TW200930899A - Cooling apparatus - Google Patents
Cooling apparatus Download PDFInfo
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- TW200930899A TW200930899A TW097135215A TW97135215A TW200930899A TW 200930899 A TW200930899 A TW 200930899A TW 097135215 A TW097135215 A TW 097135215A TW 97135215 A TW97135215 A TW 97135215A TW 200930899 A TW200930899 A TW 200930899A
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- piezoelectric vibrator
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- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06F—ELECTRIC DIGITAL DATA PROCESSING
- G06F1/00—Details not covered by groups G06F3/00 - G06F13/00 and G06F21/00
- G06F1/16—Constructional details or arrangements
- G06F1/20—Cooling means
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F04—POSITIVE - DISPLACEMENT MACHINES FOR LIQUIDS; PUMPS FOR LIQUIDS OR ELASTIC FLUIDS
- F04D—NON-POSITIVE-DISPLACEMENT PUMPS
- F04D33/00—Non-positive-displacement pumps with other than pure rotation, e.g. of oscillating type
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L23/00—Details of semiconductor or other solid state devices
- H01L23/34—Arrangements for cooling, heating, ventilating or temperature compensation ; Temperature sensing arrangements
- H01L23/46—Arrangements for cooling, heating, ventilating or temperature compensation ; Temperature sensing arrangements involving the transfer of heat by flowing fluids
- H01L23/467—Arrangements for cooling, heating, ventilating or temperature compensation ; Temperature sensing arrangements involving the transfer of heat by flowing fluids by flowing gases, e.g. air
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- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05K—PRINTED CIRCUITS; CASINGS OR CONSTRUCTIONAL DETAILS OF ELECTRIC APPARATUS; MANUFACTURE OF ASSEMBLAGES OF ELECTRICAL COMPONENTS
- H05K7/00—Constructional details common to different types of electric apparatus
- H05K7/20—Modifications to facilitate cooling, ventilating, or heating
- H05K7/20009—Modifications to facilitate cooling, ventilating, or heating using a gaseous coolant in electronic enclosures
- H05K7/20136—Forced ventilation, e.g. by fans
- H05K7/20172—Fan mounting or fan specifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L2924/00—Indexing scheme for arrangements or methods for connecting or disconnecting semiconductor or solid-state bodies as covered by H01L24/00
- H01L2924/0001—Technical content checked by a classifier
- H01L2924/0002—Not covered by any one of groups H01L24/00, H01L24/00 and H01L2224/00
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- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Physics & Mathematics (AREA)
- Theoretical Computer Science (AREA)
- General Physics & Mathematics (AREA)
- General Engineering & Computer Science (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Mechanical Engineering (AREA)
- Computer Hardware Design (AREA)
- Power Engineering (AREA)
- Human Computer Interaction (AREA)
- Thermal Sciences (AREA)
- Structures Of Non-Positive Displacement Pumps (AREA)
- Cooling Or The Like Of Electrical Apparatus (AREA)
- Cooling Or The Like Of Semiconductors Or Solid State Devices (AREA)
Abstract
Description
200930899 九、發明說明: 【發明所屬之技術領域】 本發明係關於為將電子機器内部之熱朝電子機器外部排 出之使用壓電風扇之冷卻裝置。 . 【先前技術】 • 近年,特別是攜帶型電子機器,隨著小型化與構件之高 挽度安裝化之進展,電子機器内部之熱對策已成為課題。 作為前述課題特別重要之攜帶型電子機器之一例,可舉 攜帶型個人電腦為例。攜帶型個人電腦中,致力於小型化 之技術開發之同時,為提高資訊處理力之cpu之高速化亦 在進展。因此,構件之高密度安裝造成電子機器内部之通 風性直線下降,因CPU之發熱量增大,將該熱量朝電子機 器外部排出以抑制電子機器内部之溫度上昇益發困難。 先如與發熱體之發熱部接連之散熱器空出所要之間隔 並設之多數散熱片之間介有空氣包含構造之可動片,旋轉 Q 或擺動該可動片以朝散熱片間送入冷氣,排出散熱片間之 暖氣般之放熱器如專利文獻1所示。 另方面,具有含有壓電振動子之出風振動子,排氣口 與吸氣口設於同一面而構成之壓電風扇揭示於專利文獻 2。該壓電風扇’如夹住出風振動子之兩側般,設有從箱 本體之開口部向内側延長之一對隔板,該各隔板與箱本體 之兩側部之間之開口形成為吸氣口,夾住兩隔板所成之開 口形成為排氣口。 此處’對專利文獻2之屢電風扇之構成,基於圖!進行說 134432.doc 200930899 明。圖1中,虔電風扇i,於形成為偏平箱狀之風扇箱2内 藏由壓電振動子3與出風振動子4所構成之風扇本體5,於 風扇箱2之同一面形成吸氣口 6(6A、6B)與排氣口 7。風扇 箱2係由具有底面部8a、左右兩側面部8b、8c及背面部8d • 且於前面部成為開放之方式所形成之箱本體8與於該箱本 . 體8之上面氣密性固著之平板狀蓋體9所構成。 [專利文獻1]日本實開平〇2_127796號公報 φ [專利文獻2]日本特開20〇2-3;39900號公報 【發明内容】 [發明所欲解決之問題] 但,前述攜帶型電子機器中,若直接使用如專利文獻i 之放熱器,從小型化之觀點而言並不適宜。因&,考慮取 代該專利文獻I之可動片,而使用如專利文獻2所示之麼電 風扇。 使用塵電風扇時,其出風能力雖依存於出風振動子中之 ® Μ電振動子之變位量,但壓電振動子之變位量並 文獻1之可動片之動作量大。 ,因此’有必要考慮盡量高效率地進行電子機器内部之冷 卻。專利文獻2中記述,兩隔板間之間隔,基本而言盡量 、接,出風板之寬度,即以盡量縮小兩隔板與出風板:間隙 為宗旨。 ' 用以將專利文m之放熱器之散熱片間之暖氣排出 動片,即使存在㈣於可動片動作之空氣“,目 如電動機之強力驅動源旋轉或擺動’故可動片之動作並不 134432.doc 200930899 會因空氣阻力之影響而被阻礙,而使用專利文獻2之壓電 風扇之出風振動子’若相當於兩隔板之散熱片間之間隔與 出風板之寬度接近’則將因出風振動子之動作所產生之空 氣阻力而阻礙變位。200930899 IX. Description of the Invention: [Technical Field] The present invention relates to a cooling device using a piezoelectric fan for discharging heat inside an electronic device to the outside of the electronic device. [Prior Art] In recent years, in particular, portable electronic devices have become a subject of thermal countermeasures within electronic devices as miniaturization and high-profile installation of components have progressed. An example of a portable electronic device that is particularly important as the above-mentioned problem is a portable personal computer. In the portable personal computer, the development of technology for miniaturization is progressing, and the speed of cpu for improving information processing is progressing. Therefore, the high-density mounting of the member causes the ventilating property inside the electronic device to drop linearly, and the heat generated by the CPU is increased, and the heat is discharged to the outside of the electronic device to suppress the temperature rise inside the electronic device. First, if the heat sink connected to the heat generating portion of the heating element is vacated, and a plurality of heat sinks are provided with a movable piece containing air, the rotating piece Q or the movable piece is sent to send cold air between the heat sinks. A radiator-like radiator that discharges between the fins is as shown in Patent Document 1. On the other hand, a piezoelectric fan having an outlet vibrator including a piezoelectric vibrator and an exhaust port and an intake port provided on the same surface is disclosed in Patent Document 2. The piezoelectric fan is provided with a pair of partitions extending inward from the opening of the box body, such as sandwiching the two sides of the wind vibrator, and the openings between the partitions and the two sides of the box body are formed. For the suction port, the opening formed by sandwiching the two partitions is formed as an exhaust port. Here, the composition of the electric fan of Patent Document 2 is based on the figure! Said 134432.doc 200930899 Ming. In Fig. 1, a fan fan i houses a fan body 5 composed of a piezoelectric vibrator 3 and an outlet vibrator 4 in a fan case 2 formed in a flat box shape, and forms an air suction on the same side of the fan case 2. Port 6 (6A, 6B) and exhaust port 7. The fan case 2 is made of a case body 8 having a bottom surface portion 8a, left and right side surface portions 8b and 8c, and a back surface portion 8d, and is opened at the front surface portion, and is airtight on the upper surface of the box body 8. The flat cover 9 is formed. [Patent Document 1] Japanese Laid-Open Patent Publication No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. If the radiator of Patent Document i is used as it is, it is not suitable from the viewpoint of miniaturization. In view of &, it is considered to replace the movable piece of Patent Document 1, and an electric fan as shown in Patent Document 2 is used. When a dust electric fan is used, the air blowing capacity depends on the displacement amount of the ® 振动 electric vibrator in the wind vibrator, but the displacement amount of the piezoelectric vibrator and the movable piece of the document 1 are large. Therefore, it is necessary to consider the cooling of the inside of the electronic machine as efficiently as possible. Patent Document 2 describes that the interval between the two separators is basically as close as possible to the width of the air outlet plate, that is, to minimize the two partition plates and the air outlet plate: the gap. 'The heat is used to discharge the heat between the heat sinks of the radiator of the patent, even if there is (4) the air moving in the movable piece ", such as the strong driving source of the motor rotates or oscillates", the action of the movable piece is not 134432 .doc 200930899 will be hindered by the influence of air resistance, and the wind vibrator of the piezoelectric fan of Patent Document 2 will be 'if the interval between the fins of the two partitions is close to the width of the air outlet plate' The displacement is hindered by the air resistance generated by the action of the wind vibrator.
