Abbe Number 1 Abbe Number

Total Page:16

File Type:pdf, Size:1020Kb

Abbe Number 1 Abbe Number Abbe number 1 Abbe number In physics and optics, the Abbe number, also known as the V-number or constringence of a transparent material, is a measure of the material's dispersion (variation of refractive index with wavelength) in relation to the refractive index, with high values of V indicating low dispersion (low chromatic aberration). It is named after Ernst Abbe (1840–1905), the German physicist who defined it. The Abbe number,[2][3] V , of a D material is defined as where n , n and n are the refractive An Abbe diagram plots the Abbe number against refractive index for a range of different D F C glasses (red dots). Glasses are classified using the Schott Glass letter-number code to indices of the material at the reflect their composition and position on the diagram. wavelengths of the Fraunhofer D-, F- and C- spectral lines (589.3 nm, 486.1 nm and 656.3 nm respectively). Abbe numbers are used to classify glass and other optically transparent materials. For example, flint glass has V < 50 and crown glass has V > 50. Typical values of V range from around 20 for very dense flint glass, around 30 for polycarbonate plastics, and up to 65 for very light crown glass, and up to 85 for fluor-crown glass. Abbe numbers are only a useful measure of dispersion Influences of selected glass component additions on the Abbe [1] for visible light, and for other number of a specific base glass. wavelengths, or for higher precision work, the group velocity dispersion is used. Due to the difficulty and inconvenience in producing sodium and hydrogen lines, alternate definitions of the Abbe number are used in some contexts (ISO 7944).[4] The value V is given by d which defines the Abbe number with respect to the yellow Fraunhofer d (or D ) helium line at 587.5618 nm 3 wavelength. It can also be defined at the green mercury E-line at 546.073 nm: where F' and C' are the blue and red cadmium lines at 480.0 nm and 643.8 nm, respectively. Abbe number 2 An Abbe diagram is produced by plotting the Abbe number V of a material versus its refractive index n . Glasses d d can then be categorised by their composition and position on the diagram. This can be a letter-number code, as used in the Schott Glass catalogue, or a 6-digit glass code. Abbe numbers are used to calculate the necessary focal lengths of achromatic doublet lenses to minimize chromatic aberration. The following table lists standard wavelengths at which n is usually determined, indicated by subscripts.[5] For example, n is measured at 589.3 nm: D λ in nm Fraunhofer's symbol Light source Color 365.01 i Hg UV 404.66 h Hg violet 435.84 g Hg blue 479.99 F' Cd blue 486.13 F H blue 546.07 e Hg green 587.56 d He yellow 589.3 D Na yellow 643.85 C' Cd red 656.27 C H red 706.52 r He red 768.2 A' K IR 852.11 s Cs IR 1013.98 t Hg IR References [1] Abbe number calculation of glasses (http:/ / glassproperties. com/ abbe_number/ ) [5] L. D. Pye, V. D. Frechette, N. J. Kreidl: "Borate Glasses"; Plenum Press, New York, 1977 Article Sources and Contributors 3 Article Sources and Contributors Abbe number Source: http://en.wikipedia.org/w/index.php?oldid=544283510 Contributors: Afluegel, Alro, BenFrantzDale, Bgwhite, BinaryPhoton, Carbuncle, Cedders, Conversion script, DrBob, EdH, Eric Bajart, FocalPoint, Fountains of Bryn Mawr, Garvin58, Giftlite, Gisling, Highrool, Karada, Kaszeta, Looxix, MichaelGoldshteyn, Mpolyanskiy, Outlook, Peak, Reelrt, Renato Caniatti, Rich Farmbrough, Rjwilmsi, Ryulong, Sam Paris, Srleffler, Superm401, Tarquin, XJaM, 15 anonymous edits Image Sources, Licenses and Contributors Image:Abbe-diagram 2.svg Source: http://en.wikipedia.org/w/index.php?title=File:Abbe-diagram_2.svg License: Creative Commons Attribution-ShareAlike 3.0 Unported Contributors: Abbe-diagram.png: Bob Mellish Abbe-diagram.svg: Eric Bajart derivative work: Eric Bajart Image:SpiderGraph Abbe Number-en.svg Source: http://en.wikipedia.org/w/index.php?title=File:SpiderGraph_Abbe_Number-en.svg License: GNU Free Documentation License Contributors: SpiderGraph_Abbe_Number.gif : Afluegel Derivative work : Eric Bajart License Creative Commons Attribution-Share Alike 3.0 Unported //creativecommons.org/licenses/by-sa/3.0/.
