TWI587163B - System and method of lens design - Google Patents
System and method of lens design Download PDFInfo
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- TWI587163B TWI587163B TW105125556A TW105125556A TWI587163B TW I587163 B TWI587163 B TW I587163B TW 105125556 A TW105125556 A TW 105125556A TW 105125556 A TW105125556 A TW 105125556A TW I587163 B TWI587163 B TW I587163B
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Description
本發明是關於一種鏡片設計系統及其方法,特別是關於一種設計自由曲面之準直透鏡,並經由調整準值透鏡相關參數之比例,以設計出符合不同照明需求之透鏡。 The present invention relates to a lens design system and method thereof, and more particularly to a collimating lens that designs a free-form surface and adjusts the ratio of parameters associated with the quasi-value lens to design a lens that meets different lighting requirements.
目前一般之準直鏡片的製造方式多為針對單一鏡片與一發光二極體之間之搭配進行製造與設計,然而,雖然可以製造出單一之準直透鏡,卻難以在需要改變照射光型或是照明範圍時進行適當的變化,因此,可能無法滿足各種不同需求,使得鏡片之用途過度單一化。 At present, the general method of manufacturing collimating lenses is mostly for the manufacture and design of a single lens and a light-emitting diode. However, although a single collimating lens can be manufactured, it is difficult to change the illumination type or Appropriate changes are made in the illumination range, and therefore, various needs may not be met, making the use of the lens excessively singular.
另一方面,鏡片之製造常常需要借助經驗,因此若是製造出之透鏡不敷使用,則將形成不必要的成本增加,因此建立一系統化之設計方法對於鏡片製造是十分重要的。 On the other hand, the manufacture of lenses often requires experience, so if the lens is not used, an unnecessary cost increase will occur, so establishing a systematic design method is very important for lens manufacturing.
有鑑於上述習知之問題,本發明之目的係提出一種鏡片設計系統及其方法,用以解決昔知鏡片設計方法之缺點。 In view of the above-mentioned problems, the object of the present invention is to provide a lens design system and a method thereof for solving the shortcomings of the prior art lens design method.
基於上述目的,本發明係提供一種鏡片設計系統,其包含輸入模組以及處理模組。輸入模組可輸入複數個條件參數,複數個條件參數包含鏡片折射率、發光二極體之光源座標點、自由曲面與發光二極體之起始距離、入射角、光型或其組合。處理模組可根據複數個條件參數計算複數個斜率以及複數 個座標,且處理模組根據臨界角度計算複數個反射面斜率及複數個折射面斜率,並根據複數個反射面斜率及複數個折射面斜率計算複數個三維座標點,根據預設軌跡及光型延伸及調整複數個三維座標點。複數個三維座標點可構成包含至少一出光表面以及橫截面,當出光表面由處理模組處理而為非水平設置時,照明範圍相對於水平設置係放大或縮小。 Based on the above objects, the present invention provides a lens design system including an input module and a processing module. The input module can input a plurality of condition parameters, and the plurality of condition parameters include a refractive index of the lens, a light source coordinate point of the light emitting diode, a starting distance of the free curved surface and the light emitting diode, an incident angle, a light type, or a combination thereof. The processing module can calculate a plurality of slopes and complex numbers according to a plurality of condition parameters a coordinate, and the processing module calculates a plurality of reflection surface slopes and a plurality of refractive surface slopes according to the critical angle, and calculates a plurality of three-dimensional coordinate points according to the slopes of the plurality of reflection surfaces and the slopes of the plurality of refractive surfaces, according to the preset trajectory and the light pattern Extend and adjust a plurality of three-dimensional coordinate points. The plurality of three-dimensional coordinate points may be configured to include at least one light-emitting surface and a cross-section. When the light-emitting surface is non-horizontally disposed by the processing module, the illumination range is enlarged or reduced relative to the horizontal setting.
較佳地,橫截面可依據預設軌跡延伸。 Preferably, the cross section may extend according to a preset trajectory.
