五、新型說明： 【新型所屬之技術領域】 本創作係與發光二極體透鏡領域相關，特別是關 於一種利用聚光原理而得加強光強，且可均勻照射效 果並呈現出一類矩形照明區域之偏光式路燈光學透 鏡。 【先前技術】 發光二極體（Light Emitting Diode，LED)相較於 一般傳統光源而言，係具有低電壓、低耗電、壽命長 等優點。因此，LED於現今生活中已被廣泛地應用於 各種需光源提供之特殊相關領域。例如，運用於顯示 器之背光模組，指示燈光源，一般照明設備等等。其 中由於LED具有特別顯著之節能省電優勢，故在最為 印遍運用之照明目的下，其實用性便顯得格外重要。 例如將LED光源運用於夜間路燈之照明實施即為其 示例。 然，相較於傳統光源，發光二極體之光線發散角 度較小，以致於運用於路燈之照明時，中心亮度過於 集中，進而導致路燈鄰近處與遠離處之亮度大小差異 甚鉅，無法有效均句地提供路面照明。對此，嘗有利 用二次光學原理用以改變LED投射出之光學性能而 對於各種不同之使用條件下，皆能提供最佳之照明狀 嘘。以兩側路燈為例，其照明要求至少需能夠呈現— 類矩形區域之照明效果，用以提供於平行道路走向與 M395836 垂直道路走向皆能於其涵蓋範圍内。因此，如何有效 針對該LED光源之投射強度、投射範圍，以及其照射 均勾度進行改善’係為本領域相關從業者極欲改善之 課題。 有鑑於此，本創作人感其未臻完善而竭其心智苦 心研究’並憑其從事該項產業多年之累積經驗，針對 現行路燈普遍向度及路面長寬比例，已陸續提出並經 核准公告在案之台灣公告號M380480專利，利用非對 稱式之透鏡結構特性’使LED光源經該透鏡後得以產 生偏移照射區域之效果。於此本創作人係更進一步研 發出一種可利用聚光原理而得加強光強，且可均勻照 射效果並呈現出一類矩形照明區域之偏光式路燈光 學透鏡’徹底將LED光源有效照射於路面，而於加強 夜間行車及用路人安全之際，又能達到兼具節能省碳 之環保要求。 【新型内容】 鑑於上述問題，本創作之目的在於提供一種利用 一-人光學原理進而改變LED之光學特性之偏光式路 燈光學透鏡。藉此，用以達到加強光照射強度，均勻 …、射效果並呈現出一類矩形照明區域之特殊效果，使 於加強夜間行車及用路人安全之際，又能達到兼具節 能省碳之環保要求。 為達上述目的，本創作係提出一種偏光式路燈光 學透鏡，具有一透鏡本體，包含：一投射曲面，係由 M395836 為使貴審查委員能清楚了解本創作之内容，謹 以下列說明搭配圖式，敬請參閱。 請參閱第1、2、3及4圖，係分別為本創作之立 體外觀圖、本創作於X-Z平面之側視圖、於χ·γ平面 之上視圖及於Υ-Ζ平面之剖視圖。由圖觀之，本創作 係提供一種偏光式路燈光學透鏡，具有一透鏡本體 - 卜包含：一投射曲面10及一底面12。其中該投射曲 Φ 面1 〇係由複數個曲面點1 〇2所組成。利用幾何學原 理，由點構成線，線構成面之基礎概念，將該投射曲 面10上之該等曲面點102表列，藉此進一步定義曲 線與曲面，而給定之該等曲面點102多寡亦將決定該 杈射曲面10之平滑程度。由於工程上利用該等曲面 點102建立曲線及曲面之方式有多種作法，於此並不 加以詳述。主要係利用光滑連接之概念，使之得以保 證曲線在給定之曲面點1〇2處連接，使切線連續以及 • 曲線曲率連續，進而再架構出該投射曲面10。 - 於此’本創作所提供之偏光式路燈光學透鏡於空 間中係利用二維座標將各曲面點1 〇2表列其相應位 置。其中該投射曲面1〇邊緣係形成一基準面1〇4，且 該基準面1〇4具有一長軸1〇6與—短轴1〇8，以該長 軸1〇6為Χ軸方向、該短軸108為Υ軸方向，（1為一 單位座標長，該長軸與該短軸1〇8相交處為三維 座標原點，其中該等曲面點102於χ-ζ座標平面上， 具有各點（χ’ζ)為（〇,7 29)、U 84 7 叫、（3 97 7 28)、 7 M395836 (6.18,6.81) 、 (7.76,6.03) 、 (9.04,4.88)、 (9.80,3.59)、（1〇·〇9,2.00)、（1〇 〇9，14〇)、（ι〇 〇9 〇);於χ-γ座標平面上，具有各點（x，y)為（〇,6 49)、’ (1.70,6.62) ' (3.62,6.94) . (5.47,6.91) ' (7.20,6.45) ^ (8.54,5.54)、（9.49,4.08)、（9.96,2.50)、（10.〇9，i.〇4)、 (1 0·02,0)以及（0,-5.06)、（ U U 32)、（2 66，_5 66)、 (4.03,-5.68)、（5.47,-5.44)、（6.67,-4,97)、（7.77,-4.23)、 (8.58,-3.39)、（9.23,-2.42)、（9.70，-1.36)、（ι0·01〇); 於γ-ζ座標平面上，具有各點（y z)為（〇 7 28)、 (0.99,7.32) ^ (2.19,7.20) . (3.40,6.84) ' (4.60,6.18) > (5.37,5.52)、（5.99,4.76)、（6.53,3.81)、（6.88,2·78) ' (6.89,0.88) 、（6.72,〇)以及（〇,7.28)、（-0.84,7.14)、 (·1·68,6·90)、 （-2.47,6.55)、 （·3.24,6.10)、 （-4.07,5·43)、 (-4.6 5,4.8 0)' (-5.19,4.02)> (.5.70,2.40)' (-5.48,0.90). (-5.11，0)。因此該等曲面點1〇2至χ、γ、ζ軸之距離 係將該相應之（x，y，z)座標再分別乘以該單位座標長d 即是，例如（xd，yd，zd)。 又該等曲面點102至Χ、γ、z轴距離分別亦可容 許具有一相對誤差p，且·d/2〇SpSd/2〇。因此於該 相對誤差範圍β ’亦為本創作所欲主張之權利範圍: 而該底面12其邊緣與該基準面1〇4邊緣係相互連接 形成該透鏡本體卜且該底面12中心處内凹形成一容 置室122,供以容置發光二極體之用。該透鏡本體ι 係以Υ-Ζ面為基礎，僅鏡向對稱於χ軸方向。而於以 8 M395836 型扣具’進而相對於該led基板以旋合之方式將該偏 光式路燈光學透鏡固定於上。 本創作之功效在於利用偏光式路燈光學透鏡之 非球面寬照角度設計，使發光二極體之光源經該偏光 式路燈光學透鏡後產生折射效果，使其光線投射之照 明區域大致對應於長短轴方向基準面而成兩側對稱 之照明效果。又利用非對稱之透鏡本體結構，達到偏 I 光式之效果’使整體照明區域有所偏移，而得以更有 效且適切地照射於路面。據此，確能徹底將LED光源 有效照射於路面，而於使用LED燈具達到兼具節能省 碳環保要求之際，又能加強夜間行車及用路人安全。 以上所述者，僅為本創作之較佳實施例而已，並 非用以限定本創作會# α阁 令』卞貫鈿之範圍，故此等熟習此技術所 作出等效或輕易的變 " 變化者在不脫離本創作之精神與 範圍下所作之均等蠻仆命 變化與修飾，皆應涵蓋於本創作之 _ 專利範圍内。 M395836 【圖式簡單說明】 第 1 圖 為 本創 作 之 立體 外觀 圖 〇 第 2 圖 為 本創 作 於 X-Z 平面 之 側視圖。 第 3 圖 為 本創 作 於 X-Y 平面 之 上視圖。 第 4 圖 為 本創 作 於 Y-Z 平面 之 剖視圖。 第 5 圖 為 本創 作 於 X-Z 平面 之 光線路徑不意圖。 第 6 圖 為 本創 作 於 Y-Z 平面 之 光線路徑不意圖。 第 7 圖 為 本創 作 搭載LED使 .用 之等照分布圖。 第 8 圖 為 本創 作 搭 載LED使 .用 之配光曲線圖。 