TWM502800U - Optical lens - Google Patents

Optical lens Download PDF

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Publication number
TWM502800U
TWM502800U TW103219905U TW103219905U TWM502800U TW M502800 U TWM502800 U TW M502800U TW 103219905 U TW103219905 U TW 103219905U TW 103219905 U TW103219905 U TW 103219905U TW M502800 U TWM502800 U TW M502800U
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Taiwan
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light
optical lens
depth
wall
curvature
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TW103219905U
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Chinese (zh)
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Shun Wang
Shun-Wen Teng
Hsin-Chieh Huang
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Chun Kuang Optics Corp
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Priority to TW103219905U priority Critical patent/TWM502800U/en
Publication of TWM502800U publication Critical patent/TWM502800U/en

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光學透鏡 optical lens

本新型是關於光學元件,且特別是有關於一種用以提供特殊光強度分佈的光學透鏡。 The present invention relates to optical components, and more particularly to an optical lens for providing a particular light intensity distribution.

發光二極體為一種半導體光源,其係透過將電能轉換為光能以達到發光效果的半導體元件。發光二極體的發光效果是通過施加電流在P型半導體及N型半導體組成的化合物半導體中,讓P型半導體及N型半導體接面處電子及電洞再結合(或稱復合)而產生。由於發光二極體是以半導體被電子與電洞結合自然輻射發光,工作時不易發熱,故相較於一般白熾燈泡,不存在燈絲發光易燒、熱沉積、光衰等問題,使用壽命可達6萬至10萬小時,是白熾燈泡使用壽命的10倍以上。 A light-emitting diode is a semiconductor light source that is a semiconductor element that converts electrical energy into light energy to achieve a light-emitting effect. The light-emitting effect of the light-emitting diode is generated by applying a current to a compound semiconductor composed of a P-type semiconductor and an N-type semiconductor to recombine (or combine) electrons and holes at the junction of the P-type semiconductor and the N-type semiconductor. Since the light-emitting diode is a semiconductor that is combined with natural radiation by electrons and holes, it is not easy to generate heat during operation. Therefore, compared with the general incandescent light bulb, there is no problem of filament light-emitting, heat deposition, light decay, etc. 60,000 to 100,000 hours, more than 10 times the life of incandescent bulbs.

其次,發光二極體運用冷光源,眩光小,無輻射,使用中不產生有害物質,也不含汞元素,較白熾燈泡具有更佳的環保效益,屬於典型的綠色照明光源。 Secondly, the light-emitting diode uses a cold light source, which has small glare and no radiation. It does not produce harmful substances during use, and does not contain mercury. It has better environmental benefits than incandescent bulbs and is a typical green illumination source.

又,發光二極體的工作電壓低,採用直流驅動方式,超低功耗,電光功率轉換接近100%,在相同照明效果下比白熾燈泡節能80%以上。 In addition, the operating voltage of the LED is low, and the DC driving method is adopted. The ultra-low power consumption and the electro-optical power conversion are close to 100%, and the energy saving of the incandescent bulb is more than 80% under the same lighting effect.

基於如上優點,發光二極體已被廣泛地應用於顯示器、居家、汽車車燈、室內及室外照明。但是,發光二極體只朝向特定方向發 出光線,而不是以全部方向發出光線,以及它的方位角(orientation angle)通常約有120度。相較於以全部方向發光的現有戶外照明設備,發光二極體的光分佈特性與其差別很大,因此發光二極體用於戶外照明設備有其限制。 Based on the above advantages, light-emitting diodes have been widely used in displays, homes, automobile lights, indoor and outdoor lighting. However, the light emitting diode only emits in a specific direction Light is emitted, not in all directions, and its orientation angle is typically about 120 degrees. Compared with existing outdoor lighting devices that emit light in all directions, the light distribution characteristics of the light emitting diodes are very different, and thus the light emitting diodes have limitations for use in outdoor lighting devices.

一般室外大型廣告看板主要是在其一側或相對二側擺放光源以照亮廣告圖層,然而,由於發光二極體的方位角僅約有120度,且光分佈特性不如傳統用以提供光源以照亮廣告圖層的投射燈,故無法有效地照亮廣告圖層。 Generally, large outdoor advertising billboards mainly display light sources on one side or opposite sides to illuminate the advertising layer. However, since the azimuth of the light emitting diode is only about 120 degrees, and the light distribution characteristics are not as good as conventional to provide a light source. To illuminate the advertising layer's projection lights, the advertising layer cannot be effectively illuminated.

因此,在發光二極體被應用在作為室外大型廣告看板的照射光源時或其它市場,亟需透過二次透鏡以將發光二極體射出之光線引導到所欲方位角。 Therefore, when the light-emitting diode is applied to an illumination source as an outdoor large-sized billboard, or in other markets, it is not necessary to pass the secondary lens to guide the light emitted from the LED to a desired azimuth.

