201244331 六、發明說明： 【發明所屬之技術領域】 本發明隸屬一種應用於馬達或發電機之電磁技術， 具體而言係指一種馬達或發電機之永久磁鐵呈同極相對 的一種應用同極對向磁組之電磁裝置，藉以提升發電效 率或提高馬達運轉效能。 【先前技術】 按，電為工業之母，更是現代人生活不可或缺的基 本能源，然而無論是運用核能、火力、風力或水力發電 ，都必須經過電磁機構的發電過程才能將各種能源轉換 成電能，因此用於發電的電磁機構之效率，其攸關著各 •種能源的消耗速度和替代能源的開發。而現有的電磁機 構主要係由線圈與磁鐵所組成之定子與轉子的旋轉機為 主，該電磁機構之旋轉機依其作動方式不同被定義為驅 動用的馬達或發電機，而其運作原理係如第1、2圖所 示，依照弗來明右手定律而言，其中磁力線方向、電流 方向及運動方向呈相互垂直，因此在磁鐵之S極與N極 的磁場中設有可移動之導線，如此當導線相對垂直之磁 力線由内向外移動時，可使導線内產生由右向左流出之 電流； 以其中作為發電機的電磁機構而言，如第3圖所示 ，通常係以相對之磁鐵（Ml、M2)作為定子，而兩相對 磁鐵（Ml、M2)的磁極係呈相異狀【亦即磁鐵Ml的S 極對應磁鐵M2的N極】，且於兩磁鐵（Ml、M2)之間 設有一作為轉子之線圈（L)，線圈（L)的兩端分別連 201244331 接集電單元，當線圈（L)的圈面垂直於磁場方向時， 通過線圈（L)内的磁力線數最多；當線圈（L)的圈面 平行於磁場方向時，通過線圈（L)内的磁力線數最少 ;如此線圈（L)在磁場中轉動時，每轉動半圈【180 度】，線圈（L)内的電流即改變方向一次【正極或負 極】，因此當完成轉動一圈時，才能完成一整個切割數 【即為一個360度的弦波】，即所輸出電流方向交替變 換形成交流電。 由於線圈（L)在磁鐵（Ml、M2)磁場中運動所產 生之電流非常小，所以發電機都利用多組線圈（L)在 磁鐵（Ml、M2)磁場中運動，或利用多組磁鐵（Ml、M2 )之磁場在線圈（L)内運動，以產生較大的電量。然 不論採用何者，都會加大發電機的體積與重量，無形間 也會加大其轉子的啟動力。因此截至目前為止，擔負將 各種能源轉換為電能之重任的發電裝置，承如前述，其 發電效率仍受限於傳統技術而未能有效發揮，且進一步 更可歸納為如下幾點原因： 1、 無法超越弗來明右手定律：如第1、2圖所示， 磁電結構的三大要素為運動方向、電流方向和磁力線方 向，其中運動方向和電流方向容易設定，而磁力線方向 則難以掌控，因此磁力線通常都會選擇如第3圖所示界 於N—S或S —N間方向固定之慣性磁流，而難以超越。 2、 無法駕馭頑固的磁場和多個固定磁鐵交互作用 的磁力線變化：如第3圖所示為呈N—S或S—N排列之 磁組，其磁力線場即具有多樣性的變化，因此傳統磁電 裝置使用固定磁鐵（Ml、M2)的數量有其實務上的困難 201244331 而受到限制。 3、 由於受到N—S或S—N排列磁組會產生如圖三 所示之物理慣性反向磁流AF，此環場磁流之方向與兩 磁鐵間之主磁流之方向是相反的，因此欲藉由増加固定 磁組數，以提高切割數之可行性極低。 4、 傳統N—S或S—N結構之電磁組合為降低漏磁 之傷害，以及提高磁通量，通常會在N—S或S—N磁組 的兩磁鐵（Ml、M2)中置入包含鐵蕊結構之線圈（L) 以達到導磁之目的，此實務結構固然可達到預期之效果 ，但也會因本裝置在靜止狀態下，此包含鐵蕊之線圈（ L)與磁鐵（Ml、M2)間即會因此產生磁吸效應，而需 極大的啟動電流，始能·運轉，且有功㈣耗的問題 〇 叫㈢π 1寻虮馬用枝術的最大缺點即是固定磁鐵之 :，大家都知道固定磁鐵之磁力線是由Ν極以 數St:::，構是以2個(或倍 應用僅限於=單應邊=磁力4 夕成权 . ^ 46極，而未運用到另一邊 =磁=!3圖所示，2個串接之磁場擁有極為 互相影響而減::力其向的磁力線方向’並 密度，這 係令:二 201244331 重量大及啟動電流大’造成其存在有功率損耗大及發電 效率差的問題，且即便該電磁機構係供作為驅動馬達， 也因其磁吸效應的影響，而需較大的啟動力，無形間增 加功率的損耗，造成能源的浪費，因此，值此全球傳統 能源曰漸枯竭而反核能聲浪曰漸高漲的年代，如何提升 電磁機構的效率’係目前業界的當務之急。 緣是’本發明人乃針對前述現有電磁裝置在使用 所面臨的問題深入探討，並藉由多年從事研發的經驗與 使用的需求，而積極尋求解決之道，經不斷努力的研/究 與試作’終於成功的開發出一種應用同極對向磁組之$ 磁裝置’藉以克服現有電磁裝置因採異向磁組所造成的 問題與困擾。 【發明内容】 因此，本發明之主要目的係在提供一種應用同極對 向磁組之電磁裝置，藉以能用於發電機中，其能有效的 增加切割數，且不致增加體積與重量，同時減少磁吸效 應的影響，提高其運轉速度，進而大幅提高其發電效率 0 又，本發明之另一主要目的係在提供一種應用同極 對向磁組之電磁裝置，藉以能用於馬達中，其能減少磁 吸現象，降低其啟動電流，從而降低功率的損耗，達到 節能減碳之目的。 基於此，本發明主要係透過下列的技術手段，來實 現前述之目的及其功效，本發明之電磁裝置具有一或多 數磁組’該等磁組係由兩兩固定相對的磁鐵所組成，且 201244331 該等磁組的兩相對磁鐵係以同極對向的方式排列， 等磁組之兩相對磁鐵的磁場間可供一或多數之線圈^該 Λ ^*^*· 藉此 … 达迺W迅衩術于段的展現，本發明之電磁 置的每一磁組之固定磁鐵係呈同極對向排列，其鹿广 互相排斥的作用’因此在磁力通道内的磁力線，g成Ί 壓迫而緊密的’且磁力通道内的磁力線方向是固定的】 使其一組同極對向的磁組即可產生一切割，可大巾5择力 其切割數，因此可獲得極大之電流及電壓輸出之目^ ^ 而達到大幅提昇發電效率和馬達運轉效能之目的。 為使貴審查委員能進一步了解本發明的構成、特 徵及其他目的’以下乃舉本發明之較佳實施例，並配入 圖式詳細說明如后’同時讓熟悉該項技術領域者能夠具 體實施。 ^ 【實施方式】 本發明係一種應用同極對向磁組之電磁裝置，隨附 圖例示之本發明電磁裝置的具體實施例及其構件中，所 有關於前與後、左與右、頂部與底部、上部與下部、以 及水平與垂直的參考，僅用於方便進行描述，並非限制 本發明，亦非將其構件限制於任何位置或空間方向。圖 式與說明書中所指定的尺寸，當可在不離開本發明之申 請專利範圍内，根據本發明之具體實施例的設計與需求 而進行變化。 而關於本發明應用同極對向磁組之電磁裝置的構成 ’則係如第4、6圖所示，該電磁裝置可供將其作為發 201244331 電機或馬達，且該電磁裝置可選自盤式或輪圈式，又該 電磁震置具有一或多數磁組⑴），該等磁組（1〇)係 ，兩^固定相對的磁鐵（m、M2)所組成，且該等磁組 (10)的兩相對磁鐵（M1、M2)係以同極對向的方式排 列，如令兩磁鐵（Ml、M2)呈N—N極相對【如第4圖 所示】或S—S極相對【如第6圖所示】之排列模式， 2該等磁組（10)之兩相對磁鐵m 多數之線圈⑴通過，再者可依需求將磁組 )疋義為轉子、而線圈（L)定義為定子，又或將 磁組（10)域紋子、而線圈⑴㈣為轉子 ^磁組（1〇)之磁流方向係如第5、7圖所示， :圖為第4 ®所揭示之磁組（1())排列方式的磁 7圖為第6圖所揭示之磁組⑽排列方 ==向。由圖示可見’由於兩個固定磁鐵⑽、 M2)係呈同極對向排列’其應力為互相排斥的作用，因 此在^磁力線（C1)及磁力線（⑻組成的磁力通道（ 而緊密的’且磁力通道（c)内的磁力線 (C卜C2)方向是蚊的，而不會如傳統電磁裝置以異 =向排列模式【如第3 _示】會產生反向慣性磁流 之狀況，如此當一個線圈⑴通過每-個磁組〇0) 之兩相對磁鐵⑷、M2)的磁力通道⑹時 生一切割數； 丨J座 因此，當-個線圈⑴通過該 力線(⑴時，可根據弗來明右手定律產生道前 ，再經另一向的磁力線⑽時產生後半週電•，如此 即可產生一完整的交流«。故本發明應㈣極對向磁201244331 VI. Description of the Invention: [Technical Field] The present invention belongs to an electromagnetic technology applied to a motor or a generator, and specifically refers to an application of the same pole pair of a permanent magnet of a motor or a generator The electromagnetic device of the magnetic group is used to improve the power generation efficiency or improve the running performance of the motor. [Previous technology] According to electricity, electricity is the mother of industry, and it is an indispensable basic energy for modern people's life. However, whether it is using nuclear energy, firepower, wind power or hydropower, it must be converted by electric power generation to convert various energy sources. In terms of electrical energy, the efficiency of the electromagnetic mechanism used for power generation is related to the development of various energy sources and the development of alternative energy sources. The existing electromagnetic mechanism is mainly composed of a rotating machine of a stator and a rotor composed of a coil and a magnet. The rotating machine of the electromagnetic mechanism is defined as a motor or a generator for driving according to the manner of operation thereof, and the operating principle thereof is As shown in the first and second figures, according to Fleming's right-hand rule, the direction of the magnetic flux, the direction of the current, and the direction of motion are perpendicular to each other, so that a movable wire is provided in the magnetic field of the S pole and the N pole of the magnet. Thus, when the relatively perpendicular magnetic lines of force move from the inside to the outside, the current flowing from the right to the left