Plasma Discharge in Water and Its Application for Industrial Cooling Water Treatment

Total Page:16

File Type:pdf, Size:1020Kb

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. Finally I wish to express my gratitude to my family. Without their love, support, encouragement and understanding all these years, this doctoral thesis would not have been possible. iv Table of Contents List of Tables………………………………………………………………………...vii List of Figures……………………………………………………………………….viii Abstract……………………………………………………………………………...xvi Chapter 1. Introduction to Plasma in Water…………………………………………..1 1.1. Needs for Plasma Water Treatment………………………………………1 1.1.1. Cooling Water Management…………………………………..1 1.1.2. Water Sterilization…………………………………………….4 1.2. Previous Studies on the Plasma Water Treatment………………………..5 1.3. Process of Conventional Electrical Breakdown in Water……………….10 Chapter 2. Underwater Plasma Sources……………………………………………...18 2.1. Direct Discharges in Liquid……………………………………………..18 2.2. Bubble Discharges in Liquid……………………………………………23 Chapter 3. Dynamics of Non-Equilibrium Plasma on Liquid Water………………...27 3.1. Plasma Diagnostic Platform……………………………………………..27 3.2. Imaging of Plasma Initiation in Nanosecond Time Regime…………….29 3.3. Imaging of Plasma Initiation in Sub-nanosecond Time Regime………..31 Chapter 4. Analysis of Microsecond Streamer Propagation………………………...34 4.1. Electrostatic Model……………………………………………………...35 4.2. Thermal Model…………………………………………………………..44 v 4.3. Stability Analysis………………………………………………………..51 4.3.1. Electrostatic Pressure………………………………………...53 4.3.2. Surface Tension……………………………………………...54 4.3.3. Hydrodynamic Pressure……………………………………..54 Chapter 5. Application of Spark Discharge for Scale Removal on Filter Membranes……………………………………………………………….60 5.1. Spark Discharge System………………………………………………...61 5.2. Results and Discussions…………………………………………………66 Chapter 6. Plasma-Assisted Calcium Carbonate Precipitation………………………73 6.1. Experiment Setup……………………………………………………….74 6.1.1. Water preparation……………………………………………75 6.1.2. Pulsed Spark Discharge Generation System…………………76 6.1.3. Water Treatment……………………………………………..79 6.2. Calcium Carbonate Precipitation Results……………………………….80 6.2.1. Effect of Immediate Plasma Exposure……………………….80 6.2.2. Effect of Spray Circulation…………………………………..90 6.3. Calcium Carbonate Precipitation Mechanism Study……………………92 6.3.1. Discussions of Possible Mechanisms………………………...92 6.3.2. Effect of UV Radiation……………………………………..101 6.3.3. Effect of Reactive Species………………………………….102 6.3.4. Effect of Micro-heating…………………………………….104 6.3.5. Non-thermal Effect of Plasma……………………………...109 vi 6.3.6. Further Discussions…………………………………………112 Chapter 7. Application for Mineral Fouling Mitigation in Heat Exchangers………116 7.1. Mineral Fouling System………………………………………………..118 7.1.1. Heat Transfer Fouling Tests………………………………...118 7.1.2. Pulsed Spark Discharge Generation System………………..122 7.1.3. Artificial Hard Water……………………………………….123 7.2. Results and Discussion………………………………………………...125 7.2.1. Cycle of Concentration (COC)……………………………..125 7.2.2. Fouling Resistance………………………………………….126 7.2.3. Scanning Electron Microscope Images……………………..135 7.2.4. X-Ray Diffraction Tests…………………………………….136 Bibliography………………………………………………………………………..138 VITA……………………………………………………………………………….153 vii List of Tables Table 1. Summary of the characteristics of pulsed corona, pulsed arc and pulsed spark discharge in water…………………………………………………………...13 Table 2. Oxidation potential of active species produced by plasma in water………..14 Table 3. Chemical compositions of water samples collected in the laboratory cooling tower………………………………………………………………………...75 Table 4. Results obtained by laser particle counting………………………………...88 Table 5. Thermochemical data of Reactions 1, 2 and 3……………………………...94 Table 6. Amount of CaCl2 and NaHCO3 used in artificial hard water……………..123 viii List of Figures Figure 1. US freshwater withdrawal (2000). Source: USGS, Estimated use of water in the United States in 2000, USGS Circular 1268, March 2004……………………..1 Figure 2. Average daily national freshwater consumption for thermoelectric power generation 2005-2030 (predicted). Source: DOE/Office of Fossil Energy's Energy & Water R&D Program. 