本新型揭示內容之一技術態樣在於提供一種光學透鏡,所述光學透鏡用以改善由光學元件射出之光線的方位角,同時且製造明暗截止線。 One aspect of the present disclosure is to provide an optical lens for improving the azimuth of light emitted by an optical element while fabricating a cut-off line.

根據本新型之一具體實施方式,提供一種光學透鏡,包含第一側表面、第二側表面、出光面、底面及凹槽,第一側表面相對於第二側表面,第一側表面及第二側表面經配置使得光學透鏡相對於其中心軸呈非對稱旋轉。出光面連接第一側表面及第二側表面,底面相對於出光面,並連接第一側表面及第二側表面。 According to an embodiment of the present invention, an optical lens includes a first side surface, a second side surface, a light exit surface, a bottom surface, and a groove, the first side surface being opposite to the second side surface, the first side surface, and the first side surface The two side surfaces are configured such that the optical lens rotates asymmetrically with respect to its central axis. The light emitting surface is connected to the first side surface and the second side surface, and the bottom surface is opposite to the light emitting surface, and connects the first side surface and the second side surface.

凹槽形成在底面,並朝向出光面的方向延伸,凹槽係由內壁及側壁所構成,內壁具有預定角度傾斜地連接側壁,使側壁具有一第一深度及一第二深度,第一深度大於第二深度,側壁具有第一深 度之一側係對應第一側表面設置,側壁具有第二深度之一側係對應第二側表面設置。 The groove is formed on the bottom surface and extends toward the light exiting surface. The groove is formed by the inner wall and the side wall. The inner wall has a predetermined angle obliquely connecting the side wall, so that the side wall has a first depth and a second depth, the first depth Greater than the second depth, the sidewall has a first depth One side of the degree corresponds to the first side surface, and one side of the side wall having the second depth corresponds to the second side surface.

藉此,由發光元件發出之光線在通過光學透鏡後,會由內壁發生折射,並於第一側表面及第二側表面發生全內反射,而使得光線偏移光軸地朝向光學透鏡具有第二側表面的一方向的出光面射出。 Thereby, the light emitted by the light-emitting element is refracted by the inner wall after passing through the optical lens, and total internal reflection occurs on the first side surface and the second side surface, so that the light is offset from the optical axis toward the optical lens. The light exiting surface in one direction of the second side surface is emitted.

此外,第一側表面具有第一曲率,第二側表面具有第二曲率,第二曲率可大於第一曲率;當然,第二曲率也可以等於或小於第一曲率。凹槽的深度可為該光學透鏡厚度之30~70%;同時,預定角度可介於1~45度。又,光學透鏡更可包含一凸部,形成在出光面,凸部由出光面朝著相反於底面的方向凸出,且凸部位於凹槽在出光面的投影範圍內。凸部的形狀係以光學透鏡之俯視面觀之,為一圓形,且凹槽的外徑由底面向出光面逐漸縮小。 Further, the first side surface has a first curvature, the second side surface has a second curvature, and the second curvature may be greater than the first curvature; of course, the second curvature may also be equal to or smaller than the first curvature. The depth of the groove may be 30 to 70% of the thickness of the optical lens; and the predetermined angle may be between 1 and 45 degrees. Moreover, the optical lens may further include a convex portion formed on the light-emitting surface, the convex portion protruding from the light-emitting surface in a direction opposite to the bottom surface, and the convex portion is located in a projection range of the groove on the light-emitting surface. The shape of the convex portion is a circular shape in a plan view of the optical lens, and the outer diameter of the concave portion is gradually reduced from the bottom surface toward the light exit surface.

1、1a、1b‧‧‧光學透鏡 1, 1a, 1b‧‧‧ optical lens

10‧‧‧出光面 10‧‧‧Glossy

100‧‧‧凸部 100‧‧‧ convex

12‧‧‧底面 12‧‧‧ bottom

14‧‧‧第一側表面 14‧‧‧First side surface

15‧‧‧第二側表面 15‧‧‧Second side surface

16‧‧‧凹槽 16‧‧‧ Groove

160‧‧‧內壁 160‧‧‧ inner wall

162‧‧‧側壁 162‧‧‧ side wall

3‧‧‧發光元件 3‧‧‧Lighting elements

A‧‧‧中心軸 A‧‧‧ center axis

H1‧‧‧第一深度 H1‧‧‧first depth

H2‧‧‧第二深度 H2‧‧‧second depth

I‧‧‧光軸 I‧‧‧ optical axis

P‧‧‧平面 P‧‧‧ plane

θ 1、θ 2、θ 3‧‧‧預定角度 θ 1, θ 2, θ 3‧‧‧ predetermined angle

圖1為本創作第一實施方式之光學透鏡之立體圖。 1 is a perspective view of an optical lens according to a first embodiment of the present invention.

