TWI721443B - Light source module with uniform projected light intensity - Google Patents
Light source module with uniform projected light intensity Download PDFInfo
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- TWI721443B TWI721443B TW108118889A TW108118889A TWI721443B TW I721443 B TWI721443 B TW I721443B TW 108118889 A TW108118889 A TW 108118889A TW 108118889 A TW108118889 A TW 108118889A TW I721443 B TWI721443 B TW I721443B
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21K—NON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
- F21K9/00—Light sources using semiconductor devices as light-generating elements, e.g. using light-emitting diodes [LED] or lasers
- F21K9/20—Light sources comprising attachment means
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21K—NON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
- F21K9/00—Light sources using semiconductor devices as light-generating elements, e.g. using light-emitting diodes [LED] or lasers
- F21K9/60—Optical arrangements integrated in the light source, e.g. for improving the colour rendering index or the light extraction
- F21K9/64—Optical arrangements integrated in the light source, e.g. for improving the colour rendering index or the light extraction using wavelength conversion means distinct or spaced from the light-generating element, e.g. a remote phosphor layer
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21V—FUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
- F21V19/00—Fastening of light sources or lamp holders
- F21V19/001—Fastening of light sources or lamp holders the light sources being semiconductors devices, e.g. LEDs
- F21V19/0015—Fastening arrangements intended to retain light sources
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21Y—INDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO THE FORM OR THE KIND OF THE LIGHT SOURCES OR OF THE COLOUR OF THE LIGHT EMITTED
- F21Y2115/00—Light-generating elements of semiconductor light sources
- F21Y2115/10—Light-emitting diodes [LED]
Abstract
Description
本發明係有關一種光源模組,特別是指一種具有均勻投射光強度之光源模組。The present invention relates to a light source module, in particular to a light source module with uniform projection light intensity.
深度感測器主要應用在3D感測,其係由於傳統2D的平面影像辨識只有X、Y軸,在判斷影像的景深時較易受到拍攝角度和環境照明等因素的干擾,而3D感測則多了深度偵測,從平面的X、Y軸增加到X、Y、Z三軸立體座標,擷取目標物的深度影像並得到空間的立體資訊,不但提高辨識的精準度,應用也更加廣泛,其中,飛行時間(time of flight, TOF) 是深度感測的其中一種技術,如第1圖所示,利用光源模組100發射主動光源投射至目標物,被目標物反射後經濾光片110濾光,再利用光感測器120接收相關光源之反射,透過光線折返的時間計算出時間相位差,以得到待測物的深度訊息。然而,投射在物體上的光源均勻度會影響到計算深度距離的誤差,傳統使用紅外線做為主動光源,其光源投射至物體上時光強度分佈會隨光束角度而變化。Depth sensors are mainly used in 3D sensing. Because traditional 2D plane image recognition only has X and Y axes, it is more susceptible to interference from factors such as shooting angle and ambient lighting when judging the depth of field of the image, while 3D sensing is More depth detection, from the plane X, Y axis to X, Y, Z three-axis three-axis three-dimensional coordinates, to capture the depth image of the target and obtain the three-dimensional information of the space, not only improves the accuracy of recognition, but also has a wider range of applications. , Where time of flight (TOF) is one of the depth sensing technologies. As shown in Figure 1, the
然而將LED應用在深度感測器上具有以下缺點:單個LED功率低,為了獲得大功率,需要多個並聯使用;LED只在直視的狹小角度內有高亮度,而偏離該角度後光線迅速減弱;以及照射角度有限制,一般只能照射120°。特別是其中LED照射角度太小、超過範圍亮度會迅速減弱等二點為深度感測器的硬傷,因為LED發光太具有指向性、光線太過集中,反而使光強度不夠均勻,而最大只能照射120°會影響到光源發射的視場角度,限制在空間的應用範圍。上述的問題都是直接限制3D深度感測系統的應用範圍。However, the application of LEDs to depth sensors has the following disadvantages: a single LED has low power, in order to obtain high power, multiple parallel use is required; LEDs only have high brightness in a narrow angle of direct viewing, and the light will quickly weaken after deviating from this angle ; And the irradiation angle is limited, generally only 120°. In particular, the LED illumination angle is too small, the brightness of the exceeding range will be rapidly reduced, etc. Two points are the flaws of the depth sensor, because the LED light is too directional and the light is too concentrated, but the light intensity is not uniform enough, and the maximum is only The ability to illuminate 120° will affect the field of view angle of the light source, which limits the scope of application in space. The above-mentioned problems directly limit the application range of the 3D depth sensing system.