can be generated in the wire; in the electromagnetic mechanism as the generator, as shown in FIG. 3, the magnet is usually opposite. (Ml, M2) as the stator, and the magnetic poles of the two opposing magnets (M1, M2) are in a different shape [that is, the S pole of the magnet M1 corresponds to the N pole of the magnet M2], and is in the two magnets (Ml, M2) There is a coil (L) as a rotor. The two ends of the coil (L) are connected to the current collector unit of 201244331. When the circle surface of the coil (L) is perpendicular to the direction of the magnetic field, the number of magnetic lines passing through the coil (L) is the most. When the coil (L) When the circle surface is parallel to the direction of the magnetic field, the number of magnetic lines of force passing through the coil (L) is the least; when the coil (L) rotates in the magnetic field, the current in the coil (L) changes direction every half rotation [180 degrees]. Once [positive or negative], when the rotation is completed, an entire number of cuts (that is, a 360-degree sine wave) can be completed, that is, the output current direction is alternately transformed to form an alternating current. Since the current generated by the movement of the coil (L) in the magnetic field of the magnet (M1, M2) is very small, the generator uses multiple sets of coils (L) to move in the magnetic field of the magnet (Ml, M2), or utilizes multiple sets of magnets ( The magnetic field of Ml, M2) moves within the coil (L) to generate a larger amount of electricity. However, no matter which one is used, the volume and weight of the generator will be increased, and the invisible force will increase the starting force of the rotor. Therefore, as far as this is concerned, the power generation device that is responsible for converting various energy sources into electric energy, as mentioned above, its power generation efficiency is still limited by the conventional technology and cannot be effectively utilized, and further can be summarized as the following reasons: It is impossible to transcend Fleming's right-hand law: as shown in Figures 1 and 2, the three major elements of the magnetoelectric structure are the direction of motion, the direction of current, and the direction of magnetic field lines, where the direction of motion and the direction of current are easy to set, and the direction of magnetic lines of force is difficult to control. The magnetic field lines usually select the inertial magnetic current that is fixed in the direction between N-S or S-N as shown in Fig. 3, and it is difficult to exceed. 2. Unable to control the change of magnetic field lines between the stubborn magnetic field and multiple fixed magnets: as shown in Figure 3, the magnetic group in the N-S or S-N arrangement has a variety of magnetic field lines, so the tradition The number of magnetoelectric devices using fixed magnets (Ml, M2) is limited by the practical difficulties 201244331. 3. Since the magnetic group is arranged by N-S or S-N, the physical inertial reverse magnetic current AF shown in Fig. 3 is generated, and the direction of the magnetic field of the ring field is opposite to the direction of the main magnetic current between the two magnets. Therefore, it is extremely feasible to increase the number of cuts by adding a fixed number of magnetic groups. 4. The electromagnetic combination of the traditional N-S or S-N structure is to reduce the leakage magnetic damage and increase the magnetic flux. Usually, the iron is placed in the two magnets (Ml, M2) of the N-S or S-N magnetic group. The coil (L) of the core structure is used for the purpose of magnetic conduction. Although the practical structure can achieve the desired effect, but also because the device is in a static state, the coil (L) and the magnet (Ml, M2) Between the two, it will produce a magnetic effect, but it needs a great starting current, it can start and run, and the problem of active (four) consumption is squeaking. (3) The biggest disadvantage of π 1 seeking horses is the fixed magnet: Know that the magnetic line of the fixed magnet is made up of the number of St::: by the bungee, and the structure is 2 (or the application is limited to = single side = magnetic 4 夕成权. ^ 46 pole, but not applied to the other side = magnetic =! 