Light-Emitting Diodes in the Solid-State Lighting Systems
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Fundamentals of Microelectronics Chapter 3 Diode Circuits
9/17/2010 Fundamentals of Microelectronics CH1 Why Microelectronics? CH2 Basic Physics of Semiconductors CH3 Diode Circuits CH4 Physics of Bipolar Transistors CH5 Bipolar Amplifiers CH6 Physics of MOS Transistors CH7 CMOS Amplifiers CH8 Operational Amplifier As A Black Box 1 Chapter 3 Diode Circuits 3.1 Ideal Diode 3.2 PN Junction as a Diode 3.3 Applications of Diodes 2 1 9/17/2010 Diode Circuits After we have studied in detail the physics of a diode, it is time to study its behavior as a circuit element and its many applications. CH3 Diode Circuits 3 Diode’s Application: Cell Phone Charger An important application of diode is chargers. Diode acts as the black box (after transformer) that passes only the positive half of the stepped-down sinusoid. CH3 Diode Circuits 4 2 9/17/2010 Diode’s Action in The Black Box (Ideal Diode) The diode behaves as a short circuit during the positive half cycle (voltage across it tends to exceed zero), and an open circuit during the negative half cycle (voltage across it is less than zero). CH3 Diode Circuits 5 Ideal Diode In an ideal diode, if the voltage across it tends to exceed zero, current flows. It is analogous to a water pipe that allows water to flow in only one direction. CH3 Diode Circuits 6 3 9/17/2010 Diodes in Series Diodes cannot be connected in series randomly. For the circuits above, only a) can conduct current from A to C. CH3 Diode Circuits 7 IV Characteristics of an Ideal Diode V V R = 0⇒ I = = ∞ R = ∞⇒ I = = 0 R R If the voltage across anode and cathode is greater than zero, the resistance of an ideal diode is zero and current becomes infinite. -
Compact Fluorescent Light Bulbs
Compact Fluorescent Light Bulbs What is a compact fluorescent lamp (CFL) bulb? A CFL bulb is a type of fluorescent bulb that screws into a standard light socket, such as a lamp or ceiling light fixture. CFLs use much less energy and last up to 10 times longer than standard light bulbs. What is in a compact fluorescent lamp (CFL) bulb? A CFL bulb is made of glass, a ceramic and metal base, a luminous powder called phosphor, and a small amount of mercury. How much mercury is contained in a CFL bulb? Manufacturers report that the amount of mercury contained in a CFL bulb is five milligrams, which is less than two ten-thousandths of an ounce. The mercury could be in the form of an invisible vapor or in a bead the size of the period at the end of this sentence. A mercury fever thermometer contains about 100 times more mercury than a CFL bulb. Is it harmful is it to be in the room where a CFL bulb has broken? The amount of mercury vapor that is released from one broken bulb is not enough to make anyone sick. However, it is best to avoid any exposure to mercury. We recommend that you ventilate the room air to the outdoors by opening a window or a door and leave the room for a few hours before cleaning up the broken bulb. How should I clean up a broken CFL bulb? It is not necessary to hire a professional to clean up the bulb. By following the directions below, you can safely clean up a broken CFL bulb. -
M7 Electroluminescence of Polymers
Universität Potsdam Institute of Physics and Astronomy Advanced Physics Lab Course March 2020 M7 ELECTROLUMINESCENCE OF POLYMERS I. INTRODUCTION The recombination of holes and electrons in a luminescent material can produce light. This emitted light is referred to as electroluminescence (EL) and was discovered in organic single crystals by Pope, Magnante, and Kallmann in 1963.[1] EL from conjugated polymers was first reported by Burroughes et al.