11.1 Magnetic Dipole Field. 11.1 Magnetic Dipole Field (2) B 

Slides:



Advertisements
Similar presentations
Quiet-time F2-layer Disturbances: Morphology and some Formation Mechanisms Quiet-time F2-layer Disturbances: Morphology and some Formation Mechanisms Andrei.
Advertisements

Introduction to the Ionosphere
MURI,2008 Electric Field Variability and Impact on the Thermosphere Yue Deng 1,2, Astrid Maute 1, Arthur D. Richmond 1 and Ray G. Roble 1 1.HAO National.
Ionosphere Climate Studied by F3 / COSMIC Constellation C. H. Liu Academia Sinica In Collaboration with Tulasi Ram, C.H. Lin and S.Y. Su.
ASEN 5335 Aerospace Environments -- Geomagnetism 1 Paleomagnetism Natural remnant magnetism (NRM) of some rocks (and archeological samples) is a measure.
DEFINITION, CALCULATION, AND PROPERTIES OF THE Dst INDEX R.L. McPherron Institute of Geophysics and Planetary Physics University of California Los Angeles.
Propagation Index and Short Wave Communications Rodney Wolfe N3XG.
ESS 7 Lecture 14 October 31, 2008 Magnetic Storms
Spatio-temporal structures of equatorial F-region plasma irregularities & Geomagnetic Regular Daily Variations (Sq, Solar quiet) as seen in space and at.
Auroral dynamics EISCAT Svalbard Radar: field-aligned beam  complicated spatial structure (
Ch 6 Solar Wind Interactions. Earth’s Magnetic Field
Ionospheric Electric Field Variations during Geomagnetic Storms Simulated using CMIT W. Wang 1, A. D. Richmond 1, J. Lei 1, A. G. Burns 1, M. Wiltberger.
Reinisch_ Solar Terrestrial Relations (Cravens, Physics of Solar Systems Plasmas, Cambridge U.P.) Lecture 1- Space Environment –Matter in.
SCHOOL OF PHYSICS Space Weather in the Equatorial Ionosphere Robert Stening School of Physics, University of New South Wales Acknowledge help from Dr J.
Solar system science using X-Rays Magnetosheath dynamics Shock – shock interactions Auroral X-ray emissions Solar X-rays Comets Other planets Not discussed.
5. Simplified Transport Equations We want to derive two fundamental transport properties, diffusion and viscosity. Unable to handle the 13-moment system.
補充教材. 2.1 The solar-terrestrial system The Earth’s upper atmosphere is ionized by solar radiations (a) electromagnetic: radio - - X-ray; speed
Magnetometer Tutorial PowerPoint March, 2007 THEMIS: The Science Behind Magnetometer Signatures Laura Peticolas GEONS workshop.
Belle Tamir, Sharet High School Nitzan Atia, Tchernichovsky High School Netanya, Israel.
Julie A. Feldt CEDAR-GEM workshop June 26 th, 2011.
How do gravity waves determine the global distributions of winds, temperature, density and turbulence within a planetary atmosphere? What is the fundamental.
Tuija I. Pulkkinen Finnish Meteorological Institute Helsinki, Finland
Solar wind-magnetosphere- atmosphere coupling: effects of magnetic storms and substorms in atmospheric electric field variations Kleimenova N., Kozyreva.
Antarctic Peninsula is a very suitable area for experimental investigations of troposphere-to-ionosphere energy transfer because this place characterized.
Introduction to Space Weather
How does the Sun drive the dynamics of Earth’s thermosphere and ionosphere Wenbin Wang, Alan Burns, Liying Qian and Stan Solomon High Altitude Observatory.
Computational Astrophysics: Magnetic Fields and Charged Particle Dynamics 11-dec-2008.
University of Colorado 1 ; Delft University of Technology 2 ; University of Alaska 3 ; Centre National d’Etudes Spatiales 4 ; National Center for Atmospheric.
Magnetosphere-Ionosphere coupling processes reflected in
The Relations Between Solar Wind Variations and the North Atlantic Oscillation Rasheed Al-Nuaimi and Kais Al-Jumily Department of Atmospheric Sciences.
How does energy from magnetic storms get transferred from high to low latitudes Anthea Coster, MIT Haystack Observatory How does energy from magnetic storms.
Space Science MO&DA Programs - September Page 1 SS It is known that the aurora is created by intense electron beams which impact the upper atmosphere.
Dynamo Processes in the Sun Earth System Variations of the Earth’s magnetic Field Christine Amory-Mazaudier LPP/CNRS/UMPC, 4 Avenue d Neptune Saint-Maur-des-Fossés.
Radiation belt particle dynamics Prepared by Kevin Graf Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global AWESOME Network.
Ionospheric Current and Aurora CSI 662 / ASTR 769 Lect. 12 Spring 2007 April 24, 2007 References: Prolss: Chap , P (main) Tascione: Chap.
A generic description of planetary aurora J. De Keyser, R. Maggiolo, and L. Maes Belgian Institute for Space Aeronomy, Brussels, Belgium
Scott Thaller Van Allen Probes EFW meeting University of Minnesota June 10-12, 2014.
CEDAR 2008 Workshop Observations at the Plasmaspheric Boundary Layer with the Mid-latitude SuperDARN radars Mike Ruohoniemi, Ray Greenwald, and Jo Baker.
Response of the Earth’s environment to solar radiative forcing
ESS 200C Lecture 13 The Earth’s Ionosphere
New Science Opportunities with a Mid-Latitude SuperDARN Radar Raymond A. Greenwald Johns Hopkins University Applied Physics Laboratory.
What is a geomagnetic storm? A very efficient exchange of energy from the solar wind into the space environment surrounding Earth; These storms result.
MULTI-INSTRUMENT STUDY OF THE ENERGY STEP STRUCTURES OF O + AND H + IONS IN THE CUSP AND POLAR CAP REGIONS Yulia V. Bogdanova, Berndt Klecker and CIS TEAM.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Sun: Magnetic Structure Feb. 16, 2012.
Substorms: Ionospheric Manifestation of Magnetospheric Disturbances P. Song, V. M. Vasyliūnas, and J. Tu University of Massachusetts Lowell Substorms:
Characteristics and source of the electron density irregularities in the Earth’s ionosphere Hyosub Kil Johns Hopkins University / Applied Physics Laboratory.
Energy inputs from Magnetosphere to the Ionosphere/Thermosphere ASP research review Yue Deng April 12 nd, 2007.
Planetary waves in the equatorial mesosphere and ionosphere measurements Lourivaldo Mota Lima (UEPB) Luciana R. Araújo, Maxwelton F. Silva (UEPB) H. Takahashi,
Coupled Thermosphere Ionosphere Plasmasphere Model with self-consistent Electrodynamics (CTIPe) Global thermosphere km, solves momentum, energy,
When Lower Atmosphere Waves Invade the Upper Atmosphere
PART I: Local Ionospheric processes, and terrestrial ionospheres
Chapter 8 Antennas Propagation Dave Piersall, N6ORB.
CEDAR Frontiers: Daytime Optical Aeronomy Duggirala Pallamraju and Supriya Chakrabarti Center for Space Physics, Boston University &
Atmosphere-Ionosphere Wave Coupling as Revealed in Swarm Plasma Densities and Drifts Jeffrey M. Forbes Department of Aerospace Engineering Sciences, University.
Disturbance Dynamo Effects in the Low Latitude Ionosphere
Ionospheric Models Levan Lomidze Center for Atmospheric and Space Sciences Utah State University CEDAR-GEM Student Workshop, June.
Thermosphere-Ionosphere Issues for DASI - I:
The ionosphere is much more structured and variable than ever predicted. Solar Driven Model Since 2000, we have seen more, very clear evidence that the.
Ionosphere, Magnetosphere and Thermosphere Anthea Coster
Astrid Maute, Art Richmond, Ben Foster
Presented by Jim Garver, K7YO for Ken Neubeck, WB2AMU
Earth’s Ionosphere Lecture 13
Energy conversion boundaries
Ionosphere References: Prolss: Chap. 4, P (main)
Using Old Geomagnetic Data to Say Something about the Sun
Alexander S. Medvedev1, Erdal Yiğit2 and Paul Hartogh1
Han-Li Liu, Raymond G. Roble, Arthur D. Richmond, Stanley C
Magnetosphere: Bow Shock Substorm and Storm
The Upper Atmosphere: Problems in Developing Realistic Models
The Ionosphere Equatorial Anomaly.
Presentation transcript:

11.1 Magnetic Dipole Field

11.1 Magnetic Dipole Field (2) B 

11.1 Magnetic Dipole Field (3) B BB BrBr dr rd  r  r

11.2 Geomagnetic Field

11.2 Geomagnetic Field (2)

11.3 Geomagnetic variations

11.3 Geomagnetic variations (1) The geomagnetic field shows significant variability during quiet times and magnetically disturbed periods. Quiet time variability results from tidal waves caused by solar heating and lunar gravitational forces. Tidal motion moves ions across field lines generating dynamo electric fields. –Solar-quiet current system – Sq currents –Lunar current system – L currents

11.3 Geomagnetic variations (2) Disturbance field D=B-B Sq -B L –D=D st -D s D st is the storm-time variation caused by the ring current disturbances D s is the disturbance caused by auroral particle precipitation Kp index –Local K index: 12 stations (in the northern mid-latitudes) measure the average magnetic variation for every 3 hours with log scale –0 0, 0 +, 1 -, 1 0, 1 +, 2 -, … 9 -, 9 0, 9 + –Planetary Kp index: average of the 12 stations

11.4 Ionospheric Layers

11.4 Ionospheric Layers (2)

11.4 Ionospheric Layers (3)

11.4 Ionospheric Layers (4)

11.4 Dominant Processes in the Ionosphere E and F1 region: photochemistry is dominant F2 region: photochemistry and diffusion Topside F2 region: diffusion is dominant Plasma motion along B Ambipolar diffusive forces are vertical: F a ~g, dT/dz, dn/dz F a|| =F a sinI u az =u a|| sinI See Fig.11.7 for effects of neutral wind and E. I FaFa u az F a || B u a|| I

11.4 Ionospheric Layers (5)