3 shows that the two series connected magnetic fields have extremely mutual influence and are reduced: the direction of the magnetic field direction of the force is 'the density, which is the order: 2 201244331 The weight is large and the starting current is large', causing its power loss. Large and poor power generation efficiency, and even if the electromagnetic mechanism is used as a drive motor, The influence of its magnetic attraction effect requires a large starting force, which increases the loss of power invisibly, resulting in waste of energy. Therefore, in the era when global traditional energy sources are gradually depleted and anti-nuclear energy waves are rising, how to improve electromagnetics The efficiency of the organization is a top priority in the industry. The reason is that the inventor has in-depth discussion on the problems faced by the existing electromagnetic devices, and actively seeks solutions through years of experience in research and development and the needs of use. Through continuous research and research and trial work, 'a magnetic device that uses the same-pole magnetic group' has been successfully developed to overcome the problems and problems caused by the existing electromagnetic devices. Therefore, the main object of the present invention is to provide an electromagnetic device using the same pole opposite magnetic group, which can be used in a generator, which can effectively increase the number of cuts without increasing the volume and weight while reducing the magnetic attraction. The effect of the effect, the speed of its operation is increased, and the power generation efficiency is greatly improved. Further, another main object of the present invention is The utility model relates to an electromagnetic device applying the same pole opposite magnetic group, which can be used in a motor, which can reduce the magnetic attraction phenomenon and reduce the starting current thereof, thereby reducing the power loss and achieving the purpose of energy saving and carbon reduction. Based on this, the present invention mainly The foregoing objects and effects are achieved by the following technical means. The electromagnetic device of the present invention has one or more magnetic groups 'the magnetic groups are composed of two fixed magnets, and 201244331 The two opposite magnets are arranged in the same direction of the same pole, and one or more coils are available between the magnetic fields of the two opposing magnets of the equal magnetic group. ^Λ^**· By this, 迺 迺 衩 衩 段It is revealed that the fixed magnets of each magnetic group of the electromagnetic device of the present invention are arranged in the same direction of the same pole, and the deer are mutually repelled. Therefore, the magnetic lines of force in the magnetic path are pressed and compacted and the magnetic channel is The direction of the magnetic lines of force is fixed.] A group of magnetic poles facing the same pole can produce a cut, and the large towel 5 can select the number of cuts, so that the maximum current and voltage output can be obtained. Large The purpose liter motor power generation efficiency and effectiveness of the operation. The following is a description of the preferred embodiments of the present invention, and the detailed description of the present invention will be described in the following drawings, and the embodiments of the present invention can be specifically implemented. . [Embodiment] The present invention relates to an electromagnetic device using the same pole opposite magnetic group, and the specific embodiments of the electromagnetic device of the present invention and the components thereof, as illustrated in the accompanying drawings, all relate to front and rear, left and right, top and The bottom, upper and lower, and horizontal and vertical references are for convenience of description only and are not limiting of the invention, nor are they limited to any position or spatial orientation. The drawings and the dimensions specified in the specification can be varied in accordance with the design and needs of the specific embodiments of the present invention without departing from the scope of the invention. The configuration of the electromagnetic device using the same-pole magnetic group of the present invention is as shown in Figures 4 and 6, and the electromagnetic device can be used as the motor or motor of 201244331, and the electromagnetic device can be selected from the disk. Or rim type, and the electromagnetic shock has one or more magnetic groups (1)), the magnetic groups (1 〇) are composed of two fixed magnets (m, M2), and the magnetic groups ( 10) The two opposing magnets (M1, M2) are arranged in the same pole opposite direction, such as making the two magnets (Ml, M2) N-N pole relative [as shown in Figure 4] or S-S pole relative [As shown in Fig. 6], the arrangement mode of the two magnetic groups (10) is opposite to the majority of the magnets m (1), and the magnetic group can be converted into a rotor and a coil (L) according to requirements. The direction of the magnetic current defined as the stator, or the magnetic group (10) domain, and the coil (1) (four) as the rotor magnet group (1〇) is shown in Figures 5 and 7, as shown in Figure 4 The magnetic 7 diagram of the magnetic group (1()) arrangement is the arrangement of the magnetic group (10) disclosed in Fig. 6 == direction. As can be seen from the figure, 'because the two fixed magnets (10) and M2 are arranged in the same direction, the stresses are mutually exclusive, so the magnetic lines (C1) and the magnetic lines ((8) consist of magnetic channels (and close' And the magnetic field line (C bu C2) in the magnetic path (c) is in the direction of the mosquito, and does not generate the reverse inertial magnetic current in the same manner as the conventional electromagnetic device in the opposite direction arrangement mode (such as the third embodiment). When a coil (1) passes through the magnetic path (6) of the two opposite magnets (4), M2) of each magnetic group 〇0), a number of cuts is generated; 丨J seat, therefore, when the coil (1) passes the force line ((1), According to Fleming's right-hand rule, the front half of the road is generated, and the other half of the magnetic field line (10) produces the second half of the electricity. Thus, a complete communication can be generated. Therefore, the present invention should (4) the pole-opposing magnetic
