M412365 五、新型說明： 【新型所屬之技術領域】 本創作係關於-種光源模擬器，詳言之，係關於一種聚 光型光源模擬器。 【先前技術】 隨著環保與節能之議題日漸受到重視，太陽能電池模組 逐漸蓬勃發展。然而當太陽能電池模組製造完成後所面臨 的一個重大問題就是測試。由於自然光（太陽光）在一天之 中會有強有弱，其並不穩定而且無法經由人為方式控制， 所以通常不會把製造完成後之太陽能電池模組搬到室外作 測试，一般習知之測試方式是在室内使用人工的光源來模 擬日照以取得太陽能電池模組相關的產品特性。 該太陽能電池模組在實際使用時，為了提高其效率，通 常會搭配使用一追日裝置，該追日裝置可使太陽光類平行 地照射到該太陽能電池模組。然而，太陽光實際上具有一 約〇·5度的發.散角度。因此，如何在測試時模擬出上述情 況，便是一大課題。 【新型内容】 本創作提供一種聚光型光源模擬器，其包括一光源、一 橢圓反射面鏡、一透鏡、一柱狀鏡組及一準直鏡。該光源 係用以產生光線。該橢圓反射面鏡具有一第一焦點及一第 二焦點，該光源係位於該第一焦點，使得其產生之光線經 由該橢圓反射面鏡反射。該透鏡係用以將來自該橢圓反射 面鏡之光線平行射出。該柱狀鏡組截面具有一最大寬度， 154594.doc M412365 該柱狀鏡組包括複數個柱狀鏡單元，用以將來自該透鏡之 光線聚焦後再發散而投射於該準直鏡上。其中通過每一柱 狀鏡單元之光線會涵蓋整個準直鏡，該準直鏡與該柱狀鏡 組間隔一距離，該最大寬度/該距離之比值係介於〇 〇〇3至 0.017，該準直鏡用以將來自該柱狀鏡組之光線類平行地 投射於一投射面上。 本創作另提供一種聚光型光源模擬器，其包括一光源、 一橢圓反射面鏡、一透鏡、一柱狀鏡組及一準直鏡。該光 源係用以產生光線。該橢圓反射面鏡具有一第一焦點及一 第二焦點，該光源係位於該第一焦點，使得其產生之光線 經由該橢圓反射面鏡反射後聚焦於該第二焦點。該透鏡係 用以將來自該橢圓反射面鏡之光線平行射出。該柱狀鏡組 包括複數個柱狀鏡單元，該柱狀鏡組係用以將來自該透鏡 之光線聚焦後再發散出去。該準直鏡係用以將來自該柱狀 鏡組之光線類平行地投射於一投射面上。其中通過每一柱 狀鏡單元之光線會涵蓋整個準直鏡，當然該光線也會涵蓋 整個投射面。該準直鏡與該柱狀鏡組間隔一距離，且該距 離係為該準直鏡之焦距。 在本創作令’藉由調整該柱狀鏡組截面之最大寬度以及 該準直鏡與該柱狀鏡組間之距離，可使得投射在該投射面 上之光線之最大發散角約為0.5度，其與太陽光之發散角 相同。爰此’該聚光型光源模擬器所產生之光線可以類平 行地照射到位於該投射面之待測試模組。故，該聚光型光 源模擬器可以模擬實際之太陽光，完全符合高聚光型太陽 154594.doc 能（High C〇nCentrated ph〇t〇v〇ltaic，Hcpv)模組之測試需 求。 【實施方式】 凊參考圖1，顯示本創作聚光型光源模擬器之第一實施 例之不意圖。本創作之聚光型光源模擬器1係可以在室内 使用來模擬日照以測試太陽能電池模組而取得其相關的產 rrn特性，如太陽能電池模組的電流電壓曲線。然而，可以 理解的是’本創作之聚光型光源模擬器1也可以應用於其 他需要準直及均勻光線之場所，其適用領域並不具偈限 性。該聚光型光源模擬器丨包括一光源n、一橢圓反射面 鏡12、一透鏡13、一柱狀鏡組14及一準直鏡15。 該光源11係用以產生光線。在本實施例中，該光源丨j係 為一點光源’例如：氙燈，其包括二個端電極111。該等 端電極11 1係連接至一電源，以供給該光源丨丨點亮時所需 的電壓及電流。附帶一提’該光源丨丨只要符合點光源的概 念’並且是氣體放電燈，該光源丨丨並不侷限於氙燈。 該橢圓反射面鏡12之内側壁係為一橢圓面，其具有一第 一焦點121及一第二焦點122。該光源11係位於該第一焦點 121 ’使得其產生之光線經由該橢圓反射面鏡12反射出 去°較佳地，該橢圓反射面鏡12係附著於一燈罩上。 在本實施例中，該聚光型光源模擬器1更包括一支撐座 1 9係用以支撐該光源丨丨。該橢圓反射面鏡12更包括一開口 123 ’該光源11之一端係穿過該開口 123而固設於該支撐座 19。 ! 54594.doc M412365 該透鏡13用以將來自該橢圓反射面鏡12之光線平行射 出。該透鏡13可以是一凸透鏡、凹透鏡或球面透鏡。在本 實施例中，該透鏡13係為一雙凸透鏡，且其設置於該第二 焦點122之外。亦即，該第二焦點122係位於該第一焦點 121及該透鏡13之間，使得該光源n產生之光線經由該橢 圓反射面鏡12反射後先聚焦於該第二焦點122後，再經由 該透鏡13平行射至該柱狀鏡組14。 然而，在其他實施例中，該透鏡13係為一雙凹透鏡，且 其係位於該第一焦點121及第二焦點122之間，使得該光源 π產生之光線經由該橢圓反射面鏡12反射後直接經由該透 鏡13平行射至該柱狀鏡組14，而不會聚焦在該第二焦點 122。 ’’ 請同時參考圖2 ’顯示本創作聚光型光源模擬器之第一 實施例中柱狀鏡組之第-態樣之前視示意^該柱狀鏡組 14之截面具有一最大寬度〇。該柱狀鏡組14包括複數個柱 狀鏡單S Μ卜該等柱狀鏡單元⑷之外形可以是為矩形 (如圖2所示）、圓形或六邊形（如圖3所示）。或者，該等柱 狀鏡單元141也可以區分為複數個聚集部分(例如四個聚集 部份，如圖4所示），且該等聚集部分之間利用遮光材料 142做區隔》 在圖2中，該等柱狀鏡單元141之材質係為石英，石英可 以耐高溫同時保持高的紫外光穿透率。該柱狀鏡組Μ係大 致上由該等柱狀鏡單元141排列成—個㈣陣列之矩形。也 就說該柱狀鏡組14會有6χ6個柱狀鏡單元ΐ4ι，但不以㈣ 154594.doc M412365 個為限。該最大寬度D係為整個該柱狀鏡組14截面之對角 線長度，實際上若以一個虛圓將該柱狀鏡組14做最小包 覆該最大寬度D即為該虛圓的直徑。 凊繼續參考圖5，其顯示本創作聚光型光源模擬器之第 一實施例中柱狀鏡組之柱狀鏡單元之示意圖。具體而言， 每一柱狀鏡單元141都由一個第一透鏡單元1411與一個第 二透鏡單元1412所組成，該第二透鏡單元1412恰位於該第 一透鏡單元1411的焦點。光線由該透鏡13平行射至每一柱 狀鏡單元141的第一透鏡單元1411，然後該光線聚焦於該 第一透鏡單元1411的焦點上，也就是直接聚焦於該第二透 鏡單元1412上。最終該光線再由該第二透鏡單元1412發散 出去。 該準直鏡1 5係用以將來自該柱狀鏡組14之光線類平行地 投射於一投射面16上，其中通過每一柱狀鏡單元141之光 線會涵蓋整個該準直鏡15。在本實施例中，該準直鏡15係 為一菲淫爾透鏡（Fresnel Lens)。該投射面16係用以置放一 待測試模組（例如一太陽能電池模組）（圖中未示），該投射 面16與該準直鏡15間隔一適當距離。 睛同時參考圖6’該準直鏡15與該柱狀鏡組14間隔一距 離L’且該距離L係為該準直鏡15之焦距。由圖中可看出， 通過每一柱狀鏡單元141之光線會涵蓋整個該準直鏡15， 且該柱狀鏡組14中相距最遠之二個柱狀鏡單元ι41投射於 該該準直鏡15之同一點時之夹角係定義為θ，因此，再經 過該準直鏡15折射出去之光線之最大發散角亦為0。由於 154594.doc M412365 該距離L遠大於該柱狀鏡組μ截面之最大寬度d，因此該 柱狀鏡組14截面之最大寬度d/該距離l之比值係定義為 sine，且〇.2〇。<0<1。。亦即’該最大寬度D/該距離[之比值 係介於0.003至0.017。在一實施例中，θ=〇.5。，該比值為 0-0087，D=17.45 mm，L=2000 mm，該準直鏡 15之焦距亦 等於2000 mm，且該投射面16之面積係為3〇 cmx3〇 cm。 整體說來，本創作之聚光型光源模擬器1利用調配最大寬 度D與距離L’使得投射於該準直鏡15光線之最大發散角θ 收斂在〇.2〇。<0<1。之間。