因此,本發明即提出一種具有均勻投射光強度之光源模組,有效解決上述該等問題,具體架構及其實施方式將詳述於下:Therefore, the present invention proposes a light source module with uniform projected light intensity to effectively solve the above-mentioned problems. The specific structure and implementation methods will be described in detail below:
本發明之主要目的在提供一種具有均勻投射光強度之光源模組,其使用不同光束角的發光二極體互相搭配組成一發光元件陣列,且靠中間部分的為散射型發光二極體,靠外圍部分的為標準型發光二極體,以使光強度均勻化。The main purpose of the present invention is to provide a light source module with uniform projected light intensity, which uses light-emitting diodes with different beam angles to form a light-emitting element array, and the middle part is a scattering light-emitting diode. The outer part is a standard light-emitting diode to make the light intensity uniform.
本發明之另一目的在提供一種具有均勻投射光強度之光源模組,其將發光元件陣列中的複數發光二極體以兩兩成對的方式、以不同的光束中心線傾斜角或旋轉角度改變發光二極體的照射方向,以擴大投影面上的光強度分佈範圍。Another object of the present invention is to provide a light source module with uniform projected light intensity, which combines a plurality of light-emitting diodes in a light-emitting element array in pairs with different inclination or rotation angles of the centerline of the beam Change the illumination direction of the light-emitting diode to expand the light intensity distribution range on the projection surface.
本發明之再一目的在提供一種具有均勻投射光強度之光源模組,其可將多組發光元件陣列加以排列,以在不同工作距離時補強光強度。Another object of the present invention is to provide a light source module with uniform projected light intensity, which can arrange multiple groups of light-emitting element arrays to enhance the light intensity at different working distances.
為達上述目的,本發明提供一種具有均勻投射光強度之光源模組,包括:至少一發光元件陣列,包括:二第一型發光二極體,分別具有一第一傾斜角;或至少一該第一型發光二極體及至少一對第二型發光二極體,該第二型發光二極體係設於該第一型發光二極體之外圍,每一對該第二型發光二極體具有一第二傾斜角,該第二傾斜角大於該第一傾斜角。To achieve the above objective, the present invention provides a light source module with uniform projected light intensity, including: at least one light emitting element array, including: two first-type light emitting diodes, each having a first tilt angle; or at least one A first-type light-emitting diode and at least a pair of second-type light-emitting diodes, the second-type light-emitting diode system is arranged on the periphery of the first-type light-emitting diode, and each of the second-type light-emitting diodes The body has a second inclination angle, and the second inclination angle is greater than the first inclination angle.
根據本發明之實施例,該第一傾斜角為該第一型發光二極體之光束中心線與一垂直線之夾角,且該第一型發光二極體中愈靠近該發光元件陣列之中心者,其所具有的該第一傾斜角愈小。According to an embodiment of the present invention, the first inclination angle is the angle between the beam center line of the first-type light-emitting diode and a vertical line, and the closer the first-type light-emitting diode is to the center of the light-emitting element array Otherwise, the first angle of inclination it has is smaller.
根據本發明之實施例,該第二傾斜角為該第二型發光二極體之光束中心線與一垂直線之夾角。According to an embodiment of the present invention, the second inclination angle is the angle between the beam center line of the second-type light-emitting diode and a vertical line.
