, the coil 15 will generate an upward force Since one side of the coil 15 is connected to the shaft hole rod 17, and its shaft hole 170 is pivotally connected to a shaft (not shown in the figure), the coil 15 as a whole is forced to take the shaft hole 170 as the center of the circle along the A-A' section. Counterclockwise circular motion, its counterclockwise circular motion direction is shown by the hollow arrow in Figure 1D; take the lower side of the coil 15 in Figure 1D as an example, since the current flows from the left to the right, and the magnetic field is from the top Injecting vertically downward into the paper surface, according to the right-hand Ampere's law, the coil 15 will also generate an upward force. Due to the relationship between the shaft hole 170, the coil 15 as a whole is forced to take the shaft hole 170 as the center of the circle along the A-A' section. Counterclockwise circular movement, and its counterclockwise circular movement direction is also shown by the hollow arrow in Figure 1D. In this way, the coil 15 will simultaneously drive the visor 16 to perform counterclockwise circular movement along the A-A' section with the shaft hole 170 as the center of the circle Please refer to FIG. 1E, if the current in the coil 15 is accurately adjusted, the angle of the circular motion of the coil 15 can be controlled, so that the visor 16 can adjust the size of the aperture.

当线圈15中没有任何电流流过时,线圈15与第一磁铁11与第二磁铁12之间的磁场便没有任何的磁感应作用,此时,由于弹簧18被拉伸后会产生一个弹性回复力,同时由于其轴孔170的关系,亦使得线圈15整体被迫使以轴孔170为圆心沿着A-A′剖面作顺时针圆周运动,其顺时针圆周运动方向同样如图1E中的空心箭头所示,弹簧18便可将线圈15、轴孔杆17以及遮光板16拉回原来的预设位置上。When there is no current flowing through the coil 15, the magnetic field between the coil 15 and the first magnet 11 and the second magnet 12 does not have any magnetic induction effect. At this time, since the spring 18 is stretched, an elastic restoring force will be generated. At the same time, due to the relationship of the shaft hole 170, the coil 15 as a whole is forced to make a clockwise circular motion along the A-A' section with the shaft hole 170 as the center, and the clockwise circular motion direction is also shown by the hollow arrow in Figure 1E, The spring 18 can pull the coil 15, the shaft hole rod 17 and the light shielding plate 16 back to their original preset positions.

但是,这样的磁动光圈调节器基本上有下列几个缺点,一是这样的线圈结构复杂,不容易制造且生产成本高;另一是由于磁铁的结构设计,使所产生的两个磁场不易均匀,使得线圈中的电流量与线圈的圆周运动相对关系复杂,造成控制不易;其次,这样的磁动光圈调节器为了达到足够的致动能力,其体积通常很大,特别是其宽度无法缩小;此外,以弹簧作为光圈调节器的回复动力,因为其弹簧的弹性回复力会随着弹簧拉伸程度而有改变,也就是说,弹簧拉伸程度愈大,则弹簧回复力就愈大,这使得弹簧的回复力不易控制,此外,弹簧本身会有寿命问题,当长时间拉伸弹簧后,将使得弹簧失去原先的回复力,这些问题都使光学装置的设计者非常头痛。However, such a magnetic aperture adjuster basically has the following disadvantages. One is that the structure of such a coil is complicated, it is not easy to manufacture and the production cost is high; Uniformity makes the relative relationship between the amount of current in the coil and the circular motion of the coil complicated, making it difficult to control; secondly, in order to achieve sufficient actuation capability, such a magnetic aperture adjuster usually has a large volume, especially its width cannot be reduced ;In addition, the spring is used as the restoring force of the aperture adjuster, because the elastic restoring force of the spring will change with the stretching degree of the spring, that is to say, the greater the stretching degree of the spring, the greater the restoring force of the spring. This makes it difficult to control the restoring force of the spring. In addition, the spring itself has a lifespan problem. When the spring is stretched for a long time, the spring will lose its original restoring force. These problems make the designers of optical devices very troublesome.

发明内容Contents of the invention

本发明的目的是提供一种磁动光圈调节器,其特殊的磁力致动结构可以提供更有效率的致动能力,同时,将其感磁组件所提供的磁动力作为光圈调节器的遮光板的回复力,克服现有磁动光圈调节器的缺点。The purpose of the present invention is to provide a magnetic aperture adjuster, its special magnetic actuation structure can provide more efficient actuation capability, and at the same time, the magnetic force provided by its magnetic sensing component can be used as the light shield of the aperture adjuster The recovery force overcomes the shortcomings of the existing magnetic aperture adjuster.

本发明的磁动光圈调节器,应用于一光学装置上,其包含:一轭铁,其包含一第一穿孔以及一第二穿孔,使轭铁形成一外框以及一轨道所组成的「日」字形状,其中轨道是位于第一穿孔与第二穿孔之间,其剖面可为圆弧环形、长方形或是多边环形;一第一磁铁,位于第一穿孔内并与外框内侧贴合;一第二磁铁,位于第二穿孔内并与外框内侧贴合,且第一磁铁与第二磁铁是以相同极性相对设置,其中,第一磁铁与第二磁铁的剖面可为圆弧环形、长方形或是多边环形;一线圈,是以一电线环绕该轨道而成,其一侧延伸出一轴孔杆,其轴孔杆上包含一轴孔;一遮光板,连接于线圈的相对于轴孔的另一侧;一感磁组件,位于轨道的外且连接于线圈的一侧;其中,当线圈中有电流流通时,线圈受到第一磁铁与第二磁铁的磁场感应,使线圈沿着轨道作往复运动,以使遮光板进行调节光圈大小的动作;当线圈中没有电流流通时,感磁组件所产生的磁动力将带动遮光板回复至一预设位置。The magnetic aperture adjuster of the present invention is applied to an optical device, and it includes: a yoke, which includes a first through hole and a second through hole, so that the yoke forms an outer frame and a "day" composed of a track. "" shape, wherein the track is located between the first through hole and the second through hole, and its cross section can be arc-shaped, rectangular or polygonal; a first magnet is located in the first through-hole and attached to the inner side of the outer frame; A second magnet is located in the second through hole and attached to the inner side of the outer frame, and the first magnet and the second magnet are arranged opposite to each other with the same polarity, wherein the cross section of the first magnet and the second magnet can be circular arc ring , rectangular or polygonal ring; a coil is formed by a wire surrounding the track, a shaft hole rod extends from one side, and the shaft hole rod contains a shaft hole; a light shield is connected to the coil relative to the The other side of the shaft hole; a magnetic induction component is located outside the track and connected to one side of the coil; wherein, when there is current flowing in the coil, the coil is induced by the magnetic field of the first magnet and the second magnet, so that the coil moves along the The reciprocating movement along the track enables the shading plate to adjust the size of the aperture; when there is no current flowing in the coil, the magnetic force generated by the magnetic sensing component will drive the shading plate to return to a preset position.