最終，藉由該準直鏡15之導正， 俾使所有投射在該投射面16上的光線之最大發散角0亦收 斂在0·20°<θ<1。之間’換言之，因為光線之發散角0很小， 故’吾人定義光線得以類平行的方式投射在該投射面丨6。 進一步說明，該準直鏡15之功用僅在於將投射之光線做一 方位之轉換以配合該投射面16，並不會改變光線之發散角 Θ的大小，合此述明》 請參考圖7 ’顯示本創作聚光型光源模擬器之第二實施 例之示意圖。較佳地，該聚光型光源模擬器2更包括一遽 鏡17及一勻光元件18。該濾鏡17係位於該柱狀鏡組14及該 準直鏡15之間，其用以過濾通過該柱狀鏡組14之光線，以 增進光讚的表現（Performance)。該勻光元件18(例如一檔 片或鐵絲網）係位於該濾鏡1 7及該準直鏡1 5之間，用以增 加該投射面16上之光線之均勻性。詳言之，使用者可藉由 該投射面16上光線均勻性之變化，動態的使用該勻光元件 18以遮擋光線強度較強之處，遂利於該投射面16整體光線 I54594.doc M412365 均勻性之表現。 綜上所述’在本創作中，投射在該投射面16上之光線之 最大發散角為Θ，藉由調整該柱狀鏡組丨4截面之最大寬度d 以及該準直鏡15與該柱狀鏡組14間之距離l，可使得該最 大發散角Θ約為0.5度’其與太陽光之發散角相同。爰此， 該聚光型光源模擬器1所產生之光線可以類平行地照射到 位於該投射面16之待測試模組。故，該聚光型光源模擬器 1可以模擬實際之太陽光，完全符合高聚光型太陽能（HighM412365 V. New Description: [New Technology Field] This creation is about a kind of light source simulator. In more detail, it is about a concentrating light source simulator. [Prior Art] With the increasing emphasis on environmental protection and energy conservation, solar cell modules have gradually flourished. However, one of the major problems faced when solar cell modules are manufactured is testing. Since natural light (sunlight) is strong and weak during the day, it is unstable and cannot be controlled by humans. Therefore, the solar cell module after the completion of manufacturing is usually not moved to the outside for testing. The test method is to use artificial light sources indoors to simulate sunshine to obtain product characteristics related to solar cell modules. In order to improve the efficiency of the solar battery module in actual use, a day-tracking device is usually used in combination with the sun-lighting device to allow sunlight to be irradiated to the solar battery module in parallel. However, the sunlight actually has a divergence angle of about 5 degrees. Therefore, how to simulate the above situation during testing is a major issue. [New content] The present invention provides a concentrating light source simulator comprising a light source, an elliptical reflecting mirror, a lens, a cylindrical mirror and a collimating mirror. This light source is used to generate light. The elliptical reflecting mirror has a first focus and a second focus, and the light source is located at the first focus such that light generated by the elliptical reflecting mirror is reflected by the elliptical reflecting mirror. The lens is used to emit light from the elliptical mirror in parallel. The cylindrical lens section has a maximum width, 154594.doc M412365 The cylindrical lens set includes a plurality of cylindrical mirror elements for focusing the light from the lens and then diverging and projecting onto the collimating mirror. The light passing through each of the cylindrical mirror units covers the entire collimating mirror, and the collimating mirror is spaced apart from the cylindrical mirror group by a ratio of 〇〇〇3 to 0.017. The collimating mirror is used to project light rays from the lenticular lens group in parallel on a projection surface. The present invention further provides a concentrating light source simulator comprising a light source, an elliptical reflecting mirror, a lens, a cylindrical mirror group and a collimating mirror. This light source is used to generate light. The elliptical reflecting mirror has a first focus and a second focus, and the light source is located at the first focus such that the generated light is reflected by