Tuesday, August 25, 2015

New paper finds 'robust' relationship between cosmic rays and global temperature, corroborates Svensmark's solar-cosmic ray theory of climate

A reply paper published today in PNAS "identifies a causal relationship between cosmic rays (CRs) and interannual variation in global temperature (ΔGT)." The authors find a "robust" cosmic ray-global temperature relationship, as demonstrated in Fig. 1 below, and thus provide further corroboration of the solar/cosmic ray theory of climate of Svensmark et al.

Reply to Luo et al.: Robustness of causal effects of galactic cosmic rays on interannual variation in global temperature

Tsonis et al. (1) recently used convergent cross mapping (CCM) (2) to identify a causal relationship between cosmic rays (CRs) and interannual variation in global temperature (ΔGT). Subsequently, Luo et al. (3) questioned this finding using the Clark implementation of CCM (version 1.0 of the multispatial CCM package).* This version of the CCM code, which has since been debugged by Clark, unfortunately contains errors that are not in the original rEDM software package that Tsonis et al. used.† Thus, though well-intentioned, the Luo et al. (3) analysis is incorrect.
However, despite the erroneous analysis, Luo et al. (3) raise valid concerns over the robustness of the finding. Here, we demonstrate that the CR effect on ΔGT is robust to reasonable measures of global temperature, and clarify technical details for determining significance with CCM.
CCM uses cross-map prediction as a metric for causality: a variable y has a causal effect on x when the attractor manifold constructed from lags of x can estimate values of y. Causality is established when cross-map performance increases with library size, L, and is significantly better than an appropriate null model at the largest L. Sugihara et al. (2) were the first (to our knowledge) to construct an effective test for causality using these ideas.
As Luo et al. suggest, different ways of subsampling the data to construct libraries, can yield slightly different values for ρ. Indeed, the rEDM software package provides three different sampling methods: (i) taking contiguous segments of length L from among the available x as in ref. 2, (ii) taking bootstrap samples with replacement as in ref. 4, and (iii) taking random subsamples without replacement as in ref. 1.
There are reasons for choosing one method over another. For example, method i should not be used to examine a strongly autocorrelated time series and either ii or iii would be preferable as they sample libraries without consideration for time. Also note that the rEDM cross-validation procedure addresses Luo et al.’s (3) concern over having the pair (xj, yj) in the library when predicting yj.
The second issue raised by Luo et al. (3) is the robustness of the CR–ΔGT relationship to different temperature data records. As discussed in the Intergovernmental Panel on Climate Change AR5 report, HadCRUT4 is the most primary and credible global temperature record (5), with reasonable uncertainty estimates. Other records such as Goddard Institute for Space Studies (GISS) and National Climatic Data Center (NCDC) data have periods that fall outside the 90% confidence interval of HadCRUT4 (see figure 2.19 of ref. 5) and are not as highly regarded. This is partly due to infilling, spatial averaging, or interpolation: smoothing practices known to obscure nonlinearity (6), which would diminish residual interannual CR effects, especially if first differenced time series are used. Thus, among available records, the HadCRUT4 and HadCRUT3v time series are sensible choices for this study, whereas GISS and NCDC are not.
Fig. 1 examines the CR–ΔGT relationship using all three library-sampling methods as well as the four temperature time series examined by Luo et al. (3). As shown, this relationship is robust to both library sampling and reasonable data choices. We note that the significance of causality is determined only at the largest library size, with convergence being a further necessary condition to demonstrate causation.
Fig. 1.
CCM results for four different global temperature time series (HadCRUT3v as in ref. 1, HadCRUT4, GISS, NCDC) and using three different library-sampling methods (contiguous segments, bootstraps, and subsamples). For each panel, the blue line denotes the effect of CRs on interannual temperature variability (“ΔGT xmap CR”), whereas the red line denotes causality in the opposite direction (“CR xmap ΔGT”). The red and blue regions denote the lower 95% quantile for null distributions generated using phase-randomized surrogates. Other parameters were the same as in ref. 1 (selection of E, τ, and prediction delay), but due to an indexing error in ref. 1, data from 1899–2011 were used, and the prediction delay is −1 (instead of −2) for HadCRUT3v xmap CR. Medians over different library samples were computed as a robust measure of central tendency to account for nonnormal and system-specific distributions of ρ. Both HadCRUT3v and HadCRUT4 show the influence of CRs, whereas the more processed GISS and NCDC time series fail to do so. Conversely, there is no evidence for an effect of temperature on CRs (as expected).

