Global Warming...New Report...and it ain't happy news

there really is no more to add to the utter demolition of the original IPCC boondoggle.

http://epw.senate.gov/public/index.cfm?FuseAction=Minority.Blogs&ContentRecord_id=f80a6386-802a-23ad-40c8-3c63dc2d02cb
As of December 20, 2007, more than 400 prominent scientists from more than two dozen countries have voiced significant objections to major aspects of the alleged UN IPCC "consensus" on man-made global warming.

393
Aerospace engineer and physicist Dr. Michael Griffin, the top administrator of NASA and former head of the Space Department at Johns Hopkins University's Applied Physics Laboratory, expressed man-made global warming skepticism in 2007. "To assume that [global warming] is a problem is to assume that the state of Earth's climate today is the optimal climate, the best climate that we could have or ever have had and that we need to take steps to make sure that it doesn't change," Griffin said in a May 31, 2007 interview on National Public Radio's (NPR) "Morning Edition." "I guess I would ask which human beings - where and when - are to be accorded the privilege of deciding that this particular climate that we have right here today, right now is the best climate for all other human beings. I think that's a rather arrogant position for people to take," Griffin explained. "I have no doubt that a trend of global warming exists. I am not sure that it is fair to say that it is a problem we must wrestle with," he added. (LINK)

The average temperature and average irradiance trends on the chart you posted end on 2005. Only the temperature and irradiance cycles go to 2010.

Why don't you show what happened to Temperature and Irradiance after 2005?

if you will look at your Hadcrut grtaphs you will notice that the average global temp (the black line) ends before 2010

Quote:

The average temperature and average irradiance trends on the chart you posted end on 2005. Only the temperature and irradiance cycles go to 2010.

Quote:

Why don't you show what happened to AVERAGE Temperature and AVERAGE Irradiance after 2005?

http://www.cru.uea.ac.uk/cru/data/temperature/hadcrut3gl.txt
1998 0.492 0.756 0.548 0.647 0.596 0.606 0.671 0.647 0.393 0.420 0.351 0.444 0.548

1999 0.370 0.552 0.294 0.315 0.233 0.263 0.270 0.236 0.267 0.228 0.210 0.327 0.297

2000 0.206 0.361 0.331 0.450 0.241 0.234 0.255 0.339 0.320 0.194 0.150 0.164 0.271

2001 0.324 0.286 0.487 0.430 0.390 0.413 0.453 0.506 0.404 0.378 0.506 0.321 0.408

2002 0.598 0.611 0.609 0.445 0.443 0.474 0.479 0.427 0.412 0.358 0.393 0.328 0.465

2003 0.525 0.441 0.425 0.417 0.437 0.442 0.455 0.525 0.520 0.566 0.428 0.523 0.475

2004 0.504 0.571 0.510 0.494 0.323 0.347 0.369 0.416 0.446 0.478 0.526 0.376 0.447

2005 0.461 0.380 0.499 0.534 0.481 0.512 0.536 0.509 0.513 0.508 0.483 0.370 0.482

2006 0.319 0.448 0.380 0.370 0.338 0.438 0.444 0.493 0.422 0.480 0.445 0.523 0.425

2007 0.610 0.509 0.438 0.472 0.373 0.384 0.407 0.364 0.412 0.367 0.269 0.215 0.402

2008 0.053 0.192 0.449 0.271 0.278 0.308 0.417 0.395 0.376 0.443 0.393 0.327 0.325

2009 0.387 0.374 0.374 0.417 0.407 0.508 0.515 0.554 0.465 0.433 0.457 0.433 0.444

2010 0.502 0.493 0.586 0.571 0.511 0.534 0.000 0.000 0.000 0.000 0.000 0.000 0.533

http://www.climate4you.com/Sun.htm#Recent%20solar%20irradiance
Solar activity

List of content

Recent visual sun

Recent sunspot activity

Recent solar irradiance

Sunspot activity since 1700

Solar irradiance and sunspot number

Solar irradiance reconstructed since 1610

Global temperature and sunspot number

Cosmic ray intensity and sunspot activity

Open Climate4you homepage





Recent visual sun



The Sun seen on July 29, 2010. Two sunspots are visible. Photo by courtesy of SOHO/MDI/spaceweather.com. Click here and here to read the latest about the present solar minimum.



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Recent sunspot activity



Daily observations of the number of sunspots since 1 January 1990 according to Solar Influences Data Analysis Center (SIDC). The thin line indicates the daily sunspot number, while the thick line indicates the running annual average. The recent low sunspot activity is clearly reflected in the recent low values for the total solar irradiance. Last day shown: 31 January 2010. Last diagram update: 27 February 2010.

Click here to download the entire annual sunspot number data series since 1818 from the Solar Influences Data Analysis Center (SIDC).

Click here to read about data smoothing.



In 1848 the Swiss astronomer Johann Rudolph Wolf introduced a daily measurement of sunspot number. His method, which is still used today, counts the total number of spots visible on the face of the sun and the number of groups into which they cluster, because neither quantity alone satisfactorily measures sunspot activity (NOAA's National Geophysical Data Center; NGDC) .

An observer computes a daily sunspot number by multiplying the number of groups he sees by ten and then adding this product to his total count of individual spots. Results, however, vary greatly, since the measurement strongly depends on observer interpretation and experience and on the stability of the Earth's atmosphere above the observing site. Moreover, the use of Earth as a platform from which to record these numbers contributes to their variability, too, because the sun rotates and the evolving spot groups are distributed unevenly across solar longitudes. To compensate for these limitations, each daily international number is computed as a weighted average of measurements made from a network of cooperating observatories. Today, much more sophisticated measurements of solar activity are made routinely, but none has the link with the past that sunspot numbers have (NOAA's National Geophysical Data Center; NGDC) .


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Recent solar irradiance



Total solar irradiance since 25 February 2003, according to the Laboratory of Atmospheric and Space Physics (LASP). These data are obtained using the SORCE Total Irradiance Monitor (TIM). The thin line indicates daily TSI values, while the thick line represents the running simple 183 day (c. 6 months) average. The measured values for the total solar irradiation (TSI) are somewhat lower than reported by most other TSI-measuring instruments, which typically report TSI values around 1366 W/m2. Click here to read about the background for this difference, or see the text paragraphs below this diagram. However, the recent low sunspot activity is clearly reflected in the TIM data provided by LASP. Last day shown: 22 July 2010. Last diagram update: 29 July 2010.

Click here to download the entire series of TSI data from the Laboratory of Atmospheric and Space Physics (LASP).

Click here to make use of an online data plot facility kindly made available by LASP.

Click here to read about data smoothing.




