A look at the Thompson et al paper – hi tech wiggle matching and removal of natural variables

Thompson et al (2009) – High-Tech Wiggle Matching Helps Illustrate El Nino-Induced Step Changes

Guest Post by Bob Tisdale

Thompson_et_al

INTRODUCTION

In “Identifying signatures of natural climate variability in time series of global-mean surface temperature: Methodology and Insights”, Thompson et al (2009) remove the effects of three natural variables from the Global Surface Temperature record (January 1900 to March 2009). Those three natural variables are El Nino-Southern Oscillation, stratospheric aerosols emitted by explosive volcanic eruptions, and “variations in the advection of marine air masses over the high latitude continents during winter”, which they condense to “dynamically induced variability” or Tdyn in the paper. Thompson et al use “a series of novel methodologies to identify and filter out of the unsmoothed monthly-mean time series of global-mean land and ocean temperatures the variance associated with ENSO, dynamically-induced atmospheric variability, and volcanic eruptions.”

Thompson et al (2009) Link:

http://ams.allenpress.com/perlserv/?request=get-abstract&doi=10.1175%2F2009JCLI3089.1

Preprint Version:

http://www.atmos.colostate.edu/ao/ThompsonPapers/TWJK_JClimate2009_revised.pdf

Thompson et al (2009) also provided a link to five of the datasets they used and created while preparing the paper. The webpage is identified as “Data for Thompson, Wallace, Jones, Kennedy”:

http://www.atmos.colostate.edu/~davet/ThompsonWallaceJonesKennedy/

OVERVIEW

This post briefly discusses the data made available by Thompson et al (2009), it illustrates the ENSO and volcanic aerosol residuals that remained in the global temperature anomaly data after the effects of ENSO, volcanic aerosols, and dynamically induced variability were said to be removed, and it illustrates the El Nino-induced step changes that resulted from the significant El Nino events that occurred since 1976.

The post does not discuss the erroneous assumption made by Thompson et al (2009), which is that the relationship between ENSO and global temperature is linear. It is not. The non-linear relationship between ENSO and global temperatures was discussed in the following three posts, which all cover the same subject, fundamentally, though there are differences in the presentation:

1. The Relationship Between ENSO And Global Surface Temperature Is Not Linear

2. Multiple Wrongs Don’t Make A Right, Especially When It Comes To Determining The Impacts Of ENSO

3. Regression Analyses Do Not Capture The Multiyear Aftereffects Of Significant El Nino Events.”

The data furnished by Thompson et al actually reinforces the fact that the global temperature response to El Nino events is not linear.

THOMPSON ET AL (2009) DATA

INITIAL NOTE: The title block of the graphs in this post use the nomenclature from the “Data for Thompson, Wallace, Jones, Kennedy” webpage linked above.

Figure 1 illustrates the residual global temperature time-series data after the effects of ENSO, volcanic aerosols, and dynamically induced variability were removed. It is identified throughout this post as “Tdyn/ENSO/Volcano residual global mean”. ENSO continues to make its presence known in the “Tdyn/ENSO/Volcano residual global mean” data in Figure 1, indicating that Thompson et al failed to remove all of the effects. Note the spike from the 1997/98 El Nino and the dip due to the 2007/08 La Nina. Both are reduced in magnitude, but they are still quite visible. There are other El Nino event residuals in the data, as will be illustrated later.

http://i37.tinypic.com/4r8apz.png

Figure 1

Figure 2 is a comparative graph of the raw “Tdyn/ENSO/Volcano residual global mean” data and Global Surface Temperature anomalies (listed as “Global mean” on the “Data for Thompson, Wallace, Jones, Kennedy” webpage linked above). Thompson et al (2009) identifies the “Global mean” data as HadCRUT3, which is the Hadley Centre’s combined land surface temperature and SST data.

