Reviewing the Summer School Solar Labs Nicholas Gross.

Slides:



Advertisements
Similar presentations
Global Properties of Heliospheric Disturbances Observed by Interplanetary Scintillation M. Tokumaru, M. Kojima, K. Fujiki, and M. Yamashita (Solar-Terrestrial.
Advertisements

Chapter 8 The Sun – Our Star.
Interaction of coronal mass ejections with large-scale structures N. Gopalswamy, S. Yashiro, H. Xie, S. Akiyama, and P. Mäkelä IHY – ISWI Regional meeting.
The Solar Wind and Heliosphere Bob Forsyth - 15 th October 2007 TOPICS The Sun – interior and atmosphere Origin of the solar wind Formation of the heliosphere.
General Properties Absolute visual magnitude M V = 4.83 Central temperature = 15 million 0 K X = 0.73, Y = 0.25, Z = 0.02 Initial abundances: Age: ~ 4.52.
1 Diagnostics of Solar Wind Processes Using the Total Perpendicular Pressure Lan Jian, C. T. Russell, and J. T. Gosling How does the magnetic structure.
Comparing the Large-Scale Magnetic Field During the Last Three Solar Cycles Todd Hoeksema.
Evolution of the Large-Scale Magnetic Field Over Three Solar Cycles Todd Hoeksema.
A General Cone Model Approach to Heliospheric CMEs and SEP Modeling Magnetogram-based quiet corona and solar wind model The SEPs are modeled as a passive.
1 WSA Model and Forecasts Nick Arge Space Vehicles Directorate Air Force Research Laboratory.
Identifying Interplanetary Shock Parameters in Heliospheric MHD Simulation Results S. A. Ledvina 1, D. Odstrcil 2 and J. G. Luhmann 1 1.Space Sciences.
Solar Activity and VLF Prepared by Sheila Bijoor and Naoshin Haque Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global AWESOME.
Center for Space Environment Modeling W. Manchester 1, I. Roussev, I.V. Sokolov 1, 1 University of Michigan AGU Berkeley March.
The “cone model” was originally developed by Zhao et al. ~10 (?) years ago in order to interpret the times of arrival of ICME ejecta following SOHO LASCO.
Predictions of Solar Wind Speed and IMF Polarity Using Near-Real-Time Solar Magnetic Field Updates C. “Nick” Arge University of Colorado/CIRES & NOAA/SEC.
RT Modelling of CMEs Using WSA- ENLIL Cone Model
Thomas Zurbuchen University of Michigan The Structure and Sources of the Solar Wind during the Solar Cycle.
Solar Probe: Mission to the Sun Donald M. Hassler/David J. McComas Southwest Research Institute.
The Asymmetric Polar Field Reversal – Long-Term Observations from WSO J. Todd Hoeksema, Solar Observatories H.E.P.L., Stanford University SH13C-2278.
Fundamental properties of the Sun. Last time Described the Sun’s size (diameter), mass, chemical composition, and temperature Today, additional features.
The Sun and the Heliosphere: some basic concepts…
1 Interpreting SECCHI White Light Images: FOV Sensitivity & Stereo Viewing Paulett Liewer, JPL; Russ Howard & Dennis Socker, NRL SECCHI Consortium Meeting.
Numerical simulations are used to explore the interaction between solar coronal mass ejections (CMEs) and the structured, ambient global solar wind flow.
1 C. “Nick” Arge Space Vehicles Directorate/Air Force Research Laboratory SHINE Workshop Aug. 2, 2007 Comparing the Observed and Modeled Global Heliospheric.
Assessing Predictions of CME Time- of-Arrival and 1 AU Speed to Observations Angelos Vourlidas Vourlidas- SHINE
Solar System Missions Division Solar Orbiter Next major Solar and Heliospheric mission ESA ILWS flagship Now with the Inner Heliospheric Sentinels.
The Sun: Part 3 and Measuring the Stars: Part 1. Net result: 4 protons → 4 He + 2 neutrinos + energy Hydrostatic Equilibrium: pressure from fusion reactions.
Abstract Although Parker was the first to describe the solar wind successfully at the time, his elegant theory still masks a number of fundamental problems.
1 THE RELATION BETWEEN CORONAL EIT WAVE AND MAGNETIC CONFIGURATION Speakers: Xin Chen
Space Weather from Coronal Holes and High Speed Streams M. Leila Mays (NASA/GSFC and CUA) SW REDISW REDI 2014 June 2-13.