The SORCE Total Irradiance Monitor (TIM) measures the Total Solar Irradiance (TSI), a measure of the absolute intensity of solar radiation, integrated over the entire solar irradiance spectrum.

The TIM's measured value of TSI at 1 AU is lower than that reported by other TSI-measuring instruments; an upcoming solar minimum value of 1361 W/m2 is estimated from the above TIM data. This is due to unresolved differences between the various TSI instruments in operation. The TIM measures TSI values 4.7 W/m2 lower than the VIRGO and 5.1 W/m2 lower than ACRIM III.

This difference exceeds the ~0.1% stated uncertainties on both the ACRIM and VIRGO instruments. Differences between the various data sets are solely instrumental and will only be resolved by careful and detailed analyses of each instrument's uncertainty budget. LASP report only the TSI measurements from the TIM, and make no attempt to adjust these to other TSI data records.

The TIM TSI data available are based on fundamental ground calibrations done at CU/LASP, NIST, and NASA. On-orbit calibrations measure the effects of background thermal emission, instrument sensitivity changes, and electronic gain. The TIM TSI data products have been corrected for instrument sensitivity and degradation, background thermal emission, instrument position and velocity, and electronic gain. The TIM relies on several component-level calibrations, as no calibration source or detector is available with the level of accuracy desired for this instrument -- a level of accuracy nearly 10 times better than that previously attempted for space-based radiometry.



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Sunspot activity since 1700



Annual sunspot activity since 1700 according to the Solar Influences Data Analysis Center (SIDC). The blue line shows annual values, red line shows the running 11 yr average. Last year shown: 2009. Last diagram update: 8 January 2010.

Click here to download the entire annual sunspot number data series since 1700 from the Solar Influences Data Analysis Center (SIDC).

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Solar irradiance and sunspot number





Solar irradiance and sunspot number since January 1979 according to NOAA's National Geophysical Data Center; NGDC. The thin lines indicate the daily irradiance (red) and sunspot number (blue), while the thick lines indicate the running annual average for these two parametres. The total variation in solar irradiance is about 1.3 W/m2 during one sunspot cycle, as an order of magnitude.

Click here to download the composite series of irradiance data 1978-2003 (file name: composite_d25_07_0310a.dat).

Click here or here to download the entire series of daily NOAA NGDC and Solar Influences Data Analysis Center (SIDC) sunspot number since 1818, respectively.

Click here to read about data smoothing.



The number of sunspots correlates with the intensity of solar radiation over the period (since 1979) when satellite measurements of absolute radiative flux were available. Since sunspots are darker than the surrounding photosphere it might be expected that more sunspots would lead to less solar radiation and a decreased solar constant. However, the surrounding margins of sunspots are hotter than the average, and so are brighter; overall, more sunspots increase the sun's solar constant or brightness.

The variation caused by the sunspot cycle to solar output is relatively small, on the order of 0.1% of the solar constant (a peak-to-trough range of 1.3 W/m2 compared to 1366 W/m2 for the average solar constant). This number refers to the projected area of planet Earth, as seen from the Sun. However, the total surface area of the planet is four times the projected area, and the variation of 1.3 W/m2 therefore corresponds to about 0.325 W/m2 for the entire planet surface. This value might be compared with the IPCC 2007 estimate of 1.6 W/m2 for the total effect of all recognized climatic drivers 1750-2006, including release of greenhouse gasses from the burning of fossil fuels.

During the Maunder Minimum in the 17th Century (c.1650-1720) there were hardly any sunspots at all, and in all likelihood, the intensity of solar radiation was low. This event coincides with a documented period of maximum cooling within the Little Ice Age.

Irradiance is the radiometry term for the power of electromagnetic radiation at a surface, per unit area. Irradiance due to solar radiation is also called insolation. Total solar irradiance describes the radiant energy emitted by the sun over all wavelengths that falls each second on 1 square meter outside the earth's atmosphere, a quantity proportional to the "solar constant" observed earlier in this century. It measures the solar energy flux in Watts/square meter.



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Solar irradiance reconstructed since 1610



Solar irradiance since 1610 as reconstructed by Lean et al (1995) and Lean (2000). The thin line indicates the annual reconstructed solar irradiance, while the thick line shows the running 11 average. The values shown include a background component. See Lean (2000) for discussion of the amplitude of the background component. Last year included in the Lean (2000) analysis: 2000. The small green columns in the bottom panel indicate different kind of historical evidence for past climate change effects. Click on the green columns for more information on each of these events. Last diagram update: 24 April 2009.

Click here to download the data series of reconstructed solar irradiance 1610-2000.

Click here to read about data smoothing.



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Global temperature and sunspot number





Variation of global surface air temperature (HadCRUT3) and observed sunspot number (NOAA's National Geophysical Data Center; NGDC) since 1960. The global monthly average surface air temperature is a cooperative effort between the Hadley Centre for Climate Prediction and Research and the University of East Anglia's Climatic Research Unit (CRU), UK. The thin lines represent the monthly values, while the thick lines is the simple running 37 month average, nearly corresponding to a running 3 yr average. The variation in global temperature is about 0.2oC during one sunspot period, superimposed on the general increasing temperature trend during the period shown. The somewhat asymmetrical temperature 'bumps' around 1973 and 1998 are reflecting oceanographic El Niño effects. Last month incorporated: January 2010 (HadCRUT3) and January 2010 (NOAA). Last diagram update: 27 February 2010.

Click here to download the entire series of estimated HadCRUT3 global monthly surface air temperatures since January 1850.

Click here to download the entire series of monthly NOAA NGDC sunspot number since January 1749.

Click here to read about data smoothing.






Variation of global sea surface temperature (HadSST2) and observed sunspot number (NOAA's National Geophysical Data Center; NGDC) since 1960. The global monthly average sea surface temperature is estimated by University of East Anglia's Climatic Research Unit (CRU), UK. The HadSST2 data series are described by Ranier et al. (2006). Base period: 1961-1990. The thin lines in the diagram represent the monthly values, while the thick lines is the simple running 37 month average, nearly corresponding to a running 3 yr average. The variation in global sea surface temperature is 0.15 - 0.2oC during one sunspot period, superimposed on the general increasing temperature trend during the period shown. The somewhat asymmetrical temperature 'bumps' around 1973 and 1998 are reflecting oceanographic El Niño effects. Last month incorporated: January 2010 (HadSST2) and January 2010 (NOAA). Last diagram update: 27 February 2009.

Click here to download the entire HadSST2 temperature series since 1850.

Click here to download the entire series of monthly NOAA NGDC sunspot number since January 1749.

Click here to read about data smoothing.



