M253703 勾、創作說明（1) 【新型所屬之技術領域遍 本創作係有關一種磁浮軸承，尤一 結構。 r/T心/予固疋之％形軸承 【先前技 習用風 銅式及液 件間形成 時會產生 愈高，發 多，且對 鐘五千轉 轉速風扇 片（GPU) 及機箱上 用數量如 嗓音及震 適，於是 然而磁 力卻始終 圖）所示， 磁壞（B )， 中可看出 術】 轉軸所使用之轴承，不外乎滾珠式、、、由 :式荨幾種，•此類轴承無可避免的皆合：油 哗’而必有摩擦力之產生，4高速運； 熱以：上；由：：：；=運作速度愈來 =能，亦非常之高，其轉速動概超過；:; 邛桌上型電腦除最基本的Cpu 以北及Λ?應器至少需使用-具風扇外，:二 亦皆有曰曰上、記憶體模組(RAM M〇dule)、燒錄機 此多! ί 用散熱風扇以幫助散熱，在風扇使 況下：若皆採習用之機械式軸承，則其 ，、白極為嚴重，對使用者之電腦操作造成不 有兹洋軸承之問世。 承之發展雖已有一段時日，但其懸浮之固定 进理想，如美國專利第6 6 1 7732號專利（第一 ς =承結構主要係由二對稱之靜磁環（Α)及一 Λ Λ環（Β)係套設於馬達之轉軸⑹上，由圖 石兹環（Β )係位於兩靜磁環（a )之間，其鄰接面M253703 Hook, creation instructions (1) [The new technology belongs to this field. This creation is about a magnetic bearing, especially a structure. r / T heart / Yu Guzhen's% -shaped bearing [previously used in the wind copper type and the formation between liquid parts will produce higher, more and more, and it is used on the fan fan (GPU) and chassis of 5,000 rpm The number is like the voice and the vibration, so the magnetic force is always shown.) The magnetic breakdown (B) can be seen in the above.] The bearings used for the shaft are nothing more than ball type, type, and type: • This kind of bearing is unavoidable: oil rushes and friction must be generated, 4 high-speed transport; heat to: above; from :::; = operating speed is getting more and more = can, also very high, its The speed will probably exceed ;: 邛 Except for the north of the most basic CPU and Λ? The desktop computer needs to be used at least-with a fan, there are also two: a memory module (RAM M〇dule) There are so many burners! Ί Use a cooling fan to help dissipate the heat. Under the condition of the fan: if all mechanical bearings are used, it will be very serious, which will cause users to operate the computer. The advent of bearings. Although the development of Cheng has been for some time, its suspension has been fixed ideally, such as US Patent No. 6 1 7732 (the first = = bearing structure is mainly composed of two symmetrical magnetostatic rings (Α) and Λ The Λ ring (B) is set on the shaft ⑹ of the motor, and the Turzitz ring (B) is located between the two magnetostatic rings (a), and its abutting surface
Ι1Η_ 第6頁 M253703 四、創作說明（2) 係為同一磁極，且為平行 該钭夕u二 斜 可產生斜向斥力，藉由 必针句斤力之水平分力及恭 i，rrx ^ . ^ , ^ A 孟直刀力，可對動磁環（B)及轉 時之困魏二上軸向之固定力”隹此種結構在實際製造 接之4+^ ^ 2 ’其原、因在於靜磁環（A)與動磁環⑻鄰 接之斜面傾角必需非常精密的吻 之任何一點皆俘捭相Π „欧 丨乂而便％形斜面間 二、，.，，占白保持相同間隙，此外，動靜磁環（A，Β)間之 立個辦 # ^ ^ 一 靜兹辰（A)係分為兩個獨 立個體，其磁力要保持完全相同杂 只I甘士 μ处士 了凡王相w貝非易事，而這兩個部份 轉失本正你而雜 土 P曰付砰磁壞（B)及轉軸（〇之旋 f寻天去平衡，即難以達到動 m ^ ^ , 動合P篓献，w 衡，因而發生震動，且震 能q者轉速的增加，故此種設計幾無商品化之可 另有一種设计係如中華民岡直4丨丨^ Π Ο Ο π η , 239 !i 5 而成，兮―in ()卜磁環（D)所對應套合 使轉軸(F)上，該二磁環(D，E)係 使“體之内外裱壁各成對應之單 -，外磁環⑻之内環壁及内 :所 Μ — L JL ^ X 必、w <外％壁皆為同一之 極（如南^ ^其分別對應之另一環壁則為第二磁 Γ Λ ϊ“外磁環（D，E)之鄰接面產生同極斥 此外，位於％壁上之磁極強度壌 磁擇广Γ>、々向T班、〆 乃付緣之配置’如外 =衣（2)之内％壁近兩端面處之磁力較強，中 磁i衷（E )則恰好相反，且内磁環（E ) 、 乂》 產生位向及斜向之斥力（如圖中箭號所示），而可使内磁環Ι1Η_ Page 6 M253703 Fourth, the creation description (2) is the same magnetic pole, and is parallel to the two slopes u can produce oblique repulsive force, through the horizontal force of the force of the required sentence and respect, i, rrx ^. ^, ^ A Meng's straight knife force, can fix the upper axial force of the moving magnetic ring (B) and the time-wrenching Wei Er ". 