Troy's Scratchpad

September 17, 2012

My ESD paper on cloud feedbacks was published

Filed under: Uncategorized — troyca @ 7:17 am

ESD being Earth System Dynamics, and is available open-access here (along with the code and data supplement).  The abstract is as follows:

A detailed analysis is presented in order to determine the sensitivity of the estimated short-term cloud feedback to choices of temperature datasets, sources of top-of-atmosphere (TOA) clear-sky radiative flux data, and temporal averaging. It is shown that the results of a previous analysis, which suggested a likely positive value for the short-term cloud feedback, depended upon combining all-sky radiative fluxes from NASA’s Clouds and Earth’s Radiant Energy System (CERES) with reanalysis clear-sky forecast fluxes when determining the cloud radiative forcing (CRF). These results are contradicted when ΔCRF is derived using both all-sky and clear-sky measurements from CERES over the same period. The differences between the radiative flux data sources are thus explored, along with the potential problems in each. The largest discrepancy is found when including the first two years (2000–2002), and the diagnosed cloud feedback from each method is sensitive to the time period over which the regressions are run. Overall, there is little correlation between the changes in the ΔCRF and surface temperatures on these timescales, suggesting that the net effect of clouds varies during this time period quite apart from global temperature changes. Given the large uncertainties generated from this method, the limited data over this period are insufficient to rule out either the positive feedback present in most climate models or a strong negative cloud feedback.

As you may recall, this primarily grew out of my frustration with the Dessler (2010) Science paper, which concluded that the shortwave, longwave, and total components of the short-term cloud feedback were all likely positive, as I found that if you didn’t substitute in the reanalysis values for clear-sky (and just use the same CERES flux source), this resulted in an estimated negative cloud feedback.  I did a guest post on this at Lucia’s over a year ago, and Steve McIntyre posted on this as well.  Moreover, the reference given in Dessler (2010) as the reason for avoiding CERES clear-sky discusses the absolute OLR bias, which would not directly affect the SW component in any significant way, and other results suggested this would not affect interannual anomalies (Allan et al., 2003) either.  My paper is basically a sensitivity test, highlighting the sensitivities to clear-sky flux, the time period used, as well the temperature dataset chosen. 

Ultimately, I think subsequent research into the topic has revealed a variety of issues in all data sets (as reflected in the paper), and the introduction of the global EBAF dataset in the interim has made things more interesting.  I believe the paper has improved in the open review process from the referee comments, including those from Dr. Dessler who served as non-anonymous reviewer, despite the fact that I think he ultimately disagrees with some of my conclusions.

So, what does the paper show?  Basically, as you can see from the abstract, I don’t believe that regressing global temperature anomalies induced by ENSO variations against the cloud forcing in this manner tells us much of interest with respect to the "cloud feedback" one may expect in relation to a doubling of CO2.  It certainly doesn’t in models.  This is the reason for such sensitivity to various methodological choices.  With ENSO, you essentially have a progression of when the warming occurs at different areas, so that the estimate for the cloud feedback varies wildly at different time lead/lags or using ocean vs. SAT vs. lower tropospheric temperatures.  (Some related discussion of modeled cloud biases during ENSO vs. long-term can be found in Sun et al., 2009)

The paper has already gotten some publicity from James Annan, although I haven’t really done any other promoting given that I don’t think the results are particularly groundbreaking, despite it being “controversial” for criticizing an earlier paper.  One thing I learned – I don’t have much desire to be lead or sole author on another “controversial” paper anytime soon…it seems quite exhausting for a hobby!

September 8, 2012

Temperature and CO2 diff lags with GFDL-ESM2M

Filed under: Uncategorized — troyca @ 8:53 am

Thanks to Ob and Richard Telford, who in the comments of that last post suggested I try the demonstration using one of the CMIP5 scenario runs as well.  Again, this demonstration is to show why the Humlum, Stordahl, and Solheim (2012) DIFF12 method is not useful for determining the long-term cause vs. effect of the increase in CO2 vs. surface temperatures.  Other commentators have made better points on exactly why – basically, the DIFF12 method removes the trend, and if ENSO variations dominate for the CO2 rate-of-change fluctuations (NOT changes in CO2 itself, where the long-term trend of prescribed CO2 dominates the ENSO fluctuations) in these models, the HSS2012 method incorrectly diagnoses what is the overall cause.

I ran into a few issues getting the proper model output.  I first tried NCAR CESM1 from the Earth System Grid CMIP5 data archive, for the rcp4.5 scenario along with two of the runs from the idealized 1pct CO2 increase experiment.  Unfortunately, the output for the “co2” variable appears to be garbled for the 1pct CO2 increase runs (It starts at the wrong level from the experiment, decreases exponentially to what should be the start value, then goes to 0), so I sent an e-mail to the errata admin…and I noticed the errata also notes that the rcp4.5 scenario variables are corrupted, as I experienced as well.    I tried to obtain NorESM data through ESG, but kept getting a server (tomcat) error. 

Thus, I decided to go back to the GFDL data portal and simply use the GFDL-ESM2M 1 pct CO2 experiment.  Oh, and a word of warning for those who want to do something similar: I was tempted by the “co2mass” variable, since it already includes a global sum of CO2 mass in atmosphere, but from what I can tell this may be a prescribed value and thus does not show the ENSO-induced fluctuations of the co2 mole fraction (which I simply averaged here globally at 600mb, just a bit higher than the Mauna Loa station).  The script is available here.

Anyhow, without further ado, here are the graphs of CO2 and temperature anomalies:

CO2_GFDL_ESM2M_1pcttas_GFDL_ESM2M_1pct

And our graph of the DIFF12 values:

tas_co2_diff_GFDL_ESM2M_1pct

Again, according to the HSS12 method, this would seem to imply that the changes in surface temperature are causing the increase in CO2, which we know is simply not true for this model (where the increase in CO2 is prescribed).  A closer look at the cross-correlation in this model shows:

ccf_diff_GFDL_ESM2M_1pct

So one thing of interest here is that this model seems to show a maximum correlation between CO2 and surface temperature diffs at 4 month lags, rather than 9 to 11 months from the HSS12 paper.  To me, this might have been a more interesting paper if the authors had compared their results to several of the CMIP5 models to see how well those models reproduced ENSO-induced CO2 changes.  This would have spoiled their conclusions that CO2 increases are caused by ocean warming, but it could have been constructive. 

P.S. For some more info on carbon cycles in GCMs, this presentation looks interesting.

The Silver is the New Black Theme. Blog at WordPress.com.

Follow

Get every new post delivered to your Inbox.