A Practical Guide to Selecting the Right Lens for Your Machine Vision Camera Pete Kepf [email protected]
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About Raspberry Pi HQ Camera Lenses Created by Dylan Herrada
All About Raspberry Pi HQ Camera Lenses Created by Dylan Herrada Last updated on 2020-10-19 07:56:39 PM EDT Overview In this guide, I'll explain the 3 main lens options for a Raspberry Pi HQ Camera. I do have a few years of experience as a video engineer and I also have a decent amount of experience using cameras with relatively small sensors (mainly mirrorless cinema cameras like the BMPCC) so I am very aware of a lot of the advantages and challenges associated. That being said, I am by no means an expert, so apologies in advance if I get anything wrong. Parts Discussed Raspberry Pi High Quality HQ Camera $50.00 IN STOCK Add To Cart © Adafruit Industries https://learn.adafruit.com/raspberry-pi-hq-camera-lenses Page 3 of 13 16mm 10MP Telephoto Lens for Raspberry Pi HQ Camera OUT OF STOCK Out Of Stock 6mm 3MP Wide Angle Lens for Raspberry Pi HQ Camera OUT OF STOCK Out Of Stock Raspberry Pi 3 - Model B+ - 1.4GHz Cortex-A53 with 1GB RAM $35.00 IN STOCK Add To Cart Raspberry Pi Zero WH (Zero W with Headers) $14.00 IN STOCK Add To Cart © Adafruit Industries https://learn.adafruit.com/raspberry-pi-hq-camera-lenses Page 4 of 13 © Adafruit Industries https://learn.adafruit.com/raspberry-pi-hq-camera-lenses Page 5 of 13 Crop Factor What is crop factor? According to Wikipedia (https://adafru.it/MF0): In digital photography, the crop factor, format factor, or focal length multiplier of an image sensor format is the ratio of the dimensions of a camera's imaging area compared to a reference format; most often, this term is applied to digital cameras, relative to 35 mm film format as a reference. -
About Resolution
pco.knowledge base ABOUT RESOLUTION The resolution of an image sensor describes the total number of pixel which can be used to detect an image. From the standpoint of the image sensor it is sufficient to count the number and describe it usually as product of the horizontal number of pixel times the vertical number of pixel which give the total number of pixel, for example: 2 Image Sensor & Camera Starting with the image sensor in a camera system, then usually the so called modulation transfer func- Or take as an example tion (MTF) is used to describe the ability of the camera the sCMOS image sensor CIS2521: system to resolve fine structures. It is a variant of the optical transfer function1 (OTF) which mathematically 2560 describes how the system handles the optical infor- mation or the contrast of the scene and transfers it That is the usual information found in technical data onto the image sensor and then into a digital informa- sheets and camera advertisements, but the question tion in the computer. The resolution ability depends on arises on “what is the impact or benefit for a camera one side on the number and size of the pixel. user”? 1 Benefit For A Camera User It can be assumed that an image sensor or a camera system with an image sensor generally is applied to detect images, and therefore the question is about the influence of the resolution on the image quality. First, if the resolution is higher, more information is obtained, and larger data files are a consequence. -
High-Aperture Optical Microscopy Methods for Super-Resolution Deep Imaging and Quantitative Phase Imaging by Jeongmin Kim a Diss
High-Aperture Optical Microscopy Methods for Super-Resolution Deep Imaging and Quantitative Phase Imaging by Jeongmin Kim A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Engineering { Mechanical Engineering and the Designated Emphasis in Nanoscale Science and Engineering in the Graduate Division of the University of California, Berkeley Committee in charge: Professor Xiang Zhang, Chair Professor Liwei Lin Professor Laura Waller Summer 2016 High-Aperture Optical Microscopy Methods for Super-Resolution Deep Imaging and Quantitative Phase Imaging Copyright 2016 by Jeongmin Kim 1 Abstract High-Aperture Optical Microscopy Methods for Super-Resolution Deep Imaging and Quantitative Phase Imaging by Jeongmin Kim Doctor of Philosophy in Engineering { Mechanical