此處’根據本案之發明者實驗所得之出風板(以下稱 「葉片」)前端之振幅與空氣阻力之關係如圖2所示。得出 忒結果之壓電振動子之尺寸為6 mmxl2 mm,葉片之尺寸 為6 mmxl8 mmx40 μηι,兩者以短邊部分彼此接合。 因考慮到空氣阻力與空氣密度基本成比例,空氣密度與 氣壓成比例,故該實驗藉由於特定之減壓環境下之葉片由 壓電振動子驅動時之氣壓與葉片前端之振幅調查而進行。 如圖2所不’帛片之振幅受到氣壓,即空氣阻力之影響, 空氣阻力越大振幅越小。 如此,即使使相當於兩隔板之散熱片間之間隔與葉片之 寬度盡量接近’亦將因葉片之動作所產生之空氣阻力而阻 礙變位’而存在有反而難以增大葉片之振幅之問題。 因此,本發明之目的,在於提供一 大葉片之振幅以提高送風能力,另, 熱效果以使冷卻能力提升 [解決問題之技術手段] 種冷卻裝置,其可增 提高來自散熱片之散 因該待排出之暖氣係由散熱片之發熱 久/71停 1¾溫部分华 者,故散熱片間之空間之溫度分布並不均 中於散熱片之壁面附近。 另 考慮散熱片間空氣流動時之流速分布 雖散熱片間 134432.doc 200930899 之中央。P空氣之流速快,但因相對於散熱片之壁面存在空 氣之粘性阻力,故越接近散熱片之壁面流速越慢。 即,僅單純於散熱片間使空氣流動,則存在於散熱片間 之中央部之溫度相對較低之空氣雖被排出,但存在於散熱 • 片之壁面附近之高溫之暖氣卻未被充分排出。 、 本發明之發明者們從各種各樣之實驗及模擬中發現,無 論散熱片間之空氣是否全部由葉片排出,若藉由掃除散熱 ❹ 4之壁面附近之暖氣般使f片動作,使暖氣向散熱片間之 中央部移動,以使暖氣易於排出,就可充分高效地將電子 機器内部之熱向電子機器外部排出。 因此,本發明如下所述構成。 (1)由具備根據電壓施加而彎曲之壓電振動子與接著於或 -體化於該壓電振動子藉由前述壓電振動子而擺動之葉片 之壓電風扇’與具備至少2片散熱片之散熱器構成, 前述葉片,形成為從前述壓電振動子延伸之長條狀,並 ❿ ⑨不抵接於前述散熱片且於鄰接散熱片間之空間擺動之位 置配置前述壓電振動子及前述葉片, 於則述葉片設有開口部或缺口部。 藉由該構造,因開口部或缺口部而減少空氣阻力,增大 ' U之振幅。即使開口部或缺口部所造成之整體之出風量 降低,散熱片之壁面附近之暖氣之掃除效果亦不會降低, 伴隨振中田之增大亦將提高整體之冷卻能力。此外,因散轨 片之壁面附近之暖氣流剝離而向中央部方向波浪般流動y 散熱片附近之暖氣優先掃除,故散熱效果將提高,冷卻能 134432.doc 200930899 力將提升。 (2) 則述葉片之遠離前述壓電振動子側之前端部或前端附 近亦可設有配重。 藉由該構造,因配重而使慣性力矩增大,以包含配重之 . 葉片之共振頻率驅動,藉此葉片之振幅將增大。因此,冷 卻能力將提高。 (3) 前述葉片亦可將前述長條之長度方向短縮化般為曲折 形狀。 藉由該構造’葉片之全長將增長,振幅將增大。因此, 冷卻能力將提高。 (4) 前述壓電振動子將前述葉片之端部從兩面夾住般配 置’亦可將則述壓電振動子及前述葉片構成為雙壓電晶片 型振動子。 藉由該構成,相對於施加電壓之彎曲變位量將增大,葉 片之振幅將增大。因此’冷卻能力將進一步提高。 , (5)對於前述散熱片亦可於該散熱片之側壁間於空氣流動 方向設置產生氣流之風扇。 藉由該構成,因開口部或缺口部之存在而使散熱片之壁 面附近之暖氣流剝離向中央部方向波浪般流動之暖氣藉由 另設之風扇高效率流出,整體之冷卻能力將提高。 (6)前述開口部沿前述葉片之長度方向為長形狀,從前述 葉片之長度方向之邊至與該邊平行之前述開口部之邊之尺 寸,比前述散熱片與前述葉片之間之間隙尺寸大。 由此,可得到更高冷卻能力。 134432.doc 200930899 [發明效果] 根據本發明’葉片之振幅將增大進而冷卻能力將提 高。另,與之同時來自散熱片之散熱欵果將提高進而冷 卻能力將提升。 • 【實施方式】 . «第1實施形態》 圖3係第1實施形態之冷卻裝置所使用之壓電風扇之立 ❿ «。圖3中之壓電風扇Μ,由具有開口部22之葉片21及 壓電振動子2G構成。壓電振動子2(),係於作為中間電極 之金屬板之兩面配置壓電元件所構成雙壓電晶片型之壓 電振動子。即,作為該壓電振動子2〇之中間電極之金屬 板之兩側之壓電元件’於各自之表面形成電極膜,該等 之電極與作為中間電極之金屬板之間,藉由施加對應壓 電元件之分極方向之驅動電壓進行分極處理⑽長度方 向(L1尺寸方向)彎曲以進行彎曲振動。 _ 帛片21係相對於不錄鋼板貫通矩形狀之開口部22者, 其端部接著於壓電振動子2〇之端部。 圖3所示之壓電風仙之各部尺寸如下所述。 L1 : 12 mm * L2 : 18 mm W : 6 mm t : 50 μιη 另’開口部22之尺卄皂μ ^ 兩12 mmx2 mm ’其靠近根部之端 部重合於壓電振動子2〇之端部。 134432.doc -11 - 200930899 圖4(A)係圖3所示之壓電風扇31配置於散熱器之特定位 置所構成之冷卻裝置之主要部之立體圖。散熱器中如圖4 所不之複數之散熱片30彼此平行突出,鄰接之散熱片3〇 間使壓電風扇31之葉片21不抵接於散熱片30而擺動般配 置麗電風扇31。 圖4(B)係從散熱片之延伸方向(與送風方向對面之方 向)所見之冷卻裝置整體之正面圖。 散熱器40具備彼此平行延伸之複數之散熱片3〇。該例 中於電路基板120之上部安裝CPU等發熱體(發熱構 件)110,於該11 〇之上面熱性結合般配置散熱器之底 面。 如此藉由散熱器40與複數之壓電風扇31構成冷卻裝置 100 ° 圖5係關於圖3、圖4所示之壓電風扇31之葉片21所設之 開口部22之有無及散熱片3〇之有無所產生之葉片前端之 振幅變化之示意。 如此若於葉片之兩側存在散熱片則與作為開放空間之 情形相比葉片前端之振幅將減少。例如關於輸入電壓3〇 V且無開口部之情形進行比較,相對於無散熱片之情形 下葉片前端之振幅為9.2 mm,存在散熱片時葉片前端之 振幅減少至5.5 mm。但,藉由設置開口部22可使葉片前 端之振幅增大至7.5 mm。 此係因為,藉由開口部22之存在’擺動葉片21之實質 性面積被削減,另經由如後所述之開口部22改善抽取空 134432.doc 12 200930899 氣,空氣阻力相應減少。 藉由如此於葉片設開口部22,可知即使於散熱片間之 空間内亦可以比較大之振幅擺動葉片。 ❹ ❹ 圖6係關於設於葉片21之開口部22之效果之示意圖1 電風扇3!以壓電振動子2〇之支持部(圖中左端)為中以 葉片2!於圖中所示之箭頭u、d方向擺動。藉此,散熱片 3 0所夾住之空間内之空氣成為如箭頭A f所示之氣流進行 流動。此時,亦產生從上方向下方、及從下方向上 過開口部22之氣流,與流動於葉片21之上面側及下面側 Μ流混合。另,與此㈣,散熱片30之壁面附近之暖 氣流於葉片之側端緣剝離’該暖氣向開口部22之方向, 即向2片鄰接之散熱片3〇夹 ° 11王之二間内之中央部方向流 動。 如部22並非僅僅減少空氣阻力增大葉片η之振 幅、、剝離散熱片30之壁面附近之暖氣流之同時,與以 二接:散熱片3〇所夹住之空間内之整體氣流一起掃除至 外口Ρ般作用。(以下,今作田从田 ’、 .^ ”作用政果稱為「掃除效果」)因Here, the relationship between the amplitude of the front end of the air outlet plate (hereinafter referred to as "blade") obtained by the inventor of the present invention and the air resistance is as shown in Fig. 2. The resulting piezoelectric vibrator has a size of 6 mm x 12 mm and a blade size of 6 mm x 18 mm x 40 μη, which are joined to each other by short sides. Since the air resistance is substantially proportional to the air density and the air density is proportional to the air pressure, the experiment was carried out by investigating the air pressure when the blade is driven by the piezoelectric vibrator in a specific decompression environment and the amplitude of the tip of the blade. As shown in Fig. 2, the amplitude of the cymbal is affected by the air pressure, that is, the air resistance. The larger the air resistance, the smaller the amplitude. In this way, even if the interval between the fins corresponding to the two spacers is as close as possible to the width of the blade, the displacement will be hindered by the air resistance generated by the action of the blade, and there is a problem that it is difficult to increase the amplitude of the blade. . Therefore, the object of the present invention is to provide a large blade amplitude to improve the air blowing capability, and a thermal effect to improve the cooling capacity [technical means for solving the problem] a cooling device which can increase the dissipation factor from the heat sink. The heat to be discharged is heated by the heat sink for a long time / 71 stops 13⁄4 temperature part, so the temperature distribution of the space between the heat sinks is not even near the wall surface of the heat sink. Also consider the flow velocity distribution when the air flows between the fins, although the center of the heat sink is 134432.doc 200930899. The flow rate of P air is fast, but since there is viscous resistance of air relative to the wall surface of the heat sink, the flow velocity toward the wall surface of the heat sink is slower. That is, only the air flowing between the fins is simply discharged, and the air having a relatively low temperature in the central portion between the fins is discharged, but the high-temperature heater existing near the wall surface of the fins is not sufficiently discharged. . The inventors of the present invention have found from various experiments and simulations that regardless of whether or not the air between the fins is completely discharged by the vanes, if the heat is applied to the vicinity of the wall surface of the heat sink 4, the heating is performed. By moving to the center portion between the fins so that the heater is easily discharged, the heat inside the electronic device can be efficiently and efficiently discharged to the outside of the electronic device. Therefore, the present invention is constructed as follows. (1) A piezoelectric fan having a piezoelectric vibrator that is bent according to a voltage application and a blade that is or is oscillated by the piezoelectric vibrator to be oscillated by the piezoelectric vibrator, and having at least two heat sinks In the heat sink of the sheet, the blade is formed in a strip shape extending from the piezoelectric vibrator, and the piezoelectric vibrator is disposed so as not to abut against the fin and oscillate in a space between adjacent fins. And the blade, wherein the blade is provided with an opening or a notch. With this configuration, the air resistance is reduced by the opening or the notch, and the amplitude of 'U is increased. Even if the overall air volume caused by the opening or the notch is lowered, the effect of cleaning the heater near the wall surface of the heat sink is not lowered, and the overall cooling capacity is improved with the increase of the vibration field. In addition, since the heating flow near the wall surface of the loose rail piece is peeled off and flows toward the center portion, the heat in the vicinity of the heat sink is preferentially removed, so that the heat dissipation effect is improved, and the cooling energy is increased by 134432.doc 200930899. (2) A weight may be provided in the vicinity of the front end or the front end of the blade away from the piezoelectric vibrator side. With this configuration, the moment of inertia is increased by the weight, and is driven by the resonance frequency of the blade including the weight, whereby the amplitude of the blade is increased. Therefore, the cooling capacity will increase. (3) The blade may have a zigzag shape in which the longitudinal direction of the long strip is shortened. With this configuration, the full length of the blade will increase and the amplitude will increase. Therefore, the cooling capacity will increase. (4) The piezoelectric vibrator is disposed such that the end portions of the vanes are sandwiched from both sides. The piezoelectric vibrator and the vane may be formed as a bimorph type vibrator. With this configuration, the amount of bending displacement with respect to the applied voltage will increase, and the amplitude of the blade will increase. Therefore, the cooling capacity will be further improved. (5) For the heat sink, a fan that generates an air flow may be disposed between the sidewalls of the heat sink in the air flow direction. According to this configuration, the heating flow in the vicinity of the wall surface of the fin is separated by the presence of the opening or the notch, and the heater that flows in a wave direction toward the center portion flows out efficiently by the additional fan, and the overall cooling capacity is improved. (6) The opening portion has a long shape along the longitudinal direction of the blade, and a dimension from a side in a longitudinal direction of the blade to a side of the opening parallel to the side is larger than a gap between the fin and the blade Big. Thereby, a higher cooling capacity can be obtained. 