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Cosmic ray intensity and sunspot activity





Variation of cosmic ray intensity and monthly sunspot activity since 1958 according to the Germany Cosmic Ray Monitor in Kiel (GCRM) and NOAA's National Geophysical Data Center (NGDC), respectively. High sunspot activity correlates with low cosmic ray intensity, and vice versa. Last month incorporated: August 2009 (GCRM) and October 2009 (NGDC). Last diagram update: 6 November 2009.

Click here to download the entire series of monthly GCRM cosmic ray counts since January 1958.

Click here to download the entire series of monthly NOAA NGDC sunspot number since January 1749.



Galactic cosmic rays (GCR) are energetic particles originating from space that impinge on Earth's atmosphere. Almost 90% of all the incoming cosmic ray particles are protons, about 9% are helium nuclei (alpha particles) and about 1% are electrons (beta minus particles). The term "ray" is a misnomer, as cosmic particles arrive individually, not in the form of a ray or beam of particles.

The flux of galactic cosmic rays varies inversely with the solar cycle. Svensmark and Friis-Christensen (1997) suggested that galactic cosmic rays enhance low cloud formation, explaining variations on the order of 3 percent global total cloud cover over a solar cycle. A 3 percent cloud cover change corresponds to a radiative net change of about 0.5 W/m2, which may be compared with the IPCC 2007 estimate of 1.6 W/m2 for the total effect of all recognized climatic drivers 1750-2006, including release of greenhouse gasses from the burning of fossil fuels. Click here to read more about clouds in general, and click here to read more about the climatic influence of clouds.



