Image Credit: WoodForTrees.org

Guest Post By Werner Brozek, Edited By Just The Facts, Update/Additional Explanatory Commentary from Nick Stokes

UPDATE: RSS for October has just come out and the value was 0.207. As a result, RSS has now reached the 204 month or 17 year mark. The slope over the last 17 years is -0.000122111 per year.
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The graphic above shows 5 lines. The long horizontal line shows that RSS is flat since November 1996 to September 2013, which is a period of 16 years and 11 months or 203 months. All three programs are unanimous on this point. The two lines that are sloped up and down and which are closer together include the error bars based on Nick Stokes’ Temperature Trend Viewer page. The two lines that are sloped up and down and which are further apart include the error bars based on SkS’s Temperature Trend Calculator. Nick Stokes’ program provides much tighter error bars and therefore his times for a 95% significance are less than that of SkS. In my previous post on August 25, I said: On six different data sets, there has been no statistically significant warming for between 18 and 23 years. That statement was based on the trend from the SkS page. However based on the trend from Nick Stokes’ page, there has been no statistically significant warming for between 16 and 20 years on several different data sets. In this post, I have used Nick Stokes’ numbers in section 2 as well as row 8 of the table below. Please let us know what you think of this change. I have asked that Nick Stokes join this thread to answer any questions pertaining to the different methods of calculating 95% significance and defend his chosen method. Nick’s trend methodology/page offers the numbers for Hadsst3 so I have also switched from Hadsst2 to Hadsst3. WFT offers numbers for Hadcrut3 but I can no longer offer error bars for that set since Nick’s program only does Hadcrut4.

In the future, I am not interested in using the trend methodology/page that offers the longest times. I am not interested in using trend methodology/page that offers the shortest times. And I am not interested in using trend methodology/page that offers the highest consensus. What I am interested in is using the trend methodology/page that offers that is the most accurate representation of Earth’s temperature trend. I thought it was SkS, but I may have been wrong. Please let us know in comments if you think that SkS or Nick Stokes’s methodology/page is more accurate, and if you can offer a more accurate one, please let us know that too.

According to NOAA’s State of the Climate In 2008 report:

The simulations rule out (at the 95% level) zero trends for intervals of 15 yr or more, suggesting that an observed absence of warming of this duration is needed to create a discrepancy with the expected present-day warming rate.

In this 2011 paper “Separating signal and noise in atmospheric temperature changes: The importance of timescale” Santer et al. found that:

Because of the pronounced effect of interannual noise on decadal trends, a multi-model ensemble of anthropogenically-forced simulations displays many 10-year periods with little warming. A single decade of observational TLT data is therefore inadequate for identifying a slowly evolving anthropogenic warming signal. Our results show that temperature records of at least 17 years in length are required for identifying human effects on global-mean tropospheric temperature.

In 2010 Phil Jones was asked by the BBC, “Do you agree that from 1995 to the present there has been no statistically-significant global warming?”, Phil Jones replied:

Yes, but only just. I also calculated the trend for the period 1995 to 2009. This trend (0.12C per decade) is positive, but not significant at the 95% significance level. The positive trend is quite close to the significance level. Achieving statistical significance in scientific terms is much more likely for longer periods, and much less likely for shorter periods.

I’ll leave it to you to draw your own conclusions based upon the data below.

Note: If you read my recent article RSS Flat For 200 Months (Now Includes July Data) and just wish to know what is new with the August and September data, you will find the most important new information from lines 7 to the end of the table. And as mentioned above, all lines for Hadsst3 are new.

In the sections below, we will present you with the latest facts. The information will be presented in three sections and an appendix. The first section will show for how long there has been no warming on several data sets. The second section will show for how long there has been no statistically significant warming on several data sets. The third section will show how 2013 to date compares with 2012 and the warmest years and months on record so far. The appendix will illustrate sections 1 and 2 in a different way. Graphs and a table will be used to illustrate the data.

Section 1

This analysis uses the latest month for which data is available on WoodForTrees.com (WFT). All of the data on WFT is also available at the specific sources as outlined below. We start with the present date and go to the furthest month in the past where the slope is a least slightly negative. So if the slope from September is 4 x 10^-4 but it is – 4 x 10^-4 from October, we give the time from October so no one can accuse us of being less than honest if we say the slope is flat from a certain month.
On all data sets below, the different times for a slope that is at least very slightly negative ranges from 8 years and 9 months to 16 years and 11 months.

1. For GISS, the slope is flat since September 1, 2001 or 12 years, 1 month. (goes to September 30, 2013)
2. For Hadcrut3, the slope is flat since May 1997 or 16 years, 5 months. (goes to September)
3. For a combination of GISS, Hadcrut3, UAH and RSS, the slope is flat since December 2000 or 12 years, 10 months. (goes to September)
4. For Hadcrut4, the slope is flat since December 2000 or 12 years, 10 months. (goes to September)
5. For Hadsst3, the slope is flat since November 2000 or 12 years, 11 months. (goes to September)
6. For UAH, the slope is flat since January 2005 or 8 years, 9 months. (goes to September using version 5.5)
7. For RSS, the slope is flat since November 1996 or 17 years (goes to October)
RSS is 203/204 or 99.5% of the way to Ben Santer’s 17 years.
The next link shows just the lines to illustrate the above for what can be shown. Think of it as a sideways bar graph where the lengths of the lines indicate the relative times where the slope is 0. In addition, the sloped wiggly line shows how CO2 has increased over this period.