134432.doc 200930899 [Effect of the Invention] According to the present invention, the amplitude of the blade will increase and the cooling ability will be improved. In addition, at the same time, the heat dissipation results from the heat sink will increase and the cooling capacity will increase. [Embodiment] «First Embodiment" Fig. 3 is a diagram of a piezoelectric fan used in a cooling device according to the first embodiment. The piezoelectric fan 图 in Fig. 3 is composed of a blade 21 having an opening 22 and a piezoelectric vibrator 2G. The piezoelectric vibrator 2() is a bimorph type piezoelectric vibrator in which piezoelectric elements are arranged on both surfaces of a metal plate as an intermediate electrode. That is, the piezoelectric element 'on both sides of the metal plate as the intermediate electrode of the piezoelectric vibrator 2' forms an electrode film on each surface, and the electrode is applied to the metal plate as the intermediate electrode by applying a corresponding The driving voltage in the polarization direction of the piezoelectric element is subjected to polarization processing (10) bending in the longitudinal direction (L1 dimensional direction) to perform bending vibration. The cymbal sheet 21 is formed so as to penetrate the rectangular opening portion 22 with respect to the non-recorded steel sheet, and the end portion thereof is followed by the end portion of the piezoelectric vibrator 2 . The dimensions of the respective portions of the piezoelectric fan shown in Fig. 3 are as follows. L1 : 12 mm * L2 : 18 mm W : 6 mm t : 50 μιη Another 'opening 22's 卄 soap μ ^ 2 12 mmx2 mm 'The end near the root coincides with the end of the piezoelectric vibrator 2〇 . 134432.doc -11 - 200930899 Fig. 4(A) is a perspective view showing the main part of the cooling device in which the piezoelectric fan 31 shown in Fig. 3 is disposed at a specific position of the heat sink. In the heat sink, a plurality of fins 30 as shown in Fig. 4 are protruded in parallel with each other, and the adjacent fins 3 are arranged such that the blades 21 of the piezoelectric fan 31 do not abut against the fins 30, and the electric fan 31 is arranged in a swinging manner. Fig. 4 (B) is a front view of the entire cooling device as seen from the direction in which the fins extend (the direction opposite to the blowing direction). The heat sink 40 is provided with a plurality of fins 3 延伸 extending in parallel with each other. In this example, a heat generating body (heat generating member) 110 such as a CPU is mounted on the upper portion of the circuit board 120, and the bottom surface of the heat sink is disposed on the upper surface of the 11 〇. Thus, the heat sink 40 and the plurality of piezoelectric fans 31 constitute a cooling device 100°. FIG. 5 is the presence or absence of the opening 22 provided in the blade 21 of the piezoelectric fan 31 shown in FIGS. 3 and 4, and the heat sink 3〇. The presence or absence of an indication of the amplitude variation of the leading end of the blade. Thus, if there are fins on both sides of the blade, the amplitude of the tip of the blade will be reduced as compared with the case of an open space. For example, when the input voltage is 3 〇 V and there is no opening, the amplitude of the tip of the blade is 9.2 mm with respect to the case without the fin, and the amplitude of the tip of the blade is reduced to 5.5 mm when the fin is present. However, by providing the opening portion 22, the amplitude of the leading end of the blade can be increased to 7.5 mm. This is because the substantial area of the oscillating vane 21 is reduced by the presence of the opening portion 22, and the extraction air is improved by the opening portion 22 as will be described later, and the air resistance is correspondingly reduced. By providing the opening portion 22 in the blade as described above, it is understood that the amplitude swinging blade can be relatively large even in the space between the fins. Fig. 6 is a schematic view showing the effect of the opening portion 22 provided on the blade 21; the electric fan 3! The support portion (the left end in the figure) of the piezoelectric vibrator 2 is the middle blade 2; The arrows u and d oscillate. Thereby, the air in the space sandwiched by the fins 30 flows as the air flow indicated by the arrow A f. At this time, the airflow passing through the opening 22 from the upper side to the lower side and from the lower side is also turbulently mixed with the upper side and the lower side of the blade 21. In addition, (4), the heating flow near the wall surface of the heat sink 30 is separated from the side edge of the blade, and the heating is directed toward the opening portion 22, that is, the two adjacent heat sinks 3 are sandwiched between the two kings. The direction of the central part flows. The portion 22 is not only reduced in the air resistance to increase the amplitude of the blade η, but also in the vicinity of the wall surface of the heat sink 30, and is removed together with the overall airflow in the space sandwiched by the heat sink 3〇. The external mouth is like a role. (Here, the current work of the field from the field ‘, .^ ” is called “sweeping effect”
此可提尚散熱效果。 」JU 圖7係為說明具備設有開 之圖。圖7中亮度低之#片之麗電風扇之作用 高, 低之分為低溫區域,亮度高之部分為 肉,孤(he场〇 v 為求得圖4所示構造之冷 間之氣流之溫度分布雖有、㈣S熱片間之空 廇大有要進行3維模擬,但因計算量 龐大,此處替換為2维模擬。 134432.doc 200930899 圖=)係鄰接之2片散熱片3。、3〇昇至特定高溫之同 ,〜散熱片3G彼此所夾住之空間内,於时從 右方向流動特定溫度之冷風之情形之溫度分布之示音〇 如此於散熱片30彼此夾住之空間内流; 流,則越靠近空間之中央部产这抵… 為層 T兴机逮越大,散熱片30之壁面 因空氣之枯性阻力理論上流速為〇。因此從左端流… 風經過散熱片30彼此所夾住之空間内之中央部仍舊為二This can improve the heat dissipation effect. Fig. 7 is a diagram showing the presence of an opening. In Fig. 7, the low-intensity #片丽丽电风扇 has a high effect, and the low part is divided into a low temperature region, and the high-brightness portion is meat, and the so-called (he field 〇v is the airflow of the cold space constructed as shown in Fig. 4). Although the temperature distribution is (4), the space between the S-hot sheets is large, and the 3D simulation is required. However, due to the large amount of calculation, the two-dimensional simulation is replaced here. 134432.doc 200930899 Figure =) Two fins 3 adjacent to each other. The sound distribution of the temperature distribution in the case where the heat sink 3G is in the space sandwiched by the heat sink 3G and the cold air flowing at a specific temperature from the right direction is thus sandwiched between the heat sinks 30. The flow in the space; the flow is closer to the central part of the space. This is the case. For the layer T, the wall surface of the heat sink 30 is theoretically flowable due to the dry resistance of the air. Therefore, the flow from the left end... The central portion of the space in which the wind passes through the heat sink 30 is still two
