Indirect Solar Forcing of Climate by Galactic Cosmic Rays: An Observational Estimate

By Dr. Roy Spencer, PhD (reprinted from his blog with permission)

UPDATE (12:35 p.m. CDT 19 May 2011): revised corrections of CERES data for El Nino/La Nina effects.

While I have been skeptical of Svensmark’s cosmic ray theory up until now, it looks like the evidence is becoming too strong for me to ignore. The following results will surely be controversial, and the reader should remember that what follows is not peer reviewed, and is only a preliminary estimate.

I’ve made calculations based upon satellite observations of how the global radiative energy balance has varied over the last 10 years (between Solar Max and Solar Min) as a result of variations in cosmic ray activity. The results suggest that the total (direct + indirect) solar forcing is at least 3.5 times stronger than that due to changing solar irradiance alone.

If this is anywhere close to being correct, it supports the claim that the sun has a much larger potential role (and therefore humans a smaller role) in climate change than what the “scientific consensus” states.

BACKGROUND

The single most frequently asked question I get after I give my talks is, “Why didn’t you mention the sun?” I usually answer that I’m skeptical of the “cosmic ray gun” theory of cloud changes controlling climate. But I point out that Svensmark’s theory of natural cloud variations causing climate change is actually pretty close to what I preach — only the mechanism causing the cloud change is different.

Then, I found last year’s paper by Laken et al. which was especially interesting since it showed satellite-observed cloud changes following changes in cosmic ray activity. Even though the ISCCP satellite data they used are not exactly state of the art, the study was limited to the mid-latitudes, and the time scales involved were days rather than years, the results gave compelling quantitative evidence of a cosmic ray effect on cloud cover.

With the rapid-fire stream of publications and reports now coming out on the subject, I decided to go back and spend some time analyzing ground-based galactic cosmic ray (GCR) data to see whether there is a connection between GCR variations and variations in the global radiative energy balance between absorbed sunlight and emitted infrared energy, taken from the NASA CERES radiative budget instruments on the Terra satellite, available since March 2000.

After all, that is ultimately what we are interested in: How do various forcings affect the radiative energy budget of the Earth? The results, I must admit, are enough for me to now place at least one foot solidly in the cosmic ray theory camp.

THE DATA

The nice thing about using CERES Earth radiative budget data is that we can get a quantitative estimate in Watts per sq. meter for the radiative forcing due to cosmic ray changes. This is the language the climate modelers speak, since these radiative forcings (externally imposed global energy imbalances) can be used to help calculate global temperature changes in the ocean & atmosphere based upon simple energy conservation. They can then also be compared to the estimates of forcing from increasing carbon dioxide, currently the most fashionable cause of climate change.

From the global radiative budget measurements we also get to see if there is a change in high clouds (inferred from the outgoing infrared measurements) as well as low clouds (inferred from reflected shortwave [visible sunlight] measurements) associated with cosmic ray activity.

I will use only the ground-based cosmic ray data from Moscow, since it is the first station I found which includes a complete monthly archive for the same period we have global radiative energy budget data from CERES (March 2000 through June 2010). I’m sure there are other stations, too…all of this is preliminary anyway. Me sifting through the myriad solar-terrestrial datasets is just as confusing to me as most of you sifting through the various climate datasets that I’m reasonably comfortable with.

THE RESULTS

The following plot (black curve) shows the monthly GCR data from Moscow for this period, as well as a detrended version with 1-2-1 averaging (red curve) to match the smoothing I will use in the CERES measurements to reduce noise.

Detrending the data isolates the month-to-month and year-to-year variability as the signal to match, since trends (or a lack of trends) in the global radiative budget data can be caused by a combination of many things. (Linear trends are worthless for statistically inferring cause-and-effect; but getting a match between wiggles in two datasets is much less likely to be due to random chance.)