第 9 圖 為 本創 作 具 卡合 部之 立 體外觀圖。 【主要元件符號說明】 1 透鏡本體 10 投射曲面 102 曲面點 104 基準面 106 長軸 108 短軸 12 底面 122 容置室 2 卡合部 12V. New description: [New technology field] This creation is related to the field of light-emitting diode lenses, especially regarding the use of the principle of concentrating to enhance the light intensity, and can evenly illuminate the effect and present a kind of rectangular illumination area. Polarized street light optical lens. [Prior Art] Light Emitting Diode (LED) has the advantages of low voltage, low power consumption, and long life compared to conventional light sources. Therefore, LEDs have been widely used in various related fields where light sources are required in today's life. For example, a backlight module for a display, an indicator light source, a general lighting device, and the like. Among them, LED has a particularly significant energy-saving and power-saving advantage, so its practicality is particularly important in the most widely used lighting purposes. For example, the application of LED light sources to the illumination of nighttime streetlights is an example of this. However, compared with the conventional light source, the light diverging angle of the light-emitting diode is small, so that when the light is applied to the illumination of the street lamp, the central brightness is too concentrated, which causes the brightness of the vicinity of the street lamp to be different from the distance, and cannot be effective. Provide street lighting in a uniform manner. In this regard, it is advantageous to use the secondary optics principle to change the optical properties projected by the LEDs to provide optimum illumination for a variety of different conditions of use. For example, the streetlights on both sides need to be able to present at least the illumination effect of the rectangular-like area, which can be provided in the parallel road direction and the M395836 vertical road direction. Therefore, how to effectively improve the projection intensity, projection range, and illumination uniformity of the LED light source is a problem that the practitioners in the field are eager to improve. In view of this, the creator feels that he has tried his best to study and 'has been working hard on the industry's accumulated experience. For the current general trend of street lamps and the length and width of roads, they have been proposed and approved. In the Taiwan Patent No. M380480 patent, the effect of offsetting the illumination area is obtained by using the asymmetric lens structure characteristic to make the LED light source pass through the lens. The creator further developed a polarized streetlight optical lens that can enhance the light intensity by using the principle of concentrating, and can uniformly illuminate the effect and present a kind of rectangular illumination area, and completely illuminate the LED light source on the road surface. In order to strengthen the night driving and the safety of passers-by, it can meet the environmental protection requirements of both energy saving and carbon saving. [New content] In view of the above problems, the purpose of the present invention is to provide a polarized streetlight optical