TW200422560A - High efficient light collecting module - Google Patents
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200422560 五、發明說明(l) --- k 【發明所屬之技術領域】 本發明是一種集光模組,利用此技術可提升聚光型燈 源的集光效率。 【先前技術] 一般投影顯示系統裝置皆需要利用集光模組來進行分 光、調變、合光及成像。然而,光利用效率的好與壞,直 接關係整體顯像品質的亮度、均勻度、色彩的表現。不僅 如此’隨著投影顯示器價格下滑的趨勢,投影顯示器所使 用的影像調變面板(如DMD panel等)的尺寸也愈來愈 小 以郎省成本,並且在單位面積上的像素也愈來愈多使 得面板的穿透率降低,不僅如此,光的利用效率會隨著面 板面積的縮小而降低。故各薇家,無不潛心研究如何提升 光源的利用效率。 一般來判斷光源經過反射罩所得之光束之效率的好 壞’可以用Etendue這個參數來表示。Etendue的定義及方 程式如下: E= 5 5 cos 0 dAd Ω 而0 、dA、d Ω的關係可參閱第一圖。 此處dA表示光束所投影的面積,表示通過dA之光束 的立體角,而0表示平面dA的法向量與d Ω之中心軸的夾 角。 此方程式表示光束的幾合性質(ge〇metric property ),而光束的能量密度、強度、亮度等的性質, 並不在這個方程式中被顯示出來。在同流明的光束下,當200422560 V. Description of the invention (l) --- k [Technical field to which the invention belongs] The present invention is a light-collecting module, which can improve the light-collecting efficiency of a light source by using this technology. [Previous technology] Generally, projection display system devices need to use a light collection module to perform light splitting, modulation, light combining and imaging. However, the light use efficiency is directly related to the performance of brightness, uniformity, and color of the overall development quality. Not only that, as the price of projection displays declines, the size of image modulation panels (such as DMD panels, etc.) used by projection displays is getting smaller and smaller to save costs, and the number of pixels per unit area is getting more and more It often reduces the transmittance of the panel. Not only that, the light utilization efficiency will decrease as the area of the panel decreases. Therefore, all Wei's families are all concentrating on how to improve the utilization efficiency of light sources. Generally, the efficiency of the light beam obtained by the light source passing through the reflector can be judged by the parameter Etendue. The definition and equation of Etendue are as follows: E = 5 5 cos 0 dAd Ω, and the relationship between 0, dA, and d Ω can be seen in the first figure. Here dA represents the area projected by the beam, represents the solid angle of the beam passing through dA, and 0 represents the angle between the normal vector of the plane dA and the central axis of d Ω. This equation represents the geometric property of the beam, and the properties of the energy density, intensity, and brightness of the beam are not shown in this equation. Under the same lumen beam, when
200422560 五、發明說明(2)200422560 V. Description of Invention (2)
Etendue愈小,表示光束的面積、光束與平面法線的夾角 及光束之立體角的積分值是愈小的;也就是說,光的利用 效率也較高。由以上的概念,光學設計工程師可以容易的 辨定光源模組的光利用效率的好壞。 一般利用於投影顯示器的集光模組,大致可分為橢球 面型燈泡(爹閱弟一圖)及抛物面型燈泡(來閱第三 圖)。在第二圖中,光源131a置於橢球面型反射罩111&的 第一焦點F1111 a上’由光源1 3 1 a所發出的光線,經由橢球 面型反射罩11 la聚焦於第二焦點F1 112a上,光線再進入柱 狀積分器21 a得到均勻化後,再進行分光、合光、成像 等。 參閱第三圖中,光源131a置於拋物面型反射罩i2la的 焦點F 1 2 11 a上’由光源所發出的光線,經由拋物面型反射 罩1 2 1 a的反射,光線彼此之間平行射出反射罩,經由置於 反射罩前的正透鏡4a,將光線匯聚於柱狀積分器2丨&進行 均勻化的處理。 一由於反射罩與光源的搭配,還有其他因素須考量,諸 ^光源的散熱問題、反射罩的鍍膜問題、反射罩開模的問 題及光源與反射罩之間調整的問題。林林總總,總是使得 反射罩的體積無法縮小(也就是說光束經由反射罩的投射 面積無法縮小),並且由於UHP (ultra-high pressure met^ufy lamp )光源的特性,使得聚光點的面積及光束的 立組=無法縮小。因此,當一般投影用的燈泡使用在小尺 寸的’v像,周變面板的之下,往往難以得到理想的光學效The smaller the Etendue, the smaller the integrated value of the area of the beam, the angle between the beam and the plane normal, and the solid angle of the beam; that is, the higher the light utilization efficiency. From the above concepts, the optical design engineer can easily determine the quality of the light utilization efficiency of the light source module. The light-collecting modules generally used in projection displays can be roughly divided into ellipsoidal light bulbs (figure 1) and parabolic light bulbs (figure 3). In the second figure, the light source 131a is placed on the first focus F1111a of the ellipsoidal reflector 111 & the light emitted by the light source 1 3 1a is focused on the second