較佳地,延伸之複數個三維座標點可適用於至少一光源。 Preferably, the plurality of extended three-dimensional coordinate points are applicable to at least one light source.
基於上述目的,本發明再提供一種鏡片設計方法,其適用於一鏡片設計系統,包含下列步驟包含下列步驟:提供輸入模組輸入複數個條件參數,複數個條件參數更包含鏡片折射率、發光二極體之光源座標點、自由曲面與發光二極體之起始距離、入射角、光型或其組合。 Based on the above object, the present invention further provides a lens design method, which is applicable to a lens design system, and includes the following steps: providing an input module to input a plurality of condition parameters, and the plurality of condition parameters further include a lens refractive index and a light emission The source point of the polar body, the starting distance of the free-form surface and the light-emitting diode, the incident angle, the light type, or a combination thereof.
藉由處理模組根據複數個條件參數計算複數個斜率以及複數個座標。 The processing module calculates a plurality of slopes and a plurality of coordinates according to the plurality of condition parameters.
使用處理模組根據臨界角度計算複數個反射面斜率及複數個折射面斜率。 The processing module calculates a slope of the plurality of reflecting surfaces and a slope of the plurality of refractive surfaces according to the critical angle.
藉由處理模組根據複數個反射面斜率及複數個折射面斜率計算複數個三維座標點。 The processing module calculates a plurality of three-dimensional coordinate points according to the slope of the plurality of reflecting surfaces and the slope of the plurality of refractive surfaces.
藉由處理模組根據預設軌跡及光型將複數個三維座標點延伸。 The processing module extends a plurality of three-dimensional coordinate points according to the preset trajectory and the light pattern.
複數個三維座標點可構成包含至少一出光表面以及橫截面,當出光表面由處理模組處理而為非水平設置時,照明範圍相對於水平設置可放大或縮小。 The plurality of three-dimensional coordinate points may be configured to include at least one light-emitting surface and a cross-section. When the light-emitting surface is non-horizontally disposed by the processing module, the illumination range may be enlarged or reduced relative to the horizontal setting.
較佳地,橫截面可依據預設軌跡延伸。 Preferably, the cross section may extend according to a preset trajectory.
較佳地,延伸之複數個三維座標點可適用於至少一光源。 Preferably, the plurality of extended three-dimensional coordinate points are applicable to at least one light source.
承上所述,依本發明之鏡片系統及其設計方法,其可具有一或多個下述優點: As described above, the lens system and method of designing the same according to the present invention may have one or more of the following advantages:
(1)本發明之鏡片系統及其設計方法,可以藉由調整透鏡相關參數之比例,以設計出符合不同照明需求之透鏡。 (1) The lens system of the present invention and its design method can be designed to meet lenses of different illumination requirements by adjusting the ratio of lens related parameters.
(2)本發明之鏡片系統及其設計方法,可以製成具有大範圍照明效果之透鏡,且可依需求調整光型。 (2) The lens system of the present invention and the design method thereof can be made into a lens having a wide range of illumination effects, and the light pattern can be adjusted as needed.
1‧‧‧鏡片設計系統 1‧‧‧Lens Design System
11‧‧‧輸入模組 11‧‧‧Input module
12‧‧‧處理模組 12‧‧‧Processing module
13‧‧‧顯示模組 13‧‧‧Display module
14‧‧‧驗證模組 14‧‧‧ verification module
i‧‧‧入射角度 I‧‧‧incidence angle
ic‧‧‧臨界角度 Ic‧‧‧critical angle
N‧‧‧自由曲面鏡片之法線 The normal of N‧‧‧ free-form lens
Tp‧‧‧自由曲面鏡片之切線 Tp‧‧‧ tangent to freeform lens
S11~S16、S201~S209、S301~S310‧‧‧步驟 S11~S16, S201~S209, S301~S310‧‧‧ steps
第1圖係根據本發明之實施例之鏡片設計系統第一實施例之方塊圖。 1 is a block diagram of a first embodiment of a lens design system in accordance with an embodiment of the present invention.
