TW202336360A - Electromagnetic pull-in assembly and brake - Google Patents
Electromagnetic pull-in assembly and brake Download PDFInfo
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- 230000005291 magnetic effect Effects 0.000 claims abstract description 137
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims abstract description 14
- 238000009434 installation Methods 0.000 claims description 21
- 230000007423 decrease Effects 0.000 claims description 7
- 230000006698 induction Effects 0.000 abstract description 16
- 238000013461 design Methods 0.000 description 14
- 238000000034 method Methods 0.000 description 14
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- 230000000694 effects Effects 0.000 description 4
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- 230000008859 change Effects 0.000 description 3
- 230000005389 magnetism Effects 0.000 description 3
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- 239000004020 conductor Substances 0.000 description 2
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F16—ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
- F16D—COUPLINGS FOR TRANSMITTING ROTATION; CLUTCHES; BRAKES
- F16D65/00—Parts or details
- F16D65/14—Actuating mechanisms for brakes; Means for initiating operation at a predetermined position
- F16D65/16—Actuating mechanisms for brakes; Means for initiating operation at a predetermined position arranged in or on the brake
Abstract
Description
本案屬於機械制動技術領域,具體涉及一種電磁吸合組件及制動器。This case belongs to the field of mechanical braking technology, specifically involving an electromagnetic attraction component and a brake.
傳統形式的電磁制動器在設計時,磁軛鐵芯的內部設有用於安裝線圈的環形槽,環形槽在軸向切面上的截面為矩形,對應的線圈的截面也為矩形。根據安培環路定理,通電導體周圍會形成封閉磁場,且磁場方向與電流方向垂直,同理,當線圈中通入勵磁電流時,環繞線圈的磁軛鐵芯和銜鐵中會產生磁場,在銜鐵和磁軛鐵芯沿徑向的厚度一定的情況下,銜鐵的內圈和磁軛鐵芯的內圈對應的圓周面面積較小,則磁力線分布較密集,單位面積通過的磁力線較多;銜鐵的外周和磁軛鐵芯的外周對應的圓周面面積較大,則磁力線分布較稀疏,單位面積通過的磁力線較少,則制動器內的徑向上磁路的磁感應強度分布不均,當徑向內側(對應磁軛鐵芯的內圈和銜鐵的內圈)磁路的磁場飽和時,徑向外側(對應磁軛鐵芯的外圈和銜鐵的外圈)磁路的磁場未飽和,從磁場角度看,不僅材料利用率不高,而且限制了銜鐵與磁軛鐵芯之間的氣隙中的磁力,又由於磁力是用來克服制動器的彈簧力,最終也限制了制動器的制動力矩。When designing a traditional electromagnetic brake, the inside of the yoke core is provided with an annular groove for installing the coil. The cross section of the annular groove on the axial section is rectangular, and the corresponding cross section of the coil is also rectangular. According to Ampere's loop theorem, a closed magnetic field will be formed around the energized conductor, and the direction of the magnetic field is perpendicular to the direction of the current. Similarly, when the excitation current is passed into the coil, a magnetic field will be generated in the yoke core and armature surrounding the coil. When the thickness of the armature and the yoke core in the radial direction is constant, the corresponding circumferential surface area of the inner ring of the armature and the inner ring of the yoke core is smaller, so the magnetic field lines are densely distributed, and more magnetic field lines pass through the unit area; If the circumferential area corresponding to the outer circumference of the armature and the outer circumference of the yoke core is larger, the distribution of magnetic field lines will be sparse, and fewer magnetic field lines will pass through per unit area. Therefore, the magnetic induction intensity of the radial magnetic circuit in the brake will be unevenly distributed. When the radial direction When the magnetic field of the magnetic circuit on the inner side (corresponding to the inner ring of the yoke core and the inner ring of the armature) is saturated, the magnetic field of the magnetic circuit on the radially outer side (corresponding to the outer ring of the yoke core and the outer ring of the armature) is not saturated. From the magnetic field From a perspective, not only is the material utilization rate not high, but it also limits the magnetic force in the air gap between the armature and the yoke core. Since the magnetic force is used to overcome the spring force of the brake, it ultimately limits the braking torque of the brake.
本案實施例提供一種電磁吸合組件及制動器,旨在解決磁場局部飽和導致制動力矩受限的技術問題,從而能夠防止制動器內磁路的磁場局部飽和,使得磁感應強度均勻分布,進而提高制動器的制動力矩。The embodiment of this case provides an electromagnetic attraction component and a brake, aiming to solve the technical problem of limited braking torque caused by local saturation of the magnetic field, thereby preventing local saturation of the magnetic field in the magnetic circuit within the brake, making the magnetic induction intensity evenly distributed, thereby improving the braking performance of the brake. moment.
第一方面,本案實施例提供一種電磁吸合組件,包括:In the first aspect, the embodiment of this case provides an electromagnetic attraction component, including:
磁軛鐵芯,該磁軛鐵芯上同軸設有環形的安裝槽,該安裝槽開口朝向該磁軛鐵芯的第一軸側;銜鐵,設於該磁軛鐵芯的第一軸側,該銜鐵具有朝向或遠離該磁軛鐵芯移動的自由度,該銜鐵對應於該安裝槽開口處區域形成有環形的對應面,該對應面與該安裝槽形成環形的磁路空間,該磁路空間的寬度沿背離該磁軛鐵芯軸線的方向逐漸增加,該磁路空間的寬度方向平行於該磁軛鐵芯的軸線方向;以及線圈,置於該磁路空間內,該線圈能在通電時產生磁場,以使該銜鐵朝向該磁軛鐵芯移動。The yoke core is coaxially provided with an annular mounting slot, and the opening of the mounting slot faces the first axial side of the yoke core; the armature is located on the first axial side of the yoke core, The armature has the freedom to move toward or away from the yoke core. The armature is formed with an annular corresponding surface corresponding to the opening area of the mounting slot. The corresponding surface and the mounting slot form an annular magnetic circuit space. The magnetic circuit The width of the space gradually increases in a direction away from the axis of the yoke core, and the width direction of the magnetic circuit space is parallel to the axis direction of the yoke core; and a coil is placed in the magnetic circuit space, and the coil can be energized A magnetic field is generated to cause the armature to move toward the yoke core.
結合第一方面,在一種可能的實現方式中,該磁路空間的截面形狀為直角梯形,該安裝槽的槽底面為錐面,該對應面為平面。In connection with the first aspect, in a possible implementation manner, the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the bottom surface of the installation groove is a tapered surface, and the corresponding surface is a flat surface.