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ftp://ftp.cmdl.noaa.gov/ccg/co2/trends/co2_mm_mlo.txt
# --------------------------------------------------------------------
# USE OF NOAA ESRL DATA
#
# These data are made freely available to the public and the
# scientific community in the belief that their wide dissemination
# will lead to greater understanding and new scientific insights.
# The availability of these data does not constitute publication
# of the data. NOAA relies on the ethics and integrity of the user to
# assure that ESRL receives fair credit for their work. If the data
# are obtained for potential use in a publication or presentation,
# ESRL should be informed at the outset of the nature of this work.
# If the ESRL data are essential to the work, or if an important
# result or conclusion depends on the ESRL data, co-authorship
# may be appropriate. This should be discussed at an early stage in
# the work. Manuscripts using the ESRL data should be sent to ESRL
# for review before they are submitted for publication so we can
# insure that the quality and limitations of the data are accurately
# represented.
#
# Contact: Pieter Tans (303 497 6678; [email protected])
#
# File Creation: Fri Aug 6 17:36:06 2010
#
# RECIPROCITY
#
# Use of these data implies an agreement to reciprocate.
# Laboratories making similar measurements agree to make their
# own data available to the general public and to the scientific
# community in an equally complete and easily accessible form.
# Modelers are encouraged to make available to the community,
# upon request, their own tools used in the interpretation
# of the ESRL data, namely well documented model code, transport
# fields, and additional information necessary for other
# scientists to repeat the work and to run modified versions.
# Model availability includes collaborative support for new
# users of the models.
# --------------------------------------------------------------------
#
#
# See www.esrl.noaa.gov/gmd/ccgg/trends/ for additional details.
#
# Data from March 1958 through April 1974 have been obtained by C. David Keeling
# of the Scripps Institution of Oceanography (SIO) and were obtained from the
# Scripps website (scrippsco2.ucsd.edu).
#
# The "average" column contains the monthly mean CO2 mole fraction determined
# from daily averages. The mole fraction of CO2, expressed as parts per million
# (ppm) is the number of molecules of CO2 in every one million molecules of dried
# air (water vapor removed). If there are missing days concentrated either early
# or late in the month, the monthly mean is corrected to the middle of the month
# using the average seasonal cycle. Missing months are denoted by -99.99.
# The "interpolated" column includes average values from the preceding column
# and interpolated values where data are missing. Interpolated values are
# computed in two steps. First, we compute for each month the average seasonal
# cycle in a 5-year window around each monthly value. In this way the seasonal
# cycle is allowed to change slowly over time. We then determine the "trend"
# value for each month by removing the seasonal cycle; this result is shown in
# the "trend" column. Trend values are linearly interpolated for missing months.
# The interpolated monthly mean is then the sum of the average seasonal cycle
# value and the trend value for the missing month.
#
# NOTE: In general, the data presented for the last year are subject to change,
# depending on recalibration of the reference gas mixtures used, and other quality
# control procedures. Occasionally, earlier years may also be changed for the same
# reasons. Usually these changes are minor.
#
# (-99.99 missing data; -1 no data for #daily means in month)
#
# decimal average interpolated trend #days
# date (season corr)
1958 3 1958.208 315.71 315.71 314.69 -1
1958 4 1958.292 317.45 317.45 315.21 -1
1958 5 1958.375 317.50 317.50 314.77 -1
1958 6 1958.458 -99.99 317.11 314.87 -1
1958 7 1958.542 315.86 315.86 314.97 -1
1958 8 1958.625 314.93 314.93 315.99 -1
1958 9 1958.708 313.20 313.20 315.84 -1
1958 10 1958.792 -99.99 312.61 315.54 -1
1958 11 1958.875 313.33 313.33 315.25 -1
1958 12 1958.958 314.67 314.67 315.64 -1
1959 1 1959.042 315.62 315.62 315.70 -1
1959 2 1959.125 316.38 316.38 315.84 -1
1959 3 1959.208 316.71 316.71 315.69 -1
1959 4 1959.292 317.72 317.72 315.48 -1
1959 5 1959.375 318.29 318.29 315.56 -1
1959 6 1959.458 318.16 318.16 315.90 -1
1959 7 1959.542 316.55 316.55 315.66 -1
1959 8 1959.625 314.80 314.80 315.86 -1
1959 9 1959.708 313.84 313.84 316.48 -1
1959 10 1959.792 313.26 313.26 316.27 -1
1959 11 1959.875 314.80 314.80 316.72 -1
1959 12 1959.958 315.59 315.59 316.56 -1
1960 1 1960.042 316.43 316.43 316.51 -1
1960 2 1960.125 316.97 316.97 316.43 -1
1960 3 1960.208 317.58 317.58 316.56 -1
1960 4 1960.292 319.02 319.02 316.78 -1
1960 5 1960.375 320.02 320.02 317.29 -1
1960 6 1960.458 319.59 319.59 317.33 -1
1960 7 1960.542 318.18 318.18 317.29 -1
1960 8 1960.625 315.91 315.91 316.97 -1
1960 9 1960.708 314.16 314.16 316.80 -1
1960 10 1960.792 313.83 313.83 316.84 -1
1960 11 1960.875 315.00 315.00 316.92 -1
1960 12 1960.958 316.19 316.19 317.16 -1
1961 1 1961.042 316.93 316.93 317.01 -1
1961 2 1961.125 317.70 317.70 317.16 -1
1961 3 1961.208 318.54 318.54 317.52 -1
1961 4 1961.292 319.48 319.48 317.24 -1
1961 5 1961.375 320.58 320.58 317.85 -1
1961 6 1961.458 319.77 319.77 317.51 -1