S 201244331 組之電磁裝置的發電方式為一切割即可獲得一單位電壓 ，而無需如傳統異極對向【N—S模式】的電磁裝置， 其線圈必須在N—S間旋轉一週才能產生一電壓。因此 ，本發明電磁裝置之發電效率首重切割數，而非如傳統 者著重在轉速，如此在同一軸線上，當磁組（1〇)越多 、或線圈（L)越多、又或磁組（1〇)與線圈同時 增加時，均可獲得倍數之電流及電壓的輸出，再進一步 運用適當縮減磁組（10)之兩相對磁鐵（Ml、M2)間之 距離，以壓縮磁力通道（c)之磁力密度，其能進一步 提升磁力切割之效能； 藉此，組構成可提昇發電效率和馬達運轉效能之一 種應用同極對向磁組之電磁裝置者。 至於本發明電磁裝置可應用於不同的實施例： 實施例1同徑之盤式電磁裝置 如第8、9及10圖所示，該電磁裝置（20)具有至 少一線圈盤（21)及至少二間隔設置之磁置盤（22)所 組成，亦即令線圈盤（21)與磁置盤（22)交錯間隔排 列’且該等線圈盤（21)外緣利用一固定座（23)予以 固定，又該等線圈盤（21)與該等磁置盤（22)之軸心 間共同穿設有一轉軸（24)，該轉軸（24)可與該等線 圈盤（21)呈樞轉狀、且能帶動各磁置盤（22)同步轉 動’使該等線圈盤（21)被定義為電磁裝置（2〇)之定 子’而該等磁置盤（22)被定義為電磁裝置（2〇)之轉 子，再者該等線圈盤（21)上設有至少一線圈（25)， 其係於線圈盤（21)上形成有至少一貫穿之容槽（21〇 201244331 )，使容設於容槽（210)内的線圈（25)兩側可突出 【如第10圖所示】，而本發明係以8個同徑等角設置 之線圈（25)為主要實施例，又該等磁置盤（22)於對 應線圈盤（21)線圈（25)的同徑位置設有至少一磁鐵 (26)，而本發明係以8個同徑等角設置之磁鐵（26) 為主要實施例，且各線圈盤（21)兩側之磁置盤（22) 上的相對磁鐵（26)形成一個固定磁組（ι〇；)，而該等 磁組（10)之磁鐵（26)係以同極對向的方式排列，如 令兩磁鐵（26)呈Ν—Ν極相對【如第4圖所示】或s —S極相對【如第6圖所示】之排列模式，又該等磁置 盤（22)上於對應各磁鐵（26)位置形成有一容槽（ 220 )，供磁鐵（26)可容設於容槽（ 220 )内【如第 ίο圖所示】，再者兩相對磁鐵（26)與線圈（25)具 有適當之距離，以壓縮其磁力通道之磁力密度，其能^ 步長:升磁力切割之效能，而組構成一發電效率極佳之 電磁裝置。 實施例2異徑同心之盤式電磁裝置 該電磁裝置（20)之線圈盤（21)的線圈（25A、 25B)與磁置盤（22)的相對磁鐵（26A、26B)係以相 對應之異徑同心狀分佈【如第n圖所示】。另該電磁 裝置（20)之兩磁置盤（22)的相對磁鐵（26A、26B) 係以相對應之異徑同心狀分佈、而線圈盤（21)上的線 圈（25)則可同步對應磁置盤（22)的異徑同心磁鐵（ 26A、26B)【如第12圖所示】，又或電磁裝置（2〇) 之線圈盤（21)上的線圈（25A、25B)係以異徑同心狀 分佈、而兩側磁置盤（22)的相對磁鐵（26)則可同步 201244331 對應線圈盤（21)上異徑同心的線圈（25A、25B)。 實施例3多層之盤式電磁裝置 該電磁裝置（20)具有多個線圈盤（2^-210及 間隔設置之多個磁置盤（22,-22^)所組成【如第13 圖所示】’再者該等線圈盤（21,〜21„)上設有至少一 線圈（25丨〜25n)，而該等磁置盤（22ι〜22n+1)於對應 線圈盤（2^-210線圈（25i〜25n)的同徑對向【如 第10圖所示】或異徑對向【如第U、12圖所示】的位 置設有至少一磁鐵（261〜26n+1)，其中Ml與M3之磁極 方向相同，而皆與M2互呈反向，而產生兩個磁力通道 ，以此類推，則n+1個磁置盤即可產生n個磁力通道， 因此具有大幅節省硬體成本卻可獲得極大電機效益之優 點，其能進一步提升磁力切割之效能，而組構成一發電 效率極佳之電磁裝置。 實施例4盤式電磁裝置應用於發電機或馬達時之磁組佈 設方式 ’ 如第14、15圖所示，當該盤式電磁裝置（2〇)作 為發電機或馬達時，該電磁|置（2G)具有—或多個線 圈盤（2l·〜21η)及間隔設置之一或多個磁置盤（221〜 22η+1)所組成，再者該等線圈盤（2l·〜21η)上設有至 少一線圈（25^250 ’而該等磁置盤（22ι〜22η+ι)於 對應線M 〜21〇線圈（25^250的同徑對向 【如第ίο圖所示】或異徑對向【如第u、12圖所 的位置設有至少-磁鐵（26l〜26n+i)，且該等相對之 磁置盤（22!〜22州）中同徑的相鄰磁鐵（26i〜26 11 201244331 可呈同極排列’如同為N極或同為S極設置的模式【如 第14圖所示】。又或該等相對之磁置盤（22,-22^) 中同徑的相鄰磁鐵（26!〜26 n+l)可呈異極排列，為N 極與S極交錯間隔設置的模式【如第15圖所示】。 實施例5盤式電磁裝置應用於馬達時之磁組佈設方式 如第15圖所示’當該盤式電磁裝置（2〇)作為馬 達時，該電磁裝置（20)具有一或多個線圈盤（21ι〜 21n)及間隔設置之一或多個磁置盤（22丨〜22η+ι)所紐 成’再者S亥專線圈盤（21l〜21η)上設有至少一線圈（ 25丨〜25„)，而該等磁置盤（22丨〜22η+〇於對應線圈盤 (2ll〜21η)線圈（25l〜25η)的同徑對向【如第1〇圖 所不】或異徑對向【如第11、12圖所示】的位置設有 至少一磁鐵，且該等相對之磁置盤（22ι 〜22"+丨）中同徑的相鄰磁鐵（2⑴〜26州）係呈異極排列 ’為Ν極與S極交錯間隔設置的模式【如第15圖所示 "此種排列模式’可將電磁裝置（2〇)產生之定向磁 I、查1 \C2延伸為如圖15之如及以2,而有助於無刷 *…違之效率，以提高馬達運轉效能。 實施例6輪圈式電磁裝置 如弟16、17圖所示 二線，環（31)及至少二間隔設置之磁置環（32^ 轴交=令不同徑的線圈環（31)與磁置環（3以: 而=間隔環設’其中該等線圈環（31)可呈固定浓 ^ 4磁置環（32)可被同步轉勤 )被定義為雷磁“= 使該等線圏環( 戮為電磁裝置（30)之定子，而該等磁置環（The electromagnetic generation of the S 201244331 group can be obtained by one cut to obtain one unit voltage, without the need for a conventional heteropolar opposite [N-S mode] electromagnetic device, the coil must be rotated between N-S for one week to produce a Voltage. Therefore, the power generation efficiency of the electromagnetic device of the present invention is the first to cut the number, instead of focusing on the rotation speed as in the conventional one, so on the same axis, when the magnetic group (1〇) is more, or the coil (L) is more, or magnetic When the group (1〇) and the coil are simultaneously increased, the current and voltage output of the multiples can be obtained, and the distance between the two opposing magnets (M1, M2) of the magnetic group (10) is further reduced to compress the magnetic channel ( c) The magnetic density, which can further enhance the performance of the magnetic cutting; thereby, the group constitutes an electromagnetic device applying the same polarity opposite magnetic group which can improve the power generation efficiency and the motor running efficiency. As for the electromagnetic device of the present invention, it can be applied to different embodiments: Embodiment 1 of the same type of disk electromagnetic device, as shown in Figures 8, 9, and 10, the electromagnetic device (20) has at least one coil disk (21) and at least The magnetic disk (22) is arranged at intervals, that is, the coil disk (21) and the magnetic disk (22) are alternately arranged and the outer edges of the coil disks (21) are fixed by a fixing seat (23). And a coil (24) is coaxially disposed between the coil discs (21) and the shafts of the magnetic discs (22), and the rotating shaft (24) is pivotable with the coil discs (21). And the magnetic disk (22) can be rotated synchronously to make the coil disk (21) be defined as the stator of the electromagnetic device (2〇) and the magnetic disk (22) is defined as an electromagnetic device (2〇) And the coil (21) is provided with at least one coil (25) formed on the coil disk (21) with at least one through groove (21〇201244331), so as to be accommodated in the rotor disk (21) The coils (25) in the pockets (210) can be protruded on both sides [as shown in Fig. 10], and the present invention is mainly composed of eight coils (25) of the same diameter equiangular arrangement. For example, the magnetic disk (22) is provided with at least one magnet (26) at the same diameter position of the coil (25) of the corresponding coil disk (21), and the present invention is a magnet with eight equal-diameter equiangular angles. (26) As a main embodiment, the opposing magnets (26) on the magnetic disks (22) on both sides of each coil disk (21) form a fixed magnetic group (ι;;) and the magnetic groups (10) The magnets (26) are arranged in the same direction of the same pole, such as making the two magnets (26) appear Ν-Ν pole relative to [as shown in Figure 4] or s-S pole relative [as shown in Figure 6] In the arrangement mode, the magnetic disk (22) is formed with a cavity (220) at a position corresponding to each magnet (26), and the magnet (26) can be accommodated in the cavity (220) [as shown in FIG. As shown, the two opposing magnets (26) and the coil (25) have an appropriate distance to compress the magnetic density of the magnetic path, which can be stepped: the performance of the magnetic cutting, and the group constitutes a power generation efficiency Good electromagnetic device. Embodiment 2 Reducing Concentric Disc Electromagnetic Device The coil (25A, 25B) of the coil disk (21) of the electromagnetic device (20) and the opposing magnet (26A, 26B) of the magnetic disk (22) are corresponding to each other. Heterogeneous concentric distribution [as shown in Figure n]. In addition, the opposing magnets (26A, 26B) of the two magnetic disks (22) of the electromagnetic device (20) are concentrically distributed with corresponding different diameters, and the coils (25) on the coil disk (21) are synchronously corresponding. The different diameter concentric magnets (26A, 26B) of the magnetic disk (22) are as shown in Fig. 12, or the coils (25A, 25B) on the coil disk (21) of the electromagnetic device (2〇) are different. The diameters are concentrically distributed, and the opposing magnets (26) of the magnetic disk (22) on both sides can synchronize the coils (25A, 25B) of the different diameters and concentrics on the coil disk (21) in 201244331. Embodiment 3 Multi-layer disk electromagnetic device The electromagnetic device (20) has a plurality of coil disks (2^-210 and a plurality of magnetic disks (22, -22^) arranged at intervals [as shown in Fig. 13] 】 'There are at least one coil (25丨~25n) on the coil discs (21,~21„), and the magnetic discs (22ι~22n+1) are on the corresponding coil discs (2^-210) The coils (25i to 25n) are provided with at least one magnet (261~26n+1) at the same direction as shown in Fig. 10 or in the opposite direction (as shown in Figs. U and 12). Ml and M3 have the same magnetic pole direction, and both are opposite to M2, and two magnetic channels are generated, and so on, n+1 magnetic discs can generate n magnetic channels, thus greatly saving hardware. The cost can obtain the advantage of great motor benefit, which can further improve the performance of magnetic cutting, and form an electromagnetic device with excellent power generation efficiency. Embodiment 4 Magnetic disk layout mode when the disk electromagnetic device is applied to a generator or a motor ' As shown in Figures 14 and 15, when the disc type electromagnetic device (2〇) is used as a generator or a motor, the electromagnetic | (2G) has - a plurality of coil discs (2l·~21n) and one or more magnetic discs (221 to 22n+1) are arranged at intervals, and at least one coil is provided on the coil discs (2l·~21n) ( 25^250 ' and the magnetic disk (22 ι ~ 22 η + ι) in the corresponding line M ~ 21 〇 coil (25 ^ 250 of the same diameter opposite [as shown in Figure ίο] or the opposite direction [such as The positions of the u and 12 are provided with at least magnets (26l~26n+i), and the adjacent magnets of the same diameter (26i~26 11 201244331) can be presented in the opposite magnetic discs (22!~22 states). The same pole arrangement 'like the mode set for the N pole or the same S pole [as shown in Figure 14] or the adjacent magnets of the same diameter in the opposite magnetic discs (22, -22^) (26 !