風流向右端方向之量較多,散熱片30之散熱效果低/ 7 圖7⑻’係近接於散熱片3〇之壁面之柴ρ於圖中左右方 向振動之情形之溫度分布之示意。其他條件與㈧之情形 相同。該計,係相當於圖4所示之葉片21中開口部^之 兩側部之部位者。 如此分布於散熱片30之壁面之暖氣(高溫空氣層)向空 間之中央部波浪般流動以隨著流過整個空間内之氣流而 被掃除。因此可提高整體之散熱效果。 «第2實施形態》 第1實施形態中相對於葉片21形成於葉片之長度方向延 伸之單一開口部22,但圖8係關於與之不同之2種構成之 壓電風扇之示意。 圖8(A)之例,係為於葉片21之前端部(遠離壓電振動子 2〇側)’形成有於葉片21之長度方向延伸之缺口部23之壓 電風扇32之不意。該圖8(Α)所示之構造,開口部之位置 亦可為配置於葉片21之前端部。如此即使於葉片21之前 端部形成缺口部23亦可因空氣阻力之減少得到葉片2丨之 134432.doc 14· 200930899 振幅增大效果及散熱片壁面之高溫空氣之掃除效果。 圖8(B)之例’係形成複數之開口部22a〜22d之葉片21接 合於壓電振動子20構成壓電風扇33者。 與該等葉片21相對之開口部之位置及數量所產生之作 • 用效果差異如下所述。 , 首先,如圖3所示,開口部22靠近葉片之根部(壓電振 動子20側)形成之情形,因開口部22存在於葉片21之擺動 φ 時變位小之處所,故空氣阻力之減少效果小,葉片21之 振幅增大效果小,但葉片21前端部之空氣之押出效果未 因開口部而損耗故送風性高。 另一方面,若如圖8(A)般缺口部23形成於葉片21之前 端部附近(或開口部形成於前端部附近),則空氣阻力之 減少效果高而葉片21之振幅增大。因此散熱片壁面之高 溫空氣之掃除效果增大。但因從葉片前端部之氣流之押 出效果下降故送風性下降。 〇 因如此般送風性與掃除效果某種程度上為折衷關係, 故以得到最高冷卻能力之方式確定開口部之形狀、位 置、大小即可。 此外,即使如圖8(B)般開口部設置複數個之情形,該 等開口部之大小、形成位置、數量等係考慮前述送風性 與掃除效果加以決定。 另’開口部形成於葉片之根部(壓電振動子2〇側)附近 之情形,雖葉片21之彎曲應力使相對較大之位置之實質 性寬度變小,但藉由使開口部22為不於葉片21之寬方向 134432.doc -15- 200930899 而於長度方向延伸之形狀,可緩和彎曲應力之集中,確 保長期驅動時之信賴性。 «第3實施形態》 圖9係第3實施形態之冷卻裝置所使用之壓電風扇之立 體圖。該例係藉由形成開口部22,前端部具備配重24a、 24b之葉片21及壓電振動子20構成壓電風扇34。The amount of wind flow to the right end is large, and the heat sink 30 has a low heat dissipation effect. 7 Fig. 7(8)' is a schematic representation of the temperature distribution of the case where the wall of the heat sink 3 is vibrated in the left and right directions in the figure. Other conditions are the same as in (8). This is equivalent to the portion on both sides of the opening portion ^ in the blade 21 shown in Fig. 4 . The heat (high-temperature air layer) thus distributed on the wall surface of the heat sink 30 flows toward the center of the space to be swept away as it flows through the air flow in the entire space. Therefore, the overall heat dissipation effect can be improved. «Second Embodiment" In the first embodiment, the single opening 22 extending in the longitudinal direction of the blade is formed with respect to the blade 21. However, Fig. 8 is a schematic view of a piezoelectric fan having two different configurations. In the example of Fig. 8(A), the piezoelectric fan 32 having the notch portion 23 extending in the longitudinal direction of the blade 21 is formed at the front end portion of the blade 21 (away from the side of the piezoelectric vibrator 2). In the structure shown in Fig. 8 (Α), the position of the opening may be arranged at the front end of the blade 21. Thus, even if the notch portion 23 is formed at the end portion of the blade 21, the effect of increasing the amplitude of the blade 2 and the effect of sweeping the high temperature air of the wall surface of the fin can be obtained by the reduction of the air resistance. In the example of Fig. 8(B), the blade 21 in which the plurality of openings 22a to 22d are formed is joined to the piezoelectric vibrator 20 to constitute the piezoelectric fan 33. The difference in the effect of the position and number of the openings facing the blades 21 is as follows. First, as shown in FIG. 3, the opening portion 22 is formed near the root portion of the blade (the side of the piezoelectric vibrator 20), and since the opening portion 22 is present at a small oscillating position of the blade 21, the air resistance is small. The effect of the reduction is small, and the effect of increasing the amplitude of the blade 21 is small, but the effect of the air being pushed out at the tip end portion of the blade 21 is not lost by the opening portion, so that the air blowing property is high. On the other hand, when the notch portion 23 is formed in the vicinity of the end portion of the blade 21 (or the opening portion is formed in the vicinity of the tip end portion) as shown in Fig. 8(A), the effect of reducing the air resistance is high and the amplitude of the blade 21 is increased. Therefore, the sweeping effect of the high temperature air on the wall surface of the fin is increased. However, since the effect of the air flow from the tip end portion of the blade is lowered, the air blowing property is lowered. 〇 Because the airflow and sweeping effects are somewhat compromised, the shape, position, and size of the opening can be determined in such a way as to obtain the highest cooling capacity. Further, even if a plurality of openings are provided as shown in Fig. 8(B), the size, formation position, number, and the like of the openings are determined in consideration of the air blowing property and the sweeping effect. In the case where the opening portion is formed in the vicinity of the root portion of the blade (the side of the piezoelectric vibrator 2〇), the bending stress of the blade 21 makes the substantial width of the relatively large position small, but the opening portion 22 is not The shape extending in the longitudinal direction of the blade 21 in the width direction 134432.doc -15-200930899 can alleviate the concentration of bending stress and ensure the reliability in long-term driving. «Third Embodiment> Fig. 9 is a perspective view showing a piezoelectric fan used in a cooling device according to a third embodiment. In this example, the piezoelectric fan 34 is constituted by the blade 21 having the opening 22, the tip end portion having the weights 24a and 24b, and the piezoelectric vibrator 20.
❹ 配重24a、24b與葉片21相同均由不銹鋼構成,藉由接 著劑接合。該配重24a、24b之圖中尺寸L3為2 mm,d為 0.5 mm。另葉片21之厚度尺寸為100 μηι。其他尺寸u、 L2、W與圖3所示之第1實施形態之情形相同為[1 = 12 mm、L=18 mm、W=6 mm。開口部22之形成位置及尺寸 與圖3所示者相同。 園ιυ係具備 -Vt五曰。里汉 開口部之效果之示意圖。可知,如此藉由具備配重24a、 24b及開口部22’比起配重及開口部均未設置之壓電風扇 於開放空間振動之情形可得到更大之振幅。例如施加輸 入電壓3GV時’於配重及開口部均未設置之壓電風扇之 情形葉片前端之振幅為約5.5_,但相對地,具備如圖 1〇所不之配重及開口部之壓電風扇之情形,葉片前端之 振幅增大至9.5 mm。 月]々 如此藉由於葉片21之前端部安裝配重24a、24b,因配 重使慣性力矩增大,藉由以包含配 因配 驅動,即使於如圖4所示之散 以之共振頻率 電風扇34之情形亦可增大 住之空間内配置壓 葉片21之振幅。故可提高冷卻 134432.doc 200930899 能力。 另,配重之附加與開口部之形成存在相乘效果。此係 因為’配重之附加與‘部之形成使葉片重心向前端部 移動’葉片每質量之慣性力矩増大。 . 因此因配重24a、24b亦使葉片之振幅增大,開口部22 • 所產生之掃除效果可進一步提高。 «第4實施形態》 〇 圖11係第4實施形態之廢電風扇之立體圖。該例中,設 有開口部22b、22c之同時,整體為長條狀,由於以使長 度方向短縮化之方式曲折之葉片21,及將之接合之壓電 振動子20構成壓電風扇35。藉由如此構造,葉片21之全 長增長II由對帛片21以基本頻率共振般驅動使振幅增 大提同冷卻旎力。另葉片21盡管全長較長但因可將長度 方向尺寸整體性短縮化,故可抑制冷卻裝置整體之大型 化並提高冷卻能力。 © 另,該例中葉片21分成以21a、21b、21C所示之3部位 般曲折,於壓電振動子20附近之部位21a未形成開口部, 於部位21b、21c各形成開口部22b、22c。此外,開口部 22b、22c避開曲折部分而形成。藉由如此構造,壓電振 . 動子側之根部之彈性加強,前端部之彈性減弱,部位 21b、21c之振幅(特別是21c之振幅)增大。因此,進行團 扇運動般擺動,可得到高送風能力。 另,因應力不集令於開口部,故可確保長期驅動時之 信賴性。 ^ 134432.doc 200930899 另,該等曲折構造之葉片之前端部或特定處所,亦可 安裝上如圖9所示之配重。 «第5實施形態》 圖12係第5實施形態之壓電風扇之側面圖。截至目前所 示之各實施形態係於葉片21之一面接合壓電振動子2〇之 類型’但圖12所示之壓電風扇36,係將葉片21之端部從 兩面夾住般分別配置壓電元件20a、20b,由壓電元件 2〇a、20b及葉片21構成雙壓電晶片型振動子。 於壓電元件20a、20b之各自表面形成電極膜,該等電 極與葉片21之間,藉由施加對應於壓電元件2〇a、2〇b之 分極方向之驅動電壓使壓電元件20a、20b向相反方向伸 縮’作為雙壓電晶片型壓電振動子進行驅動。 藉由成為如此之雙壓電晶片型,因壓電元件2〇a、2〇b 可增大葉片21相對於施加電壓之彎曲變位量,可進一步 高效增大葉片21之振幅。 ❹ 圖12中雖顯示開口部22形成於葉片21之壓電風扇之 例’但對於如圖9之於葉片21之前端部安裝配重之構造, 或如圖11之使葉片21彎曲構造之壓電風扇亦同樣適用。 ' «第6實施形態》 - 圖13係第6實施形態之冷卻裝置所用之壓電風扇之立體 圖。將如同圖所示之2個壓電振動子26a、26b之各自一端 彼此經由墊片28接合構成U字型壓電振動子單元,一方 之壓電振動子26a之端部經由墊片29與葉片21接合構成壓 電風扇3 7。該例中於葉片21形成開口部22。 134432.doc 18 200930899 另’前述塾片28、29並非必須者。 圖14係前述U字型壓電振動子單元之電壓施加時之彎曲 模式之示意。圖14(A)係相對於2個壓電振動子26a、26b之 施加電壓為0時之狀態,(B)係施加正電壓時之狀態,(C)係 施加負電壓時之狀態。❹ The weights 24a and 24b are made of stainless steel in the same manner as the blades 21, and are joined by an adhesive. The figure of the weights 24a, 24b has a dimension L3 of 2 mm and a d of 0.5 mm. The other blade 21 has a thickness of 100 μm. The other dimensions u, L2, and W are the same as in the first embodiment shown in Fig. 3 as [1 = 12 mm, L = 18 mm, and W = 6 mm. The position and size of the opening 22 are the same as those shown in Fig. 3. Park υ is equipped with -Vt five. A schematic diagram of the effect of Lihan's opening. It can be seen that a larger amplitude can be obtained by the fact that the counterweights 24a, 24b and the opening 22' are vibrated in the open space compared to the piezoelectric fan which is not provided with the counterweight and the opening. For example, when the input voltage is 3GV, the amplitude of the tip of the blade is about 5.5_ in the case where the counterweight and the piezoelectric fan are not provided in the opening, but the counterweight and the opening are not shown in Fig. 1 . In the case of an electric fan, the amplitude of the front end of the blade is increased to 9.5 mm. Because of the weighting of the moments 24a, 24b at the front end of the blade 21, the moment of inertia is increased by the weight, and by the inclusion of the matching, even at the resonant frequency as shown in FIG. In the case of the fan 34, the amplitude of the pressure vanes 21 can be increased in the space in which it is accommodated. Therefore, it can improve the cooling capacity of 134432.doc 200930899. In addition, the addition of the weight has a multiplication effect with the formation of the opening. This is because the addition of the counterweight and the formation of the 'part makes the center of gravity of the blade move toward the front end portion'. The inertia moment per mass of the blade is large. Therefore, since the weights of the blades are also increased by the weights 24a, 24b, the sweeping effect produced by the opening portion 22 can be further improved. «Fourth embodiment" Fig. 11 is a perspective view of a waste electric fan according to a fourth embodiment. In this example, the openings 22b and 22c are provided, and the entire blade is elongated, and the blade 21 that is bent so as to be shortened in the longitudinal direction and the piezoelectric vibrator 20 that is joined thereto constitute the piezoelectric fan 35. With such a configuration, the full length growth II of the blade 21 is driven by