Download - Report on ‘Extreme Space Weather Events’ workshop that I co-organized in Boulder in June 2014
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Report on ‘Extreme Space Weather Events’ workshop that I co-organized
in Boulder in June 2014
Leif SvalgaardStanford University
Stanford Solar Group Science MeetingsJuly 2, 1024
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Extreme Space Weather Events II
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ProgramMonday, June 09 (chair: Noe Lugaz)
09:00 NASA Presentation on LWS Program
09:15 Invited talk: The Maunder and other Grand Minima (Owens)
Session 3: Limits to the maximum flare energy of stars from formation to solar age (Soderblom/Osten)
Session 4: Conditions Leading to Extreme SEP Events (Cohen/Mewaldt/Li)
Session 9: Understanding the Maunder Minimum (Svalgaard/Riley)
Tuesday, June 10 (chair: Dave Soderblom)
Session 9: Understanding the Maunder Minimum (Svalgaard/Riley)
Session 7: Extreme Space Weather: Campaign Events (Dayeh/Lugaz)
Session 1: Interpretation of Ice Core Records as Proxies of ESWEs (Smart/Dibb/Randall)
Session 5: Extreme CMEs: Origins and Evolution (Manchester/Torok)
Wednesday, June 11 (chair: Leif Svalgaard)
Session 2: 775 event and Aurora during ancient times (Shea)
Session 6: Extreme Events: What constitutes them and what are their effects? (Townsend)
Session 8: Propagation of extreme events through the atmosphere (Randall/Solomon)
http://www.predsci.com/eswe-workshop/presentations-unsorted/
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14C increase 775 and 993 AD:
Aurora observations in ancient times.
M. A. Shea
Session 2
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Jull et al., 2014
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Possible explanations:
Extreme Solar Proton EventComet Collision - January 773Gamma-ray Burst – Super Nova
HOW CAN OUR MODERN KNOWLEDGE HELP IN THE UNDERSTANDING OF
HISTORICAL PHENOMENA?
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Sharp rise may indicate a near West-limb flare. If so, the CME may not have hit Earth
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THINGS WE HAVE LEARNED:
MAJOR SPEs FROM CENTRAL MERIDIAN ACTIVITYGENERALLY HAVE SOFTER SPECTRA THAN EVENTS FROM THE WEST LIMB.
MAJOR HIGH ENERGY ( 4 GeV) SPEs FROM CENTRAL MERIDIAN ACTIVITY ARE RARE.
MAJOR HIGH ENERGY SPEs ARE NOT ALWAYS ASSOCIATED WITH A SUBSEQUENT GEOMAGNETIC STORM.
MAJOR GEOMAGNETIC STORMS CAN OCCUR WITHOUT A LARGE SPE.
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CAN IDENTIFICATION OF LOW LATITUDE AURORA HELP TO RESOLVE UNUSUAL GEOPHYSICAL RECORDS SUCH AS 14C INCREASES IN TREE RINGS?
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CHANGE IN MAGNITUDE OF THE G(1,0) TERM OF THE EARTH’S MAGNETIC FIELD, 1600-2010
(18% decrease in 400 years)
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EXAMPLES OF GEOMAGNETIC LATITUDE CHANGES
LOCATION 1000 2000 CHANGE
S. SPAIN 35° N 40° N 5° NSAN DIEGO 25° N 40° N 15° NCHICAGO 36° N 51° N 15° NEGYPT 34° N 28° N 6° STASMANIA 38° S 50° S 12° S
(VALUES ARE APPROXIMATE)
So far, no known aurorae in ~775 AD
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HISTORIC MID AND LOW LATITUDE AURORA
• Oct 817 Iraq• 816/817 Yemen• Oct 879 Morocco• 939-940 Syria• May 941 Spain• Aug 977 Egypt• Sept 979 Morocco• 991-992 Egypt*• Apr 1050 Egypt*• 1059-1060 Egypt
• 1176 Syria*• May 1179 Syria• Nov 1203 Yemen• 1223 Syria*• 1264 Syria*• 1321/1322 Yemen• Nov 1370 Syria• 1422-23 Egypt• Aug 1449 Yemen• 1570-71 Spain
• * Suspected aurora
Ref: Basurah, Sol. Phys, 225,2005; JASTP, 68, 2006
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We have the Needle, where is the haystack?