focus F1 through the ellipsoidal reflector 11a On 112a, the light enters the columnar integrator 21a to be homogenized, and then performs beam splitting, light combining, and imaging. Referring to the third figure, the light source 131a is placed on the focal point F 1 2 11 a of the parabolic reflector i2la. The light emitted by the light source is reflected by the parabolic reflector 1 2 1 a, and the light is reflected parallel to each other. The cover, through the positive lens 4a placed in front of the reflecting cover, collects light on the columnar integrator 2 & and performs a homogenization process. First, due to the combination of the reflector and the light source, there are other factors to consider, such as the heat dissipation of the light source, the coating of the reflector, the problem of the mold opening of the reflector, and the adjustment between the light source and the reflector. In all cases, the volume of the reflector cannot be reduced (that is, the projection area of the light beam through the reflector cannot be reduced), and due to the characteristics of the UHP (ultra-high pressure met ^ ufy lamp) light source, the area of the focusing point and Beam group = cannot be reduced. Therefore, when a general projection lamp is used in a small-sized 'v image, it is often difficult to obtain the ideal optical effect
200422560 五、發明說明(3) 率。因此,各廠商無不想盡辦法,改變上述三個因子 (0、Α、Ω),以提升光學效率。 參閱第四圖,此集光模組為Philips在這方面的傑 作。這是利用在燈管13a上的石英圓球體(bulbof': bUrner) l32a的外表面為圓球面的特性,鍍上一 132la,使得圓球體可以料球賴,㈣自光和⑽ 輻射出來的光線,再折回原路徑,使得光源13la之發光角 變為原來的一半,而達到小etendue的作用,以提升光學 效率。 光源131a被包覆在中空石英圓球體U2a (bulb 〇f the bUrner)的球心位置,且光源131&也位於橢球面型反 射罩111 a的第一焦點F111 a位置。在石英圓球體的右半側 的外表面,鍍上乙層反射鍍膜層13218,使得由光源Ula 所輻射出來的光線向右侧射出的部份,經由反射鍍膜層 1321a再反射回石英圓球體132a的球心位置。由於光源 131a被置於橢球面型反射罩111&的第一焦點?1113處,所 以右半側反射回來的光線重新經過第一焦點FUla後,再 向左侧射出。左侧的光線,經由橢球面型反射罩丨丨丨a的反 射後,光束匯聚於橢球面型反射罩丨丨^的第二焦點FU12a 處。 由於最終光源1 3 1 a的光線只向左側射出,再經由橢球 面型反射罩1 Π a聚焦,所以與第二圖之橢球面型反射罩相 比’第四圖的橢球面型反射罩要明顯小許多。也就是在橢 球面型反射罩的第一焦點F 11 la右半邊的反射罩皆用不200422560 V. Description of Invention (3) Rate. Therefore, manufacturers have no intention to change the above three factors (0, A, Ω) to improve optical efficiency. Refer to the fourth picture, this light collecting module is the masterpiece of Philips in this respect. This is the use of the characteristics of the quartz bulb (bulb ': bUrner) l32a on the lamp tube 13a. The outer surface of the bulb is a spherical surface. , And then fold back to the original path, so that the luminous angle of the light source 13la becomes half of the original, and achieves the role of small etendue to improve optical efficiency. The light source 131a is coated on the center position of the hollow quartz sphere U2a (bulb uf the bUrner), and the light source 131 & is also located at the first focus point F111 a of the ellipsoidal reflector 111 a. On the outer surface of the right half of the quartz sphere, a B reflective coating layer 13218 is plated, so that the portion emitted by the light source Ula to the right is reflected back to the quartz sphere 132a through the reflective coating layer 1321a. Center position. Since the light source 131a is placed at the first focus of the ellipsoidal reflector 111 & At 1113, the light reflected from the right half passes through the first focus FUla again, and then exits to the left. After the light on the left side is reflected by the ellipsoidal reflector 丨 丨 丨 a, the light beam is converged at the second focus FU12a of the ellipsoidal reflector 丨 丨 ^. Because the light from the final light source 1 3 1 a only exits to the left and is focused by the ellipsoidal reflector 1 Π a, compared with the ellipsoidal reflector of the second figure, the ellipsoidal reflector of the fourth figure requires Much smaller. That is, the reflector at the right half of the first focus F 11 la of the ellipsoidal reflector is not used.