the resonance of the diaphragm 21 at the fundamental frequency to increase the amplitude and the cooling force. Further, although the blade 21 has a long overall length, the length dimension can be shortened as a whole, so that the overall size of the cooling device can be suppressed and the cooling capacity can be improved. Further, in this example, the blade 21 is divided into three portions as shown by 21a, 21b, and 21C, and an opening portion is not formed in the portion 21a near the piezoelectric vibrator 20, and openings 22b and 22c are formed in the portions 21b and 21c. . Further, the openings 22b and 22c are formed avoiding the meandering portions. With such a configuration, the elasticity of the root portion of the piezoelectric vibrator is enhanced, the elasticity of the tip end portion is weakened, and the amplitudes of the portions 21b and 21c (especially the amplitude of 21c) are increased. Therefore, it is possible to obtain a high air blowing capability by swinging in a fan motion. In addition, since the stress is not concentrated in the opening portion, reliability in long-term driving can be ensured. ^ 134432.doc 200930899 In addition, the front end of the blade of the meandering structure or the specific space may be fitted with a counterweight as shown in FIG. «Fifth Embodiment> Fig. 12 is a side view showing a piezoelectric fan according to a fifth embodiment. Each of the embodiments shown so far is based on the type in which the piezoelectric vibrator 2' is joined to one surface of the blade 21. However, the piezoelectric fan 36 shown in Fig. 12 is configured such that the end portions of the vane 21 are sandwiched from both sides. The electric elements 20a and 20b constitute a bimorph type vibrator by the piezoelectric elements 2a and 20b and the vane 21. An electrode film is formed on each surface of the piezoelectric elements 20a and 20b, and the piezoelectric element 20a is formed between the electrodes and the blade 21 by applying a driving voltage corresponding to the polarization directions of the piezoelectric elements 2a and 2b. 20b is stretched in the opposite direction to drive as a bimorph type piezoelectric vibrator. With such a bimorph type, the piezoelectric elements 2a, 2b can increase the amount of bending displacement of the blade 21 with respect to the applied voltage, and the amplitude of the blade 21 can be further efficiently increased. ❹ In FIG. 12, the example in which the opening 22 is formed in the piezoelectric fan of the blade 21 is shown, but the configuration in which the weight is attached to the front end of the blade 21 as shown in FIG. 9, or the pressure of the curved structure of the blade 21 as shown in FIG. Electric fans are also suitable. 'The sixth embodiment>> Fig. 13 is a perspective view of a piezoelectric fan used in the cooling device of the sixth embodiment. The respective ends of the two piezoelectric vibrators 26a and 26b as shown in the figure are joined to each other via the spacer 28 to form a U-shaped piezoelectric vibrating subunit, and the end of one of the piezoelectric vibrators 26a is connected to the blade via the spacer 29. The 21 joint constitutes the piezoelectric fan 37. In this example, the opening portion 22 is formed in the blade 21. 134432.doc 18 200930899 The other aforementioned cymbals 28, 29 are not required. Fig. 14 is a view showing a bending mode at the time of voltage application of the U-shaped piezoelectric vibrating subunit. Fig. 14(A) shows a state in which the applied voltage is zero with respect to the two piezoelectric vibrators 26a and 26b, (B) a state in which a positive voltage is applied, and (C) a state in which a negative voltage is applied.
此處因下側之遷電振動子2 6 b之前端被固定,故上側之 壓電振動子26a之前端與使用單一壓電振動子之情形相 比,以約2倍之角度擺動。因此,可進一步增大圖I]所示 之葉片21之振幅。 另,圖13之例雖以開口部22形成於葉片21之壓電風扇為 例示意’但對於如圖9之於葉片21之前端部安裝.配重之構 造,或如圖11之使葉片21彎曲構造之壓電風扇亦同樣適 用0 «第7實施形態》 圖15係第7實施形態之冷卻裝置所使用之壓電風扇之立 體圖。如同圖所示相對於具備3個壓電振動子27a、2几、 27c部分之整體為E字型之壓電振動子單元經由墊片29接合 葉片21構成壓電風扇38。該例中開口部22形成於葉片2ι。 圖16之(AMC)係前述E字型之壓電振動子單元部分之彎 曲模式之示意。另,圖16(D)〜(F)係前述壓電風扇“之葉片 之擺動之示意。 ’' 27c之施加電壓 (C)係施加負電 圖16(A)係相對於壓電振動子27a、2几 為〇時之狀態’(B)係施加正電壓時之狀維 壓時之狀態。 134432.doc -19- 200930899 此處因壓電振動子27a、27b之前端被固定,故中央之壓 電振動子27c之前端與使用單一之壓電振動子之情形相比 以約2倍之角度擺動。因此,可進一步增大圖15所示之葉 片21之振幅。 ' 另’圖15之例雖以開口部22形成於葉片21之壓電風扇為 . 例示意,但對於如圖9之於葉片21之前端部安裝配重之構 造’或如圖11之使葉片21彎曲構造之壓電風扇亦同樣適 用0 ❹ «第8實施形態》 圖17係第8實施形態之冷卻裝置之構成之示意圖。該冷 卻襞置101由壓電風扇31、散熱器4〇及送風風扇50構成。 第1〜第8之實施形態,基本而言由壓電風扇與散熱器構成 冷卻裝置,壓電風扇雖以掃除由散熱器之散熱片所包圍之 空間内之空氣進行散熱般構成,但該圖〗7所示之例中,散 熱器40之散熱片30所形成之空間内之空氣由壓電風扇31攪 參 動’藉由送風風扇50使之整體向外部送風。 壓電風扇31,由形成開口部22之葉片21與壓電振動子2〇 構成,基本而言與圖3所示者相同。但,該例中葉片21之 朝向係相對於散熱片30之長度方向以約45〇c傾斜。由此壓 . 電振動子20之支持部(固定部)可設於散熱器40之外部,壓 電風扇31之安裝易於進行。 另,開口部22藉由送風風扇5〇增加與氣流對向之成分, 可更接近於圖7(B)所示之模擬條件,提高散熱片3〇壁面之 高溫空氣之掃除效果。 134432.doc .20· 200930899 另’圖17之例雖以開口部22形成於葉片21之壓電風扇為 例不意,但對於如圖9之於葉片21之前端部安裝配重之構 造’或如圖11之使葉片21彎曲構造之壓電風扇亦同樣適 用。 - «第9實施形態》. - 圖18(A)係第9實施形態之冷卻裝置之構成之立體圖,圖 18(B)係該壓電風扇之俯視圖。 φ 如圖18(B)所示,壓電風扇39,具備根部為一體,而突 出複數之葉片21之金屬板19。開口部22形成於各葉片21。 金屬板19上,壓電振動子25貼著於葉片21之根部^金屬板 19藉由螺絲42安裝於支持構件41。藉由對壓電振動子25施 加交變電壓,使金屬板19及葉片21以支持構件41之位置為 支點而擺動。 如圖18(A)所示,冷卻裝置102,藉由將前述壓電風扇39 距離散熱器40之底面一定高度(中央高度或比之略低之高 〇 度)配置而構成。散熱器40中具備彼此平行之複數之散熱 片30,鄰接之散熱片30之間以壓電風扇39之葉片21不抵接 於散熱片30而擺動般配置壓電風扇39。 如此,構成具備以單一壓電振動子擺動複數葉片之壓電 • 風扇之冷卻裝置102。 «第10實施形態》 圖19係第10實施形態之壓電風扇之俯視圖。 圖19 (A)之例中,將金屬板19分成左側之區域[、中央之 區域C、右側之區域R之3個區域,壓電振動子25[、25C、 134432.doc -21- 200930899 25R分別設於各個區域。藉此可獨立擺動該㈣區域。 同樣圖19(B)之例中,將金屬板19分成左側之區域[與 右側之區域尺之2個區域,壓電振動子25L、25R分別設於 各個區域。藉此可獨立擺動該2個區域。 藉由該構成,可根據目的擺動各區域之葉片Μ。例如, 圖19(A)之情形’ #由以正相電壓驅動壓電振動子η、 25R,以逆相電壓驅動壓電振動子25(:,可使支持構件“ 所受反作用力減小。同樣,圖19(B)之情形,#由以正相 電壓驅動壓電振動子25L,以逆相電壓驅動壓電振動子 25R ’可使支持構件41所受反作用力減小。 如此,可抑制安裝有該支持構件41之構件之振動,達到 靜音化。 另,區域之分割數或各區域内之葉片數量,並不局限於 圖19所示者,使金屬板19及葉片21以預期之振動模式振動 般適當設定即可。Here, since the front end of the electric vibrator 2 6 b is fixed at the lower side, the front end of the piezoelectric vibrator 26a on the upper side is swung at an angle of about 2 times as compared with the case where a single piezoelectric vibrator is used. Therefore, the amplitude of the blade 21 shown in Fig. 1] can be further increased. In addition, the example of FIG. 13 is exemplified by a piezoelectric fan in which the opening portion 22 is formed in the blade 21, but the structure of the counterweight is attached to the front end of the blade 21 as shown in FIG. 9, or the blade 21 is as shown in FIG. Similarly, a piezoelectric fan having a curved structure is also applied. 0 «Seventh Embodiment FIG. 15 is a perspective view of a piezoelectric fan used in a cooling device according to a seventh embodiment. As shown in the figure, the piezoelectric fan 38 is formed by joining the blades 21 via the spacers 29 to the piezoelectric vibrating subunits having the E-shaped integral portions of the three piezoelectric vibrators 27a, 2, and 27c. In this example, the opening portion 22 is formed in the blade 2ι. Fig. 16 (AMC) is an illustration of the bending mode of the piezoelectric vibrating sub-unit portion of the aforementioned E-shape. 16(D) to (F) are diagrams showing the swing of the blade of the piezoelectric fan. The applied voltage (C) of the 27C is a negative electric current image 16 (A) with respect to the piezoelectric vibrator 27a. (2) The state when the voltage is applied to the positive voltage. (B) is the state when the positive voltage is applied. 134432.doc -19- 200930899 Here, since the front ends of the piezoelectric vibrators 27a and 27b are fixed, the pressure at the center The front end of the electric vibrator 27c swings at an angle of about 2 times as compared with the case of using a single piezoelectric vibrator. Therefore, the amplitude of the blade 21 shown in Fig. 15 can be further increased. The piezoelectric fan in which the opening portion 22 is formed in the blade 21 is exemplified, but the piezoelectric fan in which the weight is attached to the front end of the blade 21 as shown in Fig. 9 or the blade 21 is bent as shown in Fig. 11 The same applies to the "0" «Eighth Embodiment" Fig. 17 is a schematic view showing the configuration of a cooling device according to the eighth embodiment. The cooling device 101 is composed of a piezoelectric fan 31, a radiator 4, and a blower fan 50. In the embodiment of the eighth embodiment, the piezoelectric fan and the heat sink basically constitute a cooling device, and the piezoelectric fan The air in the space surrounded by the heat sink of the heat sink is swept to dissipate heat. However, in the example shown in FIG. 7, the air in the space formed by the heat sink 30 of the heat sink 40 is stirred by the piezoelectric fan 31. The fan fan 31 is configured to blow air as a whole to the outside by the blower fan 50. The piezoelectric fan 31 is constituted by the blade 21 forming the opening 22 and the piezoelectric vibrator 2A, and is basically the same as that shown in Fig. 3. In this example, the orientation of the blade 21 is inclined at about 45 〇c with respect to the longitudinal direction of the heat sink 30. Thereby, the support portion (fixed portion) of the electric vibrator 20 can be disposed outside the heat sink 40, and the piezoelectric fan The installation of 31 is easy to carry out. Further, the opening portion 22 increases the component opposed to the airflow by the blower fan 5, and can be closer to the simulation condition shown in Fig. 7(B), thereby improving the high temperature air of the heat sink 3 wall surface. 