Category Archives: Solar Activity

Solar Cycle 24 Update June 2012


The Sunspots and F10.7 flux are slightly lower in June than in the previous month.  April next year is still the expert’s rough timing for Cycle 24 maximum.   After the usual charts, a chart is added  showing how Solar Cycles 21, 22 and 23 compare with the current Cycle 24.    This is a good illustration of how much less active Cycle 24 is. This chart is from:     http://www.solen.info/solar/

(click on the charts for clarity)

These charts would have been posted earlier but a death within the family has occupied my time for the past several weeks.

cbdakota

Decoding Solar Flare Classifications


When a solar expert says that there are multiple M-Class solar flares being detected on the Sun, do you know what that means?   From today’s (5 July) posting on Solarham.net:

Solar Update / High Solar Activity:
Solar activity is currently at high levels with multiple M-Class solar flares being detected around mostly large Sunspot 1515 in the southern hemisphere. This region retains its Beta-Gamma-Delta magnetic configuration and may produce an X-Class solar flare within the next 24-48 hours. Sunspot 1513 located in the northern hemisphere did generate an M1.8 event on Wednesday and was associated with a possible Earth directed CME. An impact is expected by July 7 the earliest. Minor geomagnetic activity will be possible.” 

This Solarham.net solar update reports M-Class flares are being detected and that an X-Class flare maybe produced in the next 24 to 48 hours.    Are these conditions a threat to Earth?

Knowing the classifications for Solar Flares  may serve you well. The classifications can be found in this website: The HandyMan’s Guide to Solar/Geomagnetic Conditions by Paul Harden, NA5N

Solar Flare Classification  

Flare Class

Type of Flare

HF Radio Effects

Resulting Geomagnetic Storm

A

Very Small

None

None

B

Small

None

None

C

Moderate

* Low Absorptons

* Active to Minor

M

Large

* High absorption

* Minor to Major

X

Extreme

* Possible Blackout

* Major to Severe*

*Conditions cited if Earth is in the trajectory of the flare emissions

Flare class is further rated from 1-9, ex. M1, M2, M3…M9

The larger the number, the larger the flare within that class. An X7-X9 is considered a “Grand Daddy” flare. Only a few have occurred over the past 30 years and cause total disruptions to communications, huge auroras, power grid failures, etc. Radio and X-Ray emissions from a flare affect the Earth for the duration of the solar event, usually 30 minutes or less. The Earth is 8 light-minutes from the Sun.

Conflicting Sunspot Classifications

I believe the Sunspot classification shown in  The HandyMan’s Guide to Solar/Geomagnetic Conditions by Paul Harden, NA5N groups the consequences reasonably well.  However,  the Sunspots classifications used in the Solar Update follow the Mount Wilson classification system which can be seen here.  It has a more detailed grouping system, including a gamma designation not included in the HandyMan’s Guide.

cbdakota

  

 

Cycle 24 May Update


Not much new. Solar Cycle 24 is tracking the recent forecasts and should reach a Maximum in the Spring of 2013.  Below are the updated through May charts (click on charts to clarify):

cbdakota Continue reading

Do The Planets Control Our Climate?


The scientists that believe that the planets have a major influence on the Earth’s climate do not broadcast about aliens and UFOs from a house trailer outside of Elko, Nevada from midnight to six am.  But rather, they are legitimate and they have good arguments/research going for them.

Courtesy of: Jose Antonio Penas/Science Photo Library

They are persuaded that the Sun, not CO2, is the primary driver of the Earth’s climate.  History shows that solar cycles that have low activity are accompanied by cooling climate.   For example, several minimally active cycles in succession have yielded the Maunder Minimum and the Dalton Minimum.  The temperature drop during the Maunder Minimum was so large as to give that Minimum the name—-“little ice age”.   The earlier Minimums were characterized by the low sunspot count.  Now we can add to that the F10.7cm radio flux, the geomagnetic readings, and many other ways to characterize the level of solar activity.  Even as new satellites and other investigative science provide us with greater understanding of the Sun, it still is not clear as to why Solar Cycle 24 is so inactive.  While many observers claim they knew 24 was going to be minimally active, the record shows most forecast that 24 would be pretty robust and not be appreciably different from Cycle 23.  Just like the weatherman that forecast rain for Maryland tomorrow because it is raining in West Virginia today, the solar experts now “know” that Cycle 25 will be like Cycle 24.