~ -I a 第6頁 200422560 五、發明說明(4) 4 到,所以可取消 D APhilips 於 2002 SID (Holger Moench, Arnd Ritz, Higher Output, More Compact UHP Lamp Systems, SID 02)所發表的論文可知,在小 Etendue的狀況下(5〜15πιπΓ2 ster),收光效率可提升2〇 〜3 0%。~ -I a Page 6 200422560 V. Description of the invention (4) 4 to, so you can cancel the paper published by D APhilips in 2002 SID (Holger Moench, Arnd Ritz, Higher Output, More Compact UHP Lamp Systems, SID 02) Under the condition of small Etendue (5 ~ 15πππΓ2 ster), the light collection efficiency can be improved by 20 ~ 30%.
Phi 1 ips這種光源模組有幾個問題:(一)石英圓球 體132a的球面經久變形:由於UHP lamp在使用時所產生的 咼熱及高壓,會使石英圓球體發生變形,所以反射回來的 光線就不會沿原路徑回到圓球體球心位置,所以光學效率 會隨時間而降低。(二)燈泡壽命縮短:經石英圓球體 1 3 2 a之反射鍍膜層1 3 21 a反射回來的光線有部份會被電極 1322a遮擋,造成光學效率降低及加熱電極,造成燈泡壽 命縮短。(三)球面製作不易:在製造石英圓球體132a 時’石英圓球體之球面不易製作,造成反射光線不會沿原 路徑回到球心,所以光學效率降低。(四)貨源取得不 易·這種特殊光源模組,只有p h i η p s生產。 參閱第五圖。此光源模組為美國專利(us 635670 0 B1 )由—件橢球面型反射罩31a及一件球面型反射罩32a組 成’其中光源131a被置於橢球面型反射罩31a之第一焦點 F311a上,而球面型反射罩之球心C321與橢球面型反射 罩之第一焦點F 3 11 a與光源1 3 1 a都共點。而燈管1 3 a的對稱 轴A133與光軸(光軸系橢球面型反射罩3 la之第一焦點 F 3 11 a及第二焦點F 3 1 2 a的連線)垂直。光源右半侧的光線 射出後,經由球面型反射罩32a反射後,再沿原路徑經過The Phi 1 ips light source module has several problems: (1) The spherical surface of the quartz round sphere 132a is permanently deformed: Due to the heat and high pressure generated by the UHP lamp during use, the quartz round sphere will be deformed, so it reflects back The light will not return to the center position of the sphere along the original path, so the optical efficiency will decrease with time. (2) Shortened lamp life: Some of the light reflected by the reflective coating 1 3 2 a of the quartz sphere 1 3 21 a will be blocked by the electrode 1322a, resulting in reduced optical efficiency and heating the electrode, resulting in shortened lamp life. (3) Spherical surface is not easy to produce: When manufacturing the quartz spherical body 132a, the spherical surface of the 'quartz spherical body is not easy to produce, resulting in that the reflected light will not return to the center of the sphere along the original path, so the optical efficiency is reduced. (4) It is not easy to obtain the supply source. This special light source module can only be produced by p h i η p s. See Figure 5. This light source module is a U.S. patent (us 635670 0 B1) consisting of a piece of ellipsoidal reflector 31a and a piece of spherical reflector 32a 'where the light source 131a is placed on the first focus F311a of the ellipsoidal reflector 31a The spherical center C321 of the spherical reflector and the first focal point F 3 11 a of the ellipsoidal reflector are in common with the light source 1 3 1 a. The symmetry axis A133 of the lamp tube 1 3 a is perpendicular to the optical axis (the line connecting the first focal point F 3 11 a and the second focal point F 3 1 2 a of the optical axis system ellipsoidal reflector 3 la). After the light from the right half of the light source is emitted, it is reflected by the spherical reflector 32a and then passes along the original path.
