TWM404278U - Structure of blade for wind power generation device - Google Patents
Structure of blade for wind power generation device Download PDFInfo
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- TWM404278U TWM404278U TW099213685U TW99213685U TWM404278U TW M404278 U TWM404278 U TW M404278U TW 099213685 U TW099213685 U TW 099213685U TW 99213685 U TW99213685 U TW 99213685U TW M404278 U TWM404278 U TW M404278U
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- Y02E10/722—
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Description
M404278M404278
尤指一種應用 五、新型說明: 【新型所屬之技術領域】 本案係關於渦輪翼片氣動力外型結構 於風力發電機的翼片結構。 【先前技術】Especially an application 5. New description: [New technical field] This case is about the airfoil structure of the wind turbine. [Prior Art]
風力發電機,主要藉由氣體自然風速的動能,即風吹 動翼Μ風力葉片、風力滿輪)’透過翼片使風力動能轉換 成旋轉的力量,進而轉動發電機以產生電#。一般風力發 電設備的翼片結構是自習用的送風設備逆向運用,雖缺看 似都與空氣動能㈣,實際上差異甚大,送風設備之目的 在於產生空氣動能,而風力發電設備的翼片結構則是承受 空氣動能並將空氣動能轉換為機械能及電能輸出,因此若 僅是簡單的將送風設備的螺旋槳(㈣pe㈣裝在風力發電 、轉子上則效率比不上該螺旋紫作為送風設備時的效 率。故不能單純的將送風設備的螺旋樂轉用在風力發電機 上’需要重新的設相針對風力發電的情形。 爰是之故,申請人有鑑於習知技術之缺失,創作出本 案「應用於小型風力發電機的翼片氣動力外型結構」,用以 改善上述習用手段之缺失。 【新型内容】 本新型之目的在於更有效的應用自然風速的動能,即 =翼片帶動發電機有效的將氣體動能轉換為電能,可以 。於200W〜400W水平式風力發電機之轉動翼片。 為了達到上述之目的’本創作提供一種應用於風力發 3 M4U4278 電機的翼片結構,包括 你仇4 10ϋ26 θ 匕括一翼根部’位於該翼片結構的一螭γ 一翼尖部,位於該背μ,, . 翼片結構的另一端;以及一迎風面,位 於該翼根部與該翼尖部之間,並具有—迎風角其中該 迎η角自該翼根部至該翼尖部為逐漸增大,而該翼根部與 該翼大部的翼型均為國家再生能源研究室(NREL)的翼型 S 8 3 1 〇 如上所述的翼片結構,其中該迎風角的增大是呈拋物 曲線變化〇 - 如上所述的翼片結構,其中該翼根部的弦長大於該翼鲁 尖部的弦長。 如上所述的翼片結構,其中該翼尖部的迎風角大於該 翼根部的迎風角17度至23度。 如上所述的翼片結構,其中該翼片結構具有一有效翼 展而It翼根部的弦長為該有效翼展的四分之一至五分之 —之間。 A如上所述的翼片結構,其中該翼尖部的弦長為該翼根 #的弦長的八分之—至七分之一之間。 · 如上所述的翼片結構,其中該翼根部更形成—連接部。 所述的翼片結構,更包括一背風面,其令該背風 面的實際面積大於該迎風面的實際面積。 如上所述的翼片,其中該翼尖部的弦長與該翼根部的 的縮小量是呈拋物曲線變化。 緣如别所迷的翼片,其中該翼片具有一翼前緣與一翼後 緣且各自在轉動平面上的投影形狀大致上呈拋物線狀, Μ4Ό4278 而拋物線的方程式y = ax3 + bx2+cx + d,而χ表示弦長方^ 變化量,而y表示翼展方向的變化量。而以翼前緣而言 各係數的較佳值為:a=3E-07 ’ b = -0.0004,c=〇.2;215 d=-47.824 ;至於以翼後緣而言,各係數的較佳值為: a=-6E-07,b = 0,0009,c=-〇_5〇31,d=110.72。 【實施方式】 * 以下針對本案之應用於風力發電機的翼片結構的較佳 實施例進行描述,請參考附圖,但實際之配置及所採行的 鲁方法並不必須完全符合所描述的内容,熟習本技藝者當能 在不脫離本案之實際精神及範圍的情況下,做出種種變化 及修改。 請參閱圖1,為本創作的翼片結構的設置示意圖。其 中揭示一風力旋翼1’包括一整流罩10,以及一翼片2透 過一連接部20設置在該整流罩1〇,通常為了確實達到整 - 流的效果’連接部2 〇是埋在整流罩10内。圖1是揭示翼 Φ 片2與整流罩10的相對位置與連結關係,不論是翼片2的 翼尖或是翼根都是類似的相對位置與連結關係。而翼片2 具有一弦線2’,由圖1可見弦線2’是自轉動平面PR逆時 針轉一角度’因此當風來以轴向風向AW吹向翼片2時, 翼片2是以轉轴RA為軸向圖1的圖面上方之方向轉動, 故而翼片2可分為翼前緣21、翼後緣22、迎風面23、與 背風面24。此外’迎風面23距離弦線2,較近而背風面24 距離弦線2’較遠’因此背風面24的整個弧面面積是大於迎 風面23的。 5 /6 年月日 請參閱圖2,為本創作的翼W其 圏。其中可見翼根部2a”與連接部2〇連結,若由圖 向右視之,可見翼片2自g 目異根部2a延伸到翼尖2b”, 圖2中可見翼前緣21、翼後緣22的位置, 給 製的翼型則顯示了本案的翼型 、’ j共主仕異月2上不同位置因 的變化而導致的外型大小比例的變化’為了有效使風力葉 片在不同風速及轉速達到最佳發電效益,翼根冑&,,有較長 並向翼2b呈現先陡後緩呈抛物曲線狀縮短 翼弦長。Wind turbines, mainly by the kinetic energy of the natural wind speed of the gas, that is, the wind blows the wind blades, the wind full wheel)', through the fins, converts the wind kinetic energy into the rotating force, and then turns the generator to generate electricity#. The wing structure of the general wind power generation equipment is the reverse operation of the air supply equipment for self-study. Although it seems to be different from the air kinetic energy (4), the difference is actually large. The purpose of the air supply equipment is to generate air kinetic energy, and the wing structure of the wind power generation equipment is It is subjected to air kinetic energy and converts air kinetic energy into mechanical energy and electric energy output. Therefore, if the propeller of the air supply device is simply installed on the wind power generation and the rotor, the efficiency is inferior to that of the spiral purple device as the air supply device. Therefore, it is not possible to simply use the spiral music of the air supply equipment on the wind power generator. 