TWI222505B - High efficient light collecting module for light source - Google Patents
High efficient light collecting module for light source Download PDFInfo
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^22505 ΐΓί ·|·「Π_ _ I Ι_ , 1 ' ' ~1 >_. wfc犯5· 2〇修正 年月Η4 五、發明說明(1) 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、调變、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 ^ ’以節省成本;並且在單位面積上的像素也愈來愈多使 知面板的穿透率降低,不僅如此,光的利用效率會隨著面 板面積的縮小而降低。故各廠家,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 cos ΘdAd Ω 而0 、dA、d Ω的關係可參閱第一圖。 此處dA表不光束所投影的面積,表示通過^之光束 的立體角’而0表示平面以的法向量與άΩ之中心轴的夾 角。 此方程式表示光束的幾合性質(ge〇metric proper ^ ),而光束的能量密度、強度、亮度等的性質, 並不在圪個方程式中被顯示出來。在同流明的光束下,當^ 22505 ΐΓί · | · 「Π_ _ I Ι_, 1 ′ ~ 1 > _. Wfc commits 5. · 20 revised year 4 Ⅴ. Description of the invention (1) The technical field to which the invention belongs] The present invention is a collection Optical module, using this technology can improve the light collection efficiency of the condensing light source. [Previous technology] ^ General projection display system devices all need to use the light collecting module to perform light splitting, modulation, light combining and imaging. However, The efficiency of light utilization is directly related to the performance of the brightness, uniformity, and color of the overall imaging quality. Not only that, as the price of projection displays declines, image modulation panels (such as DMD panels, etc.) used by projection displays ) 'S size is getting more and more ^' to save costs; and more and more pixels on a unit area reduce the transparency of the panel, not only that, the light utilization efficiency will decrease as the panel area shrinks. Therefore, various manufacturers are all dedicated to studying how to improve the utilization efficiency of the light source. Generally, to judge the efficiency of the light beam obtained by the light source through the reflector, it can be expressed by the parameter Etendue. And the equation is as follows: E = ^ 5 cos ΘdAd Ω and the relationship between 0, dA, d Ω can be seen in the first figure. Here dA represents the area projected by the light beam, which represents the solid angle of the light beam passing through ^, and 0 represents a plane The angle between the normal vector and the central axis of άΩ. This equation represents the geometric proper ^ of the beam, and the properties of the beam such as energy density, intensity, and brightness are not shown in one equation. . Under the same lumen beam, when
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五、發明說明(2)V. Description of the invention (2)
Et endue愈小,表示光束的面積、光束與平面法線的夾角 及光束之士體角的積分值是愈小的;也就是說,光的利用 效率也車乂回由以上的概念,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(參閱第二圖)及拋物面型燈泡(參閱第三 圖)在第圖中’光源131a置於橢球面型反射罩1113的 第一焦點F 1111 a上,由光源丨31 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丨12a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121&的 焦點F1 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2la進行 均勻化的處理。 由於反射罩與光源的搭配,還有其他因素須考量,諸 如光源的散熱問題、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 mercury lamp )光源的特性,使得聚光點的面積及光束的 立體角無法縮小。因此,當一般投影用的燈泡使用在小尺 寸的影像調變面板的之下,往往難以得到理想的光學效 圓The smaller the Et endue, the smaller the integrated value of the area of the beam, the angle between the beam and the plane normal, and the angle of the beam body angle; that is, the efficiency of light utilization is also reflected in the above concept, optical design Engineers can easily determine the light utilization efficiency of the light source module. The light collecting module generally used in projection displays can be roughly divided into ellipsoidal bulbs (see the second figure) and parabolic bulbs (see the third figure). In the figure, the light source 131a is placed in the ellipsoidal reflector 1113. At the first focal point F 1111 a, the light emitted by the light source 丨 31 a is focused on the second focal point F1 丨 12a through the ellipsoidal reflector 11 la, and the light enters the cylindrical integrator 21 a to be homogenized. , And then perform spectroscopic, combined light, imaging and so on. Referring to the third figure, the light source 131a is placed on the focal point F1 2 11 a of the parabolic reflector 121 & 'the light emitted by the light source is reflected by the paraboloid reflector 1 2 1 a' and the light is emitted parallel to each other The cover, through the positive lens 4a placed in front of the reflection cover, collects light on the columnar integrator 2la for uniform processing. 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 beam through the reflector cannot be reduced), and due to the characteristics of the UHP (ultra-high pressure mercury lamp) light source, the area of the focusing point and the beam The solid angle cannot be reduced. Therefore, when a general projection lamp is used under a small-sized image modulation panel, it is often difficult to obtain an ideal optical effect.