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Hypothetical 775 AD Free Space Doses
• Organ doses behind 5 g cm-2 Al shielding- skin: 9 Gy-Eq (1.5) (NASA limits)
- eye lens: 7 Gy-Eq (1.0)- BFO: 4.1 Gy-Eq (0.25)- CNS: 4.3 Gy-Eq (0.5)- Heart: 3.4 Gy-Eq (0.25)- Eff. Dose:4.1 Sv (≤ 1.2) (4π)
• These doses are likely lethal Larry Townsend
2 cm
1 Gy-Eq (gray) is an absorbed dose of 1 J/kg
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Feb 1956 Free Space Doses
• Organ doses behind 5 g cm-2 Al shielding
- skin: 0.42 Gy-Eq (1.5)
- eye lens: 0.33 Gy-Eq (1.0)
- BFO: 0.19 Gy-Eq (0.25)
- CNS: 0.20 Gy-Eq (0.5)
- Heart: 0.16 Gy-Eq (0.25)
- Eff. Dose: 0.19 Sv (≤ 0.6) (2π)• These doses are below applicable NASA limits
Largest GLE observed
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Hypothetical 775 AD Free Space Doses
• Organ doses behind 40 g cm-2 Al shielding- skin: 1.5 Gy-Eq (1.5)- eye lens: 1.5 Gy-Eq (1.0)- BFO: 1.2 Gy-Eq (0.25)- CNS: 1.3 Gy-Eq (0.5)- Heart: 1.4 Gy-Eq (0.25)- Eff. Dose: 1.4 Sv (≤ 1.2)
• Possibly lethal but certainly acute radiation syndrome effects (“radiation sickness”).
15 cm
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Solar Flare Energetics
C. Schrijver, How bad can it get?
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White-Light Flaring on Stars,
Kepler
Kepler
Sun
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Extreme Solar Flares. Where are they?
Maximum for cool stars in general: ~3 1036 erg
Kepler observations of Sun-like stars suggest continuation up to at least ~5 1035 erg
Estimated fluence needed to create the 775AD 14C spike
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Sizes of Spots as a Function of Flare Energy
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The Worst Space Weather
Stellar data reveal that some space weather can be much more severe than what we have recently experienced:
• Solar flares may reach energies up to 100-300 times above those observed in the past four decades.
• Effects on Earth may (luckily) saturate at values several times Space-Age maxima
• All these potential extremes exceed the levels to which modern technologies, connected in a network of growing complexity, have been exposed.
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INTRODUCTION AND OVERVIEW OF
ICE CORE RECORDS AND
EXTREME SOLAR PROTON EVENTS
The Current Nitrate Spike Controversy
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VERY LARGE HIGH ENERGY SOLAR COSMIC RAY EVENTS DURING THE COSMIC RAY MEASUREMENT ERA
GLE = Ground Level Event of Solar Cosmic Rays. Only ~72 are known
1956 GLE biggest observed
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24Nitrate ( ) and conductivity (▄ ▼) data from the GISP2-H ice core for 1955-1957.
GLE # 5
GLE#6
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Historic NO(y) events
McCracken et al. documented 70 potential impulsive NO(y) increases in the interval 1562 to 1950, all equivalent to or larger than the February 1956 event.
These have been essentially ignored, except for a few.
Jack Dibb noted a probable biomass event in 1895
Note that there are impulsive NO(y) increases where
there are not large increases in conductivity.
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There are at least 40 impulsive nitrate events in the last 300 years, each as large as the February 1956 high energy solar cosmic ray event that should be detectable in high time resolution polar ice cores.
None of these correspond to dated biomass burning events in the Zoe or D4 ice cores.
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Po
lar
Nig
ht
A stable polar vortex
isolates air.
NOx
diabatically descends over winter pole.
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Conclusions• SPEs significantly increase reactive nitrogen and decrease ozone in
the stratosphere following November 2000 events.
• No convincing evidence that SPEs are related to impulsive nitrate spikes.
• Tropospheric sources provide an alternative explanation for nitrate spikes at Summit during the winter of 2000-2001.