~26 n+l) can be arranged in a different polarity, which is a mode in which the N pole and the S pole are alternately spaced [as shown in Fig. 15]. The magnetic group layout method of the fifth embodiment of the disk electromagnetic device applied to the motor is as follows: As shown in Fig. 15, when the disk electromagnetic device (2 turns) is used as a motor, the electromagnetic device (20) has one or more coil disks (21o to 21n) and one or more magnetic disks (e. 22丨~22η+ι)本纽成' Furthermore, at least one coil (25丨~25„) is provided on the S-coil coils (21l~21η), and the magnetic discs (22丨~22η+〇 are corresponding to the coils of the corresponding coil discs (2ll~21η)) 25l~25η) is provided with at least one magnet at the same position as the opposite direction (as shown in Fig. 1) or the opposite direction (as shown in Figs. 11 and 12), and the opposite magnetic discs ( 22ι 〜22"+丨) The adjacent magnets of the same diameter (2(1)~26 states) are in a different pole arrangement'. The pattern is set between the drain and the S pole. [As shown in Fig. 15] 'The directional magnetic I generated by the electromagnetic device (2〇) can be extended to 1 and C2 as shown in Fig. 15 and 2, which contributes to the efficiency of brushless*...in order to improve the running efficiency of the motor. Embodiment 6 rim type electromagnetic device, such as the two lines shown in the figures 16, 17 and the ring (31) and at least two spaced magnetic rings (32 ^ axis intersection = ring coils (31) with different diameters and magnetic arrangement The ring (3 is: and the spacer ring is set to 'where the coil ring (31) can be fixed and the magnetic ring (32) can be synchronously transferred) is defined as the lightning magnetic "= make the wire loop (戮 is the stator of the electromagnetic device (30), and the magnetic rings (
S 12 201244331 )被定義為電磁裝置（30)之轉子。又或該等線圈環（ 31)可被同步轉動、而該等磁置環（32)係呈固定狀， 使該等線圈環（31)被定義為電磁裝置（30)之轉子， 而該等磁置環（32)被定義為電磁裝置（30)之定子。 再者該等線圈環（31)上設有至少一線圈（35)，而本 發明係以8個同徑等角設置之線圈（35)為主要實施例 ’又該等磁置環（32)於對應線圈環（31)線圈（35) 的位置s又有至少一磁鐵（36 )，而本發明係以4個同徑 等角设置之磁鐵（36)為主要實施例，且各線圈環（31 )内、外緣之磁置環（32)上的相對磁鐵（36)形成一 個固定磁組（10)，而該等磁組（10)之磁鐵（36)係 以同極對向的方式排列，如令兩磁鐵（36)呈Ν—Ν極 相對【如第16圖所示】或S—S極相對【如第17圖所 不】之排列模式，再者兩相對磁鐵（36)與線圈（35) 具f適f之距離，以壓縮其磁力通道之磁力密度，其能 進一步提升磁力蝴之效能，而組構成-發f效率極佳 之電磁裝置。 實施例7隨異位之輪圈式電磁裝置 _、該電磁襄置（3〇)之線圈環（31)的線圈（35A、 與磁置環（32)的相對磁鐵（36A、36B)係以相 異位狀分佈【如第18圖所示】。另該電磁 I 兩磁置環（32)的相對磁鐵（、36B) 圈^3;) 5之同徑異位狀分佈、而線圈環（31 )上的線 圈㈤射畔對應【如第19圖射】。 深 實施例8多圈之輪圈式電磁裝置 13 201244331 該電磁裝置（30)具有多個線圈環（3i1〜3in)及 間隔設置之多個磁置環（32l〜32n+1)所組成，再者該等 線圈環（3l·〜31n)上設有至少一線圈（35ι〜35η)， 而該等磁置環（32丨〜32n+1)於對應線圈環（31丨〜31n) 線圈（35!〜35„)的位置設有至少一磁鐵（3匕〜36n丨） ，其能進一步提升磁力切割之效能，而組構成一發電效 率極佳之電磁裝置。 實施例9輪圈式電磁裝置應用於發電機或馬達時之磁組 佈設方式 * 如第16、17及20、21圖所示，當該輪圈式電磁裝 置（30)作為發電機或馬達時，該電磁裝置（3〇)具有 一或多個線圈環（3h〜31n)及間隔設置之一或多個磁 置環（32丨〜32η+ι)所組成，再者該等線圈環（31丨〜31n )上設有至少一線圈（351〜35〇，而該等磁置環（32l 〜32n+1)於對應線圈環（3l·〜31〇線圈（35丨〜35n)的 位置設有至少一磁鐵，且該等相對之磁置 環（32丨〜32叫）中同徑的相鄰磁鐵（36丨〜36n+丨）可呈同 極排列’如同為N極或同為S極設置的模式【如第16 、20圖所示】。又或該等相對之磁置環（321〜32㈣） 中同徑的相鄰磁鐵可呈異極排列，為N極 與S極交錯間隔設置的模式【如第17、21圖所示】。 實施例10輪圈式電磁裝置應用於馬達時之磁組佈設方 式 如第17、21圖所示，當該輪圈式電磁震置（3〇) 作為馬達時，該電磁裝置（30)具有一或多個線圈環（ 201244331 31〜31„)及間隔设置之一或多個磁置環 所組成’再者該等線圈環（3ll〜3ln)上設有至少一線 圈^〜35n) ’而該等磁置(32ι〜32n+〇於對應線 圈裱（31ι〜31„)線圈（35^3“）的位置設有至少一 磁鐵（36^36-)，且該等相對之磁置環（32i〜3d 中同徑的相鄰磁鐵（36l〜36n+1)係、呈異極排列，為_ 與s極交錯間隔設置的模式【如第17、21圖所示】， 其月b減少功率的損耗，以提高馬達運轉效率。 透過前述的說明，實務上為求得最大切割數和較大 電力輸出，可採多層狀或多圈狀之排列方式，且在盤式S 12 201244331 ) is defined as the rotor of the electromagnetic device (30). Or the coil loops (31) can be rotated synchronously, and the magnetic loops (32) are fixed, such that the coil loops (31) are defined as the rotor of the electromagnetic device (30), and such The magnetic ring (32) is defined as the stator of the electromagnetic device (30). Furthermore, at least one coil (35) is disposed on the coil loops (31), and the present invention uses eight coils (35) arranged at equal angles as the main embodiment and the magnetic loops (32). There is at least one magnet (36) at the position s of the coil (35) corresponding to the coil ring (31), and the present invention uses four magnets (36) arranged at equal angles as the main embodiment, and each coil ring ( 31) The opposing magnets (36) on the inner and outer magnetic rings (32) form a fixed magnetic group (10), and the magnets (36) of the magnetic groups (10) are aligned in the same polarity. Arrange, such as the two magnets (36) are Ν-Ν pole relative to [as shown in Figure 16] or S-S pole relative to [as shown in Figure 17], and then two opposing magnets (36) and The coil (35) has a distance of f to f, in order to compress the magnetic density of the magnetic path, which can further enhance the performance of the magnetic butterfly, and the composition constitutes an electromagnetic device with excellent efficiency. Embodiment 7 is a rim-type electromagnetic device _, a coil (35A of the coil ring (31) of the electromagnetic device (3 、), and a counter magnet (36A, 36B) of the magnetic ring (32) The dissimilar distribution is as shown in Fig. 18. The electromagnetic (I) magnetic ring (32) is opposite to the magnet (, 36B) ring ^3;) 5 isotropically distributed, and the coil ring ( 31) The coil (5) on the shot corresponds to [as shown in Figure 19]. Deep Embodiment 8 Multi-turn rim type electromagnetic device 13 201244331 The electromagnetic device (30) is composed of a plurality of coil loops (3i1 to 3in) and a plurality of