lens that utilizes the one-human optical principle to further change the optical characteristics of the LED. In this way, it is used to enhance the intensity of light irradiation, uniformity, and effect, and presents a special effect of a kind of rectangular illumination area, so as to enhance the environmental protection requirements of energy saving and carbon saving while strengthening night driving and safety of passers-by. . In order to achieve the above objectives, the present invention proposes a polarized streetlight optical lens having a lens body comprising: a projection curved surface, which is used by M395836 to enable the reviewing committee to clearly understand the content of the creation. Please see. Please refer to Figures 1, 2, 3 and 4, which are the exterior views of the original creation, the side view of the creation on the X-Z plane, the top view on the χ·γ plane, and the cross-sectional view on the Υ-Ζ plane. In view of the above, the present invention provides a polarized street light optical lens having a lens body - including a projection curved surface 10 and a bottom surface 12. The projection Φ surface 1 〇 is composed of a plurality of surface points 1 〇 2 . Using geometric principles, the lines are formed by points, and the lines form the basic concept of the surface, and the curved surface points 102 on the projected curved surface 10 are listed to further define curves and curved surfaces, and given the number of such curved surface points 102 The smoothness of the pupil surface 10 will be determined. There are a number of ways in which the curve and surface can be created by using the surface points 102 in engineering, and are not described in detail herein. Mainly by using the concept of smooth joints, it is ensured that the curve is connected at a given curved point 1〇2, so that the tangent is continuous and the curvature of the curve is continuous, and then the projected curved surface 10 is constructed. - The polarized streetlight optical lens provided by this creation uses a two-dimensional coordinate to represent each surface point 1 〇 2 in its space. Wherein the projection surface 1〇 edge forms a reference surface 1〇4, and the reference surface 1〇4 has a long axis 1〇6 and a short axis 1〇8, and the long axis 1〇6 is in the x-axis direction, The short axis 108 is in the direction of the x-axis, (1 is a unit coordinate length, and the intersection of the long axis and the short axis 1〇8 is a three-dimensional coordinate origin, wherein the curved points 102 are on the χ-ζ coordinate plane, Each point (χ'ζ) is (〇, 7 29), U 84 7 is called, (3 97 7 28), 7 M395836 (6.18, 6.81), (7.76, 6.03), (9.04, 4.88), (9.80, 3.59), (1〇·〇9, 2.00), (1〇〇9,14〇), (ι〇〇9 〇); on the χ-γ coordinate plane, each point (x, y) is (〇 , 6 49), ' (1.70, 6.62) ' (3.62, 6.94) . (5.47, 6.91) ' (7.20, 6.45) ^ (8.54, 5.54), (9.49, 4.08), (9.96, 2.50), (10 .〇9,i.