Propagation of Cathode-Directed Streamer Discharges in Air

Size: px
Start display at page:

Download "Propagation of Cathode-Directed Streamer Discharges in Air"

Transcription

1 Propagatio of Cathode-Directed Streamer Discharges i Air Yuriy Serdyuk Associate Professor High Voltage Egieerig Chalmers Uiversity of Techology SE Gotheburg, Swede yuriy.serdyuk@chalmers.se

2 Outlie Itroductio Drift-diffusio model of streamer discharges i air Model implemetatio Simulatios of positive streamers Cocludig remarks

3 Electrical gas discharges Pheomea associated with trasport of electrical charges through eutral gas due to applied electric fields. Trasport processes are usually strogly domiated by space charge effects. Examples of o-thermal discharges: electro avalaches, streamers, coroas, statioary glow discharges, dielectric barrier discharges (DBD). A streamer discharge is a self-sustaied ioizatio wave propagatig i eutral gas.

4 Positive streamers i air Streamers develop as thi plasma chaels sustaied by productio of electros i the strog field regio at the head. Depedig upo coditios (pressure, legth, power iput, overvoltage, etc.) they may experiece brachig. Trasitio from glow to streamer: eedle-plae gap, legth 20mm, U app = +21 kv, exposure 5 s. T. M. P. Briels et al., Positive ad egative streamers i ambiet air: measurig diameter, velocity ad dissipated eergy, J. Phys. D: Appl. Phys., 2008, 41, T. Czech et al., Optical emissio spectroscopy of poit-plae coroa ad back-coroa discharges i air, Eur. Phys. J. D, 2011, 65,

5 Drift-diffusio model of air discharges Charge carriers are represeted as electroic ad ioic fluids ad are characterized by averaged properties. Mass coservatio equatios for electros ad ios: Poisso equatio for electric potetial : Appropriate (problem depedet) boudary ad iitial coditios are to be provided for all the PDEs. ) ( ) ( / ) ( ) ( / ) ( ) ( / E S D t E S D t E S D t p p p p p p e e e e e e E E E E, ) ( ) ( 0 e p q

6 Icorporatig photoioizatio i air Mechaism: e * * N 2 N 2 e N 2 N 2 h ( m) O2 h O No-local ioizatio: electros are created by photos at a distace from a source of radiatio. The photoioizatio rate is icluded as j where the terms (r) satisfy Helmholtz equatios ( * ) 2 S j ph S ph ( r) ( p j O 2 j 2 ) S ( r) A p I( r) 2 ph j O2 Two expoetial fit is used with the parameters ad A j. ( * ) A. Bourdo et al., Efficiet models for photoioizatio produced by othermal gas discharges i air based o radiative trasfer ad the Helmholtz equatios, Plasma Sources Sci. Techol., 2007, 16, j S ph( r) S ph ( r) j j e

7 Model implemetatio Set of PDEs: three drift-diffusio, Poisso s, two Helmholtz. Source term stabilizatio is implemeted for the DD PDEs. Mesh size at streamer frot is ~10 µm, withi the plasma chael ~70 µm ad larger i the rest of the domai. The mesh was refied maually. Solver: direct, segregated (two steps) with cotiues Jacobia update. Time steppig: BDF with variable order.

8 Simulatios of streamers i air Hyperbolic eedle-plae electrodes, pressure 760 Torr, temperature 293 K, voltage rise time 0.1 s. A sigle discharge is cosidered ad the model is implemeted i 2D utilizig axial symmetry. The discharge is iitiated from a seedig charge spot of Gaussia shape ( e = p = m -3, σ = 30 µm) located at 0.1 mm from the eedle tip. Drift of ios is eglected due to the short duratio of the discharge. Two study cases: - gap legth 5 mm (applied voltage +15 kv dc) - gap legth 30 mm (voltage +40 kv dc).

9 Short streamer: dyamics of electros plae eedle

10 Short streamer: electric field plae eedle

11 Log streamer: dyamics of electros plae eedle

12 Log streamer: electric field plae eedle

13 Calculated discharge curret Streamer 5 mm Streamer 30 mm

14 Calculated parameters of streamers Velocity at stable propagatio: 5 mm streamer - ~ m/s 30 mm streamer - ~ m/s Chael radius at stable propagatio : 5 mm streamer µm (strogest field) µm (strogest S ph ) 30 mm streamer µm (strogest field) µm (strogest S ph )

15 Typical parameters of streamers A. Luque et al., Positive ad egative streamers i ambiet air: modellig evolutio ad velocities, J. Phys. D: Appl. Phys. 41 (2008) T. M. P. Briels et al., Circuit depedece of the diameter of pulsed positive streamers i air, J. Phys. D: Appl. Phys. 39 (2006)

16 Cocludig remarks The drift-diffusio (fluid) model of o-thermal discharges i air has bee implemeted. Lessos leart: meshig, umerical stability, settig proper boudary coditios, optimizig solver properties, etc. Wish list : - implemetatio of a movig frame with a fie mesh for resolvig gradiets at streamer frot; - implemetatio of a high order umerical scheme or techique allowig for flux correctio; - implemetatio of fiite volume approach for drift-diffusio equatios (to preserve positivity).