magnetic rings (32l~32n+1) arranged at intervals, and then The coil loops (3l·~31n) are provided with at least one coil (35ι~35n), and the magnetic loops (32丨~32n+1) are corresponding to the coil loops (31丨~31n) coils (35) At least one magnet (3匕~36n丨) is provided at the position of ~35„), which can further enhance the performance of magnetic cutting, and the group constitutes an electromagnetic device with excellent power generation efficiency. Embodiment 9 Application of rim type electromagnetic device Magnetic group arrangement method for generator or motor * As shown in Figures 16, 17, and 20, 21, when the rim type electromagnetic device (30) is used as a generator or a motor, the electromagnetic device (3 〇) has One or more coil loops (3h~31n) and one or more magnetic loops (32丨~32η+ι) are arranged at intervals, and at least one of the coil loops (31丨~31n) is provided Coils (351 to 35 〇, and the magnetic rings (32l to 32n+1) are provided to the corresponding coil loops (3l·~31〇 coils (35丨~35n)) to a magnet, and the adjacent magnets of the same diameter (32丨~36n+丨) in the opposite magnetic ring (32丨~32) can be arranged in the same pole as the mode set for the N pole or the S pole. [As shown in Figures 16 and 20], or in the opposite magnetic ring (321~32(4)), the adjacent magnets of the same diameter may be arranged in different poles, and the N-pole and S-pole are alternately spaced. As shown in Figures 17 and 21, the magnetic group layout method of the embodiment 10 rim type electromagnetic device applied to the motor is as shown in Figs. 17 and 21, when the rim type electromagnetic shock (3 〇) is used as the motor. When the electromagnetic device (30) has one or more coil loops (201244331 31~31 „) and one or more magnetic loops of the interval arrangement, the coil loops (3ll~3ln) are further provided. At least one coil ^~35n) ' and at least one magnet (36^36-) is provided at the position of the corresponding coil (32^3") coil (35^3") The opposite magnetic rings (the adjacent magnets (36l~36n+1) of the same diameter in the 32i~3d are arranged in different poles, and are arranged in a pattern of _ and s-stagger spacing [such as the 17th, 21st As shown in the figure, the monthly b reduces the power loss to improve the motor operating efficiency. Through the above description, in practice, in order to obtain the maximum number of cuts and large power output, a multi-layer or multi-ring arrangement can be adopted. And in the disc
電磁裝置（20)的線圈（25A、25B)或磁鐵（26A、26B )上可呈異徑同心的模式排列，又或在輪圈式電磁裝置 (30)的線圈（35A、35B)或磁鐵（36A、36B)上可呈 同徑異位的模式排列，如此一轉即可獲得磁組數（M) X 線圈數（C)之切割數，相較於傳統必須提高轉數才能 提尚切割數之方式，其效率之差異不言可喻，而能用於 製作南效能的發電機或用於生產高效能的馬達。 綜上’由於本發明之電磁裝置（20、30)各磁級（ 1〇)的相對磁鐵（26、36)係呈同極對向排列【如 N極相對或S—S極相對】，其應力為互相排斥的作用 ’因此在磁力通道内的磁力線，是受到壓迫而緊密的， 且磁力通道内的磁力線方向是固定的，使其一組線圈（ 25、35)通過同極對向的磁組（1〇)即可產生一切割， 而產生一完整的交流電壓，因此本發明的發電效率首重 切。〗數而非轉速，透過切割數的增加，可獲得極大之電 流及電麗輸出，且相較於傳統同規格之發電機或馬達， 15 201244331 可大幅縮小其體積與重量，同時線圈（25、35)與磁鐵 (26、36)間因同極相斥，故不致產生磁吸效應，如此 可大幅降低其啟動電流，並使其運轉更為順暢，而能易 於啟動扭距大之高效馬達，並可有效減少功率損耗，而 具有提昇發電效率和馬達運轉效能之效。 藉此，可以理解到本發明為一創意極佳之創作，除 了有效解決習式者所面臨的問題，更大幅增進功效，: 在相同的技術領域中未見相同或近似的產品創作或公開 使用，同時具有功效的增進，故本發明已符合發明專利The coils (25A, 25B) or magnets (26A, 26B) of the electromagnetic device (20) may be arranged in a concentric concentric pattern, or in the coil (35A, 35B) or magnet of the rim type electromagnetic device (30). 36A, 36B) can be arranged in the same-diameter mode, so that the number of magnetic groups (M) X number of coils (C) can be obtained by one revolution, and the number of cuts can be increased compared with the conventional one. In this way, the difference in efficiency is self-evident, and can be used to make a south-efficiency generator or to produce a high-performance motor. In summary, the opposing magnets (26, 36) of the magnetic stages (1, 〇) of the electromagnetic device (20, 30) of the present invention are arranged in the same polarity (such as N-pole or S-S pole), The stress acts as a mutual exclusion'. Therefore, the magnetic lines of force in the magnetic path are tightly pressed, and the direction of the magnetic lines in the magnetic path is fixed, so that a group of coils (25, 35) pass through the same pole. The group (1〇) can produce a cut and generate a complete AC voltage, so the power generation efficiency of the present invention is first cut. 〖Number instead of rotation speed, through the increase of the number of cuts, you can get very large current and electric output, and compared with the traditional generator or motor of the same specification, 15 201244331 can greatly reduce its volume and weight, while the coil (25, 35) Because the magnets (26, 36) are repelled by the same pole, they do not cause a magnetic attraction effect, so that the starting current can be greatly reduced, and the operation can be made smoother, and the high-efficiency motor with a large torque can be easily started. It can effectively reduce power loss, and has the effect of improving power generation efficiency and motor running efficiency. In this way, it can be understood that the present invention is an excellent creation, and in addition to effectively solving the problems faced by the practitioners, the effect is greatly enhanced:: The same or similar product creation or public use is not seen in the same technical field. At the same time, it has an improvement in efficacy, so the invention has been in accordance with the invention patent
