Comparing the Large-Scale Magnetic Field During the Last Three Solar Cycles Todd Hoeksema.

Slides:



Advertisements
Similar presentations
The Solar Polar Field Reversal Observed By SOHO/MDI Yang Liu, J. Todd Hoeksema, X-P Zhao – Stanford University
Advertisements

1 Livingston & Penn Data and Findings so Far (and some random reflections) Leif Svalgaard Stanford, July 2011.
2011/08/ ILWS Science Workshop1 Solar cycle prediction using dynamos and its implication for the solar cycle Jie Jiang National Astronomical Observatories,
An overview of the cycle variations in the solar corona Louise Harra UCL Department of Space and Climate Physics Mullard Space Science.
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.
Study of Galactic Cosmic Rays at high cut- off rigidity during solar cycle 23 Partha Chowdhury 1 and B.N. Dwivedi 2 1 Department of Physics, University.
Reviewing the Summer School Solar Labs Nicholas Gross.
Weaker Solar Wind Over the Protracted Solar Minimum Dave McComas Southwest Research Institute San Antonio, TX With input from and thanks to Heather Elliott,
Planetary tides and solar activity Katya Georgieva
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.
Scientific astrology: planetary effects on solar activity Katya Georgieva Solar-Terrestrial Influences Lab., Bulgarian Academy of Sciences In collaboration.
“Insights” on Coronal Hole Magnetic Fields From a High-Order PFSS Model D.J. Bercik and J.G. Luhmann Space Sciences Lab, UC Berkeley 1 FEW 2011, Aug 24.
Chip Manchester 1, Fang Fang 1, Bart van der Holst 1, Bill Abbett 2 (1)University of Michigan (2)University of California Berkeley Study of Flux Emergence:
Evolution of the Large-Scale Magnetic Field Over Three Solar Cycles Todd Hoeksema.
High-latitude activity and its relationship to the mid-latitude solar activity. Elena E. Benevolenskaya & J. Todd Hoeksema Stanford University Abstract.
Synoptic maps and applications Yan Li Space Sciences Laboratory University of California, Berkeley, CA HMI team meeting, Jan 27, 2005, Stanford.
1 Synoptic Maps of Magnetic Field from MDI Magnetograms: polar field interpolation. Y. Liu, J. T. Hoeksema, X. P. Zhao, R. M. Larson – Stanford University.
On the Cause of Solar Differential Rotation Ling-Hsiao Lyu Institute of Space Science, National Central University 呂凌霄 中央大學太空科學研究所 太陽差動自轉的成因.
Relationship between the High and mid latitude Solar Magnetic Field Elena E. Benevolenskaya J. Todd Hoeksema Stanford University.
1 July 31, 2007 SHINE 2007 – Heliospheric Plasma Sheet The Unusual Heliospheric Current Sheet at the End of Cycle 23 A Comparison of Cycles 21,22,& 23.
Helicity as a Component of Filament Formation D.H. Mackay University of St. Andrews Solar Theory Group.
Absence of a Long Lasting Southward Displacement of the HCS Near the Minimum Preceding Solar Cycle 24 X. P. Zhao, J. T. Hoeksema and P. H. Scherrer Stanford.
Session 6 Key Questions for Understanding This Unusual Solar Minimum Alan Gabriel Todd Hoeksema Janet Luhmann Bill Matthaeus Neil Sheeley.
Thomas Zurbuchen University of Michigan The Structure and Sources of the Solar Wind during the Solar Cycle.
A topological view of 3D global magnetic field reversal in the solar corona Rhona Maclean Armagh Observatory 5 th December 2006.
The Asymmetric Polar Field Reversal – Long-Term Observations from WSO J. Todd Hoeksema, Solar Observatories H.E.P.L., Stanford University SH13C-2278.
1 Long-term Solar Synoptic Measurements with Implications for the Solar Cycle Leif Svalgaard Stanford University 23 April 2013.
Solar Rotation Lab 3. Differential Rotation The sun lacks a fixed rotation rate Since it is composed of a gaseous plasma, the rate of rotation is fastest.
