Electrical Discharge Light Sources : a Challenge for the Future
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Article Soot Photometer Using Supervised Machine Learning
Atmos. Meas. Tech., 12, 3885–3906, 2019 https://doi.org/10.5194/amt-12-3885-2019 © Author(s) 2019. This work is distributed under the Creative Commons Attribution 4.0 License. Classification of iron oxide aerosols by a single particle soot photometer using supervised machine learning Kara D. Lamb1,2 1Cooperative Institute for Research in Environmental Sciences, University of Colorado Boulder, Boulder, CO, USA 2NOAA Earth System Research Laboratory Chemical Sciences Division, Boulder, CO, USA Correspondence: Kara D. Lamb ([email protected]) Received: 15 March 2019 – Discussion started: 22 March 2019 Revised: 20 June 2019 – Accepted: 21 June 2019 – Published: 15 July 2019 Abstract. Single particle soot photometers (SP2) use laser- each class are compared with the true class for those particles induced incandescence to detect aerosols on a single particle to estimate generalization performance. While the specific basis. SP2s that have been modified to provide greater spec- class approach performed well for rBC and Fe3O4 (≥ 99 % tral contrast between their narrow and broad-band incandes- of these aerosols are correctly identified), its classification of cent detectors have previously been used to characterize both other aerosol types is significantly worse (only 47 %–66 % refractory black carbon (rBC) and light-absorbing metallic of other particles are correctly identified). Using the broader aerosols, including iron oxides (FeOx). However, single par- class approach, we find a classification accuracy of 99 % for ticles cannot be unambiguously identified from their incan- FeOx samples measured in the laboratory. The method al- descent peak height (a function of particle mass) and color lows for classification of FeOx as anthropogenic or dust-like ratio (a measure of blackbody temperature) alone. -
The Ball Lightning Conundrum
most famous deadis due to ball lightning occun-ed in 1752 or 1753, when die Swedish sci entist Professor Georg Wilhelm Richman was The Ball attempting to repeat Benjamin Franklin's observa dons with a lightning rcxl. An eyewitness report ed that when Richman w;is "a foot away from the iron rod, the] looked at die elecuical indicator Lightning again; just then a palish blue ball of fire, ;LS big as a fist, came out of die rod without any contaa whatst:)ever. It went right to the forehead of die Conundrum professor , who in diat instant fell back without uttering a sound."' Somedmes a luminous globe is said to rapidly descend 6own die path of a linear lightning WILLIAM D STANSFIELD strike and stop near the ground at die impact site. It may dien hover motionless in mid-air or THE EXISTENCE OF BALL UGHTNING HAS move randomly, but most often horizontally, at been questioned for hundreds of years. Today, die relatively slow velocities of walking speed. the phenomenon is a realit>' accepted by most Sometimes it touches or bounces along or near scientists, but how it is foniied and maintiiined the ground, or travels inside buildings, along has yet to be tully explained. Uncritical observers walls, or over floors before being extingui.shed. of a wide variety of glowing atmospheric entities Some balls have been observed to travel along may be prone to call tliem bail lightning. Open- power lines or fences. Wind does not .seem to minded skepdas might wish to delay judgment have any influence on how diese balls move. -
Introduction 1
1 1 Introduction . ex arte calcinati, et illuminato aeri [ . properly calcinated, and illuminated seu solis radiis, seu fl ammae either by sunlight or fl ames, they conceive fulgoribus expositi, lucem inde sine light from themselves without heat; . ] calore concipiunt in sese; . Licetus, 1640 (about the Bologna stone) 1.1 What Is Luminescence? The word luminescence, which comes from the Latin (lumen = light) was fi rst introduced as luminescenz by the physicist and science historian Eilhardt Wiede- mann in 1888, to describe “ all those phenomena of light which are not solely conditioned by the rise in temperature,” as opposed to incandescence. Lumines- cence is often considered as cold light whereas incandescence is hot light. Luminescence is more precisely defi ned as follows: spontaneous emission of radia- tion from an electronically excited species or from a vibrationally excited species not in thermal equilibrium with its environment. 