Understanding the Formation of Magnetic Field And

Total Page:16

File Type:pdf, Size:1020Kb

Understanding the Formation of Magnetic Field And UNDERSTANDING THE FORMATION OF MAGNETIC FIELD AND PLASMA STRUCTURES IN THE MAGNETOTAIL VIA THE RECONNECTION PROCESS Segheen Beyene Mullard Space Science Laboratory Department of Space and Climate Physics University College London A thesis submitted to UCL for the degree of Doctor of Philosophy March 2013 1 I, Segheen Beyene, 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. Signed: The first study of the thesis has been previously published: Beyene, S., Owen, C. J., Walsh, A. P., Forsyth, C., Fazakerley, A. N., Kiehas, S., Dandouras, I., and Lucek, E.: Cluster observations of a transient signature in the magnetotail: implications for the mode of reconnection, Ann. Geophys., 29, 2131-2146, doi:10.5194/angeo-29-2131-2011, 2011 2 Abstract This thesis studies the formation of products of magnetotail reconnection using models and observations. Three studies are presented, the first is an analysis of observations from the Cluster spacecraft, located in different regions of the magnetotail, which allow simultaneous sampling of a Travelling Compression Region (TCR) in the lobe and the underlying magnetic structure in the plasma sheet causing it. Previous work suggests that these structures are created by either single-X-line time-dependent reconnection, forming a flux-bulge, or multiple-X-line reconnection, forming a flux-rope. The observations are analysed and compared to the predictions of these models to determine which mode of reconnection created the structure. The second study presents an adaptation to a single particle model of time- dependent reconnection in the magnetotail previously published by Owen and Cowley (1987). This new model relaxes the cold plasma approximation and assesses the stress balance conditions on reconnected field lines threading the current sheet when the outflow particles have a perpendicular pressure. This is modeled as a result of pitch angle scattering of field-aligned inflow particles as they cross the current sheet on hairpin- like reconnected field lines. The new results show that this accounts for a flux-bulge and a TCR which is consistent with observations. The third study presents a numerical particle model which simulates the evolution of a plasmoid, modeled as a single magnetic field loop in the 3 magnetotail. The model magnetotail has a magnetic, density and velocity gradient along the tail axis. The plasma within the plasmoid splits into two groups, the movement of these groups causes the plasmoid size to oscillate. The initial tailward movement of the plasmoid is caused by the magnetic gradient but continues in its absence due to the net momentum of the plasma inside the plasmoid, with the tailward travelling particles travel faster than the Earthward travelling particles. 4 Acknowledgements Firstly I would like to thank my supervisors, Professors Chris Owen and Andrew Fazakerley for their help and guidance over the years. Thank you to my parents for everything before and during the PhD, they went above and beyond their parental duty and I am very grateful of that. Thank you to my sister Melei for all of the help, knowledge and for looking out for me during the early years. Thank you to my brother, Aflay for the times he cooked dinner, for bringing me along to the Jay-Z and Kanye West concert and for being someone to hang out with during the breaks between work. Thank you to my sister Settit for the long talks about music and TV shows and the healthy eating and travelling you do that is inspiring. Thank you to my brother-in-law, Hermon, for helping me perfect the personal statement of my PhD application and for helping me with my car troubles. Thank you to Phillip Hunt for all the help during the undergrad days. Thank you to my office mates, Andrew Walsh, Colin Forsyth and Roger Duthie for answering my many questions. Thank you to all of the people who drove me to and from the lab: Kimberly Steed, Annie Wellbrock, Sheila Kanani, Missagh Medipour, Ehsan Pedram, Awat Rahimi & Paul Prior. Thank you to Dr. Stefan Kiehas, Dr. Elizabeth Lucek, Dr. Iannis Dandouras for helping on the first study and to the teams behind the Cluster Active Archive, the QSAS software and the CIS, PEACE and FGM instruments of Cluster. Finally, I would like to thank the Science and Technology Funding Council (STFC) for funding my PhD. 5 Contents Abstract ......................................................................................................... 3 Acknowledgements ....................................................................................... 5 Contents ......................................................................................................... 6 List of Figures ............................................................................................... 9 List of Tables ............................................................................................... 11 List of Acronyms ......................................................................................... 11 1 Introduction ........................................................................................... 12 1.1 Plasma Physics ............................................................................... 13 1.1.1 Plasma ...................................................................................... 13 1.1.2 Single particle motion .............................................................. 15 1.1.3 Kinetic Theory ......................................................................... 