第2圖係根據本發明之實施例之鏡片設計方法第一實施例之流程圖。 2 is a flow chart of a first embodiment of a lens design method according to an embodiment of the present invention.
第3圖係根據本發明之實施例之鏡片設計方法第二實施例之流程圖。 Figure 3 is a flow chart of a second embodiment of a lens design method in accordance with an embodiment of the present invention.
第4圖係根據本發明之實施例之自由曲面鏡片之第二實施例示意圖。 Figure 4 is a schematic illustration of a second embodiment of a freeform lens in accordance with an embodiment of the present invention.
第5圖係根據本發明之實施例之自由曲面鏡片之第二實施例二維剖面示意圖。 Figure 5 is a two-dimensional cross-sectional view showing a second embodiment of a free-form lens according to an embodiment of the present invention.
第6圖係根據本發明之實施例之光線經由自由曲面鏡片反射後平行光射出之示意圖。 Figure 6 is a schematic illustration of the parallel illumination of light reflected by a freeform lens in accordance with an embodiment of the present invention.
第7圖係根據本發明之實施例之光線經由自由曲面鏡片折射後平行光射出之示意圖。 Figure 7 is a schematic illustration of the parallel illumination of light rays refracted by a freeform lens according to an embodiment of the present invention.
第8圖係根據本發明之實施例之鏡片設計方法第三實施例之流程圖 8 is a flow chart of a third embodiment of a lens design method according to an embodiment of the present invention.
第9圖係根據本發明之實施例之第三實施例之二維剖面示意圖。 Figure 9 is a two-dimensional cross-sectional view showing a third embodiment of an embodiment of the present invention.
第10圖係根據本發明之實施例之第三實施例示意圖。 Figure 10 is a schematic view of a third embodiment of an embodiment of the present invention.
為利 貴審查員瞭解本發明之技術特徵、內容與優點及其所能達成之功效,茲將本發明配合附圖,並以實施例之表達形式詳細說明如下,而其中所使用之圖式,其主旨僅為示意及輔助說明之用,未必為本發明實施後之真實比例與精準配置,故不應就所附之圖式的比例與配置關係解讀、侷限本發明於實際實施上的權利範圍,合先敘明。 The technical features, contents, and advantages of the present invention, as well as the advantages thereof, can be understood by the present inventors, and the present invention will be described in detail with reference to the accompanying drawings. The subject matter is only for the purpose of illustration and description, and is not necessarily the true proportion and precise configuration after the implementation of the present invention. Therefore, the scope and configuration relationship of the attached drawings should not be interpreted or limited. First described.
以下將參照相關圖式,說明依本發明之鏡片設計系統及其方法之實施例,為使便於理解,下述實施例中之相同元件係以相同之符號標示來說明。 Embodiments of the lens design system and method thereof according to the present invention will be described below with reference to the accompanying drawings. For the sake of understanding, the same elements in the following embodiments are denoted by the same reference numerals.
請先行參閱第1圖,其係為根據本發明之實施例之高鏡片設計系統第一實施例之方塊圖。如圖所示,本發明之鏡片設計系統1包含輸入模組11、處理模組12、顯示模組13、驗證模組14。 Please refer to FIG. 1, which is a block diagram of a first embodiment of a high lens design system in accordance with an embodiment of the present invention. As shown in the figure, the lens design system 1 of the present invention comprises an input module 11, a processing module 12, a display module 13, and a verification module 14.
實施上,本發明主要系統以及方法多沿用前案之方法及系統。首先就所需要條件於輸入模組11先行輸入複數個條件參數,其中複數個條件參數可包含鏡片折射率、發光二極體之光源座標點、自由曲面與發光二極體之起始距離、入射角、光型等等。 In practice, the main systems and methods of the present invention mostly follow the methods and systems of the previous case. First, a plurality of condition parameters are first input to the input module 11 according to the required condition, wherein the plurality of condition parameters may include a refractive index of the lens, a light source coordinate point of the light emitting diode, a starting distance of the free curved surface and the light emitting diode, and incidence. Angle, light type, etc.
