CN113467064B - Ultraviolet irradiation device for solar simulator - Google Patents

Ultraviolet irradiation device for solar simulator Download PDF

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CN113467064B
CN113467064B CN202110799730.2A CN202110799730A CN113467064B CN 113467064 B CN113467064 B CN 113467064B CN 202110799730 A CN202110799730 A CN 202110799730A CN 113467064 B CN113467064 B CN 113467064B
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focal point
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李宇
于强
刘宠
张永泰
徐博文
王晶虎
姜海富
郑慧奇
赵越阳
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Beijing Institute of Spacecraft Environment Engineering
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B19/00Condensers, e.g. light collectors or similar non-imaging optics
    • G02B19/0004Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed
    • G02B19/0019Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed having reflective surfaces only (e.g. louvre systems, systems with multiple planar reflectors)
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B19/00Condensers, e.g. light collectors or similar non-imaging optics
    • G02B19/0033Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
    • G02B19/0038Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with ambient light
    • G02B19/0042Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with ambient light for use with direct solar radiation
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B19/00Condensers, e.g. light collectors or similar non-imaging optics
    • G02B19/0033Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
    • G02B19/0095Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with ultraviolet radiation
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
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Abstract

本申请公开了一种用于太阳模拟器的紫外辐照装置。包括:聚光镜本体,其具有位于中心的平面非反射区和与所述平面非反射区边沿连接的环状椭球面反射区;本申请具体地设计聚光镜本体,其具有位于中心的平面非反射区与与平面非反射区边沿连接的环状椭球面反射区,通过在环状椭球面反射区内壁上沿平面非反射区法线方向依次交替设置第一环区与第二环区,并且二者具备相同的第一焦点,光源自第一焦点发射光线,光线经第一环区反射汇聚至第二焦点,经第二环区反射汇聚至第三焦点,使得光线能量均匀分布在两个焦点,使得反射后的聚焦光斑均匀化,改善聚焦光斑分布方式。

Figure 202110799730

The application discloses an ultraviolet irradiation device for a solar simulator. Comprising: a condenser body, which has a plane non-reflection area at the center and an annular ellipsoid reflection area connected to the edge of the plane non-reflection area; the application specifically designs the condenser body, which has a plane non-reflection area at the center and For the annular ellipsoid reflective area connected to the edge of the plane non-reflective area, the first ring area and the second ring area are arranged alternately on the inner wall of the annular ellipsoid reflective area along the normal direction of the plane non-reflective area, and both have The same first focus, the light source emits light from the first focus, the light is reflected by the first ring area and converged to the second focus, and then reflected by the second ring area and converged to the third focus, so that the light energy is evenly distributed in the two focuses, so that The reflected focused spot is homogenized and the distribution of the focused spot is improved.

Figure 202110799730

Description

一种用于太阳模拟器的紫外辐照装置An ultraviolet irradiation device for solar simulator

技术领域technical field

本公开一般涉及航天器紫外辐照试验技术领域,具体涉及一种用于太阳模拟器的紫外辐照装置。The present disclosure generally relates to the technical field of spacecraft ultraviolet irradiation test, and in particular relates to an ultraviolet irradiation device for a solar simulator.

背景技术Background technique

在航天领域中,为保证航天器能够在空间环境中正常工作,需要在发射前进行一系列空间环境模拟试验。其中,紫外辐照试验是关键试验项目之一。在真空环境中,没有地球大气层的保护,航天器长期暴露在紫外辐照条件下,很多部件可能会产生损坏、形变和老化等问题,会对航天器的运行产生影响。为准确模拟出空间紫外辐照环境,需要相应的模拟设备,即紫外辐照源。In the aerospace field, in order to ensure that the spacecraft can work normally in the space environment, it is necessary to conduct a series of space environment simulation tests before launch. Among them, ultraviolet radiation test is one of the key test items. In a vacuum environment, without the protection of the earth's atmosphere, the spacecraft is exposed to ultraviolet radiation for a long time, and many components may be damaged, deformed, and aging, which will affect the operation of the spacecraft. In order to accurately simulate the space ultraviolet radiation environment, corresponding simulation equipment, that is, the ultraviolet radiation source, is needed.