22 1.1.4 MagnetoHydroDynamics (MHD) ............................................ 23 1.2 Magnetospheric Physics ................................................................. 30 1.2.1 Coordinate systems .................................................................. 30 1.2.2 Solar Wind................................................................................ 31 1.2.3 Magnetosphere ......................................................................... 32 1.2.4 Dungey Cycle ........................................................................... 42 1.2.5 NENL model of Substorms ...................................................... 45 1.2.6 Travelling Compression Regions ............................................. 47 1.3 Modes of Reconnection .................................................................. 50 1.3.1 Multiple X-line Reconnection (MXR) ..................................... 50 1.3.2 MHD Model of Time Dependent Reconnection ...................... 54 1.3.3 Cold Particle Model of Time Dependent Reconnection .......... 60 2 Cluster Observations of a Transient Signature in the Magnetotail: Implications for the Mode of Reconnection ............................................... 62 2.1 Introduction .................................................................................... 62 2.2 Comparison of the Reconnection Products .................................... 64 6 2.3 Instrumentation ............................................................................... 65 2.3.1 FGM ......................................................................................... 66 2.3.2 PEACE ..................................................................................... 67 2.3.3 CIS ............................................................................................ 71 2.3.4 Cluster location and separation ................................................ 73 2.4 Observations ................................................................................... 74 2.5 Analysis .......................................................................................... 89 2.5.1 Orientation of Magnetic Structure ........................................... 89 2.5.2 Velocity Calculation ................................................................. 90 2.5.3 Configuration in MVA derived co-ordinate system ................ 93 2.5.4 Observations in MVA derived co-ordinate system .................. 95 2.6 Discussion ....................................................................................... 99 2.6.1 Interpretation of observations .................................................. 99 2.6.2 Multiple-X-line Reconnection Interpretation ........................ 104 2.6.3 Time Dependent Reconnection Interpretation ....................... 105 2.7 Conclusions .................................................................................. 106 Chapter 3 ................................................................................................... 108 3 Modelling the Effects of Time-Varying Reconnection Leading to the Formation of Travelling Compression Regions in the Magnetotail ......... 108 3.1 Introduction .................................................................................. 108 3.1.1 Comparison of the two existing models ................................. 109 3.2 Cold Particle Model of Time-Dependent Reconnection .............. 110 3.2.1 Marginal Firehose Stability Equation .................................... 110 3.2.2 Frames of Reference .............................................................. 113 3.2.3 Separatrix Height ................................................................... 116 3.2.4 Height of PO boundary .......................................................... 120 3.3 A New Hot Particle Model of Time-Dependent Reconnection ... 124 3.3.1 Horizontal Stress balance ....................................................... 124 3.3.2
Recommended publications
  • Lecture 4: Magnetohydrodynamics (MHD), MHD Equilibrium, MHD Waves
    HSE | Valery Nakariakov | Solar Physics 1 Lecture 4: Magnetohydrodynamics (MHD), MHD Equilibrium, MHD Waves MHD describes large scale, slow dynamics of plasmas. More specifically, we can apply MHD when 1. Characteristic time ion gyroperiod and mean free path time, 2. Characteristic scale ion gyroradius and mean free path length, 3. Plasma velocities are not relativistic. In MHD, the plasma is considered as an electrically conducting fluid. Gov- erning equations are equations of fluid dynamics and Maxwell's equations. A self-consistent set of MHD equations connects the plasma mass density ρ, the plasma velocity V, the thermodynamic (also called gas or kinetic) pressure P and the magnetic field B. In strict derivation of MHD, one should neglect the motion of electrons and consider only heavy ions. The 1-st equation is mass continuity @ρ + r(ρV) = 0; (1) @t and it states that matter is neither created or destroyed. The 2-nd is the equation of motion of an element of the fluid, "@V # ρ + (Vr)V = −∇P + j × B; (2) @t also called the Euler equation. The vector j is the electric current density which can be expressed through the magnetic field B. Mind that on the lefthand side it is the total derivative, d=dt. The 3-rd equation is the energy equation, which in the simplest adiabatic case has the form d P ! = 0; (3) dt ργ where γ is the ratio of specific heats Cp=CV , and is normally taken as 5/3. The temperature T of the plasma can be determined from the density ρ and the thermodynamic pressure P , using the state equation (e.g.