When two things are plotted as I have done, the left only shows a temperature anomaly.

The actual numbers are meaningless since all slopes are essentially zero and the position of each line is merely a reflection of the base period from which anomalies are taken for each set. No numbers are given for CO2. Some have asked that the log of the concentration of CO2 be plotted. However WFT does not give this option. The upward sloping CO2 line only shows that while CO2 has been going up over the last 17 years, the temperatures have been flat for varying periods on various data sets.

The next graph shows the above, but this time, the actual plotted points are shown along with the slope lines and the CO2 is omitted:

Section 2

For this analysis, data was retrieved from Nick Stokes moyhu.blogspot.com. This analysis indicates for how long there has not been statistically significant warming according to Nick’s criteria. Data go to their latest update for each set. In every case, note that the lower error bar is negative so a slope of 0 cannot be ruled out from the month indicated.

On several different data sets, there has been no statistically significant warming for between 16 and 20 years.

The details for several sets are below.

For UAH: Since November 1995: CI from -0.001 to 2.501
For RSS: Since December 1992: CI from -0.005 to 1.968
For Hadcrut4: Since August 1996: CI from -0.006 to 1.358
For Hadsst3: Since May 1993: CI from -0.002 to 1.768
For GISS: Since August 1997: CI from -0.030 to 1.326

Section 3

This section shows data about 2013 and other information in the form of a table. The table shows the six data sources along the top and other places so they should be visible at all times. The sources are UAH, RSS, Hadcrut4, Hadcrut3, Hadsst3, and GISS. Down the column, are the following:
1. 12ra: This is the final ranking for 2012 on each data set.
2. 12a: Here I give the average anomaly for 2012.
3. year: This indicates the warmest year on record so far for that particular data set. Note that two of the data sets have 2010 as the warmest year and four have 1998 as the warmest year.
4. ano: This is the average of the monthly anomalies of the warmest year just above.
5. mon: This is the month where that particular data set showed the highest anomaly. The months are identified by the first three letters of the month and the last two numbers of the year.
6. ano: This is the anomaly of the month just above.
7. y/m: This is the longest period of time where the slope is not positive given in years/months. So 16/2 means that for 16 years and 2 months the slope is essentially 0.
8. sig: This the first month for which warming is not statistically significant according to Nick’s criteria. The first three letters of the month is followed by the last two numbers of the year.
9. Jan: This is the January, 2013, anomaly for that particular data set.
10. Feb: This is the February, 2013, anomaly for that particular data set, etc.
21. ave: This is the average anomaly of all months to date taken by adding all numbers and dividing by the number of months. However if the data set itself gives that average, I may use their number. Sometimes the number in the third decimal place differs by one, presumably due to all months not having the same number of days.
22. rnk: This is the rank that each particular data set would have if the anomaly above were to remain that way for the rest of the year. It may not, but think of it as an update 45 minutes into a game. Due to different base periods, the rank is more meaningful than the average anomaly.

Source	UAH	RSS	Had4	Had3	Sst3	GISS
1. 12ra	9th	11th	9th	10th	9th	9th
2. 12a	0.161	0.192	0.448	0.406	0.346	0.58
3. year	1998	1998	2010	1998	1998	2010
4. ano	0.419	0.55	0.547	0.548	0.416	0.67
5. mon	Apr98	Apr98	Jan07	Feb98	Jul98	Jan07
6. ano	0.66	0.857	0.829	0.756	0.526	0.94
7. y/m	8/9	16/11	12/10	16/5	12/11	12/1
8. sig	Nov95	Dec92	Aug96		May93	Aug97
Source	UAH	RSS	Had4	Had3	Sst3	GISS
9. Jan	0.504	0.440	0.450	0.390	0.292	0.63
10.Feb	0.175	0.194	0.479	0.424	0.309	0.51
11.Mar	0.183	0.204	0.405	0.384	0.287	0.60
12.Apr	0.103	0.218	0.427	0.400	0.364	0.48
13.May	0.077	0.139	0.498	0.472	0.382	0.57
14.Jun	0.269	0.291	0.457	0.426	0.314	0.61
15.Jul	0.118	0.222	0.514	0.488	0.479	0.54
16.Aug	0.122	0.167	0.527	0.491	0.483	0.61
17.Sep	0.297	0.257	0.534	0.516	0.455	0.74
Source	UAH	RSS	Had4	Had3	Sst3	GISS
21.ave	0.205	0.237	0.474	0.444	0.374	0.588
22.rnk	6th	8th	9th	7th	6th	9th

If you wish to verify all of the latest anomalies, go to the following links, For UAH, version 5.5 was used since that is what WFT used, RSS, Hadcrut4, Hadcrut3, Hadsst3,and GISS

To see all points since January 2013 in the form of a graph, see the WFT graph below:

Appendix

In this section, we summarize data for each set separately.

