Nicholeen Viall NASA/GSFC

Slides:



Advertisements
Similar presentations
Uncovering the Global Slow Solar Wind Liang Zhao and Thomas H. Zurbuchen Department of Atmospheric, Oceanic and Space Sciences, University of Michigan.
Advertisements

Reviewing the Summer School Solar Labs Nicholas Gross.
ESS 7 Lecture 14 October 31, 2008 Magnetic Storms
Global Distribution of Slow Solar Wind N. U. Crooker, S. W. Antiochos, X. Zhao, Yi-M. Wang, and M. Neugebauer.
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.
Five Spacecraft Observations of Oppositely Directed Exhaust Jets from a Magnetic Reconnection X-line Extending > 4.3 x 10 6 km in the Solar Wind Gosling.
STEREO AND SPACE WEATHER Variable conditions in space that can have adverse effects on human life and society Space Weather: Variable conditions in space.
On the Extrapolation of the Sun to the Heliosphere R. A. Howard ACE / SOHO / STEREO / WIND Workshop 8-10 June 2010.
HMI – Synoptic Data Sets HMI Team Meeting Jan. 26, 2005 Stanford, CA.
Synoptic maps and applications Yan Li Space Sciences Laboratory University of California, Berkeley, CA HMI team meeting, Jan 27, 2005, Stanford.
Solar system science using X-Rays Magnetosheath dynamics Shock – shock interactions Auroral X-ray emissions Solar X-rays Comets Other planets Not discussed.
February 26, 2007 KIPAC Workshop on Magnetism Modeling/Inferring Coronal And Heliospheric Field From Photospheric Magnetic Field Yang Liu – Stanford University.
Plasma in the Heliosheath John Richardson M.I.T. Collaborators: J. Belcher, J. Kasper, E. Stone, C. Wang.
1. Background2. Flux variation3. Polarity reversal4. Electron evolution5. Conclusions The role of coronal mass ejections in the solar cycle evolution of.
Thomas Zurbuchen University of Michigan The Structure and Sources of the Solar Wind during the Solar Cycle.
The Sun and the Heliosphere: some basic concepts…
The Sun. Solar Prominence Sun Fact Sheet The Sun is a normal G2 star, one of more than 100 billion stars in our galaxy. Diameter: 1,390,000 km (Earth.
Numerical simulations are used to explore the interaction between solar coronal mass ejections (CMEs) and the structured, ambient global solar wind flow.
Assessing Predictions of CME Time- of-Arrival and 1 AU Speed to Observations Angelos Vourlidas Vourlidas- SHINE
Solar System Physics Group Heliospheric physics with LOFAR Andy Breen, Richard Fallows Solar System Physics Group Aberystwyth University Mario Bisi Center.
195 Å image – behind 195 Å image – Sun- Earth line – SOHO/ EIT image 195 Å image – Sun- Earth line – SOHO/ EIT image 195 Å image – ahead SECCHI Extreme.
A Presentation to the SHINE ’02 Workshop by J.G. Luhmann (August 19, 2002) CME initiation: A zoo not an animal (Images from the on-line CDAW CME catalogue.
The Role of Magnetic Geometry and Reconnection in the Origin of the Solar Wind Basic SW energy balance: Velli Solar wind Radiation Thermal Conduction.
The Solar Wind.
The Solar Orbiter mission Solar Orbiter represents a new approach to solar studies. –A huge increase in discovery space The payload consists of a suite.
Valentina Zharkova 1 and Olga Khabarova Department of Mathematics, University of Bradford, Bradford BD7 1DP, UK ( ) 2.
SOHO-20 “Transient events on the Sun and In the Heliosphere” – August 28, 2008, Ghent SOHO-20 “Transient events on the Sun and In the Heliosphere” – August.
Small-scale transients in the slow solar wind during solar activity minimum K.E.J. Huttunen 1,2, J.G. Luhmann 1, J.T. Gosling 3, Y. Li 1, D. Larson 1,
Energy conversion at Saturn’s magnetosphere: from dayside reconnection to kronian substorms Dr. Caitríona Jackman Uppsala, May 22 nd 2008.