Footnotes

References

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Saturday, August 22, 2015

New paper confirms the gravito-thermal greenhouse effect on 6 planets including Earth, falsifies CAGW

An important new paper published in Advances in Space Research determines that the Earth surface temperature (as well as the surface temperatures of 5 other rocky planets in our solar system) can be very accurately determined (R2 = 0.9999! & tiny standard error σ=0.0078) solely on the basis of two variables: 

1) atmospheric pressure at the surface, and 

2) solar irradiance at the top of the atmosphere, 

and without any consideration of any greenhouse gas concentrations or 'radiative forcing' from greenhouse gases whatsoever. 

Thus, the paper adds to the works of at least 40 others (partial list below) who have falsified the Arrhenius radiative theory of catastrophic global warming from increased levels of CO2, and also thereby demonstrated that the Maxwell/Clausius/Carnot/Boltzmann/Feynman atmospheric mass/gravity/pressure greenhouse theory is instead the correct explanation of the 33C greenhouse effect on Earth, and which is independent of "radiative forcing" from greenhouse gases. 

Using observed data from the planets Earth, Venus, the Moon, Mars, Titan, and Triton, the authors,
"apply the Dimensional Analysis (DA) methodology to a well-constrained data set of six celestial bodies representing highly diverse physical environments in the solar system, i.e. Venus, Earth, the Moon, Mars, Titan (a moon of Saturn), and Triton (a moon of Neptune). Twelve prospective relationships (models) suggested by DA are investigated via non-linear regression analyses involving dimensionless products comprised of solar irradiance, greenhouse-gas partial pressure/density and total atmospheric pressure/density as forcing variables, and two temperature ratios as dependent (state) variables. One non-linear regression model is found to statistically outperform the rest by a wide margin. Our analysis revealed that GMATs [Global Mean Atmospheric Temperatures] of rocky planets can accurately be predicted over a broad range of atmospheric conditions [0% to over 96% greenhouse gases] and radiative regimes only using two forcing variables: top-of-the-atmosphere solar irradiance and total surface atmospheric pressure [a function of atmospheric mass & gravity]. The new model displays characteristics of an emergent macro-level thermodynamic relationship heretofore unbeknown to science that deserves further investigation and possibly a theoretical interpretation."


Fig. 4. 
Dependence of the relative atmospheric thermal enhancement (Ts/Tna) on mean surface air pressure according to Eq. (10a) derived from data representing a broad range of planetary environments in the Solar System. Saturn’s moon Titan has been excluded from the regression analysis leading to Eq. (10a). Error bars of some bodies are not clearly visible due to their small size relative to the scale of the axes. See Table 2 for the actual error estimates.
"The above comparisons indicate that Eq. (10b) rather accurately reproduces the observed variation of mean surface temperatures across a wide range of planetary environments characterized in terms of solar irradiance (from 1.5 W m-2 to 2,602 W m-2), total atmospheric pressure (from near vacuum to 9,300 kPa), and greenhouse-gas concentrations (from 0.0% to over 96% per volume). While true that Eq. (10a) is only based on data from 6 planetary bodies, one should keep in mind that these represent all objects in the Solar System meeting our criteria (discussed in Section 2.3) for the quality of available data. The fact that only one of the investigated twelve non-linear regressions yielded a tight relationship suggests that Model 12 might be describing a macro-level thermodynamic property of planetary atmospheres heretofore unbeknown to science . A function of such predictive skill spanning the breadth of the Solar System may not be just a result of chance. Indeed, complex natural systems consisting of myriad interacting agents have been known to exhibit emergent behaviors at higher levels of hierarchical organization that are amenable to accurate modeling using top-down statistical approaches (e.g. Stolk et al. 2003). Equation (10) also displays several other characteristics that lend further support to the above conjecture."


Comparison of the two best-performing regression models according to statistical scores presented inTable 5. Vertical axes use linear scale to better illustrate the difference in skills between the models.
Added: The top model incorporates greenhouse gas partial pressures and has a standard error over 20 times worse than the bottom model which does not consider greenhouse gas concentrations or radiative forcing whatsoever. 
Fig. 5. 
Absolute differences between predicted average global surface temperatures (Eq. 10b) and observed GMATs (Table 2) for studied celestial bodies. Titan represents an independent data point, since it was excluded from the non-linear regression analysis leading to Eq. (10a). 
Added: The surface temperatures of 5 planets are determined within hundredths of degrees C using the Eqn 10a as a sole function of surface pressure and solar insolation. 
Fig. 7. 
a)   Dry adiabatic response of the air/surface temperature ratio to pressure changes in the free atmosphere according to Poisson’s formula (Eq. 12). The reference pressure is arbitrarily assumed to be po=100 kPa;b) The SB radiation law expressed as a response of a blackbody temperature ratio to variation in photon pressure (see text for details). Note the similarity in shape between these two curves and the one portrayed in Fig. 4 depicting Eq. (10a).

