Index of Refraction: Glass Plates
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Thermal Shock
TEACHER INSTRUCTIONS Thermal Shock Objective: To illustrate thermal expansion and thermal shock. Background Information: In physics, thermal expansion is the tendency of matter to increase in volume or pressure when heated. For liquids and solids, the amount of expansion will normally vary depending on the material’s coefficient of thermal expansion. When materials contract, tensile forces are created. When things expand, compressive forces are created. Thermal shock is the name given to cracking as a result of rapid temperature change. From the laboratory standpoint, there are three main types of glass used today: borosilicate, quartz, and soda lime or flint glass. Borosilicate glass is made to withstand thermal shock better than most other glass through a combination of reduced expansion coefficient and greater strength, though fused quartz outperforms it in both respects. Some glass-ceramic materials include a controlled proportion of material with a negative expansion coefficient, so that the overall coefficient can be reduced to almost exactly zero over a reasonably wide range of temperatures. Improving the shock resistance of glass and ceramics can be achieved by improving the strength of the materials or by reducing its tendency to uneven expansion. One example of success in this area is Pyrex, the brand name that is well known to most consumers as cookware, but which is also used to manufacture laboratory glassware. Pyrex traditionally is made with a borosilicate glass with the addition of boron, which prevents shock by reducing the tendency of glass to expand. Demo description: Three different types of glass rods will be heated so that students can observe the amount of thermal shock that occurs. -
The American Ceramic Society 25Th International Congress On
The American Ceramic Society 25th International Congress on Glass (ICG 2019) ABSTRACT BOOK June 9–14, 2019 Boston, Massachusetts USA Introduction This volume contains abstracts for over 900 presentations during the 2019 Conference on International Commission on Glass Meeting (ICG 2019) in Boston, Massachusetts. The abstracts are reproduced as submitted by authors, a format that provides for longer, more detailed descriptions of papers. The American Ceramic Society accepts no responsibility for the content or quality of the abstract content. Abstracts are arranged by day, then by symposium and session title. An Author Index appears at the back of this book. The Meeting Guide contains locations of sessions with times, titles and authors of papers, but not presentation abstracts. How to Use the Abstract Book Refer to the Table of Contents to determine page numbers on which specific session abstracts begin. At the beginning of each session are headings that list session title, location and session chair. Starting times for presentations and paper numbers precede each paper title. The Author Index lists each author and the page number on which their abstract can be found. Copyright © 2019 The American Ceramic Society (www.ceramics.org). All rights reserved. MEETING REGULATIONS The American Ceramic Society is a nonprofit scientific organization that facilitates whether in print, electronic or other media, including The American Ceramic Society’s the exchange of knowledge meetings and publication of papers for future reference. website. By participating in the conference, you grant The American Ceramic Society The Society owns and retains full right to control its publications and its meetings. -
Chapter 22 Reflection and Refraction of Light
Chapter 22 Reflection and Refraction of Light Problem Solutions 22.1 The total distance the light travels is d2 Dcenter to R Earth R Moon center 2 3.84 108 6.38 10 6 1.76 10 6 m 7.52 10 8 m d 7.52 108 m Therefore, v 3.00 108 m s t 2.51 s 22.2 (a) The energy of a photon is sinc nair n prism 1.00 n prism , where Planck’ s constant is 1.00 8 sinc sin 45 and the speed of light in vacuum is c 3.00 10 m s . If nprism 1.00 1010 m , 6.63 1034 J s 3.00 10 8 m s E 1.99 1015 J 1.00 10-10 m 1 eV (b) E 1.99 1015 J 1.24 10 4 eV 1.602 10-19 J (c) and (d) For the X-rays to be more penetrating, the photons should be more energetic. Since the energy of a photon is directly proportional to the frequency and inversely proportional to the wavelength, the wavelength should decrease , which is the same as saying the frequency should increase . 1 eV 22.3 (a) E hf 6.63 1034 J s 5.00 10 17 Hz 2.07 10 3 eV 1.60 1019 J 355 356 CHAPTER 22 34 8 hc 6.63 10 J s 3.00 10 m s 1 nm (b) E hf 6.63 1019 J 3.00 1029 nm 10 m 1 eV E 6.63 1019 J 4.14 eV 1.60 1019 J c 3.00 108 m s 22.4 (a) 5.50 107 m 0 f 5.45 1014 Hz (b) From Table 22.1 the index of refraction for benzene is n 1.501. -
Negative Refractive Index in Artificial Metamaterials