一些實施例中,該線圈的截面形狀為矩形;或,該線圈的截面形狀為直角梯形,以在背離該銜鐵的一側面形成錐面,該線圈的錐面能貼合於該安裝槽的槽底面的錐面。In some embodiments, the cross-sectional shape of the coil is a rectangle; or, the cross-sectional shape of the coil is a right-angled trapezoid to form a tapered surface on a side away from the armature, and the tapered surface of the coil can fit into the groove of the mounting slot. The conical surface of the base.
結合第一方面,在一種可能的實現方式中,該磁路空間的截面形狀為直角梯形,該安裝槽的槽底面為平面,該對應面為錐面;或,該磁路空間的截面為等腰梯形,該安裝槽的槽底面和該對應面均為錐面。In conjunction with the first aspect, in one possible implementation, the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the bottom surface of the installation groove is a flat surface, and the corresponding surface is a tapered surface; or, the cross-section of the magnetic circuit space is equal to The waist is trapezoidal, and the bottom surface of the installation groove and the corresponding surface are both tapered surfaces.
一些實施例中,該銜鐵包括由內向外依次同軸設置的內環板、中間環板以及外環板,該中間環板的內圈與該安裝槽的內圈平齊,該中間環板的外圈與該安裝槽的外圈平齊,該內環板、該中間環板以及該外環板背離該線圈的一側面平齊,該中間環板朝向該線圈的一側面形成該對應面;該中間環板的厚度沿背離該磁軛鐵芯軸線的方向逐漸減小,以使該對應面形成錐面。In some embodiments, the armature includes an inner ring plate, an intermediate ring plate and an outer ring plate arranged coaxially in sequence from the inside to the outside. The inner ring of the intermediate ring plate is flush with the inner ring of the installation groove, and the outer ring of the intermediate ring plate is flush with the inner ring of the mounting groove. The ring is flush with the outer ring of the installation groove, the inner ring plate, the middle ring plate and the side of the outer ring plate facing away from the coil are flush, and the side of the middle ring plate facing the coil forms the corresponding surface; The thickness of the intermediate ring plate gradually decreases in a direction away from the axis of the yoke core, so that the corresponding surface forms a tapered surface.
一些實施例中,該內環板的厚度與該中間環板的最大厚度相等,該外環板的厚度與該中間環板的最小厚度相等。In some embodiments, the thickness of the inner ring plate is equal to the maximum thickness of the middle ring plate, and the thickness of the outer ring plate is equal to the minimum thickness of the middle ring plate.
一些實施例中,該磁軛鐵芯包括處於該安裝槽外圈的第一環形部和處於該安裝槽內圈的第二環形部,該第一環形部的厚度大於該第二環形部的厚度,該第一環形部和該外環板之間的間隔等於該第二環形部和該內環板之間的間隔。In some embodiments, the yoke core includes a first annular portion located on the outer ring of the mounting groove and a second annular portion located on the inner ring of the mounting groove. The thickness of the first annular portion is greater than that of the second annular portion. The thickness of the first annular portion and the outer annular plate is equal to the distance between the second annular portion and the inner annular plate.
一些實施例中,該第一環形部和該外環板之間形成第一氣隙面,該第二環形部和該內環板之間形成第二氣隙面,該第一氣隙面和該第二氣隙面均垂直於該磁軛鐵芯的軸線,且該第一氣隙面和該第二氣隙面不共面。In some embodiments, a first air gap surface is formed between the first annular portion and the outer ring plate, and a second air gap surface is formed between the second annular portion and the inner ring plate. The first air gap surface The first air gap surface and the second air gap surface are both perpendicular to the axis of the yoke core, and the first air gap surface and the second air gap surface are not coplanar.
一些實施例中,該內環板的厚度與該外環板的厚度相等,該內環板的厚度等於該中間環板的最大厚度,使得該中間環板與該外環板形成避讓該線圈的第一凹槽。In some embodiments, the thickness of the inner ring plate is equal to the thickness of the outer ring plate, and the thickness of the inner ring plate is equal to the maximum thickness of the middle ring plate, so that the middle ring plate and the outer ring plate form a gap to avoid the coil. First groove.
一些實施例中,該磁軛鐵芯包括處於該安裝槽外圈的第一環形部和處於該安裝槽內圈的第二環形部,該第一環形部的厚度等於該第二環形部的厚度,該第一環形部和該外環板之間的間隔等於該第二環形部和該內環板之間的間隔。In some embodiments, the yoke core includes a first annular portion located on the outer ring of the mounting groove and a second annular portion located on the inner ring of the mounting groove, and the thickness of the first annular portion is equal to that of the second annular portion. The thickness of the first annular portion and the outer annular plate is equal to the distance between the second annular portion and the inner annular plate.
一些實施例中,該第一環形部和該外環板之間形成第一氣隙面,該第二環形部和該內環板之間形成第二氣隙面,該第一氣隙面和該第二氣隙面均垂直於該磁軛鐵芯的軸線,且該第一氣隙面和該第二氣隙面共面。In some embodiments, a first air gap surface is formed between the first annular portion and the outer ring plate, and a second air gap surface is formed between the second annular portion and the inner ring plate. The first air gap surface The first air gap surface and the second air gap surface are both perpendicular to the axis of the yoke core, and the first air gap surface and the second air gap surface are coplanar.
一些實施例中,該線圈的截面形狀為矩形;或,該線圈的截面形狀為適應於該磁路空間截面形狀的梯形。In some embodiments, the cross-sectional shape of the coil is a rectangle; or, the cross-sectional shape of the coil is a trapezoid adapted to the spatial cross-sectional shape of the magnetic circuit.
結合第一方面,在一種可能的實現方式中,該磁路空間的截面形狀為普通梯形,該安裝槽的槽底面和該對應面均為錐面。In connection with the first aspect, in a possible implementation manner, the cross-sectional shape of the magnetic circuit space is a common trapezoid, and the bottom surface of the installation groove and the corresponding surface are both tapered surfaces.
一些實施例中,該線圈的截面形狀為矩形;或,該線圈的截面形狀為適應於該磁路空間截面形狀的梯形。In some embodiments, the cross-sectional shape of the coil is a rectangle; or, the cross-sectional shape of the coil is a trapezoid adapted to the spatial cross-sectional shape of the magnetic circuit.
第二方面,本案實施例還提供了一種制動器,包括上述電磁吸合組件。In a second aspect, this embodiment also provides a brake, including the above-mentioned electromagnetic attraction component.