17 Thak you for your attetio!!

Modeling of Plasmas and Neutrals Including Plasma-Wall Interaction for Long Term Tokamak Operation

Modeling of Plasmas and Neutrals Including Plasma-Wall Interaction for Long Term Tokamak Operation odelig of Plasmas ad Neutrals Icludig Plasma-Wall Iteractio for Log Term Tokamak Operatio Akiyoshi Hatayama 1, Kousuke Okamoto 1, Ryoko Tatsumi 1, Kazuhiro. Abe 1, ad Kazuaki Haada 2 1. Backgroud/otivatio

More information

SOLUTIONS: ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 3/27/13) e E i E T

SOLUTIONS: ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 3/27/13) e E i E T SOUIONS: ECE 606 Homework Week 7 Mark udstrom Purdue Uiversity (revised 3/27/13) 1) Cosider a - type semicoductor for which the oly states i the badgap are door levels (i.e. ( E = E D ). Begi with the

More information

Mark Lundstrom Spring SOLUTIONS: ECE 305 Homework: Week 5. Mark Lundstrom Purdue University

Mark Lundstrom Spring SOLUTIONS: ECE 305 Homework: Week 5. Mark Lundstrom Purdue University Mark udstrom Sprig 2015 SOUTIONS: ECE 305 Homework: Week 5 Mark udstrom Purdue Uiversity The followig problems cocer the Miority Carrier Diffusio Equatio (MCDE) for electros: Δ t = D Δ + G For all the

More information

FYS Vår 2016 (Kondenserte fasers fysikk)

FYS Vår 2016 (Kondenserte fasers fysikk) FYS3410 - Vår 2016 (Kodeserte fasers fysikk) http://www.uio.o/studier/emer/matat/fys/fys3410/v16/idex.html Pesum: Itroductio to Solid State Physics by Charles Kittel (Chapters 1-9 ad 17, 18, 20) Adrej

More information

Lecture 9: Diffusion, Electrostatics review, and Capacitors. Context

Lecture 9: Diffusion, Electrostatics review, and Capacitors. Context EECS 5 Sprig 4, Lecture 9 Lecture 9: Diffusio, Electrostatics review, ad Capacitors EECS 5 Sprig 4, Lecture 9 Cotext I the last lecture, we looked at the carriers i a eutral semicoductor, ad drift currets

More information

Modeling of spin-polarized transport in semiconductor nanostructures

Modeling of spin-polarized transport in semiconductor nanostructures Modelig of spi-polarized trasport i semicoductor aostructures Semio K. Saiki Uiversity of Califoria, Sa Diego Semicoductor Spitroics Advatages Electric gate cotrol Couplig to photos vs. Complicatios Electrical

More information

THE LEVEL SET METHOD APPLIED TO THREE-DIMENSIONAL DETONATION WAVE PROPAGATION. Wen Shanggang, Sun Chengwei, Zhao Feng, Chen Jun

THE LEVEL SET METHOD APPLIED TO THREE-DIMENSIONAL DETONATION WAVE PROPAGATION. Wen Shanggang, Sun Chengwei, Zhao Feng, Chen Jun THE LEVEL SET METHOD APPLIED TO THREE-DIMENSIONAL DETONATION WAVE PROPAGATION We Shaggag, Su Chegwei, Zhao Feg, Che Ju Laboratory for Shock Wave ad Detoatio Physics Research, Southwest Istitute of Fluid

More information

Finite-Difference Time-Domain Simulation of Light Propagation in 2D Periodic and Quasi-Periodic Photonic Structures

Finite-Difference Time-Domain Simulation of Light Propagation in 2D Periodic and Quasi-Periodic Photonic Structures JNS 3 (213) 359-364 Fiite-Differece Time-Domai Simulatio of Light Propagatio i 2D Periodic ad Quasi-Periodic Photoic Structures N. Dadashadeh a,b*, O.G. Romaov b a Islamic Aad Uiversity of Hadishahr, Hadishahr,

More information

Excitation of Ion Acoustic Waves in Plasmas with Electron Emission from Walls

Excitation of Ion Acoustic Waves in Plasmas with Electron Emission from Walls Excitatio of Io Acoustic Waves i Plasmas with Electro Emissio from Walls IEPC-015-340 /ISTS-015--340 Preseted at Joit Coferece of 30th Iteratioal Symposium o Space Techology ad Sciece 34th Iteratioal Electric

More information

A numerical Technique Finite Volume Method for Solving Diffusion 2D Problem

A numerical Technique Finite Volume Method for Solving Diffusion 2D Problem The Iteratioal Joural Of Egieerig d Sciece (IJES) Volume 4 Issue 10 Pages PP -35-41 2015 ISSN (e): 2319 1813 ISSN (p): 2319 1805 umerical Techique Fiite Volume Method for Solvig Diffusio 2D Problem 1 Mohammed

More information

SLAC Summer School on Electron and Photon Beams. Tor Raubenheimer Lecture #3: High Gain FEL s

SLAC Summer School on Electron and Photon Beams. Tor Raubenheimer Lecture #3: High Gain FEL s SLAC Summer School o Electro ad Photo Beams Tor Raubeheimer Lecture #3: High Gai FEL s Outlie Sychrotro radiatio Bedig magets Wigglers ad udulators Iverse Compto scatterig Free Electro Lasers FEL Oscillators

More information

Streamfunction-Vorticity Formulation

Streamfunction-Vorticity Formulation Streamfuctio-Vorticity Formulatio A. Salih Departmet of Aerospace Egieerig Idia Istitute of Space Sciece ad Techology, Thiruvaathapuram March 2013 The streamfuctio-vorticity formulatio was amog the first

More information

Finite-Difference Time-Domain Method (FDTD)

Finite-Difference Time-Domain Method (FDTD) Computatioal Photoics Semiar 05 Fiite-Differece Time-Domai Method (FDTD) Lear how to implemet a D versio of the FDTD method ted the code to 3D problems D FDTD: Yee Grid for & Compoets Chagig of ide otatio

More information

Numerical Astrophysics: hydrodynamics

Numerical Astrophysics: hydrodynamics Numerical Astrophysics: hydrodyamics Part 1: Numerical solutios to the Euler Equatios Outlie Numerical eperimets are a valuable tool to study astrophysical objects (where we ca rarely do direct eperimets).

