TW201131947A - Magnetic transmission assembly and driving motor thereof - Google Patents

Magnetic transmission assembly and driving motor thereof Download PDF

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Publication number
TW201131947A
TW201131947A TW99128536A TW99128536A TW201131947A TW 201131947 A TW201131947 A TW 201131947A TW 99128536 A TW99128536 A TW 99128536A TW 99128536 A TW99128536 A TW 99128536A TW 201131947 A TW201131947 A TW 201131947A
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Taiwan
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ring
magnetic
blocks
stator
sub
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TW99128536A
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Chinese (zh)
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TWI441424B (en
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Ming-Tsan Peng
Li-Ju Cheng
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Ind Tech Res Inst
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Priority to TW99128536A priority Critical patent/TWI441424B/en
Priority to US12/904,946 priority patent/US8541922B2/en
Priority to JP2011043943A priority patent/JP2011182638A/en
Publication of TW201131947A publication Critical patent/TW201131947A/en
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Publication of TWI441424B publication Critical patent/TWI441424B/en

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Abstract

A magnetic transmission assembly is adapted to integrate with a power generator or an electrical motor. The assembly includes a rotor, a stator and a permeable element. The stator coaxially covers the rotor. The stator and the rotor have ST1 and R pole pairs, respectively. Permeable element is disposed between the stator and the rotor and has several permeable regions. When the permeable element is activated, the permeable element selectively makes PN1 or PN2 permeable regions correspond to and sandwiched between the R and ST1 pole pairs. The sandwiched permeable regions react with both the magnetic field of R and ST1 pole pairs to in a specific gear-ratio. Accordingly, a motor driver can drive the magnetic transmission assembly and make the rotor rotate at different rotational speeds.

Description

201131947 六、發明說明: 【發明所屬之技術領域】 本提案係為一種變速組成(transmission assemWy),特別β 一 磁性變速組成。 【先前技術】 變速器係應用於動力傳輸,除了能將動力進行中繼與傳送 外’另具有將動力源的轉速減速或增速的功能u於傳統汽車 引擎的變速組成有機械式的變速箱及油壓式變速箱。應用於電動 車或油電混合車的則有磁性變速器。 變速馬達之技術可見於西元1976年9月14日公告之美國第 3,980,937 rFractional Horsepower Gear Motor j > ^ 達所輸出的動力經過機械式齒輪組以達到扭力轉換及變速效果。 另於西元1998年10月20日公告之美國第5,825,111號專利 Single-phase induction motot 4/6 pole common winding connection with magnetic motive force symmetrically distributed」及西元 2009 年10月ό日公告之美國第7,598,648號專利「2/6 pole single-phase induction motor having shared windings」,係揭露利用改變感應馬達 定子的極數的方式來達成變速之目的。 磁性變速器之相關技術亦可見於由K. Atallah及D. Howe於國 際電機電子工程師學會期刊在西元2001年7月發表的文章「A Novel High-Performance Magnetic Gear」(IEEE Transactions on201131947 VI. Description of the invention: [Technical field to which the invention pertains] This proposal is a transmission assemWy, in particular a β-magnetic shifting composition. [Prior Art] The transmission is used for power transmission. In addition to relaying and transmitting power, it has the function of decelerating or increasing the speed of the power source. The gearbox of the conventional automobile engine has a mechanical gearbox and Hydraulic gearbox. For electric vehicles or hybrid vehicles, there are magnetic transmissions. The technology of the variable speed motor can be found in the US 3,980,937 rFractional Horsepower Gear Motor j > announced on September 14, 1976. ^ The output power of the motor passes through the mechanical gear set to achieve the torque conversion and shifting effect. In addition, US Patent No. 5,825,111 issued on October 20, 1998, "Single-phase induction motomoto 4/6 pole common winding connection with magnetic motive force symmetrically distributed" and the United States No. 7,598,648 announced on October 30, 2009 The patent "2/6 pole single-directional induction motor having shared windings" discloses the purpose of achieving shifting by changing the number of poles of the induction motor stator. The related technology of the magnetic transmission can also be found in the article "A Novel High-Performance Magnetic Gear" published by K. Atallah and D. Howe in the Journal of the International Society of Electrical and Electronics Engineers in July 2001.

Magnetics,Vol. 37, No. 4, July, 2001)。 201131947 前述機械式變速器係有噪音大與重量重之缺點,而一般磁性 變速器雖可減少振動與噪音,但亦不能減少重量。此外,在電動 車々應用上’電動馬達須配合不同的行車扭力及行駛速度之需 求’亦須兼顧高效率運轉之要求,故常將馬達與變速ϋ搭配,在 此種心配料下,馬達與魏難體雜動辨密度通常不易提 高(因馬達與變速器的總重量重)。 【發明内容】 基於上述問題,所提出之磁性變速組成係易與電動機(如電動 馬達)或發電機做⑽整合而具有重量輕之特色,故能提高驅動功 率密度。 依據實%例,一種磁性變速組成包含轉子、定子及導磁元 件。轉子與定子係_套設,轉子具有多個磁極並具有r個極對 數。定子具有多個磁極及個極對數。導磁元件位於轉子與定 子之間並具有乡個導磁體。當導磁元件被致動時,導磁元件係選 擇性地使ΡΝ1個或ρΝ2健些導磁體職於轉子與定?之間其 中 ΡΝ1-3 $ R+ST1 $ ρνι+3,ΡΝ2-3 ^ R+STl g ΡΝ2+3。 依據導磁元件的—實施例,前述導磁元件包含第—環及第二 環,第一環與第二環係軸向連接,第-環具有PN1個導磁子塊, 第二環具有PN2個導磁子塊’當導磁元件被軸向致動時導磁元 件係選擇性地使第·環或第二環被移至轉子與定子之間。 依據導磁元件的第一實施例’前述導磁元件包含第一環及第 -壤’第-環係位於第二環之徑向外㈣且第—環與第二環配置於" Ιό] 5 201131947 定子與轉子之間,當導磁元件被致鱗,第_環與第二環係相對 位移於第-位置與第二位置之間’當第一環與第二環位於第一位 置時’導磁元件具有PN1個該導磁體,當第—環與第二環位於第 二位置時,導磁元件具有|^2個該導磁體。 依據另-實關,定子包含多佩應_及極數調變電路, 感應線圈被導電時伽彡成雜,而極數碰電路係選擇性地切換 感應線圈於前述ST1個極對數及一 ST2個極對數之間。其中, PN2-3 S R+ST2 $ PN2+3。 依據又一實施例,磁性變速組成包含轉子、定子及導磁元件。 轉子具有多個磁極,轉子的磁極具有R個極對數。定子與轉子同 軸套设,疋子並具有多個磁極,定子的磁極具有ST1個極對數。 導磁元件被配置於轉子與定子之間並具有pNl個導磁子塊,pN1 個導磁子塊對應配置於轉子與定子之間,其中,ρΝ1·3 g r+sti S PN1+3。 前述導磁元件配置於定子與轉子之間,藉由導磁元件可選擇 性地變動導磁體數量(意即其磁隙數量亦變動)的設計,即可在定子 與轉子間產生不同的變速比(定子轉速比轉子轉速)。其次,在另一 實施例中,定子的磁對數亦具有可變換之設計’如此一來’搭配 導磁元件與轉子’亦能達到產生不同變速比之目的前述的導磁 元件、定子及轉子均可為中空環形之設計,使得整個磁性變速組 成之體積及重量都相當小,並能夠易於與電動馬達做内部整合, 得到較高的驅動功率密度(瓦/公斤,W/Kg或瓦/體積,W/m3)。 201131947 有關本提案的特徵與實作’航合圖式及實施舰明如下。 【實施方式】 ° 錢,請同時參閱「第!圖」及「第2圖」,其係分別為依據 本提案-實施例的立體結構示意圖及立體分解圖。圖中可以見 悉’磁性變速組成係包含轉子2〇、定子3〇及導磁元件4〇(亦可稱 為導磁變速元件)。磁性變速組成可適於與電動機(如電動馬達)或 發電機進行整合。例如若與電動車之電動馬達進行整合,由馬達 鲁驅動器輪出電力予磁性變速組成,則磁性變速組成即能從轉子處 產生旋轉動力,同時’由馬達驅動器適當地㈣雜變速組成之 變速比’磁性變速組成即能輸出不同的功率(功率=驅出扭力X轉 速)。由於此磁性變速組朗時包含了電動機與變速器之功能,整 體體積及重里較低,目而能制較高魏動功率密度。此處的驅 動功率^度可以是但不限於輸出功率除以體積,或者是輸出功率 除、重星(即(輸出扭力χ轉速)/體積、或(輪出扭力X轉速)/重量)。 _ 从’若是將磁性變速組錢用於電械巾,則可由轉子2〇 承接旋轉動力,定子30的_(容後詳述)即可輸出經磁場切割所 產生的電力^電力可經過整流及穩壓電路後輸出。由於磁性變 速組成可以經由控制而產生變速比,故當輸入的旋轉動力有較大 的變動’或者欲得到較佳H哺換效率,可以由控繼調整磁 性變速組成的變速比來達成。 请續參閱「第1圖」及「第2圖」,定子30可為固定磁鐵或 感應磁鐵(或稱電磁鐵),在本實施例中係以感應磁鐵為例。定t 7 201131947 30之内側係環形配置有多個凸塊32a,32b。各凸塊32a,32b係纏 繞有感應線圈(容後詳述),感應線圈被通電時,即可形成磁極。以 圖式的實施例為例,定子30具有48個凸塊32a,32b,每個凸塊 32a,32b被通電後即可形成一磁極對。在此例中,共有四相(4 phases),母一相即有12個極對數(20 Pole Pairs) ^請同時參照「第 3圖」,其係為依據本提案一實施例的定子3〇的磁對數示意圖。 圖中可以看出’相鄰的磁極為相反極性(磁北極N與磁南極s)。二 個相鄰相反極性的磁極為一磁對(例如圖式的S1,N1為一磁對 從圖中可以看出共有12個極對數,此極對數僅為一實施態樣,本 提案並不限於此磁對數,以下以ST1個極對數表示。 轉子20可為固定磁鐵或感應磁鐵,在本實施例中,轉子2〇 係以固定磁鐵為例進行說明。轉子20具有多個磁極並具有r個極 對數’在本實施例中,轉子20係以具有20個極對數為例。定子 與轉子20係同軸配置(同軸套設),且在此實施例中,轉子2〇 係配置於定子30的徑向内側,但並不以此為限。亦可將定子3〇 配置於轉子20的徑向内侧,仍能達到本提案之目的。其次,轉子 20的磁極(磁力線)的方向係朝向定子3〇的磁極(磁力線)的方向。 導磁元件40可以是薄片鋼(laminated steel),其材料可以是軟 越材料(Soft Magnetic Composite,SMC),以減少渦電流(EddyMagnetics, Vol. 37, No. 4, July, 2001). 201131947 The aforementioned mechanical transmission has the disadvantages of high noise and heavy weight, while the general magnetic transmission can reduce vibration and noise, but it cannot reduce the weight. In addition, in the application of electric ruts, 'the need for electric motors to match different driving torques and driving speeds' must also take into account the requirements of high-efficiency operation. Therefore, the motor and the shifting cymbal are often matched. Under such heart ingredients, the motor and Wei Difficult body dynamism is usually not easy to increase (due to the total weight of the motor and the transmission). SUMMARY OF THE INVENTION Based on the above problems, the proposed magnetic shifting composition is easy to integrate with an electric motor (such as an electric motor) or a generator (10) and has a light weight characteristic, so that the driving power density can be improved. According to the real example, a magnetic shifting composition includes a rotor, a stator, and a magnetically permeable member. The rotor and the stator are sleeved, and the rotor has a plurality of magnetic poles and has r pole pairs. The stator has a plurality of magnetic poles and a number of pole pairs. The magnetically conductive element is located between the rotor and the stator and has a magnetizer. When the magnetically permeable element is actuated, the magnetically permeable element selectively causes the ΡΝ1 or ρΝ2 to act as the stator and the stator. Between ΡΝ 1-3 $ R+ST1 $ ρνι+3, ΡΝ 2-3 ^ R+STl g ΡΝ2+3. According to an embodiment of the magnetically conductive element, the magnetic conductive element comprises a first ring and a second ring, the first ring and the second ring are axially connected, the first ring has PN1 magnetic sub-blocks, and the second ring has PN2 The magnetically permeable sub-blocks' selectively bias the first or second ring between the rotor and the stator when the magnetically permeable element is axially actuated. According to a first embodiment of the magnetically permeable element, the magnetic conductive element comprises a first ring and a first-thickness-first ring system located radially outward of the second ring (four) and the first ring and the second ring are disposed at " 5 201131947 Between the stator and the rotor, when the magnetically conductive element is scaled, the first ring and the second ring are relatively displaced between the first position and the second position 'When the first ring and the second ring are in the first position The magnetically conductive element has PN1 of the magnetizer, and when the first ring and the second ring are in the second position, the magnetic conductive element has |^2 of the magnetizers. According to another-reality, the stator comprises a multi-penetration _ and a pole-number modulation circuit, wherein the induction coil is galvanically mixed when conducting, and the pole-number circuit selectively switches the induction coil to the ST1 pole pair and one ST2 between the pole pairs. Among them, PN2-3 S R+ST2 $ PN2+3. According to yet another embodiment, the magnetic shifting composition comprises a rotor, a stator and a magnetically permeable element. The rotor has a plurality of magnetic poles, and the magnetic poles of the rotor have R pole pairs. The stator and the rotor are sleeved on the same shaft, and the dice have a plurality of magnetic poles, and the magnetic poles of the stator have ST1 pole pairs. The magnetic conductive element is disposed between the rotor and the stator and has pN1 magnetic conductive sub-blocks, and the pN1 magnetic conductive sub-blocks are correspondingly disposed between the rotor and the stator, wherein ρΝ1·3 g r+sti S PN1+3. The magnetic conductive element is disposed between the stator and the rotor, and the design of the magnetic flux element can selectively change the number of the magnetic conductive bodies (that is, the number of magnetic gaps also changes), so that different gear ratios can be generated between the stator and the rotor. (The stator speed is higher than the rotor speed). Secondly, in another embodiment, the magnetic logarithm of the stator also has a convertible design. Thus, the magnetic conducting component, the stator and the rotor can be used for the purpose of generating different gear ratios. Designed as a hollow ring, the entire magnetic shifting composition is relatively small in size and weight, and can be easily integrated with an electric motor for high drive power density (Watt/kg, W/Kg or watt/volume, W/m3). 201131947 Characteristics and implementation of this proposal 'The chart and implementation of the ship's chart are as follows. [Embodiment] Please refer to "Fig. 2" and "2nd drawing" at the same time, which are respectively a three-dimensional structure and an exploded view according to the present proposal-embodiment. As can be seen in the figure, the magnetic shifting composition includes a rotor 2, a stator 3, and a magnetically permeable element 4 (also referred to as a magnetically permeable element). The magnetic shifting composition can be adapted to be integrated with an electric motor (such as an electric motor) or a generator. For example, if it is integrated with the electric motor of the electric vehicle and the motor is driven by the motor-driven drive to the magnetic shifting component, the magnetic shifting component can generate rotational power from the rotor, and the gear ratio of the motor drive is appropriately (four) misaligned. 'Magnetic shifting composition can output different power (power = drive out torque X speed). Since the magnetic shifting group includes the functions of the electric motor and the transmission, the overall volume and weight are low, and the high dynamic power density can be achieved. The drive power here can be, but is not limited to, output power divided by volume, or output power divided by, heavy star (ie (output torque χ speed) / volume, or (round torque x speed) / weight). _ From 'If the magnetic shifting group is used for the electric mechanical towel, the rotary power can be received by the rotor 2〇, and the electric power generated by the magnetic field cutting can be outputted by the stator 30 (detailed later). After the voltage regulator circuit is output. Since the magnetic speed change composition can be controlled by the gear ratio, when the input rotary power has a large variation or the better H feed efficiency is obtained, it can be achieved by controlling the speed ratio of the magnetic shift. Continuing to refer to "Fig. 1" and "Fig. 2", the stator 30 may be a fixed magnet or an induction magnet (or an electromagnet). In the present embodiment, an induction magnet is exemplified. The inner ring of the fixed t 7 201131947 30 is provided with a plurality of bumps 32a, 32b. Each of the bumps 32a, 32b is wound with an induction coil (described in detail later), and when the induction coil is energized, a magnetic pole can be formed. Taking the embodiment of the drawing as an example, the stator 30 has 48 bumps 32a, 32b, and each of the bumps 32a, 32b is energized to form a pair of magnetic poles. In this example, there are four phases (4 phases), and the parent phase has 12 pole pairs (20 Pole Pairs). Please also refer to "3", which is a stator 3 according to an embodiment of the present proposal. Schematic diagram of the magnetic logarithm. It can be seen in the figure that the adjacent magnetic poles have opposite polarities (magnetic north pole N and magnetic south pole s). Two adjacent magnetic poles of opposite polarity are a magnetic pair (for example, S1 of the figure, N1 is a magnetic pair. It can be seen from the figure that there are 12 pole pairs in total, and the pole logarithm is only one implementation. This proposal does not The number of magnetic pairs is limited to ST1 poles. The rotor 20 may be a fixed magnet or an induction magnet. In the present embodiment, the rotor 2 is described by taking a fixed magnet as an example. The rotor 20 has a plurality of magnetic poles and has r In this embodiment, the rotor 20 is exemplified by having 20 pole pairs. The stator and the rotor 20 are coaxially arranged (coaxially sleeved), and in this embodiment, the rotor 2 is disposed on the stator 30. The radial inner side is not limited thereto. The stator 3〇 may be disposed on the radially inner side of the rotor 20, and the object of the present invention can still be achieved. Secondly, the direction of the magnetic pole (magnetic field line) of the rotor 20 is directed toward the stator. The direction of the magnetic pole (magnetic line) of the 3 。. The magnetic conductive element 40 may be laminated steel, and the material thereof may be a Soft Magnetic Composite (SMC) to reduce eddy current (Eddy)