http://i38.tinypic.com/jacsaw.png

Figure 2

Smoothing both datasets with 13-month filters, Figure 3, helps to highlight the ENSO residuals left in the “Tdyn/ENSO/Volcano residual global mean” data. It also illustrates how well the methods used by Thompson et al (2009) appear to have removed the effects of volcanic aerosols. Note the differences in the datasets immediately following the 1982 and 1991 volcanic eruptions of El Chichon and Mount Pinatubo.

http://i38.tinypic.com/2ed8voh.png

Figure 3

Thompson et al (2009) uses Cold Tongue Index data [5S-5N, 180-90W] as the base for its “ENSO fit” data, Figure 4. Link to “ENSO fit” data:

http://www.atmos.colostate.edu/~davet/ThompsonWallaceJonesKennedy/TGlobe1900March2009_ENSOfit

NOTE: The methods used by Thompson et al (2009) to create the “ENSO fit” (“Volcano fit” and “Dynamic fit”) datasets will not be discussed in this post. Refer to the paper for further information.

http://i34.tinypic.com/f53lme.png

Figure 4

Figure 5 is comparative graph of scaled HADSST Cold Tongue Index data (downloaded through the KNMI Climate Explorer) and the “ENSO fit” data. The model used by Thompson et al (2009) exaggerated the Cold Tongue Index data in some months and suppressed it in others.

http://i38.tinypic.com/10rikb4.png

Figure 5

A time-series graph of the “Volcano fit” data is presented in Figure 6. Link to “Volcano fit” data:

http://www.atmos.colostate.edu/~davet/ThompsonWallaceJonesKennedy/TGlobe1900March2009_VOLCANOfit

http://i34.tinypic.com/2n0n5p0.png

Figure 6

The data source for volcanic aerosols in Thompson et al (2009) is the Sato Stratospheric aerosol optical depth data available though GISS:

http://data.giss.nasa.gov/modelforce/strataer/

Specifically:

http://data.giss.nasa.gov/modelforce/strataer/tau_line.txt

Figure 7 compares the “Volcano fit” data and the inverted and scaled Sato Mean Optical Thickness data. There are minor differences in the month-to-month variations between the source data and the model output.

http://i36.tinypic.com/2qcp7ar.png

Figure 7

The “Dynamic fit” dataset, Figure 8, is unique to Thompson et al (2009). As noted above, it accounts for the “variations in the advection of marine air masses over the high latitude continents during winter.” They provide a detailed description of the dataset starting on page 9 of the paper. Link to “Dynamic fit” data:

http://www.atmos.colostate.edu/~davet/ThompsonWallaceJonesKennedy/TGlobe1900March2009_TDYNfit http://i38.tinypic.com/amfxup.png

Figure 8

Figure 9 is a comparative graph of the “ENSO fit”, “Volcano fit”, and “Dynamic fit” datasets for those who are interested in seeing their relative magnitudes. The data have been smoothed with 13-month running average filters.

http://i36.tinypic.com/2rc4prl.png

Figure 9

DETRENDED “Tdyn/ENSO/Volcano residual global mean” DATA

To provide an alternate view of the “Tdyn/ENSO/Volcano residual global mean” data, I’ve excluded the first 11 years of data, a short period of declining temperatures, and divided the remainder into three epochs, Figure 10: January 1912 to December 1943 (period of temperature increase), January 1944 to December 1975 (period of flat to declining temperatures), and January 1976 to March 2009 (period of temperature increase). I then detrended the “Tdyn/ENSO/Volcano residual global mean” data during those periods and compared them to the “ENSO fit” and “Volcano fit” datasets, the two major climate variables, to illustrate how much of the ENSO signal remained after the effects of the three variables were removed.

http://i38.tinypic.com/2i0c0mx.png

Figure 10

Figure 11 covers the period of Jan 1976 to March 2009. It compares detrended “Tdyn/ENSO/Volcano residual global mean” data to “ENSO fit” and “Volcano fit” data. There appears to be very little of the 1982 volcanic eruption left in the “Tdyn/ENSO/Volcano residual global mean” data, while the some of the 1991 eruption remains.