其後,經由輸入模組11輸入之複數個條件參數經由處理模組12根據複數個進行條件參數以進行計算複數個斜率以及複數個座標,且處理模組12根據臨界角度計算複數個反射面斜率以及複數個折射面斜率,並根據複數個反射面斜率及複數個折射面斜率計算複數個三維座標點。 Thereafter, the plurality of condition parameters input through the input module 11 are processed by the processing module 12 according to the plurality of condition parameters to calculate a plurality of slopes and a plurality of coordinates, and the processing module 12 calculates the slopes of the plurality of reflection surfaces according to the critical angle. And a plurality of refractive surface slopes, and calculating a plurality of three-dimensional coordinate points according to the slopes of the plurality of reflecting surfaces and the slopes of the plurality of refractive surfaces.
上述資料經由處理模組12計算之後,將經由顯示模組13顯示出複數個三維座標點,最後經由驗證模組14根據複數個條件以及複數個三維座標點驗證複數個三維座標點所製成之鏡片之光型及照度是否符合需求。 After the above data is calculated by the processing module 12, a plurality of three-dimensional coordinate points are displayed via the display module 13, and finally, the verification module 14 is used to verify a plurality of three-dimensional coordinate points according to a plurality of conditions and a plurality of three-dimensional coordinate points. Whether the light type and illumination of the lens meet the requirements.
現請參閱第2圖,第2圖係為根據本發明之實施例之鏡片設計方法第一實施例之流程圖。 Referring now to Figure 2, there is shown a flow chart of a first embodiment of a lens designing method in accordance with an embodiment of the present invention.
首先如步驟S11及步驟S12所示,步驟S11為提供輸入模組輸入複數個條件參數,其後步驟S12為藉由處理模組根據複數個條件參數計算複數個斜率以及複數個座標。其中,在步驟S11中,複數個條件參數可為鏡片折射率、發光二極體光源的座標點、自由曲面與發光二極體之的起始距離以及入射角度等參數。其後,於步驟S12透過處理模組根據輸入模組輸入的複數個條件參數計算複數個斜率、複數個座標、臨界角度、複數個反射面斜率、複數個折射面斜率以及複數個三維座標點等內容。 First, as shown in step S11 and step S12, step S11 inputs a plurality of condition parameters for providing the input module, and then step S12 is to calculate a plurality of slopes and a plurality of coordinates according to the plurality of condition parameters by the processing module. Wherein, in step S11, the plurality of condition parameters may be parameters such as a refractive index of the lens, a coordinate point of the light-emitting diode source, a starting distance of the free-form surface and the light-emitting diode, and an incident angle. Then, in step S12, the processing module calculates a plurality of slopes, a plurality of coordinates, a critical angle, a plurality of reflection surface slopes, a plurality of refractive surface slopes, and a plurality of three-dimensional coordinate points according to the plurality of condition parameters input by the input module. content.
當經由步驟S12計算出上述資訊之後,將經由步驟S121透過處理模組根據入射角計算複數個反射面斜率,並經由步驟S122藉由處理模組根據入射角及複數個反射面斜率最終計算出複數個反射點座標。 After the information is calculated in step S12, the processing module performs a plurality of reflection surface slopes according to the incident angle through the processing module, and finally calculates the complex number according to the incident angle and the slopes of the plurality of reflection surfaces by the processing module via step S122. Reflection point coordinates.