IMI 1222505 岣5%2〇修正](IMI 1222505 岣 5% 20)
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。 ^閱第四圖,此集光模組為Phi lips在這方面的傑 作。這是利用在燈管13a上的石英圓球體(bulb 〇f七“ burner) 132a的外表面為圓球面的特性,鍍上一層反射層 1321a,使得圓球體可以作為球面鏡,而將自光源131&所 韓射出來的光線,再折回原路徑,使得光源131&之發光角 I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132a (bulb of 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F丨丨丨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13213,使得由光源131a 所輻射出來的光線向右側射出的部份,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1118的第一焦點?111&處,所 以右半侧反射回來的光線重新經過第一焦點F丨丨丨&後,再 向左側射出。左側的光線,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111&的第二焦點F1112a 處。 由於最終光源1 31 a的光線只向左侧射出,再經由橢球 面型反射罩111a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?1113右半邊的反射罩皆用不V. Description of the invention (3) Rate. Therefore, manufacturers have no intention to change the above three factors (0, A, Ω) to improve optical efficiency. ^ See the fourth picture, this light module is the masterpiece of Phi lips in this respect. This is to take advantage of the characteristic of the outer surface of the quartz bulb sphere 132a on the lamp tube 13a as a spherical surface. A reflective layer 1321a is plated so that the spherical body can be used as a spherical mirror, and the light source 131 & The light emitted by the Korea is turned back to the original path, so that the light emitting angle I of the light source 131 & is half of the original, and achieves the effect of small etendue to improve the optical efficiency. The light source 131a is covered with a hollow quartz sphere 132a (bulb of the burner), and the light source 131 & is also located at the first focal point F 丨 丨 丨 a of the ellipsoidal reflector 111a. On the outer surface of the right half of the quartz sphere, a B-layer reflection The coating layer 13213 enables the part of the light emitted by the light source 131a to be emitted to the right side, and then reflects back to the center position of the quartz sphere 132a through the reflective coating layer 1321a. Because the light source 131a is placed in the ellipsoidal reflector 1118, The first focus is at 111 &, so the light reflected from the right half passes through the first focus F 丨 丨 丨 & and then exits to the left. The light on the left passes through the ellipsoidal reflector After the reflection of a, the light beam is converged at the second focus F1112a of the ellipsoidal reflector 111 & Since the light from the final light source 1 31 a only exits to the left and is focused by the ellipsoidal reflector 111a, The ellipsoidal reflector in the second figure is significantly smaller than the ellipsoidal reflector in the fourth figure. That is, the first focus of the ellipsoidal reflector? 1113 The reflector on the right half is not used.