    [Show full text]
  • Astrophysical Fluid Dynamics: II. Magnetohydrodynamics
    Winter School on Computational Astrophysics, Shanghai, 2018/01/30 Astrophysical Fluid Dynamics: II. Magnetohydrodynamics Xuening Bai (白雪宁) Institute for Advanced Study (IASTU) & Tsinghua Center for Astrophysics (THCA) source: J. Stone Outline n Astrophysical fluids as plasmas n The MHD formulation n Conservation laws and physical interpretation n Generalized Ohm’s law, and limitations of MHD n MHD waves n MHD shocks and discontinuities n MHD instabilities (examples) 2 Outline n Astrophysical fluids as plasmas n The MHD formulation n Conservation laws and physical interpretation n Generalized Ohm’s law, and limitations of MHD n MHD waves n MHD shocks and discontinuities n MHD instabilities (examples) 3 What is a plasma? Plasma is a state of matter comprising of fully/partially ionized gas. Lightening The restless Sun Crab nebula A plasma is generally quasi-neutral and exhibits collective behavior. Net charge density averages particles interact with each other to zero on relevant scales at long-range through electro- (i.e., Debye length). magnetic fields (plasma waves). 4 Why plasma astrophysics? n More than 99.9% of observable matter in the universe is plasma. n Magnetic fields play vital roles in many astrophysical processes. n Plasma astrophysics allows the study of plasma phenomena at extreme regions of parameter space that are in general inaccessible in the laboratory. 5 Heliophysics and space weather l Solar physics (including flares, coronal mass ejection) l Interaction between the solar wind and Earth’s magnetosphere l Heliospheric
    [Show full text]
  • Experimental Investigation of Plasma Dynamics in Jets and Bubbles
    University of New Mexico UNM Digital Repository Electrical and Computer Engineering ETDs Engineering ETDs Fall 11-14-2016 Experimental Investigation of Plasma Dynamics in Jets and Bubbles Using a Compact Coaxial Plasma Gun in a Background Magnetized Plasma Yue Zhang University of New Mexico Follow this and additional works at: https://digitalrepository.unm.edu/ece_etds Part of the Electrical and Computer Engineering Commons, and the Plasma and Beam Physics Commons Recommended Citation Zhang, Yue. "Experimental Investigation of Plasma Dynamics in Jets and Bubbles Using a Compact Coaxial Plasma Gun in a Background Magnetized Plasma." (2016). https://digitalrepository.unm.edu/ece_etds/309 This Dissertation is brought to you for free and open access by the Engineering ETDs at UNM Digital Repository. It has been accepted for inclusion in Electrical and Computer Engineering ETDs by an authorized administrator of UNM Digital Repository. For more information, please contact [email protected]. Yue Zhang Candidate Electrical and Computer Engineering Department This dissertation is approved, and it is acceptable in quality and form for publication: Approved by the Dissertation Committee: Mark Gilmore, Chairperson Edl Schamilogu Scott Hsu Ylva M Pihlstrom EXPERIMENTAL INVESTIGATION OF PLASMA DYNAMICS IN JETS AND BUBBLES USING A COMPACT COAXIAL PLASMA GUN IN A BACKGROUND MAGNETIZED PLASMA By YUE ZHANG B.S., Electrical Engineering, Xi'an Jiaotong University, 2003 M.S., Electrical Engineering, Xi'an Jiaotong University, 2006 DISSERTATION Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy Engineering The University of New Mexico Albuquerque, New Mexico December, 2016 Dedication To my parents Zhiping Zhang and Fenghong Ji iii Acknowledgements I would like to my dissertation committee, Dr.