根據本發明之實施例,該第一型發光二極體為散射型發光二極體,其更包括一第一光束角,其為該第一型發光二極體之視場範圍夾角。該第一光束角約為45~90度角。According to an embodiment of the present invention, the first-type light-emitting diode is a scattering type light-emitting diode, which further includes a first beam angle, which is the angle of the field of view of the first-type light-emitting diode. The first beam angle is about 45 to 90 degrees.
根據本發明之實施例,該第二型發光二極體為標準型發光二極體,其更包括一第二光束角,其為該第二型發光二極體之視場範圍夾角。該第二光束角約為20~45度角。According to an embodiment of the present invention, the second-type light-emitting diode is a standard-type light-emitting diode, which further includes a second beam angle, which is the angle of the field of view of the second-type light-emitting diode. The second beam angle is about 20 to 45 degrees.
根據本發明之實施例,該第一型發光二極體之數量為偶數時,其係兩兩成對並對稱傾斜,愈靠中心者,其第一傾斜角愈小。而當該第一型發光二極體之數量為奇數時,位於正中間之該第一型發光二極體之第一傾斜角為0。According to an embodiment of the present invention, when the number of the first-type light-emitting diodes is an even number, they are symmetrically inclined in pairs. The closer to the center, the smaller the first inclination angle. When the number of the first-type light-emitting diode is an odd number, the first inclination angle of the first-type light-emitting diode in the middle is zero.
根據本發明之實施例,其中每一對該第二型發光二極體係對稱傾斜。該第二型發光二極體中愈靠近該發光元件陣列之邊緣者,其所具有的該第二傾斜角愈大。According to an embodiment of the present invention, each of them is symmetrically inclined to the second-type light-emitting diode system. The closer the second-type light-emitting diode is to the edge of the light-emitting element array, the greater the second inclination angle it has.
本發明提供一種具有均勻投射光強度之光源模組,其可應用在如第1圖所示之深度感測器中,在使用複數發光二極體之光源模組中使投影面積增加,且使投影面的光強度均勻化,解決先前技術中當光源發射後,光強度隨著光束發散而導致投射到投影面的光線產生強度分佈的改變或衰減,而使光強度的均勻度不佳。The present invention provides a light source module with uniform projected light intensity, which can be used in a depth sensor as shown in Figure 1. In a light source module using a plurality of light-emitting diodes, the projection area is increased, and The uniformity of the light intensity on the projection surface solves the problem that when the light source is emitted in the prior art, the light intensity changes or attenuates the intensity distribution of the light projected on the projection surface due to the divergence of the light beam, resulting in poor light intensity uniformity.
由於單顆發光二極體能提供的亮度有限,在一個大環境的空間中,為了應付不同工作距離的使用,必須要並聯多顆發光二極體來提供足夠的亮度和視場,第2圖即為本發明之發光元件陣列之示意圖,將m*n顆發光二極體10排列成一發光元件陣列12。Due to the limited brightness provided by a single light-emitting diode, in a large environmental space, in order to cope with the use of different working distances, it is necessary to connect multiple light-emitting diodes in parallel to provide sufficient brightness and field of view. It is a schematic diagram of the light-emitting element array of the present invention. The m*n light-emitting