圖2為本創作第一實施方式之光學透鏡之俯視圖。 2 is a plan view of the optical lens of the first embodiment of the present invention.

圖3為本創作第一實施方式之光學透鏡之剖視圖。 3 is a cross-sectional view of the optical lens of the first embodiment of the present invention.

圖4為本創作第一實施方式之光學透鏡之另一剖視圖。 4 is another cross-sectional view of the optical lens of the first embodiment of the present invention.

圖5為對應本創作第一實施方式之光學透鏡之光強度分布圖。 Fig. 5 is a view showing a light intensity distribution of an optical lens corresponding to the first embodiment of the present invention.

圖6為本創作第二實施方式之光學透鏡之剖視圖。 Figure 6 is a cross-sectional view of the optical lens of the second embodiment of the present invention.

圖7為對應本創作第二實施方式之光學透鏡之光強度分布圖。 Fig. 7 is a view showing a light intensity distribution of an optical lens corresponding to the second embodiment of the present invention.

圖8為本創作第三實施方式之光學透鏡之剖視圖。 Figure 8 is a cross-sectional view showing the optical lens of the third embodiment of the present invention.

圖9為對應本創作第三實施方式之光學透鏡之光強度分布圖。 Fig. 9 is a view showing a light intensity distribution of an optical lens according to a third embodiment of the present invention.

圖10為本創作之光學透鏡之使用示意圖。 Figure 10 is a schematic view showing the use of the optical lens of the present invention.

請參考隨附圖示,本新型揭示內容之以上及額外目的、特徵及優點將透過本揭示內容之較佳實施例之以下闡釋性及非限制性詳細描敘予以更好地理解。 The above and other objects, features, and advantages of the present invention will be better understood from the following description of the preferred embodiments.

配合參閱圖1、圖2及圖3,分別為本新型第一實施方式之光學透鏡之立體圖、俯視圖及剖視圖。光學透鏡1適用於設置在發光元件3上,藉以改善由光學元件3射出之光線的方位角,使光線具有特殊光強度分佈。發光元件3具有一光軸I,且發光元件3可例如(但不限定)為發光二極體(light emitting diode,LED)。在此要說明的是,發光二極體的使用數量可以為一個或多個,且其形態可以是表面封裝形式的發光二極體或發光二極體晶粒。光學透鏡1是使用玻璃或樹脂材料等可透光材料製成。 1 , 2 and 3 are respectively a perspective view, a plan view and a cross-sectional view of the optical lens according to the first embodiment of the present invention. The optical lens 1 is adapted to be disposed on the light-emitting element 3, thereby improving the azimuth of the light emitted by the optical element 3, so that the light has a special light intensity distribution. The light-emitting element 3 has an optical axis I, and the light-emitting element 3 can be, for example, but not limited to, a light emitting diode (LED). It should be noted that the number of the light-emitting diodes may be one or more, and the shape may be a light-emitting diode or a light-emitting diode die in a surface package form. The optical lens 1 is made of a light-transmitting material such as glass or a resin material.

光學透鏡1出光面10、底面12、第一側表面14及第二側表面15,底面12相對於出光面10,底面12設計為平面。第一側表面14及第二側表面15相對設置並分別連接出光面10及底面12。第一側表面14具有第一曲率,第二側表面15具有一第二曲率;在本實施方式中,第二曲率大於第一曲率,實際實施時,第一曲率及第二曲率設計為第一曲率小於第二曲率,或者第一曲率等於第二曲率。第一側表面14及第二側表面15經配置使得光學透鏡1相對於其中心軸A呈非對稱旋轉。 The light-emitting surface 10, the bottom surface 12, the first side surface 14, and the second side surface 15, the bottom surface 12 is opposite to the light-emitting surface 10, and the bottom surface 12 is designed to be a flat surface. The first side surface 14 and the second side surface 15 are oppositely disposed and respectively connected to the light surface 10 and the bottom surface 12. The first side surface 14 has a first curvature, and the second side surface 15 has a second curvature. In the embodiment, the second curvature is greater than the first curvature. In actual implementation, the first curvature and the second curvature are designed as the first The curvature is less than the second curvature, or the first curvature is equal to the second curvature. The first side surface 14 and the second side surface 15 are configured such that the optical lens 1 rotates asymmetrically with respect to its central axis A.

光學透鏡1更包含凹槽16,凹槽16形成在底面12,並朝向出光面10的方向凹陷,凹槽16的深度係為光學透鏡1厚度之30~70%。發光元件3容置於凹槽16中,用以朝向光學透鏡1投射光線。由光學透鏡1的俯視角度觀之,凹槽16的形狀為圓形。發光元件3的光軸I與光學透鏡1的中心軸A重合。 The optical lens 1 further includes a recess 16 formed on the bottom surface 12 and recessed toward the light exit surface 10, and the recess 16 has a depth of 30 to 70% of the thickness of the optical lens 1. The light-emitting element 3 is housed in the recess 16 for projecting light toward the optical lens 1. The shape of the groove 16 is circular in view of the angle of view of the optical lens 1. The optical axis I of the light-emitting element 3 coincides with the central axis A of the optical lens 1.