    [Show full text]
  • Magnetohydrodynamics (MHD) Philippa Browning Jodrell Bank Centre for Astrophysics University of Manchester
    Magnetohydrodynamics (MHD) Philippa Browning Jodrell Bank Centre for Astrophysics University of Manchester STFC Summer School – Magnetohydrodynamics MagnetoHydroDynamics (MHD) 1. The MHD equations 2. Magnetic Reynolds number and ideal MHD 3. Some conservation laws 4. Static plasmas - magnetostatic equilibria and force-free fields 5. Flowing plasmas – the solar wind STFC Summer School – Magnetohydrodynamics The solar corona Druckmuller 2011 • The corona is the hot (T ≈ 106 - 107 K) tenuous outer atmosphere of the Sun Solar Dynamic Observatory (SDO) •Highly dynamic and structured •Streaming into space as the solar wind Magnetic fields in the solar corona All structure and activity in solar atmosphere is controlled by magnetic field STFC Summer School – Magnetohydrodynamics Solar wind interaction with Earth Not to scale! STFC Summer School – Magnetohydrodynamics The bigger picture – the Heliosphere 1. The magnetohydrodynamic (MHD) equations STFC Summer School - Magnetohydrodynamics The MHD model and its applicability • One approach to modelling plasmas is kinetic theory – this models the distribution functions fs(r,v,t) for each species (s = “ions” or “electrons”) See Tsiklauri lecture • From kinetic theory we may take moments (integrate over velocity space) and derive multi-fluid models (each species treated as a separate fluid) or single fluid models • MagnetoHydroDynamics (MHD) treats the plasma as single electrically-conducting fluid which interacts with magnetic fields • Does not consider separate behaviour of ions/electrons STFC Summer
    [Show full text]
  • Solar MHD Theory MT4510
    1 (Revision 2) Solar MHD Theory MT4510 Prof Alan Hood Dr Clare Parnell 2 Contents 0 Review of Vector Calculus. 5 0.1 OperatorsinVariousCoordinateSystems. ........ 6 0.2 Flux........................................ 8 0.3 VectorIdentities................................ .. 8 0.4 IntegralTheorems................................ 9 1 Maxwell’s Equations and Magnetic Fields 11 1.1 Maxwell’sEquations .............................. 11 1.2 ElectromagneticWavesinaVacuum . .... 12 1.3 MagneticFieldLines .............................. 13 2 MHD Equations 17 2.1 ElectromagneticEquations . .... 17 2.1.1 Maxwell’sEquations . .. .. .. .. .. .. .. 17 2.1.2 Ohm’sLaw................................ 18 2.2 FluidEquations .................................. 18 2.2.1 ContinuityEquation ........................... 19 2.2.2 TheEquationofMotion . .. .. .. .. .. .. 19 2.2.3 TheEnergyEquation........................... 20 2.2.4 Summary of the MHD Equations: Important to know these . ...... 20 2.2.5 GeneralRemarks ............................. 21 3 Magnetic Induction and Magnetic Energy 23 3.1 TheInductionEquation. .. 23 3.2 InductionEquation-TheDiffusionLimit . ....... 25 3.2.1 Diffusioninacurrentsheet. .. 25 3.3 InductionEquation-Frozen-in-FluxTheorem . ......... 28 3.3.1 Frozen-in-Flux Theorem (Alfv´en’s Theorem) . ....... 28 3.4 SteadyState.................................... 33 3.5 MagneticEnergy ................................. 34 4 Magnetic Forces 37 4.1 TheLorentzForce................................. 37 4.1.1 MagneticTensionForce . 38 4.1.2 MagneticPressureForce
    [Show full text]
  • Effect of a Fossil Magnetic Field on the Structure of a Young
    Mon. Not. R. Astron. Soc. 000, 000{000 (0000) Printed 9 August 2021 (MN LATEX style file v2.2) Effect of a fossil magnetic field on the structure of a young Sun V. Duez?, S. Mathisy, S. Turck-Chi`ezez DSM/IRFU/SAp, CEA Saclay, 91191 Gif-sur-Yvette Cedex, France; AIM, UMR 7158, CEA - CNRS - Universit´eParis 7, France 9 August 2021 ABSTRACT We study the impact of a fossil magnetic field on the physical quantities which describe the structure of a young Sun of 500 Myr. We consider for the first time a non force-free field composed of a mixture of poloidal and toroidal magnetic fields and we propose a specific configuration to illustrate our purpose. In the present paper, we estimate the relative role of the different terms which appear in the modified stellar structure equations. We note that the Lorentz tension plays a non negligible role in addition to the magnetic pressure. This is interesting because most of the previous stellar evolution codes ignored that term and the geometry of the field. The solar structure perturbations are, as already known, small and consequently we have been able to estimate each term semi-analytically. We develop a general treatment to calculate the global modification of the structure and of the energetic balance. We estimate also the gravitational multipolar moments associated with the presence of a fossil large-scale magnetic field in radiative zone. The values given for the young Sun help the future implementation in stellar evolution codes. This work can be repeated for any other field configuration and prepares the achievement of a solar MHD model where we will follow the transport of such field on secular timescales and the associated transport of momentum and chemicals.