Comparison of the 3D MHD Solar Wind Model Results with ACE Data 2007 SHINE Student Day Whistler, B. C., Canada C. O. Lee*, J. G. Luhmann, D. Odstrcil,
SLIDE SHOW 3 B changes due to transport + diffusion III -- * * magnetic Reynold number INDUCTION EQUATION B moves with plasma / diffuses through it.
Charles Hakes Fort Lewis College1. Charles Hakes Fort Lewis College2 Chapter 9 The Sun.
The Solar Wind.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Heliosphere: The Solar Wind March 01, 2012.
CDS meeting September 2005 Solar Physics at UCLan Dr Barbara Bromage Centre for Astrophysics University of Central Lancashire.
Faraday Rotation: Unique Measurements of Magnetic Fields in the Outer Corona Justin C. Kasper (UM), Ofer Cohen (SAO), Steven Spangler (Iowa), Gaetan Le.
Conclusions Using the Diffusive Equilibrium Mapping Technique we have connected a starting point of a field line on the photosphere with its final location.
Advanced Solar Theory (MT5810) OUTLINE 1.Observational properties of the Sun 2.MHD equations (revision) 3.Induction equation - solutions when R m >1 4.Magnetic.
Solar System Physics Group IPS Using EISCAT and MERLIN: Extremely-Long Baseline Observations at Multiple Frequencies R.A.Fallows, A.R.Breen, M.M.Bisi,
The Sun The Sun imaged in white light by the SOHO spacecraft.
Interplanetary Shocks in the Inner Solar System: Observations with STEREO and MESSENGER During the Deep Solar Minimum of 2008 H.R. Lai, C.T. Russell, L.K.
ORIGIN OF THE SLOW SOLAR WIND K. Fujiki , T. Ohmi, M. Kojima, M. Tokumaru Solar-Terrestrial Environment Laboratory, Nagoya University and K. Hakamada Department.
Modeling 3-D Solar Wind Structure Lecture 13. Why is a Heliospheric Model Needed? Space weather forecasts require us to know the solar wind that is interacting.
A105 Stars and Galaxies  Homework 6 due today  Next Week: Rooftop Session on Oct. 11 at 9 PM  Reading: 54.4, 55, 56.1, 57.3, 58, 59 Today’s APODAPOD.
8:30-9:10 AM: Philip Scherrer, What Can We Hope to Learn from SDO Overview of SDO HMI Investigation HMI Instrument.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Fall, 2009 Copyright © The Heliosphere: Solar Wind Oct. 08, 2009.
Solar Wind Helium Abundance and the Minimum Speed of the Solar Wind
State of NOAA-SEC/CIRES STEREO Heliospheric Models STEREO SWG Meeting, NOAA/SEC, Boulder, CO, March 22, 2004 Dusan Odstrcil University of Colorado/CIRES.
1 Pruning of Ensemble CME modeling using Interplanetary Scintillation and Heliospheric Imager Observations A. Taktakishvili, M. L. Mays, L. Rastaetter,
Detecting, forecasting and modeling of the 2002/04/17 halo CME Heliophysics Summer School 1.
An Introduction to Observing Coronal Mass Ejections
On the three-dimensional configuration of coronal mass ejections
Sun: General Properties
Xuepu Zhao Oct. 19, 2011 The Base of the Heliosphere: The Outer (Inner) Boundary Conditions of Coronal (Heliospheric) models.
Review Question Why does the Sun shine?.
Introduction to Space Weather Interplanetary Transients
SLIDE SHOW 6. SOLAR WIND (Mariner 2, 1962)
D. Odstrcil1,2, V.J. Pizzo2, C.N. Arge3, B.V.Jackson4, P.P. Hick4
Solar Wind Transients and SEPs
Exploring Large-scale Coronal Magnetic Field Over Extended Longitudes With EUVI EUVI B EIT EUVI A 23-Mar UT Nariaki Nitta, Marc DeRosa, Jean-Pierre.
The Sun: close-up of a spectral class G main sequence star
Forecasting the arrival time of the CME’s shock at the Earth
How does the solar atmosphere connect to the inner heliosphere?
Lecture 5 The Formation and Evolution of CIRS
Section 2: Solar Activity
Modeling Coronal Mass Ejections with EUHFORIA
Introduction to Space Weather
Physics 320: Interplanetary Space and the Heliosphere (Lecture 24)
WHAT DO YOU THINK? How does the mass of the Sun compare with that of the rest of the Solar System? Are there stars nearer the Earth than the Sun is? What.
Presentation transcript:

Reviewing the Summer School Solar Labs Nicholas Gross

Background Target Audience is 1 st year graduate students Excellent set of activities using research quality materials Developed independently with little coordination Sequencing sometimes rough Developed on multiple platforms

Minor Renovation Separate goals so labs build on one another Group related activities Use uniform platform (CISMDX) where appropriate Introduce guided inquiry questions Continue to include most resent research findings and professional tools

Today’s Mission Identify fundamental concepts that students should have after attending the summer school Continue to evolve the summer school material to reflect the latest research findings and tools.

Solar Labs –Lab 2: Structure of the near Solar Magnetic Field –Lab 3: Sources of the Solar Wind –Lab 4: Heliospheric Structure –Lab 5: Evolution of Coronal Mass Ejections Holistic Goal –Study the structure and evolution of the solar corona and solar wind and their role as drivers of geospace processes.

Lab 2: Structure of Near Solar Magnetic Field Overall Goal: Holistic understanding of solar magnetic field at various phases in the solar cycle Activity 1: Use synoptic maps to study the structure of active regions at various phases in the solar cycle. Activity 2: Use MAS results to visualize the magnetic field structure at various phases in the solar cycle.

Lab 2: Structure of Near Solar Magnetic Field Goal 1: Structure and Evolution of Active Regions –White light vs. magnetogram –Magnetograms from rotation to rotation –Magnetograms over the solar cycle –Magnetograms from one cycle to the next

Lab 2: Structure of Near Solar Magnetic Field Goal 2:Structure of solar magnetic field during solar minimum –B r = 0 contour is simple –Closed field lines connect across these contours –Closed lines confined to lower latitudes near the sun –Open field lines originate near poles –Open field lines separated by a current sheet

Goal 3: Compare the structure of the solar magnetic field at solar minimum and solar maximum. –B r =0 contour more complicated for solar maximum –closed and open field lines can originate from almost anywhere –Close field lines still do not extend far from the sun –Open field lines still separated by a current sheet –Solar Max Current sheet is far more complicated Lab 2: Structure of Near Solar Magnetic Field

Lab 3: Sources of the Solar Wind Overall Goals –Students will be able to identify the likely sources of fast solar wind. –Interpret the coronal hole maps generated by WSA run at SEC.

Lab 3: Sources of the Solar Wind Goal 1:Relationship between photospheric magnetic field and coronal hole structure –compare synoptic magneto-grams and EIT images –observe that coronal holes with areas away from active regions –differences between the coronal hole structures at solar minimum and solar maximum –polar coronal holes common during solar minimum – coronal holes at lower latitudes likely at solar maximum –open field line foot points occur at coronal holes

Lab 3: Sources of the Solar Wind Goal 2: Relationship between coronal hole structure, open field lines, and solar wind speed –Slow solar wind is observed near the current sheet while fast solar wind is observed away from the current sheet. –Parcels of solar wind at 5 solar radii can be traced back to a particular coronal hole on the sun. –Solar wind near the current sheet originates nearer the edges of coronal holes. –Solar wind away from the current sheet originates nearer the middle of the coronal holes.

Lab 3: Sources of the Solar Wind

Lab 4: Heliospheric Structure Overall Goal: Students will explore structures in the solar wind including changes with distance, variation in the azimuthal direction, and properties of co-rotating interaction regions. –Activity 1: Use visualization and line plots to explore the variations with distance and latitude. –Activity 2: Use visualizations and line plots to explore variations across CIR boundaries.

Lab 4: Heliospheric Structure Goal 1: Radial flow with parameters that vary with distance from the sun. –density and magnetic field strength decrease as roughly 1/r 2 –Velocity is radial and roughly constant with distance from the sun out to 1 AU. –relate the last two observations to the continuity equation and frozen in flux –explore the temperature profile and relate it to the equation of state

Lab 4: Heliospheric Structure Goal 2: Solar wind speeds vary with latitude in a way that changes depending on the solar cycle phase. –solar minimum the solar wind is highly structured with fast solar wind at the poles and slow solar wind near the solar equator –solar maximum, the solar wind is less ordered, on average being isotropic

Lab 4: Heliospheric Structure Goal 3: Properties of Magnetic field segment structure and Co-rotating Interaction Regions (CIR’s) –Existence of Magnetic Segments and CIR’s –Relation between magnetic segment boundaries and CIR’s –CIR’s involve interaction of fast and slow solar wind –Evidence for shocks at CIR boundaries Change in velocity Change in density Change in magnetic field

Lab 5: Evolution of Coronal Mass Ejections Predict arrival time of a CME from white light corona images –Activity: Use difference coronagraphs to estimate the velocity of CME and its arrival time Explore structure of CME at solar minimum and solar maximum –Activity: Use simulation results to visualize evolution of CME structure as it travels from the sun

Lab 5: Evolution of Coronal Mass Ejections Goal 1: CME arrival time can be predicted form difference coronagraphs. –A “halo” CME is the result of a CME launched almost directly towards Earth. –The expansion rate can be used to estimate the launch speed of the CME –The speed is filtered by an average acceleration due to the solar wind conditions that the CME evolves in.

Lab 5: Evolution of Coronal Mass Ejections Goal 2: CME evolves differently depending on the phase of the solar cycle –CME flattens as it moves out from the sun –Solar wind structure affects the evolution of the CME –CME launched during solar maximum is isotropic –CME launched during solar minimum has a strongly varying azimuthal structure.

Way Forward Questions and Feedback? Review summer school materials and adjust tools and manuals accordingly Feedback to Volunteers?