the elliptical reflecting mirror and then focused on the second focus. The lens is used to emit light from the elliptical reflecting mirror in parallel. The lenticular lens assembly includes a plurality of lenticular mirror units for focusing the light from the lens and then dissipating it. The collimating mirror is used to project light rays from the lenticular lens group in parallel onto a projection surface. The light passing through each of the lenticular elements covers the entire collimating mirror, which of course covers the entire projection surface. The collimating mirror is spaced from the cylindrical mirror group by a distance and the focal length is the focal length of the collimating mirror. In the present invention, by adjusting the maximum width of the cross section of the lenticular lens and the distance between the collimating mirror and the lenticular lens set, the maximum divergence angle of the light projected on the projection surface is about 0.5 degrees. It is the same as the divergence angle of sunlight. The light generated by the concentrating light source simulator can be illuminated in parallel to the module to be tested located on the projection surface. Therefore, the concentrating light source simulator can simulate actual sunlight, and fully meets the test requirements of the high-concentration solar 154594.doc (High C〇nCentrated ph〇t〇v〇ltaic, Hcpv) module. [Embodiment] Referring to Fig. 1, a first embodiment of the present concentrating light source simulator is shown. The concentrating light source simulator 1 of the present invention can be used indoors to simulate sunlight to test solar cell modules to obtain related rrn characteristics, such as current and voltage curves of solar cell modules. However, it can be understood that the concentrating light source simulator 1 of the present invention can also be applied to other places where collimation and uniform light are required, and the applicable field is not limited. The concentrating light source simulator 丨 includes a light source n, an elliptical reflecting mirror 12, a lens 13, a cylindrical mirror group 14, and a collimating mirror 15. The light source 11 is used to generate light. In the present embodiment, the light source 丨j is a one-point light source 'e.g., a xenon lamp, which includes two terminal electrodes 111. The terminal electrodes 11 1 are connected to a power source to supply the voltage and current required for the light source to illuminate. Incidentally, the light source 丨丨 is a gas discharge lamp as long as it conforms to the concept of a point light source, and the light source 丨丨 is not limited to a xenon lamp. The inner side wall of the elliptical reflecting mirror 12 is an elliptical surface having a first focus 121 and a second focus 122. The light source 11 is located at the first focus 121 ′ such that the light generated therefrom is reflected by the elliptical reflecting mirror 12 . Preferably, the elliptical reflecting mirror 12 is attached to a lamp cover. In this embodiment, the concentrating light source simulator 1 further includes a support base for supporting the light source 丨丨. The elliptical reflecting mirror 12 further includes an opening 123'. One end of the light source 11 is fixed to the supporting seat 19 through the opening 123. 