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Chapter 3 (Aberrations)
Chapter 3 Aberrations 3.1 Introduction In Chap. 2 we discussed the image-forming characteristics of optical systems, but we limited our consideration to an infinitesimal thread- like region about the optical axis called the paraxial region. In this chapter we will consider, in general terms, the behavior of lenses with finite apertures and fields of view. It has been pointed out that well- corrected optical systems behave nearly according to the rules of paraxial imagery given in Chap. 2. This is another way of stating that a lens without aberrations forms an image of the size and in the loca- tion given by the equations for the paraxial or first-order region. We shall measure the aberrations by the amount by which rays miss the paraxial image point. It can be seen that aberrations may be determined by calculating the location of the paraxial image of an object point and then tracing a large number of rays (by the exact trigonometrical ray-tracing equa- tions of Chap. 10) to determine the amounts by which the rays depart from the paraxial image point. Stated this baldly, the mathematical determination of the aberrations of a lens which covered any reason- able field at a real aperture would seem a formidable task, involving an almost infinite amount of labor. However, by classifying the various types of image faults and by understanding the behavior of each type, the work of determining the aberrations of a lens system can be sim- plified greatly, since only a few rays need be traced to evaluate each aberration; thus the problem assumes more manageable proportions. -
PETZVAL's LENS and CAMERA by Rudolf Kingslake
PETZVAL'S LENS AND CAMERA by Rudolf Kingslake Joseph Max Petzval was born on January 6, 1807, in Hungary of German parentage; he died 84 years later in September 1891. Being a member of the mathematics faculty of the University of Vienna, he naturally approached the problem of lens design from a mathematical rather than from an empir ical standpoint, which probably accounted in part for his suc cess. He actually designed two lenses in 1839, the Portrait lens which he immediately commissioned P. F. von Voigtlander to make, and the Orthoscopic lens which was not manufactured T THE OFFICIAL ANNOUNCEMENT of the Daguerreotype until 1856. Petvzal's interest in optics continued throughout the A process in 1839, Austria was represented by Professor A. rest of his life, and he reported in 1843 that "by order of the F. von Ettingshausen. He was so impressed with the possibilities General-Director Archduke Ludwig, he was assisted in his of photography that upon his return to Vienna, he induced his calculations for several years by two officers and eight friend and colleague the mathematician Joseph Petzval to undertake the design of a wide-aperture lens suitable for por traiture. Petzval, then 33 years old, devoted himeslf enthusiasti cally to the problem and was amazingly successful. He used a well-corrected telescope objective the right way round for his front component, and added an airspaced doublet behind it, the rear doublet being mathematically designed to give sharp de finition and to flatten the field. The formula was handed to the old-established Viennese optician Voigtlander, who first supplied the lens to a focal length of 150 mm and an aperture of f/3.6, mounted in a conical metal camera having a circular ground-glass focusing screen 94 mm diameter with a focusing magnifier permanently installed behind it. -
Portraiture, Surveillance, and the Continuity Aesthetic of Blur
