Closing the Books on Cycle 24 J

Slides:



Advertisements
Similar presentations
Sunspots and the Scientific Method: Models. Hypothesis Driven Science Hypothesis: An educated speculation about how a particular phenomenon behaves- very.
Advertisements

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.
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.
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.
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.
AGU – Fall 2006 The Solar Polar Field – Cycles 21 – 23 The Solar Polar Field During Solar Cycles J. Todd Hoeksema, Yang Liu, XuePu Zhao & Elena Benevolenskaya.
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,
Identifying and Modeling Coronal Holes Observed by SDO/AIA, STEREO /A and B Using HMI Synchronic Frames X. P. Zhao, J. T. Hoeksema, Y. Liu, P. H. Scherrer.
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.
Accurate Polar and small scale observations during the solar cycle Elena E. Benevolenskaya Yang Liu J. Todd Hoeksema Stanford University HMI/AIA meeting,
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.
1 A Statistical Study about Transequatorial loops Jie Chen National Astronomical Observatories Chinese Academy of Sciences.
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.
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.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Sun: Magnetism Feb. 09, 2012.
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.
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.
The Sun and Cycle 24 David Treharne, N8HKU Ford Amateur Radio League January 12th, 2012.
Charles Hakes Fort Lewis College1. Charles Hakes Fort Lewis College2 Chapter 9 The Sun.
The Solar Wind.
Propagation Trends Dayton 2014 Solar Maximum! But the slow decline to solar minimum in 2020 is likely to begin later this year.
Solar Maximum ! A Double Peaked Sunspot Cycle ?
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.
PCI analysis of Sunspot and Background Magnetic Field variations in the cycles V.V. Zharkova 1, S.I. Zharkov 2, Shepherd S.J. 3 and Popova 4 Zharkov.
1 The Mean Field of the Sun Leif Svalgaard Stanford University Sept. 2, 2011.
ILWS Workshop,Ubatuba, Brazil, October What is Solar Minimum and Why Do We Care? W. Dean Pesnell NASA, Goddard Space Flight Center.
Polar Magnetic Field Elena E. Benevolenskaya Stanford University SDO Team Meeting 2009.
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.
The Helioseismic and Magnetic Imager (HMI) on NASA’s Solar Dynamics Observatory (SDO) has continuously measured the vector magnetic field, intensity, and.
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.
CSI /PHYS Solar Atmosphere Fall 2004 Lecture 04 Sep. 22, 2004 Solar Magnetic Field, Solar Cycle, and Solar Dynamo.
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.
Estimation of acoustic travel-time systematic variations due to observational height difference across the solar disk. Shukur Kholikov 1 and Aleksander.
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.
The Sun.
The Decline to Solar Minimum 2014 through about 2020
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)
Introduction to Space Weather
A Comparison of Solar Polar Coronal Hole Areas
Chapter 1 Cycles of the Sky
Large-Scale Solar Magnetic Fields – How is Solar Cycle 24 Different?
What is the most basic reaction that happens in the sun?
Carrington Rotation 2106 – Close-up of AR Mr 2106 Bt 2106
Current HMI Polar Fields
Astronomy-Part 10 Notes The Earth-Moon-Sun Systems
Introduction to Space Weather
Solar Activity Chapter 8 Section 3.
­Long-Term Variation of Latitudinal Distribution of Coronal Holes
Solar and Heliospheric Physics
Solar Activity Chapter 8 Section 3.
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.
What is an Extreme Solar Minimum?
by Andreas Keiling, Scott Thaller, John Wygant, and John Dombeck
Presentation transcript:

Closing the Books on Cycle 24 J Closing the Books on Cycle 24 J.T Hoeksema, Solar Observatories Group, Stanford University This material is based in part upon work supported by the National Science Foundation under Grant Number #1836370 Opinions, finding, and conclusions or recommendations expressed in this material are those of the author and do not necessarily reflect the view of the NSF The Mean Field and Large-Scale Multipole Components The figures show the solar magnetic field from May 1976 to the present, covering nearly 4 solar cycles. Cycle 24 was weak. (Top): The mean field (MF) shows the Sun viewed as a star, where all magnetic signals from the visible disk are integrated. The MF typically peaks during solar maximum or a little later. Cycle 24 was relatively weak, but the peak was comparable to or larger than recent cycles and was reached 2015 as a consequence of the development of a large low-latitude unipolar region over several months. (Second Plot) The global photospheric field can also be decomposed into multipoles. The polar dipole reverses at or a little after solar minimum. The three panels show the total dipole and its polar and equatorial components. (Third Plot) The total magnitude of the low-order multipoles of the solar field – dipole, quadrupole, and octupole – show different aspects of the evolving solar cycle because they are sensitive to different parts of the Sun. (Fourth Plot) The axial zonal (m=0) multipoles for l=1-8 are shown in the panels of the bottom plot. The odd axial multipoles are in some ways similar evolution to the dipole(l=1), being sensitive to the poles. The even multipoles reflect more of what happens at lower latitudes and are sensitive to hemispheric asymmetry. Zonal Averages (Top) The upper two panels show zonal averages of the magnetic field from 1976 to the present. The lower panel resembles the butterfly diagram; it tracks the total unsigned flux at each latitude averaged over complete solar rotations with time. The upper panel is the average of the net flux vs latitude. It shows the emergence of leading and following polarity bands in the activity belt with poleward surges of following polarity reaching high latitudes a year or two later. (Bottom) Similar zonal average of the net flux in Cycle 24 computed using higher-resolution HMI data. The effects of active regions can be seen in some detail, as can the development and evolution of the poleward surges. Arriving surges erode or reinforce the predominant polar field. From X. Sun and M. Bobra at jsoc.stanford.edu/data/hmi/polarfield Solar activity has waned to the point where the end of Cycle 24 appears to be at hand and we can start looking for the first signs of Cycle 25. This is a good time to look back on Cycle 24, identify some of its key features, make comparisons with earlier cycles, and look forward to the next one. Both polar fields have reversed and intensified. There have already been many spotless days. The magnetic structure of the corona and heliosphere is simplifying. By most measures Cycle 24 was the weakest in a century, the asymmetry between north and south was great, and despite being the best-measured cycle in history, it was not well forecast. The Polar Field The Sun’s polar field reverses independently in the north and south as a consequence of dissipating active-region flux carried by meridional flow from lower latitudes. Cycle 24 showed an early, gradual reversal in the north, followed 16 months later by a more typical abrupt reversal in the south. The top three figures show the flux measured in the pole-most pixel above 55 degrees at the WSO since 1976. (Top) The north and negative of the South are plotted in the top figure along with their average. (Two middle) The next two panels show the north and south separately. There is a strong annual variation due to the changing view of the Sun’s polar regions. (Bottom) The bottom panel shows a similar plot (60 degrees and above) for Cycle 24 from 2010 to the present computed from HMI on SDO. The north is red and the south blue. The north (south) reversal was Nov 2012 (Mar 2014). The anomaly in the north is due to some temporarily missing data at the time the plot was made. Searching for the New Cycle Hints of Cycle 25 are beginning to emerge. As reported at SpaceWeather.com on November 20: … Ephemeral sunspots possibly belonging to Solar Cycle 25 have already been reported on Dec. 20, 2016, and April 8, 2018. Now we can add Nov. 17, 2018, to list. The new spots so far have been weak and short lived. The two HMI images from November 17 show the magnetic field and flattened continuum intensity observed at 21 UT. Can you detect the new spots inside the circle? Butterfly Diagram The latitudinal location of magnetic flux evolves during the solar cycle. The classic butterfly diagram since the 1870s shows the locations of sunspot during each cycle. Sunspots emerge at lower latitudes as each cycle progresses. Cycles can overlap at different latitudes. The plot was last updated by D. Hathaway in 2016. Tilt Angle Effects of solar activity extend into the helio-sphere. One consequence is the shape of the heliospheric current sheet. The HCS separates regions in the solar wind where the magnetic field points predominantly toward or away from the Sun along the Parker spiral. See the purple figure for a classic artist’s representation of the HCS. The shape of the HCS surface changes with the solar cycle, being relatively flat at solar minimum and reaching to high latitude at solar maximum. The maximum latitude (averaged over the two hemispheres) is frequently called the tilt angle. The figure shows how the tilt angle has evolved from 1976 to the present as determined by a calculation of the coronal field using a potential field – source surface model applied to photospheric observations from WSO. Sunspot Number These recent plots published by the Royal Observatory of Belgium show characteristics of the last several solar cycles. (Above Left) Sunspot numbers since 1700 show that Cycle 24 was small, but not much different than Cycle 14 at the beginning of the 20th century and was larger than cycles 4 and 5 early in the 19th. (Above Center) The middle panel shows the difference in northern and southern hemisphere sunspot numbers since 1950. Green(red) indicates a larger number in the north (south). Cycle 24 was the most asymmetric. (Above Right) Daily, monthly, and smoothed sunspot number since 2006 showing Cycle 24. The minimum at the end of Cycle 24 is at hand.