本案實施例所示的方案,與習知技術相比,本案電磁吸合組件中銜鐵和磁軛鐵芯形成的磁路空間的寬度沿背離磁軛鐵芯的軸向逐漸增加,在磁路空間的變化趨勢下,則銜鐵和/或磁軛鐵芯的內圈圓周面的面積近似等於或略小於外圈圓周面的面積,進而使得內圈和外圈單位面積通過的磁力線密度接近,使得磁感應強度接近或均勻,相較於傳統截面為矩形的磁路空間,本案實施例結構可以在相同的線圈磁動勢下,產生較大的氣隙磁力,從而可以克服更大的彈簧力,增大制動器的制動力矩。In the solution shown in the embodiment of this case, compared with the conventional technology, the width of the magnetic circuit space formed by the armature and the yoke core in the electromagnetic attraction assembly of this case gradually increases along the axial direction away from the yoke core. In the magnetic circuit space Under the changing trend, the area of the inner ring circumferential surface of the armature and/or the yoke iron core is approximately equal to or slightly smaller than the area of the outer ring circumferential surface, thus making the density of magnetic field lines passing through the inner ring and outer ring per unit area close, making the magnetic induction The strength is close to or uniform. Compared with the traditional magnetic circuit space with a rectangular cross-section, the structure of the embodiment of this case can generate a larger air gap magnetic force under the same coil magnetomotive force, thereby overcoming the larger spring force and increasing the magnetic force. The braking torque of the brake.
為了使本案所要解決的技術問題、技術方案及有益效果更加清楚明白,以下結合圖式及實施例,對本案進行進一步詳細說明。應當理解,此處所描述的具體實施例僅僅用以解釋本案,並不用於限定本案。In order to make the technical problems, technical solutions and beneficial effects to be solved in this case more clear, this case will be further described in detail below with reference to drawings and examples. It should be understood that the specific embodiments described here are only used to explain the present case and are not used to limit the present case.
請一並參閱第1圖至第14圖,現對本案提供的電磁吸合組件進行說明。Please refer to Figures 1 to 14 together for a description of the electromagnetic attraction components provided in this case.
參閱第2圖、第5圖至第7圖、第9圖、第12圖至第14圖,該電磁吸合組件,包括磁軛鐵芯10、銜鐵30以及線圈20,磁軛鐵芯10上同軸設有環形的安裝槽11,安裝槽11的開口朝向磁軛鐵芯10的第一軸側;銜鐵30設於磁軛鐵芯10的第一軸側,銜鐵30具有朝向或遠離磁軛鐵芯10移動的自由度,銜鐵30對應於安裝槽11開口處區域形成有環形的對應面301,對應面301與安裝槽11形成環形的磁路空間,磁路空間的寬度沿背離磁軛鐵芯10軸線的方向逐漸增加;線圈20置於磁路空間內,線圈20能在通電時產生磁場,以使銜鐵30朝向磁軛鐵芯10移動。可以理解的是,對應面301為銜鐵30在第一軸側的端面。對應面301與安裝槽11共同圍合形成磁路空間。Referring to Figures 2, 5 to 7, 9, 12 to 14, the electromagnetic attraction component includes a
需要說明的是,磁路空間的寬度方向平行於磁軛鐵芯10的軸向。磁軛鐵芯10為具有中心孔的環狀結構,在組裝成制動器之後,被制動軸的軸線穿過該中心孔,磁軛鐵芯10的軸線方向與被制動軸的軸線方向重合。磁軛鐵芯10具有沿軸線方向分布的第一軸側和第二軸側,第一軸側和第二軸側可以理解為磁軛鐵芯10的兩個相對的端面。磁軛鐵芯10更可以被稱為磁軛、外殼、導磁體、導磁殼體、殼體等。磁軛鐵芯10和銜鐵30本身不具有磁性,當線圈20通電時,磁軛鐵芯10和銜鐵30均被磁化,產生磁性,進而相互吸引;當線圈20不通電時,磁軛鐵芯10和銜鐵30的磁性消失。It should be noted that the width direction of the magnetic circuit space is parallel to the axial direction of the
本實施例提供的電磁吸合組件,在具體使用的時候,電磁吸合組件安裝在制動器上,除了電磁吸合組件自身所包括的磁軛鐵芯10、線圈20和銜鐵30外,還需要在磁軛鐵芯10上安裝彈簧、摩擦盤40等組件,制動器上的摩擦盤40與軸套或電機軸配合,並隨電機軸旋轉。制動器可以採用斷電制動方式,也可以採用通電制動方式,以斷電制動方式為例,在電機軸正常轉動的時候,線圈20通電使其外周產生磁場,磁軛鐵芯10和銜鐵30之間的氣隙中會產生磁力,進而吸引銜鐵30靠近磁軛鐵芯10移動,銜鐵30靠近磁軛鐵芯10並擠壓彈簧,此時銜鐵30與摩擦盤40間隔,摩擦盤40正常轉動;當線圈20斷電後磁場消失,即磁軛鐵芯10與銜鐵30之間氣隙中的磁力消失,彈簧回彈推動銜鐵30遠離磁軛鐵芯10,此時銜鐵30擠壓於摩擦盤40上,通過摩擦阻力實現制動。When the electromagnetic attraction component provided by this embodiment is actually used, the electromagnetic attraction component is installed on the brake. In addition to the
需要說明的是,如第2圖和第5圖所示,銜鐵30的內圈圓周面35和外圈圓周面36指的是與安裝槽11的兩個槽側面分別平齊的圓周面,磁軛鐵芯10的內圈圓周面14和外圈圓周面15指的是與安裝槽11的兩個槽側面分別平齊的圓周面。It should be noted that, as shown in Figures 2 and 5, the inner ring
與習知技術相比,本案電磁吸合組件中銜鐵30和磁軛鐵芯10形成的磁路空間的寬度沿背離磁軛鐵芯10的軸向逐漸增加,在磁路空間的變化趨勢下,則銜鐵30和/或磁軛鐵芯10的內圈圓周面(35和/或14)的面積近似等於或略小於外圈圓周面(36和/或15)的面積,進而使得內圈和外圈單位面積通過的磁力線密度接近,使得磁感應強度接近或均勻,相較於傳統截面為矩形的磁路空間,本案實施例結構可以在相同的線圈磁動勢下,產生較大的氣隙磁力,從而可以克服更大的彈簧力,增大制動器的制動力矩。Compared with the conventional technology, the width of the magnetic circuit space formed by the
需要說明的是,本案實施例中的附圖標記請一並參考第1圖至第14圖,如對應視圖未顯示,則可以參考其他附圖,例如,磁軛鐵芯10的結構示意圖參考第4圖和第11圖,銜鐵30的結構示意圖參考第3圖和第10圖,磁軛鐵芯10的內圈圓周面14和外圈圓周面15、銜鐵30的內圈圓周面35和外圈圓周面36參考第2圖和第5圖。It should be noted that the reference numbers in the embodiment of this case please refer to Figures 1 to 14 together. If the corresponding view is not shown, you can refer to other figures. For example, for the structural schematic diagram of the
