Category Archives: Solar Cycle 24

Solar Cycle 24 March Update


Solar Cycle 24 activity picked up in March.  Several coronal mass ejections (CME) came our way thanks largely to the sunspot group 1429.  March began  with a CME directed toward Earth.  Although the warnings suggested more severe problems than actually occurred,  it still was a reasonably strong storm. The Sun’s rotation brought sunspot 1429 back again at month-end and it provided a little more excitement.   A good summary of the solar activity in March can be found on the Solarham.com site.  To take a look at the summary,  click here.  This solar activity and it’s affect on the Earth’s geomagnetic field can be seen on the chart below: (click on charts to improve clarity)

Both the sunspot number and the F10.7 flux were below the predicted  monthly numbers in March but seem to be generally following the forecast Solar Cycle 24 forecast path.  See charts below:

 

Cycle 24—February Update


Cycle 24 activity took another drop in February.  The Sunspot number for February was about 30 versus the 60+ in January. (Click on Charts to expand.)

That’s a major drop in the sunspot number.  Cycle 24 certainly looks like it will be the least active cycle in the last hundred years.

Dr Hathaway of NASA has again revised his forecast of Cycle 24 Sunspots.  He now says that  the Cycle 24 sunspot number will peak (maximum) at 59. Below is his March 2012 sunspot number forecast:


F10.7 cm radio flux is down as well.  First shown on the NOAA chart followed by Dr Hathaways revised chart:

And the magnetic activity as indicated by the Ap index remains low:

cbdakota

Global Temperature Update—February 2012


The UAH satellite global temperatures have been posted by Dr Roy Spencer on his website.  The February temperature anomaly is -0.12 C.   That is just slightly down from the January number of -0.09C.

Above is Dr Spencer’s chart (click on it to enlarge) of the global temperature anomalies since the start of the satellite temperature-measuring program in the late seventies.  The average global temperature departure is about 0.16C warmer that the average temperature for the period 1981-2010.  Dr Spencer might not approve of this calculation but 0.16 C over that 30-year period might indicate a warming of about 0.6C per century.  Further, if solar Cycle 24 and the next Cycle 25 perform as many are now forecasting, we may see the anomaly go negative for many years.

cbdakota

Reliable Solar Cycle Forecasting Requirements


 

Dr David Hathaway is NASA’s solar cycle guru.  In 2010, he published in Solar Physics a review of the methods used to forecast solar cycle activity.   The review, titled TheSolar Cycle” is worth reading.  He discusses many of the techniques currently in use that purport to be the method for solar cycle forecasting. 

This post will only look at the key features that Hathaway says must be explained by any viable theory or model in order to provide a reliable forecast. 

The Abstract for “The Solar Cycle”  follows:

The Solar Cycle is reviewed. The 11-year cycle of solar activity is characterized by the rise and fall in the numbers and surface area of sunspots. We examine a number of other solar activity indicators including the 10.7 cm radio flux, the total solar irradiance, the magnetic field, flares and coronal mass ejections, geomagnetic activity, galactic cosmic ray fluxes, and radioisotopes in tree rings and ice cores that vary in association with the sunspots. We examine the characteristics of individual solar cycles including their maxima and minima, cycle periods and amplitudes, cycle shape, and the nature of active latitudes, hemispheres, and longitudes. We examine long-term variability including the Maunder Minimum, the Gleissberg Cycle, and the Gnevyshev–Ohl Rule. Short-term variability includes the 154-day periodicity, quasi-biennial variations, and double peaked maxima. We conclude with an examination of prediction techniques for the solar cycle.

Hathaway lists the critical features for making an accurate forecast:  

Understanding the solar cycle remains as one of the biggest problems in solar physics. It is also one of the oldest. Several key features of the solar cycle have been reviewed here and must be explained by any viable theory or model.  (I am adding several charts to aid in visualize his thinking.)

  • The solar cycle has a period of about 11 years but varies in length with a standard deviation of about 14 months.
  • Each cycle appears as an outburst of activity that overlaps with both the preceding and following cycles by about 18 months.
  • Solar cycles are asymmetric with respect to their maxima – the rise to maximum is shorter than the decline to minimum and the rise time is shorter for larger amplitude cycles.
  • Big cycles usually start early and leave behind a short preceding cycle and a high minimum of activity.
  • The activity bands widen during the rise to maximum and narrow during the decline to minimum.
These  sunspot charts show the last stages of cycle 21, cycles 23 and 23 fully and the current status of cycle 24.  The overlapping between the end of one cycle and the start of the other is apparent.   The relatively steep rise in the sunspot count at the begining of a new cycle and the more gradual decent.  Cycle 24’s rise is not nearly as steep as its predecessors.  Charts by Leif Svalgaard.
  • Sunspots erupt in low latitude bands on either side of the equator and these bands drift toward the equator as each cycle progresses.
  • At any time one hemisphere may dominate over the other but the northern and southern hemispheres never get completely out of phase.
  • Sunspots erupt in groups extended in longitude but more constrained in latitude with one magnetic polarity associated with the leading (in the direction of rotation) spots and the opposite polarity associated with the following spots.
  • The leading spots in a group are positioned slightly equatorward of the following spots and this tilt increases with latitude.