200422560 五、發明說明(5) 弟一焦點F 3 11 a到橢球面型反射罩3 1 a上,經橢球面型反射 罩3 1 a反射後,與光源1 3 1 a左侧的光線經橢球面型反射罩 31a—同反射後,共同匯聚於橢球面型反射罩31&之第二焦 點F312a 上。 、、 本件除了可提升光學利用效率外,還有其他缺點: (一)組裝不易(二)經球面型反射罩再反射回來的光 線,有部份會被電極遮擋,造成光利用效率降低。(三) 承上’被電極遮撞的光線’會加熱電極,造成電極冷卻困 難。(四)組件成本過高,均非標準品。(五)體積過 大。 參閱第六圖。此光源模組由一件球狀型反射罩3 2 a及 兩個拋物面型反射罩331a、332a並一燈管I3a組成。球面 型反射單32a的球心C321與第一抛物面型反射軍Mia的焦 點F33 11a及光源131a共心。光源下半侧的光線經由球面型 反射罩3 2 a的反射,沿原路徑回到球心,再朝第一拋物面 型反射罩Mla射出。光線經由第一拋物面型反射罩331a的 反射成平行光,平行光再經第二拋物面型反射罩332a的反 射,最終光線匯聚於第二拋物面型反射罩3 3 2 a的焦點 F3321a。第六圖的優、缺點與第五圖相同。 【發明内容】 本發明的目的’在於提供一種集光模組,可有效縮小 Etendue,以提升光的利用效率。 因此,本集光模組包括 一聚光型的燈源系統,係一種使發光源所產生的光線共同200422560 V. Description of the invention (5) The first focus F 3 11 a on the ellipsoidal reflector 3 1 a is reflected by the ellipsoidal reflector 3 1 a, and the light on the left side of the light source 1 3 1 a passes through the ellipse. Spherical reflector 31a—After co-reflection, they collectively converge on the second focus F312a of the ellipsoid reflector 31 & In addition to improving the optical utilization efficiency, this part also has other disadvantages: (1) the assembly is not easy (2) the light reflected back by the spherical reflector is partially blocked by the electrode, resulting in a decrease in light utilization efficiency. (3) The “light blocked by the electrode” will heat the electrode and make it difficult to cool the electrode. (4) The component cost is too high, and all are not standard products. (5) The volume is too large. See Figure 6. This light source module is composed of a spherical reflector 3 2 a, two parabolic reflectors 331 a and 332 a, and a lamp tube I 3 a. The spherical center C321 of the spherical reflection unit 32a is concentric with the focal point F33 11a and the light source 131a of the first parabolic reflection unit Mia. The light from the lower half of the light source is reflected by the spherical reflector 3 2 a, returns to the center of the sphere along the original path, and is emitted toward the first parabolic reflector Mla. The light is reflected by the first parabolic reflector 331a into parallel light, and the parallel light is reflected by the second paraboloid reflector 332a. Finally, the light is collected at the focal point F3321a of the second paraboloid reflector 3 3 2a. The advantages and disadvantages of the sixth diagram are the same as those of the fifth diagram. [Summary of the Invention] The object of the present invention is to provide a light collection module, which can effectively reduce Etendue to improve the light utilization efficiency. Therefore, the light-concentrating module includes a light-condensing type light source system, which is a kind of common light source
74H 第8頁 200422560 五、發明說明(6) 聚焦於某一點上; 一反射罩,當光線會聚於其焦點再由反射罩反射時,可將 光線平行射出或是再次會聚於其第二焦點上或依預定目 的方向射出。 &、 在聚光型的燈源系統與反射罩的焦點之間光線的行經 路徑中,可裝置一傾斜的平面反射鏡,經由此傾斜平^ ^ 射鏡的作用,將可使聚光型的燈源系統的焦點位置轉折, 使光線聚焦於反射罩的焦點上;若反射罩為橢球面型反射 罩,則再將光線聚焦於反射罩之第二焦點上。 【實施方式】 參閱第七圖。本聚光型的燈源系統由下列元件組成: 一橢球面型燈泡11、位於橢球面型燈泡U前方之45。傾斜 板4、位於傾斜板4左侧之橢球面型反射罩31、位於橢球面 型反射罩之第二焦點F3 12處之柱狀積分器21。在45。傾斜 板4靠橢球面型燈泡丨丨的光線入射面有一層反射鍍膜層、/ 41,此反射面41可將可見光的頻譜波段全部反射;在此— 45。傾斜反射鏡面4與橢球面型燈泡丨丨的光軸Ain3的交會 處的週圍,將45。傾斜反射鏡面4鑽一小圓孔42,此小圓曰孔 的大小以不大於橢球面型燈泡丨丨之集光無效區。橢球面型 垃泡11的集光無效區的範圍為由橢球面型燈泡丨丨之虛焦點 F1113 (原橢球面型燈泡丨丨之第二焦點)a起,延伸至6 / 由B沿著橢球面型反射罩U1之内緣到c,再由〇至八。所 以,45傾斜反射鏡面4在橢球面型燈泡丨丨之集光無效區 一小圓孔42,對整體之集光效果影響很小。 200422560 五、發明說明(7) * 因此,由光源1 2 1所射出來的光線,先經過橢球面型 反射罩111的反射,原本該直接聚焦於橢球面型燈泡之第 二焦點FI 113,但由於先遇到45。平面反射鏡的反射鍍模面 41,所以折向橢球面型反射罩31之第一焦點F311聚焦。由 於橢球面型燈泡11的第二焦點F 111 2與橢球面型反射罩3 1 之第二焦點F311經由45 °平面反射鏡4的反射後重合,所以 橢球面型燈泡11之光線聚於橢球面型反射罩之第一焦點 F 3 11後,再向橢球面型反射罩3 1射出。經由橢球面型反射 罩的反射,光線穿過位於45。平面反射鏡面4的小圓孔42, 並匯聚於橢球面型反射罩3 1之第二焦點f 3 1 2。之後,光線 再經由柱狀積分器2 1進行均勻化。 本圖的優點有下列幾點:(一)由第七圖之簡易光線 追跡結果可見’橢球面型反射罩31之聚光點”^之立體角 較橢球面型燈泡1 1的聚光點!?丨丨丨2之立體角小許多; (二)有效縮小光線分佈的面積;(三)光束在本集光模 組内的上、下、左、右對稱性良好,容易達到螢幕上的亮 度的均勻度的要求;(四)圖中的三個主件—橢球面型燈 泡、平面反射鏡、橢球面型反射罩的取得容易,不容易被 少數供應商控制;(五)組裝容易。 參閱第八圖。