The monthly cosmic ray data at Moscow will be compared to global monthly anomalies the NASA Terra satellite CERES (SSF 2.5 dataset) radiative flux data,

which shows the variations in global average reflected sunlight (SW), emitted infrared (LW), and Net (which is the estimated imbalances in total absorbed energy by the climate system, after adjustment for variations in total solar irradiance, TSI). Note I have plotted the variations in the negative of Net, which is approximately equal to variations in (LW+SW)

Then, since the primary source of variability in the CERES data is associated with El Nino and La Nina (ENSO) activity, I subtracted out an estimate of the average ENSO influence using running regressions between running 5-month averages of the Multivariate ENSO Index (MEI) and the CERES fluxes. I used the MEI index along with those regression coefficients in each month to correct the CERES fluxes 4 months later, since that time lag had the strongest correlation.

Finally, I performed regressions at various leads and lags between the GCR time series and the LW, SW, and -Net radiative flux time series, the results of which are shown next.

The yearly average relationships noted in the previous plot come from this relationship in the reflected solar (SW) data,

while the -Net flux (Net is absorbed solar minus emitted infrared, corrected for the change in solar irradiance during the period) results look like this:

It is that last plot that gives us the final estimate of how a change in cosmic ray flux at Moscow is related to changes in Earth’s radiative energy balance.

SUMMARY

What the above three plots show is that for a 1,000 count increase in GCR activity as measured at Moscow (which is somewhat less than the increase between Solar Max and Solar Min), there appears to be:

(1) an increase in reflected sunlight (SW) of 0.64 Watts per sq. meter, probably mostly due to an increase in low cloud cover;

(2) virtually no change in emitted infrared (LW) of +0.02 Watts per sq. meter;

(3) a Net (reflected sunlight plus emitted infrared) effect of 0.55 Watts per sq. meter loss in radiant energy by the global climate system.

WHAT DOES THIS MEAN FOR CLIMATE CHANGE?

Assuming these signatures are anywhere close to being real, what do they mean quantitatively in terms of the potential effect of cosmic ray activity on climate?

Well, just like any other forcing, a resulting temperature change depends not only upon the size of the forcing, but also the sensitivity of the climate system to forcing. But we CAN compare the cosmic ray forcing to OTHER “known” forcings, which could have a huge influence on our understanding of the role of humans in climate change.

For example, if warming observed in the last century is (say) 50% natural and 50% anthropogenic, then this implies the climate system is only one-half as sensitive to our greenhouse gas emissions (or aerosol pollution) than if the warming was 100% anthropogenic in origin (which is pretty close to what we are told the supposed “scientific consensus” is).

First, let’s compare the cosmic ray forcing to the change in total solar irradiance (TSI) during 2000-2010. The orange curve in following plot is the change in direct solar (TSI) forcing between 2000 and 2010, which with the help of Danny Braswell’s analytical skills I backed out from the CERES Net, LW, and SW data. It is the only kind of solar forcing the IPCC (apparently) believes exists, and it is quite weak:

Also shown is the estimated cosmic ray forcing resulting from the month-to-month changes in the original Moscow cosmic ray time series, computed by multiplying those monthly changes by 0.55 Watts per sq. meter per 1,000 cosmic ray counts change.

Finally, I fitted the trend lines to get an estimate of the relative magnitudes of these two sources of forcing: the cosmic ray (indirect) forcing is about 2.8 times that of the solar irradiance (direct) forcing. This means the total (direct + indirect) solar forcing on climate associated with the solar cycle could be 3.8 times that most mainstream climate scientists believe.

One obvious question this begs is whether the lack of recent warming, since about 2004 for the 0-700 meter layer of the ocean, is due to the cosmic ray effect on cloud cover canceling out the warming from increasing carbon dioxide.

If the situation really was that simple (which I doubt it is), this would mean that with Solar Max rapidly approaching, warming should resume in the coming months. Of course, other natural cycles could be in play (my favorite is the Pacific Decadal oscillation), so predicting what will happen next is (in my view) more of an exercise in faith than in science.

In the bigger picture, this is just one more piece of evidence that the IPCC scientists should be investigating, one which suggests a much larger role for Mother Nature in climate change than the IPCC has been willing to admit. And, again I emphasize, the greater the role of Nature in causing past climate change, the smaller the role humans must have had, which could then have a profound impact on future projections of human-caused global warming.

