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Evaluation of Monte Carlo Tools for High Energy Atmospheric Physics
Evaluation of Monte Carlo tools for high energy atmospheric physics Casper Rutjes1, David Sarria2, Alexander Broberg Skeltved3, Alejandro Luque4, Gabriel Diniz5,6, Nikolai Østgaard3, and Ute Ebert1,7 1Centrum Wiskunde & Informatica (CWI), Amsterdam, The Netherlands 2Astroparticules et Cosmologie, University Paris VII Diderot, CNRS/IN2P3, France 3Department of Physics and Technology, University of Bergen, 5020 Bergen, Norway 4Instituto de Astrofisica de Andalucia (IAA-CSIC), PO Box 3004, Granada, Spain 5Instituto Nacional de Pesquisas Espaciais, Brazil 6Instituto de Física, Universidade de Brasília, Brazil 7Eindhoven University of Technology, Eindhoven, The Netherlands Correspondence to: Casper Rutjes ([email protected]) Abstract. The emerging field of high energy atmospheric physics (HEAP) includes Terrestrial Gamma-ray Flashes, electron- positron beams and gamma-ray glows from thunderstorms. Similar emissions of high energy particles occur in pulsed high voltage discharges. Understanding these phenomena requires appropriate models for the interaction of electrons, positrons and photons of up to 40 MeV energy with atmospheric air. In this paper we benchmark the performance of the Monte Carlo codes 5 Geant4, EGS5 and FLUKA developed in other fields of physics and of the custom made codes GRRR and MC-PEPTITA against each other within the parameter regime relevant for high energy atmospheric physics. We focus on basic tests, namely on the evolution of monoenergetic and directed beams of electrons, positrons and photons with kinetic energies between 100 keV and 40 MeV through homogeneous air in the absence of electric and magnetic fields, using a low energy cut-off of 50 keV. We discuss important differences between the results of the different codes and provide plausible explanations. -
Sri Venkateswara College of Engineering and Technology Department of Electrical & Electronics Engineering EE 6504-Electrical
Sri Venkateswara College of Engineering and Technology Department of Electrical & Electronics Engineering EE 6504-Electrical Machines-II UNIT-I 1. Why a 3-phase synchronous motor will always run at synchronous speed? Because of the magnetic coupling between the stator poles and rotor poles the motor runs exactly at synchronous speed. 2. What are the two classification synchronous machines? The classification synchronous machines are: i. Cylindrical rotor type ii. Salient pole rotor type 3. What are the essential features of synchronous machine? i. The rotor speed is synchronous with stator rotating field. ii. Varying its field current can easily vary the speed. iii. It is used for constant speed operation. 4. Mention the methods of starting of 3-phase synchronous motor. a. A D.C motor coupled to the synchronous motor shaft. b. A small induction motor coupled to its shaft.(pony method) c. Using damper windings –started as a squirrel cage induction motor. 5. What are the principal advantages of rotating field system type of construction of synchronous machines? · Form Stationary connection between external circuit and system of conditions enable the machine to handle large amount of volt-ampere as high as 500 MVA. · The relatively small amount of power required for field system can be easily supplied to the rotating field system via slip rings and brushes. · More space is available in the stator part of the machine for providing more insulation to the system of conductors. · Insulation to stationary system of conductors is not subjected to mechanical stresses due to centrifugal action. · Stationary system of conductors can easily be braced to prevent deformation. -
Electricity Today Issue 4 Volume 17, 2005