對於磁路空間的寬度沿背離磁軛鐵芯10軸線的方向逐漸增大的結構方式不做限制,下面舉例說明。There is no restriction on the structural method in which the width of the magnetic circuit space gradually increases in the direction away from the axis of the
在一些實施例中,上述磁路空間的一種具體實施方式可以採用如第6圖及第13圖所示結構。參見第6圖及第13圖,磁路空間的截面形狀為直角梯形,安裝槽11的槽底面111為錐面,對應面301為平面。可以理解的是,磁路空間的截面形狀指的是由軸向切面所形成的截面形狀,此處錐面和平面是參照徑向切面進行區分的。當銜鐵30的厚度足夠,而磁軛鐵芯10對應安裝槽11部位的厚度不足的情況下,可僅將磁軛鐵芯10內安裝槽11的槽底面111設置為錐面,則磁路空間對應構成楔形磁路,楔形磁路僅位於磁軛鐵芯10內,進而避免了在銜鐵30上設置對應的形狀,降低製造成本。In some embodiments, a specific implementation manner of the above-mentioned magnetic circuit space may adopt the structure shown in Figure 6 and Figure 13. Referring to Figures 6 and 13, the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the
從另一角度來說,對應面301為直角腰邊,安裝槽11的槽底面111為斜腰邊。該實施例中,安裝槽11的槽底面111的斜率或斜度是恆定值,保持同一數值不變,即,整個槽底面111形成一個斜面,進而能夠形成均勻變化的磁路空間,使得磁感應強度更加接近或均勻,提高了制動效率。From another perspective, the
當磁路空間的截面形狀為直角梯形,安裝槽11的槽底面111為錐面,對應面301為平面時,在一些實施例中,上述線圈20的一種具體實施方式可以採用如第6圖及第13圖所示結構。參見第6圖及第13圖,線圈20的截面形狀為矩形;或,線圈20的截面形狀為直角梯形,以在背離銜鐵30的一側面形成錐面,線圈20的錐面能貼合於安裝槽11的槽底面111的錐面。在磁路空間的截面為直角梯形的情況下,線圈20的截面也為對應的直角梯形,進而線圈20在背離磁軛鐵芯10軸線的方向上厚度逐漸增大,繞線空間也逐漸增大,繞線的匝數也逐漸增多,線圈20的電阻增大,降低了線圈20的功率,從而降低制動器的溫升。When the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the
可以理解的是,線圈20的截面形狀指的是由軸向切面所形成的截面形狀。當線圈20的截面形狀為直角梯形時,該線圈20的截面形狀與磁路空間的截面形狀相同,但尺寸略微不同,使得線圈20能夠對應地匹配至磁路空間內。It can be understood that the cross-sectional shape of the
不同於上述實施例,在其他一些實施例中,上述磁路空間的一種具體實施方式可以採用如第2圖、第5圖、第7圖、第9圖、第12圖及第14圖所示結構。參見第7圖及第14圖,磁路空間的截面形狀為直角梯形,安裝槽11的槽底面111為平面,對應面301為錐面;或,參見第2圖、第5圖、第9圖、第12圖,磁路空間的截面形狀為等腰梯形,安裝槽11的槽底面111和對應面301均為錐面。Different from the above embodiments, in some other embodiments, a specific implementation manner of the above magnetic circuit space can be as shown in Figure 2, Figure 5, Figure 7, Figure 9, Figure 12 and Figure 14 structure. Referring to Figures 7 and 14, the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the
從另一角度來說,當磁路空間的截面形狀為直角梯形時,安裝槽11的槽底面111為直角腰邊,對應面301為斜腰邊;當磁路空間的截面形狀為等腰梯形時,安裝槽11的槽底面111和對應面301均為斜腰邊。From another perspective, when the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the
如第7圖和第14圖所示,當磁軛鐵芯10對應安裝槽11部位的厚度足夠,銜鐵30的厚度不足的情況下,可僅將銜鐵30上的對應面301設置為錐面,則銜鐵30上的錐面與磁軛鐵芯10內的安裝槽11組成截面為直角梯形的磁路空間,該結構下相比於習知結構僅需要對銜鐵30進行再加工,製造成本較低;如第2圖、第5圖、第9圖和第12圖所示,當磁軛鐵芯10對應安裝槽11部位的厚度和銜鐵30的厚度均不足的情況下,則磁軛鐵芯10內安裝槽11的槽底面111和對應面301均為錐面,該種結構可以選取厚度較小的銜鐵30和磁軛鐵芯10,進而降低整體制動器的厚度,不同的實施例設置以便滿足不同的情況。As shown in Figures 7 and 14, when the thickness of the
當然,不同於上述實施例,在其他實施例中,磁路空間的截面形狀更可以為普通梯形,安裝槽11的槽底面111和對應面301均為錐面,但二者的錐度不同。相對應地,線圈20的截面形狀可以為矩形,也可以為適應於磁路空間截面形狀的梯形。Of course, different from the above embodiment, in other embodiments, the cross-sectional shape of the magnetic circuit space can be an ordinary trapezoid, and the
此外,不同於上述實施例,在其他實施例中,磁路空間的截面形狀更可以是兩個槽側面平行於軸線,槽底面111為不同錐度的組合錐面,對應面301為平面;或者,槽底面111為平面,對應面301為不同錐度的組合錐面。In addition, unlike the above embodiment, in other embodiments, the cross-sectional shape of the magnetic circuit space can be such that the two groove side surfaces are parallel to the axis, the
習知技術中,在磁軛鐵芯中設計安裝槽時,存在將安裝槽設計為局部變窄的情況,然而,該種方式僅僅實現了局部的磁感應強度的均勻性,無法獲得均勻性和一致性更好的磁感應強度,並且,從加工難度上來說,局部變窄的工藝更加難控制,難以達到目標形狀,同時,當採用局部變窄的工藝時,如果線圈的形狀為矩形,則難以實現安裝槽空間的最大效率化,如果線圈的形狀對應設計,則局部變窄的設計難度和加工難度更大。In the conventional technology, when designing the installation slot in the yoke iron core, there are cases where the installation slot is designed to be locally narrowed. However, this method only achieves local uniformity of magnetic induction intensity and cannot achieve uniformity and consistency. Better magnetic induction intensity, and in terms of processing difficulty, the local narrowing process is more difficult to control and difficult to achieve the target shape. At the same time, when using the local narrowing process, if the shape of the coil is rectangular, it is difficult to achieve To maximize the efficiency of the installation slot space, if the shape of the coil is designed accordingly, the local narrowing will be more difficult to design and process.