隹 This structure is 4 + ^ ^ 2 ' Because the inclination angle of the inclined surface adjacent to the static magnetic ring (A) and the moving magnetic ring 必需 must be very precise, any point of the kiss must be captured. In addition, the static and dynamic magnetic ring (A, B) between the standing office # ^ ^ A Jing Zichen (A) is divided into two independent individuals, whose magnetic force must be kept the same. It ’s easy to do this, but the two parts are lost to you and the miscellaneous soil P is called the magnetic field (B) and the rotation axis (the rotation of 〇 f to find the sky to balance, that is, it is difficult to reach the moving m ^ ^, Moving and closing P baskets, w balance, so vibration occurs, and the rotational speed of the person with the increase of seismic energy q, so this design is almost non-commercial. Another design system is such as China Minoka 4 丨 丨 ^ Ο Ο π η, 239! I 5, Xi -in () Bu magnetic ring (D) corresponds to the fit on the shaft (F), the two magnetic rings (D, E) are "mounting inside and outside the body Each wall has a corresponding single-, the inner ring wall of the outer magnetic ring 及 and the inner ring: so M — L JL ^ X must, w < the outer% wall is the same pole (such as south ^ ^ its corresponding other ring The wall is the second magnetic field Γ Λ ϊ "The adjacent surfaces of the outer magnetic ring (D, E) generate homopolar repulsion. In addition, the magnetic pole strength on the% wall 壌 magnetic selectivity Γ > The configuration 'such as outer = inner (%) of the inner wall of the clothing (2) has stronger magnetic force near the two end faces, while the middle magnetic (E) is exactly the opposite, and the inner magnetic ring (E), 乂 "produce the orientation and oblique direction. Repulsive force (shown by the arrow in the figure), which can make the inner magnetic ring
第7頁 M253703 3、創作說明（3) (E )懸洋固定於外石放声〆、 之困難，即内磁淨(/;之门中。惟此種設計仍然存在製造上 力強弱之平衡，=门固定完全仰賴環體鄰接面間之磁 分別具有相同強度，且凾#152日日>灿十1丄/> 乂而 定之比例，此對一環开,哀間之對應磁力強度亦保持- 上述幾個磁力強弱常難以達成的，而 發生軸向偏移，故韓= 速懸轉時内磁環⑻會 ;y/A#Pf(F) ^ ^m it(G) 浮狀態，故仍有改L;i…問題，並非完全的懸 【新型内容】 低2ί：即在於提供-種磁浮軸7豕，其可降 度要求，即降低製造成[使其成為可確實 本I]作之另一目的，即在於提供一種磁浮軸承，其可 :ϊ ΐ f f ί狀態，且可達到極佳的動態平衡效果，完全 f:嗨音，震動程度亦可大幅縮減至幾無感覺之程 度、，將热喊之功率消耗降至最低。 ^ =成上述目的，本創作係由一内磁環及一外磁環所對 H ^二=f，其中該外磁環之内環壁之近環體兩端面處係 為弟一極，而第二磁極則配置於内環壁之中央處向外擴 第8頁 M253703 ___ 張延伸g赴 線作JE'固外環壁之梯形區域’使南：!卜；Μ — 深係由環轉 &陶北極間之零界φ 環壁之击 卜而角斜向延伸至内環壁之近中本♦ 之中央處禆盘楚<迎十央處，即内 於外磁環，帷苴1·一石^ ，内磁環之磁性配置則係對猶 區域係為第一磁極：個：環壁向内環壁中央處延伸之梯形 使内外磁π 11 ，内％壁之近兩端面處係為第-磁ώ 磁環可鄰接環壁之近兩端面處形成斜“：；内 且因内ί 斥力之對稱作用而懸4固定於外磁r Ϊ A囚内外磁瑗粼拉了四工山丄名， η又V、乂卜磁被内， 丨兹％郯接裱面中央處形成徑 巧逮旋轉時偏離脫位。 及力了避免磁環於 【實施方式】 百請參閱第四、五圖，其係為本創 合SI，i主，， 卜 < 立體分解圖及组 了看出本創作係由以永久磁鐵製成之一外磁環（） L内磁環(2)所對應套合而成，其中該内磁環(2)^(二 二略小於外磁環（丨）之内徑，使二者之鄰接環壁可保持一二 $間隙’即内磁環（2)係懸浮於外磁環（1)内，而無任何機 卜生接觸’ J--磁環（1，2)之高度相同。至於二磁環（1， 2一）之磁極配置及二者間之磁力作用狀態請參閱第六圖所 不’其中該外磁環（1)之内環壁之近環體兩端面處係為第 、磁區（21)，同為第一磁極（如北極），而第二磁區（12)則 為由内環壁之中央處向外擴張延伸至整個外環壁之梯形區 域，該第二磁區（1 2)配置為第二磁極（如南極，係使第一 與第二磁區（1 1，1 2 )間之零界中心線（1 3 )係由環體之外端 角斜向延伸至内環壁之近中央處，即内環壁之中央處係為 M253703 四、創作說明（5) 第一磁極間；内磁環⑴之極性配置 -磁極’而内環壁之近兩端 ：為： 區(，2)，並配置為第二磁極。-角开A域則為弟四磁 續請參閱第七圖，其係為内外^ ^ ^ ^ ^ ^ ^ ^ ^ ^ 部份放大圖，由於第三磁區（2n命二11、2) 4接壁面處之 心線係為斜向，使得兩磁環(2; :=(22j之零界中 力，該斥力之傾角係= = = :處 :使::=)=水定 ,.,士 ^ / 卜磁玉衣（1 )内，形成靜能孚你 此外，在兩磁環U，2)鄰接環壁 =；；千衡。 