1) The various types of lumines- cence are classifi ed according to the mode of excitation (see Table 1.1 ). Luminescent compounds can be of very different kinds: • Organic compounds : aromatic hydrocarbons (naphthalene, anthracene, phenan- threne, pyrene, perylene, porphyrins, phtalocyanins, etc.) and derivatives, dyes (fl uorescein, rhodamines, coumarins, oxazines), polyenes, diphenylpolyenes, some amino acids (tryptophan, tyrosine, phenylalanine), etc. + 3 + 3 + • Inorganic compounds : uranyl ion (UO 2 ), lanthanide ions (e.g., Eu , Tb ), doped glasses (e.g., with Nd, Mn, Ce, Sn, Cu, Ag), crystals (ZnS, CdS, ZnSe, CdSe, 3 + GaS, GaP, Al 2 O3 /Cr (ruby)), semiconductor nanocrystals (e.g., CdSe), metal clusters, carbon nanotubes and some fullerenes, etc. 1) Braslavsky , S. et al . ( 2007 ) Glossary of terms used in photochemistry , Pure Appl. -
2. Making Fires Burn Or Go out 1: Introduction to the Fire Triangle
2. Making Fires Burn or Go Out 1: Introduction to the Fire Triangle Lesson Overview: In this activity, students describe and organize what they already know Subjects: Science, Mathematics, Writing, about fire so it fits into the conceptual model of Speaking and Listening, Health and the Fire Triangle. They examine the geometric Safety stability of a triangle and how that property Duration: one half-hour session applies to fire. Group size: Whole class. Students work in groups of 2-3. Lesson Goal: Increase students’ understanding of Setting: Indoors how fires burn and why they go out. Vocabulary: Fire Triangle, fuel, heat, ignition, oxygen, model Objectives: • Students can construct a triangle out of toothpicks and gumdrops, and can label its legs with the three components of the Fire Triangle. • Students can demonstrate that removing one side of the triangle makes it collapse. • Students can identify the component(s) of the Fire Triangle that are removed in various scenarios, and explain how this makes the fire go out. Standards: 1st 2nd 3rd 4th 5th CCSS Writing 2, 7, 8 2, 7, 8 2, 7, 10 2,7, 9, 10 2,7, 9, 10 Speaking/Listening 1, 2, 4, 6 1, 2, 4, 6 1, 2, 4, 6 1, 2, 4, 6 1, 2, 4, 6 1, 2, 3, 4, Language 1, 2, 4, 6 1, 2, 4, 6 6 1, 2, 3, 4, 6 1, 2, 3, 4, 6 MP.4, MP.4, MP.4, MP.4, Math MP.5 MP.5, MP.5 MP.5 MP.4, MP.5 Matter and Its PS1.A, NGSS Interactions PS1.B PS1.B From Molecules to Organisms: Structure/Processes LS1.C Engineering Design ETS1.B ETS1.B EEEGL Strand 1 A, B, C, E, F, G A, B, C, E, F, G Teacher Background: This activity explores the chemistry of combustion as described by a conceptual model called the Fire Triangle. -
Energy Efficiency Lighting Hearing Committee On
S. HRG. 110–195 ENERGY EFFICIENCY LIGHTING HEARING BEFORE THE COMMITTEE ON ENERGY AND NATURAL RESOURCES UNITED STATES SENATE ONE HUNDRED TENTH CONGRESS FIRST SESSION TO RECEIVE TESTIMONY ON THE STATUS OF ENERGY EFFICIENT LIGHT- ING TECHNOLOGIES AND ON S. 2017, THE ENERGY EFFICIENT LIGHT- ING FOR A BRIGHTER TOMORROW ACT SEPTEMBER 12, 2007 ( Printed for the use of the Committee on Energy and Natural Resources U.S. GOVERNMENT PRINTING OFFICE 39–385 PDF WASHINGTON : 2007 For sale by the Superintendent of Documents, U.S. Government Printing Office Internet: bookstore.gpo.gov Phone: toll free (866) 512–1800; DC area (202) 512–1800 Fax: (202) 512–2104 Mail: Stop IDCC, Washington, DC 20402–0001 VerDate 0ct 09 2002 11:58 Feb 20, 2008 Jkt 040443 PO 00000 Frm 00001 Fmt 5011 Sfmt 5011 G:\DOCS\39385.XXX SENERGY2 PsN: MONICA COMMITTEE ON ENERGY AND NATURAL RESOURCES JEFF BINGAMAN, New Mexico, Chairman DANIEL K. AKAKA, Hawaii PETE V. DOMENICI, New Mexico BYRON L. DORGAN, North Dakota LARRY E. CRAIG, Idaho RON WYDEN, Oregon LISA MURKOWSKI, Alaska TIM JOHNSON, South Dakota RICHARD BURR, North Carolina MARY L. LANDRIEU, Louisiana JIM DEMINT, South Carolina MARIA CANTWELL, Washington BOB CORKER, Tennessee KEN SALAZAR, Colorado JOHN BARRASSO, Wyoming ROBERT MENENDEZ, New Jersey JEFF SESSIONS, Alabama BLANCHE L. LINCOLN, Arkansas GORDON H. SMITH, Oregon BERNARD SANDERS, Vermont JIM BUNNING, Kentucky JON TESTER, Montana MEL MARTINEZ, Florida ROBERT M. SIMON, Staff Director SAM E. FOWLER, Chief Counsel FRANK MACCHIAROLA, Republican Staff Director JUDITH K. PENSABENE, Republican Chief Counsel (II) VerDate 0ct 09 2002 11:58 Feb 20, 2008 Jkt 040443 PO 00000 Frm 00002 Fmt 5904 Sfmt 5904 G:\DOCS\39385.XXX SENERGY2 PsN: MONICA C O N T E N T S STATEMENTS Page Bingaman, Hon. -