目前,广泛应用的积分棒式紫外辐照源,通常通过反射式光路,使用椭球面聚光镜,将光源放在反射面所在椭球面的其中一个焦点上,光源发出的光经过反射后会聚到另一个焦点上,同时将积分棒一端端面中心放置于另一焦点处,使会聚光线经积分棒均匀传递到另一端面,随后经过光学成像系统,最终发射出符合紫外辐照源要求的光线。为加速老化实验,紫外辐照源通常要提供数倍太阳常数的照射,并且成像镜组通常要成一个放大多倍的实像,使得积分棒处的能量密度更是高出许多倍。因此,采用椭球聚光镜,积分棒入射端中心又是所有能量会聚的焦点,能量过于集中,导致积分棒端面很容易受到损伤。在实际使用中,微小的灰尘或瑕疵都会使积分棒端面被聚焦光线损坏,影响光线传输效果,降低设备寿命。因此,我们提出一种用于太阳模拟器的紫外辐照装置,用以解决上述的聚焦光斑分布集中,积分棒端面中心区承受能量密度极大,导致积分棒端面损伤的可能性大大增加,若端面表面存在细微颗粒干扰,积分棒端面极易被能量烧化、入侵,并且后续的紫外辐照源输出功率降低,性能迅速下降的问题。At present, the widely used integrating rod type ultraviolet radiation source usually uses an ellipsoidal condenser through a reflective optical path, and places the light source on one of the focal points of the ellipsoidal surface where the reflecting surface is located. At the focal point, place the center of one end face of the integrating rod at the other focal point at the same time, so that the converging light is uniformly transmitted to the other end face through the integrating rod, and then passes through the optical imaging system to finally emit light that meets the requirements of the ultraviolet radiation source. In order to accelerate the aging experiment, the ultraviolet radiation source usually provides irradiation several times the solar constant, and the imaging mirror group usually forms a multiple-magnified real image, so that the energy density at the integrating rod is many times higher. Therefore, using an ellipsoidal condenser, the center of the incident end of the integrating rod is the focal point where all the energy converges. The energy is too concentrated, which makes the end face of the integrating rod easily damaged. In actual use, tiny dust or flaws will cause the end face of the integrating rod to be damaged by the focused light, which will affect the light transmission effect and reduce the life of the device. Therefore, we propose an ultraviolet irradiation device for solar simulators to solve the above-mentioned concentrated spot distribution. The central area of the end face of the integrating rod bears a huge energy density, which greatly increases the possibility of damage to the end face of the integrating rod. There is fine particle interference on the surface of the end face, and the end face of the integrating rod is easily burnt and invaded by energy, and the output power of the subsequent ultraviolet radiation source is reduced, and the performance is rapidly degraded.

发明内容Contents of the invention

鉴于现有技术中的上述缺陷或不足,期望提供一种改善聚焦光斑分布方式,降低积分棒入射端面损伤概率,提升太阳模拟器系统的稳定性与寿命,结构简单且易于实现的用于太阳模拟器的紫外辐照装置。In view of the above-mentioned defects or deficiencies in the prior art, it is expected to provide a way to improve the distribution of focused light spots, reduce the probability of damage to the incident end face of the integrating rod, improve the stability and life of the solar simulator system, and be used for solar simulation with a simple structure and easy implementation. Ultraviolet irradiation device of the device.