f產生徑向吸力，•因環形分布之 抵銷’即在兩磁環（1，2)未有相對運動時，靜態 =因；：抵消而形成平衡狀態，但當内磁環(2)?逹磁 知轉時，錢之磁吸力卻會對内磁環⑴產生牽弓作）=速 :内=(2)因高速旋轉而產生軸向之偏移力時，势 力抵消忒偏移力’形成極佳的軸向固定力，使/及 絕不致偏移脫位。 兹展（2 ) 第八至第十一圖所示者係為本創作 緣之磁場強度實測結果，篦\闰灰al m μ %壁周 士曰私由 ^ ^ 弟八圖為外％壁中央處周緣夕讲 %強度，項數約在負90 0高斯，極性 缘之磁 環壁之近兩端面處之磁場強声 > ° 圖為外 ^ ^ ^ ^ ~強度，讀數約為負5 0 0高斯，成 %強度較中央處弱，極性糸志 · 4 磁 炫l'生為南極，第十圖為内環壁中央肩Page 7 M253703 3. Creation instructions (3) (E) The difficulty of hanging the ocean to fix the sound of the outer stone, that is, the gate of the inner magnetic net (/ ;. However, this design still has a balance of manufacturing strength, = The door is fixed completely depending on the magnetic strength between the adjacent surfaces of the ring body, and the ratio is determined by 凾 # 152 日 日 &;; 灿 十 1 丄 / > ，. This pair of rings is opened, and the corresponding magnetic strength of the sad room is also maintained. -The above-mentioned magnetic strength is often difficult to achieve, and an axial shift occurs, so Han = the inner magnetic ring will meet when the speed is hovering; y / A # Pf (F) ^ ^ m it (G) floating state, so There is still a change L; i ... The problem is not completely hanged [New content] Low 2ί: That is to provide-a type of magnetic levitation shaft 7 其, which can reduce the degree of requirements, that is, reduce the manufacturing to [make it assurable this I] work Another purpose is to provide a magnetic bearing, which can: ϊ ΐ ff ί state, and can achieve excellent dynamic balance effect, complete f: Hi sound, the degree of vibration can also be greatly reduced to almost no sense, , To minimize the power consumption of the hot shout. ^ = For the above purpose, this creation is made by an inner magnetic ring and an outer magnetic ring H ^ = f, where the two ends of the inner ring wall of the outer magnetic ring are near the end of the ring body, and the second magnetic pole is arranged at the center of the inner ring wall to expand outward. Page 8 M253703 ___ Zhang extension g to the line Make JE 'the trapezoidal area of the outer ring wall' to make the south :! bu; M — deep is the ring from the ring & Tao's zero boundary φ ring wall and the angle obliquely extends to the middle of the inner ring wall The central part of this book is Panchu < Welcome to the 10th central part, that is, the inner and outer magnetic rings, 1 苴 1 stone ^. The magnetic configuration of the inner magnetic ring is the first magnetic pole for the Jude area: a: ring wall The trapezoid extending to the center of the inner ring wall makes the inner and outer magnets π 11, and the near two ends of the inner% wall are the first and second magnetic rings. The magnetic ring can be adjacent to the near ends of the ring wall to form an oblique ":; The symmetrical effect of the repulsive force is fixed on the outer magnet r Ϊ A. The inner and outer magnets of the prisoner pull the name of Si Gongshan, η and V and the magnetic quilt are inside. 