More information

Adaptive numerical simulation of Streamer. Shailendra Singh

Adaptive numerical simulation of Streamer. Shailendra Singh Adaptive numerical simulation of Streamer Shailendra Singh Tools: BDV from Drift diffusion calculation Motivation: Streamer criteria works very well in moderately uniform field. But in highly non uniform

More information

ECE507 - Plasma Physics and Applications

ECE507 - Plasma Physics and Applications ECE57 - Pasma Physics ad Appicatios Lecture 9 Prof. Jorge Rocca ad r. Ferado Tomase epartmet of Eectrica ad Computer Egieerig Low temperature pasmas Low temperature pasmas are a very iterestig subject

More information

Free Surface Hydrodynamics

Free Surface Hydrodynamics Water Sciece ad Egieerig Free Surface Hydrodyamics y A part of Module : Hydraulics ad Hydrology Water Sciece ad Egieerig Dr. Shreedhar Maskey Seior Lecturer UNESCO-IHE Istitute for Water Educatio S. Maskey

More information

TiberCAD: : towards multiscale simulation of optoelectronic devices

TiberCAD: : towards multiscale simulation of optoelectronic devices TiberCAD: : towards multiscale simulatio of optoelectroic devices M. Auf der Maur, M. Povolotskyi, F. Saccoi, A. Pecchia, G. Romao, G. Peazzi ad Aldo Di Carlo Departmet of Electroic Egieerig, Uiversity

More information

Bohr s Atomic Model Quantum Mechanical Model

Bohr s Atomic Model Quantum Mechanical Model September 7, 0 - Summary - Itroductio to Atomic Theory Bohr s Atomic Model Quatum Mechaical Model 3- Some Defiitio 3- Projects Temperature Pressure Website Subject Areas Plasma is a Mixture of electros,

More information

Hydro code II. Simone Recchi

Hydro code II. Simone Recchi Hydro code II Simoe Recchi 16.06.2011 Literature E.F. Toro: Riema Solvers ad Numerical Methods for Fluid Dyamics, Spriger R.J. LeVeque: Fiite Volume Methods for Hyperbolic Problems, Cambridge Uiversity

More information

Recent Experimental Results in ADITYA Tokamak

Recent Experimental Results in ADITYA Tokamak Recet Experimetal Results i ADITYA Tokamak R. Jha ad the ADITYA Team Istitute for Plasma Research, Bhat, Gadhiagar-382 428, INDIA e-mail:rjha@ipr.res.i Abstract. Recet studies o measuremets of edge turbulece

More information

ECEN Microelectronics. Semiconductor Physics and P/N junctions 2/05/19

ECEN Microelectronics. Semiconductor Physics and P/N junctions 2/05/19 ECEN 3250 Microelectroics Semicoductor Physics ad P/N juctios 2/05/19 Professor J. Gopiath Professor J. Gopiath Uiversity of Colorado at Boulder Microelectroics Sprig 2014 Overview Eergy bads Atomic eergy

More information

Microscale Modelling of the Frequency Dependent Resistivity of Porous Media

Microscale Modelling of the Frequency Dependent Resistivity of Porous Media Preseted at the COMSOL Coferece 2008 Haover Microscale Modellig of the Frequecy Deedet Resistivity of Porous Media J.Volkma, N.Klitzsch, O.Mohke ad R.Blaschek Alied Geohysics ad Geothermal Eergy, E.ON

More information

Temperature-Dependent Kink Effect Model for Partially-Depleted SOI NMOS Devices

Temperature-Dependent Kink Effect Model for Partially-Depleted SOI NMOS Devices 254 IEEE RANSACIONS ON ELECRON DEVICES, VOL. 46, NO. 1, JANUARY 1999 emperature-depedet Kik Effect Model for Partially-Depleted SOI NMOS Devices S. C. Li ad J. B. Kuo Abstract his paper reports a closed-form

More information

a b c d e f g h Supplementary Information

a b c d e f g h Supplementary Information Supplemetary Iformatio a b c d e f g h Supplemetary Figure S STM images show that Dark patters are frequetly preset ad ted to accumulate. (a) mv, pa, m ; (b) mv, pa, m ; (c) mv, pa, m ; (d) mv, pa, m ;

More information

Characterization and Simulation of HF Propagation in a realistic disturbed and horizontally inhomogeneous Ionosphere

Characterization and Simulation of HF Propagation in a realistic disturbed and horizontally inhomogeneous Ionosphere Characterizatio ad Simulatio of HF Propagatio i a realistic disturbed ad horizotally ihomogeeous Ioosphere Vadim E. Gherm ad Nikolay N.Zerov Departmet of Radiophysics Uiversity of St.Petersburg St.Petersburg

More information

2.CMOS Transistor Theory

2.CMOS Transistor Theory CMOS LSI esig.cmos rasistor heory Fu yuzhuo School of microelectroics,sju Itroductio omar fadhil,baghdad outlie PN juctio priciple CMOS trasistor itroductio Ideal I- characteristics uder static coditios

More information

1. pn junction under bias 2. I-Vcharacteristics

1. pn junction under bias 2. I-Vcharacteristics Lecture 10 The p Juctio (II) 1 Cotets 1. p juctio uder bias 2. I-Vcharacteristics 2 Key questios Why does the p juctio diode exhibit curret rectificatio? Why does the juctio curret i forward bias icrease

More information

International Journal of Advance Engineering and Research Development APPLICATION OF MONTE CARLO METHOD FOR DEVICES SIMULATION

International Journal of Advance Engineering and Research Development APPLICATION OF MONTE CARLO METHOD FOR DEVICES SIMULATION Scietific Joural of Impact Factor (SJIF): 5.71 Iteratioal Joural of Advace Egieerig ad Research Developmet Volume 5, Issue 05, May -2018 e-issn (O): 2348-4470 p-issn (P): 2348-6406 APPLICATION OF MONTE

More information

DESIGN MATHEMATICAL MODEL FOR HEAT TRANSFER IN LASER BEAM WELDING PROCESS

DESIGN MATHEMATICAL MODEL FOR HEAT TRANSFER IN LASER BEAM WELDING PROCESS ARPN Joural of Egieerig ad Applied Scieces 2006-2018 Asia Research Publishig Networ (ARPN). All rights reserved. www.arpjourals.com DESIGN MATHEMATICAL MODEL FOR HEAT TRANSFER IN LASER BEAM WELDING PROCESS

More information

Numerical simulation of a climate energy balance model with continents distribution.