在本發明中,發光元件陣列12上之發光二極體10假設只有二顆,則為第一型發光二極體,當發光二極體10的數量大於二,則包含第一型發光二極體及第二型發光二極體等二種,其中設於中間的是第一型發光二極體,為視角較大的散射型發光二極體,通常做為指示燈使用,包括約45~90度之一第一光束角,光束角為第一型發光二極體之視場範圍夾角,且若加大散射劑的量還可使第一光束角更大;第二型發光二極體係設於第一型發光二極體之外圍,此第二型發光二極體為標準型發光二極體,其包括約20~45度之一第二光束角,為第二型發光二極體之視場範圍夾角。In the present invention, assuming that there are only two light-emitting
此外,第一、第二型發光二極體還分別具有一第一、第二傾斜角,請同時參考第3圖,傾斜角為發光二極體之光束中心線16與一垂直線18之夾角,每一對第二型發光二極體係對稱傾斜,且第二傾斜角係大於第一傾斜角,進一步,第二型發光二極體中愈靠近發光元件陣列之邊緣者,其所具有的第二傾斜角還可增大,換言之,愈靠近邊緣的第二型發光二極體,其照射的角度可愈傾斜,如此一來發光元件陣列12便可覆蓋較大的視場範圍。以下將詳述在發光元件陣列12中第一、第二型發光二極體之配置。In addition, the first and second type LEDs also have a first and a second tilt angle respectively. Please refer to Figure 3 at the same time. The tilt angle is the angle between the
請參考第3圖,其為本發明具有均勻投射光強度之光源模組之第一實施例之示意圖,由於發光二極體之數量為二,沒有中央、邊緣之分,因此皆為第一型發光二極體102,亦即散射型發光二極體,此二顆第一型發光二極體102係互相對稱傾斜,以發光元件陣列之垂直線18為基準向外傾斜或旋轉,分別得到第一光束角ψ1
及光束中心線16之第一傾斜角θ1
。若此二顆第一型發光二極體102沒有第一傾斜角θ1
,都是垂直向上照射,顯然照射面積會縮小,且重疊部分的光度會特別亮,使光強度不均勻。而本發明將發光二極體傾斜或旋轉後,不但可得到較大的照射角度與照射面積,還可使光強度均勻。Please refer to Figure 3, which is a schematic diagram of the first embodiment of the light source module with uniform projection light intensity of the present invention. Since the number of light-emitting diodes is two, there is no distinction between the center and the edge, so they are all of the first type. The light-emitting
第4圖為本發明具有均勻投射光強度之光源模組之第二實施例之示意圖,其中發光二極體之數量為三。由於發光二極體之數量為奇數,因此中間者為第一型發光二極體102(亦即散射型發光二極體),其第一傾斜角θ1
為0(圖中未示),而外側兩顆為第二型發光二極體104,亦即標準型發光二極體,其第二傾斜角為θ2
,此外,第一型發光二極體102具有第一光束角ψ1
,第二型發光二極體104具有第二光束角ψ2
,由圖中可看出,中間的第一型發光二極體102視場範圍大,而兩側的第二型發光二極體104視場範圍較小,結合第二型發光二極體104適當的傾斜或偏轉θ2
,使三顆發光二極體102、104之視場範圍增加、減少照射的重疊面積,並使投影面上的光強度均勻化。FIG. 4 is a schematic diagram of the second embodiment of the light source module with uniform projected light intensity according to the present invention, in which the number of light-emitting diodes is three. Since the number of light-emitting diodes is an odd number, the middle one is the first type light-emitting diode 102 (that is, the scattering type light-emitting diode), and its first tilt angle θ 1 is 0 (not shown in the figure), and The two outer ones are second-type light-emitting
當發光二極體之數量大於四、且為奇數時,第一型發光二極體102可為一顆或奇數顆,除了正中間的是垂直設置之外,其他的第一型發光二極體102則是兩兩成對,具有第一傾斜角θ1
。而第二型發光二極體104本身就是成對設置,可包括不只一對,舉例而言,若發光二極體之數量為7,則可包括三顆第一型發光二極體102(其中二顆成對)及兩對第二型發光二極體104;或是只有中間者為第一型發光二極體102,其餘六顆則分成三對第二型發光二極體104,每一對具有相同或不同的第二傾斜角為θ2
,當第二傾斜角θ2
不同時,愈靠外圍的第二型發光二極體104,其第二傾斜角為θ2
愈大。When the number of light-emitting diodes is greater than four and is an odd number, the number of first-type light-emitting
第5圖為本發明具有均勻投射光強度之光源模組之第三實施例之示意圖,其中發光二極體之數量為四。由於發光二極體之數量為偶數,因此中間者為一對第一型發光二極體102(亦即散射型發光二極體),其具有第一傾斜角θ1
,使二顆第一型發光二極體102的照射重疊面積減小,而外側兩顆為第二型發光二極體104,亦即標準型發光二極體,其具有第二傾斜角為θ2
,使第一、第二發光二極體102、104的照射重疊面積減小,增加視場範圍。此外,第一型發光二極體102具有第一光束角ψ1
,第二型發光二極體104具有第二光束角ψ2