其中,於步驟S121及步驟S122中,當光源入射角度越來越大時,反射點座標的垂直位置點會快速增加,亦即可能會使得自由曲面之厚度增加, 因此無法製成輕薄之鏡片。因此,更進一步,處理模組12可根據複數個條件參數計算出臨界角度,此臨界角度乃是光反射與光折射的分界角度。 Wherein, in step S121 and step S122, when the incident angle of the light source is larger and larger, the vertical position of the coordinate of the reflection point will increase rapidly, that is, the thickness of the free surface may be increased. Therefore, it is impossible to make a thin lens. Therefore, further, the processing module 12 can calculate a critical angle according to a plurality of condition parameters, which is a boundary angle between light reflection and light refraction.
因此如步驟S13所示,S13為使用處理模組根據臨界角度計算反射面之複數個反射面斜率及折射面之複數個折射面斜率。 Therefore, as shown in step S13, S13 is to use a processing module to calculate a plurality of reflection surface slopes of the reflection surface and a plurality of refraction surface slopes of the refraction surface according to the critical angle.
因此步驟S13包含下列步驟S131及步驟S132,其中,步驟S131為藉由處理模組根據臨界角度及入射角計算複數個折射面斜率,其後步驟S132藉由處理模組根據臨界角度、入射角以及複數個折射面斜率計算出複數個折射點座標。 Therefore, the step S13 includes the following steps S131 and S132, wherein the step S131 is to calculate a plurality of refractive surface slopes according to the critical angle and the incident angle by the processing module, and then the step S132 is performed by the processing module according to the critical angle, the incident angle, and A plurality of refractive index coordinates are calculated for a plurality of refractive surface slopes.
再得出上述之折射點以及反射點之座標及斜率後,經由步驟S14藉由處理模組根據複數個反射面斜率及複數個折射面斜率計算複數個三維座標點,並根據所需光型延伸複數個三維座標點。 After obtaining the above-mentioned refraction point and the coordinates and the slope of the reflection point, the processing module calculates a plurality of three-dimensional coordinate points according to the slope of the plurality of reflection surfaces and the slopes of the plurality of refraction surfaces, and extends according to the desired light pattern. A plurality of three-dimensional coordinate points.
而為了能使得將資訊圖像化以供觀察,因此如步驟S15所示,將透過顯示模組顯示複數個三維座標點。 In order to enable the information to be imaged for observation, as shown in step S15, a plurality of three-dimensional coordinate points are displayed through the display module.
而本發明為了得知所設計出之自由曲面鏡片是否足以滿足設計之照明需求,因此經由步驟S16透過驗證模組根據複數個條件以及複數個三維座標點驗證複數個三維座標點所製成之鏡片之光型及照度 In order to know whether the designed free-form lens is sufficient for the lighting requirements of the design, the method for verifying the plurality of three-dimensional coordinate points according to the plurality of conditions and the plurality of three-dimensional coordinate points is verified by the verification module via step S16. Light type and illumination
而若是所得到之結果並不如預期,可再重複步驟S14至S16進行調整,而上述各步驟的實行可由電腦搭配相應之模擬軟體達成。 If the obtained result is not as expected, the steps S14 to S16 may be repeated to perform the adjustment, and the implementation of the above steps may be achieved by the computer with the corresponding simulation software.
依據第一實施例,本發明更提出第二實施例作更進一步之舉例說明。 According to the first embodiment, the present invention further provides a second embodiment for further exemplification.
請參閱第3圖,其係為本發明之鏡片設計方法第二實施例之流程圖。請一併參閱第1圖之鏡片設計系統方塊圖,首先如步驟S201所示,步驟S201 為提供輸入模組輸入發光二極體光源的座標點設為原點(0,0)、自由曲面與發光二極體之的距離為10mm、發光二極體光源為1mm2以及入射角為0°至臨界角度。 Please refer to FIG. 3, which is a flow chart of a second embodiment of the lens design method of the present invention. Please refer to the block diagram of the lens design system of FIG. 1 first, as shown in step S201, step S201 is to provide the coordinate point of the input module input light-emitting diode light source as the origin (0, 0), free-form surface and The distance of the light-emitting diode is 10 mm, the light source of the light-emitting diode is 1 mm 2 and the incident angle is 0° to a critical angle.