Engineering and the Designated Emphasis in Nanoscale Science and Engineering University of California, Berkeley Professor Xiang Zhang, Chair Optical microscopy, thanks to the noninvasive nature of its measurement, takes a crucial role across science and engineering, and is particularly important in biological and medical fields. To meet ever increasing needs on its capability for advanced scientific research, even more diverse microscopic imaging techniques and their upgraded versions have been inten- sively developed over the past two decades. However, advanced microscopy development faces major challenges including super-resolution (beating the diffraction limit), imaging penetration depth, imaging speed, and label-free imaging. This dissertation aims to study high numerical aperture (NA) imaging methods proposed to tackle these imaging challenges. The dissertation first details advanced optical imaging theory needed to analyze the proposed high NA imaging methods. Starting from the classical scalar theory of optical diffraction and (partially coherent) image formation, the rigorous vectorial theory that han- dles the vector nature of light, i.e., polarization, is introduced. -
Preview of “Olympus Microscopy Resou... in Confocal Microscopy”
12/17/12 Olympus Microscopy Resource Center | Confocal Microscopy - Resolution and Contrast in Confocal … Olympus America | Research | Imaging Software | Confocal | Clinical | FAQ’s Resolution and Contrast in Confocal Microscopy Home Page Interactive Tutorials All optical microscopes, including conventional widefield, confocal, and two-photon instruments are limited in the resolution that they can achieve by a series of fundamental physical factors. In a perfect optical Microscopy Primer system, resolution is restricted by the numerical aperture of optical components and by the wavelength of light, both incident (excitation) and detected (emission). The concept of resolution is inseparable from Physics of Light & Color contrast, and is defined as the minimum separation between two points that results in a certain level of contrast between them. In a typical fluorescence microscope, contrast is determined by the number of Microscopy Basic Concepts photons collected from the specimen, the dynamic range of the signal, optical aberrations of the imaging system, and the number of picture elements (pixels) per unit area in the final image. Special Techniques Fluorescence Microscopy Confocal Microscopy Confocal Applications Digital Imaging Digital Image Galleries Digital Video Galleries Virtual Microscopy The influence of noise on the image of two closely spaced small objects is further interconnected with the related factors mentioned above, and can readily affect the quality of resulting images. While the effects of many instrumental and experimental variables on image contrast, and consequently on resolution, are familiar and rather obvious, the limitation on effective resolution resulting from the division of the image into a finite number of picture elements (pixels) may be unfamiliar to those new to digital microscopy. -
Super-Resolution Optical Imaging Using Microsphere Nanoscopy
Super-resolution Optical Imaging Using Microsphere Nanoscopy A thesis submitted to The University of Manchester For the degree of Doctor of Philosophy (PhD) in the Faculty of Engineering and Physical Sciences 2013 Seoungjun Lee School of Mechanical, Aerospace and Civil Engineering Super-resolution optical imaging using microsphere nanoscopy Table of Contents Table of Contents ...................................................................................................... 2 List of Figures and Tables ....................................................................................... 7 List of Publications ................................................................................................. 18 Abstract .................................................................................................................... 19 Declaration ............................................................................................................... 21 Copyright Statement ............................................................................................... 22 Acknowledgements ................................................................................................. 23 Dedication ............................................................................................................... 24 1 Introduction ...................................................................................................25 1.1 Research motivation and rationale ........................................................25 1.2 -