Current)及鐵損。 請再參閱「第1圖」及「第2圖」,導磁元件40包含第一環 42及第二環44。第一環42係位於第二環44之徑向外侧,且第一 201131947 裱與第二環44配置於定子3〇與轉子2〇之間。第一環& 二環44係可相互接觸或相距一間隙(圖係採相距一間隙方 施)。第-環42具有多辦磁子塊42(),422。第二環44亦且= .個導磁子塊物,442。當第-環&位於第二環44之麵外側^ 導=子塊俱422,44〇,442即可形成多個導磁體(容後詳述)。當第 1 42或/與第二環44被致動時,兩者可相對運動(相對轉動)於 第-位置及第二位置之間,此時,導磁體之數量亦會隨之變化, • 如下說明。 ’ 請參考「第4A圖」。「第4A圖」係為依據本提案-實施例之 導磁7L件第-實施例之剖面示意圖。此剖面示意圖係為「第2圖」 中之第-% 42套於第二環44徑向外側後,依垂直於轴向的平面 為切面所為之剖面示意圖。為了便於說明第一環42與第二環料 的相對轉動之動作,兹再將「第4A圖」中標示為429及449的弧 段於「第4B圖」進行放大。弧段429, 449所夾之弧角為45度, ^故整個第一環42與第二環44則共有8個弧段429, 449。「第4B 圖」係為第一環42與第二環44位於第一位置之狀態的局部放大 剖面不意圖。「第4C圖」則為第一環42與第二環44位於第二位 ' 置之狀態的局部放大剖面示意圖。 從「第4B圖」中可以見悉,第一環42的導磁子塊420與第 一環44的導磁子塊440係呈相連狀態(或重疊)並形成導磁體46以 同樣地’第—環42的導磁子塊422與第二環44的導磁子塊442 係呈相連狀態並形成導磁體46b。而在導磁體46a,46b之間即具有 201131947 三個磁隙48a, 48b,48c。由於整個第一環42與第二環44具有相同 的8個弧段429, 449 ’故整個第一環42與第二環44則會有24個 磁隙48a, 48b, 48c(3x8=24,亦即具有24個導磁體46a,46b)。 續請參閱「第4C圖」,此為第一環42與第二環44位於第二 位置之狀態的局部放大剖面示意圖。第一環42的導磁子塊420與 第二環44的導磁子塊440係呈相連狀態並形成導磁體46a。同樣 地,第一環42的導磁子塊422與第二環44的導磁子塊442係呈 相連狀態並形成導磁體46b。從圖中可以看出,弧段429, 449内有 四個磁隙48a,48b,48c,48d,亦具有四個導磁體46a,46b。是以, 整個第一環42與第二環44則會有32個(4x8=32)磁隙48a, 48b,48c, 48d。 前述導磁子塊420, 440呈相連狀態係指距離相近,而非僅指 相接觸之狀態,距離相近亦可為導磁子塊42〇, 44〇兩者不相接觸 但在徑向上重疊,或者導磁子塊420, 440不相接觸且徑向上或圓 周方向上有-間距。中言之,若導磁子塊,44〇未相接觸,則 導磁子塊420, 440之間係有二個距離,其一為徑向距離,其二為 •;口圓周方向的距離。就刚者之控向距離而言,經實驗,若該和白 距離在5毫米(mm)以内,均能達到形成單一導磁體4知之效果。 當然此距離亦與定子30磁力線的強度有關,若磁力線強度愈強, 此距離可以愈大。也就是說,此徑向距離可視磁性變速組成本身 的大小及磁力線強度做改變。 就前述後者之圓周方向的距離(弧長)亦可表述為導磁子塊4加 201131947 440邊界對應到圓心(定子圓心)的夾角,例如以「第4B圖」為例, 導磁子塊420的左侧邊與導磁子塊440的右側邊的夾角。為能進 一步定義此夾角或弧長,茲將導磁子塊420的左側邊與導磁子塊 440的右側邊的距離所形成的空間定義為氣縫。由於磁性變速組成 在運作時,每個磁隙48a,48b,48c(「第4B圖」)係會產生一個磁 極(以下稱磁隙磁極),當導磁子塊42〇,44〇間具有氣縫時,此氣縫 亦會具有磁極(以下稱氣縫磁極),為能讓導磁子塊42〇, 44〇形成前 導磁體46a之效果,此氣縫磁極之磁場強度較佳者為小於氣隙磁 極的磁場強度的百分之二十(2〇〇/〇)。再經由此氣縫磁極之磁場強度 所回推而得之該弧長或該失角則為較佳之圓周方向的間距。 導磁子塊42〇,似,44〇, 442之材料係可選用任何可導磁的材 料’例如鐵基之材料或軟鐵。前述第一環α與第二環Μ之相對 運動之驅動方式射採關械核電磁式方式驅動1驅動時, 係可單獨驅動第-環42或第二環44,或者是第—環Μ與第 44同時驅動,只要能使得第一 衣與第一% 44之相對位置能位 移於第一位置與第二位置之間即可。 犯圖」之位置則^:「=ΓΓ—位置(如「第 严49淑曾-》 弟C圖」之位置)之間,當第一 % 42與苐二核44位於第一位置 稱洲個胸趙恤肩,當第—環42與疋4〇具=個(以下 置時’導磁_具有32個(―個)-導:=位 ί Γ- -Ϊ 201131947 導磁元件40藉由第一環42與第二環44可相對運動之設計, 導磁兀件40可選擇性地使PN1個或PN2個導磁體46a,46b對應 於轉子20與定子3〇之間。藉由pN1個或pN2個導磁體4如,4沾 配合轉子2G的鄉蚊子3Q的磁場,即可產生-個增減速(變速) 的效果。此增減逮比可由下述計算公式(1)而得: \mp + kn\ .............................................................................. 其中,G為變速比(即增減速比),m,k為簡諧波(harmonics)級 數’ p為轉子20的極對數(p〇le pairs)、n為導磁體4如,4肋的數目 (number of steel Pieces)。於主簡諧波(filndamemal Μ·—)狀態 下’ m=-k=l ’而本實施例中,轉子2〇的極對數為2〇,以第一環 42與第二環44位於第-位置為例,導磁體4如,柳的數量為%, 套入上列公式,可得ch1x2())/(1x24_1x2())=5,蚊子的轉速比上 轉子的轉速為5α。若以第一環幻與第二環44位於第二位置為 例,導磁體46a,46b的數量為32,套入上列公式,可得G=(ix2〇)/(i x32-lx20)=1.6 ’即定子3〇的轉速比上轉子2〇的轉速為i ^。 由此可知’藉由導磁元件40、定子3〇與轉子2〇之適當配置 與設計’即可使得磁性變速組成具有變速之效果。 其次’為了驗-步提升變速_财性’經實驗可得定子 30的極對數ST卜轉子20的極對數R、及導磁元件4〇的導磁體 46a,46b的數量,麗維持在下述關係,將可得到穩定之變速 比與驅動力: 12 201131947 .…式(2) PNl-3 ^ R+ST1 ^ PN1+3 PN2-3 ^ R+ST1 ^ PN2+3 — ................................................ 以本實施例為例,導磁元件40位於第二位置時,恰滿足式(3) PN2_3 $ R+ST1 $ PN2+3。而導磁元件4〇位於第—位置時, 則雖未能滿足式(2)ΡΝ1-3 $ R+ST1 $ PN1+3,但仍屬能變速之 要求。而在本實施例中,若欲同時滿足式(2)與式⑶,則可以利用 修改導磁元件40的導磁子塊420, 422, 440, 442之設計,使得能滿Current) and iron loss. Referring again to "Fig. 1" and "Fig. 2", the magnetically permeable element 40 includes a first ring 42 and a second ring 44. The first ring 42 is located radially outward of the second ring 44, and the first 201131947 裱 and the second ring 44 are disposed between the stator 3〇 and the rotor 2〇. The first ring & second ring 44 series can be in contact with each other or at a distance (the system is separated by a gap). The first ring 42 has a plurality of magnetic sub-blocks 42(), 422. The second ring 44 also has a magnetically permeable sub-block, 442. When the first ring & is located on the outer side of the second ring 44, the sub-blocks 422, 44, 442 can form a plurality of magnetizers (described in detail later). When the first 42 or/and the second ring 44 are actuated, the two can be relatively moved (relatively rotated) between the first position and the second position, and the number of the magnetizers also changes accordingly. As explained below. Please refer to "Figure 4A". Fig. 4A is a schematic cross-sectional view showing the first embodiment of the magnetic flux 7L according to the present invention. The cross-sectional view is a cross-sectional view in which the -% 42 of the "Fig. 2" is placed on the radially outer side of the second ring 44, and the plane perpendicular to the axial direction is the cut surface. In order to facilitate the explanation of the relative rotation of the first ring 42 and the second ring material, the arcs labeled as 429 and 449 in "Fig. 4A" are further enlarged in "Fig. 4B". The arc angles of the arc segments 429, 449 are 45 degrees, so that the entire first ring 42 and the second ring 44 have a total of 8 arc segments 429, 449. The "Fig. 4B" is a partially enlarged cross-sectional view showing a state in which the first ring 42 and the second ring 44 are at the first position. Fig. 4C is a partially enlarged cross-sectional view showing the state in which the first ring 42 and the second ring 44 are in the second position. As can be seen from "Fig. 4B", the magnetically permeable sub-block 420 of the first ring 42 and the magnetically permeable sub-block 440 of the first ring 44 are connected (or overlapped) and the magnetizer 46 is formed to be similarly The magnetically permeable sub-block 422 of the ring 42 is connected to the magnetically permeable sub-block 442 of the second ring 44 and forms a magnetizer 46b. There are three magnetic gaps 48a, 48b, 48c of 201131947 between the magnets 46a, 46b. Since the entire first ring 42 and the second ring 44 have the same eight arc segments 429, 449', the entire first ring 42 and the second ring 44 will have 24 magnetic gaps 48a, 48b, 48c (3x8=24, That is, there are 24 magnetizers 46a, 46b). Continued, refer to Fig. 4C, which is a partially enlarged cross-sectional view showing the state in which the first ring 42 and the second ring 44 are at the second position. The magnetically permeable sub-block 420 of the first ring 42 and the magnetically permeable sub-block 440 of the second ring 44 are connected to each other and form a magnetizer 46a. Similarly, the magnetic permeable sub-block 422 of the first ring 42 is connected to the magnetic permeable sub-block 442 of the second ring 44 and forms a magnetizer 46b. As can be seen, the arc segments 429, 449 have four magnetic gaps 48a, 48b, 48c, 48d and also have four magnets 46a, 46b. Therefore, there will be 32 (4x8=32) magnetic gaps 48a, 48b, 48c, 48d throughout the first ring 42 and the second ring 44. The foregoing magnetically conductive sub-blocks 420, 440 are in a connected state, and the distances are similar, and not only the state of contact, but the magnetic proximity of the magnetically conductive sub-blocks 42〇, 44〇 may not be in contact but overlap in the radial direction. Alternatively, the magnetically permeable sub-blocks 420, 440 are not in contact and have a pitch in the radial or circumferential direction. In the meantime, if the magnetic sub-blocks are not in contact with each other, the magnetic sub-blocks 420, 440 are separated by two distances, one of which is a radial distance, and the other is a distance in the circumferential direction of the mouth. As far as the distance of the control is concerned, it is experimentally found that if the distance between the white and the white is within 5 mm (mm), the effect of forming a single magnetizer 4 can be achieved. Of course, this distance is also related to the strength of the magnetic field lines of the stator 30. If the strength of the magnetic lines is stronger, the distance can be larger. That is to say, this radial distance changes depending on the size of the magnetic shifting composition itself and the strength of the magnetic field lines. The distance (arc length) in the circumferential direction of the latter can also be expressed as the angle between the boundary of the magneto-optical block 4 and the 201131947 440 boundary corresponding to the center of the circle (the center of the stator). For example, taking the example of FIG. 4B, the magnetic sub-block 420 The angle between the left side of the magnetic conductive sub-block 440 and the right side of the magnetically conductive sub-block 440. In order to further define this angle or arc length, the space formed by the distance between the left side of the magnetic sub-block 420 and the right side of the magnetic sub-block 440 is defined as an air gap. Since the magnetic shifting composition is in operation, each magnetic gap 48a, 48b, 48c ("4B") generates a magnetic pole (hereinafter referred to as a magnetic gap magnetic pole), and has a gas between the magnetic conductive sub-blocks 42, 44 When the seam is sewn, the gas seam also has a magnetic pole (hereinafter referred to as an air gap magnetic pole), and the magnetic field strength of the air gap magnetic pole is preferably smaller than that of the gas to form the front magnet 46a. Twenty percent (2 〇〇 / 〇) of the magnetic field strength of the gap magnetic pole. The arc length or the corner angle obtained by retracting the magnetic field strength of the air gap magnetic pole is a preferred circumferential direction pitch. The material of the magneto-optical block 42 〇, like 44 〇, 442 can be selected from any magnetically permeable material such as an iron-based material or soft iron. When the relative motion of the first ring α and the second ring is driven by the ejector and the electromagnetic mode drive 1 is driven, the first ring 42 or the second ring 44 may be separately driven, or the first ring and the first ring The 44th simultaneous driving is as long as the relative position of the first garment and the first portion 44 can be displaced between the first position and the second position. The position of the "figure map" is: "=ΓΓ- position (such as "Zhen Yan 49 Shu Zeng -" position of the younger brother C"), when the first % 42 and the second core 44 are in the first position called the continent Chest-shirt shoulder, when the first - ring 42 and 疋 4 cookware = one (the following set 'magnetic _ has 32 (-) - lead: = bit Γ Ϊ - -Ϊ 201131947 magnetic component 40 by the first The design of the relative movement of the ring 42 and the second ring 44 allows the magnetically permeable member 40 to selectively connect the PN1 or PN2 magnetizers 46a, 46b between the rotor 20 and the stator 3〇. By pN1 or For example, if the pN2 magnetizers 4 are mixed with the magnetic field of the mosquito 3Q of the rotor 2G, an increase/deceleration (shift) effect can be produced. The increase/decrease ratio can be obtained by the following formula (1): \mp + kn\ ............................................... ............................... Where G is the gear ratio (ie, the ratio of increase/deceleration), m, k is the harmonic The harmonics series 'p is the pole pair of the rotor 20, n is the number of the magnets 4, such as the number of steel Pieces. The main harmonic (filndamemal Μ·-) In the state of 'm=-k=l' and in the present embodiment, the rotor 2〇 The pole pair is 2 〇. Taking the first ring 42 and the second ring 44 at the first position as an example, the number of the magnets 4, for example, the number of the willows, is nested in the above formula, and ch1x2())/(1x24_1x2( )) = 5, the rotation speed of the mosquito is 5α than the rotation speed of the upper rotor. For example, if the first ring and the second ring 44 are located at the second position, the number of the magnets 46a, 46b is 32, and the formula of the above formula is obtained, and G=(ix2〇)/(i x32-lx20)= 1.6 'that is, the rotation speed of the stator 3 turns is i ^ than the rotation speed of the upper rotor 2 turns. From this, it can be seen that the magnetic shifting composition has the effect of shifting by the proper arrangement and design of the magnetic conducting element 40, the stator 3〇 and the rotor 2〇. Secondly, in order to improve the shift speed of the stator 30, the number of pole pairs R of the stator 30, the number of pole pairs R of the rotor 20, and the number of the magnetizers 46a and 46b of the magnetic conducting element 4〇 are maintained in the following relationship. The stable gear ratio and driving force will be obtained: 12 201131947 .... (2) PNl-3 ^ R+ST1 ^ PN1+3 PN2-3 ^ R+ST1 ^ PN2+3 — ....... ................................... Using this embodiment as an example, magnetic conduction When element 40 is in the second position, it satisfies equation (3) PN2_3 $ R+ST1 $ PN2+3. When the magnetic conductive element 4 is located at the first position, although the formula (2) ΡΝ 1-3 $ R+ST1 $ PN1+3 is not satisfied, it is still a variable speed requirement. In the present embodiment, if both equations (2) and (3) are to be satisfied at the same time, the design of the magnetic permeable sub-blocks 420, 422, 440, 442 of the magnetically permeable element 40 can be modified to make it full.