[2] The polymer used was poly(p-phenylenevinylene) (PPV). Since then, a variety of other polymers has been investigated. Organic EL devices have applications in a wide field ranging from multi-color displays and optical information processing to lighting. Polymers have the advantage over inorganic and monomolecular materials in the ease with which thin, structurally robust and large area films can be perpared from solutions. Using printing techniques, patterned structures can be produced easily. Even flexible displays can be produced because of the good mechanical properties of polymers. In this lab course, basic optical and electrical properties of conjugated polymers will be investigated. Advanced Lab Course: Electroluminescence of Polymers 2 EXPERIMENTAL TASKS Measure the absorption spectra of your polymers (thin films spin coated onto glass substrates). Characterize the setup used for luminescence measurements. Identify possible sources of error and collect data necessary for their correction. Measure the photoluminescence emission spectra for the polymer films, using suitable excitation wavelengths. Measure the photoluminescence excitation spectra for the polymer films, using suitable detection wavelengths. Measure the current through the OLEDs and the spectral radiant intensity of electroluminescence as a function of applied voltage (the current-radiance-voltage characteristics). -
Wide Band Gap Materials: Revolution in Automotive Power Electronics
20169052 16mm Wide Band Gap Materials: Revolution in Automotive Power Electronics Luca Bartolomeo 1) Luigi Abbatelli 2) Michele Macauda 2) Filippo Di Giovanni 2) Giuseppe Catalisano 2) Miroslav Ryzek 3) Daniel Kohout 3) 1) STMicroelectronics Japan, Shinagawa INTERCITY Tower A, 2-15-1, Konan, Minato-ku, 108-6017 Tokyo, Japan (E-mail: [email protected]) 2) STMicroelectronics , Italy 3) STMicroelectronics , Czech Republic ④④④ ④④④ Presented at the EVTeC and APE Japan on May 26, 2016 ABSTRACT : The number of Electric and Hybrid vehicles on the roads is increasing year over year. The role of power electronics is of paramount importance to improve their efficiency, keeping lighter and smaller systems. In this paper, the authors will specifically cover the use of Wide Band Gap (WBG) materials in Electric and Hybrid vehicles. It will be shown how SiC MOSFETs bring significant benefits compared to standard IGBTs silicon technology, in both efficiency and form factor. Comparison of the main electrical characteristics, between SiC-based and IGBT module, were simulated and validated by experimental tests in a real automotive environment. KEY WORDS : SiC, Wide Band Gap, IGBT, Power Module 1. INTRODUCTION When considering power transistors in the high voltage range Nowadays, an increased efficiency demand is required in (above 600V), SiC MOSFETs are an excellent alternative to the power electronics applications to have lighter and smaller standard silicon devices: they guarantee lower RON*Area values systems and to improve the range of new Electric (EV) and compared to the latest silicon-based Super-Junction MOSFETs, Hybrid vehicles (HEV). There is an on-going revolution in the especially in high temperature environment (1). -
Induction in Alocasia Macrorrhiza' Received for Publication December 8, 1987 and in Revised Form March 18, 1988
Plant Physiol. (1988) 87, 818-821 0032-0889/88/87/081 8/04/$0 1.00/0 Gas Exchange Analysis of the Fast Phase of Photosynthetic Induction in Alocasia macrorrhiza' Received for publication December 8, 1987 and in revised form March 18, 1988 MIKO U. F. KIRSCHBAUM2 AND ROBERT W. PEARCY* Department ofBotany, University ofCalifornia, Davis, California 95616 ABSTRACT and Pearcy (10) used gas exchange techniques to investigate the slow phase of induction from about 1 to 45 min. These studies When leaves ofAlocasia macrorrhiza that had been preconditioned in indicated that there might also be a fast phase of induction that 10 micromoles photons per square meter per second for at least 2 hours is complete within the first minute after an increase in PFD. This were suddenly exposed to 500 micromoles photons per square meter per fast induction phase is difficult to analyze with gas exchange second, there was an almost instantaneous increase in assimilation rate. techniques because instrument response times are typically so After this initial increase, there was a secondary increase over the next slow as to obscure the underlying plant response. In the present minute. This secondary increase was more pronounced in high CO2 (1400 study, measurements of the induction response were made in a microbars), where assimilation rate was assumed to be limited by the gas-exchange system modified to resolve very fast responses. This rate of regeneration of ribulose 1,5-bisphosphate (RuBP). It was absent investigation of the fast induction phase extends our work done in low CO2 (75 microbars), where RuBP carboxylase/oxygenase (Rub- previously on the dynamics of photosynthesis of the Australian isco) was assumed to be limiting. -