'There is a need to re-set the phase for wind power generation. 爰The reason is that the applicant has created the application of the case due to the lack of the prior art. The airfoil aerodynamic structure of the small wind turbine is used to improve the lack of the above-mentioned conventional means. [New content] The purpose of the new model is to more effectively apply the kinetic energy of natural wind speed, that is, the airfoil drives the generator effectively. The conversion of gas kinetic energy into electrical energy can be performed on a rotating wing of a 200W~400W horizontal wind turbine. To achieve the above objectives, 'this creation provides a wing structure for a wind-powered 3 M4U4278 motor, including your hatred 4 10ϋ26 θ including a wing root 'located at the 螭-wing tip of the wing structure, located at the back μ , the other end of the fin structure; and a windward surface between the wing root and the wing tip and having an upwind angle wherein the angle of the welcome angle is gradually increased from the root of the wing to the tip of the wing And the airfoil of the wing root and most of the wing are both the airfoil S 8 3 1 of the National Renewable Energy Research Laboratory (NREL), and the fin structure is as described above, wherein the increase of the windward angle is a parabolic curve. Variation 〇 - a fin structure as described above, wherein the chord length of the wing root is greater than the chord length of the wing tip. The fin structure as described above, wherein the wing tip has a windward angle greater than the windward direction of the wing root Angle 17 degrees to 23 degrees. The fin structure as described above, wherein the fin structure has an effective span and the chord length of the It wing root is between one quarter and a fifth of the effective span. A fin structure as described above, wherein the chord length of the wing tip is The chord length of the wing root # is between eight and one-seventh. · The wing structure as described above, wherein the wing root further forms a joint. The wing structure further includes a leeward surface. The actual area of the leeward surface is greater than the actual area of the windward surface. The fin as described above, wherein the chord length of the wing tip portion and the reduction amount of the wing root portion are parabolically changed. a fan blade, wherein the blade has a wing leading edge and a wing trailing edge and each of the projected shapes on the plane of rotation is substantially parabolic, Μ4Ό4278 and the parabolic equation y = ax3 + bx2+cx + d, and χ represents The chord length is the amount of change, and y is the amount of change in the span direction. For the leading edge of the wing, the preferred value is: a=3E-07 ' b = -0.0004,c=〇.2;215 d = -47.824; as for the trailing edge of the wing, the preferred values for each coefficient are: a = -6E-07, b = 0,0009, c = -〇_5〇31, d=110.72. [Embodiment] * The following is a description of a preferred