1961 7 1961.542 318.58 318.58 317.69 -1
1961 8 1961.625 316.79 316.79 317.85 -1
1961 9 1961.708 314.80 314.80 317.44 -1
1961 10 1961.792 315.38 315.38 318.39 -1
1961 11 1961.875 316.10 316.10 318.02 -1
1961 12 1961.958 317.01 317.01 317.98 -1
1962 1 1962.042 317.94 317.94 318.02 -1
1962 2 1962.125 318.55 318.55 318.01 -1
1962 3 1962.208 319.68 319.68 318.66 -1
1962 4 1962.292 320.63 320.63 318.39 -1
1962 5 1962.375 321.01 321.01 318.28 -1
1962 6 1962.458 320.55 320.55 318.29 -1
1962 7 1962.542 319.58 319.58 318.69 -1
1962 8 1962.625 317.40 317.40 318.46 -1
1962 9 1962.708 316.26 316.26 318.90 -1
1962 10 1962.792 315.42 315.42 318.43 -1
1962 11 1962.875 316.69 316.69 318.61 -1
1962 12 1962.958 317.70 317.70 318.67 -1
1963 1 1963.042 318.74 318.74 318.89 -1
1963 2 1963.125 319.08 319.08 318.60 -1
1963 3 1963.208 319.86 319.86 318.72 -1
1963 4 1963.292 321.39 321.39 318.99 -1
1963 5 1963.375 322.24 322.24 319.39 -1
1963 6 1963.458 321.47 321.47 319.12 -1
1963 7 1963.542 319.74 319.74 318.87 -1
1963 8 1963.625 317.77 317.77 318.95 -1
1963 9 1963.708 316.21 316.21 318.98 -1
1963 10 1963.792 315.99 315.99 319.03 -1
1963 11 1963.875 317.12 317.12 319.06 -1
1963 12 1963.958 318.31 318.31 319.33 -1
1964 1 1964.042 319.57 319.57 319.67 -1
1964 2 1964.125 -99.99 320.11 319.62 -1
1964 3 1964.208 -99.99 320.76 319.56 -1
1964 4 1964.292 -99.99 321.79 319.51 -1
1964 5 1964.375 322.24 322.24 319.45 -1
1964 6 1964.458 321.89 321.89 319.66 -1
1964 7 1964.542 320.44 320.44 319.48 -1
1964 8 1964.625 318.70 318.70 319.82 -1
1964 9 1964.708 316.70 316.70 319.53 -1
1964 10 1964.792 316.79 316.79 319.87 -1
1964 11 1964.875 317.79 317.79 319.77 -1
1964 12 1964.958 318.71 318.71 319.68 -1
1965 1 1965.042 319.44 319.44 319.48 -1
1965 2 1965.125 320.44 320.44 319.92 -1
1965 3 1965.208 320.89 320.89 319.72 -1
1965 4 1965.292 322.13 322.13 319.72 -1
1965 5 1965.375 322.16 322.16 319.42 -1
1965 6 1965.458 321.87 321.87 319.63 -1
1965 7 1965.542 321.39 321.39 320.54 -1
1965 8 1965.625 318.80 318.80 319.97 -1
1965 9 1965.708 317.81 317.81 320.64 -1
1965 10 1965.792 317.30 317.30 320.37 -1
1965 11 1965.875 318.87 318.87 320.77 -1
1965 12 1965.958 319.42 319.42 320.34 -1
1966 1 1966.042 320.62 320.62 320.63 -1
1966 2 1966.125 321.59 321.59 321.05 -1
1966 3 1966.208 322.39 322.39 321.22 -1
1966 4 1966.292 323.87 323.87 321.43 -1
1966 5 1966.375 324.01 324.01 321.23 -1
1966 6 1966.458 323.75 323.75 321.48 -1
1966 7 1966.542 322.40 322.40 321.54 -1
1966 8 1966.625 320.37 320.37 321.57 -1
1966 9 1966.708 318.64 318.64 321.47 -1
1966 10 1966.792 318.10 318.10 321.26 -1
1966 11 1966.875 319.78 319.78 321.75 -1
1966 12 1966.958 321.08 321.08 321.97 -1
1967 1 1967.042 322.06 322.06 322.08 -1
1967 2 1967.125 322.50 322.50 321.91 -1
1967 3 1967.208 323.04 323.04 321.80 -1
1967 4 1967.292 324.42 324.42 321.99 -1
1967 5 1967.375 325.00 325.00 322.35 -1
1967 6 1967.458 324.09 324.09 321.92 -1
1967 7 1967.542 322.55 322.55 321.62 -1
1967 8 1967.625 320.92 320.92 322.08 -1
1967 9 1967.708 319.31 319.31 322.12 -1
1967 10 1967.792 319.31 319.31 322.45 -1
1967 11 1967.875 320.72 320.72 322.70 -1
1967 12 1967.958 321.96 321.96 322.85 -1
1968 1 1968.042 322.57 322.57 322.60 -1
1968 2 1968.125 323.15 323.15 322.57 -1
1968 3 1968.208 323.89 323.89 322.67 -1
1968 4 1968.292 325.02 325.02 322.73 -1
1968 5 1968.375 325.57 325.57 322.93 -1
1968 6 1968.458 325.36 325.36 323.24 -1
1968 7 1968.542 324.14 324.14 323.17 -1
1968 8 1968.625 322.03 322.03 323.15 -1
1968 9 1968.708 320.41 320.41 323.16 -1
1968 10 1968.792 320.25 320.25 323.33 -1
1968 11 1968.875 321.31 321.31 323.24 -1
1968 12 1968.958 322.84 322.84 323.73 -1
1969 1 1969.042 324.00 324.00 324.00 -1
1969 2 1969.125 324.42 324.42 323.83 -1
1969 3 1969.208 325.64 325.64 324.45 -1
1969 4 1969.292 326.66 326.66 324.29 -1
1969 5 1969.375 327.34 327.34 324.58 -1
1969 6 1969.458 326.76 326.76 324.61 -1
1969 7 1969.542 325.88 325.88 324.98 -1
1969 8 1969.625 323.67 323.67 324.83 -1
1969 9 1969.708 322.38 322.38 325.23 -1
1969 10 1969.792 321.78 321.78 324.90 -1
1969 11 1969.875 322.85 322.85 324.83 -1
1969 12 1969.958 324.12 324.12 324.97 -1
1970 1 1970.042 325.03 325.03 325.01 -1
1970 2 1970.125 325.99 325.99 325.38 -1
1970 3 1970.208 326.87 326.87 325.67 -1
1970 4 1970.292 328.14 328.14 325.81 -1
1970 5 1970.375 328.07 328.07 325.23 -1
1970 6 1970.458 327.66 327.66 325.47 -1
1970 7 1970.542 326.35 326.35 325.57 -1
1970 8 1970.625 324.69 324.69 325.86 -1
1970 9 1970.708 323.10 323.10 326.01 -1
1970 10 1970.792 323.16 323.16 326.27 -1
1970 11 1970.875 323.98 323.98 325.96 -1
1970 12 1970.958 325.13 325.13 325.92 -1
1971 1 1971.042 326.17 326.17 326.30 -1
1971 2 1971.125 326.68 326.68 326.09 -1
1971 3 1971.208 327.18 327.18 325.98 -1
1971 4 1971.292 327.78 327.78 325.49 -1
1971 5 1971.375 328.92 328.92 326.14 -1
1971 6 1971.458 328.57 328.57 326.46 -1
1971 7 1971.542 327.34 327.34 326.48 -1
1971 8 1971.625 325.46 325.46 326.52 -1
1971 9 1971.708 323.36 323.36 326.15 -1
1971 10 1971.792 323.56 323.56 326.55 -1
1971 11 1971.875 324.80 324.80 326.74 -1
1971 12 1971.958 326.01 326.01 326.92 -1
1972 1 1972.042 326.77 326.77 326.89 -1
1972 2 1972.125 327.63 327.63 327.01 -1
1972 3 1972.208 327.75 327.75 326.56 -1
1972 4 1972.292 329.72 329.72 327.39 -1
1972 5 1972.375 330.07 330.07 327.24 -1
1972 6 1972.458 329.09 329.09 326.97 -1
1972 7 1972.542 328.05 328.05 327.16 -1
1972 8 1972.625 326.32 326.32 327.36 -1
1972 9 1972.708 324.93 324.93 327.73 -1
1972 10 1972.792 325.06 325.06 328.07 -1