http://i35.tinypic.com/2n0ei8.png

Figure 11

In Figure 12, I’ve deleted the “Volcano fit” data, leaving a comparison of detrended “Tdyn/ENSO/Volcano residual global mean” and “ENSO fit” data for the period of January 1976 to March 2009. As illustrated there are very large ENSO residuals remaining in the detrended “Tdyn/ENSO/Volcano residual global mean”. Note how the lag varies with each ENSO event. It is apparent that Thompson et al failed to capture and remove a significant portion of ENSO during this period.

http://i35.tinypic.com/2znmols.png

Figure 12

Figure 13 illustrates the detrended Thompson et al (2009) “Tdyn/ENSO/Volcano residual global mean”, the “ENSO fit” and the “Volcano fit” data for January 1944 to December 1975. The major drop in detrended “Tdyn/ENSO/Volcano residual global mean” from 1943 to 1947 represents the discontinuity in the HadCRUT3 data that was first discussed in Thompson et al (2008) “A large discontinuity in the mid-twentieth century in observed global-mean surface temperature,” Nature, 453, 646–650, doi:10.1038/nature06982.Link:

http://www.nature.com/nature/journal/v453/n7195/abs/nature06982.html

http://i36.tinypic.com/2uy1zpz.png

Figure 13

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SIDE NOTE

The Hadley Centre appears to be using both papers to justify changes they are making to the HADSST dataset. In the concluding remarks of Thompson et al (2009), they write, “THE SST DATA CORRECTED FOR INSTRUMENT CHANGES IN THE MID 20TH CENTURY ARE EXPECTED TO BECOME AVAILABLE IN 2009, and it will be interesting to see how the corrections affect the time history of global-mean temperatures, particularly in the middle part of the century.” [Emphasis added.]

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Figure 14 compares detrended “Tdyn/ENSO/Volcano residual global mean” and “ENSO fit” data from January 1944 to December 1975 to illustrate, again, that there are sizable residual ENSO effects in the dataset. Note that during this period there is little to no lag between the “ENSO fit” and the detrended “Tdyn/ENSO/Volcano residual global mean” data, while there were considerable lags between the two datasets from 1976 to present. Is this a function of the magnitude of the ENSO events, where there are longer lags with larger ENSO events?

http://i35.tinypic.com/fc09jc.png

Figure 14

Figures 15 and 16 are the comparative graphs of detrended “Tdyn/ENSO/Volcano residual global mean” and “ENSO fit” data from January 1912 to December 1943. Figure 15 includes the “Volcano fit” data; Figure 16 does not. Note how there is little agreement between the multiyear variations of the ENSO data and the detrended “Tdyn/ENSO/Volcano residual global mean” data.

http://i38.tinypic.com/wb9z80.png

Figure 15

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http://i33.tinypic.com/2zrgwtj.png

Figure 16

The lack of agreement between the two datasets during this period is likely the result of the uncertainties in the datasets, especially the Cold Tongue Index data. Figures 17 and 18 illustrate the number of SST observations for the Cold Tongue region from 1845 to 1991 and from 1900 to 1950. Note how few observations were made in the early part of the Thompson et al (2009) data compared to more recent numbers. Also note that the number of observations between 1900 and 1950 was influenced by the opening of the Panama Canal in 1914 and by the two World Wars. JISAO link:

http://jisao.washington.edu/data/cti/

http://i33.tinypic.com/sfcks1.png

Figure 17

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http://i38.tinypic.com/144a981.png

Figure 18

Would the model used by Thompson et al (2009) have better determined the relationship between ENSO and global temperature during the last two epochs had they excluded the data before 1943? In other words, did the uncertainties in the Global Surface Temperature and Cold Tongue Index data prior to 1943 skew their model so that it failed to identify the true relationship between the datasets in later years. Figures 19, 20, and 21 are comparative graphs of detrended “Tdyn/ENSO/Volcano residual global mean” data and detrended “Global mean” data, which is the unadjusted global surface temperature data, for the three periods. The model used by Thompson et al (2009) appears to have removed little of the effects of ENSO.