Recommended publications
  • High-Power Solid-State Lasers from a Laser Glass Perspective
    LLNL-JRNL-464385 High-Power Solid-State Lasers from a Laser Glass Perspective J. H. Campbell, J. S. Hayden, A. J. Marker December 22, 2010 Internationakl Journal of Applied Glass Science Disclaimer This document was prepared as an account of work sponsored by an agency of the United States government. Neither the United States government nor Lawrence Livermore National Security, LLC, nor any of their employees makes any warranty, expressed or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States government or Lawrence Livermore National Security, LLC. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States government or Lawrence Livermore National Security, LLC, and shall not be used for advertising or product endorsement purposes. High-Power Solid-State Lasers from a Laser Glass Perspective John H. Campbell, Lawrence Livermore National Laboratory, Livermore, CA Joseph S. Hayden and Alex Marker, Schott North America, Inc., Duryea, PA Abstract Advances in laser glass compositions and manufacturing have enabled a new class of high-energy/high- power (HEHP), petawatt (PW) and high-average-power (HAP) laser systems that are being used for fusion energy ignition demonstration, fundamental physics research and materials processing, respectively. The requirements for these three laser systems are different necessitating different glasses or groups of glasses.
    [Show full text]
  • Test Report for Delivery Lots of Optical Glass TIE-04
    Technical Information 1 Advanced Optics Version May 2016 TIE-04 Test report for delivery lots of optical glass Introduction 1. Backtracking of material properties and With every delivery of fine annealed optical glass the customer production information of lots. 1 receives a test report in accordance with ISO 10474. The test report contains non-specific test results to confirm the compli- 2. Compilation of delivery lots ��������������������������������������������� 1 ance of the delivery with the order. That means that random 3. Marking of the delivery lot and batches ��������������������� 2 representative test samples were inspected during production to ensure the compliance with the order. The specific choice 4. Details in the test report of fine annealed of test samples and inspection procedures ensures the validity optical glass ����������������������������������������������������������������������������� 2 of results for all parts of the delivery lot even if they were not 5. Annealing schedule of coarse annealed individually tested. optical glass . 4 6. Additional test certificates . 6 7. Literature . 6 1. Backtracking of material properties and nd νd production information of lots Step 0.5* ± 0.0001 ± 0.1 % Step 1 ± 0.0002 ± 0.2 % A batch is numbered directly after melting and coarse anneal- Step 2 ± 0.0003 ± 0.3 % ing. The batch number is kept in all further processing steps Step 3 ± 0.0005 ± 0.5 % and therefore allows to backtrace all important material prop- erties and production information. * only for selected glass types Tab. 1: Tolerances for refractive index and Abbe number We recommend to preserve the batch numbers of glass pieces (according to ISO 12123) [1] used for following processing steps.
    [Show full text]
  • The Walman Optical Perspective on High Index Lenses
    Optical Perspective of Polycarbonate Material JP Wei, Ph. D. November 2011 Introduction Among the materials developed for eyeglasses, polycarbonate is one that has a number of very unique properties and provides real benefits to eyeglass wearers. Polycarbonate lenses are not only cosmetically thinner, lighter, and provide superior impact-resistance, but also produce sharp optical clarity for both central and peripheral vision. It is well-known that as the index of refraction increases dispersion also increases. In other words, the higher the refractive index, the low the ABBE value. An increase in dispersion will cause an increase in chromatic aberration. Therefore, one of the concerns in the use of lens materials such as polycarbonate is: will chromatic aberration negatively affect patient adaption? MID 1.70 LENS MATERIAL CR39 TRIVEX INDEX POLYCARBONATE 1.67 INDEX INDEX REFRACTIVE INDEX 1.499 1.529 1.558 1.586 1.661 1.700 ABBE VALUES 58 45 37 30 32 36 The refractive index of a material is often abbreviated “n.” Except for air, which has a refractive index of approximately 1, the refractive index of most substances is greater than 1 (n > 1). Water, for instance, has a refractive index of 1.333. The higher the refractive index of a lens material, the slower the light will travel through it. While it is commonly recognized that high index materials will have greater chromatic aberration than CR-39 or low refractive index lenses, there has been no quantification of the amount of visual acuity loss that results from chromatic aberration. The purpose of this paper is to review the optical properties of polycarbonate material, its advantages over other lens materials, and the impact of chromatic aberration caused by the relative low ABBE value of the material on vision and clinical significance.