Dr. Hathaway of NASA observes that the Sun’s plasma Great Conveyor Belt (GCB) moved very rapidly in 2008 and 2009 but was notably slower in 2000 and 2001.  “I believe this could explain the unusually deep solar minimum we’ve been experiencing,” says Dr. Hathaway. The high speed of the conveyor belt challenges existing models of the solar cycle and it has forced us back to the drawing board for new ideas.”

Well ok, but why did the GCB change speeds?  Could the planets be the forcing  for this and other changes?

Planets as forcing agents

What is the relationship of the planets and Earth’s climate? There is a theory based upon on the conservation of momentum that links every planet to the Sun.  Another theory is the planet induced tidal effect upon the Sun’s plasma surface. Undoubtedly there are more, but two are enough for now.

Refresher:   Some of my readers may need a refresher regarding the solar system planets.

Solar System Planetary Data (rounded)

Body Distance from Sun10^6km Mass10^22kg OrbitDays Orbit Circ.10^6 km OrbitSpeed 10^6km/day
Mercury 58 33 88 364 4.1
Venus 108 487 225 679 3
Earth 150 598 365 942 2.6
Mars 228 64 687 1432 2.1
Jupiter 778 190,000 4332 4887 1.1
Saturn 1429 56,900 10760 8977 0.8
Uranus 2871 8690 30700 18036 0.6
Neptune 4504 10280 60200 28294 0.5

The mass of the Sun is 1048 times that of Jupiter or 1.989X 10^30 .

 The Landschiedt Minimum

In 2003, Dr. Theodor Landscheidt published a paper  “New Little Ice Age Instead of Global Warming?”  In that paper he predicted that the Earth would start cooling with the coolest period about 2030 and that it would be equivalent of the Maunder Minimum (aka, “the Little Ice Age’).   Landscheidt used the Gleissberg cycle of 80 to 90-years to identify periods of cool climate on Earth. He said that within the Gleissberg cycle there is an 83-year cycle in the change of the rotary force driving the Sun’s oscillatory motion about the center of mass of the solar system.  His premise was that the collective angular momentum of the giant outer planets imposed a torque on the Sun that varies the speed of the Sun’s equatorial rotational velocity.  Some people are saying that this minimum should be called the Landscheidt Minimum. (Landscheidt died in 2004.) Landscheidt further predicted that another minimum would occur about 2200.

One might presume that the center of the Sun is the likely solar system center of mass.  Only on occasion is that true.  The center of the solar system’s mass is called the barycenter.  Watch this video to get an appreciation for the effect of the planets on the barycenter.  (no sound)

The following chart shows where the barycenter is relative to the Sun by year.

                      Figure 8:  Solar System Barycenter

Landscheidt said:

The solar dynamo theory developed by Babcock, the first still rudimentary theory of solar activity, starts from the premise that the dynamics of the magnetic sunspot cycle is driven by the sun’s rotation. Yet this theory only takes into account the sun’s spin momentum, related to its rotation on its axis, but not its orbital angular momentum linked to its very irregular oscillation about the centre of mass of the solar system (CM). Figure 8 shows this fundamental motion, described by Newton three centuries ago. It is regulated by the distribution of the masses of the giant planets Jupiter, Saturn, Uranus, and Neptune in space. The plot shows the relative ecliptic positions of the centre of mass (small circles) and the sun’s centre (cross) for the years 1945 to 1995 in a heliocentric coordinate system.

The large solid circle marks the sun’s surface. Most of the time, the CM is to be found outside of the sun’s body. Wide oscillations with distances up to 2.2 solar radii between the two centres are followed by narrow orbits which may result in close encounters of the centres as in 1951 and 1990. The contribution of the sun’s orbital angular momentum to its total angular momentum is not negligible. It can reach 25 percent of the spin momentum. The orbital angular momentum varies from -0.1�1047 to 4.3� 1047 g cm2 s-1, or reversely, which is more than a forty-fold increase or decrease (Landscheidt, 1988). Thus it is conceivable that these variations are related to varying phenomena in the sun’s activity, especially if it is considered that the sun’s angular momentum plays an important role in the dynamo theory of the sun’s magnetic activity.