根据上述构想,本发明的感磁组件是为一第三磁铁,感磁组件是受到轨道的磁吸力与磁斥力而产生磁动力,进而带动遮光板回复至预设位置。According to the above idea, the magnetic sensing component of the present invention is a third magnet. The magnetic sensing component is subjected to the magnetic attraction and magnetic repulsion of the track to generate magnetic force, and then drives the visor to return to the preset position.

根据上述构想,本发明的感磁组件是为一第三磁铁,感磁组件是受到一第四磁铁的磁吸力或是磁斥力而产生磁动力,进而带动遮光板回复至预设位置;其中,第四磁铁是位于轭铁上。According to the above idea, the magnetic sensing component of the present invention is a third magnet, and the magnetic sensing component is subjected to the magnetic attraction force or magnetic repulsion force of a fourth magnet to generate magnetic power, and then drive the visor to return to the preset position; wherein, The fourth magnet is located on the yoke.

根据上述构想,本发明的感磁组件是为一金属块,感磁组件是受到一第四磁铁的磁吸力而产生磁动力,进而带动遮光板回复至预设位置;其中,第四磁铁是位于轭铁上。According to the above idea, the magnetic sensing component of the present invention is a metal block, and the magnetic sensing component is subjected to the magnetic attraction force of a fourth magnet to generate magnetic force, and then drives the visor to return to the preset position; wherein, the fourth magnet is located at On the yoke.

根据上述构想,本发明的轭铁是由两L形轭铁板与一ㄇ形轭铁板所组成,其中两个L形轭铁板是以较长边相互贴合并镜射设置,以形成轨道与外框的一侧边,而ㄇ形轭铁板形成外框的另外三侧边。According to the above idea, the yoke iron of the present invention is composed of two L-shaped yoke iron plates and a ㄇ-shaped yoke iron plate, wherein the two L-shaped yoke iron plates are arranged with the longer sides attached to each other and mirrored to form a track and one side of the outer frame, while the ㄇ-shaped yoke iron plates form the other three sides of the outer frame.

根据上述构想,本发明的轭铁是由两ㄇ形轭铁板与一平轭铁板所组成,其中两个ㄇ形轭铁板的一侧边相互贴合且相互镜射设置,并同时将开口面向同一方向,以形成轨道与外框的三个侧边,而平轭铁板用以形成外框的另外一侧边。According to the above idea, the yoke iron of the present invention is composed of two ㄇ-shaped yoke iron plates and a flat yoke iron plate, wherein the sides of the two ㄇ-shaped yoke iron plates are attached to each other and mirrored each other, and at the same time the opening Face the same direction to form the three sides of the track and the outer frame, and the flat yoke iron plate is used to form the other side of the outer frame.

根据上述构想,本发明的磁动光圈调节器,可应用于例如:光学投影机、背投式投影机与照相机等光学装置上。According to the above idea, the magnetic diaphragm adjuster of the present invention can be applied to optical devices such as optical projectors, rear projection projectors and cameras.

附图说明Description of drawings

图1A为现有磁动光圈调节器的立体示意图。FIG. 1A is a three-dimensional schematic diagram of a conventional magnetic aperture adjuster.

图1B为现有磁动光圈调节器的另一个角度的立体示意图。FIG. 1B is a three-dimensional schematic diagram of another angle of the conventional magnetic aperture adjuster.

图1C为现有磁动光圈调节器的前视示意图。FIG. 1C is a schematic front view of a conventional magnetic aperture adjuster.

图1D为沿着图1C中的A-A′线的剖面示意图。FIG. 1D is a schematic cross-sectional view along line A-A' in FIG. 1C.

图1E为当遮光片进行调节光圈大小的动作时,沿着图1C中的A-A′线的剖面示意图。FIG. 1E is a schematic cross-sectional view along line A-A' in FIG. 1C when the light-shielding sheet is in the action of adjusting the size of the aperture.

图2A为本发明第一实施例的磁动光圈调节器的立体示意图。FIG. 2A is a three-dimensional schematic view of the magnetic aperture adjuster according to the first embodiment of the present invention.

图2B为本发明第一实施例的磁动光圈调节器的另一个角度的立体示意图。2B is a schematic perspective view of another angle of the magnetic aperture adjuster according to the first embodiment of the present invention.

图2C为本发明第一实施例的磁动光圈调节器的前视示意图。FIG. 2C is a schematic front view of the magnetic aperture adjuster according to the first embodiment of the present invention.

图2D为沿着图2C中的B-B′线的剖面示意图。FIG. 2D is a schematic cross-sectional view along line B-B' in FIG. 2C.

图2E为沿着图2C中的A-A′线,当遮光板进行调节光圈大小的动作时的剖面示意图。FIG. 2E is a schematic cross-sectional view along the line A-A' in FIG. 2C when the light-shielding plate performs the action of adjusting the size of the aperture.

图2F为沿着图2C中的A-A′线,当磁簧使遮光板进行回复动作时的剖面示意图。FIG. 2F is a schematic cross-sectional view along the line A-A' in FIG. 2C when the magnetic spring makes the visor return.

图2G为沿着图2C中的A-A′线,一种磁簧作动方式的细部结构剖面示意图。FIG. 2G is a schematic cross-sectional view of a detailed structure of a magnetic spring actuation method along the line A-A' in FIG. 2C .

图2H为沿着图2C中的A-A′线,另一种磁簧作动方式的细部结构剖面示意图。FIG. 2H is a schematic cross-sectional view of another magnetic spring actuation method along the line A-A' in FIG. 2C .

图2I为沿着图2C中的A-A′线,再一种磁簧作动方式的细部结构剖面示意图。FIG. 2I is a schematic cross-sectional view of another magnetic spring actuation method along the line A-A' in FIG. 2C .

图2J为沿着图2C中的A-A′线,再一种磁簧作动方式的细部结构剖面示意图。FIG. 2J is a schematic cross-sectional view of another magnetic spring actuation method along the line A-A' in FIG. 2C .

图3为本发明第二实施例的磁动光圈调节器的立体示意图。FIG. 3 is a schematic perspective view of a magnetic aperture adjuster according to a second embodiment of the present invention.

图4为本发明第三实施例的磁动光圈调节器的立体示意图。FIG. 4 is a schematic perspective view of a magnetic aperture adjuster according to a third embodiment of the present invention.

图5为本发明第四实施例的磁动光圈调节器的立体示意图。FIG. 5 is a three-dimensional schematic diagram of a magnetic aperture adjuster according to a fourth embodiment of the present invention.