THE ELECTRIC DISCHARGE EXPERIMENTS a Theorist’S Exploration of First Laboratory Plasmas I
THE ELECTRIC DISCHARGE EXPERIMENTS A Theorist’s Exploration of First Laboratory Plasmas I. INTRODUCTION • Who? • Experimentalists interested in electrical properties of matter • What? • Experiments with electromagnetic fields in low-pressure Gases • Where? • Germany and Britain • When? • Late nineteenth / Early twentieth centuries • Why? • Unify classical theories for light and matter • kinetic theory, electromagnetic theory • “The study of the electrical properties of gases seems to offer the most promising field for investigatinG the Nature of Electricity and Matter, for thanks to the Kinetic Theory of Gases our idea of non-electric processes in gases is much more vivid than they are for liquids or solids”– JJ Thomson [Thomson, 1896] II. RESULTS • Failure to unify classical theories for light and matter • Evidence of complex electromagnetic interactions between light and matter at the sub-atomic level • Experimental basis for Modern Era of Physics • "a New Era has beGun in Physics, in which the electrical properties of gases have played and will play a most important part.“ JJ Thomson [Thomson, 1896] III. DISCHARGE TUBE • DischarGe Tube • Weakly-Conducting Exterior Solid • Weakly-Conducting Interior Gas (WCG) • Strongly-Conducting Interior Gas (SCG) • Applied Interior Pressure (P) • Electrodes (Cathode and Anode) • Model as Ideal Capacitor with Dielectric (D) • Applied Potential Difference (V) • Applied Electric Field (E) • Particle Drifts • Electric field transfers energy to charged particles • Particles scatter in the Gas interior -
Biofluorescence
Things That Glow In The Dark Classroom Activities That Explore Spectra and Fluorescence Linda Shore [email protected] “Hot Topics: Research Revelations from the Biotech Revolution” Saturday, April 19, 2008 Caltech-Exploratorium Learning Lab (CELL) Workshop Special Guest: Dr. Rusty Lansford, Senior Scientist and Instructor, Caltech Contents Exploring Spectra – Using a spectrascope to examine many different kinds of common continuous, emission, and absorption spectra. Luminescence – A complete description of many different examples of luminescence in the natural and engineered world. Exploratorium Teacher Institute Page 1 © 2008 Exploratorium, all rights reserved Exploring Spectra (by Paul Doherty and Linda Shore) Using a spectrometer The project Star spectrometer can be used to look at the spectra of many different sources. It is available from Learning Technologies, for under $20. Learning Technologies, Inc., 59 Walden St., Cambridge, MA 02140 You can also build your own spectroscope. http://www.exo.net/~pauld/activities/CDspectrometer/cdspectrometer.html Incandescent light An incandescent light has a continuous spectrum with all visible colors present. There are no bright lines and no dark lines in the spectrum. This is one of the most important spectra, a blackbody spectrum emitted by a hot object. The blackbody spectrum is a function of temperature, cooler objects emit redder light, hotter objects white or even bluish light. Fluorescent light The spectrum of a fluorescent light has bright lines and a continuous spectrum. The bright lines come from mercury gas inside the tube while the continuous spectrum comes from the phosphor coating lining the interior of the tube. Exploratorium Teacher Institute Page 2 © 2008 Exploratorium, all rights reserved CLF Light There is a new kind of fluorescent called a CFL (compact fluorescent lamp). -
Current-Voltage Characteristics of DC Plasma Discharges Employed In