CMOS Image Sensors - Past Present and Future
CMOS Image Sensors - Past Present and Future Boyd Fowler, Xinqiao(Chiao) Liu, and Paul Vu Fairchild Imaging, 1801 McCarthy Blvd. Milpitas, CA 95035 USA Abstract sors. CMOS image sensors can integrate sensing and process- In this paper we present an historical perspective of CMOS ing on the same chip and have higher radiation tolerance than image sensors from their inception in the mid 1960s through CCDs. In addition CMOS sensors could be produced by a vari- their resurgence in the 1980s and 90s to their dominance in the ety of different foundries. This opened the creative flood gates 21st century. We focus on the evolution of key performance pa- and allowed people all over the world to experiment with CMOS rameters such as temporal read noise, fixed pattern noise, dark image sensors. current, quantum efficiency, dynamic range, and sensor format, The 1990’s saw the rapid development of CMOS image i.e the number of pixels. We discuss how these properties were sensors by universities and small companies. By the end of improved during the past 30 plus years. We also offer our per- the 1990’s image quality had been significantly improved, but spective on how performance will be improved by CMOS tech- it was still not as good as CCDs. During the first few years of nology scaling and the cell phone camera market. the 21st century it became clear that CMOS image sensor could out–perform CCDs in the high speed imaging market, but that Introduction their performance still lagged in other markets. Then, the devel- MOS image sensors are not a new development, and they opment of the cell phone camera market provided the necessary are also not a typical disruptive technology. -
Overcoming the Diffraction-Limited Spatio-Angular Resolution Tradeoff
Variable Aperture Light Field Photography: Overcoming the Diffraction-limited Spatio-angular Resolution Tradeoff Julie Chang1 Isaac Kauvar1 Xuemei Hu1,2 Gordon Wetzstein1 1Stanford University 2 Tsinghua University Abstract Small-f-number Large-f-number Light fields have many applications in machine vision, consumer photography, robotics, and microscopy. How- ever, the prevalent resolution limits of existing light field imaging systems hinder widespread adoption. In this pa- per, we analyze fundamental resolution limits of light field cameras in the diffraction limit. We propose a sequen- Depth-of-Field 10 tial, coded-aperture-style acquisition scheme that optimizes f/2 f/5.6 the resolution of a light field reconstructed from multiple f/22 photographs captured from different perspectives and f- 5 Blur-size-[mm] number settings. We also show that the proposed acquisi- 0 100 200 300 400 tion scheme facilitates high dynamic range light field imag- Distance-from-Camera-Lens-[mm] ing and demonstrate a proof-of-concept prototype system. Figure 1. Photographs captured with different f-number settings With this work, we hope to advance our understanding of exhibit different depths of field and also diffraction-limited resolu- the resolution limits of light field photography and develop tion for in-focus objects (top row). This effect is most pronounced practical computational imaging systems to overcome them. for macro photography, such as illustrated for a 50 mm lens fo- cused at 200 mm (bottom plot). Using multiple photographs cap- tured from different perspectives and with different f-number set- tings, the proposed method seeks to recover a light field with the 1. -
Improved Modulation Transfer Function Evaluation Method of a Camera at Any Field Point with a Scanning Tilted Knife Edge