    [Show full text]
  • 15. Solar MHD II
    15. Solar MHD II. Solar MHD • Particle Motion in Electric Field • Magnetic Effects • Ohm’s Law • MHD Equations • Magnetic Field Diffusion • Frozen Magnetic Flux Approximation • Magnetic Forces • MHD Waves • Magnetohydrodynamics movie: https://www.youtube.com/watch?v=QArcTylNooQ MHD Equations Consider plasma in an electro-magnetic field. The Maxwell equations are (CGS units): MHD approximation 41 E Bj neglect displacement current because MHD cct processes are slow compared to the speed of light B 0 1 B E ct neglect separation of electric charges of E 4e electrons and ions – plasma quasi-neutrality 1 j ()EvB - Ohm’s law in a non-magnetized plasma c (1)L moving with velocity v; recall the electric field transformation in a moving 1 coordinate system: E EBv c Equations of conservation of mass, momentum and energy Then, we combine the Maxwell equations with the equations of conservation of mass, momentum and energy: ()0v t dvv 1 ()vv P j B dt t c dS TQL dt where ρ is the mass density, P is the gas pressure, v is the velocity, ScV log() P is the specific entropy, Q is an energy input, L is the energy loss rate (radiative losses). Magnetic Field Diffusion 11 Applying curl to the Ohm’s equation: E j ()vB c 11 EjvB () c 4 and using the Maxwell equations: Bj c 1 B E ct we get an equation for magnetic field strength B : B 11 cc E jvB (), or tc B c2 1 ()vB B t 4 This is “the induction equation” - a central equation for solar MHD theories.
    [Show full text]
  • Magnetohydrodynamics (MHD) Philippa Browning Jodrell Bank Centre for Astrophysics University of Manchester
    Magnetohydrodynamics (MHD) Philippa Browning Jodrell Bank Centre for Astrophysics University of Manchester STFC Summer School – Magnetohydrodynamics MagnetoHydroDynamics (MHD) 1. The MHD equations 2. Magnetic Reynolds number and ideal MHD 3. Some conservation laws 4. Static plasmas - magnetostatic equilibria and force-free fields 5. Flowing plasmas – the solar wind STFC Summer School – Magnetohydrodynamics The solar corona Druckmuller 2011 • The corona is the hot (T ≈ 106 - 107 K) tenuous outer atmosphere of the Sun Solar Dynamic Observatory (SDO) •Highly dynamic and structured •Streaming into space as the solar wind Magnetic fields in the solar corona All structure and activity in solar atmosphere is controlled by magnetic field STFC Summer School – Magnetohydrodynamics Solar wind interaction with Earth Not to scale! STFC Summer School – Magnetohydrodynamics The bigger picture – the Heliosphere Plasma in the universe • Plasma - a quasi- neutral gas of charged particles exhibiting collective behaviour • > 99% of baryonic matter in universe is in plasma state • Plasmas create magnetic fields and interact with magnetic fields STFC Summer School – Magnetohydrodynamics 1. The magnetohydrodynamic (MHD) equations STFC Summer School - Magnetohydrodynamics The MHD model and its applicability • One approach to modelling plasmas is kinetic theory – this models the distribution functions fs(r,v,t) for each species (s = “ions” or “electrons”) See Tsiklauri lecture • From kinetic theory we may take moments (integrate over velocity space) and derive
    [Show full text]
  • Plasma Physics
    Plasma Physics TU Dresden Lecturer: Dr. Katerina Falk Lecture 5: Magneto-hydrodynamics Plasma Physics: lecture 5 § Principles of MHD macroscopic models for plasma § Continuity, momentum and energy equations § Moments of the distribution functions § Ohm’s law and the induction equation § Magnetic flux freezing § Magnetic pressure § Plasma ! parameter Magneto-hydrodynamics § For a large number of particles it is difficult to solve individual equations of motion. § The primary weakness of kinetic models is that the modification of E and B fields by particle motion is neglected. § The fluid model overcomes these issues. § MHD solves the motion of fluid elements instead of tracing the individual particles. § Two fluid model: electrons and ions two separate fluids that penetrate each other. § NB: in fluid dynamics particles strongly coupled, not the case in ideal plasmas! MHD basic assumptions # § Quasi-neutrality assumed → cannot model ! < $% and & < '()*+) → macroscopic model of plasma § Pressure scalar § Velocity much smaller than speed of light § Typical length scales much larger than kinetic length scales, e.g. gyro radii, skin depth, etc. § Typical time scales much slower than kinetic time scales, e.g. gyro frequencies MHD basic assumptions § Does not track individual particles § Only valid if particles localized by: • Collisions: !"#$ ≪ & • Magnetic field: '()*"+* ≪ & → MHD cannot be used without B-fields! § Momentum exchange by collisions between species or by heavier ions dragging electrons along due to charge imbalance (if collisionless). § MHD is a theory describes large-scale and slow phenomena compared to kinetic theory. Components of MHD § Mass density – ! (kg/m3) § Fluid velocity – " (m/s) § Internal energy – # (J/m3) § Pressure – $ (Pa) § Magnetic field – % (Tesla) § Current density – & (A/m2) Maxwell’s equations .
    [Show full text]