Butterfly Diagram: All the sunspots in a give cycle are plotted on the charts above. The initial sunspots appear at about 30° North and South lattitude. As new spots appear they tend to get closer to the equator. Each solar cycle ends, nominally, when the spots reach the equator. Charts by Solar Physics Group @ NASA

  • The polar fields reverse polarity during each cycle at about the time of cycle maximum.

Solar Magnetic Fields: This chart shows the North and South magnetic fields reversing at the end of a solar cycle. Note how weak the magnetic fields are for the start of the current cycle 24. Chart by Leif Svalgaard.

  • Cycle amplitudes exhibit weak quasi-periodicities like the 7 to 8-cycle Gleissberg Cycle.

The Gleissberg Cycle is a period of about 80 to 90 years that overlays the well established 11 year cycle.  The theory is that solar maxima and solar minima are forced by the gravitational pull of the major planets.  The specific alignment, particularily Jupiter and also Saturn Neptune and Uranus have a major effect on the Sun’s activity.  To see graphics of the alignment of these major planets, click here.

  • Cycle amplitudes exhibit extended periods of inactivity like the Maunder Minimum.
  • Solar activity exhibits quasi-periodicities at time scales shorter than 11 years.
  • Predicting the level of solar activity for the remainder of a cycle is reliable 2 – 3 years after cycle minimum.

Hathaway tells us that theory must be able to predict the preceding.  Until then,  people will continue to predict the features of the next solar cycle but it may be just luck if they get it right.

cbdakota

Cycle 24 January Update


Cycle 24 activity in January was low.  Cycle 24 solar maximum is probably about 18 months away.   The January sunspot number and the F10.7 flux are following the NASA forecast.  The very low Ap index seems confirm that this cycle is likely to be much less active than Cycle 23.  See the charts below, all courtesy of NOAA/SWPC. (click on charts to enlarge)

cbdakota


Forecasting Cycle 25—Great Conveyor Belt Theory


The last post reviewed a forecasted solar Cycle 25 based upon measuring the magnetic field of sunspots.   This posting uses the speed of the Sun’s Great Conveyor Belt(GCB) to forecast Cycle 25. This method considers sunspots as an indicator but the GCB speed determines how many sunspots appear.  I am not sure who, but perhaps Dibyendu Nandi of the Indian Institute of Science and Education and Research in Kolkata (aka, Calcutta) and his team  can claim this theory. The GCB has been studied for a number of years.  NASA Science says: “The Great Conveyor Belt is a massive circulating current of fire (hot plasma) within the sun. It has two branches, north and south, each taking about 40 years to complete one circuit.“  “The plasma flows travel along the Sun’s surface and plunge inward at the poles, and reappear again at the Sun’s equator.  When the sunspots begin to decay, surface currents sweep up their magnetic remains and pull them down inside the star; 300,000km below the surface, the sun’s magnetic dynamo amplifies the decaying magnetic fields.  Re-animated the sunspots become buoyant and bob up to the surface like a cork in water—voila! A new solar cycle is born.”

These belts can be likened to the Earth’s ocean currents.

NASA’s artistic sketch of the belt.

A May 2006 posting on Science News has Dr Hathaway predicting that Cycle 24 sunspots numbers would be perhaps greater than Cycle 23 (this part of the prediction is not faring well.) and Cycle 25 would be perhaps half of Cycle 23.  Dr Hathaway said that these predictions were based on a deceleration of these belts to 0.75m/s in the North and 0.35m/s in the south.  He said “We’ve never seen speeds so low”.    Hathaway in a September 2011 posting said:”…….that as the number of sunspots increases on the Sun, the speed of the GCB decreases and vice versa: fewer sunspots and the faster the speed of the Belt.”   This is somewhat contradictory,  because if the GCB speed is slowing down, based on his theory,  there would be more spots.