丨 %% is connected to the center of the mounting surface to form a clever trap. Deviation and dislocation when rotating. Try to avoid the magnetic ring in [Embodiment] Please refer to the fourth and fifth pictures, which are the three-dimensional exploded view and the group of this invention. It can be seen that this creation is made of a corresponding outer magnetic ring () made of a permanent magnet, and an inner magnetic ring (2). The inner magnetic ring (2) ^ (two two is slightly smaller than the outer magnetic ring). (丨) inner diameter, so that the adjacent ring walls of the two can maintain a gap of $ 2, that is, the inner magnetic ring (2) is suspended in the outer magnetic ring (1) without any mechanical contact. J-- The heights of the magnetic rings (1, 2) are the same. As for the arrangement of the magnetic poles of the two magnetic rings (1, 2-1) and the state of the magnetic force between them, please refer to the sixth figure. The two magnetic regions (21) at the two ends of the ring wall near the ring body are the same as the first magnetic pole (such as the North Pole), while the second magnetic zone (12) is extended outward from the center of the inner ring wall. To the trapezoidal region of the entire outer ring wall, the second magnetic region (12) is configured as a second magnetic pole (such as the South Pole, which is the centerline of the zero boundary between the first and second magnetic regions (11, 12)). 1 3) It is obliquely extended from the outer end angle of the ring body to the near center of the inner ring wall, that is, the center of the inner ring wall is M253703 IV. Creation instructions (5) Between the first magnetic poles; Polarity configuration-magnetic pole Near both ends of the wall: is: Area (2), and a second magnetic pole arranged. -The corner open A domain is the fourth magnetic continuation. Please refer to the seventh figure, which is inside and outside. The center line at the wall surface is oblique, so that the two magnetic rings (2;: = (the middle force of the zero boundary of 22j, the angle of repulsion of the repulsive force = = = ::::: =) = 水 定,., Shi ^ / Bu magnetic jade clothing (1), the formation of static energy Fu You In addition, the two magnetic rings U, 2) adjacent to the ring wall =; f produces radial suction, • due to the offset of the annular distribution 'that is, when the two magnetic rings (1, 2) have no relative movement, static = due to :: the equilibrium state is formed, but when the inner magnetic ring (2)?知 When the magnetic rotation is known, the magnetic attraction of Qian will cause a pull bow to the inner magnetic ring）) = Speed: Internal = (2) When the axial offset force is generated due to high-speed rotation, the force offsets the offset force. Develops excellent axial fixing force, so that it will never be dislocated. (2) The eighth to eleventh pictures are based on the actual magnetic field strength measurement results of the creative origin. 篦 \ 闰 灰 al m μ% wall Zhou Shiyue private reason ^ ^ The eighth figure is the center of the outer% wall Peripheral perimeter speaks% intensity, the number of terms is about minus 90 0 Gauss, strong magnetic field near the two ends of the magnetic ring wall of the polar edge > ° The picture shows the outer ^ ^ ^ ^ ~ intensity, the reading is about minus 5 0 0 Gauss,% strength is weaker than the center, the polarity is 糸. 4 magnetic dazzle l 'is born to the South Pole, the tenth picture is the central shoulder of the inner ring wall