Michigan Technological University Digital Commons @ Michigan Tech Michigan Tech Publications 6-22-2021 Portraiture, Surveillance, and the Continuity Aesthetic of Blur Stefka Hristova Michigan Technological University, [email protected] Follow this and additional works at: https://digitalcommons.mtu.edu/michigantech-p Part of the Arts and Humanities Commons Recommended Citation Hristova, S. (2021). Portraiture, Surveillance, and the Continuity Aesthetic of Blur. Frames Cinema Journal, 18, 59-98. http://doi.org/10.15664/fcj.v18i1.2249 Retrieved from: https://digitalcommons.mtu.edu/michigantech-p/15062 Follow this and additional works at: https://digitalcommons.mtu.edu/michigantech-p Part of the Arts and Humanities Commons Portraiture, Surveillance, and the Continuity Aesthetic of Blur Stefka Hristova DOI:10.15664/fcj.v18i1.2249 Frames Cinema Journal ISSN 2053–8812 Issue 18 (Jun 2021) http://www.framescinemajournal.com Frames Cinema Journal, Issue 18 (June 2021) Portraiture, Surveillance, and the Continuity Aesthetic of Blur Stefka Hristova Introduction With the increasing transformation of photography away from a camera-based analogue image-making process into a computerised set of procedures, the ontology of the photographic image has been challenged. Portraits in particular have become reconfigured into what Mark B. Hansen has called “digital facial images” and Mitra Azar has subsequently reworked into “algorithmic facial images.” 1 This transition has amplified the role of portraiture as a representational device, as a node in a network -
Tessar and Dagor Lenses
Tessar and Dagor lenses Lens Design OPTI 517 Prof. Jose Sasian Important basic lens forms Petzval DB Gauss Cooke Triplet little stress Stressed with Stressed with Low high-order Prof. Jose Sasian high high-order aberrations aberrations Measuring lens sensitivity to surface tilts 1 u 1 2 u W131 AB y W222 B y 2 n 2 n 2 2 1 1 1 1 u 1 1 1 u as B y cs A y 1 m Bstop ystop n'u' n 1 m ystop n'u' n CS cs 2 AS as 2 j j Prof. Jose Sasian Lens sensitivity comparison Coma sensitivity 0.32 Astigmatism sensitivity 0.27 Coma sensitivity 2.87 Astigmatism sensitivity 0.92 Coma sensitivity 0.99 Astigmatism sensitivity 0.18 Prof. Jose Sasian Actual tough and easy to align designs Off-the-shelf relay at F/6 Coma sensitivity 0.54 Astigmatism sensitivity 0.78 Coma sensitivity 0.14 Astigmatism sensitivity 0.21 Improper opto-mechanics leads to tough alignment Prof. Jose Sasian Tessar lens • More degrees of freedom • Can be thought of as a re-optimization of the PROTAR • Sharper than Cooke triplet (low index) • Compactness • Tessar, greek, four • 1902, Paul Rudolph • New achromat reduces lens stress Prof. Jose Sasian Tessar • The front component has very little power and acts as a corrector of the rear component new achromat • The cemented interface of the new achromat: 1) reduces zonal spherical aberration, 2) reduces oblique spherical aberration, 3) reduces zonal astigmatism • It is a compact lens Prof. Jose Sasian Merte’s Patent of 1932 Faster Tessar lens F/5.6 Prof. -
Applied Physics I Subject Code: PHY-106 Set: a Section: …………………………
Test-1 Subject: Applied Physics I Subject Code: PHY-106 Set: A Section: ………………………….. Max. Marks: 30 Registration Number: ……………… Max. Time: 45min Roll Number: ………………………. Question 1. Define systematic and random errors. (5) Question 2. In an experiment in determining the density of a rectangular block, the dimensions of the block are measured with a vernier caliper with least count of 0.01 cm and its mass is measured with a beam balance of least count 0.1 g, l = 5.12 cm, b = 2.56 cm, t = 0.37 cm and m = 39.3 g. Report correctly the density of the block. (10) Question 3. Derive a relation to overcome chromatic aberration for an optical system consisting of two convex lenses. (5) Question 4. An achromatic doublet of focal length 20 cm is to be made by placing a convex lens of borosilicate crown glass in contact with a diverging lens of dense flint glass. Assuming nr = 1.51462, nb = ′ ′ 1.52264, 푛푟 = 1.61216, and 푛푏 = 1.62901, calculate the focal length of each lens; here the unprimed and the primed quantities refer to the borosilicate crown glass and dense flint glass, respectively. (10) Test-1 Subject: Applied Physics I Subject Code: PHY-106 Set: B Section: ………………………….. Max. Marks: 30 Registration Number: ……………… Max. Time: 45min Roll Number: ………………………. Question 1. Distinguish accuracy and precision with example. (5) Question 2. Obtain an expression for chromatic aberration in the image formed by paraxial rays. (5) Question 3. It is required to find the volume of a rectangular block. A vernier caliper is used to measure the length, width and height of the block. -