1222505 % 5· 2 〇 修£ 年月Θ 4 乂— 獻. 五、發明說明(4) 到,所以可取消。由Philips於20 0 2 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(5〜15mnT2 ster ),收光效率可提升2〇 -3 0%。1222505% 5 · 2 〇 Revised Year and Month Θ 4 乂 — Contribution. V. Description of the Invention (4) has arrived, so it can be cancelled. According to a paper published by Philips in the 20 2 SID (Holger Moench, Arnd Ritz, Higher Output, More Compact UHP Lamp Systems, SID 02), it can be seen that under the condition of small Etendue (5 ~ 15mnT2 ster), the light collection efficiency can be improved 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 南熱及南壓’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 132a之反射鍍膜層1321a反射回來的光線有部份會被電極 1 32 2a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Phi 1 ips生產。 參閱第五圖。此光源模組為美國專利(US 63567〇〇 B1)由一件橢球面型反射罩3ia及一件球面型反射罩328組 成’其中光源131a被置於橢球面型反射罩3ia之第一焦點 F311a上,而球面型反射罩32a之球心C321與橢球面型反射 罩之第一焦點F31 la與光源131a都共點。而燈管13a的對稱 軸A133與光軸(光轴系橢球面型反射罩gia之第一焦點 F 3 11 a及第二焦點f 31 2 a的連線)垂直。光源右半側的光線 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 sphere 132a is permanently deformed: Because the south heat and pressure generated by the UHP lamp during use will cause the quartz sphere to deform and reflect, The returned 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: Part of the light reflected by the reflective coating 1321a of the quartz sphere 132a will be blocked by the electrode 1 32 2a, 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 source of supply: This special light source module is only produced by Phi 1 ips. See Figure 5. This light source module is a U.S. patent (US 63567〇B1) consisting of an ellipsoidal reflector 3ia and a spherical reflector 328 'where the light source 131a is placed at the first focus F311a of the ellipsoidal reflector 3ia On the other hand, the spherical center C321 of the spherical reflector 32a and the first focal point F31a of the ellipsoidal reflector are in common with the light source 131a. The symmetry axis A133 of the lamp tube 13a is perpendicular to the optical axis (the line connecting the first focus F 3 11 a and the second focus f 31 2 a of the ellipsoidal reflector gia of the optical axis system). 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.
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第一焦點F31 la到橢球面型反射罩31&上,經橢球面型反射 罩3 1 a反射後,與光源1 3 1 a左側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3ia之 隹 點F3 12a 上。 一 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,有部伤會被電極遮播,造成光利用效率降低。(三) 承上,被電極遮擋的光線,會加熱電極,造成電極冷&困 難。(四)組件成本過高,均非標準品。(五)體積過 大0 參閱第六圖。此光源模組由一件球狀型反射罩M a及 兩個抛物面型反射罩331a、332a並一燈管i3a組成。球面 型反射罩32a的球心C321與第一拋物面型反射罩331a的焦 點F331 la及光源131a共心。光源下半侧的光線經由球面型 反射罩32a的反射,沿原路徑回到球心,再朝第一拋物面 型反射罩331a射出。光線經由第一拋物面型反射罩331&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 32a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 t光型的燈源系統’係一種使發光源所產生的光線共同The first focal point F31 la is on the ellipsoidal reflector 31 &, after being reflected by the ellipsoidal reflector 3 1 a, the light on the left side of the light source 1 3 1 a passes through the ellipsoidal reflector 31a-after the same reflection, they converge together. At the point F3 12a of the ellipsoidal reflector 3ia. 1. In addition to improving the efficiency of optical use, this piece has other disadvantages: (1) it is not easy to assemble (2) the light reflected back by the spherical reflector, and some injuries will be covered by the electrode, which will reduce the light use efficiency. (3) The light blocked by the electrode will heat the electrode, making the electrode cold & difficult. (4) The component cost is too high, and all are not standard products. (V) Volume is too large 0 Refer to the sixth figure. This light source module is composed of a spherical reflecting cover Ma, two parabolic reflecting covers 331a, 332a, and a lamp tube i3a. The spherical center C321 of the spherical reflector 32a is concentric with the focal point F331a of the first parabolic reflector 331a and the light source 131a. The light from the lower half of the light source is reflected by the spherical reflector 32a, returns to the center of the sphere along the original path, and is emitted toward the first parabolic reflector 331a. The light is reflected by the first parabolic reflector 331 & 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 32a. 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 collecting module, which can effectively reduce Etendue to improve light utilization efficiency. Therefore, the light-collecting module includes a t-light type light source system, which is a type of light source