第八圖與第七圖不同的是沒有傾斜平面 ^射,’但是在拋物面型反射罩33的對稱轴^31的轴線 ΐ他 水平平面反射鏡5自抛物面型反射罩33的基點332 产在舳㈣”卜./ 而其鍍膜反射面51 /口社釉線A 3 d 1上,此水平平而泠射於 >卞十面反射知^為一矩型反射鏡,74H Page 8 200422560 V. Description of the invention (6) Focus on a certain point; a reflector, when the light converges on its focus and is reflected by the reflector, the light can be emitted in parallel or converged on its second focus again Or shoot in the direction of the intended purpose. & In the light path between the light source system of the condensing type and the focal point of the reflector, an inclined flat mirror can be installed. Through the function of this inclined flat mirror, the condensing type The turning position of the focal point of the light source system is to make the light focus on the focus of the reflector; if the reflector is an ellipsoidal reflector, the light is focused on the second focus of the reflector. [Embodiment] Refer to the seventh figure. The condensing light source system is composed of the following components: an ellipsoidal bulb 11, 45 located in front of the ellipsoidal bulb U. The inclined plate 4, the ellipsoidal reflector 31 on the left side of the inclined plate 4, and the cylindrical integrator 21 at the second focal point F3 12 of the ellipsoidal reflector. At 45. The inclined plate 4 is based on an ellipsoidal bulb, and the light incident surface has a reflective coating layer, / 41. This reflecting surface 41 can reflect all the spectral bands of visible light; here-45. Around the intersection of the inclined mirror surface 4 and the optical axis Ain3 of the ellipsoidal bulb 丨 丨, will be 45. The inclined reflecting surface 4 is drilled with a small circular hole 42. The size of the small circular hole is not larger than the light collecting invalid area of the ellipsoidal bulb. The range of the ellipsoidal bulb 11's light-collection ineffective area is from the ellipsoidal bulb 丨 丨 the virtual focus F1113 (the second focus of the original ellipsoidal bulb 丨 丨), extending to 6 / from B along the ellipsoid The inner edge of the spherical reflector U1 goes to c, and then from 0 to eight. Therefore, a small circular hole 42 in the light-collecting ineffective area of the ellipsoidal light bulb 45 with a 45-inclined reflective mirror surface 4 has little effect on the overall light-collecting effect. 200422560 V. Description of the invention (7) * Therefore, the light emitted by the light source 1 2 1 is reflected by the ellipsoidal reflector 111, which should have focused directly on the second focus FI 113 of the ellipsoidal bulb, but Because first encountered 45. The reflecting plated surface 41 of the flat mirror is focused on the first focus F311 of the ellipsoidal reflector 31. Since the second focus F 111 2 of the ellipsoidal bulb 11 and the second focus F311 of the ellipsoidal reflector 3 1 coincide with each other after being reflected by the 45 ° plane mirror 4, the light from the ellipsoidal bulb 11 is concentrated on the ellipsoidal surface. After the first focal point F 3 11 of the reflective reflector is projected toward the ellipsoidal reflector 3 1. Through the reflection of the ellipsoidal reflector, the light passes through at 45. The small circular holes 42 of the plane reflecting mirror surface 4 are converged on the second focal point f 3 1 2 of the ellipsoidal reflecting cover 3 1. After that, the light is homogenized by the column integrator 21 again. The advantages of this picture are as follows: (1) From the simple ray tracing results of the seventh picture, it can be seen that the solid angle of the ellipsoidal reflector 31 is higher than that of the ellipsoidal bulb 11! ? 