Carl Zeiss Oberkochen Large Format Lenses 1950-1972
Large format lenses from Carl Zeiss Oberkochen 1950-1972 © 2013-2019 Arne Cröll – All Rights Reserved (this version is from October 4, 2019) Carl Zeiss Jena and Carl Zeiss Oberkochen Before and during WWII, the Carl Zeiss company in Jena was one of the largest optics manufacturers in Germany. They produced a variety of lenses suitable for large format (LF) photography, including the well- known Tessars and Protars in several series, but also process lenses and aerial lenses. The Zeiss-Ikon sister company in Dresden manufactured a range of large format cameras, such as the Zeiss “Ideal”, “Maximar”, Tropen-Adoro”, and “Juwel” (Jewel); the latter camera, in the 3¼” x 4¼” size, was used by Ansel Adams for some time. At the end of World War II, the German state of Thuringia, where Jena is located, was under the control of British and American troops. However, the Yalta Conference agreement placed it under Soviet control shortly thereafter. Just before the US command handed the administration of Thuringia over to the Soviet Army, American troops moved a considerable part of the leading management and research staff of Carl Zeiss Jena and the sister company Schott glass to Heidenheim near Stuttgart, 126 people in all [1]. They immediately started to look for a suitable place for a new factory and found it in the small town of Oberkochen, just 20km from Heidenheim. This led to the foundation of the company “Opton Optische Werke” in Oberkochen, West Germany, on Oct. 30, 1946, initially as a full subsidiary of the original factory in Jena. -
The History of Petzval Lenses 11-06-11 14:43
The history of Petzval Lenses 11-06-11 14:43 Antique & Classic Cameras Home Blog Camera Appraisals Rolleiflex Rolleicords Rolleiflex Buying Tip Leica M Lenses 50 Summicron-M Lenses 35 Summicron-M Lenses Leica 28mm M-Lenses Most Watched Leica Leica M Cameras Leica Screw Lenses Leica Screw Cameras Leica Lens Reviews Leica R Lenses Sonnar Lens Petzval Lens Soft Focus Lenses Soft Focus Lenses 2 Soft Focus Lenses 3 Soft Focus Lens Sales Soft Focus Lens Test Heliar Lenses Canon RF Lens Canon 50mm F/1.2 LTM Canon RF Cameras Fuji 6x7 & 6x9 Fuji 645 Cameras Hasselblad 6x6 Hasselblad C Lenses Pentax 6x7 Lenses Ricohflex Nikon RF Lens Zeiss Contax RF Lens Contax G Lens Super Ikonta Minolta-35 RF Pentax M42 Lens Bokeh Fuji 617 Olympus Stylus Epic 1890 Lens Catalogue 1892 Steinheil Lens Ads 1892 Zeiss Lens Ads 1904 Dallmeyer Lens Ads 1904 Busch Lens Ads 1904 Goerz Lens Ads Antique Wood Cameras Photographers 1860-1900 1857 CC Harrison Lens Harrison Globe Lens 1871 Camera Catalog 1883 Blair Envelope 1895 Sunart Camera 1910 Premo Catalog 1848-1875 Advertisements Camera Books Most Watched Lens Vade Mecum Links Contact Us About Us Morgan Low Ball Dollars Petzval Portrait Lenses and Their History Daguerre announced his process to the world on August 19, 1839. The original Daguerre & Giroux Camera utilized a lens designed and manufactured by Charles Chevalier, celebrated microscope maker and son of Vincent Chevalier who founded their optical business in France. The Chevalier 16-inch telescope objective was comprised of a cemented doublet and was achromatic. The lens, which covered a whole plate, had a working aperture of f/17, and suffered from considerable spherical abberations. -
Engineering an Achromatic Bessel Beam Using a Phase-Only Spatial Light Modulator and an Iterative Fourier Transformation Algorithm
Optics Communications 383 (2017) 64–68 Contents lists available at ScienceDirect Optics Communications journal homepage: www.elsevier.com/locate/optcom Engineering an achromatic Bessel beam using a phase-only spatial light modulator and an iterative Fourier transformation algorithm Marie Walde a, Aurélie Jost a, Kai Wicker a,b,c, Rainer Heintzmann a,c,n a Institut für Physikalische Chemie (IPC), Abbe Center of Photonics, Friedrich-Schiller-Universität, Jena, Germany b Carl Zeiss AG, Corporate Research and Technology, Jena, Germany c Leibniz Institute of Photonic Technology (IPHT), Jena, Germany article info abstract Article history: Bessel illumination is an established