    [Show full text]
  • Correlation of the Abbe Number, the Refractive Index, and Glass Transition Temperature to the Degree of Polymerization of Norbornane in Polycarbonate Polymers
    polymers Article Correlation of the Abbe Number, the Refractive Index, and Glass Transition Temperature to the Degree of Polymerization of Norbornane in Polycarbonate Polymers Noriyuki Kato 1,2,*, Shinya Ikeda 1, Manabu Hirakawa 1 and Hiroshi Ito 2,3 1 Mitsubishi Gas Chemical Company, 2-5-2 Marunouchi, Chiyoda-ku, Tokyo 100-8324, Japan; [email protected] (S.I.); [email protected] (M.H.) 2 Graduate School of Science and Engineering, Yamagata University, 4-3-16 Jonan, Yonezawa, Yamagata 992-8510, Japan; [email protected] 3 Graduate School of Organic Materials Science, Yamagata University, 4-3-16 Jonan, Yonezawa, Yamagata 992-8510, Japan * Correspondence: [email protected] Received: 1 September 2020; Accepted: 16 October 2020; Published: 26 October 2020 Abstract: The influences of the average degree of polymerization (Dp), which is derived from Mn and terminal end group, on optical and thermal properties of various refractive indexed transparent polymers were investigated. In this study, we selected the alicyclic compound, Dinorbornane dimethanol (DNDM) homo polymer, because it has been used as a representative monomer in low refractive index polymers for its unique properties. DNDM monomer has a stable amorphous phase and reacts like a polymer. Its unique reaction allows continuous investigation from monomer to polymer. For hydroxy end group and phenolic end group polymers, the refractive index (nd) decreased with increasing Dp, and both converged to same value in the high Dp region. However, the Abbe number (νd) of a hydroxy end group polymer is not dependent on Dp, and the νd of a phenolic end group polymer is greatly dependent on Dp.
    [Show full text]
  • Development of Highly Transparent Zirconia Ceramics
    11 Development of highly transparent zirconia ceramics Isao Yamashita *1 Masayuki Kudo *1 Koji Tsukuma *1 Highly transparent zirconia ceramics were developed and their optical and mechanical properties were comprehensively studied. A low optical haze value (H<1.0 %), defined as the diffuse transmission divided by the total forward transmission, was achieved by using high-purity powder and a novel sintering process. Theoretical in-line transmission (74 %) was observed from the ultraviolet–visible region up to the infra-red region; an absorption edge was found at 350 nm and 8 µm for the ultraviolet and infrared region, respectively. A colorless sintered body having a high refractive index (n d = 2.23) and a high Abbe’s number (νd = 27.8) was obtained. A remarkably large dielectric constant (ε = 32.7) with low dielectric loss (tanδ = 0.006) was found. Transparent zirconia ceramics are candidates for high-refractive index lenses, optoelectric devices and infrared windows. Transparent zirconia ceramics also possess excellent mechanical properties. Various colored transparent zirconia can be used as exterior components and for complex-shaped gemstones. fabricating transparent cubic zirconia ceramics.9,13-19 1.Introduction Transparent zirconia ceramics using titanium oxide as Transparent and translucent ceramics have been a sintering additive were firstly reported by Tsukuma.15 studied extensively ever since the seminal work on However, the sintered body had poor transparency translucent alumina polycrystal by Coble in the 1960s.1 and low mechanical strength. In this study, highly Subsequently, researchers have conducted many transparent zirconia ceramics of high strength were studies to develop transparent ceramics such as MgO,2 developed.