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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的目 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,經由此傾斜平面反 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、位於橢球面型燈泡丨丨前方之4 5。傾斜 板4、位於傾斜板4左側之橢球面型反射罩3丨、位於橢球面 型反射罩之第二焦點F312處之柱狀積分器21。在45。傾斜 板4靠橢球面型燈泡11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;在此一 45。傾斜反射鏡面4與橢球面型燈泡1丨的光軸人1113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 燈泡11的集光無效區的範圍為由橢球面型燈泡丨丨之虛焦點 F111 3 (原橢球面型燈泡11之第二焦點)a起,延伸至b, 由β沿著橢球面型反射罩111之内緣到C,再由c至A。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鑽 一小圓孔42,對整體之集光效果影響很小。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 refocused on its second focus or in a predetermined direction. An inclined plane reflector can be installed in the path of light between the spotlight-type light source system and the focal point of the reflector, and the effect of the spotlight-type light source system can be achieved by the function of the inclined plane reflector. The focus position is turned so that the light is focused 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, and 4 5 in front of the ellipsoidal bulb. The inclined plate 4, the ellipsoidal reflector 3 丨 located on the left side of the inclined plate 4, and the cylindrical integrator 21 at the second focus point F312 of the ellipsoidal reflector. At 45. The inclined plate 4 has a reflective coating layer 41 on the light incident surface of the ellipsoidal bulb 11, and the 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 person 1113 of the ellipsoidal bulb 1, the 45 ° inclined reflection mirror 4 is drilled into a small circular hole 42. The size of the small circular hole is not larger than the ellipsoidal bulb.丨 The light collection invalid area. The range of the light collection ineffective area of the ellipsoidal bulb 11 is from the virtual focus F111 3 of the ellipsoidal bulb 丨 丨 (the second focus of the original ellipsoidal bulb 11) to a, extending from β along the ellipsoidal surface. The inner edge of the reflector 111 goes to C, and then from c to A. Therefore, a small circular hole 42 is drilled in the light-collecting ineffective area of the ellipsoidal light bulb 丨 45 ° inclined reflecting mirror surface 4 and has little effect on the overall light-collecting effect.
第9頁 1222505 五、發明說明(7)Page 9 1222505 V. Description of the invention (7)
因此,由光源1 21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F 111 3,但由於先遇到4 5 °平面反射鏡的反射鍍模面 4 1,所以折向橢球面型反射罩3 1之第一焦點F 3 11聚焦。由 於橢球面型燈泡11的第二焦點FI 11 2與橢球面型反射罩3 ! 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 F3 11後,再向橢球面型反射罩31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31之第二焦點F312。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!^12之立體角 較橢球面型燈泡11的聚光點F 111 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 反射鏡,但是在拋物面型反射罩33的對稱轴A331的轴線 2有一水平平面反射鏡5自拋物面型反射罩33的基點332 物面型反射罩的焦點F3311,而其鍍膜反射㈣ 化在軸線A331上;此水平平面反射鏡5為一矩型反射鏡,Therefore, the light emitted by the light source 1 21 is reflected by the ellipsoidal reflector 111 first, which should have been directly focused on the second focus F 111 3 of the ellipsoidal bulb, but because it first encountered 4 5 ° plane reflection The reflecting plated surface 41 of the mirror is focused on the first focus F 3 11 of the ellipsoidal reflector 3 1. Since the second focal point FI 11 2 of the ellipsoidal bulb 11 and the second focal point F311 of the ellipsoidal reflector 3! Overlap after being reflected by the 45 ° plane mirror 4, the light of the ellipsoidal bulb 11 is concentrated on the ellipsoidal surface. After the first focal point F3 11 of the reflective reflector is projected toward the ellipsoidal reflector 31. Through the reflection of the ellipsoidal reflector, the light passes through the small circular hole 42 located on the 45 ° plane reflector 4 and converges at the second focus F312 of the ellipsoidal reflector 31. After that, the light is homogenized by the column integrator 21 again. The advantages of this picture are as follows: (1) As can be seen from the simple ray tracing results of the seventh picture, the focusing point of the ellipsoidal reflector 31! The solid angle of ^ 12 is greater than the focusing point F of the ellipsoidal bulb 11. The solid angle of 111 2 is much smaller; (2) Effectively reduce the area of light distribution; (3) The symmetry of the top, bottom, left, and right of the beam in the light collection module is good, and it is easy to achieve the uniformity of 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 to assemble. See figure eight. The eighth figure differs from the seventh figure in that there is no inclined plane mirror, but there is a horizontal plane mirror 5 on the axis 2 of the symmetry axis A331 of the parabolic reflector 33. The base surface 332 of the parabolic reflector 33 reflects the object. The focal point of the cover is F3311, and its coating is reflected on the axis A331; this horizontal plane mirror 5 is a rectangular mirror,