Improved Modulation Transfer Function evaluation method of a camera at any field point with a scanning tilted knife edge PRESENTED AT SPIE SECURITY+DEFENSE 2020 BY ETIENNE HOMASSEL, TECHNICAL PRODUCT MANAGER HGH, 10 10 rue Maryse Bastié 91430 IGNY –France +33 (1) 69 35 47 70 [email protected] Improved Modulation Transfer Function evaluation method of a camera at any field point with a scanning tilted knife edge Etienne Homassel, Catherine Barrat, Frédéric Alves, Gilles Aubry, Guillaume Arquetoux HGH Systèmes Infrarouges, France ABSTRACT Modulating Transfer Function (MTF) has always been very important and useful for objectives quality definition and focal plane settings. This measurand provides the most relevant information on the optimized design and manufacturing of an optical system or the correct focus of a camera. MTF also gives out essential information on which defaults or aberrations appear on an optical objective, and so enables to diagnose potential design or manufacturing issues on a production line or R&D prototype. Test benches and algorithms have been defined and developed in order to satisfy the growing needs in optical objectives qualification as the latter become more and more critical in their accuracy and quality specification. Many methods are used to evaluate the Modulating Transfer Function. Slit imaging and scanning on a camera, MTF evaluation thanks to wavefront measurement or imaging fixed slanted knife edge on the detector of the camera. All these methods have pros and cons, some lack in resolution, accuracy or don’t enable to compare simulated MTF curves with real measured data. These methods are firstly reminded in this paper. -
Book VI Image
b bb bbb bbbbon.com bbbb Basic Photography in 180 Days Book VI - Image Editor: Ramon F. aeroramon.com Contents 1 Day 1 1 1.1 Visual arts ............................................... 1 1.1.1 Education and training .................................... 1 1.1.2 Drawing ............................................ 1 1.1.3 Painting ............................................ 3 1.1.4 Printmaking .......................................... 5 1.1.5 Photography .......................................... 5 1.1.6 Filmmaking .......................................... 6 1.1.7 Computer art ......................................... 6 1.1.8 Plastic arts .......................................... 6 1.1.9 United States of America copyright definition of visual art .................. 7 1.1.10 See also ............................................ 7 1.1.11 References .......................................... 9 1.1.12 Bibliography ......................................... 9 1.1.13 External links ......................................... 10 1.2 Image ................................................. 20 1.2.1 Characteristics ........................................ 21 1.2.2 Imagery (literary term) .................................... 21 1.2.3 Moving image ......................................... 22 1.2.4 See also ............................................ 22 1.2.5 References .......................................... 23 1.2.6 External links ......................................... 23 2 Day 2 24 2.1 Digital image ............................................ -
Deconvolution in Optical Microscopy
Histochemical Journal 26, 687-694 (1994) REVIEW Deconvolution in 3-D optical microscopy PETER SHAW Department of Cell Biology, John Innes Centre, Colney Lane, Norwich NR 4 7UH, UK Received I0 January 1994 and in revised form 4 March 1994 Summary Fluorescent probes are becoming ever more widely used in the study of subcellular structure, and determination of their three-dimensional distributions has become very important. Confocal microscopy is now a common technique for overcoming the problem of oubof-focus flare in fluorescence imaging, but an alternative method uses digital image processing of conventional fluorescence images-a technique often termed 'deconvolution' or 'restoration'. This review attempts to explain image deconvolution in a non-technical manner. It is also applicable to 3-D confocal images, and can provide a further significant improvement in clarity and interpretability of such images. Some examples of the application of image deconvolution to both conventional and confocal fluorescence images are shown. Introduction to alleviate the resolution limits of optical imaging. The most obvious resolution limit is due to the wavelength Optical microscopy is centuries old and yet is still at the of the light used- about 0.25 lam in general. This limi- heart of much of modem biological research, particularly tation can clearly be overcome by non-conventional in cell biology. The reasons are not hard to find. Much optical imaging such as near-field microscopy; whether it of the current power of optical microscopy stems from can be exceeded in conventional microscopy ('super-res- the availability of an almost endless variety of fluorescent olution') has been very controversial (see e.g. -