丨 丨 丨 2 The solid angle is much smaller; (2) Effectively reduce the area of light distribution; (3) The beam has good symmetry in the up, down, left, and right of the light module, and it is easy to reach the brightness on the screen (4) The three main parts in the picture-ellipsoidal bulb, flat reflector, and ellipsoidal reflector are easy to obtain and not easily controlled by a few suppliers; (5) Easy assembly. The eighth figure. The eighth figure is different from the seventh figure in that there is no oblique plane, but the axis of symmetry of the parabolic reflector 33, the axis 31 of the horizontal plane mirror 5 from the parabolic reflector 33. The base point 332 is produced by 舳 ㈣ ”Bu. / And its coating reflection surface 51 / mouth-shade glaze line A 3 d 1, this level is flat and radiated on the 卞 ten-sided reflection is known as a rectangular mirror,
742 第10頁 200422560 五、發明說明(8) 其對稱軸洽位於軸線A33 1上,且平面反射鏡的一直邊與拋 物面型反射罩33的焦點F3311相切。由於橢球面塑燈泡11 的聚焦點並非如數學上所定義的點沒有體積、大小的 點,而是聚在一個小區域(此處稱為聚光區)i 3上,且由 於橢球面型燈泡11為一對稱性的照射光源,所以聚光區的 光點也為對稱的。因此,水平平面反射鏡5與拋物面型反 射罩之焦點F 3 3 11相切的直邊,洽可將聚光區的光點等分 為左、右兩半部131及132。左半部131被水平平面反射鏡 反射’右半部1 3 2直進。故原來斜向入射於拋物面型反射 ^33的光束,經由水平平面反射鏡5的等分作用,轉為對 稱的兩個光束射向拋物面型反射罩33,因此光線即可對稱 的自拋物面型反射罩33射出。 立由於入射光束被水平平面反射鏡5分為左131、右132 兩部’所以也可被視為兩個聚焦點F334及?333, =別為下半抛物面型反射罩334…拋物面型反:單、 -隹點、、八點幻,二此上、τ兩個半拋物面型反射罩可以就此 一焦點刀別作最佳化設計。 ν ’ + u上所述者,僅為本發明之較佳實佳例而已,每 ! L及ί定本發明實施之範圍,即大A依本發明申請i 岸==書内容所作之簡單的等效變化與修飾, 應仍屬本發明專利涵蓋之範圍内。 200422560 圖式簡單說明 一 " ^- 本叙明之其他特徵及優點,在以下配合參考圖式之較佳實 施到的詳細說明中,將可清楚的明白,在圖式中: 、 第一圖是entendue的說明圖。 第二圖是一種習知的橢球面型反射罩之光源集光系 統’光線經由橢球反射面將光線反射並匯聚於橢球面之第 一焦點處,之後光線進入柱狀積分器進行光線均勻化的作 用。 第三圖是一種習知的拋物面燈的光源集光系統,光線 f由拋物面燈平行射出,經由一正透鏡,將光線聚於正透 鉍的^點上。之後再進入柱狀積分器進行光線均勻化。 第四圖為一習知小etendue的光源集光模組。燈管上 之石英圓球體(bulb of the burner)右半部表面上鍍有 =層反射層(可反射可見光部份),可將來自光源右半之 光線沿原路徑折回;而左半部為一橢球反射面。光源自左 ^部射向橢球反射罩的光線,反射並匯聚於橢球反射面之 弟一焦點處。本集光模組可提升光學效率2 〇〜3 0 %。 第五圖為一習知小etendue的光源集光模組。燈管的 左侧為一橢球面反射罩,燈管的右侧為一圓球面反射罩。 橢球面之第一焦點、圓球面之圓心、光源所在的位置,三 者共點。所以光源的右半側光線經由圓球面反射罩的反 射’沿原路徑經過圓心射向橢球面反射罩。左半側的光線 經由橢球反射罩匯聚於橢球反射罩之第二焦點處。 第六圖為一習知小etendue的光源集光模組。集光模 組由一燈管,及位於燈管下方的球面型反射罩及燈管上方742 Page 10 200422560 V. Description of the invention (8) The symmetry axis is located on the axis A33 1 and the straight side of the plane mirror is tangent to the focal point F3311 of the parabolic reflector 33. Because the focal point of the ellipsoidal plastic bulb 11 is not a point defined mathematically, it has no volume and size. Instead, it focuses on a small area (here called the light-concentrating area) i 3. 11 is a symmetrical illumination light source, so the light spots in the light-concentrating area are also symmetrical. Therefore, the straight edges that the tangent of the horizontal plane mirror 5 and the focal point F 3 3 11 of the parabolic reflector can divide the light spot of the light-concentrating area into the left and right halves 131 and 132 equally. The left half 131 is reflected by the horizontal plane mirror 'and the right half 1 3 2 goes straight. Therefore, the light beam originally incident on the parabolic reflection ^ 33 obliquely is converted into two symmetrical light beams to the parabolic reflection cover 33 through the equal division of the horizontal plane mirror 5. Therefore, the light can be reflected symmetrically from the paraboloid The hood 33 shoots. Since the incident light beam is divided into two parts, left 131 and right 132, by the horizontal plane mirror 5, it can also be regarded as two focus points F334 and? 333, = Don't use the lower half parabolic reflector 334 ... Parabolic inversion: single,-隹,, eight-point magic, two above, τ two semi-parabolic reflectors can be optimized for this focus design. ν '+ u The above is only a good example of the present invention. Each of L and 实施 determines the scope of implementation of the present invention, that is, a large A based on the application of the present invention. Effect changes and modifications should still fall within the scope of the patent of the present invention. 