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Paul Vaughan
May 22, 2011 12:17 pm

vukcevic, on interannual timescales your “hysteresis” is what Milanovic calls “spatiotemporal chaos”, but I don’t see you acknowledging the dominant lagless role of external factors on ocean currents via wind.

May 22, 2011 12:18 pm

tallbloke says:
May 22, 2011 at 11:50 am
So does this mean you can also reconstruct Earthward solar wind speed and density back to 1835
In essence, yes. The details depend on finding and digitizing the early 19th century data [this is ongoing].
and by subtracting out the activity due to sunspots, get a residual which shows us what was emanating from coronal holes and flares?
Flares are generally part of ‘activity due to sunspots’, but we can separate what is due to solar UV and what is due to solar wind [coronal holes]. This is an active area of research. The main hurdle [the “I’m not convinced’ syndrome] is past us now and we can begin to make progress. A workshop is scheduled for next year about this. One of the remaining issues is what happened prior to the 19th century as far as the floor in B is concerned. The recent solar minimum B-value of 3.93 nT nicely fits our floor value of ~4 nT. Steinhilber’s suggestion that HMF B was substantially lower around 1900 is not substantiated by the geomagnetic data.

tallbloke
May 22, 2011 12:32 pm

Paul Vaughan says:
May 22, 2011 at 12:17 pm
vukcevic, …

I would think you’ll both be pretty interested by this article, fresh out a couple of days ago.
http://www.nature.com/nature/journal/vaop/ncurrent/full/nature10013.html
Interannual atmospheric variability forced by the deep equatorial Atlantic Ocean
Peter Brandt, Andreas Funk, Verena Hormann, Marcus Dengler, Richard J. Greatbatch & John M. Toole
Climate variability in the tropical Atlantic Ocean is determined by large-scale ocean–atmosphere interactions, which particularly affect deep atmospheric convection over the ocean and surrounding continents1. Apart from influences from the Pacific El Niño/Southern Oscillation2 and the North Atlantic Oscillation3, the tropical Atlantic variability is thought to be dominated by two distinct ocean–atmosphere coupled modes of variability that are characterized by meridional4, 5 and zonal6, 7 sea-surface-temperature gradients and are mainly active on decadal and interannual timescales, respectively8, 9. Here we report evidence that the intrinsic ocean dynamics of the deep equatorial Atlantic can also affect sea surface temperature, wind and rainfall in the tropical Atlantic region and constitutes a 4.5-yr climate cycle. Specifically, vertically alternating deep zonal jets of short vertical wavelength with a period of about 4.5 yr and amplitudes of more than 10 cm s−1 are observed, in the deep Atlantic, to propagate their energy upwards, towards the surface10, 11. They are linked, at the sea surface, to equatorial zonal current anomalies and eastern Atlantic temperature anomalies that have amplitudes of about 6 cm s−1 and 0.4 °C, respectively, and are associated with distinct wind and rainfall patterns. Although deep jets are also observed in the Pacific12 and Indian13 oceans, only the Atlantic deep jets seem to oscillate on interannual timescales. Our knowledge of the persistence and regularity of these jets is limited by the availability of high-quality data. Despite this caveat, the oscillatory behaviour can still be used to improve predictions of sea surface temperature in the tropical Atlantic. Deep-jet generation and upward energy transmission through the Equatorial Undercurrent warrant further theoretical study.

May 22, 2011 12:38 pm

Leif Svalgaard says: May 22, 2011 at 12:04 pm
Declined because it did not satisfy even elementary demands on quality.
That is nonsense.
You only saw the graph, no data file, no source of data, and even more importantly what the data represents.
Only a ‘pompous academic’ could glance at graph and say:
“ did not satisfy even elementary demands on quality”
Well have another look
http://www.vukcevic.talktalk.net/CD2.htm
and specify which elementary QUALITY you are talking about, you often make demands of other posters, so follow your own form.
North Atlantic precursor has no dimension (it is just a number = ratio of two values expressed in same units) and normalised to scale of other relevant variables.