圖3所示為沿著圖2所示之光學透鏡之第一軸向X剖切的剖視圖。此剖面與發光元件3的光軸I重合,且第一軸向X垂直於光軸I。凹槽16的外徑由底面12向出光面10逐漸縮小,凹槽16包含內壁160及側壁162。內壁160具有預定角度θ 1傾斜地連接側壁162,使圖中右半部所示側壁162具有第一深度H1,圖中左半部所示側壁162具有第二深度H2,第一深度H1大於第二深度H2;故凹槽16之形狀在第一軸向X的剖面為非對稱於光軸I的四邊形。其中,第一深度H1是指內壁160與底面12之間的最長距離,第二深度H2是指內壁160與底面12之間的最短距離;預定角度θ 1介於1至45度之間,在本實施方式中,預定角度θ 1為10度。 3 is a cross-sectional view taken along the first axial direction X of the optical lens shown in FIG. 2. This cross section coincides with the optical axis I of the light-emitting element 3, and the first axial direction X is perpendicular to the optical axis I. The outer diameter of the recess 16 is gradually reduced from the bottom surface 12 toward the light exit surface 10, and the recess 16 includes an inner wall 160 and a side wall 162. The inner wall 160 has a predetermined angle θ 1 obliquely connecting the side walls 162 such that the side wall 162 shown in the right half of the figure has a first depth H1, and the side wall 162 shown in the left half of the figure has a second depth H2, the first depth H1 being greater than the first The depth H2 is such that the shape of the groove 16 in the first axial direction X is a quadrangle that is asymmetric with respect to the optical axis I. Wherein, the first depth H1 refers to the longest distance between the inner wall 160 and the bottom surface 12, and the second depth H2 refers to the shortest distance between the inner wall 160 and the bottom surface 12; the predetermined angle θ 1 is between 1 and 45 degrees In the present embodiment, the predetermined angle θ 1 is 10 degrees.

再者,側壁162具有第一深度H1之一側係對應第一側表面14設置,側壁162具有第二深度H2之一側係對應第二側表面15設置,藉此,使得光學透鏡1之形狀在第一軸向X的剖面非對稱於光軸I。 Furthermore, the side wall 162 has a first depth H1 side disposed corresponding to the first side surface 14, and the side wall 162 has a second depth H2 side disposed corresponding to the second side surface 15, whereby the shape of the optical lens 1 is made The profile in the first axial direction X is asymmetrical to the optical axis I.

配合參閱圖5,為本新型第一實施方式之光學透鏡的光強度分佈圖。在圖5中,於量測通過光學透鏡1之光線的配光曲線時,發光元件3是設置在圖中所示之圓心位置,發光元件3及光學透鏡1是面向圖中0度方向,發光元件3的光軸I與圖中0度重合,且側壁162具有第二深度H2之一側係對應設置於圖5下側。於圖5中,配光曲線L1用以表示通過光學透鏡1之光線於第一軸向X的光強度分 佈,配光曲線L2用以表示通過光學透鏡1之光線於第二軸向Y的光強度分佈。 Referring to FIG. 5, a light intensity distribution diagram of the optical lens of the first embodiment of the present invention is shown. In FIG. 5, when measuring the light distribution curve of the light passing through the optical lens 1, the light-emitting element 3 is disposed at a center position shown in the drawing, and the light-emitting element 3 and the optical lens 1 are oriented in the direction of 0 degrees in the figure, and are illuminated. The optical axis I of the element 3 coincides with 0 degrees in the figure, and one side of the side wall 162 having the second depth H2 is correspondingly disposed on the lower side of FIG. In FIG. 5, the light distribution curve L1 is used to indicate the light intensity of the light passing through the optical lens 1 in the first axial direction X. The cloth, the light distribution curve L2 is used to indicate the light intensity distribution of the light passing through the optical lens 1 in the second axial direction Y.

由配光曲線L1可知,發光元件3所發出之光線主要會聚在光軸I左偏大約15度的方向,實際實施時,可使該角度落於5至40度之間。在此要說明的是:發光元件3所發出的光線進入光學透鏡1並傳遞至第一側表面14時,第一側表面14用以使光線朝向與光軸I左偏15角度的方向(全)反射,接著再由出光面10出射。發光元件3所發出的光線進入光學透鏡1並傳遞至第二側表面15時,係朝向與表面14的方向全反射,接著再由出光面10出射。 It can be seen from the light distribution curve L1 that the light emitted by the light-emitting element 3 mainly converges on the left side of the optical axis I by about 15 degrees, and in practice, the angle can be between 5 and 40 degrees. It is to be noted that when the light emitted by the light-emitting element 3 enters the optical lens 1 and is transmitted to the first side surface 14, the first side surface 14 serves to direct the light toward the left side of the optical axis I by 15 degrees (full The reflection is then emitted by the light exit surface 10. When the light emitted from the light-emitting element 3 enters the optical lens 1 and is transmitted to the second side surface 15, it is totally reflected toward the surface 14 and then emitted from the light-emitting surface 10.