1 Negative Refractive Index in Artificial Metamaterials A. N. Grigorenko Department of Physics and Astronomy, University of Manchester, Manchester, M13 9PL, UK We discuss optical constants in artificial metamaterials showing negative magnetic permeability and electric permittivity and suggest a simple formula for the refractive index of a general optical medium. Using effective field theory, we calculate effective permeability and the refractive index of nanofabricated media composed of pairs of identical gold nano-pillars with magnetic response in the visible spectrum. PACS: 73.20.Mf, 41.20.Jb, 42.70.Qs 2 The refractive index of an optical medium, n, can be found from the relation n2 = εμ , where ε is medium’s electric permittivity and μ is magnetic permeability.1 There are two branches of the square root producing n of different signs, but only one of these branches is actually permitted by causality.2 It was conventionally assumed that this branch coincides with the principal square root n = εμ .1,3 However, in 1968 Veselago4 suggested that there are materials in which the causal refractive index may be given by another branch of the root n =− εμ . These materials, referred to as left- handed (LHM) or negative index materials, possess unique electromagnetic properties and promise novel optical devices, including a perfect lens.4-6 The interest in LHM moved from theory to practice and attracted a great deal of attention after the first experimental realization of LHM by Smith et al.7, which was based on artificial metallic structures -
Measurement of Verdet Constant in Diamagnetic Glass Using Faraday Effect
18Kasetsart J. (Nat. Sci.) 40 : 18 - 23 (2006) Kasetsart J. (Nat. Sci.) 40(5) Measurement of Verdet Constant in Diamagnetic Glass Using Faraday Effect Kheamrutai Thamaphat, Piyarat Bharmanee and Pichet Limsuwan ABSTRACT Many materials exhibit what is called circular dichroism when placed in an external magnetic field. An equivalent statement would be that the two circular polarizations have different refractive indices in the presence of the field. For linearly polarized light, the plane of polarization rotates as it propagates through the material, a phenomenon that is called the Faraday effect. The angle of rotation is proportional to the product of magnetic field, path length through the sample and a constant known as the Verdet constant. The objectives of this experiment are to measure the Verdet constant for a sample of dense flint glass using Faraday effect and to compare its value to a theoretical calculated value. The experimental values for wavelength of 505 and 525 nm are V = 33.1 and 28.4 rad/T m, respectively. While the theoretical calculated values for wavelength of 505 and 525 nm are V = 33.6 and 30.4 rad/T m, respectively. Key words: verdet constant, diamagnetic glass, faraday effect INTRODUCTION right- and left-handed circularly polarized light are different. This effect manifests itself in a rotation Many important applications of polarized of the plane of polarization of linearly polarized light involve materials that display optical activity. light. This observable fact is called magnetooptic A material is said to be optically active if it rotates effect. the plane of polarization of any light transmitted Magnetooptic effects are those effects in through the material. -
Technical Glasses
Technical Glasses Physical and Technical Properties 2 SCHOTT is an international technology group with 130 years of ex perience in the areas of specialty glasses and materials and advanced technologies. With our highquality products and intelligent solutions, we contribute to our customers’ success and make SCHOTT part of everyone’s life. For 130 years, SCHOTT has been shaping the future of glass technol ogy. The Otto Schott Research Center in Mainz is one of the world’s leading glass research institutions. With our development center in Duryea, Pennsylvania (USA), and technical support centers in Asia, North America and Europe, we are present in close proximity to our customers around the globe. 3 Foreword Apart from its application in optics, glass as a technical ma SCHOTT Technical Glasses offers pertinent information in terial has exerted a formative influence on the development concise form. It contains general information for the deter of important technological fields such as chemistry, pharma mination and evaluation of important glass properties and ceutics, automotive, optics, optoelectronics and information also informs about specific chemical and physical character technology. Traditional areas of technical application for istics and possible applications of the commercial technical glass, such as laboratory apparatuses, flat panel displays and glasses produced by SCHOTT. With this brochure, we hope light sources with their various requirements on chemical to assist scientists, engineers, and designers in making the physical properties, have led to the development of a great appropriate choice and make optimum use of SCHOTT variety of special glass types. Through new fields of appli products. cation, particularly in optoelectronics, this variety of glass types and their modes of application have been continually Users should keep in mind that the curves or sets of curves enhanced, and new forming processes have been devel shown in the diagrams are not based on precision measure oped. -
Chapter 19/ Optical Properties