足式(2)即可,例如,若ST1為12,而pN1與pN2各別為%及 29即同時滿足上式(2)與(3)。 在本實施例中,若不變更導磁元件4〇之設計,欲同時滿足式 (2)與式(3)(但式(3)須做些微變動,容後詳述),則可使用「第5a 圖」及「第5B圖」之定子30的實施例。「第5A圖」為依據本 提案磁性變速組成之定子30的另一實施例的繞線示意圖。「第5b 圖」為「第5A圖」的定子30的另一實施例的動作示意圖。 從圖中可以見悉’定子3 〇的另一實施例包含多個感應線圈3 4 34b,34c,34d及極數調變電路36。感應線圈34a, 3牝,34c,34d係各 別繞於凸塊32a,32b。在「第5A圖」及「第5B圖」中係僅繪製 三個磁極對(Nl,N2, N3, Sl,S2, S3)的感應線圈 34a, 34b, 34c, 34d ’但並不表示定子3〇僅包含感應線圈Ma, 3牝,3如,3牝。極數 調變電路36包含二個切換開關36〇, 362。當切換開關36〇, 362位 於「第5A圖」之狀態並通入電源時,各感應線圈34a,34b, 3如,34d 所形成的磁極即如「第3圖」所示之極性’意即定子3〇共具有12The foot type (2) may be, for example, if ST1 is 12, and pN1 and pN2 are % and 29, respectively, that the above formulas (2) and (3) are satisfied at the same time. In this embodiment, if the design of the magnetic conductive element 4〇 is not changed, and the formula (2) and the formula (3) are to be satisfied at the same time (however, the formula (3) needs to be slightly changed, and the details are described later), then " Embodiments of the stator 30 of Figures 5a and 5B. Fig. 5A is a winding diagram of another embodiment of the stator 30 of the magnetic shifting composition according to the present proposal. Fig. 5b is a schematic view showing the operation of another embodiment of the stator 30 of Fig. 5A. It can be seen from the figure that another embodiment of the stator 3 includes a plurality of induction coils 3 4 34b, 34c, 34d and a pole number modulation circuit 36. The induction coils 34a, 3B, 34c, 34d are wound around the bumps 32a, 32b, respectively. In "5A" and "5B", only the induction coils 34a, 34b, 34c, 34d of three magnetic pole pairs (Nl, N2, N3, Sl, S2, S3) are drawn but the stator 3 is not shown. 〇 only contains induction coils Ma, 3牝, 3, such as 3牝. The pole number modulation circuit 36 includes two switching switches 36A, 362. When the changeover switch 36A, 362 is in the state of "Fig. 5A" and the power is supplied, the magnetic pole formed by each of the induction coils 34a, 34b, 3, for example, 34d is the polarity as shown in "Fig. 3". The stator has a total of 12

f <Γ 7 t ^ J 13 201131947 個極對數。當切換開關360, 362位於「第5B圖」之狀態並通入電 源時’原形成N1,S3之感應線圈34c,34d因反向通入電源,故所 形成的磁極即會相反(即N1變為磁南極,S3變為磁北極),請參閱 「第6圖」’其為「第5A圖」及「第5B圖」極對數切換之示意 圖。 圖中可以見悉,虛線框中所表示的即為切換開關36〇, 362位 於「第5B圖」時,所形成的磁極極性的示意圖。圖中Ni,N4,N7 N10在「第5A圖」中係為磁北極,S3, S6, S9, S12在「第5A圖」 中係為磁南極,此時定子30共具有12個(以下稱ST1個)極對數(即 Nl,Sl,N2, S3...N12, S12) ’但疋在「第5B圖」中,因為切換開關 360, 362及電路之巧妙設置’使得Nl,N4, N7, N10通電後變為磁 南極,而S3, S6, S9, S12則變為磁北極,其餘維持不變,是以定子 30共具有4個(以下稱ST2個)極對數(如虛線框ΝΓ,S1,,N2,,S2,, N3’,S3’,N4’,S4’所示)。換句話說,當感應線圈34a,34b, 34c,34d 被切換至ST1個極對數時,相鄰之感應線圈34a,34b,34c,34d之 極性(磁極性)係相反’當感應線圈34a,34b,34c,34d被切換至ST2 個極對數時,感應線圈34a,34b,34c,34d係被群組為多個線圈組 35a,35b,且相鄰之線圈組35a,35b之極性係相反。在此實施例中, 每一線圈組35a, 35b係包含三個依序相鄰的感應線圈34a,34b, 34c, 34d。此處的依序相鄰係為相連接的,例如「第5B圖」中的S1,N1, S2即屬依序相鄰的感應線圈34a,34b,34c,34d。 綜上說明,定子30藉由極數調變電路36而能選擇性地切換 201131947 感應線圈Ma,Mb,Mc,3如於個(ST1個)極對數及*個阶2個) 極。將「第5A圖」之定子3〇實施例與導磁元件仙導磁 體數量之_整合後’即可得到如下表之魏比(定子轉數:轉子 轉速),並滿足上述式(2)與下式(4)。 PN2-3 ^ R+ST2 ^ PN2+3, 導磁元件位於第—位置, —--- 導磁元件位於第二位置, 極數調變電路為第5B圖 極數調變電路為第5A圖 狀態 狀態 變數比(5:1) 變數比(1.6:1) 定子 4 12 導磁元件 24 32 轉子 20 20 極數調變電路36雖僅以「第5A圖」為實施例之一,但並不f <Γ 7 t ^ J 13 201131947 The number of pole pairs. When the changeover switches 360, 362 are in the state of "Fig. 5B" and the power is supplied, the induction coils 34c, 34d which originally formed N1 and S3 are turned into the power supply in reverse, so that the magnetic poles formed are opposite (i.e., N1 is changed). For magnetic south pole, S3 becomes magnetic north pole), please refer to "Figure 6", which is a schematic diagram of the pole-to-number switching of "5A" and "5B". As can be seen from the figure, the dotted line indicates the polarity of the magnetic pole formed when the switch 36 〇 and 362 are located in the "5B". In the figure, Ni, N4, and N7 N10 are magnetic north poles in "5A", and S3, S6, S9, and S12 are magnetic south poles in "5A". At this time, the stator 30 has a total of 12 (hereinafter referred to as ST1) pole logarithm (ie Nl, Sl, N2, S3...N12, S12) 'But in "5B", because the switch 360, 362 and the clever setting of the circuit 'make Nl, N4, N7 When N10 is energized, it becomes a magnetic south pole, and S3, S6, S9, and S12 become magnetic north poles, and the rest remains unchanged. Therefore, the stator 30 has a total of four (hereinafter referred to as ST2) pole pairs (such as a dotted line frame, S1,, N2,, S2,, N3', S3', N4', S4'). In other words, when the induction coils 34a, 34b, 34c, 34d are switched to the ST1 pole pairs, the polarities (magnetic polarities) of the adjacent induction coils 34a, 34b, 34c, 34d are opposite 'When the induction coils 34a, 34b When 34c, 34d are switched to ST2 pole pairs, the induction coils 34a, 34b, 34c, 34d are grouped into a plurality of coil groups 35a, 35b, and the polarities of adjacent coil groups 35a, 35b are opposite. In this embodiment, each coil set 35a, 35b includes three sequentially adjacent induction coils 34a, 34b, 34c, 34d. Here, the adjacent adjacent systems are connected, for example, S1, N1, and S2 in "Fig. 5B" are sequentially adjacent induction coils 34a, 34b, 34c, 34d. In summary, the stator 30 can selectively switch the 201131947 induction coils Ma, Mb, Mc, 3 by one (ST1) pole pairs and * steps 2 poles by the pole number modulation circuit 36. By integrating the stator 3〇 embodiment of "5A" with the number of magnetisms of the magnetic conducting element, the Wei ratio (stator revolution: rotor speed) of the following table can be obtained, and the above formula (2) is satisfied. The following formula (4). PN2-3 ^ R+ST2 ^ PN2+3, the magnetic component is at the first position, --- the magnetic transducer is in the second position, and the pole number modulation circuit is the fifth harmonic modulation circuit. 5A state state variable ratio (5:1) variable ratio (1.6:1) stator 4 12 magnetic transducer 24 32 rotor 20 20 pole number modulation circuit 36 is only one of the embodiments with "5A" But not