54594.doc M412365 This lens 13 is used to emit light from the elliptical reflecting mirror 12 in parallel. The lens 13 can be a convex lens, a concave lens or a spherical lens. In the present embodiment, the lens 13 is a lenticular lens and is disposed outside the second focus 122. That is, the second focus 122 is located between the first focus 121 and the lens 13 such that the light generated by the light source n is reflected by the elliptical reflecting mirror 12 and then focused on the second focus 122, and then The lens 13 is incident on the lenticular lens group 14 in parallel. However, in other embodiments, the lens 13 is a double concave lens and is located between the first focus 121 and the second focus 122 such that the light generated by the light source π is reflected by the elliptical reflector 12 Directly passing through the lens 13 to the lenticular lens group 14 without focusing on the second focus 122. Referring to Fig. 2' at the same time, the first embodiment of the cylindrical lens group in the first embodiment of the present concentrating light source simulator is shown in the front view. The cross section of the cylindrical lens group 14 has a maximum width 〇. The lenticular lens group 14 includes a plurality of columnar mirrors S Μ 该 该 该 该 该 该 该 该 该 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外 之外. Alternatively, the lenticular mirror unit 141 may also be divided into a plurality of concentrating portions (for example, four concentrating portions, as shown in FIG. 4), and the concentrating portions are partitioned by the light shielding material 142. The material of the columnar mirror unit 141 is quartz, and the quartz can withstand high temperatures while maintaining high ultraviolet light transmittance. The columnar lens assembly is substantially rectangular in shape by the array of mirror elements 141 in a (four) array. It is also said that the lenticular lens set 14 has 6 χ 6 cylindrical mirror elements ΐ 4ι, but not limited to (4) 154594.doc M412365. The maximum width D is the diagonal length of the entire cross section of the lenticular lens group 14. In fact, if the lenticular lens group 14 is minimized by a virtual circle, the maximum width D is the diameter of the imaginary circle. Continuing to refer to Fig. 5, there is shown a schematic view of a cylindrical mirror unit of a cylindrical lens assembly in the first embodiment of the present concentrating light source simulator. Specifically, each of the lenticular mirror units 141 is composed of a first lens unit 1411 and a second lens unit 1412 which is located at the focus of the first lens unit 1411. The light is directed by the lens 13 in parallel to the first lens unit 1411 of each of the columnar mirror units 141, and then the light is focused on the focus of the first lens unit 1411, i.e., directly focused on the second lens unit 1412. Eventually the light is again diverged by the second lens unit 1412. The collimating lens 15 is used to project light rays from the lenticular lens group 14 in parallel onto a projection surface 16, wherein the light passing through each of the lenticular mirror units 141 covers the entire collimating mirror 15. In the present embodiment, the collimating mirror 15 is a Fresnel Lens. The projection surface 16 is for placing a module to be tested (for