第一方面,本申请提供一种聚光镜,包括:In a first aspect, the application provides a condenser, comprising:

聚光镜本体,其具有位于中心的平面非反射区和与所述平面非反射区边沿连接的环状椭球面反射区;Condenser body, which has a flat non-reflective area located in the center and an annular ellipsoid reflective area connected to the edge of the flat non-reflective area;

所述环状椭球面反射区内壁上沿所述平面非反射区的法线方向依次交替设有具备第一曲率半径的第一环区和具备第二曲率半径的第二环区;The inner wall of the annular ellipsoid reflective area is alternately provided with a first annular area with a first curvature radius and a second annular area with a second curvature radius along the normal direction of the plane non-reflective area;

所述第一环区与所述第二环区具备相同的第一焦点;The first annular area and the second annular area have the same first focal point;

光源自所述第一焦点发射的光线经过所述第一环区的反射汇聚至第二焦点处,且其经过所述第二环区的反射汇聚至第三焦点处。The light emitted by the light source from the first focal point converges to the second focal point after being reflected by the first ring area, and converges to the third focal point after being reflected by the second ring area.

根据本申请实施例提供的技术方案,所述第一焦点、所述第二焦点和所述第三焦点均位于所述平面非反射区的法线方向上。According to the technical solution provided by the embodiment of the present application, the first focal point, the second focal point and the third focal point are all located in the normal direction of the planar non-reflective area.

根据本申请实施例提供的技术方案,所述环状椭球面反射区靠近所述平面非反射区一侧的直径为66mm,且其远离所述平面非反射区一侧的直径为250mm。According to the technical solution provided in the embodiment of the present application, the diameter of the ring-shaped ellipsoid reflective area near the flat non-reflective area is 66 mm, and the diameter of the side away from the flat non-reflective area is 250 mm.

根据本申请实施例提供的技术方案,所述第一环区的曲率半径为87.2mm,且所述第二环区的曲率半径为87.8mm。According to the technical solution provided in the embodiment of the present application, the radius of curvature of the first ring area is 87.2 mm, and the radius of curvature of the second ring area is 87.8 mm.

根据本申请实施例提供的技术方案,所述第二焦点处的光线能量与所述第三焦点处的光线能量相等,且二者之和等于所述光源发射的光线总能量。According to the technical solution provided by the embodiment of the present application, the energy of the light at the second focal point is equal to the energy of the light at the third focal point, and the sum of the two is equal to the total energy of the light emitted by the light source.

第二方面,本申请提供一种用于太阳模拟器的紫外辐照装置,包括:In a second aspect, the application provides an ultraviolet irradiation device for a solar simulator, comprising:

上述的一种聚光镜;Above-mentioned a kind of condenser;

光源装置,其设置在所述第一焦点处;a light source device disposed at the first focal point;

在所述光源装置发射光线时,光线经所述第一环区反射汇聚至所述第二焦点处,且其经所述第二环区反射汇聚至所述第三焦点处;所述第二焦点与所述第三焦点相邻设置,且所述第二焦点相对靠近所述第一焦点;When the light source device emits light, the light is reflected by the first ring area and converged to the second focus, and it is reflected by the second ring area and converged to the third focus; the second The focal point is adjacent to the third focal point, and the second focal point is relatively close to the first focal point;

积分棒,其入射端面位于所述第二焦点与所述第三焦点连线的中线处,且所述入射端面与所述平面非反射区的法线垂直设置。Integrating rods, the incident end surface of which is located at the midline of the line connecting the second focal point and the third focal point, and the incident end surface is perpendicular to the normal line of the planar non-reflective area.

根据本申请实施例提供的技术方案,所述光源装置为球形汞氙灯。According to the technical solution provided by the embodiment of the present application, the light source device is a spherical mercury-xenon lamp.