Variations of more than 7% in the sun’s equatorial rotational velocity, going along with variations in solar activity, were observed at irregular intervals (Landscheidt, 1976, 1984). This could be explained if there were transfer of angular momentum from the sun’s orbit to the spin on its axis. I have been proposing such spin-orbit coupling for decades (Landscheidt, 1984, 1986). Part of the coupling could result from the sun’s motion through its own magnetic fields. As Dicke (1964) has shown, the low corona can act as a brake on the sun’s surface. The giant planets, which regulate the sun’s motion about the CM, carry more than 99 percent of the angular momentum in the solar system, whereas the sun is confined to less than 1 percent. So there is a high potential of angular momentum that can be transferred from the outer planets to the revolving sun and eventually to the spinning sun.

From wiki, a somewhat analogous to the Planets/Sun interaction: The conservation of angular momentum in Earth–Moon system results in the transfer of angular momentum from Earth to Moon (due to tidal torque the Moon exerts on the Earth). This in turn results in the slowing down of the rotation rate of Earth (at about 42 nsec/day[citation needed]), and in gradual increase of the radius of Moon’s orbit (at ~4.5 cm/year rate[citation needed]).

If you want to dig further into the concept of angular momentum, the following may be of interest to you:

Angular momentum is conserved in a system where there is no net external torque, and its conservation helps explain many diverse phenomena. For example, the increase in rotational speed of a spinning figure skater as the skater’s arms are contracted is a consequence of conservation of angular momentum.  Moreover, angular momentum conservation has numerous applications in physics and engineering (e.g. the gyrocompass).  See here, here and here to get the math behind conservation of angular momentum, angular momentum, and torque.

 Tidal Effect

Dr Nicola Scafetta of the Active Cavity Radiometer Solar Irradiance Monitor Lab (ACRIM) and Duke University has recently published in the Journal of Atmospheric and Solar-Terrestrial Physics  “Does the Sun Work as a nuclear fusion amplifier of planetary tidal forces?  Etc.”

Lets look at a summary of some of the planetary interactions with the Sun that affect the nominal 11 year solar cycle that he listed in his abstract to the article:

Numerous empirical evidences suggest that planetary tides may influence solar activity. In particular, it has been shown that: (1) the well-known 11-year Schwabe sunspot number cycle is constrained between the spring tidal period of Jupiter and Saturn, 􏰁 9:93 year, and the tidal orbital period of Jupiter, 􏰁 11:86 year, and a model based on these cycles can reconstruct solar dynamics at multiple time scales (Scafetta, in press); (2) a measure of the alignment of Venus, Earth and Jupiter reveals quasi 11.07-year cycles that are well correlated to the 11-year Schwabe solar cycles; and (3) there exists a 11.08 year cyclical recurrence in the solar jerk-shock vector, which is induced mostly by Mercury and Venus

Scafetta proposes that the planets cause surface tides on the Sun.  While very small, he believes the tidal gravitational potential energy dissipated in the Sun by the tides, may produce irradiance output oscillations with a sufficient magnitude to influence the solar dynamo processes.   More from the abstract:

Here we explain how a first order magnification factor can be roughly calculated using an adaptation of the well-known mass-luminosity relation for main-sequence stars similar to the Sun. This strategy yields a conversion factor between the solar luminosity and the potential gravitational power associated to the mass lost by nuclear fusion: the average estimated amplification factor is A􏰂4:25×10^6. We use this magnification factor to evaluate the theoretical luminosity oscillations that planetary tides may potentially stimulate inside the solar core by making its nuclear fusion rate oscillate. By converting the power related to this energy into solar irradiance units at 1 AU we find that the tidal oscillations may be able to theoretically induce an oscillating luminosity increase from 0.05–0.65 W/m^2 to 0.25–1.63 W/m^2, which is a range compatible with the ACRIM satellite observed total solar irradiance fluctuations. In conclusion, the Sun, by means of its nuclear active core, may be working as a great amplifier of the small planetary tidal energy dissipated in it. The amplified signal should be sufficiently energetic to synchronize solar dynamics with the planetary frequencies and activate internal resonance mechanisms, which then generate and interfere with the solar dynamo cycle to shape solar dynamics, as further explained in Scafetta (in press). A section is devoted to explain how the traditional objections to the planetary theory of solar variation can be rebutted.