May 22, 2011 12:42 pm

Paul Vaughan says:
May 22, 2011 at 11:59 am
Useful: “the modulation is not just a simple relationship and is not well understood […]”
But that doesn’t mean it is not understood at all. Just that it is not understood as well as we would like. We do understand that [and how] the modulation is controlled by the latitudinal extent of the coronal streamer belt, that [and how] the modulation is influenced by the cosmic rays drifting in the large scale structure of the HMF, that [and how] the modulation arises from scattering from turbulent corotating interaction regions, and several other details [e.g. the dependence on particle energy]. A comprehensive, quantitative theory is still elusive, although some people claim their pet theories fit the bill.

tallbloke
May 22, 2011 1:00 pm

Leif Svalgaard says:
May 22, 2011 at 12:18 pm
The details depend on finding and digitizing the early 19th century data [this is ongoing]…
One of the remaining issues is what happened prior to the 19th century as far as the floor in B is concerned.

What are the earliest usefully calibrate-able reading you are aware of? Is there still a massive amount of paper records in danger of being lost?

Paul Vaughan
May 22, 2011 1:08 pm

Useful:
Leif Svalgaard wrote (May 22, 2011 at 10:28 am)
“The modulation of GCR is caused by GCRs scattered by the irregularities in the field, which scale with the field […] the modulation is not just a simple relationship and is not well understood […]”


To clarify: The most useful part is this part:
Leif Svalgaard wrote (May 22, 2011 at 10:28 am)
“The modulation of GCR is caused by GCRs scattered by the irregularities in the field, which scale with the field […]”

May 22, 2011 1:09 pm

vukcevic says:
May 22, 2011 at 12:38 pm
You only saw the graph, no data file, no source of data, and even more importantly what the data represents.
Undocumented stuff automatically goes in the circular bin.
But as I recall, you were plotting things upside down for periods when the phase was wrong to make it fit anyway. You could submit what you have on your own anywhere and at any time.
tallbloke says:
May 22, 2011 at 1:00 pm
What are the earliest usefully calibrate-able reading you are aware of? Is there still a massive amount of paper records in danger of being lost?
Gauss’s data from ~1833 for IDV and IHV. For the UV, the 1740s. And yes, there is a massive amount of data in danger of being lost. We are attempting to halt that loss, but it is harder than one might think it should be.

Paul Vaughan
May 22, 2011 1:22 pm

Stephen Wilde wrote (May 20, 2011 at 11:46 pm):
“My main problem with the Svensmark hypothesis is that there is no shortage of the necessary aerosols in the first place so more of them does not necessarily result in more clouds.”

Kirkby points out that aerosol concentration affects droplet size in a manner that fundamentally alters reflection.

I’ve been hoping someone might be able to point to the article from which he got the right-hand graph-panel displayed from 35:40 to 35:50:
Anyone?
This immediately struck me as a key missing link (regardless of whether GCRs, something confounded, or whatever).

tallbloke
May 22, 2011 1:37 pm

Paul,
if you mean the CCN origination slide, the legend below the graphs reads
Merikanto et al, ACP, 2009

tallbloke
May 22, 2011 1:41 pm

Leif Svalgaard says:
May 22, 2011 at 1:09 pm
yes, there is a massive amount of data in danger of being lost. We are attempting to halt that loss, but it is harder than one might think it should be.

I suppose some of the data has shifted around over the years, from closed down measuring stations, to libraries, to university faculty offices etc. Must be hard to track down. Sounds like it needs someone with some travel funding to do some dedicated running around.

John Finn
May 22, 2011 1:50 pm

tallbloke says:
May 22, 2011 at 5:17 am

John Finn says:
May 22, 2011 at 2:27 am
SC 5 didn’t begin until ~1798.


Yet you asserted that the Dalton Minimum started in 1790, at the peak of a high cycle?
And as I pointed out it does not help your argument. On the contrary, it considerably weakens it. Could you now identify when the Dalton Minimum cooling began? If indeed there was such a thing.

May 22, 2011 2:10 pm

vukcevic says:
May 22, 2011 at 12:38 pm
and specify which elementary QUALITY you are talking about, you often make demands of other posters, so follow your own form.
For one, an 11-yr moving average should end 5.5 years from the limits of the data.