综上所述,本技术方案具体地公开了一种聚光镜的具体结构。本申请具体地设计聚光镜本体,其具有位于中心的平面非反射区与与平面非反射区边沿连接的环状椭球面反射区,通过在环状椭球面反射区内壁上沿平面非反射区法线方向依次交替设置第一环区与第二环区,并且二者具备相同的第一焦点,光源自第一焦点发射光线,光线经第一环区反射汇聚至第二焦点,经第二环区反射汇聚至第三焦点,使得光线能量均匀分布在两个焦点,使得反射后的聚焦光斑均匀化,改善聚焦光斑分布方式。To sum up, the technical solution specifically discloses a specific structure of a condenser lens. The application specifically designs the condenser body, which has a plane non-reflective area located in the center and an annular ellipsoid reflective area connected to the edge of the plane non-reflective area. The direction alternately sets the first ring area and the second ring area, and both have the same first focus, the light source emits light from the first focus, the light is reflected by the first ring area and converges to the second focus, and passes through the second ring area The reflection converges to the third focal point, so that the light energy is evenly distributed in the two focal points, so that the reflected focused spot is uniform, and the distribution mode of the focused spot is improved.

附图说明Description of drawings

通过阅读参照以下附图所作的对非限制性实施例所作的详细描述,本申请的其它特征、目的和优点将会变得更明显:Other characteristics, objects and advantages of the present application will become more apparent by reading the detailed description of non-limiting embodiments made with reference to the following drawings:

图1为传统太阳模拟器中积分棒入射端面聚焦光斑功率密度分布示意图。Figure 1 is a schematic diagram of the power density distribution of the focused spot on the incident end face of the integrating rod in a traditional solar simulator.

图2为一种聚光镜及用于太阳模拟器的紫外辐照装置的结构示意图。Fig. 2 is a structural schematic diagram of a condenser and an ultraviolet irradiation device used in a solar simulator.

图3为本紫外辐照装置中积分棒入射端面聚焦光斑功率密度分布示意图。Fig. 3 is a schematic diagram of the power density distribution of the focused spot on the incident end face of the integrating rod in the ultraviolet irradiation device.

图4为传统太阳模拟器中积分棒出射端面光斑功率密度分布曲线示意图。Fig. 4 is a schematic diagram of the power density distribution curve of the light spot on the exit end face of the integrating rod in the traditional solar simulator.

图5为本紫外辐照装置中积分棒出射端面光斑功率密度分布曲线示意图。Fig. 5 is a schematic diagram of the power density distribution curve of the light spot on the exit end surface of the integrating rod in the ultraviolet irradiation device.

图中标号:1、聚光镜本体;2、光源装置;3、积分棒;4、第一环区;5、第二环区;6、第二焦点;7、第三焦点;8、入射端面。Symbols in the figure: 1. condenser body; 2. light source device; 3. integrating rod; 4. first ring area; 5. second ring area; 6. second focus; 7. third focus; 8. incident end face.

具体实施方式Detailed ways

下面结合附图和实施例对本申请作进一步的详细说明。可以理解的是,此处所描述的具体实施例仅仅用于解释相关发明,而非对该发明的限定。另外还需要说明的是,为了便于描述,附图中仅示出了与发明相关的部分。The application will be further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described here are only used to explain related inventions, rather than to limit the invention. It should also be noted that, for ease of description, only parts related to the invention are shown in the drawings.

需要说明的是,在不冲突的情况下,本申请中的实施例及实施例中的特征可以相互组合。下面将参考附图并结合实施例来详细说明本申请。It should be noted that, in the case of no conflict, the embodiments in the present application and the features in the embodiments can be combined with each other. The present application will be described in detail below with reference to the accompanying drawings and embodiments.

实施例一Embodiment one

请参考图2所示的本申请提供的一种聚光镜的结构示意图,包括:Please refer to the structural representation of a condenser provided by the application shown in Figure 2, including:

聚光镜本体1,其具有位于中心的平面非反射区和与所述平面非反射区边沿连接的环状椭球面反射区;Condenser body 1, which has a flat non-reflective area located at the center and an annular ellipsoid reflective area connected to the edge of the flat non-reflective area;

所述环状椭球面反射区内壁上沿所述平面非反射区的法线方向依次交替设有具备第一曲率半径的第一环区4和具备第二曲率半径的第二环区5;The inner wall of the annular ellipsoid reflective area is alternately provided with a first ring area 4 with a first radius of curvature and a second ring area 5 with a second radius of curvature along the normal direction of the planar non-reflective area;

