欧美肉大捧一进一出免费视频,亚洲乱码日产精品bd在线观看,无码人妻精品一区二区三区夜夜嗨,久久中文字幕人妻熟av女

撥號18861759551

你的位置:首頁 > 技術(shù)文章 > 如何測量您的成像系統(tǒng)中的景深

技術(shù)文章

如何測量您的成像系統(tǒng)中的景深

技術(shù)文章

Gauging Depth of Field in Your Imaging System

Over the years, we have answered countless questions regarding lens performance. Of those questions, none have been more difficult to define than requests for depth of field. The reason for this difficulty has more to do with the vagueness of the question than with the inability to provide a measured or calculated value. Consider for a moment what depth of field ls us. It is the distance by which an object may be shifted before an unacceptable blur is produced. For depth of field to be properly stated, it should contain not only the displacement of an image, but also a specific resolution. The depth of field specification is further complicated by a type of keystoning aberration that often occurs. This result can dramatically affect linear measurements and therefore render depth of field unusable. In this article we will take a closer look at depth of field calculations and compare them to physical measurements using the DOF 1-40 depth of field gauge. The gauge, as we will see later, offers a unique look at what depth of field really means and how we as system designers may wish to quantify this parameter. A simple geometric approximation for depth of field is shown in Figure 1.0. The linear blur (required resolution) Bp, Bm and Bf can be expressed in terms of angular blur by the following equation.

Figure 1

 

Using similar triangles, a relationship can now be made between angular blur and the focus point,

where λ is the aperture of the lens. Solving for δplus and δmin,

The derivation above is very specific to the intended resolution. However, many theoretical derivations of depth of field often assume the lens resolution to be nearly diffraction limited. The most popular of these derivations are based on microscope applications. A typical example for the total depth of field (dplus + dmin) is shown below.

Where λ is the wavelength and NA equals the numerical aperture of the lens.

In order to study depth of field we have put together a simple macro system consisting of a 25mm fixed focal length lens, 8mm spacer and Sony XC-75 monochrome CCD video camera. The system was chosen not for its performance but rather for its common real world implementation. Measurements were performed using the DOF 1-40 target. The target allows us to measure depth of field at either 1, 10, 20 or 40 lp/mm over a maximum depth of 50mm. The flat field resolution of this system is approximay 15 lp/mm at 0.3X primary magnification. For purposes of our experiment, a blur spot resolution of 0.1 mm or 10 lp/mm was chosen. Depth of field measurements were taken at three aperture settings corresponding to f/2, f/4, and f/8. An important point should be noted about aperture settings. The f-number shown on most fixed focal length lenses is calculated with the object at infinity. As a result, we have adjusted our NA and therefore our aperture values for a 95mm working distance.

The values below highlight a number of points to consider. In general our calculated and measured delta d are fairly close. However, the displacement of the image due to defocus aberrations was not predicted by our calculations. This type of displacement error could certainly be problematic if the system contained an auto iris. If we compare our measured results to the delta-theory, we notice a significant variation. As we mentioned earlier, this variation is due to a false assumption concerning system resolution.

Another property that should be noted in our DOF 1-40 observations is the non-uniform magnification seen through the depth of field range. This is a very common problem in most lenses and, as we stated earlier, can yield significant errors if measurements are made throughout the full depth of field range. Edmund Optics provides several ecentric options to correct for this type of error.

In the end, it is the total performance of an optical system that counts. As a full service supplier and manufacturer of optics, illumination, CCD cameras, monitors, mounting, and electronic imaging related products, Edmund Optics has the knowledge and resources to look at your application as a total system. In fact, innovative tools such as the DOF 1-40 have come about from our own in-house need to quantify system performance. So if you are looking for individual components that can be integrated into your system or starting from scratch, our engineers are ready to help.

聯(lián)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(wù)!

版權(quán)所有 © 2025 江陰韻翔光電技術(shù)有限公司 備案號:蘇ICP備16003332號-1 技術(shù)支持:化工儀器網(wǎng) 管理登陸 GoogleSitemap

在線咨詢
QQ客服
QQ:17041053
電話咨詢
0510-68836815
關(guān)注微信
被各种陌生人np调教灌尿| 亚洲人成人无码网www国产| 精品少妇爆乳无码av无码专区| 国产三级精品三级在线专区| 又硬又粗进去好爽a片潘金莲| 日产a一a区二区| 亚洲欧美日本韩国| 国产偷v国产偷v亚洲高清| 一本精品中文字幕在线| 日韩毛片无码永久免费看| 少妇被躁爽到高潮无码文| 亚洲精品国产suv一区88| 少妇的肉体aa片免费| 无码人妻丰满熟妇区五十路 | 国产女人18毛片水真多1| 无翼鸟少女漫画| 无码毛片aaa在线| 国产丝袜美女一区二区三区| 国内大量揄拍情侣在线视频99| 熟妇人妻中文字幕| 国产成人免费视频| 日韩精品av一区二区三区| 客厅玩朋友娇妻hd完整版视频| 《金悔瓶3》免费观看| 久久国产精品波多野结衣av| 教室停电h嗯啊好硬好湿| 饥渴老翁一晚要了我三次| 亚洲精品一区三区三区在线观看| 中文字幕| 国产精品久久久久久无码不卡| 欧洲美熟女乱又伦av影片| 中文字幕精品一区二区三区| 他揉捏她两乳不停呻吟| 色婷婷综合中文久久一本| 全彩调教本子h里番全彩无码| 久久人妻内射无码一区三区| 国产仑乱无码内谢| 国产精品日本一区二区不卡视频| 国产av无码专区亚洲a∨毛片| 国内大量揄拍情侣在线视频99 | 久久精品国产9久久综合|