1972 11 1972.875 326.50 326.50 328.52 -1
1972 12 1972.958 327.55 327.55 328.53 -1
1973 1 1973.042 328.55 328.55 328.69 -1
1973 2 1973.125 329.56 329.56 328.89 -1
1973 3 1973.208 330.30 330.30 329.10 -1
1973 4 1973.292 331.50 331.50 329.14 -1
1973 5 1973.375 332.48 332.48 329.68 -1
1973 6 1973.458 332.07 332.07 330.03 -1
1973 7 1973.542 330.87 330.87 330.00 -1
1973 8 1973.625 329.31 329.31 330.38 -1
1973 9 1973.708 327.51 327.51 330.26 -1
1973 10 1973.792 327.18 327.18 330.19 -1
1973 11 1973.875 328.16 328.16 330.14 -1
1973 12 1973.958 328.64 328.64 329.63 -1
1974 1 1974.042 329.35 329.35 329.48 -1
1974 2 1974.125 330.71 330.71 330.08 -1
1974 3 1974.208 331.48 331.48 330.21 -1
1974 4 1974.292 332.65 332.65 330.24 -1
1974 5 1974.375 333.16 333.16 330.19 15
1974 6 1974.458 332.13 332.13 329.95 27
1974 7 1974.542 330.99 330.99 330.19 31
1974 8 1974.625 329.17 329.17 330.31 31
1974 9 1974.708 327.41 327.41 330.30 29
1974 10 1974.792 327.21 327.21 330.29 29
1974 11 1974.875 328.34 328.34 330.36 29
1974 12 1974.958 329.50 329.50 330.50 31
1975 1 1975.042 330.68 330.68 330.78 31
1975 2 1975.125 331.41 331.41 330.80 28
1975 3 1975.208 331.85 331.85 330.49 26
1975 4 1975.292 333.29 333.29 330.71 30
1975 5 1975.375 333.91 333.91 330.92 30
1975 6 1975.458 333.40 333.40 331.15 29
1975 7 1975.542 331.74 331.74 330.97 27
1975 8 1975.625 329.88 329.88 331.13 31
1975 9 1975.708 328.57 328.57 331.53 30
1975 10 1975.792 328.35 328.35 331.51 17
1975 11 1975.875 329.33 329.33 331.40 25
1975 12 1975.958 -99.99 330.55 331.56 1
1976 1 1976.042 331.66 331.66 331.73 25
1976 2 1976.125 332.75 332.75 332.15 29
1976 3 1976.208 333.46 333.46 331.94 29
1976 4 1976.292 334.78 334.78 332.18 25
1976 5 1976.375 334.79 334.79 331.85 31
1976 6 1976.458 334.05 334.05 331.67 25
1976 7 1976.542 332.95 332.95 332.20 21
1976 8 1976.625 330.64 330.64 331.93 31
1976 9 1976.708 328.96 328.96 331.97 28
1976 10 1976.792 328.77 328.77 331.97 30
1976 11 1976.875 330.18 330.18 332.28 26
1976 12 1976.958 331.65 331.65 332.75 24
1977 1 1977.042 332.69 332.69 332.76 29
1977 2 1977.125 333.23 333.23 332.69 26
1977 3 1977.208 334.97 334.97 333.41 29
1977 4 1977.292 336.03 336.03 333.43 29
1977 5 1977.375 336.82 336.82 333.97 30
1977 6 1977.458 336.10 336.10 333.76 25
1977 7 1977.542 334.79 334.79 333.95 28
1977 8 1977.625 332.53 332.53 333.75 30
1977 9 1977.708 331.19 331.19 334.20 27
1977 10 1977.792 331.21 331.21 334.38 30
1977 11 1977.875 332.35 332.35 334.51 28
1977 12 1977.958 333.47 333.47 334.55 31
1978 1 1978.042 335.09 335.09 335.10 26
1978 2 1978.125 335.26 335.26 334.69 28
1978 3 1978.208 336.62 336.62 334.99 30
1978 4 1978.292 337.77 337.77 335.15 28
1978 5 1978.375 338.00 338.00 335.15 30
1978 6 1978.458 337.98 337.98 335.59 27
1978 7 1978.542 336.48 336.48 335.69 31
1978 8 1978.625 334.37 334.37 335.70 31
1978 9 1978.708 332.33 332.33 335.41 24
1978 10 1978.792 332.40 332.40 335.62 31
1978 11 1978.875 333.76 333.76 335.95 28
1978 12 1978.958 334.83 334.83 335.86 31
1979 1 1979.042 336.21 336.21 336.22 31
1979 2 1979.125 336.64 336.64 336.05 27
1979 3 1979.208 338.13 338.13 336.40 29
1979 4 1979.292 338.96 338.96 336.29 24
1979 5 1979.375 339.02 339.02 336.16 20
1979 6 1979.458 339.20 339.20 336.82 30
1979 7 1979.542 337.60 337.60 336.84 29
1979 8 1979.625 335.56 335.56 336.97 29
1979 9 1979.708 333.93 333.93 337.08 26
1979 10 1979.792 334.12 334.12 337.34 28
1979 11 1979.875 335.26 335.26 337.44 30
1979 12 1979.958 336.78 336.78 337.78 24
1980 1 1980.042 337.80 337.80 337.83 30
1980 2 1980.125 338.28 338.28 337.75 28
1980 3 1980.208 340.04 340.04 338.30 31
1980 4 1980.292 340.86 340.86 338.18 30
1980 5 1980.375 341.47 341.47 338.44 31
1980 6 1980.458 341.26 341.26 338.72 30
1980 7 1980.542 339.34 339.34 338.59 26
1980 8 1980.625 337.45 337.45 338.90 24
1980 9 1980.708 336.10 336.10 339.36 26
1980 10 1980.792 336.05 336.05 339.35 29
1980 11 1980.875 337.21 337.21 339.42 27
1980 12 1980.958 338.29 338.29 339.30 27
1981 1 1981.042 339.36 339.36 339.35 31
1981 2 1981.125 340.51 340.51 339.93 28
1981 3 1981.208 341.57 341.57 339.91 31
1981 4 1981.292 342.56 342.56 339.93 30
1981 5 1981.375 343.01 343.01 340.03 31
1981 6 1981.458 342.52 342.52 340.02 28
1981 7 1981.542 340.71 340.71 339.95 30
1981 8 1981.625 338.51 338.51 339.94 30
1981 9 1981.708 336.96 336.96 340.20 30
1981 10 1981.792 337.13 337.13 340.41 31
1981 11 1981.875 338.58 338.58 340.74 30
1981 12 1981.958 339.91 339.91 340.91 28
1982 1 1982.042 340.92 340.92 340.98 30
1982 2 1982.125 341.69 341.69 341.08 27
1982 3 1982.208 342.87 342.87 341.15 21
1982 4 1982.292 343.83 343.83 341.23 9
1982 5 1982.375 344.30 344.30 341.29 31
1982 6 1982.458 343.42 343.42 340.96 29
1982 7 1982.542 341.85 341.85 341.08 30
1982 8 1982.625 339.82 339.82 341.24 26
1982 9 1982.708 337.98 337.98 341.28 26
1982 10 1982.792 338.09 338.09 341.39 30
1982 11 1982.875 339.24 339.24 341.39 28
1982 12 1982.958 340.67 340.67 341.61 31
1983 1 1983.042 341.42 341.42 341.51 31
1983 2 1983.125 342.67 342.67 342.09 27
1983 3 1983.208 343.45 343.45 341.82 31
1983 4 1983.292 345.08 345.08 342.46 26
1983 5 1983.375 345.76 345.76 342.59 29
1983 6 1983.458 345.32 345.32 342.85 25
1983 7 1983.542 343.93 343.93 343.23 30
1983 8 1983.625 342.08 342.08 343.55 28
1983 9 1983.708 340.00 340.00 343.26 27
1983 10 1983.792 340.12 340.12 343.43 31
1983 11 1983.875 341.35 341.35 343.49 29
1983 12 1983.958 342.89 342.89 343.79 26
1984 1 1984.042 343.87 343.87 343.94 31