IRAQI JOURNAL OF APPLIED PHYSICS Current-Voltage Mohammed K. Khalaf 1 Characteristics of DC Plasma Oday A. Hammadi 2 Firas J. Kadhim 3 Discharges Employed in Sputtering Techniques In this work, the current-voltage characteristics of dc plasma discharges were 1 Ministry of Science studied. The current-voltage characteristics of argon gas discharge at different and Technology, inter-electrode distances and working pressure of 0.7mbar without magnetrons Baghdad, IRAQ 2 were introduced. Then the variation of discharge current with inter-electrode Department of Physics, distance at certain discharge voltages without using magnetron was determined. College of Education, The current-voltage characteristics of discharge plasma at inter-electrode Al-Iraqia University, Baghdad, IRAQ distance of 4cm without magnetron, with only one magnetron and with dual 3 Department of Physics, magnetrons were also determined. The variation of discharge current with inter- College of Science, electrode distance at certain discharge voltage (400V) for the cases without University of Baghdad, magnetron, using one magnetron and dual magnetrons were studied. Finally, the Baghdad, IRAQ discharge current-voltage characteristics for different argon/nitrogen mixtures at total gas pressure of 0.7mbar and inter-electrode distance of 4cm were presented. Keywords: Plasma discharge; Magnetron; Glow discharge; Sputtering 1. Introduction emission effects, which lead to increase the flowing Glow discharge is low-temperature neutral current gradually approaching the breakdown point plasma where the number of electrons is equal to the beyond which the avalanche occurs and the current number of ions despite that local but negligible increases drastically in the Townsend discharge imbalances may exist at walls [1]. -
Exterior Lighting Guide for Federal Agencies
EXTERIOR LIGHTING GUIDE FOR FederAL AgenCieS SPONSORS TABLE OF CONTENTS The U.S. Department of Energy, the Federal Energy Management Program, page 02 INTRODUctiON page 44 EMERGING TECHNOLOGIES Lawrence Berkeley National Laboratory (LBNL), and the California Lighting Plasma Lighting page 04 REASONS FOR OUTDOOR Technology Center (CLTC) at the University of California, Davis helped fund and Networked Lighting LiGHtiNG RETROFitS create the Exterior Lighting Guide for Federal Agencies. Photovoltaic (PV) Lighting & Systems Energy Savings LBNL conducts extensive scientific research that impacts the national economy at Lowered Maintenance Costs page 48 EXTERIOR LiGHtiNG RETROFit & $1.6 billion a year. The Lab has created 12,000 jobs nationally and saved billions of Improved Visual Environment DESIGN BEST PRActicES dollars with its energy-efficient technologies. Appropriate Safety Measures New Lighting System Design Reduced Lighting Pollution & Light Trespass Lighting System Retrofit CLTC is a research, development, and demonstration facility whose mission is Lighting Design & Retrofit Elements page 14 EVALUAtiNG THE CURRENT to stimulate, facilitate, and accelerate the development and commercialization of Structure Lighting LIGHtiNG SYSTEM energy-efficient lighting and daylighting technologies. This is accomplished through Softscape Lighting Lighting Evaluation Basics technology development and demonstrations, as well as offering outreach and Hardscape Lighting Conducting a Lighting Audit education activities in partnership with utilities, lighting -
Plasma Discharge in Water and Its Application for Industrial Cooling Water Treatment
Plasma Discharge in Water and Its Application for Industrial Cooling Water Treatment A Thesis Submitted to the Faculty of Drexel University by Yong Yang In partial fulfillment of the Requirements for the degree of Doctor of Philosophy June 2011 ii © Copyright 2008 Yong Yang. All Rights Reserved. iii Acknowledgements I would like to express my greatest gratitude to both my advisers Prof. Young I. Cho and Prof. Alexander Fridman. Their help, support and guidance were appreciated throughout my graduate studies. Their experience and expertise made my five year at Drexel successful and enjoyable. I would like to convey my deep appreciation to the most dedicated Dr. Alexander Gutsol and Dr. Andrey Starikovskiy, with whom I had pleasure to work with on all these projects. I feel thankful for allowing me to walk into