。Fig. 5 is a schematic diagram of a third embodiment of a light source module with uniform projected light intensity according to the present invention, in which the number of light-emitting diodes is four. Since the number of light-emitting diodes is an even number, the middle one is a pair of first-type light-emitting diodes 102 (that is, scattering-type light-emitting diodes), which have a first inclination angle θ 1 , so that two first-type light-emitting diodes The irradiation overlap area of the light-
當發光二極體之數量大於四、且為偶數時,則第一型發光二極體102可為二顆或偶數顆,兩兩成對設置,具有第一傾斜角θ1
。而第二型發光二極體104本身就是成對設置,可包括不只一對,舉例而言,若發光二極體之數量為8,則可包括四顆(二對)第一型發光二極體102及兩對第二型發光二極體104,且二對第一型發光二極體102的第一傾斜角θ1
相同或不同,當第一傾斜角θ1
不同時,靠中間者的第一傾斜角θ1
較小,二對第二型發光二極體104的第二傾斜角θ2
也可為相同或不同,當第二傾斜角θ2
不同時,靠外圍者的第二傾斜角θ2
較大;或是只有靠中間的一對為第一型發光二極體102,其餘六顆則分成三對第二型發光二極體104,每一對具有相同或不同的第二傾斜角為θ2
,第二傾斜角θ2
不同時,愈靠外圍的第二型發光二極體104,其第二傾斜角為θ2
愈大。When the number of light-emitting diodes is greater than four and is an even number, the number of first-type light-
本發明之光源模組可製作於任何材質之基板上,基板之材質不受限制。The light source module of the present invention can be fabricated on a substrate of any material, and the material of the substrate is not limited.
本發明之光強度均勻性之公式如下式: 其中Imax 為最大光強度,I光束角 為發光二極體的光束角不同時之光強度。The formula for the uniformity of light intensity in the present invention is as follows: Among them, I max is the maximum light intensity, and I beam angle is the light intensity of the light-emitting diode at different beam angles.
以下以實際實驗數據為實施例說明。當光源模組中之發光二極體數量為三顆時,假設中間的第一型發光二極體之光束角為90度,兩側之第二行發光二極體之光束角為45度,則光強度對應極座標之關係圖如第6圖所示。再模擬光強度分佈,第7A圖為先前技術中正規化的光強度對應發射角度(LED傾斜角)之光強度分佈模擬示意圖,可看出光強度都集中在中間位置,而往兩側會迅速下降,第7B圖及第7C圖則分別為二顆第二型發光二極體分別傾斜40度及50度之光強度分佈模擬示意圖,顯然傾斜角40度之結構時,光強度的總和是漸進式緩坡下降,而不是迅速下降。The following uses actual experimental data as an example for description. When the number of light-emitting diodes in the light source module is three, it is assumed that the beam angle of the first type light-emitting diode in the middle is 90 degrees, and the beam angle of the second row of light-emitting diodes on both sides is 45 degrees. Then the relationship between light intensity and polar coordinates is shown in Figure 6. Then simulate the light intensity distribution. Figure 7A is a schematic diagram of the light intensity distribution simulation of the normalized light intensity corresponding to the emission angle (LED tilt angle) in the prior art. It can be seen that the light intensity is concentrated in the middle position, and the light intensity will drop rapidly to both sides. Fig. 7B and Fig. 7C are the simulated schematic diagrams of the light intensity distribution of two second-type light-emitting diodes inclined at 40 degrees and 50 degrees respectively. Obviously, when the structure is inclined at 40 degrees, the total light intensity is progressive. A gentle slope descends, rather than a rapid descent.