The authors have used a new empirical non-linear regression method of determining the gravito-thermal greenhouse effect on 6 planets, and "might be describing a macro-level thermodynamic property of planetary atmospheres heretofore unbeknown to science," but are apparently unaware of and do not cite any of the over 36 scientific works/papers (partial list below) which have described the theoretical basis of the same 33C Maxwell/Clausius/Carnot gravito-thermal effect of atmospheric pressure, some of which also utilize the Poisson relation as illustrated in Fig 7. from the paper above. 

Only one possible explanation of the 33C 'greenhouse' effect temperature gradient on Earth can be possible, otherwise the greenhouse effect would be twice as large (i.e. 66C):


OR

2) The 33C Maxwell/Clausius/Carnot gravito-thermal effect, proven by this new paper and the works/papers of at least 36 others (and very accurately predicts the surface and atmospheric temperatures of all rocky planets with an atmosphere in our solar system):


The HS greenhouse equation

The Maxwell/Clausius et al gravito-thermal 'greenhouse effect'
Richard Feynman
Boltzmann
Chilingar et al
1976 US Standard Atmosphere
International Standard Atmosphere & here
Hans Jelbring
Connolly & Connolly
Nikolov & Zeller
Mario Berberan-Santos et al
Claes Johnson and here
Velasco et al
Huffman
Giovanni Vladilo et al



Highlights

•
Dimensional Analysis is used to model the average temperature of planetary bodies.
•
The new model is derived via regression analysis of measured data from 6 bodies.
•
Planetary bodies used by the model are Venus, Earth, Moon, Mars, Titan and Triton.
•
Two forcing variables are found to accurately predict mean planetary temperatures.
•
The predictor variables include solar irradiance and surface atmospheric pressure.

Abstract

The Global Mean Annual near-surface Temperature (GMAT) of a planetary body is an expression of the available kinetic energy in the climate system and a critical parameter determining planet’s habitability. Previous studies have relied on theory-based mechanistic models to estimate GMATs of distant bodies such as extrasolar planets. This ‘bottom-up’ approach oftentimes relies on case-specific parameterizations of key physical processes (such as vertical convection and cloud formation) requiring detailed measurements in order to successfully simulate surface thermal conditions across diverse atmospheric and radiative environments. Here, we present a different ‘top-down’ statistical approach towards the development of a universal GMAT model that does not require planet-specific empirical adjustments. Our method is based on Dimensional Analysis (DA) of observed data from the Solar System. DA provides an objective technique for constructing relevant state and forcing variables while ensuring dimensional homogeneity of the final model. Although widely utilized in some areas of physical science to derive models from empirical data, DA is a rarely employed analytic tool in astronomy and planetary science. We apply the DA methodology to a well-constrained data set of six celestial bodies representing highly diverse physical environments in the solar system, i.e. Venus, Earth, the Moon, Mars, Titan (a moon of Saturn), and Triton (a moon of Neptune). Twelve prospective relationships (models) suggested by DA are investigated via non-linear regression analyses involving dimensionless products comprised of solar irradiance, greenhouse-gas partial pressure/density and total atmospheric pressure/density as forcing variables, and two temperature ratios as dependent (state) variables. One non-linear regression model is found to statistically outperform the rest by a wide margin. Our analysis revealed that GMATs of rocky planets can accurately be predicted over a broad range of atmospheric conditions and radiative regimes only using two forcing variables: top-of-the-atmosphere solar irradiance and total surface atmospheric pressure. The new model displays characteristics of an emergent macro-level thermodynamic relationship heretofore unbeknown to science that deserves further investigation and possibly a theoretical interpretation.