134432.doc .20· 200930899 In addition, the example of FIG. 17 is exemplified by the piezoelectric fan in which the opening 22 is formed in the blade 21, but the structure in which the weight is attached to the front end of the blade 21 as shown in FIG. 'Or the piezoelectric fan of the curved structure of the blade 21 as shown in Fig. 11 - "The ninth embodiment" - Fig. 18(A) is a perspective view showing a configuration of a cooling device according to a ninth embodiment, and Fig. 18(B) is a plan view of the piezoelectric fan. Fig. 18(B) As shown in the figure, the piezoelectric fan 39 includes a metal plate 19 in which a plurality of roots are integrated to project a plurality of blades 21. The opening 22 is formed in each of the blades 21. On the metal plate 19, the piezoelectric vibrator 25 is attached to the root of the blade 21. The metal plate 19 is attached to the support member 41 by the screw 42. By applying an alternating voltage to the piezoelectric vibrator 25, the metal plate 19 and the blade 21 are swung with the position of the support member 41 as a fulcrum. As shown in Fig. 18(A), the cooling device 102 is configured by arranging the piezoelectric fan 39 at a constant height (central height or slightly higher) than the bottom surface of the heat sink 40. The heat sink 40 is provided with a plurality of heat sinks 30 which are parallel to each other, and the piezoelectric fans 39 are arranged such that the blades 21 of the piezoelectric fans 39 are not slid against the heat sinks 30 between the adjacent heat sinks 30. In this manner, a cooling device 102 having a piezoelectric fan that swings a plurality of blades with a single piezoelectric vibrator is constructed. «10th Embodiment" Fig. 19 is a plan view of a piezoelectric fan according to a tenth embodiment. In the example of Fig. 19 (A), the metal plate 19 is divided into three regions of the left side [the central region C and the right region R, and the piezoelectric vibrator 25 [, 25C, 134432.doc -21 - 200930899 25R They are located in each area. Thereby, the (four) region can be independently swung. Similarly, in the example of Fig. 19(B), the metal plate 19 is divided into the left side region [the two regions of the right side of the ruler, and the piezoelectric vibrators 25L and 25R are provided in the respective regions. Thereby, the two regions can be independently swung. With this configuration, the blade turns of the respective regions can be swung according to the purpose. For example, in the case of Fig. 19(A), the piezoelectric vibrator 25 is driven by a reverse phase voltage by driving the piezoelectric vibrators η, 25R with a positive phase voltage (:, the reaction force of the supporting member can be reduced. Similarly, in the case of Fig. 19(B), # is driven by the piezoelectric vibrator 25L with a positive phase voltage, and the piezoelectric vibrator 25R' is driven with a reverse phase voltage to reduce the reaction force of the supporting member 41. The vibration of the member to which the support member 41 is attached is silenced. In addition, the number of divisions of the region or the number of blades in each region is not limited to those shown in Fig. 19, and the metal plate 19 and the blade 21 are vibrated as expected. Just set the mode as appropriate.
«散熱片 係》 、壓電風扇、 及形成於葉片 之開口部之位置關 置之各部之位置關 對於前述各實施形態所示之冷卻裝 係、尺寸關係,此處進行探討。 片 提 器 大 作為對象之壓電風扇’以於散熱器之散熱片間插入葉 ’葉片刮取掃除散熱片纟面之熱空氣促進冷卻作為前 。為促進冷卻,增加刮取面積非常重要 戈因此増加散熱 之散熱片之表面積之同時’亦有必要伟 ’'、、 — 莱片之振幅增 ’且於彼此鄰接之散熱片間隙設置縱長之 134432.doc 22- 200930899 圖20係於散熱器之散熱片30間之間隙配置葉片21之狀態 之俯視圖。此處X方向稱為縱向方向,y方向成為寬度方 向,z方向成為厚度方向。 e 參 因欲藉由葉片21刮取散熱片30、30表面之熱空氣,故散 熱片30與葉片21之間距G越小越好。但,若縮小間距g, 擺動葉片21時之空氣阻力將增大,葉片21之振幅將縮小。 另一方面,考慮刮取散熱器之散熱片3〇表面之空氣這—目 的,刮取散熱片30間之中央部(圖20中大概以符號B所示之 區域)之空氣並非重要。因此,為減少空氣阻力於葉片h 之中央部設開口部22有其合理性。 若只注重設開口部22之目的,則可遍及葉片21之全長設 開口部22。但,根據下述理由只可於葉片。之中央部(圖 2〇中符號A所示處所)設開口部。首先考慮葉片21之根部部 分、,因根部之振幅較小,空氣阻力亦小,故無設置開口部 之必要。之後考慮葉片21之前端部分,毫無疑問因比前端 更前處並不存在葉片21,押出之空氣可簡單地散至廣闊空 門因此’葉片21之前端部分,因開口部使空氣阻力之減 少效果比較小。另,若至棻义 主莱片21之則端為止形成開口部, 則成為又薄又細長之2 y益:u 丄& 、 片葉片於狹乍散熱片間擺動。雖說 工敗阻力減小,但存為 、“/ 一存在各葉片之動作經由空氣彼此影響, 無法形成安定振動之情形 為剛硬連接。此外,前端部分適宜 蓄,—6 "、使散熱器之散熱片30間熱量不積 分,相對於送風效果之影響大,若從前二 疋程度之送風效果很有必要。振幅最大之前端部 134432.doc -23· 200930899 開口部’則易於形成一方向之安定空氣之流動。 從該等情況考慮宜只於葉片21之中央部設開口部… 關於開口部22之形狀’以如下所述之理由,關於縱向方 向’與可於除根部與前端部分以外之大範圍開設開口部相 對’關於寬度方向,有必要媒保從葉片21之長度方向之邊 至转於該邊之開口部22之邊之尺寸定程度以上。 ❹ ❹ 從-亥it况m 21原本即為縱長可知,_ 口㈣之形狀 亦為縱長。 關於開口部之縱方向尺寸: 若無視端面效果,則π向之某_位置之μ阻力可考 為’速度之平方與截面積比成比例。即,若振幅為 h(x)、頻率為f、截面積比為Γα,則,The position of each portion of the "heat sink", the piezoelectric fan, and the position of the opening formed in the blade is related to the cooling device and dimensional relationship described in the above embodiments. The extractor is large as a piezoelectric fan for the purpose of inserting a leaf between the fins of the heat sink. The blade scrapes off the hot air of the heat sink to promote cooling. In order to promote cooling, it is very important to increase the scraping area. Therefore, it is necessary to add heat to the surface area of the heat sink. It is also necessary to increase the amplitude of the sheet, and set the length of the heat sink between adjacent ones. .doc 22- 200930899 FIG. 20 is a plan view showing a state in which the blades 21 are disposed in the gap between the heat sinks 30 of the heat sink. Here, the X direction is referred to as the longitudinal direction, the y direction is the width direction, and the z direction is the thickness direction. e The parameter is intended to scrape the hot air on the surface of the fins 30, 30 by the blade 21, so the smaller the distance G between the fin 30 and the blade 21, the better. However, if the pitch g is narrowed, the air resistance when the blade 21 is swung will increase, and the amplitude of the blade 21 will decrease. On the other hand, in consideration of the air which scrapes off the surface of the heat sink 3 of the heat sink, it is not important to scrape the air at the central portion between the fins 30 (the area indicated by the symbol B in Fig. 20). Therefore, it is reasonable to provide the opening portion 22 at the center portion of the blade h in order to reduce the air resistance. If only the purpose of providing the opening portion 22 is emphasized, the opening portion 22 can be provided over the entire length of the blade 21. However, it can only be used for the blade for the following reasons. The central portion (the space indicated by symbol A in Fig. 2A) is provided with an opening portion. First, considering the root portion of the blade 21, since the amplitude of the root portion is small and the air resistance is small, there is no need to provide an opening portion. After considering the front end portion of the blade 21, there is no doubt that the blade 21 is not present in front of the front end, and the extruded air can be easily dispersed to the wide empty door. Therefore, the front end portion of the blade 21 is reduced in air resistance due to the opening portion. smaller. In addition, if an opening is formed at the end of the main sheet 21 of the Yiyi, it becomes thin and slender. 2 y benefits: u 丄&, the blade oscillates between the narrow fins. Although the resistance to work is reduced, it is saved, "/ The action of each blade is affected by the air, and the situation that the stable vibration cannot be formed is a rigid connection. In addition, the front end portion is suitable for storage, -6 " The heat between the heat sinks 30 is not integrated, and the influence on the air supply effect is large, and it is necessary to provide the air supply effect from the first two degrees. The amplitude of the front end is 134432.doc -23· 200930899 The opening portion is easy to form a direction. The flow of the air is stabilized. From these circumstances, it is preferable to provide the opening only in the central portion of the blade 21. The shape of the opening 22 is related to the longitudinal direction 'and the root portion and the front end portion for the reasons described below. In the wide range of openings, it is necessary to ensure that the size from the side of the longitudinal direction of the blade 21 to the side of the opening 22 of the side is greater than or equal to the width direction. ❹ ❹ From -Hit condition m 21 Original That is, the length is known, and the shape of the _ mouth (4) is also long. About the longitudinal dimension of the opening: If the end effect is ignored, the μ resistance of π to a certain position can be considered as 'speed. The square cross-sectional area is proportional to the ratio. That is, when the amplitude of h (x), the frequency is f, the cross-sectional area ratio Γα, then,