Julian Droms
May 22, 2011 2:16 pm

> Leif Svalgaard says:
> May 21, 2011 at 9:00 pm
>> Julian Droms says:
>> May 21, 2011 at 8:14 pm
>> Shaviv says it should be only these high energy > 10 GeV particles
>> that have the energy to penetrate into the lower atmosphere while
>> still being able to seed clouds at those altitudes At such high
>> energies, the solar modulation of GCRs is actually very small. Look
>> at the lower right-hand curves on Figure 1 of
>> http://www.srl.caltech.edu/ACE/ASC/DATA/bibliography/ICRC2005
>> /usa-wiedenbeck-M-abs3-sh34-poster.pdf
It looks to me like this paper looks at particles only from Li through Zn, and it has no actual data points above 1 GeV, much less 10 GeV (from the Advanced Composition Explorer) comparing different modulations, just extrapolations from lower energies. Also, I’m not sure how measurements on particle energies in orbit should correlate with energies in ground measurements, or whether that matters. It appears to be a poster and not a peer-reviewed article, which shouldn’t matter, if there were someone to explain in details how it relates to the current debate…

tallbloke
May 22, 2011 2:18 pm

John Finn says:
May 22, 2011 at 1:50 pm
tallbloke says:
May 22, 2011 at 5:17 am
John Finn says:
May 22, 2011 at 2:27 am
SC 5 didn’t begin until ~1798.
Yet you asserted that the Dalton Minimum started in 1790, at the peak of a high cycle?
And as I pointed out it does not help your argument. On the contrary, it considerably weakens it. Could you now identify when the Dalton Minimum cooling began? If indeed there was such a thing.

Yes, you immediately tried to shift attention away from your falsehood, and I obligingly said some colder winters were recorded after 1804. But this doesn’t change the fact that you won’t/can’t admit to falsely stating that the Dalton Minimum commenced in 1790. Perhaps at this second prompting, you will agree you are wrong about that?

May 22, 2011 2:36 pm

Leif Svalgaard says: May 22, 2011 at 1:09 pm
But as I recall, you were plotting things upside down for periods when the phase was wrong to make it fit anyway.
Another nonsense from your ‘make it up’ milling machine.
1.First nothing was plotted upside down.
2.North Atlantic precursor as:
http://www.vukcevic.talktalk.net/CD2.htm
is nothing to do with Leohle reconstruction as:
http://www.vukcevic.talktalk.net/LL.htm
with negative correlation for a fraction of time, which is just an (useful) exercise in pointing towards link of global temperature to the arctic magnetic field which may or may not have some role in climatic events.
3. I was not to disclose details directly to you (well known as a person who ridicules anything that may knot know much about or have no experience of) but was more than happy to give complete documentation to a conscientious climate scientist who would take an unbiased view.
Your above comment emphasise precisely why it is not advisable for anyone to take your opinion as a defining evaluation of a new and possibly controversial finding.
You could submit what you have on your own anywhere and at any time.
That I shall do; but what a chance for a ‘lamb’ in a den full of jackals.

May 22, 2011 2:52 pm

Julian Droms says:
May 22, 2011 at 2:16 pm
Also, I’m not sure how measurements on particle energies in orbit should correlate with energies in ground measurements, or whether that matters. It appears to be a poster and not a peer-reviewed article,
The paper was not intended to show any new result. It was just an example showing what has been known for decades for all sorts of particles. The energy outside the Earth determines if the cosmic ray even get to the ground.

May 22, 2011 3:02 pm

vukcevic says:
May 22, 2011 at 2:36 pm
with negative correlation for a fraction of time, which is just an (useful) exercise in pointing towards link of global temperature to the arctic magnetic field which may or may not have some role in climatic events […]
Perhaps part of your problem is not being upfront with what you claim. The drips that you occasionally let fly do not tell a coherent story. Based on the low quality of those, the chance that the secret paper is any better is slim.