有關「新穎性」與「進步性」的要件，乃依法提 發明專利。 F 【圖式簡單說明】 第1圖：係弗來明右手定律之手指示意圖。 第2圖：係弗來明右手定律之電磁應用示意圖。 第3圖.係習式電磁裝置的磁力線分佈示意圖。 第4圖.係本發明同極對向磁組之電磁裝置的配置示惫 圖。 第5圖·係本發明同極對向磁組之電磁裝置的磁力線分 佈示意圖。 第6圖.係本發明同極對向磁組之電磁裝置的另一種配 置示意圖。 第7圖·係本發明同極對向磁組之電磁裝置的另一種配 置之磁力線分佈示意圖。 第8圖’係本發明之盤式電磁裝置中最佳實施例的外觀 不意圖，供顯示盤式電磁裝置之狀態。 圖·係本發明之盤式電磁裝置中最佳實施例的簡要 201244331 架構示意圖。 第圖··係本發明之盤式電磁裝置中最佳實施例的側 視剖面示意圖。 第11圖：係本發明之盤式電磁裝置中異徑同心之實施 例的簡要配置示意圖。 第12圖：係本發明之盤式電磁裝置中異徑同心之另一 實施例的簡要配置示意圖。 第13圖：係本發明之盤式電磁裝置中多層狀之實施例 的簡要配置示意圖。 第14圖.係本發明之盤式電磁裝置中同徑相鄰磁鐵呈 同極排列之簡要配置示意圖。 第15圖：係本發明之盤式電磁裝置中同徑相鄰磁鐵呈 異極排列之簡要配置示意圖。 第16圖.係本發明之輪圈式電磁裝置中最佳實施例的 簡要配置示意圖。 第17圖：係本發明之輪圈式電磁裝置中另—實施例的 簡要配置示意圖。 第18圖·係本發明之輪圈式電磁裝置中同徑異位之最 佳實施例的簡要配置示意圖。 第19圖：係本發明之輪圈式電磁裝置中同徑異位之另 一實施例的簡要配置示意圖。 20圖：係本發明之輪圈式電磁裝置中呈多圈狀佈設 的簡要配置示意圖。 .係本發明之輪圈式電磁裝置中另一呈多圈狀 佈設的簡要配置示意圖。 第圖 國 【主要元件符號說明】 201244331 (10) 磁組 (Ml) 磁鐵 (M2) 磁鐵 (L) 線圈 (Cl) 磁力線 (C2) 磁力線 (C) 磁力通道 (20) 電磁裝置 (21) 線圈盤 (210) 容槽 (22) 磁置盤 ( 220) 容槽 (23) 固定座 (24) 轉軸 (25) 線圈 (26) 磁鐵 (30) 電磁裝置 (31) 線圈環 (32) 磁置環 (35) 線圈 (36) 磁鐵The requirements for "novelty" and "progressiveness" are based on the invention of patents. F [Simple description of the diagram] Figure 1: Schematic diagram of the finger of Fleming's right-hand rule. Figure 2: Schematic diagram of the electromagnetic application of Fleming's right-hand rule. Fig. 3 is a schematic diagram showing the distribution of magnetic lines of a conventional electromagnetic device. Fig. 4 is a view showing the arrangement of an electromagnetic device of the same-pole magnetic group of the present invention. Fig. 5 is a schematic view showing the distribution of magnetic lines of the electromagnetic device of the same-pole magnetic group of the present invention. Fig. 6 is a view showing another configuration of the electromagnetic device of the same-pole magnetic group of the present invention. Fig. 7 is a schematic view showing the distribution of magnetic lines of force in another configuration of the electromagnetic device of the same-pole magnetic group of the present invention. Fig. 8 is an appearance of a preferred embodiment of the disk type electromagnetic device of the present invention. It is not intended to show the state of the disk type electromagnetic device. BRIEF DESCRIPTION OF THE DRAWINGS Figure 4 is a schematic diagram of a preferred embodiment of a disk electromagnetic device of the present invention. Fig. is a side cross-sectional view showing a preferred embodiment of the disk type electromagnetic device of the present invention. Fig. 11 is a schematic view showing a schematic configuration of an embodiment in which the different diameters are concentric in the disk type electromagnetic device of the present invention. Fig. 12 is a schematic view showing the configuration of another embodiment in which the different diameters are concentric in the disk type electromagnetic device of the present invention. Fig. 13 is a schematic view showing the configuration of a multilayered embodiment of the disk type electromagnetic device of the present invention. Fig. 14 is a schematic view showing the schematic arrangement of adjacent magnets of the same diameter in the disc type electromagnetic device of the present invention. Fig. 15 is a schematic view showing a schematic arrangement of adjacent magnets of the same diameter in the disc type electromagnetic device of the present invention. Fig. 16 is a schematic view showing the configuration of a preferred embodiment of the rim type electromagnetic device of the present invention. Fig. 17 is a schematic view showing a schematic configuration of another embodiment of the rim type electromagnetic device of the present invention. Fig. 18 is a schematic view showing a schematic configuration of a preferred embodiment of the same-path eccentricity in the rim type electromagnetic device of the present invention. Fig. 19 is a schematic view showing a schematic configuration of another embodiment of the same-diameter eccentricity in the rim type electromagnetic device of the present invention. Figure 20 is a schematic view showing a schematic configuration of a multi-turn arrangement in the rim type electromagnetic device of the present invention. Another schematic configuration diagram of a multi-turn arrangement in the rim type electromagnetic device of the present invention.图图国 [Main component symbol description] 201244331 (10) Magnetic group (Ml) Magnet (M2) Magnet (L) Coil (Cl) Magnetic field line (C2) Magnetic field line (C) Magnetic channel (20) Electromagnetic device (21) Coil disk (210) Cassette (22) Magnetic plate (220) Cassette (23) Mounting seat (24) Rotary shaft (25) Coil (26) Magnet (30) Electromagnetic device (31) Coil ring (32) Magnetic ring ( 35) Coil (36) Magnet