Dr. Nandi  adds some clarification when he lays out his theory here: “The fast-moving belt rapidly dragged sunspot corpses down to sun’s inner dynamo for amplification. At first glance, this might seem to boost sunspot production, but no. When the remains of old sunspots reached the dynamo, they rode the belt through the amplification zone too hastily for full re-animation.  Sunspot production was stunted.”  Nandi  then adds that late in the decade, “….according to the model, the Conveyor Belt slowed down again, allowing magnetic fields to spend more time in the amplification zone, but the damage was already done.  New sunspots were in short supply.  Adding insult to injury, the slow moving belt did little to assist re-animated sunspots on their journey back to the surface, delaying the onset of Solar Cycle 24.”  

Hathaway’s sunspot predictions are in Red.   Also on this chart, in Pink, are the Cycle 24 sunspot predictions by NCAR’s Mausumi Dikpata and her team based on their observations of the GCB.

Nandi  has made a presentation “Forecasting the Solar Cycle”at the Harvard Smithsonian Center for Astrophysics, Cambridge, USA  but I can not access the paper.

This theory says that the change of speed of the GCB predestines the solar çycle  robustness or lack there of.  For some insight of how they are able to track these plasma flows/GCBs/jet streams, click here.

Like the declining sunspot magnetic field, the theory of the GCB seem to me to be describing consequences of some other forcing that is not known or understood.  I think it likely that Cycle 25 will be weak.  However, until we know more about the functioning of the Sun,  we will be forecasting like the weather casters—tomorrow will be rainy because rain clouds are blowing our way from the west.  Like all of these theories, only time will tell if they are really capable of predicting accurately Cycle strength.

We are not through with Cycle prediction theories.  Next posting will discuss the bicentennial decrease in Total Solar Irradiance (TSI) unbalancing the Earth’s thermal budget.

cbdakota

Forecasting Cycle 25–Livingston and Penn Method


As Cycle 24 has not yet achieved a Solar Maximum, it may seem a little early to begin forecasting Cycle 25.  But several forecasts have been made.  A recent posting in WattsUpWithThat notes such forecasts by Penn and Livingston and by David Hathaway.

You remember from previous postings on this site, that Penn and Livingston have been measuring Sunspot magnetic field strength and the temperature and luminosity of the umbra.   They began this study in 1990 and as of 2010 they have analyzed some 17,000 spots. Plotted on the chart below are data from their paper LONG-TERM EVOLUTION OF SUNSPOT MAGNETIC FIELDS through 2010 and additional readings since:

Chart courtesy of Lief Svalgaard

Focusing on the bottom chart, sunspots are plotted against magnetic field strength and time. The individual dots are representative of sunspots.  The larger blue dot represents the normalized sunspot number for each year. The black line is the trend line for the umbral magnetic field of the sunspots. The horizontal blue line indexes a magnetic field strength of ca. 1500 Gauss. Note that the sunspots extend vertically above the trend line, and below the trend line but not below the 1500 Gauss line.  The two scientists speculate that sunspots do not form when the magnetic field strength is less than 1500 Gauss.  If the trend line continues on this same slope, somewhere around the year 2025+/- at least half of the sunspots will disappear.

Using a linear decrease of 65 Gauss per year and a cycle duration of 11 years, they computed the magnetic probability distribution function for Cycles 24 and 25. Using this, a sunspot number is forecast. Cycles 24 and 25 are shown along with actual data from Cycle 23 in the chart below from their paper:

Chart provided by David Archibald, from the paper by Livingston and Penn.

The contrast of Cycle 24 and specifically Cycle 25 from the completed Cycle 23 is quite dramatic.  The Cycle 24 forecast, so far, seems to be reasonably in tune with actual data.  At a Cycle 25 sunspot number of 7, David Archibald says it would be the lowest sunspot number for a Cycle in 300 years!!!!

Livingston and Penn say that if the linear decrease were 50 Gauss per year rather than 65, the Cycle 25 sunspot number would be 20 which is still a very low number.

Livingston and Penn caution that it is always risky to extrapolate linear trends.

Next posting on this topic will be an examination of David Hathaway’s 2006 forecast of both Cycle 24 and Cycle 25.  It will also discuss one of the underlying theories for the decrease in sunspots.

cbdakota

Solar Cycle 24—Less Active in December.


Cycle 24 became a little less active in December.   The charts for Sunspot numbers, F10.7 solar flux and Ap progression are shown below.

 

cbdakota

 

 

Are Sunspots Going to Disappear by 2015?