2008…………………………………………………………...2 Figure 3. US freshwater consumption (1995). Source: USGS, Estimated use of water in the United States in 1995, USGS Circular 1220, 1998……………………………..4 Figure 4. Images of plasma discharge in water: (a) pulsed corona; (b) pulsed arc produced at Drexel Plasma Institute…………………………………………………11 Figure 5. Schematics of electrode geometries used for plasma discharges in liquid: (a) single point-to-plane; (b) multiple points-to-plane; (c) point-to-point; (d)pin hole; (e) wire-to-cylinder; (f) disk electrode; (g) composite electrode with porous ceramic layer…………………………………………………………………………………..19 Figure 6. Images of plasma discharges through a pinhole: (a) pulsed corona; (b) pulsed arc produced at Drexel Plasma Institute……………………………………...20 Figure 7. Time integrated image of discharges generated using a wire-cylinder geometry in water, where tungsten wire and stainless steel mesh cylinder were used. Chamber dimensions: 44-mm ID, 100-mm length…………………………………..21 Figure 8. Pulsed multichannel discharge array in water generated by two stainless steel disk electrodes separated by a dielectric layer………………………………….22 ix Figure 9. Multichannel pulsed electrical discharge in water generated using porous- ceramic-coated metallic electrodes…………………………………………………..23 Figure 10. Schematics of electrode geometries for bubble discharge: (a) point-to- plane; (b) parallel plate; (c) gas channel with liquid wall; (d) RF bubble discharge; (e) microwave bubble discharge…………………………………………………...…….26 Figure 11. Voltage waveform produced from the nanosecond-duration power supply ………………………………………………………………………..………28 Figure 12. Voltage waveform produced from the subnanosecond-duration power supply………………………………………………………………………………...28 Figure 13. Schematic diagram of the experiment setup……………………………...29 Figure 14. Image of a nanosecond-duration discharge in water taken at a camera gate of 100 μs……………………………………………………………………………..29 Figure 15. Images showing the dynamics of nanosecond-duration discharge emission and high-voltage potential on electrode. Images were taken at a camera gate of 1 ns……………………………………………………………………………………..30 Figure 16. Images showing the dynamics of nanosecond-duration discharge emission and high-voltage potential on electrode taken at a camera gate of 0.5 ns…………..32 Figure 17. Subnanosecond-duration discharge development for different voltages…32 Figure 18. Initiations of (a) bubble formation and (b) cylindrical filament formation in water………………………………………………………………………………….36 x Figure 19. Force balance for the electrostatic model………………………………...41 Figure 20. Variations of filament radius as a function of applied voltage and inter- electrode distance…………………………………………………………………….43 Figure 21. Variations of Mach number of streamer as a function of applied voltage and inter-electrode distance………………………………………………………….44 Figure 22. Force balance for the thermal model……………………………………..46 Figure 23. Variations of filament radius as a function of applied voltage and inter- electrode distance…………………………………………………………………….49 Figure 24. Variations of the Mach number of streamer as a function of applied voltage and inter-electrode distance………………………………………………….50 Figure 25. Schematic diagram of disturbance at the surface of filament…………….51 Figure 26. Instability growth rate ω at low applied voltages. k and ω are 3 1/2 nondimensionalized using streamer radius r0 and time scale t = (ρr0 /γ) …………56 Figure 27. Instability growth rate ω at high applied voltages. k and ω are nondimensionalized as in Figure 26…………………………………………………57 Figure 28. Schematic diagram of the testing loop…………………………………...62 Figure 29. Schematic diagram of a pulsed power system……………………………64 Figure 30. Typical voltage and current waveforms of a pulsed discharge in water…64 xi Figure 31. Changes in pressure drop at three different flow rates with an artificially hardened water……………………………………………………………………….66 Figure 32. Variations
Recommended publications
  • 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.