example, a solar cell module) (not shown), and the projection surface 16 is spaced apart from the collimating mirror 15 by an appropriate distance. Referring to Fig. 6', the collimating mirror 15 is spaced apart from the cylindrical lens group 14 by a distance L' which is the focal length of the collimating mirror 15. As can be seen from the figure, the light passing through each of the columnar mirror units 141 covers the entire collimating mirror 15, and the two columnar mirror units ι41 which are furthest apart from the columnar mirror group 14 are projected onto the quasi-lens mirror 15 The angle at which the straight mirror 15 is at the same point is defined as θ, and therefore, the maximum divergence angle of the light refracted by the collimating mirror 15 is also zero. Since the distance L is much larger than the maximum width d of the μ section of the lenticular lens group, the ratio of the maximum width d/the distance l of the cross section of the lenticular lens group 14 is defined as sine, and 〇.2〇 . <0<1. . That is, the ratio of the maximum width D / the distance [between 0.003 and 0.017. In an embodiment, θ = 〇.5. The ratio is 0-0087, D = 17.45 mm, L = 2000 mm, the focal length of the collimating mirror 15 is also equal to 2000 mm, and the area of the projection surface 16 is 3 〇 cm x 3 〇 cm. In summary, the concentrating light source simulator 1 of the present invention utilizes the maximum width D and the distance L' to converge the maximum divergence angle θ of the light projected onto the collimating mirror 15 at 〇.2〇. <0<1. between. Finally, by the conduction of the collimating mirror 15, the maximum divergence angle 0 of all the rays projected on the projection surface 16 is also converged at 0·20° < θ < In other words, since the divergence angle 0 of the light is small, the 'defined light rays are projected in the parallel plane on the projection surface 丨6. Further, the function of the collimating mirror 15 is only to convert the projected light into one direction to match the projection surface 16, and does not change the divergence angle 光线 of the light, which is described in the following description. A schematic view of a second embodiment of the present concentrating light source simulator is shown. Preferably, the concentrating light source simulator 2 further includes a frog mirror 17 and a light concentrating element 18. The filter 17 is located between the lenticular lens group 14 and the collimating mirror 15 for filtering light passing through the lenticular lens group 14 to enhance the performance of the accompaniment. The light homogenizing element 18 (e.g., a sheet or wire mesh) is positioned between the filter 17 and the collimating lens 15 for increasing the uniformity of light on the projection surface 16. In detail, the user can dynamically use the light homogenizing element 18 to block the intensity of the light by the change of the uniformity of the light on the projection surface 16, so that the overall light of the projection surface 16 is uniform, I54594.doc M412365 is uniform. Performance of sex. In summary, in the present creation, the maximum divergence angle of the light projected on the projection surface 16 is Θ, by adjusting the maximum width d of the cross section of the cylindrical lens group 以及4 and the collimating mirror 15 