Modelling Transitions in Consumer Lighting — Consequences of the E.U
Modelling Transitions in Consumer Lighting — Consequences of the E.U. ban on light bulbs Maarten Afman Energy & Industry section Infrastructure Systems & Services Faculty of Technology, Policy and Management Delft University of Technology Modelling Transitions in Consumer Lighting — Consequences of the E.U. ban on light bulbs M.Sc. Thesis ‘Final version d.d. 4th February 2010’ Maarten Afman Graduation committee: Prof.dr.ir. M.P.C. Weijnen (chair; TU Delft, Energy & Industry section ) Dr.ir. G.P.J. Dijkema (first supervisor; TU Delft, Energy & Industry section) Dr.ir. C. van Daalen (second supervisor; TU Delft, Policy Analysis section) ir. E.J.L. Chappin (daily supervisor; TU Delft, Energy & Industry section) dr. W. Jager (external supervisor; University of Groningen, Marketing department) Programme SEPAM – Systems Engineering, Policy Analysis and Management Graduation Delft, 18th February 2010 Address M.R. Afman, v.d. Heimstr. 55, 2613EA Delft, The Netherlands E-mail addr. [email protected] Student no. 9006424 Energy & Industry section Infrastructure Systems & Services Faculty of Technology, Policy and Management Delft University of Technology Summary The need for a ban on bulbs? Energy consumption of the residential lighting sector is high: 3.8 TWh per year for the Netherlands alone, approximately the production of a power plant of 800 MW. Consequently, if 40% of the energy consumption for consumer lighting could be saved, a 320 MW power plant could be taken off the grid. Such a saving would be realistic if consumers would not rely so much on outdated and inefficient lighting technology, i.e. the standard incandescent light bulb and halogen lighting. -
Comparison of Life-Cycle Analyses of Compact Fluorescent and Incandescent Lamps Based on Rated Life of Compact Fluorescent Lamp
Comparison of Life-Cycle Analyses of Compact Fluorescent and Incandescent Lamps Based on Rated Life of Compact Fluorescent Lamp Laurie Ramroth Rocky Mountain Institute February 2008 Image: Compact Fluorescent Lamp. From Mark Stozier on istockphoto. Abstract This paper addresses the debate over compact fluorescent lamps (CFLs) and incandescents through life-cycle analyses (LCA) conducted in the SimaPro1 life-cycle analysis program. It compares the environmental impacts of providing a given amount of light (approximately 1,600 lumens) from incandescents and CFLs for 10,000 hours. Special attention has been paid to recently raised concerns regarding CFLs—specifically that their complex manufacturing process uses so much energy that it outweighs the benefits of using CFLs, that turning CFLs on and off frequently eliminates their energy-efficiency benefits, and that they contain a large amount of mercury. The research shows that the efficiency benefits compensate for the added complexity in manufacturing, that while rapid on-off cycling of the lamp does reduce the environmental (and payback) benefits of CFLs they remain a net “win,” and that the mercury emitted over a CFL’s life—by power plants to power the CFL and by leakage on disposal—is still less than the mercury that can be attributed to powering the incandescent. RMI: Life Cycle of CFL and Incandescent 2 Heading Page Introduction................................................................................................................... 5 Background................................................................................................................... -
CATHODE LIGHT STRIP Single-Lamp Modular Cold Cathode Fluorescent Fixture • Model CLS