Χ處之空氣阻力〇cf2h2rA 各截面之&阻力遍及葉片長進行積分者作為整體之空氣 阻力。 另’[截面積比]=([葉片寬]_[開口部寬]}/[散熱片間之間 隔]。如此’因空氣阻力與振幅之平方成比例,故振幅小 立之根部附近之空氣阻力可無視。因此,於根部附近設開口 邛基本毫無意義。 關於前端部,即使無開口部其前端更前處存在大空間。 :此’押出之空氣,即使不通過葉片21與散熱片之狹窄縫 Γ (圖20中之G部分)亦可向前端方向流動。因此,空氣阻 ^匕無視前述之端面效果之估值要小。該端面效果之範 ’理論上基本等同於葉片21之寬。因此,至少從前端至 I34432.doc •24· 200930899 與葉片寬相等長度之範圍 設開口部之必要。 即使從空氣阻力之觀點亦無開 關於開口部之寬方向尺寸:The air resistance of the 〇 2 2 2 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 〇 In addition, '[cross-sectional area ratio] = ([blade width] _ [opening width]} / [interval between fins]. So 'the air resistance is proportional to the square of the amplitude, so the air near the root of the amplitude is small The resistance can be ignored. Therefore, it is basically meaningless to have an opening near the root. Regarding the front end, even if there is no opening, there is a large space at the front end of the opening. : This 'exhausted air, even if it does not pass through the blade 21 and the heat sink The narrow slit (part G in Fig. 20) can also flow toward the front end. Therefore, the air resistance is estimated to be small in view of the aforementioned end effect. The end effect is theoretically equivalent to the width of the blade 21. Therefore, it is necessary to provide an opening at least from the front end to I34432.doc •24·200930899 in the same length as the blade width. Even from the viewpoint of air resistance, there is no switch in the width direction of the opening:
、:鴻根據壓電風扇之有無’相對於距散熱片之距離其 --之梯度差異之示意圖。粗線係不存在壓電風扇之情 係、存在壓電風扇之情形。散熱器之散熱片間之温 -刀®21之粗線所示。壓電風扇存在並動作之情 因使葉片兩端之空氣混合,故如圖中細線所示,葉二 (圖中符號E之部分)之溫度均一化(溫度梯度平緩)。其結 散熱片與葉片之間之間隙部分(圖中符號G之部分)之 ’皿度下降,散熱片表面之溫度梯度陡峭。因熱流束與溫度 梯度成_ ’故此係從散熱片表面流出大量熱量,即冷卻 效果提升之示意。 由於此冷卻能力提升之機制,故若葉片兩端(圖20中G之 位置與G+E之位置)之溫度差不充分,則無法充分提升冷卻 能力。因此’毫無疑問〇必須設定於溫度變化大之區物 葉片2!之兩侧部應盡量靠近散熱片%),對於尺相亦有必 要確保形成充分兩端溫度差之尺寸。 若距散熱片3G之距離相當近,溫度分布大致成為直線。 若以該直線之傾斜度(=溫度梯度)融,散熱片表面之溫度 為T〇則距離散熱片之壁面為尺寸G之位置之溫度為 T〇+k*G,距離為(G+E)之位置之溫度為T〇+k*(G+E)。因葉 片21之位置處溫度完全均—化時,該葉片2ι之位置之溫度 為To k (G+E/2),故溫度梯度可估值為ρ(丨+〇.5*Ε/〇)。 134432.doc -25- 200930899 即,若E=G,則預計可提升最大5〇%之冷卻能力。考慮 到無法使葉片部之溫度分布完全均一化,溫度分布也有可 能脫離線形域之情況,為得到明確之冷卻能力提升則確定 E>G可行之有效。 • «其他實施形態》 • 以上所示之幾種實施形態中’壓電振動子之端部接著葉 片之端部構成雙壓電晶片型之壓電風扇,但葉片之端部亦 可接著壓電振動子之全面。 另,以上所示之幾種實施形態中,示意有葉片之端部接 著配重之例,但配重與葉片一體化成形亦可。此外,配重 亦可不設於葉片之最端部而設於端部附近。 另,以上所示之各實施形態中,葉片亦可使用不銹鋼以 外之磷青銅等彈性高之金屬板或樹脂板。 此外,圖12所示之構成以外之例中,雙壓電晶片型壓電 振動子接著於葉片之一面,但作為接著於葉片之一面之壓 〇 電振動子使用單一壓電元件,藉由該壓電元件與葉片構成 单壓電晶片型振動子亦可。 【圖式簡單說明】 圖1係專利文獻1之壓電風扇構成之示意圖。 圖2係壓電風扇之空氣阻力與振幅關係之示意圖。 圖3係第1實施形‘悲'之冷卻裝置所使用之壓電風扇之立體 圖。 圖4(A)、(B)係同一冷卻裝置之構成之示意圖。 圖5係第1實施形態之冷卻裝置所使用之壓電風扇之開口 134432.doc -26· 200930899 部之效果之示意圖。 圖6係葉片之擺動所產生之氣流之樣子之示意圖。 圖7(A)、(B)係隨著形成於葉片之開口部之有無,流動 於散熱片間之空間之氣流溫度分布之例之示意圖。 圖8⑷、(B)係第2實施形態之冷卻裝置所使用之麼電風 扇之立體圖。 圖9係第3實施形態之冷卻裝置所使用之壓電風扇之立體 圖。, : According to the presence or absence of a piezoelectric fan, the difference in gradient with respect to the distance from the heat sink. The thick line does not have the situation of a piezoelectric fan, and there is a case of a piezoelectric fan. The temperature between the heat sink fins is shown by the thick line of the knife®21. Piezoelectric fan exists and operates Because the air at both ends of the blade is mixed, the temperature of the leaf 2 (the part of the symbol E in the figure) is uniform (the temperature gradient is gentle) as shown by the thin line in the figure. The gap between the junction of the fin and the blade (the portion of the symbol G in the figure) decreases, and the temperature gradient of the surface of the fin is steep. Since the heat flux and the temperature gradient become _', a large amount of heat flows out from the surface of the fin, that is, the cooling effect is improved. Due to this mechanism of cooling capacity improvement, if the temperature difference between the two ends of the blade (the position of G in Fig. 20 and the position of G+E) is insufficient, the cooling capacity cannot be sufficiently improved. Therefore, there is no doubt that it must be set in the area where the temperature changes greatly. The sides of the blade 2! should be as close as possible to the fins.) For the ruler phase, it is necessary to ensure that the temperature difference between the two ends is sufficient. If the distance from the heat sink 3G is relatively close, the temperature distribution becomes substantially straight. If the inclination of the straight line (=temperature gradient) is melted, the temperature of the surface of the heat sink is T〇, and the temperature from the wall surface of the heat sink to the size G is T〇+k*G, and the distance is (G+E). The temperature at the location is T〇+k*(G+E). Since the temperature at the position of the blade 21 is completely uniform, the temperature of the position of the blade 2ι is To k (G+E/2), so the temperature gradient can be estimated as ρ(丨+〇.5*Ε/〇). . 134432.doc -25- 200930899 That is, if E=G, it is expected to increase the cooling capacity by up to 5%. Considering that the temperature distribution of the blade portion cannot be completely uniformized, the temperature distribution may be deviated from the linear domain, and it is determined that E>G is effective in order to obtain a clear cooling capacity improvement. • «Other Embodiments> • In the above-described embodiments, the end portion of the piezoelectric vibrator is followed by the end of the blade to form a bimorph type piezoelectric fan, but the end of the blade may follow the piezoelectric The vibrator is comprehensive. Further, in the above-described embodiments, the example in which the end portion of the blade is attached to the weight is shown, but the weight may be integrally formed with the blade. Further, the weight may be provided not near the end of the blade but near the end. Further, in each of the embodiments shown above, a metal plate or a resin plate having a high elasticity such as phosphor bronze other than stainless steel may be used as the blade. Further, in the example other than the configuration shown in FIG. 12, the bimorph type piezoelectric vibrator is followed by one surface of the blade, but a single piezoelectric element is used as the piezoelectric vibrator following one surface of the blade. The piezoelectric element and the blade may constitute a unimorph type vibrator. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic view showing the configuration of a piezoelectric fan of Patent Document 1. Figure 2 is a schematic diagram showing the relationship between air resistance and amplitude of a piezoelectric fan. Fig. 3 is a perspective view of a piezoelectric fan used in the first embodiment of the "sorrowful" cooling device. 4(A) and 4(B) are schematic views showing the configuration of the same cooling device. Fig. 5 is a view showing the effect of the opening of the piezoelectric fan used in the cooling device of the first embodiment 134432.doc -26· 200930899. Figure 6 is a schematic illustration of the appearance of the airflow produced by the oscillation of the blades. Fig. 7 (A) and Fig. 7(B) are diagrams showing an example of the temperature distribution of the airflow flowing in the space between the fins in accordance with the presence or absence of the opening formed in the blade. Fig. 8 (4) and (B) are perspective views of an electric fan used in the cooling device of the second embodiment. Fig. 9 is a perspective view of a piezoelectric fan used in the cooling device of the third embodiment.