图6A为一种本发明的磁动光圈调节器的轭铁、第一磁铁以及第二磁铁的组合剖面示意图。FIG. 6A is a schematic cross-sectional view of a combination of a yoke, a first magnet and a second magnet of the magnetic diaphragm adjuster of the present invention.

图6B为另一种本发明的磁动光圈调节器的轭铁、第一磁铁以及第二磁铁的组合剖面示意图。FIG. 6B is a cross-sectional view showing the combination of the yoke, the first magnet and the second magnet of another magnetic aperture adjuster of the present invention.

图6C为再一种本发明的磁动光圈调节器的轭铁、第一磁铁以及第二磁铁的组合剖面示意图。FIG. 6C is a cross-sectional view showing the combination of the yoke, the first magnet and the second magnet of another magnetic aperture adjuster of the present invention.

图6D为再另一种本发明的磁动光圈调节器的轭铁、第一磁铁以及第二磁铁的组合剖面示意图。FIG. 6D is a cross-sectional schematic diagram of another combination of the yoke, the first magnet and the second magnet of the magnetic diaphragm adjuster of the present invention.

具体实施方式Detailed ways

本发明的第一实施例请参照图2A至图2F,如图所示,本发明第一实施例的磁动光圈调节器2包含:一轭铁20、一第一磁铁21、一第二磁铁22、一线圈25、一遮光板26、一轴孔杆27以及一第三磁铁23等;其中轭铁20包含一第一穿孔207以及一第二穿孔208,使轭铁20成为一外框201以及一轨道200的组合体,其中轨道200是位于第一穿孔207与该第二穿孔208之间,其相对关系请参照图2C所示,整体轭铁20的前视图宛如一个「日」字形;第一磁铁21与第二磁铁22分别位于第一穿孔207与第二穿孔208内,同时分别贴合于外框内侧,且第一磁铁21与第二磁铁22是以相同极性相对的方式设置,以本实施例为例,请参照图2C,第一磁铁21的N极向下而S极向上,第二磁铁22的N极向上与第一磁铁21的N极相对,而第二磁铁22的S极向下,因此,在第一穿孔207中形成一由上向下的磁场,而在第二穿孔208中形成一由下向上的磁场,若是第一磁铁21与第二磁铁22的形状大小相等,其上述两个磁场大小亦会相等,上述设置当第一磁铁21与第二磁铁22的极性若是完全相反亦可实施;线圈25是以一电线环绕轨道200而成,轴孔杆27是自线圈25的一侧延伸出,较佳者,轴孔杆27与轨道200相互垂直,其中轴孔杆27上包含一轴孔270,轴孔270与现有技术相同是枢接于一轴(图中未显示)上;遮光板26则是连接于线圈25的相对于轴孔270的另外一侧,通常也是设置于光学装置的光线路径上,其遮光板26的运动方向与光线路径相互垂直,用以遮蔽光线前进,而其遮光板26的形状并不以此为限,凡是可以遮蔽光线前进的皆可;第三磁铁23则是位于轴孔杆27上,请参照图2B所示,但此设置并不以此为限,若是将第三磁铁23设置于遮光板26上,亦可以实施。Please refer to Fig. 2A to Fig. 2F for the first embodiment of the present invention, as shown in the figure, the magnetic aperture adjuster 2 of the first embodiment of the present invention comprises: a yoke 20, a first magnet 21, a second magnet 22. A coil 25, a shading plate 26, a shaft hole rod 27, a third magnet 23, etc.; wherein the yoke 20 includes a first perforation 207 and a second perforation 208, so that the yoke 20 becomes an outer frame 201 And a combination of a track 200, wherein the track 200 is located between the first through hole 207 and the second through hole 208, its relative relationship is shown in Figure 2C, the front view of the overall yoke 20 is like a "day" shape; The first magnet 21 and the second magnet 22 are located in the first through hole 207 and the second through hole 208 respectively, and are attached to the inner side of the outer frame respectively, and the first magnet 21 and the second magnet 22 are arranged in the same polarity opposite manner , taking the present embodiment as an example, please refer to Fig. 2C, the N pole of the first magnet 21 is downward and the S pole is upward, the N pole of the second magnet 22 is upward and opposite to the N pole of the first magnet 21, and the second magnet 22 Therefore, a magnetic field from top to bottom is formed in the first through hole 207, and a magnetic field from bottom to top is formed in the second through hole 208, if the shape of the first magnet 21 and the second magnet 22 Equal in size, the above-mentioned two magnetic field sizes will also be equal. The above-mentioned setting can also be implemented if the polarities of the first magnet 21 and the second magnet 22 are completely opposite; 27 extends from one side of the coil 25. Preferably, the shaft hole rod 27 is perpendicular to the track 200, wherein the shaft hole rod 27 includes a shaft hole 270, which is pivotally connected to a shaft hole 270 as in the prior art. shaft (not shown in the figure); the shading plate 26 is connected to the other side of the coil 25 relative to the shaft hole 270, and is usually also arranged on the light path of the optical device, and the moving direction of the shading plate 26 is related to the light path They are perpendicular to each other and are used to shield the light from advancing, and the shape of the shading plate 26 is not limited thereto, any one that can shield the light from advancing can be used; the third magnet 23 is located on the shaft hole rod 27, please refer to FIG. 2B Shown, but this arrangement is not limited to this, if the third magnet 23 is arranged on the light-shielding plate 26, it can also be implemented.

为了更进一步解说第一实施例的磁动光圈调节器2的结构与作动方式,请同时参照图2C至图2F;当线圈25中有电流流过时,以本实施例为例,其电流方向如图2D中的粗黑箭头所示,请再参照图2D,线圈25的上方侧由于其电流自左流向右,而磁场方向则是由上向下,根据右手安培定律,线圈25会产生进入纸面方向的力;而线圈25的下方侧由于其电流自右流向左,而磁场方向则是由下向上,根据右手安培定律,线圈25亦会产生进入纸面方向的力量,线圈25便会沿着A-A′剖面运动,再者,线圈25连接着轴孔杆27,其轴孔270枢接于一轴(图中未显示)的关系,使得线圈25整体被迫使以轴孔270为圆心沿着A-A′剖面作逆时针圆周运动,其运动方向如图2E的空心箭头方向所示,如此,线圈25因此会带动遮光板26以轴孔270为圆心沿着A-A′剖面作逆时针圆周运动,若是准确调整线圈25中的电流量,便可以控制线圈25作圆周运动的角度,进而使遮光板26可以进行调节光圈大小的动作。In order to further explain the structure and operation mode of the magnetic aperture adjuster 2 of the first embodiment, please refer to FIG. 2C to FIG. 2F at the same time; As shown by the thick black arrow in Figure 2D, please refer to Figure 2D again, because the current on the upper side of the coil 25 flows from left to right, while the direction of the magnetic field is from top to bottom, according to the right-hand Ampere's law, the coil 25 will generate The force in the direction of the paper surface; and the lower side of the coil 25 because its current flows from right to left, while the direction of the magnetic field is from bottom to top, according to the right-hand Ampere's law, the coil 25 will also generate a force entering the direction of the paper, and the coil 25 will Move along the A-A' section, moreover, the coil 25 is connected with the shaft hole rod 27, and its shaft hole 270 is pivotally connected to a shaft (not shown in the figure), so that the coil 25 as a whole is forced to take the shaft hole 270 as the center of the circle along the Make counterclockwise circular movement along the A-A' section, and its movement direction is shown in the direction of the hollow arrow in Figure 2E. In this way, the coil 25 will therefore drive the light shielding plate 26 to make a counterclockwise circular movement along the A-A' section with the shaft hole 270 as the center. If the amount of current in the coil 25 is accurately adjusted, the angle of the circular motion of the coil 25 can be controlled, so that the shading plate 26 can adjust the size of the aperture.