其次,光學元件1發出的光線在通過內壁160時,係因內壁160具有角度傾斜地連接側壁162,而使得經過側壁162的部分光線朝向第二側表面15的方向傳遞,另一部分經過側壁160的光線經過折射後往出光面10出射,進而使光線會分佈在光軸I左偏0至90度的方向,並減少落於光軸I右偏的光線,藉以製造明暗截止線。 Secondly, when the light emitted by the optical element 1 passes through the inner wall 160, the inner wall 160 is obliquely connected to the side wall 162, so that part of the light passing through the side wall 162 is transmitted toward the second side surface 15, and the other part passes through the side wall 160. The light is refracted and then exits to the exit surface 10, so that the light is distributed in the direction of 0 to 90 degrees to the left of the optical axis I, and the light that falls on the right side of the optical axis I is reduced, thereby creating a cut-off line.

圖4所示為沿著圖2所示之光學透鏡之第二軸向Y剖切之剖視圖。此剖面亦與發光元件的光軸I重合,第二軸向Y垂直於第一軸向X,第二軸向Y相同時垂直於光軸I。凹槽16之形狀在第二軸向Y的剖面為對稱於光軸I的四邊形,同時,光學透鏡1之形狀在第一軸向Y的剖面對稱光軸I。 4 is a cross-sectional view taken along the second axial direction Y of the optical lens shown in FIG. 2. This profile also coincides with the optical axis I of the illuminating element, the second axial direction Y being perpendicular to the first axial direction X, and the second axial direction Y being the same perpendicular to the optical axis I. The shape of the groove 16 in the second axial direction Y is a quadrangle symmetrical to the optical axis I, and at the same time, the shape of the optical lens 1 is symmetric with respect to the optical axis I of the first axial direction Y.

復參閱圖5,由配光曲線L2可知,光學透鏡1在Y軸剖面上呈對稱分布的曲面使第二軸向Y的光線的出光角度落於光軸I兩側分別各約30度的方向上,且於光軸I兩側各大約20度之間出射的光線大致呈均勻狀分佈。 Referring to FIG. 5, it can be seen from the light distribution curve L2 that the curved surface of the optical lens 1 symmetrically distributed on the Y-axis section causes the light-emitting angle of the light of the second axial direction to fall on the two sides of the optical axis I by about 30 degrees. The light rays which are emitted from about 20 degrees on both sides of the optical axis I are substantially uniformly distributed.

復參閱圖1及圖2,光學透鏡1更包含凸部100,凸部100形成在出光面10,並位於凹槽16在出光面10的投影範圍內。凸部100係朝著相反於底面12的方向凸出,藉以調整通過之光線的方位角;由光學元件1的俯視角度觀之,凸部100的形狀為圓形。 Referring to FIG. 1 and FIG. 2 , the optical lens 1 further includes a convex portion 100 formed on the light-emitting surface 10 and located in a projection range of the groove 16 on the light-emitting surface 10 . The convex portion 100 protrudes in a direction opposite to the bottom surface 12, thereby adjusting the azimuth angle of the light passing therethrough; the convex portion 100 has a circular shape from the viewpoint of the viewing angle of the optical element 1.

綜上所述,由發光元件3發出之光線在通過光學透鏡1後,經由內壁160發生折射之光線,與第一側表面14及第二側表面15發生全內反射之光線,而使得大部分光線偏移光軸地朝向光學透鏡1具有第二側表面15的一方向的出光面10射出。 In summary, the light emitted by the light-emitting element 3 passes through the optical lens 1 and refracts light through the inner wall 160, and the first side surface 14 and the second side surface 15 generate total internal reflection light, which makes the light large. A part of the light is shifted toward the light-emitting surface 10 of the optical lens 1 having the second side surface 15 in one direction.