embodiment of the fin structure applied to the wind power generator of the present invention, please refer to the accompanying drawings, but the actual configuration and the adopted method are not necessarily completely in accordance with the description. The content, those skilled in the art can make various changes and modifications without departing from the actual spirit and scope of the case. Please refer to FIG. 1 , which is a schematic diagram of the arrangement of the wing structure of the present invention. It is disclosed that a wind rotor 1' includes a fairing 10, and a fin 2 is disposed on the fairing 1 through a connecting portion 20, generally in order to achieve a full-flow effect. The connecting portion 2 is buried in the fairing 10. Inside. Fig. 1 is a view showing the relative position and connection relationship of the wing Φ piece 2 and the fairing 10, whether the wing tip or the wing root of the airfoil 2 has a similar relative position and connection relationship. The flap 2 has a string 2'. It can be seen from Fig. 1 that the string 2' is rotated counterclockwise from the plane of rotation PR. Thus, when the wind is blown toward the flap 2 by the axial wind AW, the flap 2 is The rotation axis RA is rotated in the direction of the upper side of the drawing of FIG. 1, so that the airfoil 2 can be divided into a wing leading edge 21, a wing trailing edge 22, a windward surface 23, and a leeward surface 24. Furthermore, the windward surface 23 is closer to the string 2, and the leeward side 24 is further away from the string 2'. Therefore, the entire arc surface area of the leeward surface 24 is larger than the windward surface 23. 5 / 6 Years and Months Please refer to Figure 2 for the wings of this creation. It can be seen that the wing root portion 2a" is coupled with the connecting portion 2". If viewed from the right, the fin 2 can be seen to extend from the g-shaped root portion 2a to the wing tip 2b". In Fig. 2, the leading edge 21 and the trailing edge of the wing can be seen. The position of 22, the airfoil of the system shows the airfoil of the case, and the change of the size ratio of the different positions of the different positions on the different moons in the different months. In order to effectively make the wind blades at different wind speeds and The speed reaches the best power generation benefit, and the wing root 胄 &, has a longer length and gives the wing 2b a steeper and slower parabolic curve to shorten the chord length.
請參閱圖3,為本創作的翼片的另一種視角的立艘圖。 其"見翼根部2a”與連接部2〇連結,若由圖3左方向右 視之,可見翼片2自翼尖2b”延伸到翼根部2a,,,並於圖3 中可見翼前緣21、翼後緣22在翼片2上的位置。此外可 以見到本案的翼片2在翼尖2b,,部也的傾角較小,而俞接 近翼根部2a”則傾角愈大。以圖3而言,翼片2的弦長由翼Please refer to Figure 3 for a stand-up view of another perspective of the created wing. Its "see wing root 2a" is connected with the connecting portion 2A. If viewed from the left and right in Fig. 3, it can be seen that the flap 2 extends from the wing tip 2b" to the wing root 2a, and can be seen in Fig. 3 The edge 21, the position of the trailing edge 22 of the wing on the flap 2. In addition, it can be seen that the wing 2 of the present case is at the wing tip 2b, and the inclination angle of the portion is also small, and the inclination angle of the hinge is closer to the root portion 2a". In Fig. 3, the chord length of the wing 2 is determined by the wing.