接著如步驟S202及步驟S204所示,步驟S202為透過處理模組根據入射角為0°至臨界角度計算複數個反射面斜率,其後經由步驟S203藉由處理模組根據入射角為0°至臨界角度及複數個反射面斜率計算複數個反射點座標,以及步驟S204利用處理模組計算出臨界角度為42.0390625°。 Then, as shown in step S202 and step S204, step S202 is to calculate a plurality of reflection surface slopes according to the incident angle from 0° to the critical angle, and then pass through the processing module according to the incident angle of 0° to step S203. The critical angle and the plurality of reflection surface slopes calculate a plurality of reflection point coordinates, and the critical angle is 42.0390625° calculated by the processing module in step S204.
再接著經由步驟S205,藉由處理模組根據臨界角度為42.0390625°以及入射角為臨界角度至90°計算複數個折射面斜率;以及步驟S26,藉由處理模組根據臨界角度為42.0390625°、入射角為臨界角度至90°以及複數個折射面斜率計算複數個折射點座標。 Then, through step S205, the processing module calculates a plurality of refractive surface slopes according to a critical angle of 42.0390625° and an incident angle of a critical angle to 90°; and step S26, by processing the module according to a critical angle of 42.0390625°, incident The angle is a critical angle to 90° and a plurality of refractive surface slopes are used to calculate a plurality of refractive point coordinates.
得出複數個折射點座標後,經由步驟S207藉由處理模組根據複數個反射面斜率及複數個折射面斜率計算複數個三維座標點。 After a plurality of refraction point coordinates are obtained, a plurality of three-dimensional coordinate points are calculated by the processing module according to the slope of the plurality of reflection surfaces and the slopes of the plurality of refraction surfaces by the processing module.
至此,可藉由步驟S208透過顯示模組顯示複數個三維座標點。 So far, a plurality of three-dimensional coordinate points can be displayed through the display module in step S208.
現請一併搭配參閱第4圖,其係為本發明之自由曲面鏡片之第二實施例示意圖。如圖所示,此示意圖是本發明之鏡片設計系統利用步驟S201至步驟S207得到複數個三維座標點,在步驟S208使用顯示模組13顯示複數個三維座標點所完成之自由曲面鏡片三維立體圖。而且,發光二極體光源通過此自由曲面鏡片,光會準直射出具有準直性,亦即此時之自由曲面鏡片為一準直透鏡,最終再透過步驟S209完成鏡片之光型及照度的驗證。 Please refer to FIG. 4 together, which is a schematic diagram of a second embodiment of the free-form lens of the present invention. As shown in the figure, the lens design system of the present invention obtains a plurality of three-dimensional coordinate points by using steps S201 to S207, and displays a three-dimensional perspective view of the free-form surface lens by using the display module 13 to display a plurality of three-dimensional coordinate points in step S208. Moreover, the light-emitting diode light source passes through the free-form lens, and the light is collimated and collimated, that is, the free-form lens is a collimating lens, and finally the light pattern and the illuminance of the lens are completed through step S209. verification.
請參閱第5圖其係為本發明之自由曲面鏡片之第二實施例二維剖面示意圖。在第5圖中,自由曲面鏡片以二維剖面圖表示,且可於鏡片底部中心處設置發光二極體晶片51,作為發光源。實線為入射光及光折射後以平行光射 出之光線,虛線為入射光及光反射後以平行光射出之光。其中,ic係為臨界角度,其臨界角度是光反射與光折射的分界角度。 Please refer to FIG. 5, which is a two-dimensional cross-sectional view showing a second embodiment of the free-form lens of the present invention. In Fig. 5, the free-form lens is represented by a two-dimensional sectional view, and a light-emitting diode wafer 51 can be disposed at the center of the bottom of the lens as a light source. The solid line is the incident light and the light is refracted and then collimated The light emitted, the dotted line is the incident light and the light reflected by the parallel light. Among them, ic is the critical angle, and its critical angle is the boundary angle between light reflection and light refraction.