their office any time, even during their busiest hours, and I’m always amazed at the width and depth of their knowledge in plasma physics. Also I would like to thank Profs. Ying Sun, Gary Friedman, and Alexander Rabinovich for their valuable advice on this thesis as committee members. I am thankful for the financial support that I received during my graduate study, especially from the DOE grants DE-FC26-06NT42724 and DE-NT0005308, the Drexel Dean’s Fellowship, George Hill Fellowship, and the support from the Department of Mechanical Engineering and Mechanics. I would like to thank the friendship and help from the friends and colleagues at Drexel Plasma Institute over the years. Special thanks to Hyoungsup Kim and Jin Mu Jung. Without their help I would not be able to finish the fouling experiments alone. -
Basic Physics of the Incandescent Lamp (Lightbulb) Dan Macisaac, Gary Kanner,Andgraydon Anderson
Basic Physics of the Incandescent Lamp (Lightbulb) Dan MacIsaac, Gary Kanner,andGraydon Anderson ntil a little over a century ago, artifi- transferred to electronic excitations within the Ucial lighting was based on the emis- solid. The excited states are relieved by pho- sion of radiation brought about by burning tonic emission. When enough of the radiation fossil fuels—vegetable and animal oils, emitted is in the visible spectrum so that we waxes, and fats, with a wick to control the rate can see an object by its own visible light, we of burning. Light from coal gas and natural say it is incandescing. In a solid, there is a gas was a major development, along with the near-continuum of electron energy levels, realization that the higher the temperature of resulting in a continuous non-discrete spec- the material being burned, the whiter the color trum of radiation. and the greater the light output. But the inven- To emit visible light, a solid must be heat- tion of the incandescent electric lamp in the ed red hot to over 850 K. Compare this with Dan MacIsaac is an 1870s was quite unlike anything that had hap- the 6600 K average temperature of the Sun’s Assistant Professor of pened before. Modern lighting comes almost photosphere, which defines the color mixture Physics and Astronomy at entirely from electric light sources. In the of sunlight and the visible spectrum for our Northern Arizona University. United States, about a quarter of electrical eyes. It is currently impossible to match the He received B.Sc. -
Arxiv:1303.1588V2 [Physics.Hist-Ph] 8 Jun 2015 4.4 Errors in the Article
Translation of an article by Paul Drude in 1904 Translation by A. J. Sederberg1;∗ (pp. 512{519, 560{561), J. Burkhart2;y (pp. 519{527), and F. Apfelbeck3;z (pp. 528{560) Discussion by B. H. McGuyer1;x 1Department of Physics, Princeton University, Princeton, New Jersey 08544, USA 2Department of Physics, Columbia University, 538 West 120th Street, New York, NY 10027-5255, USA June 9, 2015 Abstract English translation of P. Drude, Annalen der Physik 13, 512 (1904), an article by Paul Drude about Tesla transformers and wireless telegraphy. Includes a discussion of the derivation of an equivalent circuit and the prediction of nonreciprocal mutual inductance for Tesla transformers in the article, which is supplementary material for B. McGuyer, PLoS ONE 9, e115397 (2014). Contents 1 Introduction 2 2 Bibliographic information 2 3 Translation 3 I. Definition and Integration of the Differential Equations . .3 Figure 1 . .5 II. The Magnetic Coupling is Very Small . .9 III. Measurement of the Period and the Damping . 12 IV. The Magnetic Coupling is Not Very Small . 19 VII. Application to Wireless Telegraphy . 31 Figure 2 . 32 Figure 3 . 33 Summary of Main Results . 39 4 Discussion 41 4.1 Technical glossary . 41 4.2 Hopkinson's law . 41 4.3 Equivalent circuit parameters from the article . 42 arXiv:1303.1588v2 [physics.hist-ph] 8 Jun 2015 4.4 Errors in the article . 42 4.5 Modifications to match Ls with previous work . 42 ∗Present address: Division of Biological Sciences, University of Chicago, 5812 South Ellis Avenue, Chicago, IL 60637, USA. yPresent address: Department of Microsystems and Informatics, Hochschule Kaiserslautern, Amerikastrasse 1, D-66482 Zweibr¨ucken, Germany.