若是线圈25中没有电流流过时,请参照图2F,由于轨道200被第一磁铁21以及第二磁铁22的磁场感应,依本实施例为例,轨道200被感应成为S极,此时,第三磁铁23若是设置于轴孔杆27上,其N极以及S极的设置位置如图2F所示,则第三磁铁23将会受到轨道200的磁感应而产生动力,由于轴孔270枢接于一轴(图中未显示)的关系,使得轴孔杆27被迫使以轴孔270为圆心沿着A-A′剖面作顺时针圆周运动,其顺时针圆周运动方向如图2F中的空心箭头所示,轴孔杆27便带动线圈25、以及遮光板26作顺时针圆周运动,使遮光板26回到预设位置上。If there is no current flowing in the coil 25, please refer to FIG. 2F. Since the track 200 is induced by the magnetic fields of the first magnet 21 and the second magnet 22, according to this embodiment, the track 200 is induced to become an S pole. If the three magnets 23 are arranged on the shaft hole rod 27, the positions of the N pole and the S pole are as shown in FIG. The relationship of a shaft (not shown in the figure) makes the shaft hole rod 27 be forced to make a clockwise circular motion along the A-A' section with the shaft hole 270 as the center, and the clockwise circular motion direction is shown by the hollow arrow in Figure 2F , the shaft hole rod 27 will drive the coil 25 and the light shielding plate 26 to make a clockwise circular movement, so that the light shielding plate 26 will return to the preset position.

上述第三磁铁23与轨道200的组合,因为可以产生使第三磁铁23进行一顺时针圆周运动的功效,可以将整组结构称为「磁簧」,亦即「磁性弹簧」之意,而第三磁铁23便是其中的一个感磁组件,但是,本发明的磁簧作动方式并不以此为限,以下再举出数个可以实施的方式。The above-mentioned combination of the third magnet 23 and the track 200 can produce the effect of making the third magnet 23 perform a clockwise circular motion, and the whole group of structures can be called "magnetic spring", which means "magnetic spring", and The third magnet 23 is one of the magnetic sensing components, however, the magnetic spring actuation method of the present invention is not limited thereto, and several possible implementation methods are listed below.

请参照图2G,本图为沿着图2C中的A-A′线,一种磁簧作动方式的细部结构剖面示意图,图中所示一第三磁铁23是嵌设于轴孔杆27的一侧边上,其S极朝向轴孔杆27的外侧,而其N极朝向轴孔杆27,如此,由于轨道200被感应成为S极的关系,第三磁铁23的S极将受到轨道200的磁斥力,同时,第三磁铁23的N极受到轨道200的磁吸力,再由于轴孔270枢接于一轴(图中未显示)的关系,第三磁铁23受到轨道200的磁感应所产生的磁动力,将带动轴孔杆27产生一顺时针圆周运动,其顺时针圆周运动的方向如图2G的空心箭头所示,此实施方式即为本发明上述的第一实施例所陈述的详细技术。Please refer to Fig. 2G, this figure is along the A-A' line in Fig. 2C, a schematic cross-sectional view of the detailed structure of a magnetic spring actuation mode, a third magnet 23 shown in the figure is a rod 27 embedded in the shaft hole On the side, its S pole is towards the outside of the shaft hole rod 27, and its N pole is towards the shaft hole rod 27. In this way, since the track 200 is induced to become the relationship of the S pole, the S pole of the third magnet 23 will be received by the track 200. At the same time, the N pole of the third magnet 23 is subjected to the magnetic attraction force of the track 200, and because the shaft hole 270 is pivotally connected to a shaft (not shown in the figure), the third magnet 23 is produced by the magnetic induction of the track 200 The magnetic power will drive the shaft hole rod 27 to produce a clockwise circular motion, and the direction of its clockwise circular motion is shown by the hollow arrow in Figure 2G. This implementation mode is the detailed technology stated in the above-mentioned first embodiment of the present invention .

另一种磁簧作动的实施方式请参照图2H,图中所示一第三磁铁23同样嵌设于轴孔杆27的一侧边上,其S极朝向轴孔杆27的外侧,而其N极朝向轴孔杆27,其中,轭铁20的一内侧设置一第四磁铁24,其第四磁铁24的极性设置相对于第三磁铁23,如图2H所示,第四磁铁24位于轭铁20上方侧边的内侧端,其S极向下设置,而其N极向上设置,如此,第三磁铁23的S极恰相对于第四磁铁24的S极,故可以使第三磁铁23感应到一磁斥力,提供作为第三磁铁23磁动力,亦会使轴孔杆27产生一顺时针圆周运动,其顺时针圆周运动的方向如图2H的空心箭头所示;同理,请参照图2I,若是将第四磁铁24位于轭铁20下方侧边的内侧端,其S极向上设置,而其N极向下设置,如此,第三磁铁23的N极恰相对于第四磁铁24的S极,故可以使第三磁铁23感应到一磁吸力,提供作为第三磁铁23磁动力,同样可以使轴孔杆27产生一顺时针圆周运动。Please refer to FIG. 2H for another embodiment of magnetic spring action. A third magnet 23 shown in the figure is also embedded on one side of the shaft hole rod 27, and its S pole faces the outside of the shaft hole rod 27, while Its N pole is towards the shaft hole rod 27, wherein, an inner side of the yoke 20 is provided with a fourth magnet 24, and the polarity of the fourth magnet 24 is set relative to the third magnet 23, as shown in Figure 2H, the fourth magnet 24 Be positioned at the inboard end of the upper side of the yoke 20, its S pole is arranged downwards, and its N pole is arranged upwards, like this, the S pole of the third magnet 23 is just opposite to the S pole of the fourth magnet 24, so the third magnet 23 can be made The magnet 23 senses a magnetic repulsion force, which provides the third magnet 23 with a magnetic force, and also causes the shaft hole rod 27 to generate a clockwise circular motion, and the direction of the clockwise circular motion is shown by the hollow arrow in FIG. 2H; similarly, Please refer to Fig. 2I, if the fourth magnet 24 is positioned at the inner end of the side below the yoke 20, its S pole is arranged upwards, and its N pole is arranged downwards, so that the N pole of the third magnet 23 is just opposite to the fourth magnet 23. The S pole of the magnet 24 can make the third magnet 23 sense a magnetic attraction force, provide the magnetic force as the third magnet 23, and also make the shaft hole rod 27 produce a clockwise circular motion.