第6圖為光線經由自由曲面鏡片反射後平行光射出之示意圖。其中,發光二極體光源的座標點設為原點(0,0),i係為入射角度,虛線N為自由曲面鏡片之法線以及虛線Tp為自由曲面鏡片之切線,實線為光的入射線、點狀虛線為光的反射線,而粗實線為光反射部分的自由曲面鏡片。 Figure 6 is a schematic diagram of the parallel light emitted by the light reflected through the freeform lens. Wherein, the coordinate point of the light-emitting diode light source is set as the origin (0, 0), i is the incident angle, the broken line N is the normal of the free-form lens, and the broken line Tp is the tangent of the free-form lens, and the solid line is light. Into the ray, the dotted line is the reflection line of the light, and the thick solid line is the free-form lens of the light reflecting portion.
請參閱第7圖,其係為光線經由自由曲面鏡片折射後平行光射出之示意圖。其中,發光二極體光源的座標點設為原點(0,0),i係為入射角度,虛線N為自由曲面鏡片之法線以及虛線Tp為自由曲面鏡片之切線,實線為光的入射線、點狀虛線為光的折射線,而粗實線為光反射部分的自由曲面鏡片。 Please refer to Fig. 7, which is a schematic diagram of the parallel light emitted by the light after being refracted by the free-form lens. Wherein, the coordinate point of the light-emitting diode light source is set as the origin (0, 0), i is the incident angle, the broken line N is the normal of the free-form lens, and the broken line Tp is the tangent of the free-form lens, and the solid line is light. The incident ray, the dotted line is the refracting line of the light, and the thick solid line is the free-form lens of the light reflecting portion.
然而,本發明並不僅限於此,本發明之系統及方法不僅僅可製作出如第5圖中之自由曲面鏡片,亦可透過改變第5圖中自由曲面鏡片之表面501、502之傾斜角度,改變邊緣之光線之光路,使其不為準直,因此得以改變光型,並且若是原先之照明範圍不敷需求,將可改變鏡片之大小範圍。 However, the present invention is not limited thereto, and the system and method of the present invention can not only produce the free-form lens as shown in FIG. 5, but also change the inclination angle of the surfaces 501, 502 of the free-form lens in FIG. The light path of the edge light is changed so that it is not collimated, so the light type can be changed, and if the original illumination range is insufficient, the size range of the lens can be changed.
現請參閱第8圖,步驟S301至S307與第二實施例是相同的,不同地方在於,若是實際此自由曲面鏡片與實際需求不符,則需要透過步驟S308調整自由曲面鏡片。因此若需要大範圍且均勻之照射用之透鏡,舉例而言需對一距離自由曲面鏡片8公尺遠,長寬皆為8公尺之平面進行一均勻且照度足夠之照明,則需調整原本之複數個三維點座標,最終透過步驟S308、S309顯示及驗證。 Referring to FIG. 8, steps S301 to S307 are the same as the second embodiment. The difference is that if the free-form lens does not meet the actual requirements, the free-form lens needs to be adjusted through step S308. Therefore, if a lens for illumination of a wide range and uniformity is required, for example, a uniform and illuminating illumination is required for a distance of 8 meters from a free-form surface lens and a plane of 8 meters in length and width. The plurality of three-dimensional point coordinates are finally displayed and verified through steps S308 and S309.