配合參閱圖6,為本新型第二實施方式之光學透鏡之剖視圖。圖6所示為沿著圖2所示之光學透鏡之第一軸向X剖切的剖視圖。圖6所示之光學透鏡1a與第一實施方式的光學透鏡1相似,且相同的元件標示以相同的符號。值得注意的是,兩者的差異在於:圖6所示的光學透鏡1a之內壁160具有預定角度θ 2傾斜地連接側壁162,使側壁162具有第一深度H1及第二深度H2,第一深度H1大於第二深度H2,預定角度θ 2為20度;第一深度H1是指內壁160與底面12之間的最長距離,第二深度H2是指內壁160與底面12之間的最短距離。 Referring to FIG. 6, a cross-sectional view of an optical lens according to a second embodiment of the present invention is shown. Figure 6 is a cross-sectional view taken along the first axial direction X of the optical lens shown in Figure 2. The optical lens 1a shown in Fig. 6 is similar to the optical lens 1 of the first embodiment, and the same elements are denoted by the same reference numerals. It is to be noted that the difference between the two is that the inner wall 160 of the optical lens 1a shown in FIG. 6 has a predetermined angle θ 2 obliquely connected to the side wall 162 such that the side wall 162 has a first depth H1 and a second depth H2, the first depth H1 is greater than the second depth H2, the predetermined angle θ 2 is 20 degrees; the first depth H1 is the longest distance between the inner wall 160 and the bottom surface 12, and the second depth H2 is the shortest distance between the inner wall 160 and the bottom surface 12 .

光學元件1a發出的光線在通過內壁160時,係因內壁160具有角度傾斜地連接側壁162,而減少光線朝向第二側表面15的方向傳遞的量,進而使得大部分光線由內壁160折射進入光學元件1a,並與光軸I左偏0至90度方向發散。其次,發光元件3所發出的光線進入光學透鏡1a並傳遞至第一側表面14時,第一側表面14係藉由全內反射使光線朝向與光軸I左偏15度的方向(全)反射,接著再由出光面10出射。發光元件3所發出的光線進入光學透鏡1a經由 內壁162並傳遞至第二側表面15時,係朝向與光軸I左偏的方向全反射,接著再由出光面10出射。藉此,使得光線會聚在光軸I左偏大約15度的方向,如圖7所示配光曲線L1所示。 When the light emitted from the optical element 1a passes through the inner wall 160, the inner wall 160 is obliquely connected to the side wall 162, and the amount of light transmitted in the direction of the second side surface 15 is reduced, so that most of the light is refracted by the inner wall 160. It enters the optical element 1a and diverge from the left side of the optical axis I by 0 to 90 degrees. Next, when the light emitted from the light-emitting element 3 enters the optical lens 1a and is transmitted to the first side surface 14, the first side surface 14 is directed toward the left side of the optical axis I by 15 degrees by total internal reflection (all). The reflection is then emitted by the light exit surface 10. The light emitted by the light-emitting element 3 enters the optical lens 1a via When the inner wall 162 is transmitted to the second side surface 15, it is totally reflected toward the left side of the optical axis I, and then emitted by the light exit surface 10. Thereby, the light is concentrated in the direction of the left side of the optical axis I by about 15 degrees, as shown by the light distribution curve L1 shown in FIG.

另外,由配光曲線L2可知,通過光學透鏡1a第二軸向Y的光線的出光角度落於光軸I兩側分別各約25度的方向上,且於光軸I兩側各大約15度之間出射的光線大致呈均勻狀分佈。光學透鏡1a的各元件的功用與相關說明,實際上與第一實施方式的光學透鏡1相同,在此不予贅述。光學透鏡1a至少可達到與光學透鏡1相同的功能。 In addition, as can be seen from the light distribution curve L2, the light exiting angle of the light passing through the second axial direction Y of the optical lens 1a falls in a direction of about 25 degrees on each side of the optical axis I, and about 15 degrees on each side of the optical axis I. The light that exits between them is roughly uniform. The function and related description of each element of the optical lens 1a are substantially the same as those of the optical lens 1 of the first embodiment, and will not be described herein. The optical lens 1a can at least achieve the same function as the optical lens 1.

配合參閱圖8,為本新型第三實施方式之光學透鏡之剖視圖。圖8所示為沿著圖2所示之光學透鏡之第一軸向X剖切的剖視圖。圖8所示之光學透鏡1b與第一實施方式的光學透鏡1相似,且相同的元件標示以相同的符號。值得注意的是,兩者的差異在於:圖8所示的光學透鏡1b之內壁160具有預定角度θ 3傾斜地連接側壁162,使側壁162具有第一深度H1及第二深度H2,第一深度H1大於第二深度H2,預定角度θ 3為30度;第一深度H1是指內壁160與底面12之間的最長距離,第二深度H2是指內壁160與底面12之間的最短距離。 Referring to FIG. 8, a cross-sectional view of an optical lens according to a third embodiment of the present invention is shown. Figure 8 is a cross-sectional view taken along the first axial direction X of the optical lens shown in Figure 2. The optical lens 1b shown in Fig. 8 is similar to the optical lens 1 of the first embodiment, and the same elements are denoted by the same reference numerals. It is to be noted that the difference between the two is that the inner wall 160 of the optical lens 1b shown in FIG. 8 has a predetermined angle θ 3 obliquely connected to the side wall 162 such that the side wall 162 has a first depth H1 and a second depth H2, the first depth H1 is greater than the second depth H2, the predetermined angle θ 3 is 30 degrees; the first depth H1 is the longest distance between the inner wall 160 and the bottom surface 12, and the second depth H2 is the shortest distance between the inner wall 160 and the bottom surface 12 .