由於習知技術向來如此設計,是以,本案所屬技術領域中具有通常知識者基於常規設計和常規技術教導,也只能在習知技術的基礎上進行精準化設計,並不會想到進行構造改進。而本案的發明人打破傳統的固有思路,通過創造性勞動將安裝槽11的槽底面111和/或對應面301設計為整體性變化趨勢,儘管看上去好像僅僅對磁路空間的形狀進行了調整,但是,這樣的設計思路需要將磁軛鐵芯10、銜鐵30和線圈20的構造進行重新匹配性設計,並且起到了意想不到的技術效果,例如,磁感應強度的均勻性和一致性在實際應用中效果更好,加工工藝更加簡單,易於得到目標形狀,並且線圈20為規則形狀設計,可以降低設計和加工難度,超出了本案所屬技術領域中具有通常知識者對該種設計思路的想象效果。Since the known technology has always been designed in this way, a person with ordinary knowledge in the technical field to which this case belongs can only carry out precise design based on conventional design and conventional technical teachings, and will not think of structural improvements. . The inventor of this case broke the traditional inherent thinking and used creative work to design the
一項發明創造的創造高度並不僅僅在於它的方案複雜難度有多高,相反,類似於手機自拍棒、易拉罐拉環該種簡單設計,卻因為極高的實用性、意想不到的效果、極大的領域技術啟發、極大的社會進步等因素,廣為人傳和被人稱贊。The creative height of an invention does not just lie in how complex and difficult its solution is. On the contrary, simple designs such as mobile phone selfie sticks and can pull rings are extremely practical, unexpected effects, and huge. It has been widely spread and praised due to factors such as technical inspiration in the field and great social progress.
對應到本案中,本案的設計構思,一方面並不是絕對意義的簡單設計,另一方面由於對本領域技術改進具有極大的啟發意義,以及可以獲得極好的產品效果,是以,本案的設計構思值得獲得較高的創造高度和評判。Corresponding to this case, on the one hand, the design concept of this case is not a simple design in an absolute sense. On the other hand, it is of great enlightenment for technological improvements in this field and can achieve excellent product effects. Therefore, the design concept of this case is Worthy of higher creative heights and judgment.
下面對磁軛鐵芯10和銜鐵30的具體結構進行舉例說明。The specific structures of the
當採用如第6圖和第13圖所示的實施方式時,磁路空間的截面形狀為直角梯形,安裝槽11的槽底面111為斜腰邊,對應面301為直角腰邊。相對應地,由於對應面301為直角腰邊,是以,銜鐵30朝向磁軛鐵芯10的端面可以為一整個平面,當然,銜鐵30背離磁軛鐵芯10的端面也可以為一整個平面,該種情況下,銜鐵30為厚度恆定的環狀結構。When the embodiment shown in Figures 6 and 13 is adopted, the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the
當採用如第1圖至第5圖、第8圖至第12圖所示的實施方式時,磁路空間的截面形狀為等腰梯形,安裝槽11的槽底面111和對應面301均為斜腰邊。相對應地,由於對應面301為斜腰邊,是以,銜鐵30朝向磁軛鐵芯10的端面需要在空間上避開線圈20,即銜鐵30朝向磁軛鐵芯10的端面為階梯面,當銜鐵30背離磁軛鐵芯10的端面為一整個平面時,該種情況下,銜鐵30為厚度不恆定的環狀結構。When the embodiments shown in Figures 1 to 5 and 8 to 12 are adopted, the cross-sectional shape of the magnetic circuit space is an isosceles trapezoid, and the
當採用如第7圖和第14圖所示的實施方式時,磁路空間的截面形狀為直角梯形,安裝槽11的槽底面111為直角腰邊,對應面301為斜腰邊。相對應地,由於對應面301為斜腰邊,是以,銜鐵30朝向磁軛鐵芯10的端面需要在空間上避開線圈20,即銜鐵30朝向磁軛鐵芯10的端面為階梯面,當銜鐵30背離磁軛鐵芯10的端面為一整個平面時,該種情況下,銜鐵30為厚度不恆定的環狀結構。When the embodiment shown in Figures 7 and 14 is adopted, the cross-sectional shape of the magnetic circuit space is a right-angled trapezoid, the
當銜鐵30為厚度不恆定的環狀結構時,在一些實施例中,上述銜鐵30的一種具體實施方式可以採用如第1圖至第5圖、第7圖、第8圖至第12圖、第14圖所示結構。參見第1圖至第5圖、第7圖、第8圖至第12圖、第14圖,銜鐵30包括由內向外依次同軸設置的內環板31、中間環板32以及外環板33,中間環板32的內圈與安裝槽11的內圈平齊,中間環板32的外圈與安裝槽11的外圈平齊,內環板31、中間環板32以及外環板33背離線圈20的一側面平齊;中間環板32朝向線圈20的一側面形成上述對應面301;中間環板32的厚度沿背離磁軛鐵芯10軸線的方向逐漸減小,以使對應面301形成錐面。中間環板32對應的是磁軛鐵芯10的安裝槽11部分,則不改變內環板31與磁軛鐵芯10對應的面積,也不改變外環板33與磁軛鐵芯10對應的面積,可在習知銜鐵30上進行加工進而得到所需的中間環板32的部分,加工方便,並且對習知銜鐵30的再利用也適當降低了成本。When the
結合上述銜鐵30的具體結構,在一些實施例中,上述銜鐵30的一種具體實施方式可以採用如第5圖、第7圖及第12圖所示結構。參見第5圖、第7圖及第12圖,內環板31的厚度與中間環板32的最大厚度相等,外環板33與中間環板32的最小厚度相等。該種情況下,內環板31的厚度為第一恆定厚度,中間環板32的厚度為漸變式厚度,外環板33的厚度為第二恆定厚度,第一恆定厚度大於第二恆定厚度,漸變式厚度銜接於第一恆定厚度與第二恆定厚度之間且逐漸減小。該種變化趨勢,使得銜鐵30在徑向上,其環形截面(即從內圈逐漸向外圈擴張的圓周面)半徑逐漸增大,但是厚度在逐漸減小,並且最外圈的外環板33厚度最小,進而減小內圈圓周面的面積與外圈圓周面的面積差異。Combined with the specific structure of the above-mentioned
結合上述內環板31、中間環板32和外環板33的厚度情況,在一些實施例中,上述磁軛鐵芯10的一種改進實施方式可以採用如第5圖、第7圖及第12圖所示結構。參見第5圖、第7圖及第12圖,磁軛鐵芯10包括處於安裝槽11外圈的第一環形部12和處於安裝槽11內圈的第二環形部13,第一環形部12的厚度大於第二環形部13的厚度,第一環形部12和外環板33之間的間隔等於第二環形部13和內環板31之間的間隔。由於內環板31的厚度大於外環板33的厚度,磁軛鐵芯10的第一環形部12的厚度也對應的增加,防止從銜鐵30和磁軛鐵芯10之間漏磁影響設備中其他對磁場較敏感的部件工作。Combined with the thickness of the above-mentioned
需要說明的是,磁軛鐵芯10與銜鐵30之間具有氣隙,該氣隙的均勻性影響磁感應強度的均勻性和穩定性。It should be noted that there is an air gap between the