另一种磁簧作动的实施方式请参照图2J,图中所示一金属块29嵌设于轴孔杆27的一侧边上,且将一第四磁铁24设置于轭铁20下方侧边的一内侧端,金属块29将受到第四磁铁24的磁感应而产生一磁吸力,这样亦可以使轴孔杆27产生一顺时针圆周运动。Please refer to FIG. 2J for another embodiment of magnetic spring actuation. As shown in the figure, a metal block 29 is embedded on one side of the shaft hole rod 27, and a fourth magnet 24 is arranged on the lower side of the yoke 20. At an inner side end of the side, the metal block 29 will be subjected to the magnetic induction of the fourth magnet 24 to generate a magnetic attraction force, which can also cause the shaft hole rod 27 to generate a clockwise circular motion.

由上述的实施例中的磁动光圈调节器说明可知,由于其磁铁与轭铁的轨道的设计,使磁铁所产生的磁场分布均匀,更因为其线圈包围轨道的设计,使线圈的上方侧与下方侧皆可以受到磁场的感应,产生致动的效果,本发明的线圈的上方侧与下方侧占有线圈大部分的比例,相较于现有技术,在相同的线圈匝数以及面积的情形之下,可以提高致动的效率;同时,本发明设置一感磁组件,可以利用轨道的磁性感应,而产生光圈调节器的遮光板所需要的回复力,使遮光板再不使用时可以回复到预设位置处;本发明上述的第一实施例中,由于其轨道本身沿着A-A′的剖面形状是为一圆弧环形,其所产生的磁场相对于位于轴孔杆上的感磁组件而言,不管感磁组件的位置为何,其所产生的磁簧回复力是为一定值,这可以使光圈调节器的设计者易于规划与设计其磁簧回复力的大小,不致因为设计不当使遮光板回复时形成结构上的破坏。From the description of the magnetic aperture adjuster in the above-mentioned embodiment, it can be seen that due to the design of the track of the magnet and the yoke, the magnetic field generated by the magnet is evenly distributed, and because of the design of the coil surrounding the track, the upper side of the coil is in contact with the track. Both the lower side can be induced by the magnetic field to produce an actuation effect. The upper side and the lower side of the coil of the present invention occupy most of the coil. Compared with the prior art, in the case of the same coil turns and area At the same time, the present invention sets a magnetic induction component, which can use the magnetic induction of the track to generate the restoring force required by the shading plate of the aperture adjuster, so that the shading plate can return to the preset position when it is not in use. Set the position; in the above-mentioned first embodiment of the present invention, since its track itself along the A-A' cross-sectional shape is an arc ring, the magnetic field generated by it is relative to the magnetic sensing assembly located on the shaft hole rod , no matter what the position of the magnetic sensing component is, the magnetic spring restoring force generated by it is a certain value, which can make it easy for the designer of the aperture adjuster to plan and design the magnitude of the magnetic spring restoring force, so that the shading plate will not be damaged due to improper design. Structural damage occurs during recovery.

本发明的第二实施例请参照图3,如图所示,本发明第二实施例的磁动光圈调节器3同样包含:一轭铁30、一第一磁铁31、一第二磁铁32、一线圈35、一具有轴孔370的轴孔杆37、一遮光板36以及一第三磁铁23,其组件的相对位置与功效大致与第一实施例相同,不同处在于本实施例的第一磁铁31以及第二磁铁32的剖面形状是设计成为圆弧环形,更有甚者,第一磁铁31以及第二磁铁32甚至可以设计成为一多边环形(图中未显示),所谓多边环形就是当圆弧环形的圆弧边不连续,较佳者,第一磁铁31以及第二磁铁32的形状与大小相同,这样的设计,不仅在线圈35以轴孔370为圆心作圆周运动时,可以使线圈35不至于因为旋转而与轨道300接触而磨损,而且线圈35整体不致于离开一第一磁铁31与一第二磁铁32的磁场范围进行运动,这样使得线圈45在运动过程中所感应的磁场皆相同,上述设计的优点可以使线圈35的电流量与其线圈35的圆周运动角度成线性正比,使本实施例的磁动光圈调节器3的效能更容易达到设计的预期值。Please refer to Fig. 3 for the second embodiment of the present invention, as shown in the figure, the magnetic diaphragm adjuster 3 of the second embodiment of the present invention also includes: a yoke 30, a first magnet 31, a second magnet 32, A coil 35, a shaft hole rod 37 with a shaft hole 370, a light shielding plate 36 and a third magnet 23, the relative positions and functions of the components are roughly the same as those of the first embodiment, the difference lies in the first embodiment of the present embodiment. The cross-sectional shape of the magnet 31 and the second magnet 32 is designed to be a circular arc ring. What's more, the first magnet 31 and the second magnet 32 can even be designed as a polygonal ring (not shown in the figure). The so-called polygonal ring is When the circular arc edge of the arc ring is discontinuous, preferably, the shape and size of the first magnet 31 and the second magnet 32 are the same. The coil 35 will not be worn out due to the contact with the track 300 due to rotation, and the coil 35 as a whole will not move away from the magnetic field range of a first magnet 31 and a second magnet 32, so that the coil 45 is induced during the movement. The magnetic fields are all the same, and the advantages of the above design can make the current of the coil 35 linearly proportional to the circular motion angle of the coil 35, so that the performance of the magnetic aperture adjuster 3 of this embodiment can more easily reach the expected value of the design.

本发明的第三实施例请见图4,如图所示,本实施例的磁动光圈调节器4同样包含:一轭铁40、一第一磁铁41、一第二磁铁42、一线圈45、一具有轴孔470的轴孔杆47、一遮光板46以及一第三磁铁43,其组件的相对位置与功效大致与第二实施例相同,不同处在于本实施例的第一磁铁41、第二磁铁42以及轨道400的剖面形状亦可以设计成为长方形,同样具有如本发明第一实施例所数的功效。Please refer to Fig. 4 for the third embodiment of the present invention. As shown in the figure, the magnetic aperture adjuster 4 of this embodiment also includes: a yoke 40, a first magnet 41, a second magnet 42, and a coil 45 1. A shaft hole rod 47 with a shaft hole 470, a light-shielding plate 46 and a third magnet 43, the relative position and effect of its components are roughly the same as those of the second embodiment, the difference lies in the first magnet 41 of this embodiment, The cross-sectional shape of the second magnet 42 and the track 400 can also be designed as a rectangle, which also has the effects as mentioned in the first embodiment of the present invention.