method in optical imaging and manipulation to achieve an extended Received 12 June 2016 depth of field without compromising the lateral resolution. When broadband or multicolour imaging is Received in revised form required, wavelength-dependent changes in the radial profile of the Bessel illumination can complicate 13 August 2016 further image processing and analysis. Accepted 21 August 2016 We present a solution for engineering a multicolour Bessel beam that is easy to implement and Available online 2 September 2016 promises to be particularly useful for broadband imaging applications. A phase-only spatial light mod- Keywords: ulator (SLM) in the image plane and an iterative Fourier Transformation algorithm (IFTA) are used to Bessel beam create an annular light distribution in the back focal plane of a lens. The 2D Fourier transformation of Spatial light modulator such a light ring yields a Bessel beam with a constant radial profile for different wavelength. Non-diffracting beams & 2016 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY-NC-ND Iterative Fourier transform algorithm Frequency filtering license (http://creativecommons.org/licenses/by-nc-nd/4.0/). -
The Techniques and Material Aesthetics of the Daguerreotype
The Techniques and Material Aesthetics of the Daguerreotype Michael A. Robinson Submitted for the degree of Doctor of Philosophy Photographic History Photographic History Research Centre De Montfort University Leicester Supervisors: Dr. Kelley Wilder and Stephen Brown March 2017 Robinson: The Techniques and Material Aesthetics of the Daguerreotype For Grania Grace ii Robinson: The Techniques and Material Aesthetics of the Daguerreotype Abstract This thesis explains why daguerreotypes look the way they do. It does this by retracing the pathway of discovery and innovation described in historical accounts, and combining this historical research with artisanal, tacit, and causal knowledge gained from synthesizing new daguerreotypes in the laboratory. Admired for its astonishing clarity and holographic tones, each daguerreotype contains a unique material story about the process of its creation. Clues from the historical record that report improvements in the art are tested in practice to explicitly understand the cause for effects described in texts and observed in historic images. This approach raises awareness of the materiality of the daguerreotype as an image, and the materiality of the daguerreotype as a process. The structure of this thesis is determined by the techniques and materials of the daguerreotype in the order of practice related to improvements in speed, tone and spectral sensitivity, which were the prime motivation for advancements. Chapters are devoted to the silver plate, iodine sensitizing, halogen acceleration, and optics and their contribution toward image quality is revealed. The evolution of the lens is explained using some of the oldest cameras extant. Daguerre’s discovery of the latent image is presented as the result of tacit experience rather than fortunate accident. -
Petzval's Portrait Lens
Petzval’s portrait lens Lens Design OPTI 517 Prof. Jose Sasian Prof. Jose Sasian Chronology • Camera obscura; Leonardo da Vinci (1452- 1519) provided the first known technical description • The idea of capturing an image • Lois Jacques Mande Daguerre (1787-1851) succeeded in finding a photographic process. This was announced in 1939 Prof. Jose Sasian Time table 1812 W. Wollaston landscape lens; 30 deg @ f/15 1825 ~T. Young, G. Airy, J. Herschel, H. Coddington 1828 Hamilton's theory of systems of rays 1839 Photography was made a practical reality 1839 Chevalier lens 1840 Petzval (Hungarian) portrait lens; 15 deg @ f/3.6 1841 Gauss’s cardinal points, focal and principal 1856 Seidel theory Prof. Jose Sasian Joseph Petzval 1807-1891 Prof. Jose Sasian Specification R +52.9 -41.4 +436.2 +104.8 +36.8 45.5 -149.5 N-crown=1.517; N-flint=1.576 T 5.8 1.5 23.3/23.3 2.2 0.7 3.6 F=100 mm Prof. Jose Sasian Petzval portrait lens could actually take photographs of people. This likely contributed to its success. It made photography a practical reality. Prof. Jose Sasian