本實施例中,第一環形部12和外環板33之間形成第一氣隙面71,第一氣隙面71垂直於磁軛鐵芯10的軸線;第二環形部13和內環板31之間形成第二氣隙面72,第二氣隙面72也垂直於磁軛鐵芯10的軸線,並且,第一氣隙面71和第二氣隙面72不共面。當裝配磁軛鐵芯10和銜鐵30時,第一環形板12和外環板33之間、第二環形部13和內環板31之間更容易實現對齊效果,能夠提高裝配效率,保證氣隙面的均勻性和一致性,從而提高磁感應強度的均勻性和一致性,減少漏磁的可能性。In this embodiment, a first
然而,習知技術中,磁軛鐵芯和銜鐵自外周邊緣向內延伸的部分範圍內,二者之間所形成的氣隙面與磁軛鐵芯的軸線呈銳角或鈍角設置。該種氣隙方式,一方面,在製備磁軛鐵芯和銜鐵的過程中,需要嚴格保證二者的尺寸精度,加工難度較大;另一方面,在裝配磁軛鐵芯和銜鐵的過程中,由於氣隙面為傾斜狀,對齊難度極大,需要嚴格保證二者之間氣隙的均勻性和一致性,裝配難度大,當需要採用檢測器件來檢測二者之間的氣隙時,檢測器件不易伸入氣隙中,操作難度較大,無法精確測量氣隙。However, in the conventional technology, within the portion of the yoke core and the armature extending inward from the outer peripheral edge, the air gap surface formed between the two is arranged at an acute or obtuse angle with the axis of the yoke core. This air gap method, on the one hand, needs to strictly ensure the dimensional accuracy of the yoke core and armature in the process of preparing the two, making the processing difficult; on the other hand, in the process of assembling the yoke core and armature , since the air gap surface is inclined, alignment is extremely difficult. It is necessary to strictly ensure the uniformity and consistency of the air gap between the two, and assembly is difficult. When a detection device needs to be used to detect the air gap between the two, the detection It is difficult for the device to extend into the air gap, making it difficult to operate, and the air gap cannot be accurately measured.
對於習知技術中所出現的問題,本實施例中,第一氣隙面71和第二氣隙面72均垂直於磁軛鐵芯10的軸線,一方面,可以嚴格保證二者的尺寸精度,降低了加工難度,另一方面,磁軛鐵芯10和銜鐵30易於對齊,便於快速裝配,並且易於採用檢測器件伸入氣隙中進行測量,可以減少檢測時間,保證氣隙的測量精確性,保證氣隙的均勻性和一致性,進而保證磁感應強度的均勻性和一致性。Regarding the problems that arise in the conventional technology, in this embodiment, the first
與上述第5圖、第7圖及第12圖所示結構不同,在其他一些實施例中,上述銜鐵30的一種變形實施方式可以採用如第2圖、第9圖及第14圖所示結構。參見第2圖、第9圖及第14圖,內環板31的厚度與外環板33的厚度相等,內環板31的厚度等於中間環板32的最大厚度。該種情況下,內環板31的厚度為第一恆定厚度,中間環板32的厚度為漸變式厚度,外環板33的厚度為第二恆定厚度,第一恆定厚度等於第二恆定厚度,漸變式厚度自第一恆定厚度朝向第二恆定厚度延伸且逐漸減小,由於漸變式厚度的最小厚度小於第二恆定厚度,進而中間環板32和外環板33可以圍合形成第一凹槽34,即中間環板32朝向線圈20的一側面凹陷形成有第一凹槽34。Different from the structures shown in Figures 5, 7 and 12 above, in some other embodiments, a modified implementation of the
該種變化趨勢,使得中間環板32在徑向上,其環形截面(即從內圈逐漸向外圈擴張的圓周面)半徑逐漸增大,但是厚度在逐漸減小,進而減小內圈圓周面的面積與外圈圓周面的面積差異,但是內環板31和外環板33的厚度均是一定的,且沒有相應的變化趨勢,相比於第5圖、第7圖及第12圖中所示的銜鐵30實施例,減少了厚度的加工步驟,進而加工成本相對也相對較低。This changing trend causes the radius of the annular cross-section (ie, the circumferential surface that gradually expands from the inner ring to the outer ring) of the
本實施例中,第一環形部12的厚度等於第二環形部13的厚度。第一環形部12和外環板33之間形成第一氣隙面71,第二環形部13和內環板31之間形成第二氣隙面72,第一氣隙面71和第二氣隙面72均垂直於磁軛鐵芯10的軸線,且第一氣隙面71和第二氣隙面72共面。本實施例相對於習知技術的有益效果,與上述實施例中第一氣隙面71和第二氣隙面72的有益效果相同,在此不再贅述。In this embodiment, the thickness of the first
需要說明的是,當第一環形部12的厚度等於第二環形部13的厚度時,可以是絕對意義上的相等,也可以是相對意義上的相等,即,允許第一環形部12的厚度略大於第二環形部13的厚度的情況,此時,第一環形部12與第二環形部13的厚度差值很小,例如0.02毫米至0.05毫米之間,是以,該種厚度差值可以忽略不計。相對應地,第一氣隙面71和第二氣隙面72為絕對意義上的共面,或相對意義上的共面。It should be noted that when the thickness of the first
此外,如第5圖所示,上述實施例中第一氣隙面71和第二氣隙面72不共面,當製備磁軛鐵芯10和銜鐵30時,需要更加嚴格保證二者的尺寸精度,加工步驟相對較多,加工成本也相對較高;當裝配磁軛鐵芯10與鐵芯30時,由於線圈20位於磁軛鐵芯10與銜鐵30所配合的氣隙拐角處,磁感應線在空氣中容易發散,不受約束。In addition, as shown in Figure 5, the first
針對第5圖所示實施例的問題,作為更優選的實施例,如第2圖所示,第一氣隙面71和第二氣隙面72共面,且中間環板32形成第一凹槽34,如此可以減少對銜鐵30的加工步驟,保證尺寸的一致性,減少加工成本,同時,由於第一凹槽34的限製作用,可以減少磁感應線的發散,減少漏磁可能性,保證磁感應線的有效利用率。In view of the problem of the embodiment shown in Figure 5, as a more preferred embodiment, as shown in Figure 2, the first
在一些實施例中,上述線圈20的一種具體實施方式可以採用如第2圖、第5圖、第7圖、第9圖、第12圖及第14圖所示結構。參見第2圖、第5圖、第7圖、第9圖、第12圖及第14圖,線圈20的截面形狀為矩形;或,線圈20的截面形狀為適應於磁路空間形狀的梯形。In some embodiments, a specific implementation of the above-mentioned
上述已經說到,當安裝槽11的槽底面111為錐面,對應面301為平面時,線圈20背向銜鐵30的一側面也為錐面。本實施例中,當安裝槽11的槽底面111為平面,對應面301為錐面時,則線圈20朝向銜鐵30的一側面為錐面;當安裝槽11的槽底面111和對應面301均為錐面時,則線圈20的兩個軸端面也均為對應的錐面。通過使得線圈20的截面形狀適應於磁路空間的截面形狀,可以充分利用磁路空間,進而使得線圈20沿背離磁軛鐵芯10軸線的方向上繞線圈數逐漸增多,線圈20的電阻增大,降低了線圈20的功率,從而降低制動器的溫升。As mentioned above, when the
基於同一發明構思,本案實施例還提供了一種制動器,包括上述電磁吸合組件。Based on the same inventive concept, an embodiment of the present case also provides a brake including the above-mentioned electromagnetic attraction component.