第8圖為本發明第一實施例中,二顆第一型發光二極體具有不同傾斜角時之光強度分佈模擬示意圖。由圖中可清楚看出,發光二極體傾斜或旋轉之角度不同時,對光強度分佈之影響極大,當傾斜角大於27度時顯然光強度較為均勻。Fig. 8 is a simulated schematic diagram of light intensity distribution when two first-type light-emitting diodes have different inclination angles in the first embodiment of the present invention. It can be clearly seen from the figure that when the angle of tilt or rotation of the light-emitting diode is different, it has a great influence on the light intensity distribution. When the tilt angle is greater than 27 degrees, the light intensity is obviously more uniform.
第9圖為本發明第一實施例中,二顆第一型發光二極體的光束中心線傾斜(或旋轉)不同角度時,光強度在20%均勻度的視場角變化模擬示意圖。此部分係利用 Zemax 模擬一對稱光束角90°的第一型發光二極體,依不同的光軸傾斜/旋轉角度θ=0°、3°、6°、9°、12°、15°、18°、21°、24°、27°和30°時的光強度分佈。在依照上述公式定義的光強度均勻度所歸納之當光強度均勻度在 20% 時的視場角變化。當θ>24度時,視場角迅速擴大。Figure 9 is a schematic diagram of the field angle variation simulation of the light intensity at 20% uniformity when the beam center lines of two first-type light-emitting diodes are inclined (or rotated) at different angles in the first embodiment of the present invention. This part uses Zemax to simulate a first-type light-emitting diode with a symmetrical beam angle of 90°, with different optical axis tilt/rotation angles θ=0°, 3°, 6°, 9°, 12°, 15°, Light intensity distribution at 18°, 21°, 24°, 27° and 30°. According to the light intensity uniformity defined by the above formula, the field angle change when the light intensity uniformity is 20% is summarized. When θ>24 degrees, the angle of view expands rapidly.
第10圖為本發明第一實施例中,當二顆第一型發光二極體的傾斜角為27度時,在不同工作距離下之光強度變化模擬示意圖。工作距離愈大,光強度愈小。Figure 10 is a simulated schematic diagram of light intensity changes at different working distances when the inclination angle of two first-type light-emitting diodes is 27 degrees in the first embodiment of the present invention. The greater the working distance, the smaller the light intensity.
綜上所述,本發明之具有均勻投射光強度之光源模組,包含多顆兩兩成對、互相對稱的發光二極體,該對稱係以一光束中心線之傾斜/旋轉角度進行,且當發光二極體之數量為奇數時,正中間者不傾斜/旋轉,其餘者對稱傾斜或旋轉,傾斜角可自由調整;同時,本發明採用不同光束角之發光二極體,其中內側為光束角較大的第一型發光二極體,外側則使用光束角較小的第二型發光二極體來補強不同角度的光強度,以優化不同角度光強度的均勻性,且光束角亦可自由調整。當工作距離增加時,由於光強度會變弱,因此本發明還可增加發光二極體之數目(例如點亮旁邊的另一發光元件陣列)來優化工作距離的亮度。因此,本發明不但可將投影面的光強度均勻化,還可擴大投影範圍,節省光學擴散膜設計的需求,有利兼顧光強度均勻特性和降低製作成本。In summary, the light source module with uniform projected light intensity of the present invention includes a plurality of pairs of light emitting diodes that are symmetrical to each other, and the symmetry is performed at a tilt/rotation angle of the center line of the beam, and When the number of LEDs is an odd number, the one in the middle will not tilt/rotate, and the rest will tilt or rotate symmetrically, and the tilt angle can be adjusted freely. At the same time, the present invention uses LEDs with different beam angles, where the inner side is the beam The first type LED with a larger angle, the second type LED with a smaller beam angle is used on the outside to reinforce the light intensity at different angles to optimize the uniformity of the light intensity at different angles, and the beam angle can also be Free adjustment. When the working distance increases, the light intensity will become weaker, so the present invention can also increase the number of light-emitting diodes (for example, light up another light-emitting element array next to it) to optimize the brightness of the working distance. Therefore, the present invention can not only uniformize the light intensity of the projection surface, but also expand the projection range, save the need for the design of the optical diffusion film, and is beneficial to take into account the uniformity of the light intensity and reduce the production cost.