Numerical simulation of a climate energy balance model with continents distribution. Numerical simulatio of a climate eergy balace model with cotiets distributio. Lourdes Tello & Arturo Hidalgo Uiversidad Politécica de Madrid. Physical problem Some processes ivolved i global climate models:

More information

BER results for a narrowband multiuser receiver based on successive subtraction for M-PSK modulated signals

BER results for a narrowband multiuser receiver based on successive subtraction for M-PSK modulated signals results for a arrowbad multiuser receiver based o successive subtractio for M-PSK modulated sigals Gerard J.M. Jasse Telecomm. ad Traffic-Cotrol Systems Group Dept. of Iformatio Techology ad Systems Delft

More information

Nonequilibrium Excess Carriers in Semiconductors

Nonequilibrium Excess Carriers in Semiconductors Lecture 8 Semicoductor Physics VI Noequilibrium Excess Carriers i Semicoductors Noequilibrium coditios. Excess electros i the coductio bad ad excess holes i the valece bad Ambiolar trasort : Excess electros

More information

Multicomponent-Liquid-Fuel Vaporization with Complex Configuration

Multicomponent-Liquid-Fuel Vaporization with Complex Configuration Multicompoet-Liquid-Fuel Vaporizatio with Complex Cofiguratio William A. Sirigao Guag Wu Uiversity of Califoria, Irvie Major Goals: for multicompoet-liquid-fuel vaporizatio i a geeral geometrical situatio,

More information

Repetition: Micro Hardness

Repetition: Micro Hardness Repetitio: Micro Hardess Defied by the residual deformatio of a material due to the peetratio of a (ideally) udeformable test body. Test body material: + Diamod Test body geometries: + Vicers: Pyramid

More information

L 5 & 6: RelHydro/Basel. f(x)= ( ) f( ) ( ) ( ) ( ) n! 1! 2! 3! If the TE of f(x)= sin(x) around x 0 is: sin(x) = x - 3! 5!

L 5 & 6: RelHydro/Basel. f(x)= ( ) f( ) ( ) ( ) ( ) n! 1! 2! 3! If the TE of f(x)= sin(x) around x 0 is: sin(x) = x - 3! 5! aylor epasio: Let ƒ() be a ifiitely differetiable real fuctio. At ay poit i the eighbourhood of =0, the fuctio ca be represeted as a power series of the followig form: X 0 f(a) f() ƒ() f()= ( ) f( ) (

More information

CE 530 Molecular Simulation

CE 530 Molecular Simulation CE 530 Molecular Simulatio Lecture 5 Log-rage forces ad Ewald sum David A. Kofke Departmet of Chemical Egieerig SUNY Buffalo kofke@eg.buffalo.edu Review Itermolecular forces arise from quatum mechaics

More information

Perturbative Thermal Transport Studies on Alcator C-Mod

Perturbative Thermal Transport Studies on Alcator C-Mod Perturbative Thermal Trasport Studies o Alcator C-Mod A.J. Creely 1 A.E. White, 1 E.M. Edlud, 1 N.T. Howard, 2 A.E. Hubbard, 1 S. Houshmadyar 3 1 MIT 2 ORISE 3 UT Austi This work is supported by the US

More information

Goal. Adaptive Finite Element Methods for Non-Stationary Convection-Diffusion Problems. Outline. Differential Equation

Goal. Adaptive Finite Element Methods for Non-Stationary Convection-Diffusion Problems. Outline. Differential Equation Goal Adaptive Fiite Elemet Methods for No-Statioary Covectio-Diffusio Problems R. Verfürth Ruhr-Uiversität Bochum www.ruhr-ui-bochum.de/um1 Tübige / July 0th, 017 Preset space-time adaptive fiite elemet

More information

Lecture 5: HBT DC Properties. Basic operation of a (Heterojunction) Bipolar Transistor

Lecture 5: HBT DC Properties. Basic operation of a (Heterojunction) Bipolar Transistor Lecture 5: HT C Properties asic operatio of a (Heterojuctio) ipolar Trasistor Abrupt ad graded juctios ase curret compoets Quasi-Electric Field Readig Guide: 143-16: 17-177 1 P p ++.53 Ga.47 As.53 Ga.47

More information

Monte Carlo Optimization to Solve a Two-Dimensional Inverse Heat Conduction Problem

Monte Carlo Optimization to Solve a Two-Dimensional Inverse Heat Conduction Problem Australia Joural of Basic Applied Scieces, 5(): 097-05, 0 ISSN 99-878 Mote Carlo Optimizatio to Solve a Two-Dimesioal Iverse Heat Coductio Problem M Ebrahimi Departmet of Mathematics, Karaj Brach, Islamic

More information

NUMERICAL INVESTIGATION OF FEEDBACK CONTROL IN PLASMA PROCESSING REACTORS INTRODUCTION

NUMERICAL INVESTIGATION OF FEEDBACK CONTROL IN PLASMA PROCESSING REACTORS INTRODUCTION NUMERICAL INVESTIGATION OF FEEDBACK CONTROL IN PLASMA PROCESSING REACTORS Shahid Rauf ad Mark J. Kusher Departmet of Electrical ad Computer Egieerig Uiversity of Illiois 1406 W. Gree Street, Urbaa, Illiois

More information

CO-LOCATED DIFFUSE APPROXIMATION METHOD FOR TWO DIMENSIONAL INCOMPRESSIBLE CHANNEL FLOWS

CO-LOCATED DIFFUSE APPROXIMATION METHOD FOR TWO DIMENSIONAL INCOMPRESSIBLE CHANNEL FLOWS CO-LOCATED DIFFUSE APPROXIMATION METHOD FOR TWO DIMENSIONAL INCOMPRESSIBLE CHANNEL FLOWS C.PRAX ad H.SADAT Laboratoire d'etudes Thermiques,URA CNRS 403 40, Aveue du Recteur Pieau 86022 Poitiers Cedex,

More information

Hot electrons and curves of constant gain in long wavelength quantum well lasers

Hot electrons and curves of constant gain in long wavelength quantum well lasers Hot electros ad curves of costat gai i log wavelegth quatum well lasers Vera Gorfikel, Mikhail Kisi ad Serge Luryi Electrical Egieerig Departmet State Uiversity of New York at Stoy Brook Stoy Brook, NY