http://i37.tinypic.com/302xfuo.png

Figure 19

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http://i33.tinypic.com/2zs0fg1.png

Figure 20

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http://i37.tinypic.com/2eexyrq.png

Figure 21

A CLOSER LOOK AT THE RESIDUAL DATA FROM 1976 TO PRESENT REVEALS STEP CHANGES DUE TO SIGNIFICANT EL NINO EVENTS

Like many climate bloggers I have removed the linear effects of ENSO and volcanic aerosols from a number of different TLT and surface temperature datasets. While doing so, I’ve noted a curious effect in the data since 1976 but I’ve been hesitant to post the results because of the possibility of claims that I’d somehow manipulated the data to create the effect. Since the data was created by Thompson et al (2009) there should be no way for others to accuse me of misrepresenting the data. They may not agree with my results or how I segmented the data, but that is something else entirely. For them, in the closing, I’ve provided links to my posts that illustrate El Nino-induced step changes in TLT and SST data. Additionally, I would anticipate that someone will note that El Nino (and La Nina) events are not official ENSO events unless NINO3.4 SST anomalies equal or rise above (or fall below) 0.5 deg C. For that someone, global temperatures do not respond only to variations in eastern equatorial Pacific SST anomalies when the ENSO event is official; they respond to the entire ENSO signal.

Figure 22 is a comparison graph of the “ENSO fit” and “Tdyn/ENSO/Volcano residual global mean” data from 1976 to present. Neither dataset has been smoothed. What struck me was, after the initial warming from 1976 to early in 1982, the majority of the rises in the “Tdyn/ENSO/Volcano residual global mean” data occurred during the significant El Nino events of 1982/83, 1986/87/88 and 1997/98. I’ve highlighted the months when the “ENSO fit” data crosses zero for those El Nino events.

http://i37.tinypic.com/2nqxgm1.png

Figure 22

If the “Tdyn/ENSO/Volcano residual global mean” data during those El Nino events is eliminated, Figure 23, something else emerges. Note how there appears to be little to no rise in the “Tdyn/ENSO/Volcano residual global mean” data after the 1997/98 El Nino. The data looks flat. Also note how little the “Tdyn/ENSO/Volcano residual global mean” data rose between the 1986/87/88 and 1997/98 El Nino events. There’s the decline in the data between the 1982/83 and 1986/87/88 El Nino events. Last thing to note, the most substantial rise in “Tdyn/ENSO/Volcano residual global mean” data occurred from 1976 to early in 1982.

http://i34.tinypic.com/s2zhvs.png

Figure 23

If we ignore the short period between the 1982/83 and 1986/87/88 El Nino events when temperatures fell, the “Tdyn/ENSO/Volcano residual global mean” data has not been accelerating; it has been decelerating. This can be seen quite clearly if the trends during the “non-significant El Nino periods” are determined and added to the illustration. Refer to Figure 24 for those trends.

http://i33.tinypic.com/2i7o3dj.png

Figure 24

In Figure 25, keying off the trend lines, I’ve listed the rises in the “Tdyn/ENSO/Volcano residual global mean” data that occurred during the significant El Nino events of 1982/83, 1986/87/88, and 1997/98. It appears that most of the rise in “Tdyn/ENSO/Volcano residual global mean” data after early 1982 was the direct result of those El Nino events.

http://i38.tinypic.com/10nt7w3.png

Figure 25

CLOSING

Step changes in TLT anomalies and SST anomalies that resulted from significant El Nino events are discussed in detail in:

RSS MSU TLT Time-Latitude Plots…

Can El Nino Events Explain All of the Global Warming Since 1976? – Part 1

Can El Nino Events Explain All of the Global Warming Since 1976? – Part 2

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September 25, 2009 8:45 am

Juraj V: You wrote, “I am overly curious how CRU will handle that truly ‘anthropogenic’ step-down in SST in 40ties, causing similar step in all global datasets.”
What always struck me odd was that they were basing their claim of a discontinuity in 1945 for their entire SST dataset on the fact that there were no corresponding ENSO events or volcanic eruptions to cause the drop. Did they consider that maybe they overlooked a significant El Nino/La Nina event during the hand-off between U.S. and British sampling periods. Sure does look like there’s a missing significant El Nino/La Nina around 1945 to me.
http://i38.tinypic.com/nwzpj9.png
Which is more likely, that the SST data for 95% of the global oceans are wrong, or that SST data for an area that represent 5% of the global oceans are wrong?

George E. Smith
September 25, 2009 9:30 am

“”” Jeff L (06:28:51) :
I think the most significant point is that air temp lags ocean temps. Extremely significant in that most of the energy of our climate system is in the oceans, not the air. Here’s the basic math:
1) The heat capacity (unit storage of energy per unit mass) of water is 4 times larger than air.
2) The density of water is 773 times greater than air ( 1 g/cc vs 0.001293 g/cc).
3) Standard atmospheric air pressure at the surface is 14.696 psi.
4) Standard water density is 0.43353 psi/ft (strange density units for some, but commonly used in geoscience)
5) How much ocean water is equal to the weight of of the atmosphere? ==> 14.696 psi / 0.43353 psi/ft = 33 ft
6) Roughly 3/4 of the earth is covered by water, so 33/ (0.75) = 44 ft of ocean = weight of entire atmosphere
7) So, the weight of the top 44 ft of the oceans is equal to the entire weight of our atmosphere – BUT – we still have to take into account heat capacity and water is 4x air so : 44 /4 = 11 ft.
8) The basic conclusion is the top 11 FT OF THE OCEANS CONTAIN THE SAME AMOUNT OF ENERGY AS THE ENTIRE ATMOSPHERE. (assuming long term equilibrium between the two ). “””
Well I followed your stick in the sand math up through #7 which you say gives the relative heat capacities of atmosphere and 11 feet of ocean water.
But so far; not a jot of energy anywhere in either ocean or atmosphere; yet suddenly comes #8 out of the blue and decleares the two energies to be equal.
So it is like you just showed that the heat capacity of the air in my kitchen is equal to the heat capacity of one ice tray cell in my freezer; and suddenly they each have to contain the same energy; how is that ?

JAN
September 25, 2009 11:14 am

Jeff L (06:28:51) :
True, a 1 degree transient air temperature response from GHG heating (or any other source) will lead to an equilibrium temperature response of 1/60 degree after a new air/ocean equilibrium is obtained. That is assuming real world physics apply. However, this is “climate science”, so that assumption is wrong.
Climate science postulates that the relationship between the transient response and equilibrium response is different: Transient response + Positive feedback/heat in the pipeline = Equilibrium response. This means that an atmosphere heated 1 degree from increased CO2, will create a hidden energy storage in the deep oceans, that decades or centuries later will come back and be released into the atmosphere again, creating a temperature rise of 3 degrees. This is settled science.

Jeff L
September 25, 2009 11:17 am

George E. Smith (09:30:22) :
“yet suddenly comes #8 out of the blue and decleares the two energies to be equal.”
– the key is
“assuming long term equilibrium between the two” as I said at the at the end of (8)
Do you have reason to believe that the two should not be in long term thermal equilibrium (ie contain the same amount of energy) ?
With no insulator between the two, there is no reason they would not be in equilibrium over the long term (heat transfer & mixing will take some period of time )

John Finn
September 25, 2009 1:36 pm

Chris (08:27:37) :
Quick summary of post:
5. Given the above (and a quiet sun), I would be betting on cooler (versus hotter) temps going forward.