ET_4_2005 6/3/05 10:41 AM Page 1 A look at the upcoming PES IEEE General Meeting see page 5 ISSUE 4 Volume 17, 2005 INFORMATION TECHNOLOGIES: Protection & Performance and Transformer Maintenance PUBLICATION MAIL AGREEMENT # 40051146 Electrical Buyer’s Guides, Forums, On-Line Magazines, Industry News, Job Postings, www.electricityforum.com Electrical Store, Industry Links ET_4_2005 6/3/05 10:41 AM Page 2 CONNECTINGCONNECTING ...PROTECTING...PROTECTING ® ® ® HTJC, Hi-Temperature Joint Compound With a unique synthetic compound for "gritted" and "non-gritted" specifications, the HTJC high temperature "AA" Oxidation Inhibitor improves thermal and electrical junction performance for all connections: • Compression Lugs and Splices for Distribution and Transmission • Tees, Taps and Stirrups on any conductor • Pad to Pad Underground, Substation and Overhead connections For oxidation protection of ACSS class and other connector surfaces in any environment (-40 oC to +250 oC), visit the Anderson ® / Fargo ® connectors catalogue section of our website www.HubbellPowerSystems.ca Anderson® and Fargo® offer the widest selection of high performance inhibitor compounds: Hubbell Canada LP, Power Systems TM ® ® 870 Brock Road South Inhibox , Fargolene , Versa-Seal Pickering, ON L1W 1Z8 Phone (905) 839-1138 • Fax: (905) 831-6353 www.HubbellPowerSystems.ca POWER SYSTEMS ET_4_2005 6/3/05 10:41 AM Page 3 in this issue Publisher/Executive Editor Randolph W. Hurst [email protected] SPECIAL PREVIEW Associate Publisher/Advertising Sales 5 IEEE PES General Meeting has -
Liquid Dielectrics, Their Classification, Properties, and Breakdown Strength
CHAPTER 6 LIQUID DIELECTRICS, THEIR CLASSIFICATION, PROPERTIES, AND BREAKDOWN STRENGTH From the point of view of molecular arrangement, a liquid can be described as “ highly compressed gas ” in which the molecules are very closely arranged. This is known as kinetic model of the liquid structure. A liquid is characterized by free movement of the constituent molecules among themselves but without the tendency to separate. However, the movement of charged particles, their microscopic streams, and interface conditions with other materials cause a distortion in the otherwise undisturbed molecular structure of the liquids. The well known terminology describ- ing the breakdown mechanisms in gaseous dielectrics — such as impact ionization, mean free path, electron drift, and so on — are, therefore, also applicable for liquid dielectrics. Liquid dielectrics are accordingly classifi ed in between the two states of matter; that is, gaseous and solid insulating materials. Wide range of application of liquid dielectircs in power apparatus also characterizes this intermediate position of liquid dielectrics. Insulating oils are used in power and instrument transformers, power cables, circuit breakers, power capacitors, and so on. Liquid dielectrics perform a number of functions simultaneously, namely: • insulation between the parts carrying voltage and the grounded container, as in transformers • impregnation of insulation provided in thin layers of paper or other materials, as in transformers, cables and capacitors, where oils or impregnating com- pounds are used • cooling action by convection in transformers and oil fi lled cables through circulation • fi lling up of the voids to form an electrically stronger integral part of a com- posite dielectric • arc extinction in circuit breakers High Voltage and Electrical Insulation Engineering, First Edition. -
The Physics of Streamer Discharge Phenomena
The physics of streamer discharge phenomena Sander Nijdam1, Jannis Teunissen2;3 and Ute Ebert1;2 1 Eindhoven University of Technology, Dept. Applied Physics P.O. Box 513, 5600 MB Eindhoven, The Netherlands 2 Centrum Wiskunde & Informatica (CWI), Amsterdam, The Netherlands 3 KU Leuven, Centre for Mathematical Plasma-astrophysics, Leuven, Belgium E-mail: [email protected] Abstract. In this review we describe a transient type of gas discharge which is commonly called a streamer discharge, as well as a few related phenomena in pulsed discharges. Streamers are propagating ionization fronts with self-organized field enhancement at their tips that can appear in gases at (or close to) atmospheric pressure. They are the precursors of other discharges like sparks and lightning, but they also occur in for example corona reactors or plasma jets which are used for a variety of plasma chemical purposes. When enough space is available, streamers can also form at much lower pressures, like in the case of sprite discharges high up in the atmosphere. We explain the structure and basic underlying physics of streamer discharges, and how they scale with gas density. We discuss the chemistry and applications of streamers, and describe their two main stages in detail: inception and propagation. We also look at some other topics, like interaction with flow and heat, related pulsed discharges, and electron runaway and high energy radiation. Finally, we discuss streamer simulations and diagnostics in quite some detail. This review is written with two purposes in mind: First, we describe recent results on the physics of streamer discharges, with a focus on the work performed in our groups. -