More information

Semiconductors a brief introduction

Semiconductors a brief introduction Semicoductors a brief itroductio Bad structure from atom to crystal Fermi level carrier cocetratio Dopig Readig: (Sedra/Smith 7 th editio) 1.7-1.9 Trasport (drift-diffusio) Hyperphysics (lik o course homepage)

More information

Exponential transient rotating waves and their bifurcations in a ring of unidirectionally coupled bistable Lorenz systems

Exponential transient rotating waves and their bifurcations in a ring of unidirectionally coupled bistable Lorenz systems Available olie at www.sciecedirect.com Procedia IUTAM 5 (2012 ) 283 287 IUTAM Symposium o 50 Years of Chaos: Applied ad Theoretical Expoetial trasiet rotatig waves ad their bifurcatios i a rig of uidirectioally

More information

Summary of pn-junction (Lec )

Summary of pn-junction (Lec ) Lecture #12 OUTLNE Diode aalysis ad applicatios cotiued The MOFET The MOFET as a cotrolled resistor Pich-off ad curret saturatio Chael-legth modulatio Velocity saturatio i a short-chael MOFET Readig Howe

More information

NEUTRON FLUX MEASUREMENT UTILIZING CAMPBELL TECHNIQUE

NEUTRON FLUX MEASUREMENT UTILIZING CAMPBELL TECHNIQUE Iteratioal Coferece Nuclear Eergy i Cetral Europe 000 Golf Hotel, Bled, Sloveia, September 11-14, 000 NEUTRON FLUX MEASUREMENT UTILIZING CAMPBELL TECHNIQUE Marti Kropík Departmet of Nuclear Reactors Faculty

More information

Free Radical Polymerization

Free Radical Polymerization Free Radical Polymerizatio Referece: Aspe Polymers: Uit Operatios ad Reactio Models, Aspe Techology, Ic., 2013. 1. Itroductio The free-radical bulk/solutio polymerizatio model is applicable to bulk ad

More information

Approaching ballistic transport in suspended graphene. Supplementary Information

Approaching ballistic transport in suspended graphene. Supplementary Information Approachig ballistic trasport i suspeded graphee Xu Du, Iva Skachko, Athoy Barker, Eva Y. Adrei Departmet of Physics & Astroomy, Rutgers the State Uiversity of New Jersey Cotets Supplemetary Iformatio

More information

Microscopic traffic flow modeling

Microscopic traffic flow modeling Chapter 34 Microscopic traffic flow modelig 34.1 Overview Macroscopic modelig looks at traffic flow from a global perspective, whereas microscopic modelig, as the term suggests, gives attetio to the details

More information

True Nature of Potential Energy of a Hydrogen Atom

True Nature of Potential Energy of a Hydrogen Atom True Nature of Potetial Eergy of a Hydroge Atom Koshu Suto Key words: Bohr Radius, Potetial Eergy, Rest Mass Eergy, Classical Electro Radius PACS codes: 365Sq, 365-w, 33+p Abstract I cosiderig the potetial

More information

Chapter 7 z-transform

Chapter 7 z-transform Chapter 7 -Trasform Itroductio Trasform Uilateral Trasform Properties Uilateral Trasform Iversio of Uilateral Trasform Determiig the Frequecy Respose from Poles ad Zeros Itroductio Role i Discrete-Time

More information

Lecture 10: P-N Diodes. Announcements

Lecture 10: P-N Diodes. Announcements EECS 15 Sprig 4, Lecture 1 Lecture 1: P-N Diodes EECS 15 Sprig 4, Lecture 1 Aoucemets The Thursday lab sectio will be moved a hour later startig this week, so that the TA s ca atted lecture i aother class

More information

Applied Mathematical Modelling

Applied Mathematical Modelling Applied Mathematical Modellig 37 (013) 1177 1186 Cotets lists available at SciVerse ScieceDirect Applied Mathematical Modellig joural homepage: www.elsevier.com/locate/apm The effective permeability of

More information

Numerical Schemes to Solve Advective Contaminant Transport Problems with Linear Sorption and First Order Decay

Numerical Schemes to Solve Advective Contaminant Transport Problems with Linear Sorption and First Order Decay Numerical Schemes to Solve Advective Cotamiat Trasport Problems with Liear Sorptio ad First Order Decay Adré Luís Brasil Cavalcate PhD, Associate Professor, Uiversity of Brasilia, Brazil, Departmet of

More information

Analysis of composites with multiple rigid-line reinforcements by the BEM

Analysis of composites with multiple rigid-line reinforcements by the BEM Aalysis of composites with multiple rigid-lie reiforcemets by the BEM Piotr Fedeliski* Departmet of Stregth of Materials ad Computatioal Mechaics, Silesia Uiversity of Techology ul. Koarskiego 18A, 44-100

More information

Repetition: Refractive Index

Repetition: Refractive Index Repetitio: Refractive Idex (ω) κ(ω) 1 0 ω 0 ω 0 The real part of the refractive idex correspods to refractive idex, as it appears i Sellius law of refractio. The imagiary part correspods to the absorptio

More information

An Efficient Technique for the Optimization of Submillimeter-wave Schottky-diode Harmonic Multipliers

An Efficient Technique for the Optimization of Submillimeter-wave Schottky-diode Harmonic Multipliers A Efficiet Techique for the Optimizatio of Submillimeter-wave Schottky-diode Harmoic Multipliers Chih-Chie Lee 1, Boris Gelmot 1 ad Dwight Woolard 1 The Uiversity of Virgiia U.S. Army Research Laboratory

More information

Numerical simulation of two-phase Darcy-Forchheimer flow during CO 2 injection into deep saline aquifers. Andi Zhang Feb. 4, 2013

Numerical simulation of two-phase Darcy-Forchheimer flow during CO 2 injection into deep saline aquifers. Andi Zhang Feb. 4, 2013 Numerical simulatio of two-phase Darcy-Forchheimer flow durig CO 2 ijectio ito deep salie aquifers Adi Zhag Feb. 4, 2013 Darcy flow VS o-darcy flow Darcy flow A liear relatioship betwee volumetric flow