1984 2 1984.125 344.59 344.59 344.00 29
1984 3 1984.208 345.29 345.29 343.77 23
1984 4 1984.292 -99.99 346.58 343.98 2
1984 5 1984.375 347.36 347.36 344.19 27
1984 6 1984.458 346.80 346.80 344.33 25
1984 7 1984.542 345.37 345.37 344.70 29
1984 8 1984.625 343.06 343.06 344.51 24
1984 9 1984.708 341.24 341.24 344.41 29
1984 10 1984.792 341.54 341.54 344.85 27
1984 11 1984.875 342.90 342.90 345.03 28
1984 12 1984.958 344.36 344.36 345.27 27
1985 1 1985.042 345.08 345.08 345.13 29
1985 2 1985.125 345.89 345.89 345.26 26
1985 3 1985.208 347.49 347.49 346.00 28
1985 4 1985.292 348.02 348.02 345.40 27
1985 5 1985.375 348.75 348.75 345.56 31
1985 6 1985.458 348.19 348.19 345.71 30
1985 7 1985.542 346.49 346.49 345.80 28
1985 8 1985.625 344.70 344.70 346.19 27
1985 9 1985.708 343.04 343.04 346.24 27
1985 10 1985.792 342.92 342.92 346.24 27
1985 11 1985.875 344.22 344.22 346.35 29
1985 12 1985.958 345.61 345.61 346.52 29
1986 1 1986.042 346.42 346.42 346.43 26
1986 2 1986.125 346.95 346.95 346.36 26
1986 3 1986.208 347.88 347.88 346.53 31
1986 4 1986.292 349.57 349.57 347.01 30
1986 5 1986.375 350.35 350.35 347.23 30
1986 6 1986.458 349.70 349.70 347.28 24
1986 7 1986.542 347.78 347.78 346.99 31
1986 8 1986.625 345.89 345.89 347.28 30
1986 9 1986.708 344.88 344.88 347.99 25
1986 10 1986.792 344.34 344.34 347.60 30
1986 11 1986.875 345.67 345.67 347.80 30
1986 12 1986.958 346.89 346.89 347.82 30
1987 1 1987.042 348.20 348.20 348.17 30
1987 2 1987.125 348.55 348.55 347.89 28
1987 3 1987.208 349.56 349.56 348.18 27
1987 4 1987.292 351.12 351.12 348.62 30
1987 5 1987.375 351.84 351.84 348.80 31
1987 6 1987.458 351.45 351.45 349.14 28
1987 7 1987.542 349.77 349.77 348.97 28
1987 8 1987.625 347.62 347.62 349.01 26
1987 9 1987.708 346.37 346.37 349.49 29
1987 10 1987.792 346.48 346.48 349.68 30
1987 11 1987.875 347.80 347.80 349.91 27
1987 12 1987.958 349.03 349.03 349.90 30
1988 1 1988.042 350.23 350.23 350.23 29
1988 2 1988.125 351.58 351.58 350.97 27
1988 3 1988.208 352.22 352.22 350.77 31
1988 4 1988.292 353.53 353.53 350.95 30
1988 5 1988.375 354.14 354.14 351.04 31
1988 6 1988.458 353.64 353.64 351.34 29
1988 7 1988.542 352.53 352.53 351.78 31
1988 8 1988.625 350.42 350.42 351.90 30
1988 9 1988.708 348.84 348.84 351.98 30
1988 10 1988.792 348.94 348.94 352.15 31
1988 11 1988.875 349.99 349.99 352.07 27
1988 12 1988.958 351.29 351.29 352.16 30
1989 1 1989.042 352.72 352.72 352.69 31
1989 2 1989.125 353.10 353.10 352.46 28
1989 3 1989.208 353.64 353.64 352.26 30
1989 4 1989.292 355.43 355.43 352.81 30
1989 5 1989.375 355.70 355.70 352.57 31
1989 6 1989.458 355.11 355.11 352.73 30
1989 7 1989.542 353.79 353.79 353.10 31
1989 8 1989.625 351.42 351.42 352.93 29
1989 9 1989.708 349.83 349.83 352.96 28
1989 10 1989.792 350.10 350.10 353.34 30
1989 11 1989.875 351.26 351.26 353.34 30
1989 12 1989.958 352.66 352.66 353.56 28
1990 1 1990.042 353.63 353.63 353.55 30
1990 2 1990.125 354.72 354.72 354.02 28
1990 3 1990.208 355.49 355.49 354.01 31
1990 4 1990.292 356.10 356.10 353.48 29
1990 5 1990.375 357.08 357.08 353.90 30
1990 6 1990.458 356.11 356.11 353.67 30
1990 7 1990.542 354.67 354.67 354.04 29
1990 8 1990.625 352.67 352.67 354.24 30
1990 9 1990.708 351.05 351.05 354.28 27
1990 10 1990.792 351.36 351.36 354.60 31
1990 11 1990.875 352.81 352.81 354.95 29
1990 12 1990.958 354.21 354.21 355.15 30
1991 1 1991.042 354.87 354.87 354.75 29
1991 2 1991.125 355.67 355.67 354.85 28
1991 3 1991.208 357.00 357.00 355.40 27
1991 4 1991.292 358.40 358.40 355.67 30
1991 5 1991.375 359.00 359.00 355.75 31
1991 6 1991.458 357.99 357.99 355.53 30
1991 7 1991.542 355.96 355.96 355.45 29
1991 8 1991.625 353.78 353.78 355.49 31
1991 9 1991.708 352.20 352.20 355.57 30
1991 10 1991.792 352.22 352.22 355.51 31
1991 11 1991.875 353.70 353.70 355.86 30
1991 12 1991.958 354.98 354.98 355.91 31
1992 1 1992.042 356.08 356.08 355.94 30
1992 2 1992.125 356.84 356.84 356.07 29
1992 3 1992.208 357.73 357.73 356.13 29
1992 4 1992.292 358.91 358.91 356.15 30
1992 5 1992.375 359.45 359.45 356.19 31
1992 6 1992.458 359.19 359.19 356.72 30
1992 7 1992.542 356.72 356.72 356.25 30
1992 8 1992.625 354.77 354.77 356.47 30
1992 9 1992.708 352.80 352.80 356.25 29
1992 10 1992.792 353.21 353.21 356.50 30
1992 11 1992.875 354.15 354.15 356.29 30
1992 12 1992.958 355.39 355.39 356.27 31
1993 1 1993.042 356.76 356.76 356.63 28
1993 2 1993.125 357.17 357.17 356.32 28
1993 3 1993.208 358.26 358.26 356.53 31
1993 4 1993.292 359.17 359.17 356.49 30
1993 5 1993.375 360.07 360.07 356.85 31
1993 6 1993.458 359.41 359.41 356.96 30
1993 7 1993.542 357.36 357.36 356.87 27
1993 8 1993.625 355.29 355.29 357.07 27
1993 9 1993.708 353.96 353.96 357.39 23
1993 10 1993.792 354.03 354.03 357.37 30
1993 11 1993.875 355.27 355.27 357.38 30
1993 12 1993.958 356.70 356.70 357.59 31
1994 1 1994.042 358.05 358.05 357.95 27
1994 2 1994.125 358.80 358.80 358.00 27
1994 3 1994.208 359.67 359.67 358.05 30
1994 4 1994.292 361.13 361.13 358.41 30
1994 5 1994.375 361.48 361.48 358.30 30
1994 6 1994.458 360.60 360.60 358.22 30
1994 7 1994.542 359.20 359.20 358.63 31
1994 8 1994.625 357.23 357.23 358.92 31
1994 9 1994.708 355.42 355.42 358.78 30
1994 10 1994.792 355.89 355.89 359.23 31
1994 11 1994.875 357.41 357.41 359.50 30
1994 12 1994.958 358.74 358.74 359.65 31
1995 1 1995.042 359.73 359.73 359.59 31
1995 2 1995.125 360.61 360.61 359.78 28
1995 3 1995.208 361.60 361.60 359.99 30
1995 4 1995.292 363.05 363.05 360.34 30
1995 5 1995.375 363.62 363.62 360.42 29