To reacquaint you with this topic, lets do a little review.  Livingston and Penn have been measuring the umbral intensity of sunspots and the corresponding magnetic field that spawns them since 1990.  In 2006 they submitted a paper to the journal “Science” reporting on their efforts and suggested that if the trend of weaker sunspot magnetic fields continued at its current rate, they would be too weak to produce sunspots.  This paper was rejected in peer review. Undeterred, they have continued to study these phenomena and so far, they seem to be on to something.

Sunspots are the product of the enormous magnetic fields created on the Sun. What make them especially interesting is that the Earth’s climate and sunspots have a high degree of correlation.   Periods where the climate has cooled off seem to coincide with periods of few sunspots and periods of warmer climate seem to coincide with periods of high sunspot counts.

Sunspots appear as dark spots on the face of the Sun.  Very strong magnetic forces (thousands of times stronger than Earths magnetic field) block the hot solar plasma and sunspots are the result.  The spots are cooler than the surrounding surface of the Sun.  NASA says that the spots are about 3700K versus 5700K for the surrounding photosphere.

©UCAR, image courtesy Matthias Rempel, NCAR

The photo sh0ws the “spot” (the umbra) surrounded by the penumbra that is shaped by the magnetic lines of force. 

Livingston and Penn have studied over 1700 spots and they see a trend in which the darkest parts of the sunspot umbra have become warmer (45K per year) and their magnetic field strengths have decreased (77 Gauss per year**), independently of the normal 11-year sunspot cycle.

The latest data is shown in the two charts, UMBRAL INTENSITY AND UMBRAL MAGNETIC FIELD.

Charts courtesy of Leif Svalgaard

The umbral intensity is a measurement of the light from the umbra (the dark center) and compared to a measurement of the light from a calm sun surface.  Note that the umbra is getting hotter and brighter as the umbral magnetic field gets weaker.  The two scientists believe that if the magnetic field weakens to ≈1500 gauss, the sunspots will not form.   If the trend continues linearly,  that could happen in this decade. 

If there are no visible sunspots in Cycle 25,  it could mean that we would be experiencing a solar minimum like the Maunder minimum that heralded in the Little Ice Age. It should be noted that while this is a suggestion, rather than a promise, it certainly is consistent with the observable trend of a less energetic Sun.

** Gauss is measure of the strength of a magnetic field.  Its units are Maxwells per square centimeter.  A small bar magnet will range from 40 to 100 gauss. The Sun’s average magnetic field strength is 1 and the Earth’s is 0.5.

cbdakota

 

 

 

 

Cycle 24 November 2011 Update


November Cycle 24 monthly sunspot count was nearly 100, which is by far the most active period since the cycle began.    The same goes for the F 10.7 Radio Flux that racked up a value of about 155.  But of these numbers are well below those of Cycle 23 at its peak.  Cycle 23 peak sunspot count was 170 and its F10.7 was about 235.   See the  November NOAA/SWPC charts below:

CLICK ON CHARTS FOR BETTER VIEW

Solar Activity/Geomagnetism

The Ap index is a good proxy for overall solar activity. For two months it has declined.  We are seeing Cycle 24 peaks in F10.7, and sunspots simultaneously with this drop in Ap.  It may mean that the spots and F10.7 may soon be trending downward as well.

If you  are interested,  the following is a brief explanation of the various ways geomagnetism is expressed.

The magnetic activity indices K, Kp and ap are designed to measure the variations in the geomagnetic field that arise from current systems caused by regular solar radiation changes. Other irregular current systems produce magnetic field changes caused by the interaction of the solar wind with the magnetosphere, by the magnetosphere itself, by the interactions between the magnetosphere and ionosphere, and by the ionosphere itself.

The planetary 3-hour range index Kp is the mean K-index from 13 geomagnetic observatories.  The scale is 0 to 9 expressed in thirds of a unit, 5-  is 4 2/3, 5 is 5 and 5+ is 5 1/3.  This planetary index is designed to measure particle radiation by its magnetic effects.  The 3-hourly ap (equivalent range) index is derive from the Kp index as follows:

Kp = 0o   0+   1-   1o   1+   2-   2o   2+   3-   3o   3+   4-   4o   4+

ap =  0     2     3      4     5     6     7       9    12   15    18     22   27   32

Kp = 5-    5o    5+   6-   6o    6+    7-     7o     7+     8-     8o     8+    9-     9o

ap = 39   48   56    67   80   94   111  132    154   179   207  236  300  400

Now one more derivation to get to the Ap index.   The  Ap index is defined as the earliest occurring maximum 24-hour value  obtained by computing an 8-point running average of successive 3-hour ap indices during a geomagnetic storm event.

cbdakota