第10頁 1222505 五、發明說明(8)Page 10 1222505 V. Description of the invention (8)
其對稱軸洽位於轴線A 3 31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。由於橢球面型燈泡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)1 3上,且由 於擴球面型燈泡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F3311相切的直邊,洽可將聚光區的光點等分 為左、右兩半部丨31及132。左半部131被水平平面反射鏡 反射,右半部132直進。故原來斜向入射於拋物面型反射 罩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。 由於入射光束被水平平面反射鏡5分為左、右M2 兩部,所以也可被視為兩個聚焦點以^及以33,兩個 點分別為下半拋物面型反射罩334、上半拋物面型反射罩、、 333之焦點,因此上、下兩個半拋物面型反 二焦點分別作最佳化設計。 早 乂就此 惟以上所述者,僅為本發明之較佳實佳例而已,舍 能以此限定本發明實施之範圍,大凡依本 抹: :圍=明說明書内容所作之簡單的等效變化與修ς,皆】 應仍屬本發明專利涵蓋之範圍内。Its axis of symmetry lies on the axis A 3 31, and the straight side of the flat mirror is tangent to the focal point F3311 of the parabolic reflector 33. Because the focal point of the ellipsoidal bulb 11 is not a point defined mathematically-a point with no volume or size ', it is concentrated on a small area (here called the light-concentrating area) 1 3, and because of the spherical shape The bulb 11 is a symmetrical illumination light source, so the light spots in the light-concentrating region are also symmetrical. Therefore, the straight edges of the horizontal plane mirror 5 and the focal point F3311 of the parabolic reflector can bisect the light spots in the light-concentrating area into the left and right halves 31 and 132. The left half 131 is reflected by a horizontal plane mirror, and the right half 132 advances straight. Therefore, the light beam originally incident on the parabolic reflector 33 obliquely is converted into two symmetrical beams to the parabolic reflector 33 via the equal division of the horizontal plane mirror 5, so the light can be reflected symmetrically from the parabolic reflector. The hood 33 shoots. Since the incident light beam is divided into left and right M2 by the horizontal plane mirror 5, it can also be regarded as two focus points ^ and 33. The two points are the lower half parabolic reflector 334 and the upper half paraboloid. The focal points of the two reflectors, 333, so the upper and lower half parabolic anti-two focal points are optimized. As long as this is the case, the above is only a good example of the present invention. It can be used to limit the scope of the implementation of the present invention. Anyone who follows this guide: And repair, both should still fall within the scope of the invention patent.
12225051222505
本發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 二焦點處,之後光線進入柱狀積分器進行光線均勻化的作 用0 第三圖是一種習知的拋物面燈的光源集光系統,光線 經由拋物面燈平行射出,經由一正透鏡,將光線聚於正透 鏡的焦點上。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)右半部表面上鑛有 =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 半部射向橢球反射罩的光線,反射並匯聚於橢球反射面之 第二焦點處。本集光模組可提升光學效率2 〇〜3 〇 %。 第五圖為一習知小etendue的光源集光模組。燈管的 左側為一橢球面反射罩,燈管的右側為一圓球面反射罩。 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Other features and advantages of the present invention will be clearly understood in the following detailed description with reference to the preferred implementation of the drawings. In the drawings: The first figure is an explanatory diagram of the enterprise. The second figure is a light collection system of a conventional ellipsoidal reflector. The light reflects and converges at the second focal point of the ellipsoid through the ellipsoidal reflection surface, and then the light enters the cylindrical integrator to uniformize the light. The third figure is a light source light collecting system of a conventional parabolic lamp. The light is emitted in parallel through the parabolic lamp, and the light is focused on the focal point of the positive lens through a positive lens. Then it enters the cylindrical integrator for light homogenization. The fourth picture shows a small etendue light collection module. There is a layer of reflective layer (which can reflect visible light) on the surface of the right half of the quartz bulb of the burner on the lamp tube, 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 half toward the ellipsoidal reflector, and is reflected and converged at the second focal point of the ellipsoidal reflective 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.