1 C. “Nick” Arge Space Vehicles Directorate/Air Force Research Laboratory SHINE Workshop Aug. 2, 2007 Comparing the Observed and Modeled Global Heliospheric.
Proxies of the Entire Surface Distribution of the Photospheric Magnetic Field Xuepu Zhao NAOC, Oct. 18, 2011.
Magnetic mapping of solar-type stars Pascal Petit figure: © M. Jardine.
Effects of the Observed Meridional Flow Variations since 1996 on the Sun’s Polar Fields David H. Hathaway 1 and Lisa Upton 2,3 1 NASA/Marshall Space Flight.
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.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Heliosphere: The Solar Wind March 01, 2012.
Diagnostics of solar wind streams N.A.Lotova, K.V.Vladimirsky, and V.N.Obridko IZMIRAN.
The Polar Fields Seen in 17 GHz Microwave Flux and with Magnetographs Leif Svalgaard Stanford University 6 January, 2012.
Recent ‘Unprecedented’ Weak Solar Wind: A solar glitch or a harbinger for the next Maunder minimum? Conveners: Joan Feynman* and Janet Luhmann When: Wednesday.
Fifty Years Of Solar Events NOAO 50 th Anniversary Symposium.
The Rise of Solar Cycle 24: Magnetic Fields from the Dynamo through the Photosphere and Corona and Connecting to the Heliosphere Part 1: Interior and Photosphere.
The Rise of Solar Cycle 24: Magnetic Fields from the Dynamo through the Photosphere and Corona and Connecting to the Heliosphere Part 2: Corona & Heliophere.
1 Abramenko V.I., 1 Yurchyshyn, V., 2 Linker, J., 2 Mikic, Z. 1 - Big Bear Solar Observatory of NJIT; 2 – Predictive Science Inc., San Diego Anomalous.
1 The Mean Field of the Sun Leif Svalgaard Stanford University Sept. 2, 2011.
Andrés Muñoz-Jaramillo Harvard-Smithsonian Center for Astrophysics
Polar Magnetic Field Elena E. Benevolenskaya Stanford University SDO Team Meeting 2009.
Solar Magnetic Field Reversal V J Pizzo SHINE Workshop August 18, 2002.
WSM Whole Sun Month Sarah Gibson If the Sun is so quiet, why is the Earth still ringing?
Sunspot activity and reversal of polar fields in the current cycle 24 A.V. Mordvinov 1, A.A. Pevtsov 2 1 Institute of Solar-Terrestrial Physics of SB RAS,
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Fall, 2009 Copyright © The Heliosphere: Solar Wind Oct. 08, 2009.
What the Long-Term Sunspot Record Tells Us About Space Climate David H. Hathaway NASA/MSFC National Space Science and Technology Center Huntsville, AL,
Solar Magnetism: Solar Cycle Solar Dynamo Coronal Magnetic Field CSI 662 / ASTR 769 Lect. 03, February 6 Spring 2007 References: NASA/MSFC Solar Physics.
Diary of a Wimpy Cycle David H. Hathaway 1 and Lisa Upton 2,3 1 NASA/Marshall Space Flight Center/Science Research Office 2 Vanderbilt University 3 University.
CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 20, 2005 Surface Magnetic Field Aschwanden, “Physics of the Solar Corona” Chap. 5, P.
The heliospheric magnetic flux density through several solar cycles Géza Erdős (1) and André Balogh (2) (1) MTA Wigner FK RMI, Budapest, Hungary (2) Imperial.
Long-term measurements of the Sun’s poles show that reversal of the dominant magnetic polarity generally occurs within a year of solar maximum. Current.
Sun: General Properties
HMI-WSO Solar Polar Fields and Nobeyama 17 GHz Emission
Predictions for solar cycle 25
SLIDE SHOW 6. SOLAR WIND (Mariner 2, 1962)
Solar cycle variation of the heliospheric magnetic field
Large-Scale Solar Magnetic Fields – How is Solar Cycle 24 Different?
Current HMI Polar Fields
Introduction to Space Weather
The Sun: close-up of a spectral class G main sequence star
Lecture 5 The Formation and Evolution of CIRS
MDI Global Field & Solar Wind
The Sun as We See It Lecture 9
Solar and Heliospheric Physics
Observations of emerging and submerging regions with ASP and Solar-B
Closing the Books on Cycle 24 J
Presentation transcript:

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 Global Properties Corona & Heliosphere Zonal Magnetic Field Toroidal Magnetic Field

Daily Solar Mean Magnetic Field – Sun as a Star 3 Cycles – WSO Sensitivity Issues in ~2001 Rotation Modulation Observed At < 10 uT

4 Solar Minima, 3 Polar Reversals WSO Large-scale Polar Aperture 55 to Pole Surge Arrival South stronger In Cycles

MDI Measured Polar Field during Cycle Movie shows observed and Interpolated polar field above 62 Smaller 75+ Polar Field Is More Symmetric & Reverses Later Difference in Strength is Significant, but Smaller

MDI Measured Polar Field during Cycle Movie shows observed and Interpolated polar field above 62 Smaller 75+ Polar Field Is More Symmetric & Reverses Later Difference in Strength is Significant, but Smaller

Axial, Equatorial, and Total Solar Dipole – 3 Cycles Total Axial Equatorial

Total Solar Dipole, Quadrupole, Octupole – 3 Cycles Dipole Quadrupole l = 3 2.5Rs

Computed Source Surface Magnetic Field

The Computed Coronal Field & HCS During Cycle Every 10 th Rotation Each panel 2 Rots wide Reversal in Stable Structures Dipole and Quadrupole Dominate

3 Cycles of the Computed HCS Inclination Best SS Radius may be 1.8 Rs this minimum – Sun & Hoeksema SH11A-1487

From McComas et al., GRL 2008 Ulysses Observed Different Solar Wind Structure During Solar Minimum in 1996 compared with 2008 Low-latitude is more complex and wider due to Decreased importance of Polar Coronal Holes Thanks to J. Luhmann Note: Coronal snapshot useful, but may mislead since structure reflects rotation

Ulysses also saw low IMF at high heliolatitudes in 2007 (Smith et al., GRL, 2008) –OMNI data from NSSDC Thanks to J. Luhmann IMF Measured at L1 is Significantly Weaker this Minimum than the Previous Three IMF observed to be uniform at all latitudes away from HCS

Thanks to J. Luhmann Computed open flux foot points – Coronal Hole Proxy Each Panel shows ~10 years starting Low latitude holes are relatively more important during this solar minimum

(GONG website movie, MSFC sunspot illustrations) The long decline of Solar Cycle 23 has been marked by very few, well separated Active Regions

Comparison of Large-Scale Corona in Cycles 21 & 23 Panels spaced By 12 rotations. CYCLE 23: Longer Fewer Contours Gradual Flattening Structures Persist More Dipole in Declining Phase Cycle 21Cycle 23

Comparison of Large-Scale Corona in Cycles 22 & 23 Panels spaced By 12 rotations. Cycle 23: Fewer Contours Slower Flattening Structures Persist Thanks to Weak Poles Both Dipolar During Reversal Cycle 22Cycle 23

Back to the Photospheric Field

Zonal Average of Total Flux and Net Flux – 3 Cycles from WSO ~2001 WSO Sensitivity

Antisymmetric Zonal Symmetric Zonal Old Polarity Surge 2003/4

Toroidal (East-West) Field – 3 Cycles from WSO Cycles overlap several years and are extended Work with Leyan Lo & Phil Scherrer

From wattsupwiththat website Comparison of SSN for last 5 Cycles

From Wikipedia website Perspective Comes from Taking the Long View

Summary - 1 Cycle 23 was longer and weaker (relative to 21 and 22): MF, pole, meridional flow, corona, solar wind, dipole Polar Reversal on time, but no subsequent growth – no organized poleward migration Corona/Heliosphere not as constrained by dominant Polar Coronal Holes

Summary - 2 Corona/Heliosphere not constrained by dominant Polar Coronal Holes in declining phase of Cycle 23 HCS continued to reach high latitude Mid latitude structure in solar wind and low latitude coronal holes Very few spots in last few years.

Summary - 3 Zonal Flux Reduced Poleward flows small Antisymmetric flows at low latitude only 2002 not like 1991, 1981 Old polarity anti- symmetric flow in 2003 Interesting to learn what was ‘absent’ in Toroidal flux pattern about the same New flux emerges just after previous max at high latitude and expands equatorward