1 Long-term Solar Synoptic Measurements with Implications for the Solar Cycle Leif Svalgaard Stanford University 23 April 2013.

Slides:



Advertisements
Similar presentations
1 Livingston & Penn Data and Findings so Far (and some random reflections) Leif Svalgaard Stanford, July 2011.
Advertisements

The Solar Radio Microwave Flux and the Sunspot Number Leif Svalgaard Stanford University, Stanford, CA, USA. [ Hugh S Hudson University.
2011/08/ ILWS Science Workshop1 Solar cycle prediction using dynamos and its implication for the solar cycle Jie Jiang National Astronomical Observatories,
Sunspots and the Scientific Method: Models. Hypothesis Driven Science Hypothesis: An educated speculation about how a particular phenomenon behaves- very.
Microwave fluxes in the recent solar minimum H. Hudson, L. Svalgaard, K. Shibasaki, K. Tapping The time series of solar microwave flux traditionally is.
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.
Sixty+ Years of Solar Microwave Flux Leif Svalgaard Stanford University SHINE 2010, Santa Fe, NM.
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.
East-West Asymmetry of the Yohkoh Soft X-ray Corona L.W. Acton 1, D.E. McKenzie 1, A. Takeda 1, B.T. Welsch 2,and H.S. Hudson 2,3 1 Montana State University,
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.
High-latitude activity and its relationship to the mid-latitude solar activity. Elena E. Benevolenskaya & J. Todd Hoeksema Stanford University Abstract.
A particularly obvious example of daily changing background noise level Constructing the BEST High-Resolution Synoptic Maps from MDI J.T. Hoeksema, Y.
Helioseismic Magnetic Imager and Why We Study Helioseismology Junwei Zhao W. W. Hansen Experimental Physics Laboratory, Stanford University, Stanford,
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.
Relationship between the High and mid latitude Solar Magnetic Field Elena E. Benevolenskaya J. Todd Hoeksema Stanford University.
Temperature Minimum Region between the Minimum-Activity Epochs and W. Livingston and E. Avrett AGU Fall Meeting, 2003.
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.
A particularly obvious example of daily changing background noise level Constructing the BEST High-Resolution Synoptic Maps from MDI J.T. Hoeksema, Y.
Session 6 Key Questions for Understanding This Unusual Solar Minimum Alan Gabriel Todd Hoeksema Janet Luhmann Bill Matthaeus Neil Sheeley.
Polar Network Index as a magnetic proxy for the solar cycle studies Priyal, Muthu, Karak, Bidya Binay, Munoz-Jaramillo, Andres, Ravindra, B., Choudhuri,
Variation of the mm radio emission in the polar zones of the Sun. A.Riehokainen, J.Kallunki.
Prediction on Time-Scales of Years to Decades Discussion Group A.
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.
Synoptic Solar Cycle observed by Solar Dynamics Observatory Elena Benevolenskaya Pulkovo Astronomical Observatory Saint Petersburg State University ‘Differential.
Update on Cycle 24 Giuliana de Toma collaborators: Gary Chapman, Angie Cookson, Dora Preminger data sources: CSUN/SFO, USAF/SOON, McMath, SOHO/MDI, SDO/AIA.
1 Solar Wind During the Maunder Minimum Leif Svalgaard Stanford University Predictive Science, San Diego, 4 Sept
The Sun as a Star The “Surface” of the Sun and Its Structure Outer Layers – 3 distinct region Photosphere Chromosphere Corona.
1 C. “Nick” Arge Space Vehicles Directorate/Air Force Research Laboratory SHINE Workshop Aug. 2, 2007 Comparing the Observed and Modeled Global Heliospheric.
1 Something with ‘W’ Leif Svalgaard March 1, 2012.
Activity Cycles in Stars Dr. David H. Hathaway NASA Marshall Space Flight Center National Space Science and Technology Center.
Proxies of the Entire Surface Distribution of the Photospheric Magnetic Field Xuepu Zhao NAOC, Oct. 18, 2011.
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.
Modern Solar Mysteries Dr. David H. Hathaway NASA/MSFC National Space Science and Technology Center Dr. David H. Hathaway NASA/MSFC National Space Science.
Are There Any Wild Cards in Global Climate Change? Ernest M. Agee Earth & Atmospheric Sciences Purdue University 28 August 2008.
1 The Spots That Won’t Form Leif Svalgaard Stanford University 3 rd SSN Workshop, Tucson, AZ, Jan
The Polar Fields Seen in 17 GHz Microwave Flux and with Magnetographs Leif Svalgaard Stanford University 6 January, 2012.
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 The Mean Field of the Sun Leif Svalgaard Stanford University Sept. 2, 2011.
Andrés Muñoz-Jaramillo Harvard-Smithsonian Center for Astrophysics
Solar Cycle Variation of the Heliospheric Magnetic Flux, Solar Wind Flux and Galactic Cosmic Rays Charles W. Smith, Nathan A. Schwadron Ken G. McCracken,
Polar Magnetic Field Elena E. Benevolenskaya Stanford University SDO Team Meeting 2009.
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,
SHINE 2009 Workshop, August What is an Extreme Solar Minimum? W. Dean Pesnell NASA, Goddard Space Flight Center.
Universe Tenth Edition Chapter 16 Our Star, the Sun Roger Freedman Robert Geller William Kaufmann III.
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.
1 CALIBRATING 100 YEARS OF POLAR FACULAE MEASUREMENTS: IMPLICATIONS FOR THE EVOLUTION OF THE HELIOSPHERIC MAGNETIC FIELD Andrés Muñoz-Jaramillo, Neil R.
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.
Using the paleo-cosmic ray record to compare the solar activity during the sunspot minimum of with those during the Spoerer, Maunder, and Dalton.
To what extent does solar variability contribute to climate change? Dr. David H. Hathaway NASA/Marshall Space Flight Center National Space Science and.
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.
Shivam Raval Indian Institute of Technology, India
HMI-WSO Solar Polar Fields and Nobeyama 17 GHz Emission
Diagnosing kappa distribution in the solar corona with the polarized microwave gyroresonance radiation Alexey A. Kuznetsov1, Gregory D. Fleishman2 1Institute.
Estimates of the forthcoming solar cycles 24 and 25
Babcock-Leighton Dynamo Theory and Solar Cycle #24
Large-Scale Solar Magnetic Fields – How is Solar Cycle 24 Different?
The use of 17 GHz radio emission to characterize the solar minimum
Current HMI Polar Fields
Introduction to Space Weather
Solar and Heliospheric Physics
What is an Extreme Solar Minimum?
Closing the Books on Cycle 24 J
Presentation transcript:

1 Long-term Solar Synoptic Measurements with Implications for the Solar Cycle Leif Svalgaard Stanford University 23 April 2013

2 Dimensions of Synoptic Observations Time Dimension (long-term data sets) Spatial Dimension (distribution over the disk of activity, synoptic maps, height, depth) Most efficient are visualizations combining the two dimensions, e.g. Movies, Butterfly diagram, Rotation sequences, …

3 Classes of Synoptic Observations Single Point (e.g. Center Disk spectra) Full-Disk (e.g. Sunspot Number, F10.7 flux, Mean Field, Total Solar Irradiance) Image-based (e.g. Sunspot Area, Ca K line index, Magnetograms, Synoptic charts) And aggregate views derived from images, e.g. Polar Field Evolution Hemispheric Asymmetries Meridional and ‘Torsional’ circulations

4 Synoptic Observations are Important for Understanding and Predicting the Solar Cycle With limited time for this presentation Leif can only touch upon some aspects that have been important for his own research It should, however, be clear how those relate to the wider issues, like constraining dynamo theories, forming inner boundary conditions for space weather, affecting the environment of the Earth and our space assets and technological infrastructure.

5 Predicting Solar Activity Sunspots Polar Fields Solar Prediction Panel, 2006 Observations and theory suggest that the magnetic field at the poles of the Sun at solar minimum is a good predictor of the next solar cycle. Theory: Deep circu- lation? The low polar fields at the recent solar minimum predicted a small cycle 24 Sunspots MWO* WSO ?

6 How is Cycle 24 Evolving? As predicted 9 years ago using the polar field precursor method D. Hathaway Prediction Cycle 24 is beginning to look like Cycle 14 Lowest in a 100 years SIDC

7 A different view of polar fields: Nobeyama Image of 17GHz Emission ν 17 GHz = λ1.76 cm ν e = B (Tesla) × 28 GHz Beam width 10” 1.General Limb brightening: Bremsstralung (free-free) from hot atmosphere [10,000 – 13,000 K] 2.Active regions bright: Gyro- resonance from strong fields

8 Coronal Holes Everywhere Show Same Behavior as the Polar Holes 3 Days later When a coronal hole is at the limb, the bright 17GHz patches appear, otherwise not Quantifying the Brightening:

9 Evolution of Patches over the Cycle Reversal E W W S N Poles

10 Excess T b over 10,800K, signed according to WSO polar field sign WSO Sensitivity in 2001

11 Using Polar Faculae Count to determine Polar Magnetic Flux and HMF Field Strength Andrés Muñoz-Jaramillo, Neil Sheeley, et al., 2013

12 Observed Polar Field Reversals MWO: Roger Ulrich, 2012 Supersynoptic charts MWO

13 And the ‘Rush to the Pole’ of Coronal Emissions Measurements of the location of ‘peaks’ of Fe XIV coronal emission at 503 nm (the ‘Green Line Corona’) over 7 solar cycles. The plots show the probability of observing a ‘peak’ at a given latitude as a function of time. Is there an ‘extended’ cycle of 17 years?

14 Asymmetric Solar Activity Spots & Groups 18

15 Comparing Cycles 14 and 24 Cycle 14 suggests that the activity in the South might pick up in cycle 24

Year ‘Gleissberg Cycle’ in Solar Activity Asymmetry? Zolotova et al., 2010 Is this a ‘regular’ cycle or just over-interpretation of noisy data [like Waldmeier’s]? ‘Prediction’ from this: South will lead in cycle 25 or 26 and beyond. We shall see… Extreme Asymmetry during the Maunder Minimum… There are various dynamo theoretical ‘explanations’ of N- S asymmetry. E.g. Pipin, I can’t judge these…

17 Cosmic Ray Modulation Depends on the Sign of Solar Pole Polarity Miyahara, 2011 The shape of the modulation curve [alternating ‘peaks’ and ‘flat tops’] shows the polar field signs. North pole Ice cores contain a long record of 10Be atoms produced by cosmic rays. The record can be inverted to yield the cosmic ray intensity. The technique is not yet good enough to show peaks and flats, but might with time be refined to allow this. Svalgaard & Wilcox, 1976

18 The Butterfly Diagram Schwabe Staudach Arlt Hathaway

19 We Observe Fewer Spots per Sunspot Group 431,000 daily obs. There is a weak solar cycle variation on top of a general downward trend seen by all observers As the sunspot number is primarily determined by the number of spots, the SSN will be too low as a measure of solar activity

20 TSI and CME-rate no longer following the Sunspot Number

21 Conclusions To enable practical prediction of solar activity synoptic observations in both space and time are indispensable The long-term evolution of the solar cycle can only be tracked [and eventually understood] by sustained and calibrated synoptic observations I must be preaching to the choir today