    [Show full text]
  • Trivex & Polycarbonate Lenses
    Trivex Trivex was originally developed for the military, as visual armor. PPG Industries took the technology and adapted it for the optical industry. Trivex is a urethane-based pre-polymer. PPG named the material Trivex because of its three main performance properties. The three main properties are superior optics, ultra- lightweight, and extreme strength. Trivex has a high abbe value. Abbe value is a measure of the dispersion or color distortion of light through a lens into its color elements. Abbe number can also be referred to as v-value. The higher the abbe number, the less dispersion, the lower the number, the more dispersion. Trivex has an abbe number of 43-45. This is significantly higher than polycarbonate. Polycarbonate's abbe number is 30. Trivex has a very high level of light transmittance. The level is 91.4%. This is one of the highest levels of all lens materials. The high percentage is a factor that directly affects the brightness, clarity, and crispness of Trivex. Trivex has a specific gravity of 1.11. Specific gravity is the weight in grams of one cubic centimeter of the material. Specific gravity is also referred to as density. The higher the number, the more dense, or heavy, a lens material is. Trivex has the lowest specific gravity of any commonly used lens material. This makes Trivex the lightest lens material. Trivex is 16% lighter than CR-39, 25% lighter than 1.66, and 8% lighter than polycarbonate! Trivex has a refractive index of 1.53. This allows for a thinner lens than a CR-39 lens.
    [Show full text]
  • Optical Glass
    OPTICAL GLASS JAN. 2020 Contents New Glass Types . 4 3. Chemical Properties . 87 OHARA Group . 21 3 1. Water Resistance RW(p) and Main Products . 22 Acid Resistance RA(p) (Powder Method) . 88 Comparative Table of Optical Glasses, 3 .2 Weathering Resistance W(s) (Surface Method) . 89 Codes and Glass-types . 26 3 .3 Acid Resistance (SR) . 89 3 .4 Phosphate Resistance (PR) . 92 1. Designation of OHARA’s Optical Glass Types . 80 4. Thermal Properties . 93 4 1. Transformation Temperature (Tg), 2. Optical Properties . 81 Yield Point (At) . 93 2 1. Refractive Index . 81 4 .2 Softening Point (SP) . 94 2 2. Dispersion . 82 4 .3 Annealing Point (AP) . 94 2 .3 Partial Dispersion Ratio, Anomalous Dispersion 82 4.4 Linear Coefficient of Thermal Expansion (α) . 94 2 .4 Temperature Coefficient of 4 .5 Thermal Conductivity (k) . 94 Refractive Index (dn/dTrelative) . 83 2 5. Coloring . 85 2.6 Internal Transmittance λ0 .80 / λ 0 .05 . 86 2 .7 CCI . 86 2 5. Mechanical Properties . 95 8. Forms of Supply . 104 5 1. Knoop Hardness (Hk) . 95 8 1. Glass Blocks . 104 5 .2 Abrasion (Aa) . 96 8 .2 Pressings (Reheat Pressings – RP) . 105 8 .3 Saw-cut Centerless Ground Cylindrical 6. Other Properties . 97 Blanks . 107 6.1 Photoelastic Constant (β) . 97 8 .4 Dimensional Specified Blanks . 108 6 .2 Specific Gravity (d) . 97 8 .5 High Homogeneity Blanks . 109 8 .6 Polished Balls . 110 7. Guarantees of Quality . 98 8 7. Polished Preforms . 111 7 1. Refractive Index and Abbe Number . 98 8 .8 Aspherical Glass Mold Lenses .