Simulations of the Propagation of Streamers in Electrical Discharges in a 5Mm Water Filled Gap
Research Article Curr Trends Biomedical Eng & Biosci Volume 9 Issue 4 -september 2017 Copyright © All rights are reserved by Duaa A Uamran DOI: 10.19080/CTBEB.2017.09.555767 Simulations of the Propagation of Streamers in Electrical Discharges in a 5mm Water Filled Gap Thamir H Khalaf1 and Duaa A Uamran1,2* 1Department of Physics, College of Science, University of Baghdad, Iraq 2Department of Physics, College of Science, University of Kerbala, Iraq Submission: August 09, 2017; Published: September 27, 2017 *Corresponding author: Duaa A Uamran, Department of Physics, College of Science, University of Baghdad, Iraq, Email: Abstract This work is devoted to the modeling of streamer discharge, propagation in liquid dielectrics (water) gap using the bubble theory. This of the electrical discharge (streamer) propagating within adielectric liquid subjected to a divergent electric, using finite element method (in thetwo dielectric dimensions). liquid Solution gap and of indicates Laplace’s the equation minimum governs breakdown the voltage voltage andrequired electric for fielda 5mm distributions atmospheric within pressure the dielectricconfiguration, liquid the gap electrode as 22KV. configuration a point (pin) - plane configuration, the plasma channels were followed, step to step. That shows the streamer discharge bridges shown agreement with the streamer growth, according to the simulation development time. The initiated streamer grows and branches toward all elements that satisfy the required conditions. The electric potential and field distributions Keywords: Herbal; Phytochemical; Cytotoxic; Formulations Introduction and slow, heavy ions alter the propagation of discharge channels The breakdown of insulating liquids is not simple to explain [7-9]. and the mechanism responsible for the initiation of breakdown is still open to controversy. -
“Contribution to Liquid Lens Technology”
“CONTRIBUTION TO LIQUID LENS TECHNOLOGY” Thesis submitted in partial fulfillment of the requirement for the PhD Degree issued by the Universitat Politècnica de Catalunya, in its Electronic Engineering Program Nom del doctorand Maziar Ahmadi Zeidabadi Directors: Prof. Dr. Luis Castañer Prof. Dra. Sandra Bermejo data de lectura de la tesi Mayo 2016 2 3 4 Contents Contents .............................................................................................................................. 5 1 Summary ................................................................................................................... 21 1.1 Introduction........................................................................................................ 23 1.2 Thesis challenges and outlines .......................................................................... 25 2 Liquid lens (Fundamentals and theory) ................................................................... 27 2.1 Liquid lens devices overview ............................................................................ 29 2.2 Basic principles of capillarity and wetting ........................................................ 30 2.3 Hydrophobic surfaces ........................................................................................ 32 2.3.1 Wenzel model ............................................................................................. 33 2.3.2 Cassie-Baxter model................................................................................... 34 2.4 Electrical -
Birmingham Local Section
