91porn自拍视频,懂色av色香蕉一区二区蜜桃,yw永不失联国际,亚洲经典三级,一区二区麻豆av,最近最新更新2019中文字幕在线,日本xxxx色视频在线观看安装,国产精品欧美一区二区久久久
                撥號18861759551

                你的位置:首頁 > 技術文章 > 使用塑料混合非球面透鏡的優點

                技術文章

                使用塑料混合非球面透鏡的優點

                技術文章

                Advantages of Using Plastic Hybrid Aspheric Lenses

                TECHSPEC® Plastic Hybrid Aspheric Lenses are low cost optical components that lack both spherical and chromatic aberrations. These aspheric lenses provide optical designers with unique, single element solutions for achieving diffraction-limited focusing performance at high numerical apertures with broadband light sources. These aspheric lenses consist of a diffractive surface that has been added to a molded aspheric lens. The aspheric lens eliminates all spherical aberration, while the diffractive surface has a net effect of introducing negative dispersion – when properly tuned to the refractive index and wavelength design of the lens, chromatic aberration is eliminated as well.

                 

                Spherical and Chromatic Aberrations

                There are two major forms of axial optical aberrations inherent in common optical lenses: spherical aberration and chromatic aberration. Spherical aberration is an inherent characteristic of any lens whose surface is a section of a sphere. Light originating from the same object point comes to a focus at slightly different points (P and P’), depending on whether the rays pass through the center of the lens or the periphery (Figure 1).

                Figure 1: Spherical Aberration in a Single Positive Lens

                 

                igure 2.1: Transverse Chromatic Aberration of a Single Positive Lens

                 

                Figure 2.2: Longitudinal Chromatic Aberration of a Single Positive Lens

                 

                Chromatic aberration results from material dispersion. Because different colors of light refract by different amounts, an image point formed by light of one color does not coincide with the corresponding image point formed by light of a different color (Figures 2.1 and 2.2).

                 

                Important Equations

                Spherical aberration is typically eliminated by substituting an aspherical surface for the more common spherical surface. The surface profile (sag) is given by Equation 1:

                Where

                Z = sag of surface parallel to the optical axis

                s = radial distance from the optical axis

                C = curvature, inverse of radius

                k = conic constant

                A4, A6, A8 = 4th, 6th, 8th… order aspheric terms

                 

                However, this does not correct chromatic aberration. Therefore, for a monochromatic light source, the aspheric surface will provide diffraction limited focusing at a single wavelength, but will suffer a large spot size over a broader wavelength.

                 

                A diffractive surface will correct the spherical aberration, as shown in Equation 2.

                Where
                Y = radial position from center of lens (for instance, if 0 is the center of the lens, 12.5mm will be the edge of a 25mm diameter lens, etc.)
                nd = index of refraction of the material at 587.6nm
                Step Height = λ/nd-1
                λ = the wavelength of interest

                By combining the two features onto a single element, a component that eliminates both chromatic and spherical aberration is created. That surface is described simply as the sum of the Zasph and Zdiff coefficients.

                For tips on modeling diffractives in Zemax and Code V, visit the Optics Realm blog.

                 

                Customer Benefits

                Optical designers often need to focus light at very short distances, or collect and collimate as much light as possible from very divergent light sources. Basic optical principles dictate that a high numerical aperture optical lens is required for either of these scenarios. A high numerical aperture optical lens will typically have a focal length equal to or shorter than the clear aperture of the optical system, allowing the designer to maintain as compact of an optical train as possible.

                For example, an optical designer has multiple options for achieving a focal length that is equal to his clear aperture (a scenario known as an F/1 lens, or a lens with a numerical aperture of 0.50). The simplest option is to use a standard plano-convex lens, available from a number of distributors. Spot diagram, chromatic focal shift graph, polychromatic diffraction MTF, and transverse ray fan plot for the wavelength range of 486 - 656nm are provided for #45-097 25mm Diameter x 25mm FL PCX lens.

                 

                PCX Lens

                Figure 3.1: Spot Diagram for #45-097 25mm Dia. x 25mm FL PCX Lens

                Figure 3.2: Chromatic Focal Shift Graph for #45-097 25mm Dia. x 25mm FL PCX Lens

                Figure 3.3: Polychromatic Diffraction MTF Graph for #45-097 25mm Dia. x 25mm FL PCX Lens

                Figure 3.4: Transverse Ray Fan Plot for #45-097 25mm Dia. x 25mm FL PCX Lens

                 

                For improved performance, the optical designer could consider an achromatic lens of the same form factor, for example #65-553 25mm Diameter x 25mm Focal Length Achromatic Lens. Again, the same characteristics are shown over the same wavelength range. A 74% decrease in spot size with a 73% decrease in chromatic focal shift can be seen, yielding an MTF of 13 lp/mm at 40% contrast, a substantial gain versus the aforementioned singlet lens.