所述第一环区4与所述第二环区5具备相同的第一焦点;The first ring area 4 and the second ring area 5 have the same first focal point;

光源自所述第一焦点发射的光线经过所述第一环区4的反射汇聚至第二焦点6处,且其经过所述第二环区5的反射汇聚至第三焦点7处。The light emitted by the light source from the first focal point converges to the second focal point 6 after being reflected by the first ring region 4 , and converges to the third focal point 7 after being reflected by the second ring region 5 .

在本实施例中,如图2所示,聚光镜本体1,其具有位于中心的平面非反射区与与平面非反射区边沿连接的环状椭球面反射区;平面非反射区对光线无反射作用;第一环区4与第二环区5,依次交替设置在环状椭球面反射区内壁上沿平面非反射区的法线方向,用于反射光源发出的光线;In the present embodiment, as shown in Figure 2, the condenser body 1 has a plane non-reflective area positioned at the center and an annular ellipsoid reflective area connected to the edge of the plane non-reflective area; the plane non-reflective area has no reflective effect on light ; The first ring area 4 and the second ring area 5 are arranged alternately on the inner wall of the annular ellipsoid reflective area along the normal direction of the plane non-reflective area, for reflecting the light emitted by the light source;

此处,第一环区4与第二环区5具备相同的第一焦点,即相当于传统聚光镜中光源放置的焦点,光源可自第一焦点发射光线,光线经第一环区4的反射汇聚至第二焦点6处,光线经第二环区5的反射汇聚至第三焦点7处,将光线分别汇聚在两个焦点处,并且,第二焦点6处的光线能量与第三焦点7处的光线能量相等,且二者之和等于光源装置2发射的光线总能量,使得反射后的聚焦光斑均匀化。Here, the first ring area 4 and the second ring area 5 have the same first focal point, which is equivalent to the focus placed by the light source in a conventional condenser. The light source can emit light from the first focus, and the light is reflected by the first ring area 4 Converging to the second focal point 6, the light is converged to the third focal point 7 through the reflection of the second ring area 5, and the light is respectively converged at the two focal points, and the energy of the light at the second focal point 6 is the same as that of the third focal point 7 The energy of the light at is equal, and the sum of the two is equal to the total energy of the light emitted by the light source device 2, so that the reflected focused light spot is uniform.

并且,第一焦点、第二焦点6和第三焦点7均位于平面非反射区的法线方向上;And, the first focal point, the second focal point 6 and the third focal point 7 are all located in the normal direction of the plane non-reflective area;

进一步地,对每个环区进行打磨,使得相同环区具备统一的弯曲程度,即每个第一环区4均具有相同的第一曲率半径;每个第二环区5均具有相同的第二曲率半径;使得相同曲率半径的环区在反射光线时,可将光线汇聚至相应的同一焦点处。Further, each ring area is polished so that the same ring area has a uniform degree of curvature, that is, each first ring area 4 has the same first radius of curvature; each second ring area 5 has the same first radius of curvature; Two curvature radii; so that when the ring areas with the same curvature radius reflect the light, the light can be converged to the corresponding same focal point.

进一步地,第一环区4与第二环区5的排布方式,例如,如图2所示的将第一环区4置于相对靠近平面非反射区的位置,第二环区5则与此第一环区相邻设置,二者在平面非反射区的法线方向依次交替设置。Further, the arrangement of the first ring area 4 and the second ring area 5, for example, as shown in FIG. Adjacent to the first ring area, the two are arranged alternately in the normal direction of the planar non-reflective area.