Petzval Portrait lens vs Wollanston landscape lens •F/3.6 •F/15 •Field +/- 15 degrees •Field +/- 30 degrees •Artificially flattened field •Artificially flattened field •1840 •1812 •Photography process announced •Applied to camera obscura in 1839 Petzval portrait lens could actually take photographs of people. This likely contributed to its success. It made photography a practical reality. Prof. Jose Sasian Images Object Image Prof. Jose Sasian The state of the art • Telescope doublets: Chromatic aberration and spherical aberration • Periscopic lenses in the camera obscura • Airy’s study of the periscopic lens exhibiting the trade of between astigmatism and field curvature. -
Combinations of Achromatic Doublets
Combinations of achromatic doublets Introduction to aberrations OPTI 518 Prof. Jose Sasian Copyright © 2019 Plano convex lens N-BK7 : Petzval radius -151.7 mm 1 CPetzval IV Petzval n Prof. Jose Sasian Copyright © 2019 Wollaston meniscus lens WW222/0.8 220P • Artificially flattening the field • Periscopic lenses Prof. Jose Sasian Copyright © 2019 Periskop lens • Principle of symmetry • No distortion Prof. Jose Sasian Copyright © 2019 Field curvature • Old achromat • New achromat N-BK7 : Petzval radius -151.7 mm N-BK7 and N-F2: Petzval radius -139.99 mm (+139.99 for negative doublet) N-BAK1 and N-LLF6: Petzval radius -185 mm 1 12 vv 12 CPetzval IV Petzval nn12 vvnn 1212 Prof. Jose Sasian Copyright © 2019 Chevalier landscape lens WW222/0.8 220P • F/5 telescope doublet used in reverse and with an aperture stop in front Prof. Jose Sasian Copyright © 2019 Rapid rectilinear • F/8 • Glass selection is key to minimize spherical aberration while artificially flattening the field RMS spot size Prof. Jose Sasian Copyright © 2019 Lister microscope objective • Telecentric y 1 B 2 IA IB 0 22 22 IIA IIB II Ayy A IIA B B IIB y2 B IIA2 IIB III11yy B B IIB 0 1 yB *2 SSIII III2 SSSS II I Prof. Jose Sasian Copyright © 2019 Lister microscope objective Practical solution • RMS spot size in waves • Two identical doublets • Spherical aberration and coma are corrected • Astigmatism is small • Telecentric • Less vignetting Prof. Jose Sasian Copyright © 2019 Aplanatic concentric meniscus lens • Optical speed is increased by an N factor Prof. Jose Sasian Copyright © 2019 Petzval portrait objective f’=144 mm; F/3.7; FOV=+/- 16.5⁰. -
Magnesiumrich Intralensar Structures In
[Palaeontology, Vol. 50, Part 5, 2007, pp. 1031–1037] MAGNESIUM-RICH INTRALENSAR STRUCTURES IN SCHIZOCHROAL TRILOBITE EYES by MARTIN R. LEE, CLARE TORNEY and ALAN W. OWEN Department of Geographical and Earth Sciences, University of Glasgow, Gregory Building, Lilybank Gardens, Glasgow G12 8QQ, UK; e-mail: [email protected] Typescript received 14 March 2007; accepted in revised form 25 May 2007 Abstract: The interpretation of the lenses of schizochroal ucts reflect original differences in mineral chemistry between trilobite eyes as aplanatic doublets by Clarkson and Levi-Setti the upper lens unit and lower intralensar bowl. The turbidity over 30 years ago has been widely accepted. However, the of the bowl and of the core within the upper part of the lens means of achieving a difference in refractive index across the are the result of their greater microporosity and abundance interface between the two parts of each lens to overcome of microdolomite inclusions, both of which were products of spherical aberration has remained a matter of speculation diagenetic replacement of original magnesian calcite in these and lately it has been argued that the doublet structure itself areas. Such a difference in magnesium concentration in the is no more than a diagenetic artefact. Recent advances in original calcite has long been postulated as one of the ways technologies for imaging, chemical analysis and crystallo- by which the interface between these lens units could have graphic characterization of minerals at high spatial resolu- produced an aberration-free image and the present study tions have enabled a re-examination of the structure of provides the first direct evidence of such a chemical contrast, calcite lenses at an unprecedented level of detail.