以此為限。㈣適當電路及開關設計,可贿定子3()的極對數有 不同比例的增減。紐之外’定子3G的繞線方式亦可以用更為複 雜且多樣的設計,例如_—個躲表(winding ehart)的方式,以 得到更多樣的極對數需求,此繞線方式可以是但不限於LRK (Lucas,Retzbach and Kiihfcs)繞線方式、或 D_LRK 沖__ LRK) 繞線方式、或ABC繞線方式,關於此應用,容後詳述。 關於前述「第4A圖」導磁元件4〇之其他實施方式,係可見 於「第7A圖」、「第7B®」、及「第7C圖」。「第7A圖」及「第 7B圖」、及「第7C圖」之導磁元件5〇(第二實施例)係為類似 t 15 201131947 4B圖」之不意方式。圖中可以見悉,導磁元件%包含第一環%、 第二環54、第三環56及第四環58。第一環% '第二環%、第三 環56及第四環則系徑向疊置並各別具有導磁子塊分,57, 59(亦可分別稱第一、第二、第三、第四導磁子塊)。當導磁元件 5〇位於第7八圖」之位置時(第一位置),導磁子塊 間有相連接關係,使得在此弧段中即具有二個導磁體取训及 -個磁隙(磁隙即為導磁體在圓周方向上所分隔出來的空隙)。當導 磁元件50位於「第7B圖」之位置時(第二位置),導磁子塊53, 55, 57, %間則相互分離,使得在此弧段令即具有四個導磁體化,池 51c,51d及四個磁隙。此外,當導磁元件5〇位於如「第7c圖」 所示位置時(亦可稱為第三位置),其導磁子塊53, 55, 57, 59呈在徑 向完全重疊之狀態,此時,導磁元件5〇即具有二個導磁體51&,5ib 及二個磁隙’所導磁元件5〇在「第7A圖」及「第7C圖」的位 置時,雖然所得到的導磁體51a, 51b的數量相同,但其磁通量不 同因此,所能傳遞的扭力亦隨之變化,因此,導磁元件5〇可以 經由適當之設計及控制,即可改變其變速比,亦可改變其所傳遞 的扭力。 從上述「第4A圖」與「第7A圖」之導磁元件40, 50係同樣 採用多個環狀(圓筒狀)的導磁環(即前述第一環42, 52等)徑向疊 置’導磁環之數量係可依實際設計之需求而變動,意即可以有三 個或五個導磁環之結合設計,但並不限於此數量。導磁環中的導 磁子塊的尺寸、排列及數量亦可經由適當地設計而能產生不同數 201131947 里的磁隙,藉以得到所需的變數比。 續參間「篦8isi ^ — 圖」,其為依據本提案磁性變速組成之導磁元 I㈣三!施例示意圖。此導磁元件6〇包含第一環62與第二環 _ 第5衣62與第二環64係軸向連接。導磁元件6(H系配置於前 述定子30與轉子2〇之間。第一環&與第二環糾係可在定子如 與轉子2〇間軸向移動,使得在同-時間内,僅會有第-環62及 第二環64其中之一被夾置於定子30與轉子20内。易言之,當導 #磁元件60被軸向致動時’導磁元件6〇係選擇性地使第-環62或 第-% 64移至轉子20與定子30之間。前述被失置的第一環 或第一% 64方能與定子3〇與轉子2〇的磁場產生作用,而具有特 疋I:速比。如述第一環62導磁子塊63的數量(例如pNi個導磁子 塊·)係相異於第二環64導磁子塊65的數量(例如pN2個導磁子 塊)。在「第8圖」實施例中,第一環62導磁子塊63的數量為32, 而第二裱64導磁子塊65的數量為24,即為適於置換「第1圖」 •實施例中的導磁元件40。在本實施例中的每一導磁子塊63, 65即 個別形成並等效於「第4B圖」與「第4C圖」中的導磁體46a,46b。 如上所述,第一環62及第二環64係同軸連接,請再參閱「第 8圖」,第一環62及第二環64係藉由一電絕緣元件66a而同轴連 接。同時在第一環62與第二環64的二個外側端亦各別具有電絕 緣元件66b,66c。電絕緣元件66a, 66b, 66c係用以固定第二環64 的導磁子塊65及第一環62的導磁子塊63。 再者,請續參閱「第9圖」,其係為依據本提案磁性變速組成 17 201131947 第二實施的立體分解示意圖。從圖中如得知,雜組成 係包含轉子20、定子30及導磁元件7〇。轉子2〇具有多個磁極, 轉子20的磁極具有R個極對數。定子3〇與轉子2〇同轴套設,定 子30並具有多個磁極,定子30的磁極具有ST1健對數。導磁 元件70被配置於轉子20與定子30之間並具有簡個導磁子塊 72(亦可稱導磁體)’PN1個導磁子塊72對應配置於轉子2〇與定子 3〇之間’其中,_-3 g R+ST以PN1+3。因此,當R為2〇、 PN1為32而ST1為12時,此磁性變速組成之加減速比即為丨6:1(依 據上述式(1))。 其次’從「第9圖」可以見悉,導磁子塊72的兩端係由電絕 緣元件74a,74b而固定’因此,導磁子塊72因切割定子3〇與轉 子20磁場而感應的電流將會被限制於每個導磁子塊72内而不致 泡漏。 依據「第9圖」之實施例,每一導磁元件70、定子30及轉子 20均為中空環形之設計,使得整個磁性變速組成之體積及重量都 相當小,並能夠易於與電動馬達做内部整合,得到較高的驅動功 率密度(瓦/公斤,W/Kg或瓦/體積,W/m3)。依據前述實施例,經由 導磁元件40, 50, 60之不同實施態樣,即可使得磁性變速組成能切 換於不同的變速比之間。接者,若在導磁元件40, 50, 60所能切換 的導磁體46a,46b, 51a,51b,51c,51d的數量未能符合式(2)及式(3) 時,則亦可採用「第5A圖」之定子30的實施態樣(符合式(2)與式-(4»,而能提高不同變速比狀態下的穩定性。 18 201131947 再者’關於前述式(2)、式(3)、及式(4),其係以定子30的主 簡諳波為基礎所列之關係式’而若將該些關係式中的定子3〇的極 對數以鬲階導磁性簡譜波permeance harm〇nics)進行 設計’則可得下述關係式: 式⑶ 式⑹ 式⑺ PN1-3 ^ R+STr ^ PN1+3 PN2-3 ^ R+ST1J ^ PN2+3 PN2-3 $ R+ST2’ $ PN2+3This is limited to this. (4) Appropriate circuit and switch design, the pole number of bribe stator 3 () can be increased or decreased in different proportions. Outside the New York, the winding mode of the stator 3G can also be used in a more complicated and diverse design, such as _-winding ehart, to obtain more extreme pole-log requirements. This winding method can be However, it is not limited to the LRK (Lucas, Retzbach and Kiihfcs) winding method, or the D_LRK rushing __ LRK) winding method, or the ABC winding method. Other embodiments of the above-mentioned "Ath 4A" magnetic conductive element 4 can be found in "Ath 7A", "7B®", and "No. 7C". The magnetic conductive elements 5A (second embodiment) of "Fig. 7A" and "Fig. 7B" and "Fig. 7C" are similar to the manner of t 15 201131947 4B. As can be seen in the figure, the magnetic flux component % includes a first ring %, a second ring 54, a third ring 56 and a fourth ring 58. The first ring % 'second ring %, third ring 56 and fourth ring are radially stacked and each has a magnetic sub-block, 57, 59 (also referred to as first, second, third respectively) , the fourth magnetically conductive sub-block). When the magnetic conductive element 5 is located at the position of the seventh figure (the first position), there is a connection relationship between the magnetic conductive sub-blocks, so that there are two magnetizing bodies and a magnetic gap in the arc segment. (The magnetic gap is the gap separated by the magnetizer in the circumferential direction). When the magnetic conductive element 50 is located at the position of "Fig. 7B" (second position), the magnetic conductive sub-blocks 53, 55, 57, % are separated from each other, so that there are four magnetizations in this arc segment. Pools 51c, 51d and four magnetic gaps. Further, when the magnetic conductive element 5 is located at a position as shown in "Fig. 7c" (also referred to as a third position), the magnetic conductive sub-blocks 53, 55, 57, 59 are completely overlapped in the radial direction. At this time, the magnetic conductive element 5 具有 has two magnets 51 & 5ib and two magnetic gaps 'the magnetic conducting elements 5 〇 in the positions of "Ath 7A" and "7C", although obtained The number of the magnets 51a, 51b is the same, but the magnetic flux is different, so the torque that can be transmitted changes accordingly. Therefore, the magnetic conductive element 5 can be changed by the appropriate design and control, and the speed ratio can be changed. The torque it transmits. Similarly, a plurality of annular (cylindrical) magnetically conductive rings (i.e., the first rings 42, 52, etc.) are radially stacked from the magnetic conductive elements 40 and 50 of the above-mentioned "Ath 4A" and "7A". The number of 'magnetic rings' can be changed according to the actual design requirements, that is, there can be a combination of three or five magnetic rings, but it is not limited to this number. The size, arrangement and number of the magnetic sub-blocks in the magnetically permeable ring can also be appropriately designed to produce different magnetic gaps in 201131947, thereby obtaining the desired ratio of variables. Continuation of the reference section "篦8isi ^ — Figure", which is a schematic diagram of the magnetic flux I (four) three! The magnetically conductive element 6A includes a first ring 62 and a second ring _ 5th garment 62 and a second ring 64 are axially connected. The magnetic conductive element 6 (H is disposed between the stator 30 and the rotor 2〇. The first ring & and the second ring can be axially moved between the stator and the rotor 2, so that in the same time, Only one of the first ring 62 and the second ring 64 is sandwiched between the stator 30 and the rotor 20. In other words, when the magnetic element 60 is axially actuated, the magnetically conductive element 6 is selected. The first ring 62 or the -% 64 is moved between the rotor 20 and the stator 30. The aforementioned first ring or the first 64-bit energy can interact with the magnetic field of the stator 3〇 and the rotor 2〇, And having the characteristic I: speed ratio. The number of the first magnetic block 63 of the first ring 62 (for example, pNi magnetic sub-blocks) is different from the number of the magnetic blocks 65 of the second ring 64 (for example, pN2) a magnetically permeable sub-block. In the "Fig. 8" embodiment, the number of the first ring 62 of the conductive sub-blocks 63 is 32, and the number of the second 裱 64 magnetically-conductive sub-blocks 65 is 24, which is suitable Replacement "Fig. 1" • The magnetic conductive element 40 in the embodiment. Each of the magnetic conductive sub-blocks 63, 65 in the present embodiment is formed separately and is equivalent to "4B" and "4C". Guide magnets 46a, 46b. As mentioned above, The ring 62 and the second ring 64 are coaxially connected. Please refer to FIG. 8 again. The first ring 62 and the second ring 64 are coaxially connected by an electrically insulating element 66a. At the same time, the first ring 62 and the first ring 62 The two outer ends of the second ring 64 also have electrically insulating elements 66b, 66c, respectively. The electrically insulating elements 66a, 66b, 66c are used to fix the magnetically permeable sub-block 65 of the second ring 64 and the magnetic permeable body of the first ring 62. Block 63. Further, please refer to "Fig. 9", which is a perspective exploded view of the second embodiment of the magnetic shifting composition 17 201131947 according to the present proposal. As can be seen from the figure, the heterogeneous system includes the rotor 20 and the stator 30. And the magnetic conductive element 7〇. The rotor 2〇 has a plurality of magnetic poles, and the magnetic pole of the rotor 20 has R pole pairs. The stator 3〇 is coaxially sleeved with the rotor 2〇, and the stator 30 has a plurality of magnetic poles, and the magnetic poles of the stator 30 have ST1 is a logarithmic number. The magnetically permeable element 70 is disposed between the rotor 20 and the stator 30 and has a simple magnetically permeable sub-block 72 (also referred to as a magnetizer). PN1 magneto-conducting sub-blocks 72 are correspondingly disposed on the rotor 2 and the stator. Between 3〇', _-3 g R+ST is PN1+3. Therefore, when R is 2〇, PN1 is 32 and ST1 is 12, this magnetic The acceleration/deceleration ratio of the speed component is 丨6:1 (according to the above formula (1)). Next, it can be seen from Fig. 9 that both ends of the magnetic permeable sub-block 72 are electrically insulated elements 74a, 74b. Fixedly, therefore, the current induced by the magnetically permeable sub-block 72 due to the magnetic field of the stator 3 and the rotor 20 will be limited to each of the magnetically permeable sub-blocks 72 without causing bubble leakage. According to the embodiment of Fig. 9, Each of the magnetic conductive element 70, the stator 30 and the rotor 20 has a hollow annular design, so that the entire magnetic shifting composition has a relatively small volume and weight, and can be easily integrated with the electric motor to obtain a higher driving power density ( W/kg, W/Kg or watt/volume, W/m3). According to the foregoing embodiment, the magnetic shifting composition can be switched between different shift ratios via different embodiments of the magnetic conductive members 40, 50, 60. If the number of the magnets 46a, 46b, 51a, 51b, 51c, 51d that can be switched by the magnetic conductive elements 40, 50, 60 fails to conform to the formulas (2) and (3), The embodiment of the stator 30 of "Fig. 5A" (conforms to equations (2) and (4), and can improve the stability in different speed ratios. 18 201131947 Furthermore, the above equation (2), (3) and (4), which are based on the relationship of the main chopping waves of the stator 30, and if the pole pairs of the stators 3〇 in the relations are in the order of the magnetic conductivity Permeance harm〇nics) is designed to have the following relationship: Equation (3) Equation (6) Equation (7) PN1-3 ^ R+STr ^ PN1+3 PN2-3 ^ R+ST1J ^ PN2+3 PN2-3 $ R+ ST2' $ PN2+3