❷ 圖10係同-壓電風扇之配重與開口部之效果之示意圖。 圖11係第4實施形態之冷卻裝置所使用之壓電風扇之立 體圖。 之壓電風扇之側 圖12係第5實施形態之冷卻裝置所使用 面圖。 圖13係第6實施形態之冷卻裝置所使用之壓電風扇之立 體圖。 圖14(AHC)係同一壓電風扇之彎曲模式之示意圖。 圖15係第7實施形態之冷卻裝置所使用之廢電風扇之立 體圖 片擺動之示 圖16(A)-(F)係同一壓電風扇之彎曲模式及葉 意圖。 圖17係第8實施形態之冷卻裝置之構成示意圖。 圖 圖18⑷、(B)係第9實施形態之冷卻裝置之構成示意 圖19⑷、(B)係第10實施形態之冷卻裝置所使用之壓電 134432.doc -27· 200930899 風扇之俯視圖。 圖20係散熱片、壓電風扇及形成於葉片之開口 關係之示意圖。 圖21係根據壓電風扇之有無,相對於距散熱片 溫度之梯度差異之示意圖。 【主要元件符號說明】 部之位置 之距離其 19 20 > 25 ' 26 ' 27 20a、20b 金屬板 壓電振動子 壓電元件❷ Figure 10 is a schematic diagram showing the effect of the counterweight and the opening of the piezoelectric fan. Fig. 11 is a perspective view showing a piezoelectric fan used in the cooling device of the fourth embodiment. Side of the piezoelectric fan Fig. 12 is a plan view showing a cooling device according to the fifth embodiment. Fig. 13 is a perspective view showing a piezoelectric fan used in the cooling device of the sixth embodiment. Fig. 14 (AHC) is a schematic view showing a bending mode of the same piezoelectric fan. Fig. 15 is a perspective view showing the vertical image of the waste electric fan used in the cooling device of the seventh embodiment. Figs. 16(A)-(F) show the bending mode and the blade intention of the same piezoelectric fan. Figure 17 is a schematic view showing the configuration of a cooling device according to an eighth embodiment. 18(4) and (B) are schematic views showing the configuration of a cooling device according to a ninth embodiment. Figs. 19(4) and (B) are piezoelectric views of a cooling device used in a cooling device according to a tenth embodiment. 134432.doc -27· 200930899 A plan view of a fan. Figure 20 is a schematic view showing the relationship between the heat sink, the piezoelectric fan, and the opening formed in the blade. Figure 21 is a schematic diagram showing the difference in gradient with respect to the temperature of the heat sink depending on the presence or absence of the piezoelectric fan. [Description of main component symbols] Distance of the position of the part 19 20 > 25 ' 26 ' 27 20a, 20b Metal plate Piezoelectric vibrator Piezoelectric element
21 22 23 24 28、29 30 31-39 40 41 50 100 、 101 110 120 葉片 開口部 缺口部 配重 墊片 散熱片 壓電風扇 散熱器 支持構件 送風風扇 冷卻裴置 發熱體 電路基板 134432.doc -28-21 22 23 24 28, 29 30 31-39 40 41 50 100 , 101 110 120 Blade opening notch part weight spacer heat sink Piezo fan radiator support member air supply fan cooling heat generating circuit board 134432.doc - 28-
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TW097135215A TW200930899A (en) | 2007-09-14 | 2008-09-12 | Cooling apparatus |
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US (2) | US20110064594A1 (en) |
JP (1) | JP5083322B2 (en) |
CN (2) | CN102543915A (en) |
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WO (1) | WO2009034956A1 (en) |
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JP5170238B2 (en) * | 2008-03-25 | 2013-03-27 | 株式会社村田製作所 | Piezoelectric fan device and air cooling device using this piezoelectric fan device |
JP5895190B2 (en) | 2011-03-23 | 2016-03-30 | パナソニックIpマネジメント株式会社 | Electronic equipment cooling device |
CN102841615B (en) * | 2011-06-24 | 2016-06-22 | 中兴通讯股份有限公司 | A kind of regulate the method for terminal temperature, device and terminal |
TWI486747B (en) * | 2012-03-28 | 2015-06-01 | Wistron Corp | Computer system |
CN103369916B (en) * | 2012-03-30 | 2016-05-18 | 台达电子工业股份有限公司 | Cooling module |
TWI524840B (en) | 2012-03-30 | 2016-03-01 | 台達電子工業股份有限公司 | Heat dissipating module |
GB201220471D0 (en) * | 2012-11-14 | 2012-12-26 | Technology Partnership The | Pump |
CN104378948B (en) * | 2013-08-12 | 2018-01-12 | 奇鋐科技股份有限公司 | Heat sink device |
US9367103B2 (en) * | 2013-08-22 | 2016-06-14 | Asia Vital Components Co., Ltd. | Heat dissipation device |
TW201526770A (en) * | 2013-12-17 | 2015-07-01 | Wistron Corp | Heat dissipation device and control method thereof |
EP2995821B1 (en) * | 2014-07-30 | 2018-11-07 | R-Flow Co., Ltd. | Piezo fan |
WO2016032429A1 (en) * | 2014-08-25 | 2016-03-03 | Ge Aviation Systems Llc | Airflow generator and array of airflow generators |
CN106574638B (en) * | 2014-08-28 | 2020-06-05 | 通用电气航空系统有限责任公司 | Air cooling system and airflow generator |
DE102017211103A1 (en) | 2017-06-29 | 2019-01-03 | E.G.O. Elektro-Gerätebau GmbH | Ventilation device for an electrical appliance and electrical appliance with such a ventilation device |
CN110195724B (en) * | 2019-07-05 | 2024-08-23 | 常州威图流体科技有限公司 | Piezoelectric fan, radiator and electronic equipment |
US11581236B2 (en) | 2020-02-14 | 2023-02-14 | Micron Technology, Inc. | Self-cleaning heatsink for electronic components |
CN112714596A (en) * | 2020-12-24 | 2021-04-27 | 常州威图流体科技有限公司 | Oscillating radiating fin |
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US1126256A (en) * | 1913-06-12 | 1915-01-26 | Charles P Mosher | Fan. |
JPS60187799A (en) * | 1984-03-06 | 1985-09-25 | Nippon Denso Co Ltd | Piezoelectric fan |
JPS6247800U (en) * | 1985-09-12 | 1987-03-24 | ||
JPH01233796A (en) * | 1988-03-14 | 1989-09-19 | Murata Mfg Co Ltd | Radiator |
US5403160A (en) * | 1994-01-24 | 1995-04-04 | You; Yaw-Yuh | Fan blade configuration |
CN2229103Y (en) * | 1995-05-04 | 1996-06-12 | 科升科技有限公司 | Integrated circuit cooling device |
JPH08330488A (en) * | 1995-05-30 | 1996-12-13 | Sumitomo Metal Ind Ltd | Heat sink with piezoelectric fan |
IT1303113B1 (en) * | 1998-10-08 | 2000-10-30 | Gate Spa | AXIAL FAN, IN PARTICULAR FOR THE COOLING OF A HEAT EXCHANGER IN A VEHICLE. |
JP2002339900A (en) * | 2001-05-11 | 2002-11-27 | Sony Corp | Piezoelectric fan |
US7321184B2 (en) * | 2005-08-09 | 2008-01-22 | Intel Corporation | Rake shaped fan |
US20090004034A1 (en) * | 2007-06-29 | 2009-01-01 | Seri Lee | Piezoelectric fan |
-
2008
- 2008-09-09 CN CN201210025656XA patent/CN102543915A/en active Pending
- 2008-09-09 CN CN2008801076532A patent/CN101803011B/en not_active Expired - Fee Related
- 2008-09-09 JP JP2009532179A patent/JP5083322B2/en not_active Expired - Fee Related
- 2008-09-09 WO PCT/JP2008/066201 patent/WO2009034956A1/en active Application Filing
- 2008-09-12 TW TW097135215A patent/TW200930899A/en unknown
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2010
- 2010-03-12 US US12/722,650 patent/US20110064594A1/en not_active Abandoned
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JPWO2009034956A1 (en) | 2010-12-24 |
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US20120134858A1 (en) | 2012-05-31 |
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