Remaining Questions• How large would an SPE have to be to produce discernable nitrate spikes
at the surface, given the limits of solar flare energy?• Longer-term variations in nitrate related to solar activity continue to be
of interest (Gleissberg cycles, millennial variations, etc.). • Are there alternative proxies for SPEs? On what timescale can
cosmogenic radionuclides (e.g., 14C and 10Be) or other isotopes be used to study solar variability? The controversy continues…
K .A. Duderstadt, J.E. Dibb, C.H. Jackman, C.E. Randall, S.C. Solomon, M.J. Mills, N.A. Schwadron, H.E. Spence
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To predict Extreme Events we need to understand Ordinary
Events and Ordinary ‘Background’ in the historical setting
Svalgaard, Boulder 2014
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Progress in Reconstructing Solar Wind Magnetic Field back to 1840s
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1840 1850 1860 1870 1880 1890 1900 1910 1920 1930 1940 1950 1960 1970 1980 1990 2000 2010 2020
LEA13 Done Right
u HLS
u, IDV(1d)
u Bartels u ESK
IDV13
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1840 1850 1860 1870 1880 1890 1900 1910 1920 1930 1940 1950 1960 1970 1980 1990 2000 2010
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IDV
B
StDev
nT
HMF
InterDiurnal Variability Index IDV and Reconstructed Heliospheric Magnetic Field B
Even using only ONE station, the ‘IDV’ signature is strong enough to show the effect
Svalgaard 2014
Using u-measure
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After a Decade of Struggle, Lockwood et al. (2014) are Fast Approaching the Svalgaard et al. Reconstructions of 2003
This is a healthy development and LEA should be congratulated for their achievement, although their model, based on a flawed Sunspot Number series, is not doing too well
Svalgaard et al. 2003
Svalgaard et al. 2003
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Schwadron et al. (2010)
HMF B Model,
with my set of parameters
von Neumann: “with four parameters I can fit an elephant, and with five I can make him wiggle his trunk”
This model has about eight parameters…
“It is not clear if the version of the code obtained from the original authors is incomplete or in some other way inaccurate”
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The Tale of Two Models…
Too Low
GSN too low SSN too low
The models operate with the ‘open [radial] flux’, so it is important to get that right
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As the Sunspot Number is used as Model input it is important to get that right
• Four recent Sunspot Number Workshops (2011-2014) have critically examined the historical sunspot number record(s)
• There is now broad consensus among the participants that we have identified the major problems with the SSN series:
• A) Error (65%) in Wolf-Wolfer calibration for the GSN before ~1882
• B) Weighting of sunspot counts (20%) for the Int. SSN starting in 1940s
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Counting with no Weighting
1
6
2
9
1xx
19
5x10+44=94 5x10+19=69
94/69 = 1.36
Recounted 2003-2014: ~55,000 spots
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Effect on the Wolf Number
Factor to remove weighting 0.8535 [inverse of 1.17]
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SSN4: No Modern Grand Maximum
The preliminary new sunspot record expressed in terms of the number of sunspot groups. Of note is that there is a maximum in every century, none of them particularly ‘Grand’.
The new Wolf Number should be used as model input and we should understand the behavior and the fit of the model to the new perspective and to HMF B before we can extrapolate with any degree of confidence to the Maunder Minimum.
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No Rising Background ‘Base Level’
Open Flux TSI (LASP)
GSN Corr. SSN
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Perhaps the Maunder Minimum was Less Extreme than we Thought
The emergence of ‘ephemeral regions’ does not show any solar cycle dependence [e.g. Hagenaar, 2008], thus no ever-increasing background
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MHD Modeling [Riley et al.]
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1994 1996 1998 2000 2002 2004 2006 2008 2010 2012 2014 2016
0.0
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1.0|Br| nT
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Radial component HMF at Earth
Br
-Br
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B
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1-minute averages
0.45
|Br|1day
Computed Radial HMF at 1 AU
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-10 -9 -8 -7 -6 -5 -4 -3 -2 -1 0 1 2 3 4 5 6 7 8 9 10
2009 OMNI, 480796 1-minute data,Bin-width 0.1 nT
-1.60 nT +1.75 nT
Radial Component of B
|Br| = 1.68 nT 2009
Polar Fields needed
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Cosmic Ray Proxy [Berggren et al., 2009]
GSNM.M.
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We do not understand the 10Be modulation“we have an upper limit to the absolute maximum 10Be flux which is only ~1.25 times the recent average maximum intensity of 10Be measured. This value corresponds to the lowest bound of the shaded region in Figure 5. This lower bound includes many other earlier time periods with 10Be flux values that exceed those possible from 10Beproduction alone from the full LIS spectrum. Indeed this implies that more than 50% the 10Be flux increase around, e.g., 1700 A.D., 1810 A.D. and 1895 A.D. is due to non-production related increases! “
“Other influences on the ice core measurements, as large as or larger than the production changes themselves, are occurring. These influences could be climatic or instrumentally based. We suggest new ice core measurements that might help in defining more clearly what these influences are and-if
possible-to correct for them. “ Webber et al. arXiv:1004.2675 (2010)
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‘Burning Prairie’ => Magnetism
Foukal & Eddy, Solar Phys. 2007, 245, 247-249
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Birth of an Active Region
Visible Light
NOAA 11158, February, 2011
Solar Dynamics Observatory (SDO)
“All the Sun, All the Time”
Sunspots grow by the accumulation of smaller spots and pores.
You may have to click on the area to play the movie.
It may not play on a Mac.
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My Personal Working Hypothesis
• The Maunder Minimum was not a serious deficit of magnetic flux, but
• A lessening of the efficiency of the process that compacts magnetic fields into visible spots
• This may now be happening again soon
• If so, there is new solar physics to be learned
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Perhaps like this:
2012-10-17
Magnetic Field Visible Light
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The Maunder Minimum is as Mysterious as Ever
(but so was the notion a decade ago that we would ever
successfully reconstruct the solar wind properties for the
past 170 years…)