CATHODE LIGHT STRIP Single-Lamp Modular Cold Cathode Fluorescent Fixture • Model CLS U.S. and international patents pending. Conference Room, Anadarko Petroleum Photo: Eric Long Washington, DC Architect: Davis Carter Scott © 2002 Cathode Lighting Systems Inc. 8020 Queenair Drive, Gaithersburg, MD 20879 • ph: 301 921 4120 • fax: 301 963 3050 e-mail: [email protected] • website: www.CathodeLightingSystems.com INALLY, THE LOOK OF A CUSTOM COLD CATHODE INSTALLATION IN AN OFF- FTHE-SHELF MODULAR SYSTEM. OUR ARCHITECTURAL-GRADE COLD CATHODE FIXTURE MAKES DESIGNING SEAMLESS SPECIAL EFFECTS LIGHTING EASIER THAN EVER. LAMPS ARE ILLUMINATED FROM END TO END, CREATING TRUE SHADOWLESS LINEAR FLUORESCENT LIGHT. STANDARD INTEGRAL DIMMING BALLASTS, SIMPLE INSTALLATION, AND A LAMP LIFE OF 50,000 HOURS MAKE CATHODE LIGHT STRIP THE CLEAR CHOICE WHEN THE HIGHEST-QUALITY LONG-LIFE LIGHTING EFFECTS ARE REQUIRED. CATHODE LIGHT STRIP, PERFECT ELEGANCE WAS NEVER SO EASY. Model CLS-4 shown equipped with a warm white (30TC) lamp. FEATURES: • SEAMLESS ILLUMINATION: Lamp illumination is • DIMMABLE: Fixtures are supplied standard with integral complete, from end to end, with no dark spots or socket dimmable ballasts. shadow. • ALL FIXTURES DIM AT THE SAME RATE: Cathode Light • ULTRA-LONG LAMP LIFE: The cold cathode lamp has Strip has been engineered to dim evenly from fixture to a life of 50,000 hours +. fixture, regardless of length or combinations of differing • LOW PROFILE: Just 2 5/8" wide and 3 1/2" tall, much lengths. smaller than traditional custom cold cathode. • STREAMLINED AND LIGHTWEIGHT: Fixtures are • AVAILABLE IN A VARIETY OF LENGTHS: With eight made from satin anodized architectural-grade, snap-fit standard sizes available, fixtures can be combined or aluminum extrusion. -
Vacuum Tube Theory, a Basics Tutorial – Page 1
Vacuum Tube Theory, a Basics Tutorial – Page 1 Vacuum Tubes or Thermionic Valves come in many forms including the Diode, Triode, Tetrode, Pentode, Heptode and many more. These tubes have been manufactured by the millions in years gone by and even today the basic technology finds applications in today's electronics scene. It was the vacuum tube that first opened the way to what we know as electronics today, enabling first rectifiers and then active devices to be made and used. Although Vacuum Tube technology may appear to be dated in the highly semiconductor orientated electronics industry, many Vacuum Tubes are still used today in applications ranging from vintage wireless sets to high power radio transmitters. Until recently the most widely used thermionic device was the Cathode Ray Tube that was still manufactured by the million for use in television sets, computer monitors, oscilloscopes and a variety of other electronic equipment. Concept of thermionic emission Thermionic basics The simplest form of vacuum tube is the Diode. It is ideal to use this as the first building block for explanations of the technology. It consists of two electrodes - a Cathode and an Anode held within an evacuated glass bulb, connections being made to them through the glass envelope. If a Cathode is heated, it is found that electrons from the Cathode become increasingly active and as the temperature increases they can actually leave the Cathode and enter the surrounding space. When an electron leaves the Cathode it leaves behind a positive charge, equal but opposite to that of the electron. In fact there are many millions of electrons leaving the Cathode. -
Indoor Lighting Design Guide
CSU Office of the Chancellor Indoor Lighting Design Guide Indoor Lighting Design Guide Rev: 12/12/18 CSU Office of the Chancellor Indoor Lighting Design Guide ACKNOWLEDGEMENT The California State University (CSU) gratefully acknowledges the effort and work of Jai Agaram, John Andary, Douglas Effenberger, Kent Peterson, Steven Strauss, and Steve Taylor. Comments or inquiries may be directed to: The California State University Office of the Chancellor Capital Planning Design and Construction Long Beach, California Attention: Thomas Kennedy, Chief Architecture and Engineering Telephone: (562) 951-4129 E-mail: [email protected] CSU Office of the Chancellor Indoor Lighting Design Guide TABLE OF CONTENTS EXECUTIVE SUMMARY .......................................................................................................................................................... 