其中’ ST1’及ST2’分別為定子30的高階導磁之極對數。舉例 而言’若定子30之主簡諧波的極對數為4,則其三階導磁(the third permeance harmonics)之極對數即為12 ’因此,在設計轉子2〇的極 對數R、及導磁元件40的導磁體46a,46b的數量pN1, pN2時則 有更大的彈性選擇空間。 此外,在上述關係式中,定子3〇所產生的磁場除了採用與轉 子20的極對數尺及導磁元件4〇的導磁4如,4邰同步方式之外, 亦可採用賴步之設計H亦可#由控制奸3G之極對數及 /或導磁元件40而在同步與非同步之間做切換。 接著’請續參考「第10A圖」、「第10B圖」、及「第圖」, 其各別為依縣提案磁性魏組狀導磁元件㈣四實施例示意 圖、「第10A圖」在10B-10B位置之局部剖面示意圖及動作示意 圖。 圖中可以見悉,導磁元件80包含有第一環82及第二環84。 第-環82料乡_互平行、祕狀並以環形方續狀導磁天 L Ο 19 201131947 塊820(亦可稱第一導磁子塊)。第二環84亦包含多個相互平行、 呈條狀並以環形方式排列之導磁子塊84〇(亦可稱第二導磁子塊)。 第一環82之導磁子塊820與第二環84之導磁子塊84〇係在徑向 交互列置並夾置於於定子30與轉子20(請參閱「第】圖」)之間。 意即第一環82之導磁子塊820與第二環84之導磁子塊84〇係位 於相同或相接近之半徑位置,此點可以從「第1〇B圖」中看出。 第10B圖」為「第l〇A圖」在10B-10B位置之局部剖面圖, 此局部剖面之方式係類似於「第4B圖」與「第2圖」及「第4A 圖」之剖面關係。意即,「第l〇B圖」所示意的僅為「第1〇A圖」 部分弧段之剖面圖。 「第10B圖」係示意導磁元件80之第一環82與第二環84位 於第一位置之狀態,在此第一位置時,導磁子塊82〇, 840相互之 間均具有一個距離’且各導磁子塊820, 840自成一個導磁體。此 處所述之距離在圖式中雖呈等距狀態,但並不以此為限,只要兩 兩導磁子塊820, 840間形成前述之氣隙,而使得相鄰之導磁子塊 820, 840不形成前述之導磁體作用時’即可,即使導磁子塊82〇, 840 間的距離非等距亦可。 而在「第10C圖」中則示意導磁元件80之第一環82與第二 環84位於第二位置之狀態,在第二位置時,二相鄰之導磁子塊82〇, 840相互靠攏,使得兩兩靠攏的導磁子塊82〇, 840形成一個導磁 體。此處所述之靠攏係指兩相鄰之導磁子塊820, 840之間的距離 足夠小到使該兩相鄰之導磁子塊820, 840形成單一導磁體之狀態。 20 / 201131947 從「第10B圖」及「第l〇C圖」可以得知,在「1〇B圖」所 形成之導磁體數量係為「第10C圖」之導磁體數量的兩倍。因此, 導磁元件80可以經由控制而改變其導磁體數量。 關於控制導磁元件80變化其導磁體數量之致動元件沾(請參 閱「第10A圖」.),係可以採用電動馬達或氣壓閥等元件。此致動 元件88亦可應用於「第1圖」、「第7A圖」、「第8圖」、及「第 11A圖」之實施例中。當然,若將此致動元件88改成固定式,由 p 人工撥動控制亦可。 續,請參閱「第11A圖」、「第11B圖」、及「第11C圖」,其 各別為依據本提案磁性變速組成之導磁元件的第四實施例示意 圖、「第11A圖」在11B-11B位置之局部剖面示意圖及動作示意 圖。其圖式表示方式與「第l〇A圖」、「第1〇B圖」、及「第1〇匸 圖」相似,故不再贅述。 從圖中可以看出導磁元件之第四實施例包含第一環92、第 # 一環94、及第二環96。第一環92、第二環94及第三環96各別具 有多個導磁子塊920, 940, 960(亦可各別稱為第一、第二、第三導 磁子塊)’第一導磁子塊920、第二導磁子塊94〇、及第三導磁子塊 960係在經向依序列置並被夾置於該定子%與該轉子%之間,各 導磁子域920, 940, 960係位於_或相接近之半徑位置(即距離圓 心1半技相當),因此,當第一環92、第二環94及第三環%位於 如「第11B圖」所示之第一位置時,各導磁子塊92〇, 94〇,畑各 自成為個獨立的導磁體,使此導磁元件9〇具有順個導磁體, τ <τ_ 21 201131947 而第一環92、第二環94及第三環%位於如「第11C圖」所示之 第二位置時,相鄰的三個導磁子塊920, 940, _相互靠攏並形成 -個導磁體’使此導磁元件9〇具有pN2個導磁體,因此,位於第 -位置之導磁元件90所形成的導磁體的數量pNH系為位於第二位 置之導磁體的數量PN2的三倍。 除此之外’請參閱「第11D圖」,其係為第一環%、第二環 94及第一環96位於第二位置之示意圖圖中可以看見,第三環 %之導磁子塊係與第二環94之導磁子塊94〇相互靠搬,而第 -環92之導磁子塊920則未與(第二、第三)導磁子塊_靠 攏(或稱接近或接觸)’因此’靠攏的導磁子塊940, 960形成導磁 體,而(第一)導磁子塊920則獨立形成一個導磁體,使導磁元件 90具有PN3個導磁體,是以「第lm圖」所形成之導磁體的數量 PN3為「第11C圖」所形成導磁體數量pN2的二倍。其中簡可 滿足下式(5): ' PN3-3 ^ R+ST1 ^ pN3+3. 々/0、 ......................................... 再者第% 92、第二環94及第三環%之相對位置亦可採 用非等距之方式排列’而使得導磁體所佔弧長與磁騎佔弧長不 相等’亦能達到傳遞動力之目的,唯其所傳遞之扭矩亦將有所變 動。 關於前述式⑴中之關係,除了上述的之外, 亦可採用m=k=卜如此一來,定子3〇的極對數st卜轉子加的 極對數R、及導磁元件40的導磁體咖,畅的數量削,舰的 22 201131947 …….式(9) ••…式(10) ·....式(11) ^ R+3 ' 時,其關 R-3 ^ PN1+ST1 ^ R+3............................. R-3 ^ PN2+ST1 ^ R+3............................ R-3 ^ PN3+ST1 ^ R+3.............................. PN3-3 $ R+ST1 $ PN3+3、或 R_3 $ pN3+sTi 或 ST1-3 $ PN3+R $ ST1+3。Wherein 'ST1' and ST2' are the pole pairs of the higher-order magnetic permeability of the stator 30, respectively. For example, if the pole pair of the main harmonic of the stator 30 is 4, the pole logarithm of the third permeance harmonics is 12 '. Therefore, the pole log R of the rotor 2〇 is designed. The number of conductive magnets 46a, 46b of the magnetically permeable element 40 has a greater flexibility in the selection of the number of pN1, pN2. In addition, in the above relation, the magnetic field generated by the stator 3〇 can be designed in addition to the pole-to-pole of the rotor 20 and the magnetic conductive 4 of the magnetic conductive element 4, for example, a synchronous method. H can also switch between synchronous and asynchronous by controlling the pole logarithm of the 3G and/or the magnetically permeable element 40. Then, please refer to "Picture 10A", "Picture 10B" and "Picture". Each of them is a schematic diagram of the four-part embodiment of the magnetic Wei-shaped magnetic conductive element (4) proposed by Yixian, and "10A" in 10B. A partial cross-sectional view and an action diagram of the -10B position. As can be seen, the magnetically permeable element 80 includes a first ring 82 and a second ring 84. The first-ring 82 material township _ mutual parallel, secret shape and magnetic continuity in the shape of a circular ring L Ο 19 201131947 block 820 (also known as the first magnetic sub-block). The second ring 84 also includes a plurality of magnetically conductive sub-blocks 84A (also referred to as second magnetically conductive sub-blocks) that are parallel to each other, are strip-shaped, and are arranged in an annular manner. The magnetically permeable sub-block 820 of the first ring 82 and the magnetically permeable sub-block 84 of the second ring 84 are alternately arranged in the radial direction and sandwiched between the stator 30 and the rotor 20 (see "Fig.") . That is, the magnetic permeable sub-block 820 of the first ring 82 and the magnetic permeable sub-block 84 第二 of the second ring 84 are located at the same or close to the radial position, which can be seen from the "Fig. 1B". Figure 10B is a partial cross-sectional view of Figure 10B-10B. This section is similar to the section relationship of Figure 4B and Figure 2 and Figure 4A. . That is to say, "Fig. 1B" is only a cross-sectional view of the arc of the "1st A". The "10B" diagram illustrates the state in which the first ring 82 and the second ring 84 of the magnetically permeable member 80 are in the first position. In this first position, the magnetically permeable sub-blocks 82, 840 have a distance from each other. And each of the magnetically permeable sub-blocks 820, 840 is self-contained as a magnetizer. The distances described herein are in an equidistant state in the drawings, but are not limited thereto, as long as the aforementioned air gaps are formed between the two magnetically conductive sub-blocks 820, 840, so that the adjacent magnetically conductive sub-blocks are formed. When 820, 840 does not form the aforementioned magnetism, it is sufficient, even if the distance between the magnetic conductive sub-blocks 82, 840 is not equidistant. In the "10C", the first ring 82 and the second ring 84 of the magnetically permeable member 80 are in a second position. In the second position, the two adjacent magnetic sub-blocks 82, 840 are mutually Close together, the magnetically permeable sub-blocks 82 〇 840 of the two close together form a magnetizer. As used herein, the proximity means that the distance between two adjacent magnetically permeable sub-blocks 820, 840 is sufficiently small that the two adjacent magnetically permeable sub-blocks 820, 840 form a single magnet. 20 / 201131947 It can be seen from "Fig. 10B" and "Fig. 1C" that the number of magnetisms formed in "1〇B diagram" is twice the number of magnets in "10C". Therefore, the magnetic conductive element 80 can change the number of its magnetizers via control. Regarding the actuating element which controls the amount of the magnetizer of the magnetic conductive element 80 (refer to Fig. 10A), an electric motor or a pneumatic valve or the like can be used. The actuating element 88 can also be applied to the embodiments of "Fig. 1", "Fig. 7A", "Fig. 8", and "Fig. 11A". Of course, if the actuating element 88 is changed to a fixed type, it can also be controlled by p manual shifting. Continuing, please refer to "11A", "11B" and "11C", each of which is a schematic diagram of a fourth embodiment of a magnetically permeable component of the magnetic shifting composition according to the present proposal, and "11A" Partial cross-section diagram and action diagram of position 11B-11B. Its schema representation is similar to that of "1〇A", "1〇B", and "1第", so it will not be described again. It can be seen from the figure that the fourth embodiment of the magnetically permeable element comprises a first ring 92, a # a ring 94, and a second ring 96. The first ring 92, the second ring 94, and the third ring 96 each have a plurality of magnetically conductive sub-blocks 920, 940, 960 (also referred to as first, second, and third magnetically conductive sub-blocks respectively). The magnetic sub-block 920, the second magnetic sub-block 94 〇, and the third magnetic permeable sub-block 960 are arranged in the warp direction and sandwiched between the stator % and the rotor %, each of the magnetic domains 920, 940, 960 are located at _ or close to the radial position (ie, half the distance from the center of the circle), so when the first ring 92, the second ring 94 and the third ring % are located as shown in Figure 11B In the first position, each of the magnetic conductive sub-blocks 92〇, 94〇, 畑 each becomes an independent magnetizer, so that the magnetic conductive element 9〇 has a parallel magnet, τ <τ_ 21 201131947 and the first ring 92 When the second ring 94 and the third ring % are located at the second position as shown in FIG. 11C, the adjacent three magnetic conductive sub-blocks 920, 940, _ are close to each other and form a magnetizer. The magnetic conductive element 9A has pN2 magnetizers, and therefore, the number of conductive magnets pNH formed by the magnetic conductive element 90 at the first position is three times the number PN2 of the magnetic conductors located at the second position. In addition, please refer to "11D", which can be seen in the schematic diagram of the first ring %, the second ring 94 and the first ring 96 in the second position, the third ring % of the magnetic sub-block The magnetically permeable sub-blocks 94 of the second ring 94 are moved against each other, and the magnetically permeable sub-blocks 920 of the first ring 92 are not close to (or close to) the (second, third) magnetically permeable sub-blocks. The magnetic flux blocks 940, 960, which are close together, form a magnetizer, and the (first) magnetically conductive sub-block 920 independently forms a magnetizer, so that the magnetically permeable element 90 has PN3 magnetizers, The number of magnetizers PN3 formed in the figure is twice the number of magnetizers pN2 formed in "11C". Which can satisfy the following formula (5): ' PN3-3 ^ R+ST1 ^ pN3+3. 々/0, ....................... .................. Further, the relative positions of the %92, the second ring 94 and the third ring % may also be arranged in a non-equidistant manner to make the magnetizer The arc length and the magnetic arc occupying the arc length are not equal 'can also achieve the purpose of transmitting power, but the torque transmitted will also change. Regarding the relationship in the above formula (1), in addition to the above, m=k=b, the pole pair number of the stator 3〇, the pole pair number R of the rotor, and the magnetizer of the magnetic conductive element 40 may be used. , the number of smooth cuts, the ship's 22 201131947 ....... (9) ••...Formula (10) ·....Formula (11) ^ R+3 ', when it is closed R-3 ^ PN1+ST1 ^ R+3............................. R-3 ^ PN2+ST1 ^ R+3....... ..................... R-3 ^ PN3+ST1 ^ R+3.................. ............ PN3-3 $ R+ST1 $ PN3+3, or R_3 $ pN3+sTi or ST1-3 $ PN3+R $ ST1+3.