    [Show full text]
  • Abbe Number 404 Absorption 570 by Transition Metals 234 Edge 333
    INDEX (Bold Type indicates Chapter) A c Cab-O-SiI™ 7 Abbe number 404 Cadmium sulfide 332 Absorption 570 selenide 338 by transition metals 234 telluride 338 edge 333 Calorimetry 209 Acetyl acetonates 159, 176,239 Catalysis 360 Aerogels 23, 96, 366 Catalysts for hydrolysis 41 Aerosol 161 acid 3, 86 ammonia 86, 330 Alumina 160, 170, 376 base 86 Aluminosilicate 302 Catalyst supports 343 Li/Mg0365 Auger electron spectroscopy (AES) 179, 492 Ru/Si02 359 Autoclaving 24 Pd/Si02359 Pt/Ti02363 B Pt-Sn/AI203364 Barium titanate 43 Cerarners 427 BET method 345, 547 Cermet Birefringence 272, 441 silica-precious metal 344 Bloating 26 Chalcogenides 473 Boria 402, 493 Chelating agents b-diketones 44, 259, 457 Boric acid 17 5 glycol 259, 426 Borosilicates 493 Chemical leaching 296, 375 with baria 407 584 Chemical vapor deposition (CVD) 256 Conductivity modified (MCVD) 157 electrical 268 thermal 24 Chlorination 27, 103 Conventional melting 60, 83, 328 Chromophores bipyridyltriscarbonylchloro Copper bromide 340 rhenium (ReCI(CO)3 birpy) 302 Copper chloride 340 DEANST (diethylamino­ nitrostyrene) 429 Coupling efficiency 525 HNPP (N -(3-hydroxy-4-nitro­ phenyl)-(L)-prolinol) Crosslinking 49, 451 429 NPP (N--(4-nitrophenyl)-(L)­ Crystallization 28, 132, 207, 266, 332, prolinol) 429 502 PNA (para-nitroaniline) 420 D Clean room conditions 144,470 Defects Coatings (see also Layers, Thin Films) bubbles 66 adhesion of 268 colored 233 Dehydration conductive 173,269,431 chemical 27, 66, 102 electroc:hromic 178,497 chlorine treatments 27, 103 multilayer 171, 242 thermal
    [Show full text]
  • Teaching Optics
    Optica Applicata. Vol. XXXI, No. 4, 2001 Teaching optics Possibilities of aberration correction in a single spectacle lens M arek Zając Institute of Physics, Wrocław University of Technology, Wybrzeże Wyspiańskiego 27, 50-370 Wrocław, Poland. Spectacle-wearers make up a considerable part of present-day society, so spectacles are one of the most popular optical instruments — very simple instruments since they are in lact single lenses. On the other hand their mode of operation and the demands for imaging quality are very specific. Therefore, spectacle lenses are interesting objects for aberration analysis and are excellent examples for illustrating purposes while teaching geometrical optics. Typically, the spectacle lens is fixed at some distance in front of the eye. When looking at distant objects, the eye rotates around its centre of rotation while the field-of-view angle is limited practically only by the spectacle frame. The chief ray, connecting point of fixation and centre of eye pupil always passes through the eyeball centre of rotation. Therefore we can assume that spectacle lens has shifted output pupil while preserving a relatively large field of view. Consequently, it is important to correct field aberrations, in particular astigmatism. It is interesting to investigate relationships between spherical aberration, coma and field curvature each as a function of output pupil shift and to point out that it is possible to correct fully astigmatism and minimise spherical aberration or coma 1. Introduction For about 700 years spectacles have been used for correction of such vision defects as myopia, hypermetropia, astigmatism or presbyopia. Except for very few cases, single lenses — mainly of spherical or toroidal surfaces — have been used to this aim.
    [Show full text]
  • Transparent Ceramics Find Wide Use in Optics
    Transparent Ceramics Find Wide Use in Optics Mohan Ramisetty, Suri A. Sastri and Lee Goldman, Surmet Corp. Polycrystalline ceramics with the cubic spinel structure enable multiple defense applications, including night-vision goggles and IR optics for military systems such as domes, lenses, reconnaissance and sensor windows – they also have applications in nonmilitary arenas such as semiconductor processing, oil and gas drilling, medical optics and lasers. Spinel ceramics have been around for a very long time, and ALON – a ceramic based on a composition of aluminum oxynitride with a cubic spinel crystal structure – has been around for over 50 years. However, until the late 1990s or so, the majority of research related to these materials stayed within the laboratories and academia. Commercialization efforts have taken the fast track in the recent 10 years or so. Thanks to growing interest and efforts from the defense and aerospace industries, both ALON and spinel now are commercially available in the US. This is expected to usher in multiple industrial and civilian applications that can benefit from the unique optical and mechanical properties of ALON and spinel. And these transparent ceramic materials have broad appeal to the precision optics community as well. Several factors are driving the commercial development of ALON and spinel ceramics. At the top of the list are their extreme durability, their high-temperature performance and their superior mechanical properties over glasses, as well as their ease of scalability and manufacturability compared with single crystals such as sapphire. Being polycrystalline – as opposed to a single crystal – makes their fabrication into large and complex shapes using a variety of powder processing approaches easier.