唯以上所述者,僅為本發明之較佳實施例而已,並非用來限定本發明實施之範圍。故即凡依本發明申請範圍所述之特徵及精神所為之均等變化或修飾,均應包括於本發明之申請專利範圍內。Only the above are only preferred embodiments of the present invention, and are not used to limit the scope of implementation of the present invention. Therefore, all equivalent changes or modifications made in accordance with the characteristics and spirit of the application scope of the present invention shall be included in the patent application scope of the present invention.
100:光源模組
110:濾光片
120:光感測器
10:發光二極體
102:第一型發光二極體
104:第二型發光二極體
12:發光元件陣列
16:光束中心線
18:垂直線100: light source module
110: filter
120: light sensor
10: Light-emitting diode
102: The first type of light-emitting diode
104:
第1圖為應用於深度感測器之側面示意圖。 第2圖為本發明之發光元件陣列之示意圖。 第3圖為本發明具有均勻投射光強度之光源模組之第一實施例之示意圖,其中發光二極體之數量為二。 第4圖為本發明具有均勻投射光強度之光源模組之第二實施例之示意圖,其中發光二極體之數量為三。 第5圖為本發明具有均勻投射光強度之光源模組之第三實施例之示意圖,其中發光二極體之數量為四。 第6圖為應用本發明之光源模組的光強度對應極座標之關係圖。 第7A圖為正規化光強度對應發射角度(LED傾斜角)之光強度分佈模擬示意圖。 第7B圖及第7C圖分別為本發明第二實施例中,二顆第二型發光二極體傾斜40度及50度之光強度分佈模擬示意圖。 第8圖為本發明第一實施例中,二顆第一型發光二極體具有不同傾斜角時之光強度分佈模擬示意圖。 第9圖為本發明第一實施例中,二顆第一型發光二極體的光束中心線傾斜(或旋轉)不同角度時,光強度在20%均勻度的視場角變化模擬示意圖。 第10圖為本發明第一實施例中,當二顆第一型發光二極體的傾斜角為27度時,在不同工作距離下之光強度變化模擬示意圖。Figure 1 is a schematic side view of a depth sensor applied to it. Figure 2 is a schematic diagram of the light-emitting element array of the present invention. Figure 3 is a schematic diagram of the first embodiment of the light source module with uniform projected light intensity according to the present invention, in which the number of light-emitting diodes is two. Figure 4 is a schematic diagram of the second embodiment of the light source module with uniform projected light intensity according to the present invention, in which the number of light-emitting diodes is three. Figure 5 is a schematic diagram of a third embodiment of a light source module with uniform projected light intensity according to the present invention, in which the number of light-emitting diodes is four. Figure 6 is a diagram showing the relationship between the light intensity of the light source module to which the present invention is applied to the polar coordinates. Figure 7A is a schematic diagram of the light intensity distribution simulation of the normalized light intensity corresponding to the emission angle (LED tilt angle). Fig. 7B and Fig. 7C are respectively schematic diagrams of simulated light intensity distribution of two second-type light-emitting diodes inclined at 40 degrees and 50 degrees in the second embodiment of the present invention. Fig. 8 is a simulated schematic diagram of light intensity distribution when two first-type light-emitting diodes have different inclination angles in the first embodiment of the present invention. Figure 9 is a schematic diagram of the field angle variation simulation of the light intensity at 20% uniformity when the beam center lines of two first-type light-emitting diodes are inclined (or rotated) at different angles in the first embodiment of the present invention. Figure 10 is a simulated schematic diagram of light intensity changes at different working distances when the inclination angle of two first-type light-emitting diodes is 27 degrees in the first embodiment of the present invention.
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