當當轉子20的極對數R小於定子3〇的極對數sti 係式如下: ST1-3 ^ PN1+R ^ ST1+3...... .......................................(12) ST1-3 ^ PN2+R ^ ST1+3..... ...................................... (13) ST1-3 ^ PN3+R ^ ST1+3 — (14) 上述式⑼到式(14)中的定子3〇極對數阳,阳亦可分別替換 前述之高階導磁之極對數ST1,或STr(即將式⑶到式⑺中的阳 # ST2 替換為 STl,,ST2,)。 ’ 最後’關於前述將本提案之磁性變速組成應用於分段相位驅 動(Split phase)或電磁變速之馬達之方式,茲說明如下。其中分段 相健動所得狀變速比敍於丨,㈣速方式之變速比= 能大於或小於1。 請搭配「第12圖」閱覽之。圖中可以見悉,定子3〇是位於 轉子20之徑向内侧’而導磁元件99則位於定子3〇與轉子 ^ 間。定子30具有繞線臂300,從圖中可以看出,定子邓共有1 、 to 23 201131947 個繞線臂300。在使用傳統之分段相位驅動(Splitphase)或電磁變速 之馬達時,須參考一繞線表(winding chart,或稱分段相位繞線表), ^下表所示,此繞線表並非用以限制本提案之範圍。 磁數(# of magnet Poles) '^^ 2 4 定子繞線臂的數量(number of stator arms) (或稱定子極對數x2) 減 速 比 3 6 9 12 ABC AbCaBc AacBBaCCb AAccBBaaCCbb 1:1 ABC ABCABC ABaCAcBCb AcBaCbAcBaCb 2:1 6 無 無 ABCABCABC 無 3:1 8 ABC ABCABC AaABbBCcC ABCABCABCABC 4:1 10 ----^ 12 ABC AbCaBc AaABbBCcC AabBCcaABbcC A-b-C-a-B-c 5:1 無 無 ABCABCABC 無 6:1 14 ABC AcBaCb ACaBAbCBc AacCBbaACcbB A-b-C-fl-B-c 7:1 16 ABC ABCABC AAbCCaBBc ABCABCABCABC 8:1 18 ----— 20 L----—___ 無 無 無 無 9:1 ABC ABCABC AbbCaaBcc AbCaBcAbCaBc 10:1 201131947When the pole pair number R of the rotor 20 is smaller than the pole pair number sti of the stator 3〇, the following equation is as follows: ST1-3 ^ PN1+R ^ ST1+3...... .............. .........................(12) ST1-3 ^ PN2+R ^ ST1+3..... ...... ................................ (13) ST1-3 ^ PN3+R ^ ST1+3 — (14) The stator 3 of the above formulas (9) to (14) has a logarithmic logarithm of yang and yang, and may also replace the polar logarithm ST1 of the higher-order magnetic permeability, or STr (that is, replace the positive #ST2 in the equations (3) to (7) with ST1, , ST2,). The last method regarding the application of the magnetic shifting component of the present invention to the motor of the split phase or electromagnetic shift is explained below. Among them, the gear ratio of the segmented phase movement is described in 丨, and the gear ratio of the (four) speed mode is greater than or less than 1. Please read it with "Figure 12". As can be seen, the stator 3 is located radially inward of the rotor 20 and the magnetically permeable element 99 is located between the stator 3 and the rotor ^. The stator 30 has a winding arm 300. As can be seen from the figure, the stator has a total of 1, 23, 31,131,947 winding arms 300. When using a conventional segmented phase drive (Splitphase) or electromagnetic variable speed motor, refer to a winding chart (or segmented phase winding table). ^ The winding table is not used as shown in the table below. To limit the scope of this proposal. # of magnet Poles '^^ 2 4 Number of stator arms (or stator pole pairs x2) Reduction ratio 3 6 9 12 ABC AbCaBc AacBBaCCb AAccBBaaCCbb 1:1 ABC ABCABC ABaCAcBCb AcBaCbAcBaCb 2:1 6 No ABCABCABC No 3:1 8 ABC ABCABC AaABbBCcC ABCABCABCABC 4:1 10 ----^ 12 ABC AbCaBc AaABbBCcC AabBCcaABbcC AbCaBc 5:1 No ABCABCABC No 6:1 14 ABC AcBaCb ACaBAbCBc AacCBbaACcbB AbC-fl- Bc 7:1 16 ABC ABCABC AAbCCaBBc ABCABCABCABC 8:1 18 ----- 20 L-----___ Nothing Nothing 9:1 ABC ABCABC AbbCaaBcc AbCaBcAbCaBc 10:1 201131947

磁數(# of magnet poles) 定子繞線臂的數量(number of stator arms) (或稱定子極對數x2) 減 速 比 15 18 .2 AAACCbbbaaCCCbb AAAcccBBBaaaCCCbbb 1:1 4 AAcBaCCbAcBBaCb AAcBBaCCbAAcBBaCCb 2:1 6 無 AcBaCbAcBaCbAcBaCb 3:1 8 AcaCABabABCbcBc ABaCAcBCbABaCAcBCb 4:1 10 ABCABCABCABCABC AcabABCbcaCABabcBC 5:1 12 無 ABCABCABCABCABC AaBbCcAaBbCcAaBbCc A-B-C-A-B-C-A-B-C 6:1 14 AaAaABbBbBCcCcC AabcCABbcaABCcabBC 7:1 16 AaAaACcCcCBbBbB AaABbBCcCAaABbBCcC 8:1 18 無 無 9:1 20 ABCABCABCABCABC AaABbBCcCAaABbBCcC 10:1 虽將此繞線表應用於未有本提案之導磁元件99之結構下(也 就疋將第12圖」中之導磁元件99移除之結構),可用以得知定 子3〇之各繞線臂300所需繞線之方式及可得之減速比。圖中所示 之A,B,C各別表示第一相位繞線方式、第二相位繞線方式、第三 才4凡線方式’而a,b,c則各別表示與第一相位反相之繞線方式、 與第二相位反相之繞線方式、及與第三相位反相之燒線方式。在S】 25 201131947 未採用導磁元件"之結構時,若轉子2〇之磁數為4 ’而定子3〇 繞線臂勘的數量為9,且其採用_八嶋方式緩線’則可得 到2:1的減速比。 其中ABaW每财詞代表—個繞料的繞線方 式’並蚊子30的繞線臂_採順時針或逆時針方式配置,以上 述施以⑽繞線方式為例,第一繞線臂採用帛-相位繞 線方式㈧、第二繞線臂採用第二相位繞線方式 3。。採用與第一相位相反之繞線方式⑻、而蝴 用第二相位繞線方式(C),以下依此類推。前述第一、二、三、四 繞線臂係奴子%上依順時針方式依序相鄰之繞線臂獨。 Γ—參-」之應㈣,狀子3嘴12個繞線臂 右母…300獨立繞設線圈且相鄰燒線臂300繞設不 同相位之顧時,麻定子3Q將具有12_鋪 的^細為雜數_數爾)。轉子Μ R為K)(即磁極數為•導磁元件99之__ 因此,依下述式⑽可以得知在導磁元件99 為 990中的定子側極對數幻即 ^ 之間的空隙 -HR-PN,....................為2。心奴子綱極數為 4。 ::該定子側磁極數4與定;的磁= 查上述繞線表,可得到其繞線方式為杨CbAcBaCb,是以在導 磁元件99與定子3〇間可得到之減速比為z 與導磁元件99間的減逮比貝⑷,是以「Λ圖 26 201131947 的整個分段相位驅動馬達的減速比將達到1〇:1 (即2:ι乘上5 ”。 此外’若將上述定子30中兩兩相鄰之繞線臂雇視為一繞線# of magnet poles The number of stator arms (or the number of stator poles x2) reduction ratio 15 18 .2 AAACCbbbaaCCCbb AAAcccBBBaaaCCCbbb 1:1 4 AAcBaCCbAcBBaCb AAcBBaCCbAAcBBaCCb 2:1 6 No AcBaCbAcBaCbAcBaCb 3: 1 8 AcaCABabABCbcBc ABaCAcBCbABaCAcBCb 4: 1 10 ABCABCABCABCABC AcabABCbcaCABabcBC 5: 1 12 None ABCABCABCABCABC AaBbCcAaBbCcAaBbCc ABCABCABC 6: 1 14 AaAaABbBbBCcCcC AabcCABbcaABCcabBC 7: 1 16 AaAaACcCcCBbBbB AaABbBCcCAaABbBCcC 8: 1 18 None None 9: 1 20 ABCABCABCABCABC AaABbBCcCAaABbBCcC 10: 1, although this winding The table is applied to the structure in which the magnetic conductive element 99 of the present invention is not provided (that is, the structure of the magnetic conductive element 99 in FIG. 12 is removed), and the winding arm 300 of the stator 3 can be used. The way to wind and the available reduction ratio. The A, B, and C shown in the figure respectively indicate the first phase winding mode, the second phase winding mode, and the third mode 4, and a, b, and c respectively indicate that they are opposite to the first phase. The winding method of the phase, the winding method in which the second phase is inverted, and the firing method in which the third phase is inverted. In the case of S = 25 201131947, if the structure of the magnetic conductive element is not used, if the magnetic number of the rotor 2〇 is 4' and the number of the stator 3 winding arm is 9, and the _ gossip mode is used, A 2:1 reduction ratio is obtained. Among them, ABaW represents a winding method of winding material and the winding arm of mosquito 30 is arranged clockwise or counterclockwise. Taking the above-mentioned (10) winding method as an example, the first winding arm adopts 帛- Phase winding method (8), and the second winding arm adopts a second phase winding mode 3. . The winding method (8) opposite to the first phase is used, and the second phase winding method (C) is used, and so on. The first, second, third, and fourth winding arm slaves are in a clockwise manner and are adjacent to each other in a clockwise manner. Γ—参-” (4), 12 nozzles of the shape of the mouth, 12 winding arms, right mother... 300 independent winding coils and adjacent firing arm 300 around the different phases, the hemp stator 3Q will have 12_ shop ^ Fine for the number _ number of er). The rotor Μ R is K) (that is, the number of magnetic poles is __ of the magnetic conductive element 99. Therefore, according to the following formula (10), it can be known that the magnetic flux between the stator side poles of the stator element 990 in the 990 is - HR-PN,.................... is 2. The number of heart slaves is 4. :: The number of poles on the stator side is 4 and the magnetic = Checking the above-mentioned winding table, the winding method is Yang CbAcBaCb, which is a reduction ratio between the magnetic permeability element 99 and the stator 3 and a reduction ratio between the magnetic component 99 and the magnetic conductive element 99 (4). "The reduction ratio of the entire segmented phase drive motor of Figure 26 201131947 will reach 1〇:1 (ie 2:ι times 5". In addition, if the two adjacent winding arms of the above stator 30 are regarded as a winding