1 Interplanetary Magnetic Flux Enhancements as seen by STEREO C.T. Russell, L.K. Jian and J.G. Luhmann 18 th STEREO Science Working Group April Meudon,
Solar System Physics Group Simultaneous Heliospheric Imager and Interplanetary Scintillation observations of CMEs and CIRs Gareth D. Dorrian
CME Propagation CSI 769 / ASTR 769 Lect. 11, April 10 Spring 2008.
ORIGIN OF THE SLOW SOLAR WIND K. Fujiki , T. Ohmi, M. Kojima, M. Tokumaru Solar-Terrestrial Environment Laboratory, Nagoya University and K. Hakamada Department.
Inherent Length Scales and Apparent Frequencies of Periodic Solar Wind Number Density Structures Nicholeen Viall 1, Larry Kepko 2 and Harlan Spence 1 1.
Variability of the Heliospheric Magnetic Flux: ICME effects S. T. Lepri, T. H. Zurbuchen The University of Michigan Department of Atmospheric, Oceanic,
1 Pruning of Ensemble CME modeling using Interplanetary Scintillation and Heliospheric Imager Observations A. Taktakishvili, M. L. Mays, L. Rastaetter,
Manuela Temmer Institute of Physics, University of Graz, Austria Tutorial: Coronal holes and space weather consequences.
CME rate: 1/3 (4) day -1 at solar min (max) [LASCO CME catalogue. Yahsiro et al., 2005] |B| at 1 AU: 5 (8) nT at solar min (max) [OMNI data] D (fraction.
New tools to relate imagery with in-situ and modeling data and their application to space-weather forecasting Alexis P. Rouillard 1,2 D. Odstrcil 3, B.Lavraud.
Time-Dependence (structuring) of the Alpha-to-Proton Ratio (A He ) in the Solar Wind at 1 AU: Initial results, Implications, and Speculations Harlan E.
Poster X4.137 Solar Wind Trends in the Current Solar Cycle (STEREO Observations) A.B. Galvin* 1, K.D.C. Simunac 2, C. Farrugia 1 1.Space Science Center,
The Sun. Sun Fact Sheet The Sun is a normal G2 star, one of more than 100 billion stars in our galaxy. Diameter: 1,390,000 km (Earth 12,742 km or nearly.
Inferring the Heliospheric Magnetic Field Back to the Maunder Minimum
Evolution of the heliospheric magnetic field
Nanoflare Properties in the Solar Corona
An Introduction to Observing Coronal Mass Ejections
Driving 3D-MHD codes Using the UCSD Tomography
Session: Connecting Slow Wind Theories to Current and Future Observations by Justin Edmondson, Ben Lynch, Aleida Higginson, Xudong Sun and Liang Zhao.
Determination of the North-South Heliospheric Magnetic Field from Inner-Corona Closed-Loop Propagation B.V. Jackson Center for Astrophysics and Space Sciences,
Scientists Propose Mechanism to Describe Solar Eruptions of All Sizes
Olga Khabarova 1, valentina zharkova 2 & vladimir kuznetsov 1
Lecture 12 The Importance of Accurate Solar Wind Measurements
Xuepu Zhao Oct. 19, 2011 The Base of the Heliosphere: The Outer (Inner) Boundary Conditions of Coronal (Heliospheric) models.
ARTEMIS – solar wind/ shocks
Solar Probe Plus – SWG September 2, 2016
The Structure of the HPS
Introduction to Space Weather Interplanetary Transients
Evolution of solar wind structures between Venus and Mars orbits
Solar cycle variation of the heliospheric magnetic field
D. Odstrcil1,2, V.J. Pizzo2, C.N. Arge3, B.V.Jackson4, P.P. Hick4
Nicholeen Viall NASA/GSFC
Solar Wind Transients and SEPs
How does the solar atmosphere connect to the inner heliosphere?
Lecture 5 The Formation and Evolution of CIRS
Introduction to Space Weather
Physics 320: Interplanetary Space and the Heliosphere (Lecture 24)
Reconnection of Loops and Open Field Lines
Slit and Slot Interchange
Richard B. Horne British Antarctic Survey Cambridge UK
A Presentation to the SHINE ’02 Workshop by J.G. Luhmann
Presentation transcript:

Understanding the Origin of the Slow Solar Wind by Linking Remote and In Situ Observations Nicholeen Viall NASA/GSFC In collaboration with : Larry Kepko, Spiro Antiochos, Sue Lepri, Angelos Vourlidas, and Jon Linker

Connecting the Sun to the Heliosphere August 1, 2008 Pseudostreamer and helmet streamer Which solar structures become structures in the Heliosphere? Success with large-scale (e.g. CIRs; CMEs), but not for smaller-scales

Success indirectly linking solar structures to heliosphere (in situ) on smaller scales ~tens of minutes up to a few hours ~100 Mm up to a few thousand Mm radial length scale ‘small’ – compared to current heliospheric imager resolution and in situ composition measurements ‘large’ – compared to turbulence (energy containing scales) and Earth’s magnetosphere/space weather I’m going to talk about some Solar Orbiter will finally give a DIRECT link of these smaller scale sizes

Connecting helmet streamer structures and in situ structures in the Heliospheric Current Sheet In situ at 1 AU Viall & Vourlidas 2015 Kepko, Viall, Antiochos, Lepri, Kasper, Weberg 2016 Left –STEREO images of helmet streamers creating density structures; FFTs show a characteristic ~90 minute timescale Helmet streamers have long been known to be highly dynamic (e.g. 6-12 hours ‘Sheeley blobs’; Rouillard et al; Sanchez-Diaz et al.) Indirect (not even from same time) link of Helmet streamer-> HCS structures

Flying Through a Train of Density Structures Heat flux shows Heliospheric current sheet (HCS) crossing Proton density changes coincide with changes in alphas, C, O, charge state (no V change) – solar origin Specially processed, high time resolution ACE composition; typical resolution averages over these structures, and leads to incorrect interpretation of ‘steady’ slow solar wind We observed perdiocid density structures in situ Note ‘periodic’ = characteristic time scale, these are not waves Kepko, Viall, Antiochos, Lepri, Kasper, Weberg 2016

Flying Through a Train of Density Structures Heat flux (strahl) and B field changes associated with structures (one structure in the train is a flux rope!) this indicates magnetic reconnection (S-web) HCS are well known to contain structures created through magnetic reconnection (Crooker; Suess; Rouillard) We observed perdiocid density structures in situ Note ‘periodic’ = characteristic time scale, these are not waves

Is the HCS/Helmet streamer a special boundary where solar wind transients are injected into an otherwise steady solar wind? S-web says there are other locations Our previous in situ solar wind work says there are other locations [Viall et al. 2008] We set our undergrad summer interns loose to find solar wind structures with composition signatures that were NOT at the HCS We see periodic proton density structures in 70-80% of slow solar wind, suggesting that such structures are a substantial component of the ssw. If this is true, then we should see proton density structures (with compositional changes confirming solar source) not only at the HCS crossing, but other places as well.

PFSS as viewed by STEREO A August 2008 HCS is aimed south of Earth; pseudostreamer is aimed north PFSS as viewed by STEREO A That eclipse image from first slide and spiro

Images and in situ data show pseudostreamer continually releases ‘blobs’, ‘puffs’ and structured solar wind Still circumstantial; indirect

HI1 images show pseudostreamer continually releases ‘blobs’, ‘puffs’ and transient solar wind structures DeForest processed HI1 – on STEREO/SECCHI webpage

250 km/s (Faster ones are 400 km/s) Time-distance plots show continuous release of transient structures from pseudostreamer 250 km/s (Faster ones are 400 km/s) Like Jmaps

250 km/s (Faster ones are 400 km/s) Time-distance plots show continuous release of structures from pseudostreamer 250 km/s (Faster ones are 400 km/s)

In situ, Wind/ACE observe a stream interface, many slow In situ, Wind/ACE observe a stream interface, many slow wind structures, and no HCS Ace C & O Ace C6+/C5+ Charge State 14 days without a HCS Slow wind shows highly structured proton density, alpha, carbon, oxygen, charge state - solar source T sector A sector Two traces are 3DP and SWE

Two-day zoom-in shows series of ~2.5 hour structures Alphas and C and O track one another with similar ~2.5 hr variation: structures are from solar source Typical hour cadence would have lead to false conclusion of steady solar wind Define boundaries based on compositional changes

Magnetic reconnection releases coronal loops with different heating histories Composition boundaries generally correspond to B field tangential discontinuities and rotations, but not in a predictable orientation/way [see also Viall et al. 2009 alpha event] Two heat flux drop outs in the train of periodic density structures are signs of connectivity changes to very long field lines (e.g. through interchange rxn to flux ropes; Chollet et al. Pagel et al) Laming talk

PFSS as viewed by STEREO A Images and PFSS show HCS is depressed and aimed south of Earth; pseudostreamer directed north of Earth PFSS as viewed by STEREO A So what exactly are we mapped to at 1 AU?

In situ Event Maps to Complex S-web Arcs Predictive Science Inc

Conclusions Images show helmet streamer and pseudostreamer are highly dynamic, continuously producing slow wind ‘blobs’, ‘puffs’ and structures In situ observation of highly structured slow solar wind at 1 AU from S-web arc and helmet streamer Structure in proton density, alpha, carbon, oxygen, charge state, and B, but NOT velocity is a test on all models of slow solar wind Solar structures -> in situ structures Magnetic reconnection necessary; something like reconnection at the S-web is needed to explain observations

Prediction for Solar Orbiter: There is no such thing as ‘the steady solar wind’ No such thing as steady solar wind, just like in magnetosphere they learned (with better data) that there is no such thing as steady magnetospheric convection. Magnetic fields always store and then release energy. Solar orbiter will finally be able to make DIRECT link between solar source and heliospheric structures Key is to get high time resolution composition + modeling Crooker et al.