光學元件1b發出的光線在通過內壁160時,係因內壁160具有角度傾斜地連接側壁162,而減少光線朝向第二側表面15的方向傳遞的量,進而使得大部分光線由內壁160折射進入光學元件1b,並與光軸I左偏0至90度方向發散。其次,發光元件3所發出的光線進入光學透鏡1b並傳遞至第一側表面14時,第一側表面14係藉由全內反射使光線朝向與光軸I左偏約15度的方向全反射,接著再 由出光面10出射。發光元件3所發出的光線進入光學透鏡1b並傳遞至第二側表面15時,係朝向與光軸I左偏的方向全反射,並由出光面10出射。藉此,使得光線會聚在光軸I左偏大約15度的方向,如圖9所示配光曲線L1所示。 When the light emitted from the optical element 1b passes through the inner wall 160, the inner wall 160 is obliquely connected to the side wall 162, and the amount of light transmitted in the direction of the second side surface 15 is reduced, so that most of the light is refracted by the inner wall 160. It enters the optical element 1b and diverge from the left side of the optical axis I by 0 to 90 degrees. Next, when the light emitted by the light-emitting element 3 enters the optical lens 1b and is transmitted to the first side surface 14, the first side surface 14 is totally reflected by the total internal reflection so that the light is directed at about 15 degrees to the left of the optical axis I. And then It is emitted from the light exit surface 10. When the light emitted from the light-emitting element 3 enters the optical lens 1b and is transmitted to the second side surface 15, it is totally reflected toward the left side of the optical axis I, and is emitted from the light-emitting surface 10. Thereby, the light is concentrated in the direction of the left side of the optical axis I by about 15 degrees, as shown by the light distribution curve L1 shown in FIG.

另外,由圖9配光曲線L2可知,通過光學透鏡1b第二軸向Y的光線的出光角度落於光軸I兩側分別各約20度的方向上,且於光軸I兩側各大約10度之間出射的光線大致呈均勻狀分佈。光學透鏡1b的各元件的功用與相關說明,實際上與第一實施方式的光學透鏡1相同,在此不予贅述。光學透鏡1b至少可達到與光學透鏡1相同的功能。 In addition, as can be seen from the light distribution curve L2 of FIG. 9, the light exiting angle of the light passing through the second axial direction Y of the optical lens 1b falls in the direction of about 20 degrees on each side of the optical axis I, and is approximately on both sides of the optical axis I. The light emerging between 10 degrees is roughly uniform. The function and related description of each element of the optical lens 1b are substantially the same as those of the optical lens 1 of the first embodiment, and will not be described herein. The optical lens 1b can at least achieve the same function as the optical lens 1.

本新型的光學透鏡1、1a及1b透過側表面曲率以及內壁的傾斜角度的調整,使得通過光學透鏡1、1a及1b的光線會聚在光學透鏡1、1a及1b前方左偏大約15度的方向,換句話說,(光學透鏡1、1a及1b降低了往光軸右偏的光,如此一來,光學透鏡1、1a及1b搭配光學元件3被用來作為廣告燈或其它需要明顯截止線光型時,可以有效地照亮設置在光學透鏡1、1a及1b前方左邊大約15度方向的廣告圖層5,如圖10所示。在圖10中,光學透鏡1是設置在與廣告圖層5大致垂直的平面P上,且光學透鏡1具有第二側表面15的一側朝向廣告圖層5設置。 The optical lenses 1, 1a and 1b of the present invention are adjusted by the curvature of the side surface and the inclination angle of the inner wall such that the light passing through the optical lenses 1, 1a and 1b converges to the left of the optical lenses 1, 1a and 1b by about 15 degrees. Direction, in other words, (optical lenses 1, 1a and 1b reduce the light that is right-biased to the optical axis, so that optical lenses 1, 1a and 1b with optics 3 are used as advertising lights or others need to be clearly cut off In the line light type, the advertising layer 5 disposed in the direction of about 15 degrees to the left of the front side of the optical lenses 1, 1a and 1b can be effectively illuminated, as shown in Fig. 10. In Fig. 10, the optical lens 1 is disposed on the advertising layer. 5 is substantially perpendicular to the plane P, and one side of the optical lens 1 having the second side surface 15 is disposed toward the advertising layer 5.

由發光元件3發出的光在通過光學透鏡1後會朝向第二側表面15的方向偏移,藉以照亮位於光學透鏡1左側的廣告圖層5。 The light emitted by the light-emitting element 3 is deflected toward the second side surface 15 after passing through the optical lens 1, thereby illuminating the advertising layer 5 located on the left side of the optical lens 1.