    [Show full text]
  • Detailed Investigation of the Electric Discharge Plasma Between Copper Electrodes Immersed Into Water
    atoms Article Detailed Investigation of the Electric Discharge Plasma between Copper Electrodes Immersed into Water Roman Venger 1, Tetiana Tmenova 1,2,*, Flavien Valensi 2, Anatoly Veklich 1, Yann Cressault 2 and Viacheslav Boretskij 1 1 Electronics and Computer Systems, Faculty of Radio Physics, Taras Shevchenko National University of Kyiv, 64, Volodymyrska St., 01601 Kyiv, Ukraine; [email protected] (R.V.); [email protected] (A.V.); [email protected] (V.B.) 2 Université de Toulouse, UPS, INPT; LAPLACE (Laboratoire Plasma et Conversion d’Energie), 118 route de Narbonne, F-31062 Toulouse CEDEX 9, France; [email protected] (F.V.); [email protected] (Y.C.) * Correspondence: [email protected]; Tel.: +38-063-598-5219 Academic Editors: Milan S. Dimitrijevi´cand Luka C.ˇ Popovi´c Received: 11 September 2017; Accepted: 16 October 2017; Published: 23 October 2017 Abstract: A phenomenological picture of pulsed electrical discharge in water is produced by combining electrical, spectroscopic, and imaging methods. The discharge is generated by applying ~350 µs long 100 to 220 V pulses (values of current from 400 to 1000 A, respectively) between the point-to-point copper electrodes submerged into the non-purified tap water. Plasma channel and gas bubble occur between the tips of the electrodes, which are initially in contact with each other. The study includes detailed experimental investigation of plasma parameters of such discharge using the correlation between time-resolved high-speed imaging, electrical characteristics, and optical emission spectroscopic data. Radial distributions of the electron density of plasma is estimated from the analysis of profiles and widths of registered Hα and Hβ hydrogen lines, and Cu I 515.3 nm line, exposed to the Stark mechanism of spectral lines’ broadening.
    [Show full text]
  • Ionic Liquid and Supercritical Fluid Hyphenated Techniques for Dissolution and Separation of Lanthanides, Actinides, and Fission Products
    Project No. 09-805 Ionic Liquid and Supercritical Fluid Hyphenated Techniques for Dissolution and Separation of Lanthanides, Actinides, and Fission Products ItIntegrat tdUied Universit itPy Programs Dr. Chien Wai University of Idaho In collaboration with: Idaho National Laboratory Jack Law, Technical POC James Bresee, Federal POC 1 Ionic Liquid and Supercritical Fluid Hyphenated Techniques For Dissolution and Separation of Lanthanides and Actinides DOE-NEUP Project (TO 00058) Final Technical Report Principal Investigator: Chien M. Wai Department of Chemistry, University of Idaho, Moscow, Idaho 83844 Date: December 1, 2012 2 Table of Contents Project Summary 3 Publications Derived from the Project 5 Chapter I. Introduction 6 Chapter II. Uranium Dioxide in Ionic Liquid with a TP-HNO3 Complex – Dissolution and Coordination Environment 9 1. Dissolution of UO2 in Ionic Liquid with TBP(HNO3)1.8(H2O)0.6 2. Raman Spectra of Dissolved Uranyl Species in IL 13 3. Transferring Uranium from IL Phase to sc-CO2 15 Chapter III. Kinetic Study on Dissolution of Uranium Dioxide and Neodymium Sesquioxide in Ionic Liquid 19 1. Rate of Dissolution of UO2 and Nd2O3 in RTIL 19 2. Temperature Effect on Dissolution of UO2 and Nd2O3 24 3. Viscosity Effect on Dissolution of UO2 in IL with TBP(HNO3)1.8(H2O)0.6 Chapter IV. Separation of UO2(NO3)2(TBP)2 and Nd(NO3)3(TBP)3 in Ionic Liquid Using Diglycolamide and Supercritical CO2 Extraction 30 1. Complexation of Uranyl with Diglycolamide TBDGA in Ionic Liquid 31 2. Complexation of Neodymium(III) with TBDGA in Ionic Liquid 35 3. Solubility and Distribution Ratio of UO2(NO3)2(TBP)2 and Nd(NO3)3(TBP)3 in Supercritical CO2 Phase 38 4.