較為常見的具體實施方式可分為兩種:The more common specific implementation methods can be divided into two types:
(1)參閱第1圖至第7圖,制動器的類型為傳統式制動器:電磁吸合組件安裝在制動器上,除了電磁吸合組件自身所包括的磁軛鐵芯10、線圈20和銜鐵30外,還需要在磁軛鐵芯10上安裝彈簧、摩擦盤40、尾板60等組件,制動器上的摩擦盤40與軸套或電機軸配合,並隨電機軸旋轉,在電機軸正常轉動的時候,線圈20通電使其外周產生磁場,磁軛鐵芯10和銜鐵30之間的氣隙中會產生磁力,進而吸引銜鐵30靠近磁軛鐵芯10移動,銜鐵30靠近磁軛鐵芯10並擠壓彈簧,此時銜鐵30與摩擦盤40間隔,摩擦盤40正常轉動;當線圈20斷電後磁場消失,即磁軛鐵芯10與銜鐵30之間氣隙中的磁力消失,彈簧回彈推動銜鐵30遠離磁軛鐵芯10,此時銜鐵30擠壓於摩擦盤40上,且摩擦盤40背向銜鐵30的一端面擠壓於尾板60,通過摩擦阻力實現制動。(1) Refer to Figures 1 to 7. The type of brake is a traditional brake: the electromagnetic attraction component is installed on the brake, except for the
(2)參閱第8圖至第14圖,制動器為新型的薄型制動器:電磁吸合組件安裝在制動器上,除了電磁吸合組件自身所包括的磁軛鐵芯10、線圈20和銜鐵30外,還需要在磁軛鐵芯10上安裝彈簧、摩擦盤40、活動板50等組件,制動器上的摩擦盤40與軸套或電機軸配合,並隨電機軸旋轉,在電機軸正常轉動的時候,線圈20通電使其外周產生磁場,磁軛鐵芯10和銜鐵30之間的氣隙中會產生磁力,進而吸引銜鐵30靠近磁軛鐵芯10移動,銜鐵30靠近磁軛鐵芯10並擠壓彈簧,此時銜鐵30與活動板50連接使得活動板50與摩擦盤40間隔,摩擦盤40正常轉動;當線圈20斷電後磁場消失,即磁軛鐵芯10與銜鐵30之間氣隙中的磁力消失,彈簧回彈推動銜鐵30遠離磁軛鐵芯10,此時銜鐵30帶動活動板50擠壓於摩擦盤40上,通過摩擦阻力實現制動。(2) Refer to Figures 8 to 14. The brake is a new type of thin brake: the electromagnetic attraction component is installed on the brake. In addition to the
當然,上述兩種實施方式中,摩擦盤40均為雙面摩擦的方式,在其他實施方式中,本案實施例所提供的電磁吸合組件更可以應用於單面摩擦的制動器中,即摩擦盤40可以僅有一個端面進行摩擦制動,對此不做限制。本案的制動器旨在包括上述電磁吸合組件,對於其他組成構件的形式和構造不做限制,具有非常廣泛的應用場景。Of course, in the above two embodiments, the
與習知技術相比,本案制動器中銜鐵30和磁軛鐵芯10形成的磁路空間的寬度沿背離磁軛鐵芯10的軸向逐漸增加,在磁路空間的變化趨勢下,則銜鐵30和/或磁軛鐵芯10的內圈圓周面的面積近似等於或略小於外圈圓周面的面積,進而使得內圈和外圈單位面積通過的磁力線密度接近,使得磁感應強度接近或均勻,相較於傳統截面為矩形的磁路空間,本案實施例結構可以在相同的線圈磁動勢下,產生較大的氣隙磁力,從而可以克服更大的彈簧力,增大制動器的制動力矩。Compared with the conventional technology, the width of the magnetic circuit space formed by the
需要說明的是,習知技術中,類似於電磁離合器,可能存在將線圈設置為漸變式結構的情況,然而,在電磁離合器中,磁軛鐵芯、銜鐵、線圈、摩擦盤的空間構造與本案完全不同,無法綜合設計層疊狀的磁軛鐵芯、銜鐵和摩擦盤,無需對磁軛鐵芯、銜鐵和線圈之間的空間關係進行聯繫性設計。當本案採用漸變式的線圈20時,由於磁軛鐵芯10和銜鐵30共同包圍線圈20,是以,三者之間的關係是需要經過嚴格設計的,需要合理地設計磁軛鐵芯10的形狀和尺寸,需要對應地設計銜鐵30的形狀和尺寸,需要保證磁軛鐵芯10和銜鐵30之間的氣隙均勻性,需要考慮採用何種加工方式進行磁軛鐵芯10和銜鐵30的製作,需要考慮如何才能減少加工成本和簡化加工步驟等等,也就是說,漸變式的線圈20並非可以直接應用於本案中,存在轉用上的技術難度,需要經過上述多個方面的綜合考量,需要付出大量的創造性勞動,才能設計出具有較高磁力效果、較高實用性、較低成本、較簡單工藝等綜合性強的電磁吸合組件。It should be noted that in the conventional technology, similar to the electromagnetic clutch, there may be cases where the coil is set in a gradual structure. However, in the electromagnetic clutch, the spatial structure of the yoke core, armature, coil, and friction disk is different from that of the present case. It is completely different. It is impossible to comprehensively design the stacked yoke core, armature and friction disk, and there is no need to design the spatial relationship between the yoke core, armature and coil. When the
可以理解的是,上述實施例中的各部分可以進行自由地組合或刪減以形成不同的組合實施例,在此不再贅述各個組合實施例的具體內容,在此說明之後,可以認為本案說明書已經記載了各個組合實施例,能夠支持不同的組合實施例。It can be understood that the various parts in the above embodiments can be freely combined or deleted to form different combination embodiments. The specific content of each combination embodiment will not be described again. After this description, the description of this case can be considered Various combination embodiments have been described and different combination embodiments can be supported.