200422560 Schematic description of one " ^-Other features and advantages of this description, will be clearly understood in the following detailed description with reference to the preferred implementation of the schematic, in the diagram: The first diagram is An illustration of entendue. The second figure is a conventional ellipsoidal reflector light collection system. The light reflects and converges at the first focal point of the ellipsoid through the ellipsoidal reflection surface, and then the light enters the cylindrical integrator for uniform light Role. The third figure is a light source collecting system of a conventional parabolic lamp. The light f is emitted in parallel by the parabolic lamp, and the light is focused on the orthorhombic bismuth point through a positive lens. Then it enters the cylindrical integrator for light homogenization. The fourth picture shows a small etendue light collection module. The surface of the right half of the bulb of the burner on the tube is plated with a layer of reflective layer (which can reflect visible light), which can return the light from the right half of the light source along the original path; and the left half is An ellipsoidal reflecting surface. The light comes from the light from the left part towards the ellipsoidal reflector, and is reflected and converged at the focal point of the ellipsoidal reflecting surface. This light collecting module can improve the optical efficiency by 20 ~ 30%. The fifth picture shows a small etendue light collection module. The left side of the tube is an ellipsoidal reflector, and the right side of the tube is a spherical reflector. The first focus of the ellipsoid, the center of the sphere, and the location of the light source all have the same point. Therefore, the light from the right half of the light source is reflected by the spherical reflector through the circle along the original path to the ellipsoidal reflector. The light from the left half is collected at the second focal point of the ellipsoidal reflector through the ellipsoidal reflector. The sixth picture shows a small etendue light collection module. The light collecting module consists of a tube, and a spherical reflector and a tube above the tube.
200422560 圖式簡單說明 之雙拋物面反射罩組成。光源、球面型反射罩之球心、第 一抛物面反射罩之焦點’三點共點。光源下半部的光線經 由球面型反射罩反射沿原路徑通過光源再射向第一拋物面 鏡。光源上半部的光線及經由下半部反射來的光線,射向 第一拋物面反射罩後成平行光,平行光再射向第二拋物面 反射草’光線並匯聚於第二拋物面反射罩的焦點, 一柱狀積分器將光線均勻化後再利用。 ' 第七圖為本發明之集光系統之第一較佳實施例的俯視 圖。本集光模組由以下三項組成:一橢球燈、一 4 5。傾斜 且中央局部小區域鏤空的鏡面、一橢球面型反射罩。由於 45。傾斜鏡面的反射緣故,橢球燈之第二焦點位置與橢球 面型反射罩之第一焦點位置共點。來自橢球燈之光線經由 橢球面型反射罩反射之後,穿過45。傾斜之中央局部鏤空 之區域,匯聚於橢球面型反射罩的第二焦點處。 玉 第八圖為本發明之集光系統之第二較佳實施例的俯視 圖。擴球燈不經由任何的傾斜鏡面直接聚焦於拋物面型反 射f的焦點上,經由拋物面型反射罩的反射,光線成平行 光遠離反射罩。橢球燈之第二焦點與拋物面型反射罩之$ 點重合。然而使用一水平反射鏡於拋物面型反射罩内,; 使自橢球燈射出的光束一分為二,而得到上、下對稱的 行光自反射罩射出。 、” 【圖號說明】 〔習知〕 1 a燈泡200422560 Schematic illustration of a double parabolic reflector. The light source, the spherical center of the spherical reflector, and the focal point of the first parabolic reflector have three points in common. The light from the lower half of the light source is reflected by the spherical reflector and passes through the light source along the original path and then hits the first parabolic mirror. The light from the upper half of the light source and the light reflected from the lower half are directed to the first parabolic reflector to form parallel light, and the parallel light is then directed to the second parabolic reflector to reflect the grass' light and converge at the focus of the second parabolic reflector A cylindrical integrator will homogenize the light and reuse it. 