More information

577. Estimation of surface roughness using high frequency vibrations

577. Estimation of surface roughness using high frequency vibrations 577. Estimatio of surface roughess usig high frequecy vibratios V. Augutis, M. Sauoris, Kauas Uiversity of Techology Electroics ad Measuremets Systems Departmet Studetu str. 5-443, LT-5368 Kauas, Lithuaia

More information

D. A. D Ippolito, J. R. Myra, and D. A. Russell Lodestar Research Corporation

D. A. D Ippolito, J. R. Myra, and D. A. Russell Lodestar Research Corporation D. A. D Ippolito, J. R. Myra, ad D. A. Russell Research Corporatio Preseted at the 33rd EPS Coferece o Plasma Physics, Rome, Italy, Jue 9-3, 6 Coheret structures ( blobs ) created by edge turbulece covective

More information

The aim of the course is to give an introduction to semiconductor device physics. The syllabus for the course is:

The aim of the course is to give an introduction to semiconductor device physics. The syllabus for the course is: Semicoductor evices Prof. Rb Robert tat A. Taylor The aim of the course is to give a itroductio to semicoductor device physics. The syllabus for the course is: Simple treatmet of p- juctio, p- ad p-i-

More information

Chapter 2 Motion and Recombination of Electrons and Holes

Chapter 2 Motion and Recombination of Electrons and Holes Chapter 2 Motio ad Recombiatio of Electros ad Holes 2.1 Thermal Eergy ad Thermal Velocity Average electro or hole kietic eergy 3 2 kt 1 2 2 mv th v th 3kT m eff 3 23 1.38 10 JK 0.26 9.1 10 1 31 300 kg

More information

Supplementary Information: Flexible and tunable silicon photonic circuits on plastic substrates

Supplementary Information: Flexible and tunable silicon photonic circuits on plastic substrates Supplemetary Iformatio: Flexible ad tuable silico photoic circuits o plastic substrates Yu Che 1, Hua Li 1, ad Mo Li 11 1 Departmet of Electrical ad Computer Egieerig, Uiversity of Miesota, Mieapolis,

More information

Chapter 2 Motion and Recombination of Electrons and Holes

Chapter 2 Motion and Recombination of Electrons and Holes Chapter 2 Motio ad Recombiatio of Electros ad Holes 2.1 Thermal Motio 3 1 2 Average electro or hole kietic eergy kt mv th 2 2 v th 3kT m eff 23 3 1.38 10 JK 0.26 9.1 10 1 31 300 kg K 5 7 2.310 m/s 2.310

More information

THE FRACTAL TECHNIQUES APPLIED IN NUMERICAL ITERATIVE METHODS FRAME

THE FRACTAL TECHNIQUES APPLIED IN NUMERICAL ITERATIVE METHODS FRAME 6 th INTERNATIONAL MULTIDISCIPLINARY CONFERENCE THE FRACTAL TECHNIQUES APPLIED IN NUMERICAL ITERATIVE METHODS FRAME George MAHALU, Radu PENTIUC Uiversity of Suceava - mahalu@eed.usv.ro Abstract: May methods

More information

Effect of Temperature Variations on Strain Response of Polymer Bragg Grating Optical Fibers

Effect of Temperature Variations on Strain Response of Polymer Bragg Grating Optical Fibers Iraq J. Electrical ad Electroic Egieerig Vol.13 No.1, 17 مجلد 13 العدد 17 1 Effect of Temperature Variatios o Strai Respose of Polymer Bragg Gratig Optical Fibers Hisham K. Hisham Electrical Egieerig Departmet,

More information

Finite Difference Approximation for First- Order Hyperbolic Partial Differential Equation Arising in Neuronal Variability with Shifts

Finite Difference Approximation for First- Order Hyperbolic Partial Differential Equation Arising in Neuronal Variability with Shifts Iteratioal Joural of Scietific Egieerig ad Research (IJSER) wwwiseri ISSN (Olie): 347-3878, Impact Factor (4): 35 Fiite Differece Approimatio for First- Order Hyperbolic Partial Differetial Equatio Arisig

More information

Visco-acoustic Reverse-time Migration Using the Pseudo-analytical Method

Visco-acoustic Reverse-time Migration Using the Pseudo-analytical Method Visco-acoustic Reverse-time Migratio Usig the Pseudo-aalytical Method J. Ramos-Martiez* (Petroleum Geo-Services), A.A. Valeciao (Petroleum Geo-Services) & M. Orlovich (Petroleum Geo-Services) SUMMARY We

More information

EE 485 Introduction to Photonics Photon Optics and Photon Statistics

EE 485 Introduction to Photonics Photon Optics and Photon Statistics Itroductio to Photoics Photo Optics ad Photo Statistics Historical Origi Photo-electric Effect (Eistei, 905) Clea metal V stop Differet metals, same slope Light I Slope h/q ν c/λ Curret flows for λ < λ

More information

METHOD OF FUNDAMENTAL SOLUTIONS FOR HELMHOLTZ EIGENVALUE PROBLEMS IN ELLIPTICAL DOMAINS

METHOD OF FUNDAMENTAL SOLUTIONS FOR HELMHOLTZ EIGENVALUE PROBLEMS IN ELLIPTICAL DOMAINS Please cite this article as: Staisław Kula, Method of fudametal solutios for Helmholtz eigevalue problems i elliptical domais, Scietific Research of the Istitute of Mathematics ad Computer Sciece, 009,

More information

Velocity and Temperature Boundary- Layer Modeling Using Averaged Molecule cluster Transport Equations

Velocity and Temperature Boundary- Layer Modeling Using Averaged Molecule cluster Transport Equations IUVSTA 011 Leiseiler, May 16 th 011 Velocity ad Temperature Boudary- Layer Modelig Usig Averaged Molecule cluster Trasport Equatios R. Groll Uiversity of Breme, Am Fallturm, D-859 Breme R. Groll 1 Micro

More information

3D Numerical Analysis of the Unsteady Turbulent Swirling Flow in a Conical Diffuser using FLUENT and OpenFOAM