                Figure 4.1: pot Diagram for #65-553 25mm Dia. x 25mm FL Achromatic Lens

                Figure 4.2: Chromatic Focal Shift Graph for #65-553 25mm Dia. x 25mm FL Achromatic Lens

                Figure 4.3: Polychromatic Diffraction MTF Graph for #65-553 25mm Dia. x 25mm FL Achromatic Lens

                Figure 4.4: Transverse Ray Fan Plot for #65-553 25mm Dia. x 25mm FL Achromatic Lens

                For maximum performance, the optical designer should choose a plastic hybrid aspheric lens. In this scenario, the exact same form factor and wavelength range are used, this time with #65-992 25mm Diameter x 25mm FL Hybrid Aspheric Lens. As shown, this lens provides diffraction limited focusing performance, yielding the optimum performance for the designer.

                 

                Plastic Hybrid Lens

                Figure 5.1: Spot Diagram for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

                Figure 5.2: Chromatic Focal Shift Graph for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

                Figure 5.3: Polychromatic Diffraction MTF Graph for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

                Figure 5.4: Transverse Ray Fan Plot for #65-992 25mm Dia. x 25mm FL Hybrid Aspheric Lens

                Comparing the spot diagrams, chromatic focal shift graphs, polychromatic diffraction MTFs, and transverse ray fan plots of a plano-convex (PCX) lens, achromatic lens, and hybrid aspheric lens, it is easy to see the advantages of using plastic hybrid aspheric lenses for achieving diffraction-limited focusing performance at high numerical apertures with broadband light sources.

                 

                Selection Guide

                Edmund Optics® TECHSPEC® Plastic Aspheres and TECHSPEC® Plastic Hybrid Aspheres families are both manufactured utilizing Zeon Chemical’s Zeonex E48R material. Zeonex materials feature high transparency, low fluorescence, low birefrengence, low water absorption, and high heat and chemical resistance, making it a superior material vs. other commonly available plastics. Zeonex is a Cylco Olefin Polymer (COP) material.

                Plastic Materials Selection Guide

                Property

                Glass

                Zeonex E48R

                PMMA

                Polycarbonate

                Polystyrene

                Arton®

                Transmission

                Excellent

                Excellent

                Excellent

                Good

                Very Good

                Excellent

                Low Refractive Index

                Excellent

                Excellent

                Excellent

                Poor

                Poor

                Good

                Low Birefringence

                Excellent

                Excellent

                Excellent

                Poor

                Poor

                Excellent

                Low Water Absorption

                Excellent

                Excellent

                Poor

                Good

                Excellent

                Excellent

                Impact Resistance

                Poor

                Good

                Good

                Excellent

                Good

                Excellent

                Moldability

                Fair

                Excellent

                Good

                Excellent

                Excellent

                Good

                Heat Resistance

                Excellent

                Good

                Poor

                Good

                Poor

                Very Good

                Coating Adhesion

                Excellent

                Good

                Fair

                Fair

                Fair

                Good

                聯系我們

                地址:江蘇省江陰市人民東路1091號1017室 傳真:0510-68836817 Email:sales@rympo.com
                24小時在線客服,為您服務!

                版權所有 © 2026 江陰韻翔光電技術有限公司 備案號:蘇ICP備16003332號-1 技術支持:化工儀器網 管理登陸 GoogleSitemap

                在線咨詢
                QQ客服
                QQ:17041053
                電話咨詢
                0510-68836815
                關注微信
                主站蜘蛛池模板: 亚洲另类国产综合小说| 国产精品亚洲精品日韩已满十八小 | 亚洲色成人一区二区三区人人澡人人妻人人爽人人蜜桃麻豆 | 国内精品乱码卡一卡2卡麻豆| 曰本超级乱婬Av片免费| 男女免费观看在线爽爽爽视频| 亚洲国产精品人人做人人爱| 专干老肥熟女视频网站| 山东熟女啪啪哦哦叫| 一卡二卡三卡四卡视频区| 双乳奶水饱满少妇视频| 丰满高跟丝袜老熟女久久| 麻豆成人传媒一区二区| 国产精品福利无圣光一区二区| 人妻中文字幕无码系列| 日韩精品成人无码专区免费| 少妇愉情理伦片丰满丰满午夜| 亚洲欧洲日韩av在线观看| 欧美日本一区二区视频在线观看| 亚洲国产欧美在线成人aaaa| 中文字幕第一区| 东京热无码一区二区三区分类视频| 五月婷婷激情第四季| 少妇人妻偷人精品免费| 国产在线不卡精品网站| 国产精品亚洲а∨天堂2021| 无码人妻精品一区二区三区蜜桃| 无码国产成人午夜电影在线观看| 欧美精品一区二区三区在线| 亚洲第一极品精品无码久久| 国产免费又黄又爽又色毛| 四虎成人精品永久网站| 国产三级aⅴ在在线观看| 亚洲国产片一区二区三区| 2019最新久久久视频精品 | 国产精品美女被遭强扒开双腿 | 国产精品乱码人妻一区二区三区| 国产美女爽到喷出水来视频| 骚虎视频在线观看| 亚洲一区二区三午夜福利| 人人澡人人爽夜欢视频|