本发明的第四实施例请参照图5,如图所示,本例的磁动光圈调节器5同样包含:一轭铁50、一第一磁铁51、一第二磁铁52、一线圈55、一具有轴孔570的轴孔杆57、一遮光板56以及一第三磁铁53,其组件的相对位置与功效大致与第一实施例相同,不同处在于本实施例的一第一磁铁51与一第二磁铁52是位于第一穿孔507与第二穿孔508内而分别贴合于轨道500的两侧,而第一磁铁51与第二磁铁52同样是以相同极性相对的方式设置,其中,以本实施例而言,第一磁铁51的N极向下而S极向上,第二磁铁52的N极向上与第一磁铁51的N极相对,而第二磁铁52的S极向下,因此,在第一穿孔507中形成一由上向下的磁场,而在第二穿孔508中形成一由下向上的磁场,同理,若是第一磁铁51与第二磁铁52的形状大小相等,其上述两个磁场大小亦会相等;而本实施例的线圈55则是环绕着轨道500、第一磁铁51以及第二磁铁52而成,详细的作动方式将与第一实施例相似,在此不在赘述,其中,第三磁铁53与第一实施例的第三磁铁23相同,使磁动光圈调节器5具有磁性回复力的功能。Please refer to Fig. 5 for the fourth embodiment of the present invention. As shown in the figure, the magnetic aperture adjuster 5 of this example also includes: a yoke 50, a first magnet 51, a second magnet 52, a coil 55, A shaft hole rod 57 with a shaft hole 570, a light-shielding plate 56 and a third magnet 53, the relative position and effect of its components are roughly the same as those of the first embodiment, except that the first magnet 51 and the third magnet of this embodiment are different. A second magnet 52 is located in the first through hole 507 and the second through hole 508 and is attached to both sides of the track 500 respectively, and the first magnet 51 and the second magnet 52 are also arranged in the same polarity opposite manner, wherein In this embodiment, the N pole of the first magnet 51 is downward and the S pole is upward, the N pole of the second magnet 52 is upwardly opposite to the N pole of the first magnet 51, and the S pole of the second magnet 52 is downward , Therefore, a magnetic field from top to bottom is formed in the first through hole 507, and a magnetic field from bottom to top is formed in the second through hole 508. Similarly, if the shapes and sizes of the first magnet 51 and the second magnet 52 are equal , the magnitudes of the above two magnetic fields will also be equal; and the coil 55 of this embodiment is formed around the track 500, the first magnet 51 and the second magnet 52, and the detailed action mode will be similar to that of the first embodiment. No need to go into details here, wherein, the third magnet 53 is the same as the third magnet 23 in the first embodiment, so that the magnetic diaphragm adjuster 5 has the function of magnetic restoring force.

上述各个实施例中的轭铁,其前视图大致是成「日」字形,为了制作上的便利,轭铁可以为数个轭铁板所组成;例如第一实施例中的轭铁20,为了解说的方便,请参照图6A,轭铁20是由两L形轭铁板202、202′与一ㄇ形轭铁板203所组成,其中两个L形轭铁板202、202′是以较长边相互贴合镜射设置,其较长边相互贴合即形成轨道200,而L形轭铁板202、202′的另一边即形成外框201的一侧边,而ㄇ形轭铁板203再形成外框201的另外三侧边,即可形成一「日」字形的轭铁20,这样的作法,在制造的过程中可以当两个L形轭铁板202、202′贴合镜射设置后就可以将线圈置入轨道200中,之后再将ㄇ形轭铁板203与两个L形轭铁板202、202′连接后完成轭铁20的制作。The front view of the yoke in each of the above-mentioned embodiments is roughly in the shape of a "day". For the convenience of manufacture, the yoke can be composed of several yoke plates; for example, the yoke 20 in the first embodiment, for illustration For convenience, please refer to Fig. 6A, the yoke 20 is composed of two L-shaped yoke plates 202, 202' and a ㄇ-shaped yoke plate 203, wherein the two L-shaped yoke plates 202, 202' are longer The sides are attached to each other and mirrored, and the longer sides are attached to each other to form the track 200, and the other side of the L-shaped yoke iron plate 202, 202' forms one side of the outer frame 201, and the ㄇ-shaped yoke iron plate 203 Then form the other three sides of the outer frame 201 to form a "day"-shaped yoke 20. In this way, during the manufacturing process, two L-shaped yoke plates 202, 202' can be laminated and mirrored. After setting, the coil can be put into the track 200 , and then the U-shaped yoke plate 203 is connected with the two L-shaped yoke plates 202 , 202 ′ to complete the manufacture of the yoke 20 .

另一种轭铁20的实施方式请参照图6B所示,其L形轭铁板202、202′的较短边可以延伸至线圈20的外框201的边缘上,再将ㄇ形轭铁板203与两个L形轭铁板202、202′的内缘接合连接后完成轭铁20的制作。Another embodiment of the yoke 20 is shown in FIG. 6B. The shorter sides of the L-shaped yoke plates 202, 202′ can extend to the edge of the outer frame 201 of the coil 20, and then the ㄇ-shaped yoke plates 203 is connected with the inner edges of the two L-shaped yoke plates 202 and 202 ′ to complete the manufacture of the yoke 20 .

另一种轭铁20实施方式请参照图6C所示,轭铁20是由两ㄇ形轭铁板204、204′与一平轭铁板205所组成,其中两个ㄇ形轭铁板204、204′是以较长边相互贴合镜射设置,同时将开口面向同一方向,其中,相互贴合的一边即形成轨道200,如此即形成轨道200以及外框201的三个侧边,最后,再将平轭铁板205设置于ㄇ形轭铁板204、204′的开口端,形成外框201的另外一侧边,即可形成一「日」字形的轭铁20;其平轭铁板205可以延伸至线圈20的外框201的边缘上,如图6C所示,亦可以内缩于ㄇ形轭铁板204、204′的相互贴合的一侧的另一侧边的内缘,如图6D所示,同样可以制作出一「日」字形的轭铁20当然,本发明的构想并不以此为限,这仅是制作「日」字形的轭铁20的数个实施方式而已。Another embodiment of the yoke 20 is shown in FIG. 6C. The yoke 20 is composed of two ㄇ-shaped yoke plates 204, 204′ and a flat yoke plate 205, wherein the two ㄇ-shaped yoke plates 204, 204 ′ is arranged by mirroring the longer sides to fit each other, and at the same time, the opening faces the same direction, wherein, the side that fits each other forms the track 200, thus forming the track 200 and the three sides of the outer frame 201, and finally, The flat yoke iron plate 205 is arranged on the open end of the ㄇ-shaped yoke iron plate 204, 204' to form the other side of the outer frame 201, and a "day"-shaped yoke iron 20 can be formed; the flat yoke iron plate 205 It can extend to the edge of the outer frame 201 of the coil 20, as shown in FIG. 6C, or it can be retracted to the inner edge of the other side of the side of the ㄇ-shaped yoke iron plates 204, 204' that are attached to each other, as shown in FIG. As shown in FIG. 6D , a Japanese-shaped yoke 20 can also be manufactured. Of course, the concept of the present invention is not limited thereto, and these are just several implementations of making a "Japanese"-shaped yoke 20 .