264 MORRIS AND LISTER: THE TESTING OF [Birmingham, BIRMINGHAM LOCAL SECTION. THE TESTING OF TRANSFORMERS AND TRANSFORMER IRON. By D. K. MORRIS, Ph.D., and G. A. LISTER, Associate Members. (Paper read on April 25, 1906.) SYNOPSIS.—1. Introduction. 2. Regulation diagram. 3. Diagram of voltage charac- teristic. 4. The short-circuit test. 5. Proposed standard transformer test. 6. The 3-point wattmeter method. 7. Standard tests for—(a) core losses: separation by constant-frequency test ; (6) copper losses; (c) efficiency; (d) heating ; (e) regulation. 8. The auxiliary transformer. 9. Special tests— (a) by means of extra turns ; (b) at half power factor; (c) out-of-phase test; (<i) 3-phase transformers. 10. Hysteresis by slow cyclic change—(a) method of constant induced voltage ; (b) theory; (c) application to testing of small samples. 11. Conclusion. APPENDIX.—The 3-point method. Temperature by the wattmeter. Improvements in the constant induced voltage method. Separation of hysteresis from eddy- current loss. 1. INTRODUCTION. In the testing of transformers the principal- qualities which may have to be investigated are :— (a)' Core losses. (b) Copper losses at all loads. (c) Efficiency at light loads as well as full load. (d) Heating at full load. (e) Regulation on all loads and power factors. (/) Insulation (not dealt with in the paper). The designer and manufacturer of the transformers may also require to know the extent to which the core loss is caused by hysteresis or eddy currents. In addition, it would be useful to deter- mine the excellence of the built-up magnetic circuit, having reference to the permeability of the iron and the low magnetic resistance of the joints. -
Guideline on Electrical Power for Adp Installations
*tm iab as FIPS PUB 94 NBS \f \ RESEARCH M. INFORMATION CENTER ain <t FEDERAL INFORMATION v ./ 6<JffEAU O* PROCESSING STANDARDS PUBLICATION 1983 SEPTEMBER 21 U.S. DEPARTMENT OF COMMERCE/National Bureau of Standards GUIDELINE ON ELECTRICAL POWER FOR ADP INSTALLATIONS CATEGORY: HARDWARE JK——CATEGORY: POWER, GROUNDING, “68 AND LIFE-SAFETY • A8A3 #94 U.S. DEPARTMENT OF COMMERCE, Malcolm Baldrige, Secretary NATIONAL BUREAU OF STANDARDS, Ernest Ambler, Director Foreword The Federal Information Processing Standards Publication Series of the National Bureau of Standards is the official publication relating to standards adopted and promulgated under the provisions of Public Law 89-306 (Brooks Act) and under Part 6 of Title 15, Code of Federal Regulations. These legislative and executive mandates have given the Secretary of Commerce important responsibilities for improving the utilization and management of computers and automatic data processing in the Federal Government. To carry out the Secretary’s responsibilities, the NBS, through its Institute for Computer Sciences and Technology, provides leadership, technical guidance, and coordination of Government efforts in the development of guidelines and standards in these areas. Comments concerning Federal Information Processing Standards Publications are welcomed and should be addressed to the Director, Institute for Computer Sciences and Technology, National Bureau of Standards, Washington, DC 20234. James H. Burrows, Director Institute for Computer Sciences and Technology Abstract This recommended Guideline for Federal agencies identifies and describes the electrical environment for safe, reliable operation of automatic data processing (ADP) systems The electrical environment in and immediately outside the computer room is considered The Guideline describes the fundamentals which underlie the power, grounding, and life- safety requirements, and provides a guide and checklist for specifying and preparing ADP sites, and evaluating their suitability. -
Preparation of Monodisperse Microbubbles in a Capillary Embedded T-Junction Device and the Influence of Process Control Parameters on Bubble Size and Stability
Preparation of monodisperse microbubbles in a capillary embedded T-Junction device and the influence of process control parameters on bubble size and stability A thesis submitted in partial fulfilment of the requirements for the degree of Doctor of Philosophy By Maryam Parhizkar Department of Mechanical Engineering University College London Torrington Place, London WC1E 7JE U.K March, 2014 Declaration I, Maryam Parhizkar, confirm that the work presented in this thesis is my own. Where information has been derived from other sources, I confirm that this has been indicated in the thesis. ………………………………….. Maryam Parhizkar 1 Abstract The main goal for this work was to produce microbubbles for a wide range of applications with sizes ranging between 10 to 300 µm in a capillary embedded T- junction device. Initially the bubble formation process was characterized and the factors that affected the bubble size; in particular the parameters that reduce it were determined. In