尖部2b”到翼根部2a,,是呈現先緩後陡呈拋物曲線狀增加翼 弦長。 請參閱圖4,為本創作的翼片的_種翼展平面圖。圖4 可以說是迎風面或是背風面的平面圓。其中可見翼根部2&,, 與連接部20連結’若由圖4左方向右視之可見翼"自 翼根邛2a延伸到翼尖2b,,,並於圖4中可見翼前緣2卜翼 後緣22在翼片2上的位置。且於圖4中可以清楚的看到弦 長自土根部2a”到翼尖部2b,,的縮短變化量是先驟後緩,亦 即在靠近翼根部2a”的附近的縮短量是較大的、而接近翼尖 M404278The tip 2b" to the wing root 2a is a parabolic curve that increases the chord length first and then sharply. See Figure 4 for the wing plan of the wing of the creation. Figure 4 can be said to be the windward side. Or a flat circle of the leeward surface, wherein the wing root 2&, is connected to the connecting portion 20, if the visible wing from the left and right sides of Fig. 4 extends from the wing root 2a to the wing tip 2b, The position of the trailing edge 22 of the wing leading edge 2 on the airfoil 2 can be seen in Fig. 4. And the shortening variation of the chord length from the soil root portion 2a" to the wing tip portion 2b can be clearly seen in Fig. 4 The first step is slow, that is, the amount of shortening near the wing root 2a" is larger, and close to the wing tip M404278
2b則弦長的縮短量是較小的。 ::. V ---^-—_«— 4參閱圖5’為本創作的翼片的翼尖方向視圖。其中 以虛線繪製的翼型則顯示了本案的翼型在翼片2上不同位 置因弦長的變化而導致的外型大小比例的變化,於圖5中 可見翼片2的弦長變化是由翼根部2a”到翼尖部2b”逐漸變 小,並可於圖5中見到翼片2的傾角呈現出變化,且於圖 5中可見翼前緣21、翼後緣22在翼片2上的位置。且在翼2b, the shortening of the chord length is small. ::. V ---^-—_«— 4 See Fig. 5' for the wing tip orientation view of the created flap. The airfoil drawn by the dotted line shows the change of the size ratio of the airfoil in the different positions of the airfoil 2 due to the change of the chord length. In Figure 5, it can be seen that the change of the chord length of the airfoil 2 is The wing root 2a" to the wing tip 2b" gradually becomes smaller, and the inclination of the flap 2 is seen to change in FIG. 5, and in FIG. 5, the leading edge 21 and the trailing edge 22 of the wing are visible in the flap 2 The location on the top. And in the wing
根°卩2a後认置一連接部2〇。此外,本案所使用的翼型是 以美國國家再生能源研究室(Nati〇naI Renewab丨e EnergyAfter the root ° 2a, a connecting portion 2 is recognized. In addition, the airfoil used in this case is the National Renewable Energy Research Laboratory (Nati〇naI Renewab丨e Energy).
Lab〇ratory、NREL)的翼型S831作為整個翼片2的翼型。 圖6,為本創作的翼片的另一種翼展平面圖。圖6可 以說是由翼前緣21或是翼後緣22方向觀察翼片2的平面 圖。其中可見翼根部2a”與連接部2〇連結,若由圖6左方 向右視之,可見翼片2自翼根部2a,,延伸到翼尖2b”。由於 翼片2不論是迎風面23(請配合圖1}或背風面24(請配合圖 1)均是向外凸出的弧面,因此圖6實無法明顯區別是由翼 刖緣21或疋翼後緣22,不過可以確認的是,翼片2上方 大致上屬於迎風面23,而下方大致上屬於背風面24。 圖 為本創作的翼片的弦線傾角變化示意 圖。其中 而翼尖部2b”有一翼尖部 夾角dA的變化在17度The airfoil S831 of Lab〇ratory, NREL) is used as the airfoil of the entire fin 2. Figure 6 is another wing plan view of the flap of the present invention. Figure 6 can be said to be a plan view of the flap 2 as viewed from the leading edge 21 or the trailing edge 22 of the wing. Here, it can be seen that the wing root portion 2a" is coupled to the connecting portion 2A. As seen from the left side of Fig. 6, the flap 2 is seen to extend from the wing root portion 2a to the wing tip 2b". Since the airfoil 2, whether it is the windward surface 23 (please match the figure 1) or the leeward surface 24 (please cooperate with FIG. 1), is a convex curved surface, so the figure 6 cannot be clearly distinguished by the wing edge 21 or the 疋The trailing edge 22 of the wing, although it can be confirmed that the upper portion of the airfoil 2 generally belongs to the windward surface 23, and the lower portion substantially belongs to the leeward surface 24. The figure is a schematic diagram of the change of the inclination angle of the string of the created wing. 2b" has a tip angle change dA at 17 degrees