Optical Product News
Marshall Electronics OPTICAL SYSTEMS DIVISION PRODUCT NEWS V-ZPL06 / V-ZPL12 / V-ZPL1050 / V-ZPL-214 / V-ZPL-318 High Tech Zoom Pinhole Lenses • Available in 4-20mm Zoom or 10-50mm Zoom • High Quality Glass Elements • Removable push-on cap also acts as mounting • For 1/3” CCD with CS-Mount support • 7-12VDC operation • Manual or Motorized Control • 6” and 12” Long • Used for Industrial and Security Applications V-ZPL-214 / V-ZPL-214MZ V-ZPL-318 / V-ZPL-318MZ These lenses are ideal for those tough situations where the camera must be hidden and provide any angle of view between 4-20mm or 10-50mm. Although designed for 1/3” electronic iris cameras, these lenses are also useful on 1/2” cameras where they can provide up to a 120 degree horizontal field of view at 4mm. The V-ZPL06-MZ/ tip of the pinhole is built in to a removable push-on cap that also acts as a mounting support and protects V-ZPL06 the main optical system from damage. The motorized MZ series requires 7-12VDC to power the zoom motor. Recommended voltage is 9VDC. * f-stop = focal length / 1.6 Specifications - High Tech Zoom Pinhole Lenses Part No Range Control F-Stop O.D. x L V-ZPL-06 4-20mm Manual f2.5@4mm* 0.787” x 4” V-ZPL1050-MZ/ V-ZPL-06MZ 4-20mm Motorized f2.5@4mm* 0.787” x 4” V-ZPL1050 V-ZPL-12 4-20mm Manual f2.5@4mm* 0.787” x 13” V-ZPL-12MZ 4-20mm Motorized f2.5@4mm* 0.787” x 13” V-ZPL-1050 10-50mm Manual f2.5@10mm* 0.787” x 4.50” V-ZPL-1050MZ 10-50mm Motorized f2.5@10mm* 0.787” x 4.50” V-ZPL-214 2.8-14mm Manual f2.5@4mm* 0.79” x 3.56” V-ZPL12-MZ/ V-ZPL12 V-ZPL-214MZ 2.8-14mm Motorized f2.5@4mm* 0.79” x 3.56” V-ZPL-318 3.6-18mm Manual f2.5@4mm* 0.79” x 3.56” V-ZPL-318MZ 3.6-18mm Motorized f2.5@4mm* 0.79” x 3.56” V-ZPL-05-12 V-ZPL-05-01 Mini zoom pinhole lens Mini zoom pinhole lens with fixed pinhole cap V-ZPL-05-01 / V-ZPL-05-02 / V-ZPL-05-12 with removable pinhole cap Mini Zoom Pinhole Lenses Specifications - Mini Zoom Pinhole Lenses Image Sensor Part No. -
Pursuing the Diffraction Limit with Nano-LED Scanning Transmission Optical Microscopy
sensors Article Pursuing the Diffraction Limit with Nano-LED Scanning Transmission Optical Microscopy Sergio Moreno 1,* , Joan Canals 1 , Victor Moro 1, Nil Franch 1, Anna Vilà 1,2 , Albert Romano-Rodriguez 1,2 , Joan Daniel Prades 1,2, Daria D. Bezshlyakh 3, Andreas Waag 3, Katarzyna Kluczyk-Korch 4,5 , Matthias Auf der Maur 4 , Aldo Di Carlo 4,6 , Sigurd Krieger 7, Silvana Geleff 7 and Angel Diéguez 1,2 1 Electronic and Biomedical Engineering Department, University of Barcelona, 08028 Barcelona, Spain; [email protected] (J.C.); [email protected] (V.M.); [email protected] (N.F.); [email protected] (A.V.); [email protected] (A.R.-R.); [email protected] (J.D.P.); [email protected] (A.D.) 2 Institute for Nanoscience and Nanotechnology-IN2UB, University of Barcelona, 08028 Barcelona, Spain 3 Institute of Semiconductor Technology, Technische Universität Braunschweig, 38106 Braunschweig, Germany; [email protected] (D.D.B.); [email protected] (A.W.) 4 Department of Electronic Engineering, University of Rome “Tor Vergara”, 00133 Roma, Italy; [email protected] (K.K.-K.); [email protected] (M.A.d.M.); [email protected] (A.D.C.) 5 Faculty of Physics, University of Warsaw, 00-662 Warsaw, Poland 6 CNR-ISM, 00128 Rome, Italy 7 Department of Pathology, Medical University of Vienna, 1210 Wien, Austria; [email protected] (S.K.); [email protected] (S.G.) * Correspondence: [email protected] Abstract: Recent research into miniaturized illumination sources has prompted the development Citation: Moreno, S.; Canals, J.; of alternative microscopy techniques.