以上所述仅为本发明的较佳实施例,上述实施例仅是用来说明而非用以限定本发明的申请专利范围,本发明的范畴是由以下的本申请权利要求范围所界定。凡依本申请权利要求范围所作的等效的改变或替换,皆应属本发明的涵盖范围。The above descriptions are only preferred embodiments of the present invention. The above embodiments are only used to illustrate but not to limit the scope of the present invention. The scope of the present invention is defined by the scope of the following claims of the present application. All equivalent changes or substitutions made according to the scope of the claims of the present application shall fall within the scope of the present invention.

Claims (24)

1. Magnetomotive iris aperture regulator, it comprises:
One yoke, it comprises one first perforation and one second perforation, so that this yoke forms a housing and a track, wherein this track is between this first perforation and this second perforation;
One first magnet is positioned at this first perforation and close this housing place;
One second magnet is positioned at this second perforation and close this housing place;
One coil is to form around this track with a staple for electric wire;
One shadow shield is connected in a side of this coil;
One sense magnetic assembly is positioned at the outer of this track and is connected in a side of this coil;
Wherein, when in this coil current flowing being arranged, this coil is subjected to the magnetic field induction of this first magnet and this second magnet, makes this coil reciprocating along this track, so that this shadow shield is regulated the action of aperture size; When not having current flowing in this coil, the magnetomotive that this sense magnetic assembly is produced will drive this shadow shield and return back to a predeterminated position.
2. Magnetomotive iris aperture regulator as claimed in claim 1, it is characterized in that described sense magnetic assembly is to be one the 3rd magnet, this sense magnetic assembly is to be subjected to the magnetic induction of this track and to produce magnetomotive, and then drive this shadow shield and return back to this predeterminated position, wherein said magnetic induction comprises magnetic attraction and magnetic repulsion.
3. Magnetomotive iris aperture regulator as claimed in claim 1, it is characterized in that described sense magnetic assembly is to be one the 3rd magnet, this sense magnetic assembly is to be subjected to being positioned at the magnetic induction of one the 4th magnet on this yoke and to produce magnetomotive, and then drive this shadow shield and return back to this predeterminated position, wherein said magnetic induction is to be magnetic attraction or magnetic repulsion.
4. Magnetomotive iris aperture regulator as claimed in claim 1, it is characterized in that described sense magnetic assembly is to be a derby, this sense magnetic assembly is to be subjected to being positioned at the magnetic induction of one the 4th magnet on this yoke and to produce magnetomotive, and then drive this shadow shield and return back to this predeterminated position, wherein said magnetic induction is to be magnetic attraction.
5. Magnetomotive iris aperture regulator as claimed in claim 1 is characterized in that this track is to be selected from following shape along the section shape of the direction of motion of coil: circular arc annular, rectangle and polygon annular.
6. Magnetomotive iris aperture regulator as claimed in claim 1, it is characterized in that this first magnet is to fit in this first perforation and with this housing is inboard, and this second magnet is to fit in this second perforation and with this housing is inboard, and this first magnet and this second magnet are to be oppositely arranged with identical polar, and this first magnet is identical with size with the shape of this second magnet.
7. Magnetomotive iris aperture regulator as claimed in claim 1 is characterized in that this first magnet and this second magnet are to be selected from following shape respectively along the section shape of the direction of motion of coil: circular arc annular, rectangle and polygon annular.
8. Magnetomotive iris aperture regulator as claimed in claim 1 is characterized in that this sense magnetic assembly is to be positioned on this shadow shield.
9. Magnetomotive iris aperture regulator as claimed in claim 1, it is characterized in that also comprising an axis hole bar, the opposite side with respect to this shadow shield from this coil extends, this axis hole bar comprises an axis hole, when in this coil current flowing being arranged, this coil is the magnetic field induction that is subjected to this first magnet and this second magnet, making this coil is that circular motion is made along this track in the center of circle with this axis hole, so that this shadow shield is regulated the action of aperture size, wherein this axis hole bar is vertical mutually with this track, and wherein this sense magnetic assembly is to be positioned on this axis hole bar.
10. Magnetomotive iris aperture regulator as claimed in claim 1, it is characterized in that this yoke is made up of two L shaped yoke plates and a ㄇ shape yoke plate, wherein this L shaped yoke plate mirror is provided with, and forming a side of this track and this housing, and this ㄇ shape yoke plate forms other three sides of this housing.
11. Magnetomotive iris aperture regulator as claimed in claim 1, it is characterized in that this yoke is made up of two ㄇ shape yoke plates and a flat yoke plate, wherein a side of this ㄇ shape yoke plate is fitted and mirror setting mutually mutually, and simultaneously with opening surface to same direction, forming three sides of this track and this housing, and this flat yoke plate is in order to form an other side of this housing.
12. Magnetomotive iris aperture regulator as claimed in claim 1 is characterized in that this Magnetomotive iris aperture regulator is applied on the optical devices, wherein said optical devices are for one of following: optical projector, back projecting projector and camera.
13. a Magnetomotive iris aperture regulator, it comprises:
One yoke, it comprises one first perforation and one second perforation, so that this yoke forms a housing and a track, wherein this track is between this first perforation and this second perforation;
One first magnet is positioned at this first perforation and side of this track of fitting;
One second magnet is positioned at this second perforation and opposite side of this track of fitting;
One coil is to form around this track, this first magnet and this second magnet simultaneously with an electric wire;
One shadow shield is connected in a side of this coil;
One sense magnetic assembly is positioned at the outer of this track and is connected in a side of this coil;
Wherein, when in this coil current flowing being arranged, this coil is subjected to the magnetic field induction of this first magnet and this second magnet, makes this coil reciprocating along this track, so that this shadow shield is regulated the action of aperture size; When not having current flowing in this coil, the magnetomotive that this sense magnetic assembly is produced will drive this shadow shield and return back to a predeterminated position.
14. Magnetomotive iris aperture regulator as claimed in claim 13, it is characterized in that described sense magnetic assembly is to be one the 3rd magnet, this sense magnetic assembly is subjected to the magnetic induction of this track and produces magnetomotive, and then drive this shadow shield and return back to this predeterminated position, wherein said magnetic induction comprises magnetic attraction and magnetic repulsion.
15. Magnetomotive iris aperture regulator as claimed in claim 13, it is characterized in that described sense magnetic assembly is to be one the 3rd magnet, this sense magnetic assembly is subjected to being positioned at the magnetic induction of one the 4th magnet on this yoke and produces magnetomotive, and then drive this shadow shield and return back to this predeterminated position, wherein, the 4th magnet is to be positioned on this yoke, and described magnetic induction is to be magnetic attraction or magnetic repulsion.
16. Magnetomotive iris aperture regulator as claimed in claim 13, it is characterized in that described sense magnetic assembly is to be a derby, this sense magnetic assembly is subjected to being positioned at the magnetic induction of one the 4th magnet on this yoke and produces magnetomotive, and then drive this shadow shield and return back to this predeterminated position, wherein said magnetic induction is to be magnetic attraction.
17. Magnetomotive iris aperture regulator as claimed in claim 13 is characterized in that this track is to be selected from following shape along the section shape of the direction of motion of coil: circular arc annular, rectangle and polygon annular.
18. Magnetomotive iris aperture regulator as claimed in claim 13 is characterized in that this first magnet and this second magnet are to be selected from following shape respectively along the section shape of the direction of motion of coil: circular arc annular, rectangle and polygon annular.
19. Magnetomotive iris aperture regulator as claimed in claim 13 is characterized in that this first magnet and this second magnet are to be oppositely arranged with identical polar, this first magnet is identical with size with the shape of this second magnet.
20. Magnetomotive iris aperture regulator as claimed in claim 13 is characterized in that this sense magnetic assembly is to be positioned on this shadow shield.
21. Magnetomotive iris aperture regulator as claimed in claim 13, it is characterized in that also comprising an axis hole bar, the opposite side with respect to this shadow shield from this coil extends, this axis hole bar comprises an axis hole, when in this coil current flowing being arranged, this coil is the magnetic field induction that is subjected to this first magnet and this second magnet, making this coil is that circular motion is made along this track in the center of circle with this axis hole, so that this shadow shield is regulated the action of aperture size, in this axis hole bar vertical mutually with this track, and this sense magnetic assembly is to be positioned on this axis hole bar.
22. Magnetomotive iris aperture regulator as claimed in claim 13, it is characterized in that this yoke is made up of two L shaped yoke plates and a ㄇ shape yoke plate, wherein this L shaped yoke plate mirror is provided with, and forming a side of this track and this housing, and this ㄇ shape yoke plate forms other three sides of this housing.
23. Magnetomotive iris aperture regulator as claimed in claim 13, it is characterized in that this yoke is made up of two ㄇ shape yoke plates and a flat yoke plate, wherein a side of this ㄇ shape yoke plate is fitted and mirror setting mutually mutually, and simultaneously with opening surface to same direction, forming three sides of this track and this housing, and this flat yoke plate is in order to form an other side of this housing.
24. Magnetomotive iris aperture regulator as claimed in claim 13 is characterized in that this Magnetomotive iris aperture regulator is applied on the optical devices, wherein said optical devices are for one of following: optical projector, back projecting projector and camera.
CNB2004100685560A 2004-08-26 2004-08-26 Magnetic diaphragm regulator Expired - Fee Related CN100419565C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNB2004100685560A CN100419565C (en) 2004-08-26 2004-08-26 Magnetic diaphragm regulator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNB2004100685560A CN100419565C (en) 2004-08-26 2004-08-26 Magnetic diaphragm regulator