1222505 圖式簡單說明 之雙拋物面反射罩組成 一拋物面反射罩之焦點 由球面 鏡。光 第一拋 反射罩 一柱狀 第 圖。本 且中央 45 °傾 面型反 擴球面 之區域 第 圖。橢 射罩的 光遠離 點重合 使自橢 行光自 【圖號 〔習知 la燈泡 型反射 源上半 物面反 ,光線 積分器 七圖為 集光模 局部小 斜鏡面 射罩之 型反射 ,匯聚 八圖為 球燈不 焦點上 反射罩 。然而 球燈射 反射罩 說明】 罩反射沿原 部的光線及 射罩後成平 並匯聚於第 將光線均勻 本發明之集 組由以下三 區域鏤空的 的反射緣故 第一焦點位 罩反射之後 於橢球面型 本發明之集 經由任何的 ,經由拋物 。橢球燈之 使用一水平 出的光束一 射出。 光源、球面型反射罩之球心、第 三點共點。光源下半部的光線經 路徑通過光源再射向第一拋物面 經由下半部反射來的光線,射向 行光,平行光再射向第二拋物面 二拋物面反射罩的焦點,再經由 化後再利用。 光系統之第一較佳實施例的俯視 項組成··一橢球燈、一 4 5。傾斜 鏡面、一橢球面型反射罩。由於 ’橢球燈之第二焦點位置與橢球 置共點。來自橢球燈之光線經由 ,穿過45 °傾斜之中央局部鏤空 反射罩的第二焦點處。 光系統之第二較佳實施例的俯視 傾斜鏡面直接聚焦於拋物面型反 面型反射罩的反射,光線成平行 第一焦點與拋物面型反射罩之焦 反射鏡於拋物面型反射罩内,可 分為二,而得到上、下對稱的平 1222505 年月日補充 圖式簡單說明 11 a橢球面型燈泡 111a橢球面型反射罩 F 1111 a第一焦點 FI 112a第二焦點 111 2a橢球面型反射罩的對稱軸 12a拋物面型燈泡 121a拋物面型反射罩 F 1 2 11 a焦點 13a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 2a積分器 2 1 a柱積分器 22a矩陣透鏡積分器 3a反射罩 31a橢球面型反射罩 311a半橢球面型反射罩 F31 la橢球面型反射罩第一焦點 F312a橢球面型反射罩第二焦點 32a球面型反射罩 C321球面型反射罩圓心1222505 Brief description of the diagram The double parabolic reflector is composed of a focal point of a parabolic reflector by a spherical mirror. Light first throw Reflector a cylindrical figure. This is the area with a 45 ° inclination in the center. The light from the ellipsoidal hood coincides with the ellipsoidal light from the top half of the plane [the conventional la bulb-type reflection source. The seventh figure of the light integrator is the reflection of the local small oblique mirror hood that collects the light. Converging eight pictures show the reflector on the focus of the ball light. However, the ball lamp shoots the reflection cover] The cover reflects the light along the original part and the cover is flattened and converged on the first. The set of the present invention is uniformly reflected by the following three areas. The spherical type of the present invention passes through any, through parabolic. The ellipsoidal light uses a horizontal beam of light. The light source, the spherical center of the spherical reflector, and the third point in common. The light from the lower half of the light source passes through the light source and then hits the first parabolic surface. The light reflected from the lower half is directed to the traveling light. The parallel light is then directed to the focus of the second parabolic reflector and the second parabolic reflector. use. The top view of the first preferred embodiment of the light system is composed of an ellipsoidal lamp and a 4-5. Tilt mirror, an ellipsoidal reflector. Because the second focus position of the ellipsoidal lamp is in common with the ellipsoidal position. The light from the ellipsoidal lamp passes through the second focal point of the reflector, which is partially hollowed out at the center inclined at 45 °. The plan view of the second preferred embodiment of the optical system is directly focused on the reflection of the parabolic reflector, the light is parallel to the first focal point and the focal reflector of the parabolic reflector is inside the parabolic reflector, which can be divided into Second, and get the upper and lower symmetric flat 1225505 supplementary drawings for a simple explanation 11 a ellipsoidal bulb 111a ellipsoidal