臂組並繞有相同相位之繞線,則定子3G將具有6個磁極數而增 加其變化性。 S 其次’上述的導磁元件99若經由致動後,其導磁體之數量變 化為6_),此時之定子側極對數即為4(套用式⑽,因此,使 用繞線表時,魏即為8,產生抑之減速比。 再者,用以計算定子側極對數之式⑽亦可變化為下式⑽。 R2 = R+PN1.......................................... ..................................... 前述馬達定子線圈之驅動方式(或稱激磁方式)可以採用交流 電流方式(ACCU_t)驅動(如同步馬達方式驅動),亦可採用脈波寬 度調變(Pulse Width Modulation,PWM)方式所產生之方波或弦波 (如無刷直流馬達之驅動方式)。 綜上所述’由於實施例t的磁性變速組成包含了電動馬達或 發電機之定子與轉子的設計,並具有魏之結構設計,能易於與 電動馬達之馬達驅動器或發電機之取電電路(如整流穩塵等電路) 做整合形成可變速之馬賴可變速之發電機,此整合後 之可變速電動馬制時具有產生㈣動力及變速之魏但體積 及重罝則伽為原電動馬達之體積及重量,達顺高的驅動功率 密度。同時’磁性變速組成採用電磁式之變速,故能降低振動及 噪音。再者,在電動車產業的顧巾,此可變速電動馬達即能配 s不同的行車扭力需求及行驶速度要求,且能保持高效率運轉。 27 201131947 雖然本提案赠述之較佳實施觸露如上,财麟用以限 定本提案,任何鮮梅技·,在不雌本聽之精神和範圍 内,當可作些許之更__,目此本難之補賴範圍須視 本說明書所附之申請專概騎界定者為準。 【圖式簡單說明】 第1圖為依據本提案磁性變速組成第—實施_立體結構示 意圖。 第2圖為依據本提案磁性變速組成第—實施例的立體分解示 參 意圖The arm set is wound with the same phase, and the stator 3G will have 6 pole numbers to increase its variability. S. Secondly, if the above-mentioned magnetic conductive element 99 is actuated, the number of its magnetizers changes to 6_). At this time, the number of stator pole pairs is 4 (the formula (10) is used. Therefore, when using the winding table, Wei is For example, the reduction ratio is suppressed. Furthermore, the equation (10) for calculating the number of stator pole pairs can also be changed to the following equation (10). R2 = R+PN1............... ......................................................... .............. The drive mode (or excitation mode) of the motor stator coil can be driven by AC current (ACCU_t) (such as synchronous motor drive) or pulse width. A square wave or sine wave generated by the Pulse Width Modulation (PWM) method (such as the driving method of a brushless DC motor). In summary, the magnetic shifting composition of the embodiment t includes an electric motor or a generator. The stator and rotor are designed with Wei's structural design, which can be easily integrated with the motor drive of the electric motor or the power take-off circuit of the generator (such as rectifying and dust-reducing circuits) to form a variable-speed Malay variable-speed generator. This integrated variable speed electric horse timepiece Produce (4) Power and shifting speed, but the volume and weight are the volume and weight of the original electric motor, and the driving power density is up to the high. At the same time, the magnetic shifting component uses electromagnetic shifting, so it can reduce vibration and noise. In the electric vehicle industry, this variable-speed electric motor can be equipped with different driving torque requirements and driving speed requirements, and can maintain high efficiency operation. 27 201131947 Although the preferred implementation of this proposal is exposed as above , Cailin is used to limit this proposal, any fresh plum technology, in the spirit and scope of not listening to the female, when you can make a little more __, the scope of this difficult to rely on is attached to this manual The application for the definition of the specific rider shall prevail. [Simplified description of the drawings] Figure 1 is a schematic diagram of the magnetic shifting composition according to the present invention. The second embodiment is a three-dimensional decomposition of the magnetic shifting composition according to the present invention. Intention

實施例的定子的磁對 第4A圖為依據本提案磁性變速組成第一實施例之導磁元件 之剖面示意圖。 第4B圖為「第4A圖」之導磁元件第一實施例的局部放大剖 面示意圖。 第4C圖為「第4A圖」之導磁元件的第一實施例另—局部放 大剖面不意圖。 第5A圖為依據本提案磁性變速組成之定子的另一實施例的 繞線示意圖。 第5B圖為「第5A圖」的定子的另一實施例的動作示意圖。 第6圖為「第5A圖」及「第5B圖」極對數切換之示意圖。 第7A圖、第则及第7C圖為依據本提案磁性變速組成之 導磁元件的第二實施例示意圖。 28 201131947 第8圖為依據本提案磁性變速組成之導磁元件的第三實施例 示意圖。 第9圖為依據本提案磁性變速組成第二實施例的立體分解示 意圖。 第10A圖為依據本提案磁性變速組成之導磁元件的第四實施 例示意圖。 第10B圖及第10C圖各別為「第1〇A圖」在位置之 局部剖面示意圖及狀態示意圖。 第11A圖為依據本提案磁性變速組成之導磁元件的第四實施 例示意圖。 第11B圖及第lie圖各別為「第11A圖」在11B11B位置之 局部剖面示意圖及狀態示意圖。 第11D圖為「第11B圖」之另一狀態示意圖。 第12圖為依據本提案應用於分段相位驅動馬達之結構示意 圖。 【主要元件符號說明】 20 轉子 30 定子 300 繞線臂 32a, 32b 凸塊 34a,34b,34c,34d 感應線圈 35a, 35b 線圈組 36 極數調變電路 201131947 360, 362 切換開關 40, 50, 60, 70, 80, 90, 99 導磁元件 42, 52, 62, 82, 92 第一環 420, 422, 440, 442 導磁子塊 429, 449 弧段 44, 54, 64, 84, 94 第二環 46a, 46b 導磁體 48a, 48b, 48c, 48d 磁隙 53, 55, 57, 59 導磁子塊 51a, 51b, 51c, 51d 導磁體 56, 96 第三環 58 第四環 63, 65, 72 導磁子塊 66a, 66b, 66c, 74a, 74b 電絕緣元件 820, 840, 920, 940, 960 導磁子塊 88 致動元件 990 空隙Magnetic Pair of the Stator of the Embodiment Fig. 4A is a schematic cross-sectional view showing the magnetic conductive element of the first embodiment in accordance with the present invention. Fig. 4B is a partially enlarged cross-sectional view showing the first embodiment of the magnetic conductive element of Fig. 4A. Fig. 4C is a view showing a first embodiment of the magnetic conductive element of "Fig. 4A", and a partial enlarged cross section is not intended. Fig. 5A is a schematic view of a winding of another embodiment of the stator of the magnetic shifting composition according to the present proposal. Fig. 5B is a schematic view showing the operation of another embodiment of the stator of Fig. 5A. Figure 6 is a schematic diagram of the pole-to-number switching of "5A" and "5B". Fig. 7A, Fig. 7C and Fig. 7C are schematic views showing a second embodiment of the magnetic conducting element of the magnetic shifting composition according to the present proposal. 28 201131947 Figure 8 is a schematic view of a third embodiment of a magnetically permeable component of the magnetic shifting composition according to the present proposal. Fig. 9 is a perspective exploded view showing the second embodiment of the magnetic shifting composition according to the present proposal. Fig. 10A is a view showing a fourth embodiment of the magnetic conducting element of the magnetic shifting composition according to the present proposal. Fig. 10B and Fig. 10C are respectively a partial cross-sectional view and a state diagram of the position of "Fig. 1A". Fig. 11A is a view showing a fourth embodiment of the magnetic conducting element of the magnetic shifting composition according to the present proposal. Fig. 11B and the lie diagram are respectively a partial cross-sectional view and a state diagram of the "11A map" at the position 11B11B. Fig. 11D is a schematic view showing another state of "11B". Figure 12 is a schematic view showing the structure of a segmented phase drive motor according to the present proposal. [Main component symbol description] 20 rotor 30 stator 300 winding arm 32a, 32b bump 34a, 34b, 34c, 34d induction coil 35a, 35b coil group 36 pole number modulation circuit 201131947 360, 362 changeover switch 40, 50, 60, 70, 80, 90, 99 magnetically conductive elements 42, 52, 62, 82, 92 first ring 420, 422, 440, 442 magnetically conductive sub-block 429, 449 arc segment 44, 54, 64, 84, 94 Two rings 46a, 46b magnets 48a, 48b, 48c, 48d magnetic gaps 53, 55, 57, 59 magnetic sub-blocks 51a, 51b, 51c, 51d magnets 56, 96 third rings 58 fourth rings 63, 65, 72 magnetic sub-blocks 66a, 66b, 66c, 74a, 74b electrically insulating elements 820, 840, 920, 940, 960 magnetic sub-blocks 88 actuating elements 990 voids

3030

Claims (1)