Both theories have many critics.  I am not knowledgeable enough to support or deny these theories.   However,  Dr Hathaway’s comment about varying speeds in the Great Conveyor Belt would lend some support to these theories especially Landscheidts.   Anyway, the Sun is where the action is with respect to global climate change.  And it will probably be a number of years before any theory wins out.  Remember how much bad press the cosmic ray theory got from the experts, and this case I mean the warmers.  Now after some work at CERN, it is looking like a winner, just not yet announced.  There is hope.

cbdakota

Solar Cycle 24–April Update


Generally speaking, Solar Cycle 24’s April sunspots numbers, F10.7cm flux and the geomagnetic field Ap index all indicate reduced solar actively.  NASA as well most of the experts in this field agree that Solar Cycle 24 will be a record setter of a sort—least active in about 100 years.  One need not base this on computer models or some consensus, however.  All that is required is to look at the data.  I do not think anyone has a handle on why Cycle 24 is acting this way.  There are many theories and perhaps one of them is correct. Will Cycle 25 continue this downward trend?  Click on the charts to improve clarity.

cbdakota

Revised NASA Cycle 24 Sunspot Forecast


Dr Hathaway of NASA has revised his Cycle 24 sunspot forecast.   He predicts a smoothed sunspot number maximum of about 60 in the Spring of next year.  Cycle 24 will be the smallest in about 100 years.  For the record, his forecast graphed is shown below:

He has revised his prediction method as follows:

Recent work [see Hathaway Solar Physics; 273, 221 (2011)] indicates that the equatorward drift of the sunspot latitudes as seen in the Butterfly Diagram follows a standard path for all cycles provided the dates are taken relative to a starting time determined by fitting the full cycle. Using data for the current sunspot cycle indicates a starting date of May of 2008. Fixing this date and then finding the cycle amplitude that best fits the sunspot number data yields the current (revised) prediction.

To read more of the NASA report click here.

A reminder, Hathaway uses the smoothed International Sunspot Numbers and not the NOAA count. The International Sunspot Number for historical reasons [to be compatible with Rudolf Wolf’s count for 1849 to 1865] is reported as 0.6 x the actual count, while the NOAA count is just the raw count [actually = 10 x number of groups + number of spots].

This has not been an easy road for Cycle 24 sunspot predictions.  See the links below to get an idea how far Cycle 24 has been cut back over recent times.

https://cbdakota.wordpress.com/2012/03/06/cycle-24-february-update/

https://cbdakota.wordpress.com/2011/10/11/september-solar-cycle-24-activity-increased/

https://cbdakota.wordpress.com/2011/09/20/solar-cycle-24-august-update/

https://cbdakota.wordpress.com/2011/08/16/solar-cycle-24-continues-to-under-perform-the-early-projections/

The April Sunspot report will be out early next week and will be posted for your examination.

cbdakota

Japanese Researchers Suggest Cycle 24 Could Be The Start Of A New Maunder Minimum


The Asahi Shimbun* reports that “Officials of the National Astronomical Observatory of Japan and the Riken research foundation said on April 19 that the activity of sunspots appeared to resemble a 70-year period in the 17th century in which London’s Thames froze over and cherry blossoms bloomed later than usual in Kyoto. The sun may be entering a period of reduced activity that could result in lower temperatures on Earth, according to Japanese researchers. “ They are suggesting that solar Cycle 24 is the beginning of an era similar to the Maunder Minimum.

A solar cycle usually lasts about 11 years.  During the cycle, the poles switch polarity at about the time of the solar maximum.   Many scientists are predicting that Cycle 24’s maximum will occur about May of 2013. However, the Japanese researchers found signs of unusual magnetic changes in the sun. They report that the solar observation satellite Hinode found that the north pole of the Sun has already begun to flip—about a year earlier than expected.  They found no noticeable change in the South Pole.

The researchers add: “If that trend continues, the north pole could complete its flip in May 2012 but create a four-pole magnetic structure in the sun, with two new poles created in the vicinity of the equator of our closest star. “

Below is the National Astronomical Observatory of Japan’s representation of the Sun’s poles in May 2012:

 *The Asahi Shimbun has the second highest circulation of Japan’s national newspapers 

cbdakota

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