1 SECTION 1: INTRODUCTION ............................................................................................................................................ 2 CSU POLICY .................................................................................................................................................................................. 2 DEFINITIONS .................................................................................................................................................................................. 2 UTILITY INCENTIVES ....................................................................................................................................................................... -
Fluorescent Lighting About the Guide
RESPONSIBLE PURCHASING GUIDE fluorescent lighting About the Guide The Responsible Purchasing Guide for Lighting is published by the Responsible Purchasing Network in print, as a PDF file, and on the web. Print and PDF copies are available to the public for purchase. The online edi- tion includes additional resources available to members of the Responsible Purchasing Network, including: searchable product listings, multiple policy and specification samples, comparisons of standards, and related documents. Visit www.ResponsiblePurchasing.org to purchase a copy or to access the members-only web- based edition of the Guide. Responsible Purchasing Network © 2007 About the Responsible Purchasing Network The Responsible Purchasing Network (RPN) was founded in 2005 as the first national network of procurement-related professionals dedicated to socially and environmentally responsible purchasing. RPN is a program of the Center for a New American Dream (www.newdream.org) and guided by a volunteer Steering Committee of leading procurement stakeholders from government, industry, educational institutions, standards setting organizations, and non-profit advocacy organizations. Acknowledgements The Responsible Purchasing Network (RPN) would like to thank the following people for assisting with the development of this Guide. Their expertise helped to ensure quality and accuracy, though RPN alone accepts responsibility for any errors or omissions. Affiliations listed below were current when input was provided to RPN and are listed for identification purposes -
Towards Direct-Gap Silicon Phases by the Inverse Band Structure Design Approach
Towards Direct-Gap Silicon Phases by the Inverse Band Structure Design Approach H. J. Xiang1,2*, Bing Huang2, Erjun Kan3, Su-Huai Wei2, X. G. Gong1 1 Key Laboratory of Computational Physical Sciences (Ministry of Education), State Key Laboratory of Surface Physics, and Department of Physics, Fudan University, Shanghai 200433, P. R. China 2National Renewable Energy Laboratory, Golden, Colorado 80401, USA 3Department of Applied Physics, Nanjing University of Science and Technology, Nanjing, Jiangsu 210094, People’s Republic of China e-mail: [email protected] Abstract Diamond silicon (Si) is the leading material in current solar cell market. However, diamond Si is an indirect band gap semiconductor with a large energy difference (2.4 eV) between the direct gap and the indirect gap, which makes it an inefficient absorber of light. In this work, we develop a novel inverse-band structure design approach based on the particle swarming optimization algorithm to predict the metastable Si phases with better optical properties than diamond Si. Using our new method, we predict a cubic Si20 phase with quasi- direct gaps of 1.55 eV, which is a promising candidate for making thin-film solar cells. PACS: 71.20.-b,42.79.Ek,78.20.Ci,88.40.jj 1 Due to the high stability, high abundance, and the existence of an excellent compatible oxide (SiO2), Si is the leading material of microelectronic devices. Currently, the majority of solar cells fabricated to date have also been based on diamond Si in monocrystalline or large- grained polycrystalline form [1]. There are mainly two reasons for this: First, Si is the second most abundant element in the earth's crust; Second, the Si based photovoltaics (PV) industry could benefit from the successful Si based microelectronics industry.