3D Numerical Analysis of the Unsteady Turbulent Swirling Flow in a Conical Diffuser using FLUENT and OpenFOAM 3D Numerical Aalysis of the Usteady Turbulet Swirlig Flow i a Coical Diffuser usig FLUENT ad OpeFOAM Sebastia Mutea, Seior Researcher, Håka Nilsso, Associate Professor, Chalmers Techology, Gotheburg Romeo

More information

THE POTENTIALS METHOD FOR A CLOSED QUEUEING SYSTEM WITH HYSTERETIC STRATEGY OF THE SERVICE TIME CHANGE

THE POTENTIALS METHOD FOR A CLOSED QUEUEING SYSTEM WITH HYSTERETIC STRATEGY OF THE SERVICE TIME CHANGE Joural of Applied Mathematics ad Computatioal Mechaics 5, 4(), 3-43 www.amcm.pcz.pl p-issn 99-9965 DOI:.75/amcm.5..4 e-issn 353-588 THE POTENTIALS METHOD FOR A CLOSED QUEUEING SYSTEM WITH HYSTERETIC STRATEGY

More information

Stellar Helium Burning. He-Burning in massive Stars

Stellar Helium Burning. He-Burning in massive Stars Stellar lium Burig -Burig i massive Stars -burig is igited o the ad ashes of the precedig hydroge burig phase! Most importat reactio -triple alpha process 3 12 C 7.96 MeV Eergy productio i helium burig

More information

PROBE MEASUREMENTS IN DISCHARGE CHAMBER OF LOW- POWER ION THRUSTER

PROBE MEASUREMENTS IN DISCHARGE CHAMBER OF LOW- POWER ION THRUSTER PROBE MEASUREMENTS IN DISCHARGE CHAMBER OF LOW- POWER ION THRUSTER M.V. Zikeyev, ad A.A. Shagayda Keldysh Research Ceter 125438, Rusa, Moscow, Oezhskaya, 8/10, Tel: 007-095-456-7582 Fax: 007-095-456-8228

More information

Taylor expansion: Show that the TE of f(x)= sin(x) around. sin(x) = x - + 3! 5! L 7 & 8: MHD/ZAH

Taylor expansion: Show that the TE of f(x)= sin(x) around. sin(x) = x - + 3! 5! L 7 & 8: MHD/ZAH Taylor epasio: Let ƒ() be a ifiitely differetiable real fuctio. A ay poit i the eighbourhood of 0, the fuctio ƒ() ca be represeted by a power series of the followig form: X 0 f(a) f() f() ( ) f( ) ( )

More information

Accuracy of TEXTOR He-beam diagnostics

Accuracy of TEXTOR He-beam diagnostics Accuracy of TEXTOR He-beam diagostics O. Schmitz, I.L.Beigma *, L.A. Vaishtei *, A. Pospieszczyk, B. Schweer, M. Krychoviak, U. Samm ad the TEXTOR team Forschugszetrum Jülich,, Jülich, Germay *Lebedev

More information

The z-transform. 7.1 Introduction. 7.2 The z-transform Derivation of the z-transform: x[n] = z n LTI system, h[n] z = re j

The z-transform. 7.1 Introduction. 7.2 The z-transform Derivation of the z-transform: x[n] = z n LTI system, h[n] z = re j The -Trasform 7. Itroductio Geeralie the complex siusoidal represetatio offered by DTFT to a represetatio of complex expoetial sigals. Obtai more geeral characteristics for discrete-time LTI systems. 7.

More information

Chapter 7: The z-transform. Chih-Wei Liu

Chapter 7: The z-transform. Chih-Wei Liu Chapter 7: The -Trasform Chih-Wei Liu Outlie Itroductio The -Trasform Properties of the Regio of Covergece Properties of the -Trasform Iversio of the -Trasform The Trasfer Fuctio Causality ad Stability

More information

CSIR-UGC-NET/JRF Jue 0 CSIR-UGC NET/JRF JUNE - 0 PHYSICAL SCIENCES BOOKLET - [A] PART - B. A particle of uit mass moves i a potetial V x b ax, where a ad b are positive costats. x The agular frequecy of

More information

Improved Perfectly Matched Layers for Acoustic Radiation and Scattering Problems

Improved Perfectly Matched Layers for Acoustic Radiation and Scattering Problems Excerpt from the Proceedigs of the COMSOL Coferece 2008 Haover Improved Perfectly Matched Layers for Acoustic Radiatio ad Scatterig Problems Mario Zampolli *,1, Nils Malm 2, Alessadra Tesei 1 1 NURC NATO

More information

Numerical Simulation of Thermomechanical Problems in Applied Mechanics: Application to Solidification Problem

Numerical Simulation of Thermomechanical Problems in Applied Mechanics: Application to Solidification Problem Leoardo Joural of Scieces ISSN 1583-0233 Issue 9, July-December 2006 p. 25-32 Numerical Simulatio of Thermomechaical Problems i Applied Mechaics: Applicatio to Solidificatio Problem Vicet Obiajulu OGWUAGWU

More information

THE NUMERICAL SOLUTION OF THE NEWTONIAN FLUIDS FLOW DUE TO A STRETCHING CYLINDER BY SOR ITERATIVE PROCEDURE ABSTRACT

THE NUMERICAL SOLUTION OF THE NEWTONIAN FLUIDS FLOW DUE TO A STRETCHING CYLINDER BY SOR ITERATIVE PROCEDURE ABSTRACT Europea Joural of Egieerig ad Techology Vol. 3 No., 5 ISSN 56-586 THE NUMERICAL SOLUTION OF THE NEWTONIAN FLUIDS FLOW DUE TO A STRETCHING CYLINDER BY SOR ITERATIVE PROCEDURE Atif Nazir, Tahir Mahmood ad

More information

Potential-based Fracture Mechanics Using Cohesive Zone and Virtual Internal Bond Modeling

Potential-based Fracture Mechanics Using Cohesive Zone and Virtual Internal Bond Modeling Dissertatio Defese Potetial-based Fracture Mechaics Usig Cohesive Zoe ad Virtual Iteral Bod Modelig Kyougsoo Park 7/21/2009 Advisor/Co-advisor: Glaucio H. Paulio / Jeffery R. Roesler Departmet of Civil