实施例二Embodiment two

请参考图2所示的本申请提供的一种用于太阳模拟器的紫外辐照装置的结构示意图,包括:Please refer to the structural representation of a kind of ultraviolet radiation device for solar simulator provided by the present application shown in Fig. 2, including:

实施例一中的一种聚光镜;A kind of condenser lens among the embodiment one;

光源装置2,其设置在所述第一焦点处;a light source device 2, which is arranged at the first focal point;

在所述光源装置2发射光线时,光线经所述第一环区4反射汇聚至所述第二焦点6处,且其经所述第二环区5反射汇聚至所述第三焦点7处;所述第二焦点6与所述第三焦点7相邻设置,且所述第二焦点6相对靠近所述第一焦点;When the light source device 2 emits light, the light is reflected by the first ring area 4 and converged to the second focus 6 , and it is reflected by the second ring area 5 and converged to the third focus 7 ; The second focus 6 is adjacent to the third focus 7, and the second focus 6 is relatively close to the first focus;

积分棒3,其入射端面8位于所述第二焦点6与所述第三焦点7连线的中线处,且所述入射端面8与所述平面非反射区的法线垂直设置。The incident end surface 8 of the integrator rod 3 is located at the midline of the line connecting the second focal point 6 and the third focal point 7, and the incident end surface 8 is perpendicular to the normal of the plane non-reflective area.

在本实施例中,以传统的椭球面聚光镜为例,将光源放在反射面所在椭球面的其中一个焦点上,光源发出的光经过反射后会聚到另一个焦点上,同时将积分棒一端端面中心放置于另一焦点处,使会聚光线经积分棒均匀传递到其另一端面,随后经过光学成像系统,最终发射出符合紫外辐照源要求的光线,其中,椭球面聚光镜的参数,如表1所示,其口径为250mm,其底孔直径为66mm,其曲率半径为87.5mm,其圆锥曲面系数为-0.5625;In this embodiment, taking the traditional ellipsoidal condenser as an example, the light source is placed on one of the focal points of the ellipsoidal surface where the reflecting surface is located, and the light emitted by the light source converges to the other focal point after being reflected. The center is placed at another focal point, so that the converging light is uniformly transmitted to the other end surface through the integrating rod, and then passes through the optical imaging system, and finally emits light that meets the requirements of the ultraviolet radiation source. Among them, the parameters of the ellipsoidal condenser are as shown in the table As shown in 1, its caliber is 250mm, its bottom hole diameter is 66mm, its curvature radius is 87.5mm, and its conical surface coefficient is -0.5625;

表1传统聚光镜参数Table 1 Traditional condenser parameters

Figure GDA0004100663630000051
Figure GDA0004100663630000051

如图1所示,为利用传统聚光镜传输光线时,传统太阳模拟器中积分棒入射端面聚焦光斑功率密度分布情况,可以看出光源经单一焦点的聚光镜反射汇聚后,聚焦光斑分布集中,光斑功率密度峰值较大。As shown in Figure 1, the distribution of the power density of the focused spot on the incident end face of the integrating rod in the traditional solar simulator is shown when the light is transmitted by the traditional condenser. The density peak is larger.

基于传统的聚光镜,重新设计聚光镜反射面的面形,保留原有光线传输功能的基础上,利用多重结构代替传统的单一结构;Based on the traditional condenser, the shape of the reflective surface of the condenser is redesigned, and on the basis of retaining the original light transmission function, multiple structures are used to replace the traditional single structure;

如图2所示,本实施例具有实施例一所述的一种聚光镜;将光源装置2,设置在第一焦点处,作为发光源;此处,光源装置2的类型,例如为球形汞氙灯;As shown in Figure 2, the present embodiment has a kind of converging mirror described in Embodiment 1; the light source device 2 is arranged at the first focal point as a light source; here, the type of the light source device 2 is, for example, a spherical mercury-xenon lamp ;