and the column The distance l between the lens groups 14 is such that the maximum divergence angle Θ is about 0.5 degrees' which is the same as the divergence angle of the sunlight. Thus, the light generated by the concentrating light source simulator 1 can be illuminated in parallel to the module to be tested located on the projection surface 16. Therefore, the concentrating light source simulator 1 can simulate actual sunlight and is fully compatible with high concentrating solar energy (High
Concentrated Photovoltaic，HCPV)模組之測試需求。 上述實施例僅為說明本創作之原理及其功效，並非限制 本創作。因此習於此技術之人士對上述實施例進行修改及 變化仍不脫本創作之精神。本創作之權利範圍應如後述之 申請專利範圍所列。 【圖式簡單說明】 圖1顯示本創作聚光型光源模擬器之第一實施例之示意Concentrated Photovoltaic, HCPV) module testing requirements. The above embodiments are merely illustrative of the principles and functions of the present invention and are not intended to limit the creation. Therefore, those skilled in the art can revise and change the above embodiments without departing from the spirit of the present invention. The scope of the rights of this creation shall be as set forth in the scope of the patent application described later. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 shows a schematic diagram of a first embodiment of the present concentrating light source simulator.
Tgl · 圓， 圖2顯示本創作聚光型光源模擬器之第一實施例中柱狀 鏡組之第一態樣之前視示意圖； 圖3顯示本創作聚光型光源模擬器之第一實施例中柱狀 鏡組之第二態樣之前視示意圖； 圖4顯示本創作聚光型光源模擬器之第一實施例中柱狀 鏡組之第三態樣之前視示意圖； 圖5顯示本創作聚光型光源模擬器之第一實施例中柱狀 鏡組之柱狀鏡單元之示意圖； 154594.doc -10- M412365 圖6顯示本創作聚光型光源模擬器之第一實施例中該準 直鏡與該柱狀鏡組間之距離；及 圖7顯示本創作聚光型光源模擬器之第二實施例之示意 圖。 【主要元件符號說明】 1 本創作聚光型光源模擬器之第一實施例 2 本創作聚光型光源模擬器之第二實施例 11 光源 12 橢圓反射面鏡 13 透鏡 14 柱狀鏡組 15 準直鏡 16 投射面 17 濾鏡 18 勻光元件 19 支撐座 111 端電極 121 第一焦點 122 第二焦點 123 開口 141 柱狀鏡單元 142 遮光材料 1411 第一透鏡單元 1412 第二透鏡單元 154594.doc -11 - M412365 D 柱狀鏡組戴面之最大寬度 L 距離Tgl · circle, FIG. 2 shows a front view of a first aspect of the cylindrical lens group in the first embodiment of the present concentrating light source simulator; FIG. 3 shows a first embodiment of the present concentrating light source simulator 2 is a front view of the second aspect of the columnar lens group; FIG. 4 is a front view showing a third aspect of the columnar lens group in the first embodiment of the present concentrating light source simulator; Schematic diagram of the cylindrical mirror unit of the cylindrical lens group in the first embodiment of the light source light source simulator; 154594.doc -10- M412365 Fig. 6 shows the collimation in the first embodiment of the present concentrating light source simulator The distance between the mirror and the cylindrical lens group; and FIG. 7 shows a schematic view of the second embodiment of the present concentrating light source simulator. [Description of main component symbols] 1 The first embodiment of the present concentrating light source simulator 2 The second embodiment of the concentrating concentrating light source simulator 11 Light source 12 Elliptical reflecting mirror 13 Lens 14 Cylindrical mirror 15 Straight mirror 16 Projection surface 17 Filter 18 Dodging element 19 Support base 111 End electrode 121 First focus 122 Second focus 123 Opening 141 Column mirror unit 142 Light blocking material 1411 First lens unit 1412 Second lens unit 154594.doc - 11 - M412365 D Maximum width L of the lenticular lens
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