You should contact James Annan. He will be happy to take your bet.

cohenite
September 25, 2009 5:02 pm

JAN; “settled science”?! Perhaps you would like to comment on what OHC is doing; clue: it is going down, so where is that equilibrium response heat being stored?

H.R.
September 25, 2009 6:26 pm

Bob Tisdale (08:32:18) :
Thanks for expanding (and a little rewording). I had read the text below Fig 23 and stopped. After your response I went back and found it helpful (to me, at least) to go right through from Fig 23 to 24 to 25.
Thanks again.

Paul Vaughan
September 25, 2009 6:51 pm

When the PDO changes phase, as it did in the mid-1940s, global precipitation south of 55N tends to kick up a fuss. On top of the PDO shift, we see AMO plummet coincident with this:
http://www.sfu.ca/~plv/NutationObliquity.png

Add all of this to Bob’s earlier post:
“The Large 1945 SST Discontinuity Also Appears in Cloud Cover and Marine Air Temperature Data”
http://bobtisdale.blogspot.com/2009/03/large-1945-sst-discontinuity-also.html
I wrote to the ICOADS people and they told me the cloud observations have nothing to do with the SST measurements.
Additionally, the authors have made untenable assumptions about shared variance. This is a particularly serious error. They should be well-aware of links between NAM/AO & ENSO/SOI. (I’ll post some more graphs if/when I can find time to help illustrate the lack of independence [which has been falsely assumed in the decompositions].)

SOYLENT GREEN
September 25, 2009 6:54 pm

Did we say more intensity? We just meant more…of everything.
Sorry for the confusion.

September 25, 2009 7:04 pm

JAN: You wrote, “This is settled science”, and used “heat in the pipeline” with respect to Ocean Heat Content.
It’s my experience that bloggers who use those phrases base their understanding of climate variability on GCMs and not on the instrument temperature record.
First, many of the Global Circulation Models employed by the “settled science” of the IPCC do not model ENSO. Those that do model ENSO model it poorly. This is caused by the modelers misunderstanding of ENSO. They treat it as noise, like Thompson et al (2009), the topic of this post. ENSO is a process.
I’ve illustrated the SST anomalies for 25% of the global oceans rise in steps in response to significant ENSO events, while the remaining 75% of the oceans mimic the rises and falls of ENSO. When averaged together, those two portions of the global oceans give the impression of a gradual rise in SST anomalies that is mistaken for anthropogenic warming. These step changes were discussed in the posts I linked at the end of this post. Here they are again:
http://bobtisdale.blogspot.com/2009/01/can-el-nino-events-explain-all-of.html
http://bobtisdale.blogspot.com/2009/01/can-el-nino-events-explain-all-of_11.html
As I wrote above in a reply to Fred2 above, they also cause step increases in Ocean Heat Content:
http://bobtisdale.blogspot.com/2009/09/enso-dominates-nodc-ocean-heat-content.html
Not negative step changes, positive step changes.
Oops, almost forgot, those significant El Nino events also cause upward step changes in TLT anomalies for the mid-to-high latitudes of the Northern Hemisphere, while the rest of the world mimics the variations of ENSO. Same thing happens when you mix the two. It gives the impression of AGW. The 1997/98 El Nino and the decade afterwards offer a rare opportunity to see this because there wasn’t a major volcanic eruption to add noise and spoil the effect. Refer to the following graph:
http://i38.tinypic.com/k3ndzn.png
This is discussed further in my post:
http://bobtisdale.blogspot.com/2009/06/rss-msu-tlt-time-latitude-plots.html%5B
If and when GCMs can properly model the multiyear and decadal aftereffects of ENSO, they might be believable. At present they cannot, and are, therefore, not credible sources of forecasting or hindcasting.