M253703 四、創作說明（6)M253703 IV. Creation Instructions (6)
之磁場強度，讀數約為負3 0 0高斯，極性為南極；第十一 圖則為内環壁近兩端面處之磁場強度，讀數約為正3 0 0高 斯，即略與中央處之磁場強度相同，但極性為北極。以上 所述之磁場強度數值僅為一較佳實施例，其數值大小及強 弱關係並非固定不變，而係配合實際應用場合所需之徑向 及轴向固定力之大小而加以調整。而由此實測之數據即可 證明本創作之磁性配置乃確實可實施者，且在實際裝設於 散熱風扇中，亦確實不產生任何噪音，震動程度亦低於人 體可感覺之範圍，遠低於習用機械式軸承及磁浮軸承，實 為一極優異之設計。The magnetic field strength is about negative 300 Gauss, with the polarity being the South Pole. Figure 11 shows the magnetic field strength at the near ends of the inner ring wall. The reading is about 300 Gauss, which is slightly different from the central magnetic field. The intensity is the same, but the polarity is North Pole. The magnetic field strength value described above is only a preferred embodiment, and the magnitude and strength relationship are not fixed, but are adjusted according to the radial and axial fixing forces required for practical applications. The measured data can prove that the magnetic configuration of this creation is indeed implementable, and it is actually installed in the cooling fan, and it does not generate any noise, and the vibration level is lower than the human sensible range, which is far lower. The mechanical bearings and magnetic bearings used in practice are an excellent design.
第11頁 M253703 圖式簡單說明 第一圖 第二圖 第三圖 第四圖 第五圖 第六圖 第七圖 第八圖 圖。 第九圖 實測圖 第十圖 圖。 第十一圖：本創作之磁 度實測圖。 每每内環壁近兩端 習用磁浮軸承之縱向剖視圖。 另一習用磁浮軸承之縱向剖視圖。 第二圖之立體分解圖。 本創作之立體分解圖。 本創作之立體組合圖。 本創作之縱向剖視圖。 第七圖之局部放大圖。 本創作之磁環外環壁令央處周緣之磁場強度實測 本創作之磁環外環壁近兩端面處周緣之磁場強度 本創作之磁環内環中處 n緣之礤場強度實測 面處周緣之磁場強 元件代表符號 習知部份： A· · ·靜磁環 C · · ·轉轴 E · · ·内磁環 G. · ·阻環 B· · ·動磁環 D· ·.外磁環 F·..轉軸 本創作部份： 第12頁 M253703 圖式簡單說明 1.. .外磁環 12.. .第二磁區 2.. .内磁環 22.. .第四磁區 11.. .第一磁區 13.. .零界中心線 21.. .第三磁區 2 3…零界中心線P.11 M253703 Brief description of the drawings The first picture The second picture The third picture The fourth picture The fifth picture The sixth picture The seventh picture The eighth picture The ninth figure measured map tenth figure. Figure 11: The measured magnetic map of this creation. Longitudinal sectional views of magnetic levitation bearings used at the near ends of the inner ring wall. A longitudinal sectional view of another conventional magnetic bearing. An exploded perspective view of the second figure. A three-dimensional exploded view of this creation. A three-dimensional combination of this creation. Vertical section view of this creation. Partial enlarged view of the seventh figure. The magnetic field strength at the periphery of the central part of the magnetic ring of this creation is measured. The magnetic field strength at the periphery of the magnetic ring at the near ends of the outer ring wall of this creation. The magnetic field strong component around the periphery represents the symbol familiar part: A · · · Magnetostatic ring C · · · Rotary shaft E · · · Internal magnetic ring G. · · Resistance ring B · · · Moving magnetic ring D · · Outer Magnetic ring F ... Spinner This part of the creation: Page 12 M253703 Brief description of the diagram 1. Outer magnetic ring 12 .. Second magnetic zone 2. Inner magnetic ring 22. Fourth magnetic zone 11. .. first magnetic zone 13. .. zero boundary center line 21. .. third magnetic zone 2 3… zero boundary center line
第13頁Page 13