Publications (2)

Publication Number Publication Date
CN1740895A true CN1740895A (en) 2006-03-01
CN100419565C CN100419565C (en) 2008-09-17

Family

ID=36093322

Family Applications (1)

Application Number Title Priority Date Filing Date
CNB2004100685560A Expired - Fee Related CN100419565C (en) 2004-08-26 2004-08-26 Magnetic diaphragm regulator

Country Status (1)

Country Link
CN (1) CN100419565C (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106998429A (en) * 2016-01-26 2017-08-01 浙江大华技术股份有限公司 A kind of video camera and adjusting method for automatically adjusting sunshield
CN115308972A (en) * 2022-08-12 2022-11-08 珲春兆景电子科技有限公司 Shielding device and electronic equipment adopting same

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5528086A (en) * 1978-08-22 1980-02-28 Canon Inc Electromagnetically driven shutter device
JPS60245460A (en) * 1984-05-16 1985-12-05 Hitachi Metals Ltd Electromagnetic drive device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106998429A (en) * 2016-01-26 2017-08-01 浙江大华技术股份有限公司 A kind of video camera and adjusting method for automatically adjusting sunshield
CN106998429B (en) * 2016-01-26 2020-02-14 浙江大华技术股份有限公司 Camera capable of automatically adjusting sun-shading cover and adjusting method
CN115308972A (en) * 2022-08-12 2022-11-08 珲春兆景电子科技有限公司 Shielding device and electronic equipment adopting same

Also Published As

Publication number Publication date
CN100419565C (en) 2008-09-17

Similar Documents

Publication Publication Date Title
TWI737875B (en) Light path adjustment mechanism and fabrication method thereof
CN1265410C (en) Electromagnetic operating device
CN103809347B (en) Photographic head aperture and control and regulation method thereof
TWI698696B (en) Light path adjustment mechanism and fabrication method thereof
KR101177185B1 (en) Camera shutter device
CN112867960A (en) Optical device for enhancing image resolution or reducing speckle noise
US7455466B2 (en) Magnetic actuator for adjusting an iris diaphragm in an optical device
CN1740895A (en) Magnetic Aperture Adjuster
US7239052B2 (en) Magnetic actuators
TWI744445B (en) Light path adjustment mechanism and fabrication method thereof
CN100435019C (en) Magnetic diaphragm regulator
CN210781137U (en) Optical modules and projectors
TWI463238B (en) The magnet block structure of the auto focus module
TWI328713B (en)
KR20110096375A (en) Camera shutter device
DE102021122252B4 (en) Projection system
CN115509064B (en) Intelligent optical device and variable aperture mechanism thereof
KR101128149B1 (en) Shutter device
CN200972530Y (en) Miniature multi-stage lens drive device
CN101055406A (en) swing device
JP6432045B2 (en) Actuator and lens barrel provided with actuator
CN110007458A (en) Light-path adjusting mechanism and its manufacturing method
CN211454071U (en) Lens driving device and base
CN219916155U (en) Pixel expansion device and projection equipment
CN101055409A (en) Optical lens group and its swinging device

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20080917

Termination date: 20200826

CF01 Termination of patent right due to non-payment of annual fee