然以上所述者,僅為本新型之較佳實施例,當不能限定本新型實施之範圍,即凡依本新型申請專利範圍所作之均等變化與修飾等 ,皆應仍屬本新型之專利涵蓋範圍意圖保護之範疇。 However, the above description is only a preferred embodiment of the present invention, and the scope of the present invention is not limited, that is, the equal variation and modification of the scope of the patent application of the present invention. , shall remain within the scope of the intended protection of the scope of the patent of this new type.

1‧‧‧光學透鏡 1‧‧‧ optical lens

10‧‧‧出光面 10‧‧‧Glossy

12‧‧‧底面 12‧‧‧ bottom

14‧‧‧第一側表面 14‧‧‧First side surface

15‧‧‧第二側表面 15‧‧‧Second side surface

16‧‧‧凹槽 16‧‧‧ Groove

160‧‧‧內壁 160‧‧‧ inner wall

162‧‧‧側壁 162‧‧‧ side wall

3‧‧‧發光元件 3‧‧‧Lighting elements

I‧‧‧光軸 I‧‧‧ optical axis

θ 1‧‧‧預定角度 θ 1‧‧‧Predetermined angle

H1‧‧‧第一深度 H1‧‧‧first depth

H2‧‧‧第二深度 H2‧‧‧second depth

Claims (9)

一種光學透鏡,包含:一第一側表面;一第二側表面,相對於該第一側表面,該第一側表面及該第二側表面經配置使得該光學透鏡相對於其中心軸呈非對稱旋轉;一出光面,連接該第一側表面及該第二側表面;一底面,相對於該出光面,並連接該第一側表面及該第二側表面;以及一凹槽,形成在該底面,並朝向該出光面的方向延伸,該凹槽係由一內壁及一側壁所構成,該內壁具有一預定角度傾斜地連接該側壁,使該側壁具有一第一深度及一第二深度,該第一深度大於該第二深度,該側壁具有該第一深度之一側係對應該第一側表面設置,該側壁具有該第二深度之一側係對應該第二側表面設置。 An optical lens comprising: a first side surface; a second side surface opposite to the first side surface, the first side surface and the second side surface being configured such that the optical lens is non-positive with respect to a central axis thereof a symmetrical rotation; a light emitting surface connecting the first side surface and the second side surface; a bottom surface opposite to the light emitting surface and connecting the first side surface and the second side surface; and a groove formed in the The bottom surface extends toward the light-emitting surface, the groove is formed by an inner wall and a side wall, and the inner wall has a predetermined angle obliquely connecting the side wall, so that the side wall has a first depth and a second Depth, the first depth is greater than the second depth, the side wall having one side of the first depth corresponding to the first side surface, the side wall having one side of the second depth corresponding to the second side surface. 如請求項1所述之光學透鏡,其中該第一側表面具有一第一曲率,該第二側表面具有一第二曲率,該第二曲率大於該第一曲率。 The optical lens of claim 1, wherein the first side surface has a first curvature and the second side surface has a second curvature that is greater than the first curvature. 如請求項1所述之光學透鏡,其中該第一側表面具有一第一曲率,該第二側表面具有一第二曲率,該第二曲率小於等於該第一曲率。 The optical lens of claim 1, wherein the first side surface has a first curvature and the second side surface has a second curvature that is less than or equal to the first curvature. 如請求項2或3所述之光學透鏡,其中該凹槽的深度為係為該光學透鏡厚度之30~70%。 The optical lens of claim 2, wherein the depth of the groove is 30 to 70% of the thickness of the optical lens. 如請求項4所述之光學透鏡,其中該預定角度介於1~45度。 The optical lens of claim 4, wherein the predetermined angle is between 1 and 45 degrees. 如請求項5所述之光學透鏡,其中該凹槽的外徑由該底面向該出 光面逐漸縮小。 The optical lens of claim 5, wherein an outer diameter of the groove is facing from the bottom The glossy surface is gradually shrinking. 如請求項6所述之光學透鏡,更包含一凸部,形成在該出光面,該凸部由該出光面朝著相反於該底面的方向凸出。 The optical lens of claim 6, further comprising a convex portion formed on the light-emitting surface, the convex portion protruding from the light-emitting surface in a direction opposite to the bottom surface. 如請求項7所述之光學透鏡,其中該凸部位於該凹槽在該出光面的投影範圍內。 The optical lens of claim 7, wherein the convex portion is located within a projection range of the groove on the light exiting surface. 如請求項8所述之光學透鏡,其中該凸部的形狀係以該光學透鏡之俯視面觀之,為一圓形。 The optical lens of claim 8, wherein the convex portion has a circular shape in a plan view of the optical lens.
TW103219905U 2014-11-10 2014-11-10 Optical lens TWM502800U (en)

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