'The seventh figure is a top view of the first preferred embodiment of the light collection system of the present invention. This collection light module is composed of the following three items: an ellipsoidal lamp and a 4 5. An ellipsoidal reflector with a slanted and hollowed out central small area. Since 45. For the reflection of the inclined mirror surface, the second focus position of the ellipsoidal lamp and the first focus position of the ellipsoidal reflector are in common. The light from the ellipsoidal lamp is reflected by an ellipsoidal reflector and passes through 45. The partially hollowed-out central area converges at the second focal point of the ellipsoidal reflector. The eighth figure is a top view of a second preferred embodiment of the light collecting system of the present invention. The ball light is focused directly on the focal point of the parabolic reflection f without any inclined mirror surface, and the light is parallelized away from the reflection cover through the reflection of the parabolic reflection cover. The second focus of the ellipsoidal light coincides with the $ point of the parabolic reflector. However, a horizontal reflector is used in the parabolic reflector, and the light beam emitted from the ellipsoid lamp is divided into two, so that the upward and downward symmetrical traveling light is emitted from the reflector. "" [Illustration of the drawing number] [Learning] 1 a bulb
200422560 圖式簡單課明 11 a橢球面型燈泡 111 a橢球面型反射罩 Fill la第一焦點 FI 112a第二焦點 1 1 1 2 a橢球面型反射罩的對稱軸 1 2 a拋物面型燈泡 1 2 1 a拋物面型反射罩 F 1 2 11 a焦點 1 3 a燈管 1 3 1 a光源 132a石英圓球體 1321a反射鍍膜層 1 3 2 2 a電極 A1 3 3燈管的軸線 2 a積分器 2 1 a柱積分器 22a矩陣透鏡積分器 3 a反射罩 31a橢球面型反射罩 311a半橢球面型反射罩 F 3 11 a橢球面型反射罩第一焦點 F 3 1 2 a橢球面型反射罩第二焦點 32a球面型反射罩 C 3 2 1球面型反射罩圓心200422560 Schematic Lesson 11 a Ellipsoidal bulb 111 a Ellipsoidal reflector Fill la First focus FI 112a Second focus 1 1 1 2 a Symmetry axis of an ellipsoidal reflector 1 2 a Parabolic bulb 1 2 1 a parabolic reflector F 1 2 11 a focus 1 3 a tube 1 3 1 a light source 132a quartz round sphere 1321a reflective coating 1 3 2 2 a electrode A1 3 3 axis of the tube 2 a integrator 2 1 a Column integrator 22a Matrix lens integrator 3 a Reflector 31a Ellipsoidal reflector 311a Semi-ellipsoidal reflector F 3 11 a Ellipsoidal reflector first focus F 3 1 2 a Ellipsoidal reflector 2nd focus 32a Spherical Reflector C 3 2 1 Spherical Reflector Center
第14頁 200422560Page 14 200422560
3 3 a拋物面型反射罩 331a第一拋物面型反射罩 F 3 3 11 a第一拋物面型反射罩焦點 332a第二拋物面型反射罩 F 3 3 2 1 a弟二抛物面型反射罩焦點 333a半拋物面型反射罩 4 a正透鏡 F 41 a正透鏡焦點 〔本發明〕 1燈泡 11橢球面型燈泡 111橢球面型反射罩 F 1111第一焦點 F 111 2第二焦點 F 111 3虚焦點 A111 3橢球面型反射罩之對稱軸 12燈管 1 2 1光源 1 2 2石英圓球體 1 3聚光區(點) 1 3 1聚焦點左半部 132聚焦點右半部 2積分器 2 1柱積分器3 3 a parabolic reflector 331a first parabolic reflector F 3 3 11 a first parabolic reflector 332a second parabolic reflector F 3 3 2 1 a second parabolic reflector 333a semi-parabolic Reflector 4 a positive lens F 41 a positive lens focus [invention] 1 bulb 11 ellipsoidal bulb 111 ellipsoidal reflector F 1111 first focus F 111 2 second focus F 111 3 virtual focus A111 3 ellipsoidal Axis of symmetry of the reflector 12 Light tube 1 2 1 Light source 1 2 2 Quartz sphere 1 3 Concentration area (point) 1 3 1 Focus point left half 132 Focus point right half 2 Integrator 2 1 Column integrator
200422560 圖式簡單說明 3反射罩 3 1橢球面型反射罩 F311橢球面型反射罩第一焦點 F312橢球面型反射罩第二焦點 33拋物面型反射罩 F3311拋物面型反射罩焦點 A331對稱軸 3 3 2基點 333上半拋物面型反射罩 F333上半拋物面型反射罩的焦點 334下半拋物面型反射罩 F334下半拋物面型反射罩的焦點 4 4 5 °平面反射鏡 41平面反射鏡鑛膜面 42平面反射鏡圓孔 5水平反射鏡面 5 1鑛膜反射面200422560 Brief description of the drawing 3 reflector 3 1 ellipsoidal reflector F311 ellipsoidal reflector first focus F312 ellipsoidal reflector 2nd focus 33 parabolic reflector F3311 parabolic reflector focus A331 symmetry axis 3 3 2 Base point 333 Upper half parabolic reflector F333 Focus point of upper half paraboloid reflector 334 Lower half paraboloid reflector F334 Focus of lower half paraboloid reflector 4 4 5 ° Plane mirror 41 Plane mirror Mineral film surface 42 Plane reflection Mirror round hole 5 horizontal reflecting mirror surface 5 1 mineral film reflecting surface
第16頁 74816 Page 748
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