reflector F 1111 a first focus FI 112a second focus 111 2a ellipsoidal reflector Symmetry axis 12a Parabolic bulb 121a Parabolic reflector F 1 2 11 a Focus 13a Tube 1 3 1 a Light source 132a Quartz sphere 1321a Reflective coating 1 3 2 2 a Electrode A1 3 3 Axis of the tube 2a Integrator 2 1 a column integrator 22a matrix lens integrator 3a reflector 31a ellipsoidal reflector 311a semi-ellipsoidal reflector F31 la ellipsoidal reflector first focus F312a ellipsoidal reflector 2nd focal point 32a spherical reflector C321 Spherical Reflector Center
第14頁 修 1222505Page 14 Rev. 1222505
1W1U 圖式簡單說明 33a拋物面型反射罩 331a第一拋物面型反射罩 F3311a第一拋物面型反射罩焦點 332a第二拋物面型反射罩 F332 1 a第二拋物面型反射罩焦點 333a半拋物面型反射罩 4a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 F1111第一焦點 F111 2第二焦點 F111 3虛焦點 A111 3橢球面塑反射罩之對稱軸 12燈管 1 21光源 122石英圓球體 1 3聚光區(點) 1 31聚焦點左半部 132聚焦點右半部 2積分器 21柱積分器1W1U Brief Description of Drawings 33a Parabolic Reflector 331a First Parabolic Reflector F3311a First Parabolic Reflector Focus 332a Second Parabolic Reflector F332 1a Second Parabolic Reflector Focus 333a Half Parabolic Reflector 4a Positive Lens F 41 a Positive lens focus [Invention] 1 Bulb 11 Ellipsoidal bulb 111 Ellipsoidal reflector F1111 First focus F111 2 Second focus F111 3 Virtual focus A111 3 Spherical axis of plastic reflector 12 Light tube 1 21 Light source 122 Quartz sphere 1 3 Concentrating area (point) 1 31 Focus point Left half 132 Focus point Right half 2 Integrator 21-pillar integrator
第15頁 1222505 9a 5. 2〇#[[: 年月日V > 圖式簡單說明 3反射罩 31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 F 3 3 11拋物面型反射罩焦點 A 3 31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 45 °平面反射鏡 41平面反射鏡鍍膜面 42平面反射鏡圓孔 5水平反射鏡面 51鍍膜反射面Page 15 12225505 9a 5. 2〇 # [[: Month Day V > Brief description of the drawing 3 reflection cover 31 ellipsoidal reflection cover F311 ellipsoidal reflection cover first focus F312 ellipsoidal reflection cover second focus 33 Parabolic reflector F 3 3 11 Parabolic reflector focus A 3 31 Symmetry axis 3 3 2 Base point 333 Upper parabolic reflector F333 Focus of upper paraboloid reflector 334 Lower paraboloid reflector F334 Lower paraboloid Focus of the reflector 4 45 ° plane mirror 41 plane mirror coating surface 42 plane mirror round hole 5 horizontal mirror surface 51 coating reflection surface
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TW92109845A TWI222505B (en) | 2003-04-24 | 2003-04-24 | High efficient light collecting module for light source |
Country Status (1)
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TW (1) | TWI222505B (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI451035B (en) * | 2008-01-25 | 2014-09-01 | Osram Gmbh | Ac reflector lamp |
-
2003
- 2003-04-24 TW TW92109845A patent/TWI222505B/en not_active IP Right Cessation
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI451035B (en) * | 2008-01-25 | 2014-09-01 | Osram Gmbh | Ac reflector lamp |
Also Published As
Publication number | Publication date |
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TW200422560A (en) | 2004-11-01 |
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MM4A | Annulment or lapse of patent due to non-payment of fees |