积分棒3,其入射端面8设置在第二焦点6与第三焦点7连线的中线处,且其与平面非反射区的法线垂直设置,经第一环区4与第二环区5反射后的光线由入射端面8进入积分棒3内,经积分棒3进行多次反射,最终在其出光端面形成均匀光源;Integrator rod 3, its incident end surface 8 is set at the midline of the line connecting the second focal point 6 and the third focal point 7, and it is set perpendicular to the normal of the plane non-reflective area, passing through the first ring area 4 and the second ring area 5 The reflected light enters the integrating rod 3 from the incident end face 8, and is reflected multiple times by the integrating rod 3, finally forming a uniform light source on its light emitting end face;

具体地,如表2所示,本实施例的聚光镜的口径与底孔直径的选取与传统聚光镜的参数一致,第一曲率半径选取为87.2mm,第二曲率半径选取为87.8mm;Specifically, as shown in Table 2, the selection of the diameter of the condenser and the diameter of the bottom hole of the present embodiment are consistent with the parameters of the traditional condenser, the first radius of curvature is selected as 87.2mm, and the second radius of curvature is selected as 87.8mm;

表2本实施例聚光镜参数Table 2 Condenser parameters of this embodiment

Figure GDA0004100663630000061
Figure GDA0004100663630000061

利用球形汞氙灯发射发散光线,光线经第一环区4反射汇聚至第二焦点6处,且其经第二环区5反射汇聚至第三焦点7处,此时如图2所示,第二焦点6与第三焦点7相邻设置,且第二焦点6相对靠近第一焦点;两个焦点处的光线由入射端面8进入积分棒3,利用积分棒3对反射后的光线进行多次反射,最终在其出光端面形成均匀光源;均匀光源再经成像镜组成像至指定距离的照明面上,最终形成符合紫外辐照均匀光斑。Utilize the spherical mercury-xenon lamp to emit divergent light, the light is reflected by the first ring area 4 and converges to the second focus 6, and it is reflected by the second ring area 5 and converges to the third focus 7, as shown in Figure 2 at this time, the first The second focal point 6 is adjacent to the third focal point 7, and the second focal point 6 is relatively close to the first focal point; the light at the two focal points enters the integrating rod 3 from the incident end face 8, and the reflected light is processed by the integrating rod 3 for many times Reflection, and finally form a uniform light source on its light-emitting end surface; the uniform light source is then imaged to the lighting surface at a specified distance through the imaging mirror, and finally forms a uniform light spot that conforms to ultraviolet radiation.

并且,如图3所示,本方案中积分棒3的入射端面8的聚焦光斑分布更加均匀,峰值功率密度也更低,在能量传输效率不变的情况下,使得聚焦光斑均匀分布,以避免积分棒3受损。Moreover, as shown in Figure 3, in this solution, the distribution of the focused light spots on the incident end face 8 of the integrator rod 3 is more uniform, and the peak power density is also lower. Under the condition that the energy transmission efficiency remains unchanged, the focused light spots are evenly distributed to avoid Point stick 3 damaged.

如图4、图5所示,使用传统聚光镜与使用本方案的聚光镜分别模拟紫外辐照环境时,两种模拟试验中的积分棒3的出射端面的出射功率密度分布基本相同,可以看出,本方案重新设计的聚光镜以及紫外辐照装置可以实现原有光线传导,因此,本聚光镜以及紫外辐照装置在改善光线传输过程,均匀分布聚焦光斑,降低积分棒受损率的同时保证了能量传输效率。As shown in Fig. 4 and Fig. 5, when using the traditional condenser and the condenser of this solution to simulate the ultraviolet radiation environment respectively, the output power density distribution of the exit end face of the integrating rod 3 in the two simulation tests is basically the same. It can be seen that, The redesigned condenser and ultraviolet irradiation device of this scheme can realize the original light transmission. Therefore, the condenser and ultraviolet irradiation device can improve the light transmission process, evenly distribute the focused spot, and reduce the damage rate of the integrating rod while ensuring energy transmission. efficiency.