Chapter 19 /Optical Properties The four notched and transpar- ent rods shown in this photograph demonstrate the phenomenon of photoelasticity. When elastically deformed, the optical properties (e.g., index of refraction) of a photoelastic specimen become anisotropic. Using a special optical system and polarized light, the stress distribution within the speci- men may be deduced from inter- ference fringes that are produced. These fringes within the four photoelastic specimens shown in the photograph indicate how the stress concentration and distribu- tion change with notch geometry for an axial tensile stress. (Photo- graph courtesy of Measurements Group, Inc., Raleigh, North Carolina.) Why Study the Optical Properties of Materials? When materials are exposed to electromagnetic radia- materials, we note that the performance of optical tion, it is sometimes important to be able to predict fibers is increased by introducing a gradual variation and alter their responses. This is possible when we are of the index of refraction (i.e., a graded index) at the familiar with their optical properties, and understand outer surface of the fiber. This is accomplished by the mechanisms responsible for their optical behaviors. the addition of specific impurities in controlled For example, in Section 19.14 on optical fiber concentrations. 766 Learning Objectives After careful study of this chapter you should be able to do the following: 1. Compute the energy of a photon given its fre- 5. Describe the mechanism of photon absorption quency and the value of Planck’s constant. for (a) high-purity insulators and semiconduc- 2. Briefly describe electronic polarization that re- tors, and (b) insulators and semiconductors that sults from electromagnetic radiation-atomic in- contain electrically active defects. -
Super-Resolution Imaging by Dielectric Superlenses: Tio2 Metamaterial Superlens Versus Batio3 Superlens
hv photonics Article Super-Resolution Imaging by Dielectric Superlenses: TiO2 Metamaterial Superlens versus BaTiO3 Superlens Rakesh Dhama, Bing Yan, Cristiano Palego and Zengbo Wang * School of Computer Science and Electronic Engineering, Bangor University, Bangor LL57 1UT, UK; [email protected] (R.D.); [email protected] (B.Y.); [email protected] (C.P.) * Correspondence: [email protected] Abstract: All-dielectric superlens made from micro and nano particles has emerged as a simple yet effective solution to label-free, super-resolution imaging. High-index BaTiO3 Glass (BTG) mi- crospheres are among the most widely used dielectric superlenses today but could potentially be replaced by a new class of TiO2 metamaterial (meta-TiO2) superlens made of TiO2 nanoparticles. In this work, we designed and fabricated TiO2 metamaterial superlens in full-sphere shape for the first time, which resembles BTG microsphere in terms of the physical shape, size, and effective refractive index. Super-resolution imaging performances were compared using the same sample, lighting, and imaging settings. The results show that TiO2 meta-superlens performs consistently better over BTG superlens in terms of imaging contrast, clarity, field of view, and resolution, which was further supported by theoretical simulation. This opens new possibilities in developing more powerful, robust, and reliable super-resolution lens and imaging systems. Keywords: super-resolution imaging; dielectric superlens; label-free imaging; titanium dioxide Citation: Dhama, R.; Yan, B.; Palego, 1. Introduction C.; Wang, Z. Super-Resolution The optical microscope is the most common imaging tool known for its simple de- Imaging by Dielectric Superlenses: sign, low cost, and great flexibility. -
(12) United States Patent (10) Patent No.: US 9.410,246 B2 Winarski (45) Date of Patent: *Aug
USOO941.0246B2 (12) United States Patent (10) Patent No.: US 9.410,246 B2 Winarski (45) Date of Patent: *Aug. 9, 2016 (54) GRAPHENEOPTICFIBER LASER (58) Field of Classification Search CPC .............................. H01S 3/067; G02B6/0229 (71) Applicant: Tyson York Winarski, Mountain View, See application file for complete search history. CA (US)(US (56) References Cited (72) Inventor: feYork Winarski, Mountain View, U.S. PATENT DOCUMENTS - 2007/0030558 A1* 2, 2007 Martinelli ........ HO4B 10,25133 (*) Notice: Subject to any disclaimer, the term of this 359,334 patent is extended or adjusted under 35 2011/0222562 A1* 9/2011 Jiang ....................... HO1S 3,067 U.S.C. 154(b) by 0 days. 372/6 2011/0285999 A1* 11/2011 Kim ..................... GO1N 21,552 This patent is Subject to a terminal dis- 356,445 claimer. 2012/0039344 A1 2/2012 Kian ....................... HO1S 3,067 372/6 (21) Appl. No.: 14/710,592 2014/0341238 A1*ck 1 1/2014 Kitabayashi .......... HO1S 39. (22) Filed: May 13, 2015 OTHER PUBLICATIONS O O Ariel Ismach, Clara Druzgalski, Samuel Penwell, Adam (65) Prior Publication Data Schwartzberg, Maxwell Zheng, Ali Javey, Jeffrey Bokor, and US 2015/O255945A1 Sep. 10, 2015 Yuegang Zhang, Direct Chemical Vapor Deposition of Graphene on Dielectric Surfaces, Nano Lett. 2010, 10, 1542-1548, American Chemical Society, Apr. 2, 2010. Related U.S. Application Data Rui Wang, Yufeng Hao, Ziqian Wang, Hao Gong, and John T. L. Thong in Large-Diameter Graphene Nanotubes Synthesized Using (63) Continuation-in-part of application No. 14/070,574, Ni Nanowire Templates, Nano Lett. 2010, 10, 4844-4850, American filed on Nov. -