RSS

The slope is flat since November 1996 or 16 years and 11 months. (goes to September) RSS is 203/204 or 99.5% of the way to Ben Santer’s 17 years.
For RSS: There is no statistically significant warming since December 1992: CI from -0.005 to 1.968
The RSS average anomaly so far for 2013 is 0.237. This would rank 8th if it stayed this way. 1998 was the warmest at 0.55. The highest ever monthly anomaly was in April of 1998 when it reached 0.857. The anomaly in 2012 was 0.192 and it came in 11th.

UAH

The slope is flat since January 2005 or 8 years, 9 months. (goes to September using version 5.5)
For UAH: There is no statistically significant warming since November 1995: CI from -0.001 to 2.501
The UAH average anomaly so far for 2013 is 0.205. This would rank 6th if it stayed this way. 1998 was the warmest at 0.419. The highest ever monthly anomaly was in April of 1998 when it reached 0.66. The anomaly in 2012 was 0.161 and it came in 9th.

Hadcrut4

The slope is flat since December 2000 or 12 years, 10 months. (goes to September)
For HadCRUT4: There is no statistically significant warming since August 1996: CI from -0.006 to 1.358
The Hadcrut4 average anomaly so far for 2013 is 0.474. This would rank 9th if it stayed this way. 2010 was the warmest at 0.547. The highest ever monthly anomaly was in January of 2007 when it reached 0.829. The anomaly in 2012 was 0.448 and it came in 9th.

Hadcrut3

The slope is flat since May 1997 or 16 years, 5 months (goes to September, 2013)
The Hadcrut3 average anomaly so far for 2013 is 0.444. This would rank 7th if it stayed this way. 1998 was the warmest at 0.548. The highest ever monthly anomaly was in February of 1998 when it reached 0.756. One has to go back to the 1940s to find the previous time that a Hadcrut3 record was not beaten in 10 years or less. The anomaly in 2012 was 0.406 and it came in 10th.

Hadsst3

For Hadsst3, the slope is flat since November 2000 or 12 years, 11 months. (goes to September, 2013).
For Hadsst3: There is no statistically significant warming since May 1993: CI from -0.002 to 1.768
The Hadsst3 average anomaly so far for 2013 is 0.374. This would rank 6th if it stayed this way. 1998 was the warmest at 0.416. The highest ever monthly anomaly was in July of 1998 when it reached 0.526. The anomaly in 2012 was 0.346 and it came in 9th.

GISS

The slope is flat since September 1, 2001 or 12 years, 1 month. (goes to September 30, 2013)
For GISS: There is no statistically significant warming since August 1997: CI from -0.030 to 1.326
The GISS average anomaly so far for 2013 is 0.588. This would rank 9th if it stayed this way. 2010 was the warmest at 0.67. The highest ever monthly anomaly was in January of 2007 when it reached 0.94. The anomaly in 2012 was 0.58 and it came in 9th.

Conclusion

It appears as if we can accurately say from what point in time the slope is zero or any other value. However the period where warming is statistically significant seems to be more of a challenge. Different programs give different results. However what I found really surprising was that according to Nick’s program, GISS shows significant warming at over 95% for the months of November 1996 to July 1997 inclusive. However during those nine months, the slope for RSS is not even positive! Can we trust both data sets?

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Update: Additional Explanatory Commentary from Nick Stokes

Trends and errors:
A trend coefficient is just a weighted average of a time series, which describes the rate of increase. You can calculate it without any particular statistical model in mind.

If you want to quantify the uncertainty you have about it, you need to be clear what kind of variations you have in mind. You might want to describe the uncertainty of actual measurement. You might want to quantify the spatial variability. Or you might want to say how typical that trend is given time variability. In other words, what if the weather had been different?

It’s that last variability that we’re talking about here, and we need a model for the variation. In all kinds of time series analysis, ARIMA models are a staple. No-one seriously believes that their data really is a linear trend with AR(1) fluctuations, or whatever, but you try to get the nearest fitting model to estimate the trend uncertainty.

In my trend viewer, I used AR(1). It’s conventional, because it allows for autocorrelating based on a single delay coefficient, and there is a widely used approximation (Quenouille). I’ve described here how you can plot the autocorrelation function to show what is being fitted. The uncertainty of the trend is proportional to the area under the fitted ACF. Foster and Rahmstorf argued, reasonably, that the AR(1) underfits, and a ARMA(1,1) approx does better. Here is an example from my post. SkS uses that approach, following F&R.

You can see from the ACF that it’s really more complicated, The real ACF does not taper exponentially – it oscillates, with a period of about 4 years – likely ENSO related. Some of that effect reaches back near zero, where the ARIMA fitting is done. If it is taken out, the peak would be more slender that AR(1). But there is uncertainty with ENSO too.

So the message is, trend uncertainty is complicated.