Wednesday, August 19, 2015

Why greenhouse gases do not "remove" any alleged "missing heat" from the atmosphere

Excerpts from the comments on WUWT post The Trouble With Global Climate Models in which Quaternary geologist Kristian, TimTheToolMan, and myself explain to "Phil" why greenhouse gases do not "remove" any alleged "missing heat" from the atmosphere:


  • Planck’s Law and the theory of blackbody radiation does in fact prove my statement “A low frequency/energy photon (eg 15um CO2 photons) cannot transfer any quantum energy to a higher frequency/energy/temperature blackbody because all of those lower frequency/energy microstates & orbitals are already completely filled/saturated in the hotter body. This fact alone from quantum mechanics falsifies CAGW.”
    As shown on these calculated Planck curves, CO2 (+H2O overlap) absorbs and emits in the LWIR the same as a true blackbody would at an emitting temperature of ~217K over the LWIR band from ~12 or 13um to ~17um
    Even though CO2 has emissivity less than a true black body and line emissions centered around 15um, and observations also show CO2 emissivity decreases with temperature unlike a true BB, for purposes of this simple question, we’ll assume (like climate scientists incorrectly do) that CO2 emits and absorbs as a true BB.
    gammacrux: Can a BB at 217K cause a BB at 255K to warm by 33K to 288K as the Arrhenius theory claims?
    The lower energy/temperature/frequency microstates of a BB at a given temperature are by definition “saturated” in a perfect blackbody absorber/emitter and that explains why classical physics shown by the dashed lines in fig 4.8 does not happen in nature and instead a Planck curve of emission and absorption is found in nature. If those lower energy/temperature/frequency microstates of a BB were not saturated, then any energy level photons could be thermalized by a blackbody and the frequency vs BB energy intensity curve would go to infinity as shown by the (false) dashed lines in fig 4.8:
  • Phil: Yes or No: Can a blackbody at 193K warm a warmer blackbody at 255K by 33K to 288K?
    Phil says: “Since the ‘blackbody at 193K’ is a figment of your imagination there’s no reason to answer it, I would point out that in your pure nitrogen atmosphere the blackbody at 193K would be replacing a background at 4K, that would make quite a difference.”
    NO not even wrong.
    Phil claims the blackbody at 193K is a figment of the OLR spectra that both he and I have posted!
    Phil look very closely: do you see the blackbody Planck curves calculated for blackbodies with emitting temperatures of 220K-320K?
    Do you see that the CO2+H2O overlap corresponding Planck curve is ~217K (it is higher than 193K for pure CO2 due to presence of water vapor overlap) in the LWIR spectra of any relevance to the AGW debate 12-17um?
    THAT is the 217K “partial blackbody” I’m asking about. YOU are effectively claiming that radiation from a “partial blackbody” at a peak emitting temperature of ~217K in the 12-17um band can make a true black body e.g. the Earth warm from the 255K equilb temp with Sun by 33K to 288K!
    Secondly, I’ve already shown you (and so does Feynman’s chapter 40, vol 1, and the US Std Atmosphere, Maxwell, etc) that a pure N2 or pure N2/O2 Boltzmann distribution atmosphere would have almost the same temperature gradient as our current atmosphere:
    The “ERL” on a planet with pure N2 atmosphere is located at the surface h=0 and is exactly equivalent to the equilibrium temperature with the Sun for that planet, NOT “a blackbody at 193K” as you falsely claim above!

WSJ: Obama’s Wind-Energy Lobby Gets Blown Away

Obama’s Wind-Energy Lobby Gets Blown Away

A California judge rules in favor of bald eagles and against 30-year permits to shred them