Design and Fabrication of Nonconventional Optical Components by Precision Glass Molding
Design and Fabrication of Nonconventional Optical Components by Precision Glass Molding DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of the Ohio State University By Peng He Graduate Program in Industrial and Systems Engineering The Ohio State University 2014 Dissertation Committee: Dr. Allen Y. Yi, Advisor Dr. Jose M. Castro Dr. L. James Lee Copyright by Peng He 2014 Abstract Precision glass molding is a net-shaping process to fabricate glass optics by replicating optical features from precision molds to glass at elevated temperature. The advantages of precision glass molding over traditional glass lens fabrication methods make it especially suitable for the production of optical components with complicated geometries, such as aspherical lenses, diffractive hybrid lenses, microlens arrays, etc. Despite of these advantages, a number of problems must be solved before this process can be used in industrial applications. The primary goal of this research is to determine the feasibility and performance of nonconventional optical components formed by precision glass molding. This research aimed to investigate glass molding by combing experiments and finite element method (FEM) based numerical simulations. The first step was to develop an integrated compensation solution for both surface deviation and refractive index drop of glass optics. An FEM simulation based on Tool-Narayanaswamy-Moynihan (TNM) model was applied to predict index drop of the molded optical glass. The predicted index value was then used to compensate for the optical design of the lens. Using commercially available general purpose software, ABAQUS, the entire process of glass molding was simulated to calculate the surface deviation from the adjusted lens geometry, which was applied to final mold shape modification. -
High-Precision Micro-Machining of Glass for Mass-Personalization and Submitted in Partial Fulfillment of the Requirements for the Degree Of
High-precision micro-machining of glass for mass-personalization Lucas Abia Hof A Thesis In the Department of Mechanical, Industrial and Aerospace Engineering Presented in Partial Fulfillment of the Requirements For the Degree of Doctor of Philosophy (Mechanical Engineering) at Concordia University Montreal, Québec, Canada June 2018 © Lucas Abia Hof, 2018 CONCORDIA UNIVERSITY School of Graduate Studies This is to certify that the thesis prepared By: Lucas Abia Hof Entitled: High-precision micro-machining of glass for mass-personalization and submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Mechanical Engineering) complies with the regulations of the University and meets the accepted standards with respect to originality and quality. Signed by the final examining committee: ______________________________________ Chair Dr. K. Schmitt ______________________________________ External Examiner Dr. P. Koshy ______________________________________ External to Program Dr. M. Nokken ______________________________________ Examiner Dr. C. Moreau ______________________________________ Examiner Dr. R. Sedaghati ______________________________________ Thesis Supervisor Dr. R. Wüthrich Approved by: ___________________________________________________ Dr. A. Dolatabadi, Graduate Program Director August 14, 2018 __________________________________________________ Dr. A. Asif, Dean Faculty of Engineering and Computer Science Abstract High-precision micro-machining of glass for mass- personalization Lucas Abia Hof, -
Appendix a Definitions and Symbols
Appendix A Definitions and Symbols A.1 Symbols and Conversion Factors A absorptivity a distance aperture b net increase in number of molecules per formula unit; b = μ − 1 C constant C Euler’s constant; C = 0.577 Cp heat capacity c speed of light; c = 2.998 ×1010 cm/s cp specific heat at constant pressure [J/gK, J/molK] cv specific heat at constant volume [J/gK, J/molK] D heat diffusivity [cm2/s] transmittivity 2 Di molecular diffusion coefficient of species i [cm /s] d lateral width of laser-processed features [μm, cm] diameter E electric field [V/cm] energy [J] −2 kBT (T = 273.15 K) = 2.354 ×10 eV 1 kcal/mol =# 0.043 eV =# 5.035 ×102 K 1eV=# 1.1604 ×104 K =# 1.602 ×10−19 J 1 kcal =# 4.187 ×103 J 1cm−1 =# 1.24 ×10−4 eV =# 1.439 K 1J=# 2.39 ×10−4 kcal EF Fermi energy E activation temperature [K]; E = E/kB E ∗ normalized activation temperature; E ∗ = E /T (∞) E activation energy [eV; kcal/mol] Em activation energy for melting Ev activation energy for vaporization at Tb D. Bäuerle, Laser Processing and Chemistry, 4th ed., 739 DOI 10.1007/978-3-642-17613-5, C Springer-Verlag Berlin Heidelberg 2011 740 Appendix A Eg bandgap energy = energy distance between (lowest) conduction and (highest) valence bands E laser-pulse energy [J] e elementary charge; e = 1.602 ×10−19 C ee≈ 2.718 eV electron Volt 1eV/particle = 23.04 kcal/mol F area Faraday constant; F = 96485 C/mol f focal length [cm] Gr Grashof number G Gibbs free energy g acceleration due to gravity gT temperature discontinuity coefficient H total enthalpy [J/cm3,J/g, J/mol] reaction enthalpy H a