    [Show full text]
  • Research Paper Commerce Physics Atomic Emission Spectroscopy
    Volume-4, Issue-10, Oct-2015 • ISSN No 2277 - 8160 Commerce Research Paper Physics Atomic Emission Spectroscopy Ramanjeet Kaur Assistant Professor Physics Department, R S D College, Ferozepur City ABSTRACT The atomic emission spectroscopy is method based on the study of light emitted by atoms to determine the proportional quantity of a particular element in a given sample. Three techniques of atomic emission spectroscopy flame emission arc & spark emission and plasma atomic emission spectroscopy, their working, Principle and applications has been discussed in detail. KEYWORDS : -spectroscopy, flame, spark & arc, plasma, qualitative & quantitative analysis INTRODUCTION Atomic spectroscopy is the determination of elemental composition termining the accuracy of the analysis. The most popular sampling by its electromagnetic spectrum. Electrons exist in energy levels with- method is nebulization of a liquid sample to provide a steady flow of in an atom. These levels have well defined energies and electrons aerosol into a flame. An introduction system for liquid samples con- moving between them must absorb or emit energy equal to the dif- sists of three components: (a) a nebulizer that breaks up the liquid ference between them. The wavelength of the emitted radiant ener- into small’ droplets, (b) an aerosol modifier that removes large drop- gy is directly related to the electronic transition which has occurred. lets from the stream, allowing only droplets smaller than a certain Since every element has a unique electronic structure, the wave- size to pass, and (c) the flame or atomizer that converts the anaIyte length of light emitted is a unique property of each individual ele- into free atoms.
    [Show full text]
  • Application of Supercritical Fluids Review Yoshiaki Fukushima
    1 Application of Supercritical Fluids Review Yoshiaki Fukushima Abstract Many advantages of supercritical fluids come Supercritical water is expected to be useful in from their interesting or unusual properties which waste treatment. Although they show high liquid solvents and gas carriers do not possess. solubility solutes and molecular catalyses, solvent Such properties and possible applications of molecules under supercritical conditions gently supercritical fluids are reviewed. As these fluids solvate solute molecules and have little influence never condense at above their critical on the activities of the solutes and catalysts. This temperatures, supercritical drying is useful to property would be attributed to the local density prepare dry-gel. The solubility and other fluctuations around each molecule due to high important parameters as a solvent can be adjusted molecular mobility. The fluctuations in the continuously. Supercritical fluids show supercritical fluids would produce heterogeneity advantages as solvents for extraction, coating or that would provide novel chemical reactions with chemical reactions thanks to these properties. molecular catalyses, heterogenous solid catalyses, Supercritical water shows a high organic matter enzymes or solid adsorbents. solubility and a strong hydrolyzing ability. Supercritical fluid, Supercritical water, Solubility, Solvation, Waste treatment, Keywords Coating, Organic reaction applications development reached the initial peak 1. Introduction during the period from the second half of the 1960s There has been rising concern in recent years over to the 1970s followed by the secondary peak about supercritical fluids for organic waste treatment and 15 years later. The initial peak was for the other applications. The discovery of the presence of separation and extraction technique as represented 1) critical point dates back to 1822.
    [Show full text]
  • 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
    [Show full text]
  • Glossary of Terms
    GLOSSARY OF TERMS For the purpose of this Handbook, the following definitions and abbreviations shall apply. Although all of the definitions and abbreviations listed below may have not been used in this Handbook, the additional terminology is provided to assist the user of Handbook in understanding technical terminology associated with Drainage Improvement Projects and the associated regulations. Program-specific terms have been defined separately for each program and are contained in pertinent sub-sections of Section 2 of this handbook. ACRONYMS ASTM American Society for Testing Materials CBBEL Christopher B. Burke Engineering, Ltd. COE United States Army Corps of Engineers EPA Environmental Protection Agency IDEM Indiana Department of Environmental Management IDNR Indiana Department of Natural Resources NRCS USDA-Natural Resources Conservation Service SWCD Soil and Water Conservation District USDA United States Department of Agriculture USFWS United States Fish and Wildlife Service DEFINITIONS AASHTO Classification. The official classification of soil materials and soil aggregate mixtures for highway construction used by the American Association of State Highway and Transportation Officials. Abutment. The sloping sides of a valley that supports the ends of a dam. Acre-Foot. The volume of water that will cover 1 acre to a depth of 1 ft. Aggregate. (1) The sand and gravel portion of concrete (65 to 75% by volume), the rest being cement and water. Fine aggregate contains particles ranging from 1/4 in. down to that retained on a 200-mesh screen. Coarse aggregate ranges from 1/4 in. up to l½ in. (2) That which is installed for the purpose of changing drainage characteristics.