    [Show full text]
  • TIE-29: Refractive Index and Dispersion
    DATE April 2005 . PAGE 1/15 TIE-29: Refractive Index and Dispersion 0. Introduction The most important property of optical glass is the refractive index and its dispersion behavior. This technical information gives an overview of the following topics: - Dispersion o Principal dispersion (page 2) o Secondary spectrum (page 3) o Sellmeier dispersion equation (page 4) - Temperature dependence of refractive index (page 6) - Influence of the fine annealing process on the refractive index and Abbe number (page 9) - Tolerances (page 12) - Refractive index measurement (page 13) 1. Refractive Index If light enters a non-absorbing homogeneous materials reflection and refraction occurs at the boundary surface. The refractive index n is given by the ratio of the velocity of light in vacuum c to that of the medium v c n = (1-1) v The refractive index data given in the glass catalogue are measured relative to the refractive index measured in air. The refractive index of air is very close to 1. Practically speaking the refractive index is a measure for the strength of deflection occurring at the boundary surface due to the refraction of the light beam. The equation describing the amount of deflection is called Snell’s law: n1 × sin(a1) = n2 × sin(a 2 ) (1-2) The refractive index is a function of the wavelength. The most common characteristic quantity for characterization of an optical glass is the refractive index n in the middle range of the visible spectrum. This principal refractive index is usually denoted as nd – the refractive index at the wavelength 587.56 nm or in many cases as ne at the wavelength 546.07 nm.
    [Show full text]
  • Optical Glass
    Optical Glass Description of Properties 2011 Optical Glass Description of Properties 2011 2 Table of Contents PART I 4 Mechanical Properties . 36 4.1 Knoop Hardness . 36 Foreword & Overview . 6 4.2 Grindability . 36 1 Optical Properties . 14 4.3 Viscosity . 37 1.1 Refractive Index, Abbe Number, Dispersions, Glass Designations . 14 4.4 Coefficient of Linear Thermal Expansion . 38 1.2 Tolerances for Refractive Index and Abbe Number . 15 5 Thermal Properties . 40 1.3 Test Reports for Refractive Indices and Dispersions . 18 5.1 Thermal Conductivity . 40 1.4 Refractive Index Homogeneity . 19 5.2 Heat Capacity . 40 1.5 Internal Transmittance, Color Code . 21 1.6 Measurement Capabilities for Optical Properties . 23 6 Delivery Quality . 41 6.1 Quality Management and Quality Assurance . 41 2 Internal Properties . 24 6.2 Standard Delivery Quality . 42 2.1 Striae . 24 6.3 Enhanced Delivery Quality . 42 2.2 Bubbles and Inclusions . 25 2.3 Stress Birefringence . 27 7 Forms of Supply and Tolerances . 45 7.1 Raw Glass . 45 3 Chemical Properties . 29 7.2 Cut Blanks . 46 3.1 Climatic Resistance . 29 7.3 Pressings . 52 3.2 Stain Resistance . 30 7.4 Optical Glass Rods . 54 3.3 Acid Resistance . 31 3.4 Alkali and Phosphate Resistance . 33 8 Optical Glasses for Precision Molding . 56 3.5 Identification of Visible Surface Changes . 34 3.6 Environmental Aspects, Hazardous Substances, RoHS . 35 TAble of COnTents 3 9 Product Range of Optical Materials . 58 9.1 Preferred Materials . 58 9.2 Inquiry Glasses . 58 10 Collection of Formulas and Wavelength Table .
    [Show full text]