All Particle Simulation of a Cathodic Arc Plasma I.J. Cooper D. R. McKenzie Tim Ruppin and Andrew Rigby.

Slides:



Advertisements
Similar presentations
Outline Curriculum (5 lectures) Each lecture  45 minutes
Advertisements

States of matter and thermodynamics
Chapter 17 Direct currents
Plasma Window Options and Opportunities for Inertial Fusion Applications Leslie Bromberg Ady Herskovitch* MIT Plasma Science and Fusion Center ARIES meeting.
Electric Forces Mr. Burns
Imperial College London 1 3. Beam extraction 3. Extraction of particle beams 3.1 The space charge limit and Child-Langmuirs law 3.2 External and internal.
Discharge Lamps Chapter 14 part2 1020C.
STARTING MECHANISMS FOR HIGH PRESSURE METAL HALIDE LAMPS * Brian Lay**, Sang-Hoon Cho and Mark J. Kushner University of Illinois Department of Electrical.
Unit 12 Conduction in Liquids and Gases
General Characteristics of Gas Detectors
PS – TEST 8TH GRADE SCIENCE.
Physics definitions. Acceleration Is the rate of change in velocity of an object divided by the time taken for the change. It is measured in ms-2.
Electrostatic principles. Field pattern in a capacitor Field strength = V/d Volts per metre (voltage gradient)
Chapter 16 Section 1 Kinetic Theory.
W. Udo Schröder, 2004 Instrumentation 1. W. Udo Schröder, 2004 Instrumentation 2 Probes for Nuclear Processes To “see” an object, the wavelength of the.
1 Introduction to Plasma Immersion Ion Implantation Technologies Emmanuel Wirth.
Plasma Kinetics around a Dust Grain in an Ion Flow N F Cramer and S V Vladimirov, School of Physics, University of Sydney, S A Maiorov, General Physics.
Day 19: Electrostatic Potential Energy & CRT Applications
Electricity. Composition of matter Electrical Charge Current flow Voltage Source Cells & Batteries Resistance & Conductance Electric Circuits.
By Ollie Docherty and Lauren Moore. Heat energy can move through a substance by conduction. Metals are good conductors of heat, but non-metals and gases.
Water Water water everywhere. The structure of Water 1. It can be quite correctly argued that life only exists on Earth because of the abundance of liquid.
What is plasma? Plasma is an ionized gas comprising molecules,atoms, ions ( in their ground or excited states) electrons and photons. It is electrically.
Refining of Liquid Metal by Hydrogen Cold Plasma Shanghai University Weizhong Ding School of Material Science and Engineering Shanghai University.
Means & Methods of Homogeneous Charge Combustion P M V Subbarao Professor Mechanical Engineering Department A Sudden Combustion, Yet Needs A Care & takes.
Electrochemistry Experiment 12. Oxidation – Reduction Reactions Consider the reaction of Copper wire and AgNO 3 (aq) AgNO 3 (aq) Ag(s) Cu(s)
Chapter 27 Current and Resistance Scalar Sense determined by the movement of the positive charge carrier Average Electric Current Instantaneous Electric.
Plasmas. The “Fourth State” of the Matter The matter in “ordinary” conditions presents itself in three fundamental states of aggregation: solid, liquid.
Matter and Atomic Structure Section 3.3- State of Matter
18.1b Notes States of Matter & Phase Changes Supplement to Chapter 18.
The electron.  An indivisible quantity of charge that orbits the nucleus of the atom.
Temperature and Heat   Temperature and Thermometers   Is it hot or cold?   Mercury vs. alcohol Expansion or contraction of a material   Electrical.
Electricity Basics of electricity. Electricity Atoms – The smallest unit of each element Electrons – negatively charged particles in atoms Ions – charged.
Ideal currents in a pn Junction
Thermionic Valves.
-Plasma can be produced when a laser ionizes gas molecules in a medium -Normally, ordinary gases are transparent to electromagnetic radiation. Why then.
2 pt 3 pt 4 pt 5pt 1 pt 2 pt 3 pt 4 pt 5 pt 1 pt 2pt 3 pt 4pt 5 pt 1pt 2pt 3 pt 4 pt 5 pt 1 pt 2 pt 3 pt 4pt 5 pt 1pt Hot, hot, hot Baby, it’s cold outside.
An Estimation of Critical Electron Density at Just Starting Breakdown in Gases Mase. H Professor Emeritus of Ibaraki University.
Methods of Heat Transfer. List as many Methods of Heat Transfer.
Thermal Energy & Heat 1.Temperature – The measure of the average kinetic energy of the particles that make up a substance. 2.Temperature Scales – Fahrenheit,
Chemistry Unit 2 States of Matter and Specific Heat.
 Has fixed volume  Has fixed shape  Molecules are held in specific locations  by electrical forces  vibrate about equilibrium positions  Can be.
 Total energy in molecules of a substance including  a) kinetic E of moving molecules  b) potential E stored in chemical bonds.
Lecture 5 Heat Transfer –Conduction –Convection –Radiation Phase Changes.
Design of Ignition System for SI Engines P M V Subbarao Professor Mechanical Engineering Department A Successful Ignition leads to Efficient Combustion…
Copyright © 2009 Pearson Education, Inc. E Determined from V.
Production of nanomaterials
SPES Target Group Data…… INFN-CISAS-CNR collaboration The Ablation Ion Source for refractory metal ion beams A preliminary design.
DC Sputtering Disadvantage #1 Low secondary electron yield
Thermal Energy Transfer
States of Matter Matter commonly occurs in one of three “states”
DOE Plasma Science Center Control of Plasma Kinetics
Chapter 3 Plasma as fluids
SIMULATIONS OF HIGH-PRESSURE CATHODIC
Heat, Temperature & Specific Heat
Changes of State Page 23 Learning Target: I can explain how matter changes states when thermal energy is added or removed. Respond to LT: (Leave Space.
ArcPIC2D update: Arc spreading through flat emission Kyrre N
Temperature and Heat.
Thermal Energy Transfer
ELECTRIC FIELD VECTOR MEASUREMENTS
GENERATION OF NOVEL EEDFS IN A TANDEM PLASMA REACTOR
CONTROL OF VOLTAGE PLASMA OSCILLATIONS IN A DC
A complete circuit is required for electric current to flow
Plasma Arc / Jet Machining / Cutting
Temperature Is a property of an object which determines the direction of net heat flow when an object is placed in contact with some other object. Heat.
Basic Principles for Design of Ignition Systems
An Atom (Neil Bohr model
Thermionic Emission – Learning Outcomes
States of Matter.
Heat.
Presentation transcript:

All Particle Simulation of a Cathodic Arc Plasma I.J. Cooper D. R. McKenzie Tim Ruppin and Andrew Rigby

Traces left by an arc on tungsten cathode

3 Vacuum Arc High Current, Low Voltage discharge in vacuum ambient Current conducted in metal vapor plasma produced by discharge itself from evaporated electrode material Usually plasma production concentrated at cathode spots

Ion flow  rapid heating of micro- protrusion  shock wave traveling to base  explosion of micro- protrusion Liquid drops, energetic electrons, ions and atoms ejected from cathode leaving a micro-crater Atoms ionized by electron impact or if density sufficient, self ionization Time Evolution of Cathode Spot Cell Expanding hot dense plasma cell in non- thermal equilibrium layer New ion flow to cathode Ion flow to anode Micro-protrusions on cathode surface

Cathodic arc plasma  Subspots (fragments)  Cells  Initial confinement of plasma L = 1×10 -8 m V = 1× m 3 Number of ions 10 to 100 Density max ~ ions.m 3 Hot e - T e =3x10 4 K Cold ions

All particle N body simulation Coulomb forces between electrons and ions U p > 0 U e > 0 U pe < 0

r(i, j, t) small  problems r(i, j, t)  r(i, j, t) +  Problem: Lots of particles – lots of calculations

Can modify equations to include external electric and magnetic fields x j (t+1): q j E x  t 2 F B = q v x B B x =0, B y = 0, B z v z = 0 x(t+1): G 2 [2x(t) + (G )x(t-1) + 2G 1 y(t) – 2G 1 y(t-1)] G 1 =  t B z /2m G 2 = 1 / (1+G 1 2 )

Software MATLAB slow need to remove loops by using array operations qq = meshgrid(q,q) xx = meshgrid(x_1,x_1); yy = meshgrid(y_1,y_1); zz = meshgrid(z_1,z_1); xd = xx - xx'; yd = yy - yy'; zd = zz - zz'; rd = sqrt(xd.^2 + yd.^2 + zd.^2); rd = rd + rdMin; rd3 = rd.^3; Sx = (qq.*xd)./rd3; Sy = (qq.*yd)./rd3; Sz = (qq.*zd)./rd3; SSx = -A2.* sum(Sx'); SSy = -A2.* sum(Sy'); SSz = -A2.* sum(Sz'); xfp = 2.*x_1 - x_2 + SSx; yfp = 2.*y_1 - y_2 + SSy; zfp = 2.*z_1 - z_2 + SSz; For each time step  t ~ 1x s N steps ~ 10 7 :

SIMULATIONS single, multiple and mixed charged states H C Ti 10 ps 50 Ti + 50 e -

10 ps 100 Ti e -

10 ps 100 Ti e -

0.10 ps 50 Ti + 50 e -

10 ps 50 ions 50 e -

10 ps 100 Ti e -

10 ps 100 Ti e -

10 ps 100 Ti e -

10 ps ion.m -3  K avg ~ 3.8 eV K avg(real) ~ 60 eV  ion.m -3

Initial Volume (m 3 ) Initial Ion density (ion.m -3 ) No. of e - No. of Ti ions Average ion KE (eV) 1.0× × Ti  × × Ti  × × Ti  × × Ti + 10 Ti Ti    1.6

10 ps R = Ti 2+ / Ti +