以上所述僅為本案的較佳實施例而已,並不用以限制本案,凡在本案的精神和原則之內所作的任何修改、等同替換和改進等,均應包含在本案的保護範圍之內。The above are only preferred embodiments of this case and are not intended to limit this case. Any modifications, equivalent substitutions and improvements made within the spirit and principles of this case shall be included in the scope of protection of this case.
10:磁軛鐵芯 11:安裝槽 111:槽底面 12:第一環形部 13:第二環形部 14:內圈圓周面 15:外圈圓周面 20:線圈 30:銜鐵 301:對應面 31:內環板 32:中間環板 33:外環板 34:第一凹槽 35:內圈圓周面 36:外圈圓周面 40:摩擦盤 50:活動板 60:尾板 71:第一氣隙面 72:第二氣隙面 10:Yoke core 11:Installation slot 111:Trough bottom 12: First ring part 13:Second ring part 14: Inner ring circumferential surface 15: Outer ring circumferential surface 20: coil 30:Armature 301:Corresponding surface 31:Inner ring plate 32: Middle ring plate 33:Outer ring plate 34: First groove 35: Inner ring circumferential surface 36: Outer ring circumferential surface 40: Friction disc 50:movable board 60: Tail plate 71: First air gap surface 72: Second air gap surface
第1圖為本案實施例一提供的制動器的主視結構示意圖; 第2圖為沿第1圖中A-A線的剖視結構圖; 第3圖為本案實施例一採用的銜鐵的立體結構示意圖; 第4圖為本案實施例一採用的磁軛鐵芯的立體結構示意圖; 第5圖為本案實施例二提供的制動器的剖視結構示意圖(與第2圖視角相同); 第6圖為本案實施例三提供的制動器的剖視結構示意圖(與第2圖視角相同); 第7圖為本案實施例四提供的制動器的剖視結構示意圖(與第2圖視角相同); 第8圖為本案實施例五提供的制動器的主視結構示意圖; 第9圖為沿第8圖中B-B線的剖視結構圖; 第10圖為本案實施例五採用的銜鐵的立體結構示意圖; 第11圖為本案實施例五採用的磁軛鐵芯的立體結構示意圖; 第12圖為本案實施例六提供的制動器的剖視結構示意圖(與第9圖視角相同); 第13圖為本案實施例七提供的制動器的剖視結構示意圖(與第9圖視角相同); 第14圖為本案實施例八提供的制動器的剖視結構示意圖(與第9圖視角相同)。 Figure 1 is a schematic view of the main structure of the brake provided in Embodiment 1 of this case; Figure 2 is a cross-sectional structural view along line A-A in Figure 1; Figure 3 is a schematic diagram of the three-dimensional structure of the armature used in Embodiment 1 of this case; Figure 4 is a schematic three-dimensional structural diagram of the yoke core used in Embodiment 1 of this case; Figure 5 is a schematic cross-sectional structural view of the brake provided in Embodiment 2 of this case (same perspective as Figure 2); Figure 6 is a schematic cross-sectional structural view of the brake provided in Embodiment 3 of this case (same perspective as Figure 2); Figure 7 is a schematic cross-sectional structural view of the brake provided in Embodiment 4 of this case (same perspective as Figure 2); Figure 8 is a schematic view of the main structure of the brake provided in Embodiment 5 of this case; Figure 9 is a cross-sectional structural view along line B-B in Figure 8; Figure 10 is a schematic diagram of the three-dimensional structure of the armature used in Embodiment 5 of this case; Figure 11 is a schematic three-dimensional structural diagram of the yoke core used in Embodiment 5 of this case; Figure 12 is a schematic cross-sectional structural diagram of the brake provided in Embodiment 6 of this case (same viewing angle as Figure 9); Figure 13 is a schematic cross-sectional structural diagram of the brake provided in Embodiment 7 of this case (same viewing angle as Figure 9); Figure 14 is a schematic cross-sectional structural diagram of the brake provided in Embodiment 8 of this case (same viewing angle as Figure 9).
10:磁軛鐵芯 10:Yoke core
11:安裝槽 11:Installation slot
111:槽底面 111:Trough bottom
14:內圈圓周面 14: Inner ring circumferential surface
15:外圈圓周面 15: Outer ring circumferential surface
20:線圈 20: coil
30:銜鐵 30:Armature
301:對應面 301:Corresponding surface
34:第一凹槽 34: First groove
35:內圈圓周面 35: Inner ring circumferential surface
36:外圈圓周面 36: Outer ring circumferential surface
60:尾板 60: Tail plate
71:第一氣隙面 71: First air gap surface
72:第二氣隙面 72: Second air gap surface
Claims (15)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202220553773.2U CN216812614U (en) | 2022-03-14 | 2022-03-14 | Electromagnetic attraction-in assembly and brake |
CNCN202220553773.2 | 2022-03-14 |
Publications (1)
Publication Number | Publication Date |
---|---|
TW202336360A true TW202336360A (en) | 2023-09-16 |
Family
ID=82045184
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW111140693A TW202336360A (en) | 2022-03-14 | 2022-10-26 | Electromagnetic pull-in assembly and brake |
Country Status (3)
Country | Link |
---|---|
CN (1) | CN216812614U (en) |
TW (1) | TW202336360A (en) |
WO (1) | WO2023173731A1 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN216812614U (en) * | 2022-03-14 | 2022-06-24 | 奥创动力传动(深圳)有限公司 | Electromagnetic attraction-in assembly and brake |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP4236062B2 (en) * | 1998-12-28 | 2009-03-11 | 神鋼電機株式会社 | Spring type non-excitation electromagnetic brake |
CN107869538B (en) * | 2017-12-12 | 2023-09-26 | 珠海格力节能环保制冷技术研究中心有限公司 | Electromagnetic brake |
CN107859703A (en) * | 2017-12-12 | 2018-03-30 | 珠海格力节能环保制冷技术研究中心有限公司 | Brake stator structure and the electromagnetic brake for including it |
CN210050223U (en) * | 2019-05-18 | 2020-02-11 | 邓世韬 | Electromagnetic brake |
CN215928187U (en) * | 2021-09-18 | 2022-03-01 | 奥创动力传动(深圳)有限公司 | Brake |
CN216812614U (en) * | 2022-03-14 | 2022-06-24 | 奥创动力传动(深圳)有限公司 | Electromagnetic attraction-in assembly and brake |
-
2022
- 2022-03-14 CN CN202220553773.2U patent/CN216812614U/en active Active
- 2022-10-12 WO PCT/CN2022/124924 patent/WO2023173731A1/en unknown
- 2022-10-26 TW TW111140693A patent/TW202336360A/en unknown
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CN216812614U (en) | 2022-06-24 |
WO2023173731A1 (en) | 2023-09-21 |
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