    [Show full text]
  • Identification of the Electric Spark Electromagnetic Waveform Based on SVM
    Advances in Engineering Research, volume 127 3rd International Conference on Electrical, Automation and Mechanical Engineering (EAME 2018) Identification of the Electric Spark Electromagnetic Waveform Based on SVM Tongtong Li1,*, Ziyuan Tong2, Shoufeng Tang1, Xia Qin1, Mingming Tong1 and Zhaoliang Xu3 1China University of Mining and Technology, China 2School of Electrical Engineering and Telecommunications, The University of New South Wales, Australia 3Xuzhou Hanlin Technology Co., Ltd., China *Corresponding author Abstract—Electromagnetic wave of electrical spark is a current. potential cause to eletrical equipment failure. This research focused on identificating and comparative analyzing the different A. Electromagnetic Characteristics Extraction of the Electric types of electromagnetic waveform generated by eletrical Spark equipment failure based on SVM. After analyzing and extracting the features the electromagnetic waveform, a model was built to First, confirm that you have the correct template for your identificate the type of the elctromagnetic waveform. The paper size. This template has been tailored for output on the collected standard electromagnetic waveforms were used as the US-letter paper size. If you are using A4-sized paper, please imput of the train model and the model accuracy was improved close this file and download the file for “MSW_A4_format”. by adjusting training parameters afer analyzing the results, When the distance between the contact closure electrodes When inputting an unknown type of electromagnetic waveform, gradually decreases or a strong electric field occurs[6], the SVM may predict the output of the network according to the current density gradually increases and produces high recognition rule. Then the types of electromagnetic waveforms temperature ionization, then contact and electrode gas will be were identificated by using adjusted models.
    [Show full text]
  • Investigations of Liquid Steel Viscosity and Its Impact As the Initial Parameter on Modeling of the Steel Flow Through the Tundish
    materials Article Investigations of Liquid Steel Viscosity and Its Impact as the Initial Parameter on Modeling of the Steel Flow through the Tundish Marta Sl˛ezak´ 1,* and Marek Warzecha 2 1 Department of Ferrous Metallurgy, Faculty of Metals Engineering and Industrial Computer Science, AGH University of Science and Technology, Al. Mickiewicza 30, 30-059 Kraków, Poland 2 Department of Metallurgy and Metal Technology, Faculty of Production Engineering and Materials Technology, Cz˛estochowaUniversity of Technology, Al. Armii Krajowej 19, 42-201 Cz˛estochowa,Poland; [email protected] * Correspondence: [email protected] Received: 14 September 2020; Accepted: 5 November 2020; Published: 7 November 2020 Abstract: The paper presents research carried out to experimentally determine the dynamic viscosity of selected iron solutions. A high temperature rheometer with an air bearing was used for the tests, and ANSYS Fluent commercial software was used for numerical simulations. The experimental results obtained are, on average, lower by half than the values of the dynamic viscosity coefficient of liquid steel adopted during fluid flow modeling. Numerical simulations were carried out, taking into account the viscosity standard adopted for most numerical calculations and the average value of the obtained experimental dynamic viscosity of the analyzed iron solutions. Both qualitative and quantitative analysis showed differences in the flow structure of liquid steel in the tundish, in particular in the predicted values and the velocity profile distribution. However, these differences are not significant. In addition, the work analyzed two different rheological models—including one of our own—to describe the dynamic viscosity of liquid steel, so that in the future, the experimental stage could be replaced by calculating the value of the dynamic viscosity coefficient of liquid steel using one equation.
    [Show full text]
  • 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].
    [Show full text]
  • Electrical Breakdown and Ignition of an Electrostatic Particulate Suspension Tae-U Yu Iowa State University
    Iowa State University Capstones, Theses and Retrospective Theses and Dissertations Dissertations 1983 Electrical breakdown and ignition of an electrostatic particulate suspension Tae-U Yu Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/rtd Part of the Mechanical Engineering Commons Recommended Citation Yu, Tae-U, "Electrical breakdown and ignition of an electrostatic particulate suspension " (1983). Retrospective Theses and Dissertations. 7661. https://lib.dr.iastate.edu/rtd/7661 This Dissertation is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Retrospective Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. INFORMATION TO USERS This reproduction was made from a copy of a document sent to us for microfilming. While the most advanced technology has been used to photograph and reproduce this document, the quality of the reproduction is heavily dependent upon the quality of the material submitted. The following explanation of techniques is provided to help clarify markings or notations which may appear on this reproduction. 1. The sign or "target" for pages apparently lacking from the document photographed is "Missing Page(s)". If it was possible to obtain the missing page(s) or section, they are spliced into the film along with adjacent pages. This may have necessitated cutting through an image and duplicating adjacent pages to assure complete continuity. 2. When an image on the film is obliterated with a round black mark, it is an indication of either blurred copy because of movement during exposure, duplicate copy, or copyrighted materials that should not have been filmed.
    [Show full text]
  • 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.
    [Show full text]