Chalk one up for the bald eagle. The avian symbol of American freedom has beaten theObama administration and the wind industry in court, though the majestic birds still don’t stand a chance when flying near the subsidy-fueled blades of green-energy production.
On Aug. 11, a federal judge in the Northern District of California shot down a rule proposed by the U.S. Fish and Wildlife Service (FWS) that would have allowed the wind industry to legally kill bald eagles and golden eagles for up to three decades.
The ruling is a setback for the wind industry and President Obama’s Clean Power Plan, which depends on tripling domestic wind-energy capacity to meet the plan’s projected cuts in carbon-dioxide emissions by 2030. The ruling also exposes the Obama administration’s cozy relationship with the wind industry and the danger to wildlife posed by a major expansion of wind-energy capacity.
U.S. District Judge Lucy H. Koh, an Obama appointee, ruled in favor of the plaintiff, the American Bird Conservancy, and against the FWS’s “eagle take” rule. Judge Koh found that the FWS violated the National Environmental Policy Act in 2013 when the agency’s director, Dan Ashe, decided that the agency could issue permits to wind-energy companies that would have allowed them to lawfully kill eagles for up to 30 years without first doing an environmental-impact assessment. Permits were previously limited to five years.
Mr. Ashe, an Obama nominee who has headed the FWS since 2011, ignored the advice of a staff member who warned him, according to the ruling, that “real, significant, and cumulative biological impacts will result” if the eagle-kill permits were extended from five to 30 years. Rather than listen to his staff, Mr. Ashe sided with the wind-energy lobby, which pushed hard for the 30-year permits. More than a dozen wind companies have applied for eagle-kill permits.
Bird kills in general, and eagle kills in particular, are a legal and public-relations nightmare for an industry that promotes itself as “green.” The FWS and the Justice Department have been reluctant to prosecute the wind industry for killing protected birds—bringing only two cases against wind-energy companies over the past two years—even though a study published in the March 2013 issue of the Wildlife Society Bulletin found that wind turbines in the U.S. kill some 573,000 birds and 880,000 bats each year. The study also said there is an “urgent need to improve fatality monitoring methods” at wind facilities.
Under the Clean Power Plan, the Energy Department projects that wind-generation capacity will surge from 66 gigawatts in 2014 to some 200 gigawatts in 2030. But for that expansion to happen, the federal government will have to give wind companies formal permission to kill some of our most iconic wildlife. And that’s where the raptor meets the turbine blade.
The Clean Power Plan relies on wind more than any other form of renewable energy to reduce greenhouse gas emissions. Achieving those reductions will require covering roughly 54,000 square miles of land (an area about the size of New York state) with tens of thousands of new turbines.
Those turbines will be killing birds and bats in far greater numbers than they are now. Yet the federal government has no clear policies for how it will handle the impending slaughter or to what extent it will prosecute wind-energy companies for violating the 1940 Bald and Golden Eagle Protection Act and the 1918 Migratory Bird Treaty Act.
The rationale being used by renewable-energy promoters and the Obama administration is that future climate change trumps today’s wildlife concerns. Therefore, we have to kill lots of birds and bats with turbines to save them from the possibility of climate change. Never mind that whatever carbon-dioxide cuts we achieve will be swamped by soaring emissions growth in places like Brazil, India and Indonesia.
Meanwhile, the killing by wind turbines continues. On July 25 a wounded female golden eagle was found near a turbine at the Altamont Pass Wind Resource Area in northern California. A local 2008 study estimated that the Altamont wind facility kills some 60 golden eagles, 2,500 raptors and 7,000 non-raptors each year. The injured eagle was taken to a wildlife hospital where veterinarians found the bird’s wing had been “shredded.” Saving the bird was deemed futile and the eagle was euthanized.
Last week an FWS spokesman told me the agency is “looking into the circumstances surrounding” the eagle death at Altamont.
Mr. Bryce, a senior fellow at the Manhattan Institute, is the author of “Smaller Faster Lighter Denser Cheaper: How Innovation Keeps Proving the Catastrophists Wrong” (PublicAffairs, 2014).

WSJ: Steyer's Calfiornia green scheme fails to create jobs or save energy

Tom Steyer’s Stimulus

A California green scheme fails to create jobs or save energy.


Billionaire climate activist Tom Steyer speaks during a news conference in Santa Monica, Calif. on Aug. 5.

Aug. 18, 2015 6:57 p.m. ET THE WALL STREET JOURNAL

How many workers does it take to change an incandescent light bulb in California? Two. One to install its energy-efficient replacement, and another to ensure the job complies with government regulations. Behold Tom Steyer’s green jobs stimulus, which a new report from the Associated Press shows has been a colossal failure even by its proponents’ standards.
In 2012 the hedge-fund billionaire bankrolled a California ballot initiative (Prop. 39) hitting up corporations to finance green construction jobs. The referendum changed the way many corporations that do business across state lines calculate their tax liability. Half of the new revenues were to be earmarked for “clean energy” (e.g., LED and solar panel installations) with the rest flowing into Sacramento’s general fund for the politicians to spend.
Mr. Steyer and friends claimed the initiative would raise more than $500 million annually for green projects and create tens of thousands of jobs. Neither dream has come true. According to AP, the initiative’s clean-energy fund has raised $973 million over the past three years—about a third less than projections because companies have responded by seeking to minimize their tax liabilities.
And little of that has gone toward creating “clean energy.” Funding recipients have frittered away millions completing paperwork—energy surveys, audits, data analytics—to meet California Energy Commission’s guidelines, which require $1.05 of energy savings for every dollar spent. Schools have spent more than half of the $297 million that they’ve received on consultants and auditors. As if California’s regulatory compliance industry needed more work.
AP reports that the initiative has created all of 1,700 jobs over three years, yet the state doesn’t know how much if any energy has been saved. Credit to Mr. Steyer for his grand ambitions. His initiative may beat the 2009 Obama-Pelosi blowout as the country’s least effective jobs stimulus.
Mr. Steyer told AP the initiative has nonetheless accomplished its goal of closing a “corporate loophole.” But then results rarely matter for the supporters of green subsidies. Their good intentions in spending other peoples’ money is enough.