〇4), (1 0·02,0) and (0,-5.06), (UU 32), (2 66,_5 66), (4.03,-5.68), (5.47,- 5.44), (6.67, -4, 97), (7.77, -4.23), (8.58, -3.39), (9.23, -2.42), (9.70, -1.36), (ι0·01〇); On the ζ coordinate plane, each point (yz) is (〇7 28), (0.99, 7.32) ) ^ (2.19, 7.20) . (3.40, 6.84) ' (4.60, 6.18) > (5.37, 5.52), (5.99, 4.76), (6.53, 3.81), (6.88, 2.78) ' (6.89, 0.88), (6.72, 〇) and (〇, 7.28), (-0.84, 7.14), (·1·68, 6.90), (-2.47, 6.55), (·3.24, 6.10), (-4.07 ,5·43), (-4.6 5,4.8 0)' (-5.19,4.02)> (.5.70, 2.40)' (-5.48,0.90). (-5.11,0). Therefore, the surface points 1 The distance between 〇2 and χ, γ, and ζ is the multiplication of the corresponding (x, y, z) coordinates by the unit coordinate length d, for example, (xd, yd, zd). The distances from 102 to γ, γ, and z are respectively allowed to have a relative error p, and ·d/2〇SpSd/2〇. Therefore, the relative error range β′ is also the scope of rights claimed by the author: The bottom surface 12 and the edge of the reference surface 1〇4 are interconnected to form the lens body, and the center of the bottom surface 12 is recessed to form an accommodating chamber 122 for accommodating the LED. The lens body ι is based on a Υ-Ζ surface and is only mirror-symmetrical to the χ-axis direction. The polarized streetlight optical lens is fixed to the upper side with respect to the LED substrate by the 8 M395836 type fastener. The effect of the creation is to use the aspherical wide illumination angle design of the polarized streetlight optical lens to make the light source of the light-emitting diode pass through the polarized streetlight optical lens to produce a refraction effect, so that the illumination area of the light projection roughly corresponds to the length. The axis direction datum surface is symmetrical on both sides. In addition, the asymmetric lens body structure is used to achieve the effect of the partial light mode, so that the overall illumination area is shifted, and the road surface is more effectively and appropriately illuminated. According to this, the LED light source can be effectively irradiated to the road surface completely, and the use of the LED lamp can achieve the energy-saving, carbon-saving and environmental protection requirements, and can enhance the safety of driving at night and using passers-by. The above is only the preferred embodiment of the present invention, and is not intended to limit the scope of the present invention. Therefore, it is equivalent to the equivalent or easy change of the technology. Equal servant changes and modifications made without departing from the spirit and scope of this creation shall be covered by the scope of this creation. M395836 [Simple description of the drawing] The first drawing shows the three-dimensional appearance of the creation. The second drawing shows the side view of the X-Z plane. Figure 3 shows the top view of the creation on the X-Y plane. Figure 4 is a cross-sectional view of the creation in the Y-Z plane. Figure 5 shows the ray path created in the X-Z plane. Figure 6 shows the ray path created in the Y-Z plane. Figure 7 shows the isometric distribution of the LEDs used in this creation. Figure 8 is a diagram of the light distribution curve used in this creation. Figure 9 is a perspective view of the body of the creation with a snap fit. [Description of main component symbols] 1 Lens body 10 Projection surface 102 Surface point 104 Reference plane 106 Long axis 108 Short axis 12 Bottom surface 122 accommodating chamber 2 Engagement part 12