翼根部2a”有一翼根部弦線2a,, 弦線2b’,兩者間具有一夹角dA 至23度之間’亦即在使用的時候,g尖部几,,的迎風角 大於翼根部2a”料風角,且兩者的差距在17度至23度 之間。 7 M404278 修正 請參閱圖8,為本創作的翼片的又一 月3曰^充 圖8是將翼片2投影至轉動平面⑼(請配咕面菌7 的外型,翼展方向試圖8的縱向、而:圖0上所呈現 橫向。翼尖部2b”位於圖8的上方位置附近向則是圓8的The wing root 2a" has a wing root string 2a, a string 2b' with an angle between dA and 23 degrees between the two, that is, when used, the g-tip is larger than the wing root. 2a" wind angle, and the difference between the two is between 17 degrees and 23 degrees. 7 M404278 Correction Please refer to Figure 8. Another month of the flap of the creation is shown in Fig. 8. The projection of the flap 2 is projected onto the plane of rotation (9) (please match the appearance of the sputum 7 and the spanwise direction is 8 The longitudinal direction, but: the horizontal direction is shown in Fig. 0. The wing tip portion 2b" is located near the upper position of Fig. 8 and is round 8
則位於圖8的下方位置附近。而翼前緣21與部V 就位於翼根部2a,,與翼尖部2b, 緣22則 動羊而pp L g 翼則緣21投影在轉 上呈現的大致上是一個拋物線发 y=ax3+bx2+cx+d,而乂表示弦县古A 程式為 的橫6方6 °的變化量,亦即圖8 的橫向方向,而y表示翼展方向的變 重亦即圓8的縱 向方向《其中各係數的較佳值 一… ^ 07 * b=-0.0004 , c = 0.2215,d = _47,824。翼後緣22投影在轉動平面n上呈 現的大致上是一個拋物線,其方程式為、…, 而X表示弦長方向的變化量’亦即圓8的橫向方向,而y 表示翼展方向的變化量,亦即圖8的縱向方向。其令各係 數的較佳值為:a=-6E-07,b = 0.〇〇〇9,〇 = ,d = ll〇 72。 請參閱! 9,為本創作的風力旋翼的正面示意圖。其 中風力旋翼i包含了三個翼片2透過各自的連接部2〇設置 在整流罩1G上。而風力旋翼i的正面的觀察方向就是平行 於轉軸RA(請參考圖υ,而翼片2以轉軸Ra為軸旋轉, 則自然而然的形成一轉動平面PR,而圖8及其說明所述的 翼前/後緣投影即是投影於此轉動平面p R上。 綜上所述,本創作的「應用於小型風力發電機的翼片 結構」是透過計算流體力學反覆不斷的運算與模擬而得釗 兩個結論,其一是翼片的迎風角度在愈靠近翼尖時角度要 M404278 ^ t · ► .愈大;其二是翼片近根部的, 100. 1. 2 R丨扪弦長與近尖部的弦長要有所不 同,通常翼根部的弦续奶怎廿道 . 刃涵琛較長並導致厚度較厚;而翼尖部的 弦線較短並導致厚度較薄·立- 仔又杈存,其二,翼片在轉動平面上的投 影所顯示的外型,其翼前緣與翼後緣的圖形是大致呈拋物 線狀。簡而言之就是弦長的變化量是自翼根至翼尖呈抛物 曲線漸縮狀。之所以在翼根部與翼尖部的迎風角與翼型弦 •長要有變化是因為在風力翼片的應用情況之下,兩者的風 速與翼片轉動合成氣流狀況不同所至,因此唯有透過本創 攀作的概念才可以將空氣動能發揮到極高的效率。 上述實施例僅係為了方便說明而舉例,雖遭熟悉本技 藝之人士任施匠思而為諸般修飾,然皆不脫如附申請專利 範圍所欲保護者。 【圖式簡單說明】 圖1,為本創作的翼片結構的設置示意圖; 圖2,為本創作的翼片的其中一種視角的立體圖; # 圖3,為本創作的翼片的另一種視角的立體圖; 圖4,為本創作的翼片的一種翼展平面圖; 圖5,為本創作的翼片的翼尖方向視圖; 圖6,為本創作的翼片的另一種翼展平面圖; 圖7,為本創作的翼片的弦線傾角變化示意圖; 圖8,為本創作的翼片的又一種翼展平面圖;以及 圖9,為本創作的風力旋翼的正面示意圖。 【主要元件符號說明】 1 :風力旋翼 9 Έ404278 ίο : 2 : j 20 : 21 : 22 : 23 : 24 : 2a,: 2a” 2b, 2b,, AW PR : RA dA : 整流罩 I片 連接部 翼前緣 翼後緣 迎風面 背風面 :翼根部弦線 :翼根部 :翼尖部弦線 :翼尖部 :轴向風向 轉動平面 :轉軸 :夾角It is located near the lower position of FIG. The wing leading edge 21 and the portion V are located at the wing root portion 2a, and the wing tip portion 2b, the edge 22 is moving the sheep, and the pp L g wing edge 21 is projected on the rotation to be substantially a parabolic y=ax3+ Bx2+cx+d, and 乂 represents the 6 ° variation of the horizontal 6 square of the string county, which is the lateral direction of Figure 8, and y represents the weight of the spanwise direction, that is, the longitudinal direction of the circle 8. The preferred value of each coefficient is... ^ 07 * b = -0.0004 , c = 0.2215, d = _47, 824. The projection of the trailing edge 22 of the wing is substantially a parabola presented on the plane of rotation n, the equation is ..., and X represents the amount of change in the direction of the chord length, ie the lateral direction of the circle 8, and y represents the change in spanwise direction. The amount, that is, the longitudinal direction of FIG. The preferred values for each coefficient are: a = -6E-07, b = 0. 