进一步地,如表3所示,本方案聚光镜相较于传统聚光镜,其积分棒入射端面的光斑峰值功率密度下降约40%;光斑直径变大,50%功率密度光斑直径增加约56%,达到了很好的匀化效果,因此,此种聚光镜结构以及用于太阳模拟器的紫外辐照装置,可降低积分棒损伤概率,有效提升系统整体稳定性。Further, as shown in Table 3, compared with the traditional condenser, the peak power density of the spot on the incident end face of the integrating rod of this scheme decreases by about 40%; the spot diameter becomes larger, and the spot diameter increases by about 56% at 50% power density, reaching Therefore, this kind of condenser lens structure and the ultraviolet irradiation device used in the solar simulator can reduce the damage probability of the integrating rod and effectively improve the overall stability of the system.

表3传统椭球面聚光镜与本方案聚光镜聚焦光斑的对比Table 3 Comparison of the focus spot of the traditional ellipsoidal condenser and the condenser of this solution

Figure GDA0004100663630000071
Figure GDA0004100663630000071

以上描述仅为本申请的较佳实施例以及对所运用技术原理的说明。本领域技术人员应当理解,本申请中所涉及的发明范围,并不限于上述技术特征的特定组合而成的技术方案,同时也应涵盖在不脱离所述发明构思的情况下,由上述技术特征或其等同特征进行任意组合而形成的其它技术方案。例如上述特征与本申请中公开的(但不限于)具有类似功能的技术特征进行互相替换而形成的技术方案。The above description is only a preferred embodiment of the present application and an illustration of the applied technical principle. Those skilled in the art should understand that the scope of the invention involved in this application is not limited to the technical solution formed by the specific combination of the above-mentioned technical features, but should also cover the technical solution formed by the above-mentioned technical features without departing from the inventive concept. Other technical solutions formed by any combination of or equivalent features thereof. For example, a technical solution formed by replacing the above-mentioned features with technical features with similar functions disclosed in this application (but not limited to).

Claims (5)

1. An ultraviolet irradiation apparatus for a solar simulator, comprising:
a condenser lens, comprising:
a condenser body (1) having a planar non-reflection region at the center and an annular ellipsoidal reflection region connected to the edge of the planar non-reflection region;
a first annular region (4) with a first curvature radius and a second annular region (5) with a second curvature radius are sequentially and alternately arranged on the inner wall of the annular ellipsoidal reflecting region along the normal direction of the planar non-reflecting region;
the first annular region (4) and the second annular region (5) have the same first focus;
light emitted from the first focal point is converged at a second focal point (6) through reflection of the first annular region (4), and is converged at a third focal point (7) through reflection of the second annular region (5);
the light energy at the second focus (6) is equal to the light energy at the third focus (7), and the sum of the two is equal to the total light energy emitted by the light source;
a light source device (2) disposed at the first focal point;
when the light source device (2) emits light, the light is reflected and converged to the second focus (6) through the first annular region (4), and is reflected and converged to the third focus (7) through the second annular region (5); the second focal point (6) is arranged adjacent to the third focal point (7), and the second focal point (6) is relatively close to the first focal point;
and the incidence end surface (8) of the integrating rod (3) is positioned at the central line of the connecting line of the second focus (6) and the third focus (7), and the incidence end surface (8) is perpendicular to the normal line of the plane non-reflection area.
2. An ultraviolet irradiation device for a solar simulator according to claim 1, characterized in that the first focus, the second focus (6) and the third focus (7) are all located in the normal direction of the planar non-reflective area.
3. An ultraviolet irradiation device for a solar simulator as claimed in claim 1, wherein the diameter of the side of the annular ellipsoidal reflective region close to the planar non-reflective region is 66mm, and the diameter of the side thereof remote from the planar non-reflective region is 250mm.
4. A uv irradiation device for a solar simulator according to claim 3, wherein the first radius of curvature is 87.2mm and the second radius of curvature is 87.8mm.
5. An ultraviolet irradiation device for a solar simulator according to claim 1, characterized in that the light source device (2) is a spherical mercury xenon lamp.
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