201131947 七、申請專利範圍: 1. 一種磁性變速組成,包含: ' 一轉子,具有多個磁極’該轉子的該些磁極具有R個極對 . 數; 一定子,與該轉子同軸套設,該定子具有多個磁極,該定 子的該些磁極具有ST1個極對數;以及 一導磁元件,位於該轉子與該定子之職具有多個導磁 鲁體’當料磁元倾致動時,料磁树顧雜地使_ 個或PN2 _些導韻職於鋪子與奴子之間,其中, PN1-3 $ R+ST1 g PN1+3、或 R-3 g PN1+ST1 g R+3、 或 ST1-3 $ PN1+R $ ST1+3。 2.如請求項第i項所述之磁性變速組成,其中p腦^㈣耵 $ W2+3、或 R-3 $ PN2+ST1 $ R+3、或灯13 $ pN2+R S ST1+3。 • 3.如請求項第i項所述之雜變速組成,其中該導磁元件包含一 第-環及-第二環’該第一環與該第二環係軸向連接該第一 環具有PNH固導磁子塊,該帛二環具有pN2個導磁子塊,當 - 該導磁元件被軸向致動時,該導磁元件係選擇性地使該第一環 或該第二環移動至該轉子與該定子之間。 4.如請求項第!項所述之磁性變速組成,其中該導磁元件包含一 第-環及-第二環,該第一環係位於該第二環之徑向外側且該 第-環及該第二環係配置於該定子與該轉子之間,當該導磁& 1 S ] 31 201131947 件被致動時,該第一環與該第二環係相對運動於一第一位置與 一第二位置之間,當該第一環與該第二環位於該第一位置時, 該導磁元件具有PN1個該導磁體,當該第一環與該第二環位於 該第二位置時,該導磁元件具有PN2個該導磁體。 5. 如請求項第4項所述之磁性變速組成,其中該第一環具有多個 第一導磁子塊,該第二環具有多個第二導磁子塊,當該第一環 與該第二環位於該第一位置時,兩相鄰的該些第一導磁子塊與 該些第二導磁子塊形成該PN1個導磁體之一,當該第一環與該 第二環位於該第二位置時,該些第一導磁子塊與該些第二導磁 子塊各別形成該PN2個導磁體之一。 6. 如請求項第1項所述之磁性變速組成,其中該定子包含多個感 應線圈,該些感應線圈被通電時係形成該些磁極。 7. 如凊求項第6項所述之磁性變速組成,其中該定子另包含一極 數調變電路,該極數調變電路係選擇性地切換該些感應線圈於 該ST1個極對數及一 ST2個極對數之間。 8. 如請求項第7項所述之磁性變速組成,其中該定子另包含環形 配置之多個凸塊,該些感應線圈係各別繞於該些凸塊,當該些 感應線圈被切換至該ST1個極對數時,相鄰之該些感應線圈之 極性係相反,當該些感應線圈被切換至該ST2個極對數時,該 些感應線圈係被群組為多個線圈組,且相鄰之該些線圈組之極 性係相反。 9. 如請求項第8項所述之磁性變速組成,其中ΡΝ2·3 s r+ST2 32 201131947 ^ PN2+3 ° 10.如請求項第8項所述之磁性變速組成,其中每一該些線圈組係 包含三個依序相鄰的該些感應線圈。 11.如請求項第8項所述之磁性變速組成,其中該導磁元件包含一 第一環及一第二環,該第一環與該第二環係轴向連接,該第一201131947 VII. Patent application scope: 1. A magnetic shifting composition comprising: 'a rotor having a plurality of magnetic poles'. The magnetic poles of the rotor have R pole pairs. The stator is coaxially sleeved with the rotor. The stator has a plurality of magnetic poles, the magnetic poles of the stator have ST1 pole pairs; and a magnetic conductive component is located at the rotor and the stator, and has a plurality of magnetic conductive bodies when the material is tilted and actuated. The magnetic tree makes _ or PN2 _ some guides between the shop and the slave, where PN1-3 $ R+ST1 g PN1+3, or R-3 g PN1+ST1 g R+3, Or ST1-3 $ PN1+R $ ST1+3. 2. The magnetic shifting composition of claim i, wherein p brain ^(4) 耵 $ W2+3, or R-3 $ PN2+ST1 $ R+3, or lamp 13 $ pN2+R S ST1+3. 3. The hybrid shifting composition of claim i, wherein the magnetically permeable element comprises a first ring and a second ring, the first ring being axially coupled to the second ring system, the first ring having a PNH solid-conductive magnetic sub-block having pN2 magnetically permeable sub-blocks, the magnetically permeable element selectively causing the first or second ring when the magnetically permeable element is axially actuated Moved between the rotor and the stator. 4. As requested in the item! The magnetic shifting component of the present invention, wherein the magnetic conductive component comprises a first ring and a second ring, the first ring is located radially outward of the second ring, and the first ring and the second ring configuration Between the stator and the rotor, when the magnetic permeability & 1 S ] 31 201131947 is actuated, the first ring and the second ring system move relative to each other between a first position and a second position When the first ring and the second ring are in the first position, the magnetic conductive element has PN1 magnets, and when the first ring and the second ring are in the second position, the magnetic component There are PN2 of the magnetizers. 5. The magnetic shifting composition of claim 4, wherein the first ring has a plurality of first magnetically permeable sub-blocks, and the second ring has a plurality of second galvanic sub-blocks, when the first ring When the second ring is in the first position, the two adjacent first conductive sub-blocks and the second conductive sub-blocks form one of the PN1 magnetizers, when the first ring and the second ring When the ring is in the second position, the first conductive sub-blocks and the second magnetic conductive sub-blocks respectively form one of the PN2 magnetizers. 6. The magnetic shifting composition of claim 1, wherein the stator comprises a plurality of inductive coils, the inductive coils forming the magnetic poles when energized. 7. The magnetic shifting composition of claim 6, wherein the stator further comprises a pole number modulation circuit, the pole number modulation circuit selectively switching the induction coils to the ST1 poles Logarithm and a ST2 pole logarithm. 8. The magnetic shifting composition of claim 7, wherein the stator further comprises a plurality of bumps arranged in a ring shape, the induction coils respectively winding around the bumps, and when the induction coils are switched to When the ST1 poles are opposite, the polarities of the adjacent induction coils are opposite. When the induction coils are switched to the ST2 pole pairs, the induction coils are grouped into a plurality of coil groups, and the phases are The coil groups adjacent to each other are opposite in polarity. 9. The magnetic shifting composition as set forth in item 8 of the claim, wherein ΡΝ2·3 s r+ST2 32 201131947 ^ PN2+3 ° 10. The magnetic shifting composition as described in item 8 of the claim, each of which The coil assembly includes three induction coils adjacent in sequence. 11. The magnetic shifting composition of claim 8, wherein the magnetically conductive component comprises a first ring and a second ring, the first ring being axially coupled to the second ring system, the first 環具有ΡΝ1個導磁子塊’該第二環具有ρΝ2個導磁子塊,當 該導磁元件被軸向致動時,該導磁元件係選擇性地使該第一環 或該第二環被移至該轉子與該定子之間。 12.如請求項帛8項所述之磁性變速組成,其中該導磁元件包含一 第%及一第二環,該第一環與該第二環係徑向接觸並夾置於 該疋子與該轉子之間,當該導磁元件被致動時,該第一環與該 $二環係相對位移於-第一位置與—第二位置之間,當該第一 環與該第二環位於該第一位置時,該導磁元件具有ρΝΐ個該些 導磁體’當該第一環與該第二環位於該第二位置時該導磁元 件具有PN2個該些導磁體。 13.如^項第1項所述之磁性變速組成,其中該導磁元件包含一 第%及-第二環,該第一環具有多個環狀列置之第一導磁子 塊,該第二環具有多個環狀列置之第二導磁子塊,該些第一導 Z塊與該些第二導磁子塊係在徑向交錯列置並被夾置於該 一产/轉子之間’ #該導磁元件被致動時,該第-環與該第 相對運動於一第一位置與—第二位置之間,當該第一環 …第二環位於該第-位置時,兩相鄰_些第—導磁子塊^ 33 201131947 該些第二導磁子塊戦該丽個導顧之-,當該第—環與該 第二環位於該第二位置時,該些第一導磁子塊與該些第二導磁 子塊各別形成該PN2個導磁體之一。 14.如請求項第1項所述之磁性變速組成’其中該導磁元件包含一 第-環、-第二環、及一第三環,該第一環具有多個環狀列置 之第導磁子塊’該第二環具有多個環狀列置之第二導磁子 塊,該第三環具有多個環狀列置之第三導磁子塊,該些第一導 磁子塊、該些第二導磁子塊、及該些第三導磁子塊係在經向依 序列置並被技於該定子與該轉子之間,#該導磁元件被致動 時,該第一環、該第二環及該第三環係相對運動於一第一位 置、一第二位置及一第三位置之間,當該第一環、該第二環及 該第三環位於該第一位置時,三相鄰的該些第一導磁子塊、該 些第一導磁子塊及該些第三導磁子塊形成該PNi個導磁體之 一,當該第一環與該第二環位於該第二位置時,該些第一導磁 子塊、該些第二導磁子塊及該些第三導磁子塊各自形成該PN2 個導磁體之一,當該第一環與該第二環位於該第三位置時,兩 相鄰的該些第二導磁子塊及該些第三導磁子塊形成PN3個導 磁體之一,且該些第一導磁子塊各自形成該pN3個導磁體之 一,其中 PN3-3 S R+ST1 $ PN3+3、或 R-3 $ PN3+ST1 $ R+3、或 ST1-3 S PN3+R $ ST1+3。 15.如請求項第1項所述之磁性變速組成’其中該導磁元件之材料 為軟磁材料(Soft Magnetic Composite,SMC)。 34 201131947 16. —種磁性變速組成,包含: 轉子,具有多個磁極,該轉子的該些磁極具有R個極對 , 數; • _疋子’與該轉子同軸套設’該定子具有多個磁極,該定 子的該些磁極具有ST1個極對數及ST1,個高階導磁之極對 數;以及 一導磁元件,位於該轉子與該定子之間並具有多個導磁 • 體’當該導磁元件被致動時,料磁元件係選擇性地使PN1 個或PN2個該些導磁體對應於該轉子與該定子之間,其中, PN1-3 $ R+ST1’ g PN1+3、或 R-3 g PNl+STl,g R+3、 或 STl’-3 $ PN1+R $ STl,+3。 17. 如請求項第16項所述之磁性變速組成,其中pN2-3 ^ r+sti, S PN2+3、或 R-3 g PN2+ST1,$ R+3、或 sti,-3 $ PN2+R $ STl,+3。 • Μ.如請求項第16項所述之磁性變速組成,其中該導磁元件包含 -第-環及-第二環,該第-環與該第二_軸向連接該第 . 一環具有PN1個導磁子塊,該第二環具有PN2個導磁子塊, 當該導磁元件被軸向致動時,該導磁元件係選擇性地使該第一 環或該第二環移動至該轉子與該定子之間。 19.如請求項第16項所述之磁性魏喊,其巾該導磁元件包含 -第-環及m第-環係位於該第二環之#向外侧且 該第一環及該第二環係配置於該定子與該轉子之間,當該導汽 35 201131947 元件被致動時,該第一環與該第二環係相對運動於一第一位置 與一第二位置之間,當該第一環與該第二環位於該第一位置 時’該導磁元件具有PN1個該些導磁體,當該第一環與該第二 環位於該第二位置時,該導磁元件具有PN2個該些導磁體。 2〇·如請求項第19項所述之磁性變速組成,其中該第一環具有多 個第一導磁子塊,該第二環具有多個第二導磁子塊,當該第一 %與該第二環位於該第一位置時,兩相鄰的該些第一導磁子塊 與該些第二導磁子塊形成該PN1個導磁體之一,當該第一環與 該第二環位於該第二位置時,該些第—導磁子塊與該些第二導 磁子塊各別形成該PN2個導磁體之一。 21. —種分段相位驅動馬達,包含: 一轉子,具有多個磁極,該轉子的該些磁極具有R個極對 數; -定子’與該轉子_套設’該定子具衫個磁極,該定 子的該些磁極具有ST1個極對數;以及 -導磁元件’配置於該轉子與該定子之間並具有PN1個導 磁子塊’導磁子塊對應_轉子無定子之間並形成一定 子側極對數R2,其中R2=丨R_PN_们+觸,而幻與阳 則符合_分段她祕表(Winding Chart)。 、 22. —種磁性變速組成,包含: -轉子’具有多個磁極,該轉子的該些磁極具有r個極對 數; 36 201131947 -定子,與該轉子咖套設,該定子具有多個雜,該定 子的該些磁極具有ST1個極對數;以及 一導磁树,配置於該轉子與該定子之間並具有PN1個導 磁子塊,PN1個該些導磁子塊對應於該轉子與該定子之間,其 中 ’ PN1-3 S R+ST1 $ PN1+3、或 R_3 $ pN1+ST1 $ R+3、或 ST1-3 s PN1+R $ ST1+3。The ring has ΡΝ1 conductive sub-blocks. The second ring has ρ Ν 2 permeable sub-blocks. When the magnetically permeable element is axially actuated, the magnetically permeable element selectively causes the first ring or the second The ring is moved between the rotor and the stator. 12. The magnetic shifting composition of claim 8 wherein the magnetically permeable member comprises a first and a second ring, the first ring being in radial contact with the second ring and sandwiched between the tweezers Between the rotor and the rotor, when the magnetically permeable element is actuated, the first ring and the second ring system are relatively displaced between the first position and the second position, when the first ring and the second When the ring is in the first position, the magnetic conductive element has a plurality of the conductive magnets. When the first ring and the second ring are in the second position, the magnetic conductive element has PN2 of the conductive magnets. 13. The magnetic shifting composition of item 1, wherein the magnetically permeable element comprises a first and second ring, the first ring having a plurality of annularly disposed first magnetically permeable sub-blocks, The second ring has a plurality of annularly disposed second magnetically conductive sub-blocks, the first conductive Z-blocks and the second conductive magnetic sub-blocks are arranged in a radial staggered manner and sandwiched between the first production/ Between the rotors, when the magnetically permeable element is actuated, the first ring and the first relative movement are between a first position and a second position, and when the second ring is located at the first position When the adjacent first and second magnetic rings are located in the second position, The first conductive sub-blocks and the second magnetically conductive sub-blocks each form one of the PN2 magnetizers. 14. The magnetic shifting composition of claim 1 wherein the magnetically permeable element comprises a first ring, a second ring, and a third ring, the first ring having a plurality of annular arrays a second magnetic ring having a plurality of annularly disposed second magnetically conductive sub-blocks, the third ring having a plurality of annularly disposed third magnetically conductive sub-blocks, the first magnetically conductive sub-magnets The block, the second magnetically permeable sub-blocks, and the third magnetically permeable sub-blocks are disposed in the warp direction and are between the stator and the rotor. When the magnetic conductive element is actuated, the block The first ring, the second ring and the third ring are relatively moved between a first position, a second position and a third position, when the first ring, the second ring and the third ring are located In the first position, the three adjacent first conductive sub-blocks, the first conductive sub-blocks and the third conductive sub-blocks form one of the PNi magnetizers, when the first ring When the second ring is located at the second position, the first conductive sub-blocks, the second conductive sub-blocks, and the third conductive sub-blocks each form one of the PN2 magnetizers. First ring and When the second ring is located at the third position, the two adjacent second magnetic conductive sub-blocks and the third magnetic conductive sub-blocks form one of PN3 conductive magnets, and the first conductive magnetic sub-blocks are respectively formed One of the pN3 magnetizers, where PN3-3 S R+ST1 $ PN3+3, or R-3 $ PN3+ST1 $ R+3, or ST1-3 S PN3+R $ ST1+3. 15. The magnetic shifting composition of claim 1 wherein the material of the magnetically permeable member is a Soft Magnetic Composite (SMC). 34 201131947 16. A magnetic shifting composition comprising: a rotor having a plurality of magnetic poles, the magnetic poles of the rotor having R pole pairs, a number; • _ 疋 ' 'coaxially nested with the rotor 'the stator has a plurality of a magnetic pole, the magnetic poles of the stator have ST1 pole pairs and ST1, a pole pair of a high-order magnetic permeability; and a magnetic conductive element between the rotor and the stator and having a plurality of magnetic conductive bodies When the magnetic element is actuated, the magnetic element selectively causes PN1 or PN2 of the magnets to correspond between the rotor and the stator, wherein PN1-3$R+ST1'g PN1+3, or R-3 g PNl+STl, g R+3, or STl'-3 $ PN1+R $ STl, +3. 17. The magnetic shifting composition of claim 16 wherein pN2-3^r+sti, S PN2+3, or R-3 g PN2+ST1, $ R+3, or sti, -3 $ PN2 +R $ STl, +3. The magnetic shifting composition of claim 16, wherein the magnetically permeable element comprises a -th ring and a second ring, the first ring being connected to the second y-axis, the first ring having PN1 a magnetically permeable sub-block having PN2 magnetically permeable sub-blocks, the magnetically permeable element selectively moving the first or second ring to when the magnetically permeable element is axially actuated Between the rotor and the stator. 19. The magnetic scream of claim 16, wherein the magnetic conductive element comprises a -th ring and an m-ring system located outside the #-ring of the second ring and the first ring and the second a ring system is disposed between the stator and the rotor. When the air guiding member 35 201131947 is actuated, the first ring and the second ring system are relatively moved between a first position and a second position. When the first ring and the second ring are in the first position, the magnetic conductive element has PN1 of the conductive magnets, and when the first ring and the second ring are located at the second position, the magnetic conductive element has PN2 of these magnetizers. The magnetic shifting composition of claim 19, wherein the first ring has a plurality of first magnetically permeable sub-blocks, and the second ring has a plurality of second magnetically permeable sub-blocks, when the first % When the second ring is located at the first position, the two adjacent first magnetic conductive sub-blocks and the second magnetic conductive sub-blocks form one of the PN1 conductive magnets, when the first ring and the first ring When the second ring is located at the second position, the first magnetically conductive sub-blocks and the second magnetically conductive sub-blocks respectively form one of the PN2 conductive magnets. 21. A segmented phase drive motor comprising: a rotor having a plurality of magnetic poles, the magnetic poles of the rotor having R pole pairs; a stator 'and a rotor _ sleeve' the stator having a magnetic pole, The magnetic poles of the stator have ST1 pole pairs; and - the magnetic conducting element 'is disposed between the rotor and the stator and has PN1 magnetic conducting sub-blocks. The magnetic conducting sub-block corresponds to _ the rotor has no stator and forms a stator The side pole logarithm R2, where R2 = 丨 R_PN_ are + touch, while the illusion and yang are in accordance with the _ segmentation her cold table (Winding Chart). 22. A magnetic shifting composition comprising: - a rotor 'having a plurality of magnetic poles, the magnetic poles of the rotor having r pole pairs; 36 201131947 - a stator, with the rotor, the stator having a plurality of impurities The magnetic poles of the stator have ST1 pole pairs; and a magnetic tree disposed between the rotor and the stator and having PN1 magnetic conductive sub-blocks, and PN1 of the magnetic conductive sub-blocks correspond to the rotor and the rotor Between the stators, where 'PN1-3 S R+ST1 $ PN1+3, or R_3 $ pN1+ST1 $ R+3, or ST1-3 s PN1+R $ ST1+3. 3737
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* Cited by examiner, † Cited by third party
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CN112821716A (en) * 2021-01-11 2021-05-18 合肥工业大学 Barrel type mixed magnetic coupling
TWI750052B (en) * 2021-03-05 2021-12-11 中華汽車工業股份有限公司 Switching motor drive control system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112821716A (en) * 2021-01-11 2021-05-18 合肥工业大学 Barrel type mixed magnetic coupling
TWI750052B (en) * 2021-03-05 2021-12-11 中華汽車工業股份有限公司 Switching motor drive control system

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