〇〇〇 9, 〇 = , d = ll 〇 72. Please see! 9, a front view of the wind rotor of the creation. The wind rotor i includes three fins 2 which are disposed on the fairing 1G through respective connecting portions 2'. The viewing direction of the front side of the wind rotor i is parallel to the rotating shaft RA (please refer to the figure υ, and the fin 2 rotates with the rotating shaft Ra as an axis, and naturally forms a rotating plane PR, and FIG. 8 and the wing thereof are illustrated The front/rear edge projection is projected onto this plane of rotation p R. In summary, the "wing structure applied to small wind turbines" of this creation is obtained through computational fluid dynamics and continuous calculation and simulation. Two conclusions, one is that the windward angle of the airfoil is closer to the wing tip when the angle is M404278^t. ►. The second is the near the root of the wing, 100. 1. 2 R chord length and near The chord length of the tip is different. Usually, the chord of the wing root is stalked. The blade culvert is longer and leads to a thicker thickness; while the chord of the wing tip is shorter and leads to a thinner thickness. In addition, the shape of the fin on the plane of rotation shows that the pattern of the leading edge of the wing and the trailing edge of the wing is substantially parabolic. In short, the variation of the chord length is from the wing. The root to the tip of the wing is tapered like a parabola. The reason for the windward angle at the root of the wing and the tip of the wing The shape of the airfoil chords must be changed because the wind speed of the two is different from the airflow of the airfoil in the application of the wind flaps. Therefore, the air kinetic energy can only be achieved through the concept of the original climbing. The above embodiments are merely exemplified for convenience of explanation, and those skilled in the art can modify them as they wish, but they are not intended to be protected as claimed. Brief description of the figure] Fig. 1 is a schematic view showing the arrangement of the wing structure of the present invention; Fig. 2 is a perspective view of one of the angles of the created wing piece; #Fig. 3, a perspective view of another perspective view of the created wing piece Figure 4 is a wing plan view of the wing of the present invention; Figure 5 is a wing-tip view of the wing of the present invention; Figure 6, is another wing plan view of the wing of the present invention; Figure 7, A schematic diagram of the variation of the inclination of the string of the created wing; Figure 8 is another wing plan view of the wing of the creation; and Figure 9 is a front view of the wind rotor of the present invention. [Main component symbol description] 1 : Wind Wing 9 Έ404278 ίο : 2 : j 20 : 21 : 22 : 23 : 24 : 2a,: 2a” 2b, 2b,, AW PR : RA dA : fairing I piece connecting wing leading edge wing trailing edge windward leeward : Wing root string: Wing root: Wing tip string: Wing tip: Axial wind direction Rotating plane: Shaft: Angle
1010
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TW099213685U TWM404278U (en) | 2010-07-16 | 2010-07-16 | Structure of blade for wind power generation device |
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TW099213685U TWM404278U (en) | 2010-07-16 | 2010-07-16 | Structure of blade for wind power generation device |
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Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
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TWI553221B (en) * | 2011-12-06 | 2016-10-11 | 亞瑞華風力公司 | Assembly for fixing a rotor blade of a wind energy plant |
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TWI553221B (en) * | 2011-12-06 | 2016-10-11 | 亞瑞華風力公司 | Assembly for fixing a rotor blade of a wind energy plant |
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