this work, a polydimethylsiloxane (PDMS) block (100 x 100 x 10 mm3) was used, in which the T-shaped junction was created by embedded capillaries of fixed outer diameter. The effect of the inner diameter was investigated by varying all the inlet and outlet capillaries’ inner diameter at different stages. In addition, the effect of changes in the continuous phase viscosity and flow rate (Ql) as well as the gas pressure (Pg) on the resulting bubble size was studied. Aqueous glycerol solutions were chosen for the liquid phase, as they are widely used in experimental studies of flow phenomena and provide a simple method of varying properties through dilution. -
System Voltage Regulation
CHAPTER 7 SYSTEM VOLTAGE REGULATION H. E. LOKAY The primary objective of system voltage control is to system are discussed, as well as the characteristics of economically provide to each power user voltage that each application. The equipment is discussed by de- conforms to the voltage design limitations of the utiliza- scribing its method of operation and how it affects an tion equipment. Almost all utilization equipment is de- application. signed for use at a particular, definite terminal voltage: I. DEFINITIONS the nameplate voltage. It is economically impossible to provide each and every consumer on a distribution In discussing system voltage control, certain terminol- system with a constant utilization voltage correspond- ogy is naturally used. Following are common terms and ing to the nameplate voltage of the utilization devices. definitions used throughout this chapter. Other terms Voltage drop exists in each part of the power system that refer only to a particular section of this chapter are from the source to the consumer's service drop. Voltage defined in that particular section. drop also occurs in his interior wiring. Voltage drop Voltage drop—"Voltage drop (in a supply system) is is proportional to the magnitude and phase angle the difference between the voltage at the transmitting of the load current flowing through the entire power and receiving ends of a feeder, main, or service."' system. This essentially means that the consumer elec- The voltage drop is not necessarily the impedance trically closest to the source would receive a higher drop (IZ) of a feeder, main or service, but the difference voltage than the consumer most remote from the source. -
Electrical Breakdown in Gases
High-voltage Pulsed Power Engineering, Fall 2018 Electrical Breakdown in Gases Fall, 2018 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University Gas breakdown: Paschen’s curves for breakdown voltages in various gases Friedrich Paschen discovered empirically in 1889. Left branch Right branch Paschen minimum F. Paschen, Wied. Ann. 37, 69 (1889)] 2/40 High-voltage Pulsed Power Engineering, Fall 2018 Generation of charged particles: electron impact ionization + Proton Electron + + Electric field Acceleration Electric field Slow electron Fast electron Acceleration Electric field Acceleration Ionization energy of hydrogen: 13.6 eV 3/40 High-voltage Pulsed Power Engineering, Fall 2018 Behavior of an electron before ionization collision Electrons moving in a gas under the action of an electric field are bound to make numerous collisions with the gas molecules. 4/40 High-voltage Pulsed Power Engineering, Fall 2018 Electron impact ionization Electron impact ionization + + Electrons with sufficient energy (> 10 eV) can remove an electron+ from an atom and produce one extra electron and an ion. → 2 5/40 High-voltage Pulsed Power Engineering, Fall 2018 Townsend mechanism: electron avalanche = Townsend ionization coefficient ( ) : electron multiplication : production of electrons per unit length along the electric field (ionization event per unit length) = = exp( ) = = 푒 푒 6/40 High-voltage Pulsed Power Engineering, Fall 2018 Townsend 1st ionization coefficient When an electron travels a distance equal to its free path in the direction of the field , it gains an energy of . For the electron to ionize, its gain in energy should be at least equal to the ionization potential of the gas: 1 1 = ≥ st ∝ The Townsend 1 ionization coefficient is equal to the number of free paths (= 1/ ) times the probability of a free path being more than the ionizing length , 1 1 exp exp ∝ − ∝ − = ⁄ − A and B must be experimentally⁄ determined for different gases.