Category Archives: Solar Flux

SOLAR CYCLE 24 APRIL UPDATE// RUSSIAN TEAM SAYS COOLING MAY LAST FOR MORE THAN 200 YEARS.


There was an uptick in Sunspot numbers and F10.7cm radio flux.   Sunspots monthly average went up to 72  versus  55 in March.   Cycle 24’s  pattern seems somewhat reminiscent of Cycle 23 during its time at or near maximum. (Click on charts to enlarge.)
cycles23_24APRIL13Chart curtsey of Solen.com
Sunspots appear to be in sync with the predicted path shown as the green line in the chart.

Solar Cycle 24 March Update


There was a small upward spike in Sunspot numbers in March.   Dean Pesnell of NASA’s Goddard Space Flight Center thinks this will make Cycle 24 a double peak “maximum” event.  He says that the second peak may even last into 2014.
(Click on the Charts for more Clarity)
March13sunspots

Solar Cycle 24 Activity Compared To Previous Solar Cycles


Solar Cycle 24 activity dropped off in February.  Charts for sunspots and F10.7 cm radio flux follow:
sunspotmarch13

Solar Cycle 24 Update-January 2013


Solar Cycle 24 experienced a small uptick in the number of Sunspots and F 10.7cm solar flux in the month of January.  First the Sunspot chart:
solarcycle24sunspot4feb13
And the F 10.7cm solar flux chart:
solarcycle24f10.7cm4feb13

NASA Revises Cycle 24 Sunspot Prediction.


David Hathaway, NASA solar cycle expert, has a revised forecast for Solar Cycle 24 Sunspot number and Maximum timing.  In May 2012, he forecast the smoothed sunspot number maximum at 60 and the timing of the maximum as the spring of 2013.  His January 2013 Cycle 24  revised forecast is for 69 spots and maximum in the Fall of 2013.  He adds:
“ We are currently over four years into Cycle 24. The current predicted and observed size makes this the smallest sunspot cycle since Cycle 14 which had a maximum of 64.2 in February of 1906.”  
 jan13hathawayssn_predict
       Hathaway’s  NASA Revised January 2013 Sunspot Number Prediction

Solar Cycle 24 Nearing Maximum


Solar Cycle 24 is nearing its maximum after which the solar activity will decline.     The maximum is often pegged as the time when the Sun’s  north and south poles swap. The chart below shows the current position of the poles. Projecting their current position suggests that the swap will occur early next year.
(Click on Charts to improve clarity)
december12Solar-Polar-Fields-1966-now
    Solar Polar Field 1966 to Present –Wilcox Solar Observatory

Solar Cycle 24 Update July 2012


Solar Cycle24 July sunspot and F 10.7cm radio flux numbers are up slightly from June.  Pretty much in line with the activity projection and much below that of Solar Cycle 23. (Click on Graphs for Clarity)

Large Filament on the Sun

The Sun currently has a filament that stretches more that 400,000km across the face. Filaments are formed in magnetic loops that hold relatively cool, dense gas suspended above the surface of the Sun. Because they are cooler than the photosphere they can look dark.

courtesy of solarham.net

But when viewed in profile they look like a giant loop, called a prominence.

courtesy of NASA

Occasionally when these filaments collapse,  a coronal mass ejection (CME) can occur.   Because the filament is looking directly at the Earth,  a CME could cause problems.   Lets hope this does not happen.

cbdakota

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

  

 

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