JAN
September 26, 2009 1:00 am

cohenite (17:02:17) :
“JAN; “settled science”?! Perhaps you would like to comment on what OHC is doing; clue: it is going down, so where is that equilibrium response heat being stored?”
Where, indeed. It is my understanding the “settled science” of AGW claims that the “heat in the pipeline” is being stored in the deep oceans below the thermocline. Hence, it will not show up as OHC. AFAIK though, there isn’t even a hypothesis on the mechanisms in play for transfer of the GHG warming of the atmosphere into the deep oceans, neither is there one for the amplification of the energy in storage and subsequent release of this energy back to the atmosphere decades or centuries later. Yet, this is being propagated by the AGW community as settled science. Go figure.

JAN
September 26, 2009 1:15 am

Bob Tisdale (19:04:58) :
“JAN: You wrote, “This is settled science”, and used “heat in the pipeline” with respect to Ocean Heat Content.
It’s my experience that bloggers who use those phrases base their understanding of climate variability on GCMs and not on the instrument temperature record.”
Bob, I didn’t necessarily relate “heat in the pipeline” to OHC. As I understand it, AGW science suggests that the extra heat is stored in the deep oceans, without showing up in OHC measurements. How that is possible, I am sure I don’t know.
I think you are correct that the concept of “heat in the pipeline/stored heat” is a product of the GCM’s need to produce alarming scenarios of future warming, not a result of understanding physical processes. Since GCM’s cannot even handle effects of ENSO or other ocean oscillations, they are pretty useless in forecasting, as you say. Therefore, the concept of “heat in the pipeline/stored heat” and the “equilibrium response” resulting from this concept is only “settled science” in the AGW consensus community. Among rational people, it is no science at all.
Regards

September 26, 2009 7:15 am

H.R.: You replied, “Thanks for expanding (and a little rewording). I had read the text below Fig 23 and stopped. After your response I went back and found it helpful (to me, at least) to go right through from Fig 23 to 24 to 25.”
I’m glad it helped. I’ve gone back and revised that language at the version on my website. Thanks for pointing it out. I credited you for the find.
http://bobtisdale.blogspot.com/2009/09/thompson-et-al-2009-high-tech-wiggle.html
As you are aware, it’s difficult to edit your own work, because you read what you want it to say, not necessarily what it says. Thanks again.

Paul Vaughan
September 27, 2009 1:52 am

Adding my perspective on the exchange of Bob & H.R.:
http://www.sfu.ca/~plv/CumuSumPDO(76,88,98).png

Paul Vaughan
September 27, 2009 2:17 am
Paul Vaughan
September 28, 2009 12:28 pm

Bob has pointed out on his blog how Hadley used the 1998 El Nino as a convenient point at which to switch data sources:
http://bobtisdale.blogspot.com/2008/12/step-change-in-hadsst-data-after-199798.html
If you look here, you will discover that the wide 1940 El Nino has also been exploited:
Thompson, D.W.J.; Kennedy, J.J.; Wallace, J.M.; & Jones, P.D. (2008). A large discontinuity in the mid-twentieth century in observed global-mean surface temperature. Nature 453, 646-650. doi:10.1038/nature06982.
I think it’s time these authors pause to consider that the timing of human decisions is affected by weather/climate. Here’s another index showing a ~1945 turn:
http://www.sfu.ca/~plv/CumuSumALPI.png
Related: Some readers may find the arguments here ‘interesting’:
Bernaerts, A. (2007). Can the “Big Warming” at Spitsbergen from 1918 to 1940 be explained? PACON 2007 Proceedings 325-337.
http://www.arctic-heats-up.com/pdf/Submitted_conference_paper.pdf
What is causing what?
Here’s an excerpt from Sidorenkov (2005):
“… Our prediction methodology differs fundamentally from all the methodologies used by weather forecasters. It enables one to make weather forecasts with a daily discreteness for a 1 year period. About 75% of such forecasts proved to be correct.
We believe that this methodology can also be used to predict natural and social phenomena, such as seismicity, volcano eruptions, economic crises, epidemics, population explosions, political coups and even wars.”