May 22, 2011 3:16 pm

Leif Svalgaard says: May 22, 2011 at 2:10 pm
For one, an 11-yr moving average should end 5.5 years from the limits of the data.
Nothing wrong with my graph
http://www.vukcevic.talktalk.net/CD2.htm
In this case it is shown as a cumulative process along 11 years
Y (n+11) = { Sum [(X(n) +X(n+1) +…. X(n+11)] }/11
rather than
Y (n+6) = { Sum [(X(n) +X(n+1) +…. X(n+11)] }/11

May 22, 2011 3:18 pm

vukcevic says:
May 22, 2011 at 2:36 pm
more than happy to give complete documentation to a conscientious climate scientist who would take an unbiased view.
A good vehicle for this would have been to present it here on WUWT for a free review by all the unbiased people with completely open and receptive minds

May 22, 2011 3:26 pm

vukcevic says:
May 22, 2011 at 3:16 pm
Nothing wrong with my graph
an 11-yr moving average should end 5.5 years from the limits of the data.

Paul Vaughan
May 22, 2011 4:09 pm

tallbloke wrote (May 22, 2011 at 1:37 pm)
“[…] the legend below the graphs reads Merikanto et al, ACP, 2009”

Yes, thanks tallbloke. Looks like Figure 9B (with a slightly different color scale) from:
Merikanto, J.; Spracklen, D.V.; Mann, G.W.; Pickering, S.J.; & Carslaw, K.S. (2009). Impact of nucleation on global CCN. Atmospheric Chemistry and Physics 9, 8601-8616.
http://www.atmos-chem-phys.org/9/8601/2009/acp-9-8601-2009.pdf
Also resembles Figure 8B.

Paul Vaughan
May 22, 2011 4:23 pm

Leif Svalgaard hing vukcevic (May 22, 2011 at 3:02 pm):
“Perhaps part of your problem is not being upfront with what you claim.”

Leif’s predictable misinterpretation of 2 curves on any 1 graph:
“Claim”

savethesharks
May 22, 2011 8:09 pm

Leif Svalgaard says:
There are three strikes against the cosmic ray theory [which, BTW, did not originate with Svensmark].
1) the sun’s magnetic field that controls the amount of cosmic rays arriving at Earth is the same now as 150 years ago. Climate is not.
2) the amount of nucleation derived from GCRs is two orders of magnitude too small to have any affect. http://adsabs.harvard.edu/abs/2009GeoRL..3609820P
3) the cosmic ray intensity has varied the past several years much more than the solar modulation and the climate has not varied with it, e.g. http://www.leif.org/research/CosmicRays-GeoDipole.jpg
====================
Is this the best that you can do?
Chris
Norfolk, VA, USA

Julian Droms
May 22, 2011 8:36 pm

Julian Droms says:
>>>> Shaviv says it should be only these high energy > 10 GeV particles
>>>> that have the energy to penetrate into the lower atmosphere while
>>>> still being able to seed clouds at those altitudes
Leif Svalgaard says:
>>> At such high energies, the solar modulation of GCRs is actually very
>>> small. Look at the lower right-hand curves on Figure 1 of
>>> http://www.srl.caltech.edu/ACE/ASC/DATA/bibliography/ICRC2005
>>> /usa-wiedenbeck-M-abs3-sh34-poster.pdf
Julian Droms says:
>> It looks to me like this paper looks at particles only from Li through Zn,
>> and it has no actual data points above 1 GeV, much less 10 GeV (from the
>> Advanced Composition Explorer) comparing different modulations, just
>> extrapolations from lower energies.
Leif Svalgaard says:
> The paper was not intended to show any new result. It was just an
> example showing what has been known for decades for all sorts of
> particles. The energy outside the Earth determines if the cosmic ray
> even get to the ground.
Still, it looks to me like this poster looks at particles only from Li through Zn. If you read Wikipedia, it says that only about 1 % of cosmic rays are comprised of heavier elements, Li and above. About 99% are protons and helium nuclei. These have a much higher charge-to-mass ratio than the heavier particles and therefore I would think would be more strongly influenced by the solar wind and by the earth’s magnetosphere. Still, I don’t necessarily equate measuring 10 GeV in a satellite orbiting earth, with measuring 10 GeV at the Earth’s surface, which is what an ion chamber does. Then, there is the issue of the Earth’s magnetosphere deflecting high energy particles, which may occur at latitudes lower than the satellite in question. Doesn’t the solar wind affect the strength of currents in the Earth’s magnetosphere? I don’t know the physics really, I’m just asking….

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