現請復參閱第8圖及第9圖,其分別係為根據本發明之第三實施例之流程圖及第三實施例之二維剖面示意圖,如圖所示,從步驟301至307是與第二實施例相同的,不同處在於,可於步驟308中調整自由曲面鏡片之表面601、 602之傾斜角度,而從基礎之光學之折射原理可知光線將往外側折射,因此調整後之自由曲面鏡片之表面601、602之傾斜角度如第9圖所示,不若第5圖中之自由曲面鏡片之表面501、502為水平,因而藉此擴大了照明的範圍。 Please refer to FIG. 8 and FIG. 9 respectively, which are respectively a flow chart according to a third embodiment of the present invention and a two-dimensional cross-sectional view of the third embodiment, as shown in the figure, from steps 301 to 307. The second embodiment is the same, except that the surface 601 of the free-form lens can be adjusted in step 308, The tilt angle of 602, and from the basic optical refraction principle, the light will be refracted to the outside, so the tilt angle of the surface 601, 602 of the adjusted free-form lens is as shown in Fig. 9, not the freedom in Fig. 5. The surfaces 501, 502 of the curved lens are horizontal, thereby expanding the range of illumination.
現請參閱第10圖,第10圖係根據本發明之實施例之第三實施例示意圖,除了能對鏡片之橫截面改變照射之光型之外,亦可如圖所示,將橫截面延伸,成一更為寬廣之鏡片,我們將可依實際需求如第10圖所示將其延伸,成一圓形之自由曲面鏡片70,最終,第10圖中之第三實施中之自由曲面鏡片70可由驗證模組14驗證當自由曲面鏡片70之下設置60顆1瓦的LED燈,可以對距離自由曲面鏡片70達8公尺遠,長寬皆為8公尺之平面進行一均勻且照度足夠之照明。 Referring now to FIG. 10, FIG. 10 is a schematic view of a third embodiment of an embodiment of the present invention. In addition to changing the illumination type of the cross section of the lens, the cross section may be extended as shown. , into a wider lens, we will be able to extend it according to the actual needs as shown in Figure 10, into a circular free-form lens 70, and finally, the free-form lens 70 in the third embodiment in Figure 10 can be The verification module 14 verifies that 60 LEDs of 1 watt are disposed under the free-form lens 70, and a uniform and illuminating sufficient for the free-form lens 70 to be 8 meters away and 8 meters long and wide can be performed. illumination.
因此,本發明之自由曲面透鏡除了兼具前案之準直照明特性之外,亦可改變照明之範圍以及光型,成為一更具多用途以及多功能之自由曲面透鏡。 Therefore, the free-form surface lens of the present invention can change the range of illumination and the light type in addition to the collimated illumination characteristics of the prior case, and becomes a more versatile and multifunctional free-form surface lens.
以上所述僅為舉例性,而非為限制性者。任何未脫離本發明之精神與範疇,而對其進行之等效修改或變更,均應包含於後附之申請專利範圍中。 The above is intended to be illustrative only and not limiting. Any equivalent modifications or alterations to the spirit and scope of the invention are intended to be included in the scope of the appended claims.
S11~S16‧‧‧步驟 S11~S16‧‧‧Steps
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| Publication number | Priority date | Publication date | Assignee | Title |
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| US7580192B1 (en) * | 2008-12-23 | 2009-08-25 | Smart Champ Enterprise Limited | Collimation lens system for LED |
| US20110208489A1 (en) * | 2008-10-16 | 2011-08-25 | Simone Capeleto | Method of Designing Optical Systems and Corresponding Optical System |
| TW201137403A (en) * | 2010-04-29 | 2011-11-01 | Univ Nat Changhua Education | Collimation lens structure having freeform curve and design method thereof |
| TW201242758A (en) * | 2011-04-19 | 2012-11-01 | Univ Asia | System and method of lens design |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| US20110208489A1 (en) * | 2008-10-16 | 2011-08-25 | Simone Capeleto | Method of Designing Optical Systems and Corresponding Optical System |
| US7580192B1 (en) * | 2008-12-23 | 2009-08-25 | Smart Champ Enterprise Limited | Collimation lens system for LED |
| TW201137403A (en) * | 2010-04-29 | 2011-11-01 | Univ Nat Changhua Education | Collimation lens structure having freeform curve and design method thereof |
| TW201242758A (en) * | 2011-04-19 | 2012-11-01 | Univ Asia | System and method of lens design |
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