More information

The Chan-Vese Algorithm

The Chan-Vese Algorithm The Cha-Vese Algorithm Proect Report Rami Cohe, rc@tx.techio.ac.il Itroductio to Medical Imagig, Sprig 010 Techio, Israel Istitute of Techology This report is accompaied by a MATLAB package that ca be

More information

Finite Difference Approximation for Transport Equation with Shifts Arising in Neuronal Variability

Finite Difference Approximation for Transport Equation with Shifts Arising in Neuronal Variability Iteratioal Joural of Sciece ad Research (IJSR) ISSN (Olie): 39-764 Ide Copericus Value (3): 64 Impact Factor (3): 4438 Fiite Differece Approimatio for Trasport Equatio with Shifts Arisig i Neuroal Variability

More information

Lecture 8: Solving the Heat, Laplace and Wave equations using finite difference methods

Lecture 8: Solving the Heat, Laplace and Wave equations using finite difference methods Itroductory lecture otes o Partial Differetial Equatios - c Athoy Peirce. Not to be copied, used, or revised without explicit writte permissio from the copyright ower. 1 Lecture 8: Solvig the Heat, Laplace

More information

Applications of Distributed Arithmetic to Digital Signal Processing: A Tutorial Review

Applications of Distributed Arithmetic to Digital Signal Processing: A Tutorial Review pplicatios of Distriuted rithmetic to Digital Sigal Processig: Tutorial Review Ref: Staley. White, pplicatios of Distriuted rithmetic to Digital Sigal Processig: Tutorial Review, IEEE SSP Magazie, July,

More information

PC5215 Numerical Recipes with Applications - Review Problems

PC5215 Numerical Recipes with Applications - Review Problems PC55 Numerical Recipes with Applicatios - Review Problems Give the IEEE 754 sigle precisio bit patter (biary or he format) of the followig umbers: 0 0 05 00 0 00 Note that it has 8 bits for the epoet,

More information

Quantum Simulation: Solving Schrödinger Equation on a Quantum Computer

Quantum Simulation: Solving Schrödinger Equation on a Quantum Computer Purdue Uiversity Purdue e-pubs Birc Poster Sessios Birc Naotechology Ceter 4-14-008 Quatum Simulatio: Solvig Schrödiger Equatio o a Quatum Computer Hefeg Wag Purdue Uiversity, wag10@purdue.edu Sabre Kais

More information

Modeling of Finite Gradient Elasticity Using Optimal Transportation Method

Modeling of Finite Gradient Elasticity Using Optimal Transportation Method 9 th Iteratioal Cogress of Croatia Society of Mechaics 18-22 September 2018 Split, Croatia Modelig of Fiite Gradiet Elasticity Usig Optimal Trasportatio Method Boris JALUŠIĆ *, Christia WEIßENFELS +, Jurica

More information

Analysis of MOS Capacitor Loaded Annular Ring MICROSTRIP Antenna

Analysis of MOS Capacitor Loaded Annular Ring MICROSTRIP Antenna Iteratioal OPEN AESS Joural Of Moder Egieerig Research (IJMER Aalysis of MOS apacitor Loaded Aular Rig MIROSTRIP Atea Mohit Kumar, Suredra Kumar, Devedra Kumar 3, Ravi Kumar 4,, 3, 4 (Assistat Professor,

More information

Collisional Ionization in Lithium Vapor Excited by Nanosecond Laser Pulses

Collisional Ionization in Lithium Vapor Excited by Nanosecond Laser Pulses Vol. 122 (2012) ACTA PHYSICA POLONICA A No. 1 Collisioal Ioizatio i Lithium Vapor Excited by Naosecod Laser Pulses M.A. Mahmoud, A. El Tabal ad M. Nady Physics Departmet, Faculty of Sciece, Sohag Uiversity,

More information

Reading. Required: Witkin, Particle System Dynamics, SIGGRAPH 97 course notes on Physically Based Modeling.

Reading. Required: Witkin, Particle System Dynamics, SIGGRAPH 97 course notes on Physically Based Modeling. Particle Systems Readig Required: Witki, Particle System Dyamics, SIGGRAPH 97 course otes o Physically Based Modelig. Optioal Witki ad Baraff, Differetial Equatio Basics, SIGGRAPH 97 course otes o Physically

More information

Transmission Line on Semiconductor Substrate with Distributed Amplification

Transmission Line on Semiconductor Substrate with Distributed Amplification RAIONGINRING, VOL. 19, NO. 2, JUN 21 37 Trasmissio Lie o Semicoductor Substrate with istributed Amplificatio Michal POKORNÝ, Zbyěk RAIA epartmet of Radio lectroics, Bro Uiversity of Techology, Purkyňova

More information

Lecture #1 Nasser S. Alzayed.

Lecture #1 Nasser S. Alzayed. Lecture #1 Nasser S. Alzayed alzayed@ksu.edu.sa Chapter 6: Free Electro Fermi Gas Itroductio We ca uderstad may physical properties of metals, ad ot oly of the simple metals, i terms of the free electro

More information

THE SIMULATION OF PHOTOVOLTAIC-INTEGRATED BUILDING FACADES

THE SIMULATION OF PHOTOVOLTAIC-INTEGRATED BUILDING FACADES THE SIMULATION OF PHOTOVOLTAIC-INTEGRATED BUILDING FACADES Clarke J A, Johstoe C, Kelly N # ad Stracha P A ESRU, Dept. of Mechaical Egieerig, Uiversity of Strathclyde, Glasgow, Scotlad) ( # ow at Buildig

More information

Simulation of Dynamic BAN Channel for Navel to Arm Links Based on Antenna Motion

Simulation of Dynamic BAN Channel for Navel to Arm Links Based on Antenna Motion Simulatio of Dyamic BAN Chael for Navel to Arm Liks Based o Atea Motio Iswadi, Miseok Kim, Ju-ichi Takada, Takahiro Aoyagi Graduate School of Sciece ad Egieerig Tokyo Istitute of Techology Outlie Itroductio

More information