1995 6 1995.458 363.03 363.03 360.58 30
1995 7 1995.542 361.55 361.55 360.96 31
1995 8 1995.625 358.94 358.94 360.63 31
1995 9 1995.708 357.93 357.93 361.36 30
1995 10 1995.792 357.80 357.80 361.18 31
1995 11 1995.875 359.22 359.22 361.35 30
1995 12 1995.958 360.42 360.42 361.29 30
1996 1 1996.042 361.83 361.83 361.68 31
1996 2 1996.125 362.94 362.94 362.10 29
1996 3 1996.208 363.91 363.91 362.36 31
1996 4 1996.292 364.28 364.28 361.63 29
1996 5 1996.375 364.93 364.93 361.91 31
1996 6 1996.458 364.70 364.70 362.48 30
1996 7 1996.542 363.31 363.31 362.61 31
1996 8 1996.625 361.15 361.15 362.69 30
1996 9 1996.708 359.41 359.41 362.78 26
1996 10 1996.792 359.34 359.34 362.61 31
1996 11 1996.875 360.62 360.62 362.74 30
1996 12 1996.958 361.96 361.96 362.78 31
1997 1 1997.042 362.81 362.81 362.64 31
1997 2 1997.125 363.87 363.87 363.03 28
1997 3 1997.208 364.25 364.25 362.70 31
1997 4 1997.292 366.02 366.02 363.33 29
1997 5 1997.375 366.47 366.47 363.58 30
1997 6 1997.458 365.37 365.37 363.16 28
1997 7 1997.542 364.10 364.10 363.33 26
1997 8 1997.625 361.89 361.89 363.43 26
1997 9 1997.708 360.05 360.05 363.45 29
1997 10 1997.792 360.49 360.49 363.78 31
1997 11 1997.875 362.21 362.21 364.29 29
1997 12 1997.958 364.12 364.12 364.89 31
1998 1 1998.042 365.00 365.00 364.86 30
1998 2 1998.125 365.82 365.82 364.98 27
1998 3 1998.208 366.95 366.95 365.39 31
1998 4 1998.292 368.42 368.42 365.80 30
1998 5 1998.375 369.33 369.33 366.48 30
1998 6 1998.458 368.78 368.78 366.57 30
1998 7 1998.542 367.59 367.59 366.88 31
1998 8 1998.625 365.81 365.81 367.33 30
1998 9 1998.708 363.83 363.83 367.20 29
1998 10 1998.792 364.18 364.18 367.45 31
1998 11 1998.875 365.36 365.36 367.40 23
1998 12 1998.958 366.87 366.87 367.61 27
1999 1 1999.042 367.97 367.97 367.79 27
1999 2 1999.125 368.83 368.83 367.97 23
1999 3 1999.208 369.46 369.46 367.90 26
1999 4 1999.292 370.77 370.77 368.19 30
1999 5 1999.375 370.66 370.66 367.84 29
1999 6 1999.458 370.10 370.10 367.87 30
1999 7 1999.542 369.10 369.10 368.42 30
1999 8 1999.625 366.70 366.70 368.21 30
1999 9 1999.708 364.61 364.61 367.95 29
1999 10 1999.792 365.17 365.17 368.41 31
1999 11 1999.875 366.51 366.51 368.58 29
1999 12 1999.958 367.86 367.86 368.59 29
2000 1 2000.042 369.07 369.07 368.87 27
2000 2 2000.125 369.32 369.32 368.51 23
2000 3 2000.208 370.38 370.38 368.90 31
2000 4 2000.292 371.63 371.63 369.01 29
2000 5 2000.375 371.32 371.32 368.45 29
2000 6 2000.458 371.51 371.51 369.25 29
2000 7 2000.542 369.69 369.69 369.04 28
2000 8 2000.625 368.18 368.18 369.71 28
2000 9 2000.708 366.87 366.87 370.19 30
2000 10 2000.792 366.94 366.94 370.23 31
2000 11 2000.875 368.27 368.27 370.31 25
2000 12 2000.958 369.62 369.62 370.33 30
2001 1 2001.042 370.47 370.47 370.24 29
2001 2 2001.125 371.44 371.44 370.64 28
2001 3 2001.208 372.39 372.39 370.82 30
2001 4 2001.292 373.32 373.32 370.66 30
2001 5 2001.375 373.77 373.77 370.90 25
2001 6 2001.458 373.13 373.13 370.85 28
2001 7 2001.542 371.51 371.51 370.92 30
2001 8 2001.625 369.59 369.59 371.25 30
2001 9 2001.708 368.12 368.12 371.45 30
2001 10 2001.792 368.38 368.38 371.71 31
2001 11 2001.875 369.64 369.64 371.64 27
2001 12 2001.958 371.11 371.11 371.83 31
2002 1 2002.042 372.38 372.38 372.18 29
2002 2 2002.125 373.08 373.08 372.24 27
2002 3 2002.208 373.87 373.87 372.26 27
2002 4 2002.292 374.93 374.93 372.25 30
2002 5 2002.375 375.58 375.58 372.79 31
2002 6 2002.458 375.44 375.44 373.21 30
2002 7 2002.542 373.91 373.91 373.40 29
2002 8 2002.625 371.77 371.77 373.36 31
2002 9 2002.708 370.72 370.72 374.02 28
2002 10 2002.792 370.50 370.50 373.77 31
2002 11 2002.875 372.19 372.19 374.16 30
2002 12 2002.958 373.71 373.71 374.45 30
2003 1 2003.042 374.92 374.92 374.72 31
2003 2 2003.125 375.63 375.63 374.81 27
2003 3 2003.208 376.51 376.51 374.95 31
2003 4 2003.292 377.75 377.75 375.04 27
2003 5 2003.375 378.54 378.54 375.67 31
2003 6 2003.458 378.21 378.21 375.96 29
2003 7 2003.542 376.65 376.65 376.11 30
2003 8 2003.625 374.28 374.28 375.85 26
2003 9 2003.708 373.12 373.12 376.44 27
2003 10 2003.792 373.10 373.10 376.39 31
2003 11 2003.875 374.67 374.67 376.70 26
2003 12 2003.958 375.97 375.97 376.71 30
2004 1 2004.042 377.03 377.03 376.87 31
2004 2 2004.125 377.87 377.87 377.00 29
2004 3 2004.208 378.88 378.88 377.34 30
2004 4 2004.292 380.42 380.42 377.63 30
2004 5 2004.375 380.62 380.62 377.60 28
2004 6 2004.458 379.66 379.66 377.36 26
2004 7 2004.542 377.48 377.48 377.07 28
2004 8 2004.625 376.07 376.07 377.69 20
2004 9 2004.708 374.10 374.10 377.41 17
2004 10 2004.792 374.47 374.47 377.78 31
2004 11 2004.875 376.15 376.15 378.24 30
2004 12 2004.958 377.51 377.51 378.25 31
2005 1 2005.042 378.43 378.43 378.18 31
2005 2 2005.125 379.70 379.70 378.83 28
2005 3 2005.208 380.91 380.91 379.47 30
2005 4 2005.292 382.20 382.20 379.45 29
2005 5 2005.375 382.45 382.45 379.35 31
2005 6 2005.458 382.14 382.14 379.76 30
2005 7 2005.542 380.60 380.60 380.12 31
2005 8 2005.625 378.60 378.60 380.30 30
2005 9 2005.708 376.72 376.72 380.06 29
2005 10 2005.792 376.98 376.98 380.32 15
2005 11 2005.875 378.29 378.29 380.41 25
2005 12 2005.958 380.07 380.07 380.83 30
2006 1 2006.042 381.36 381.36 381.17 26
2006 2 2006.125 382.19 382.19 381.31 25
2006 3 2006.208 382.65 382.65 381.06 30
2006 4 2006.292 384.65 384.65 381.81 27
2006 5 2006.375 384.94 384.94 381.75 31
2006 6 2006.458 384.01 384.01 381.64 30
2006 7 2006.542 382.15 382.15 381.70 29
2006 8 2006.625 380.33 380.33 382.10 28
2006 9 2006.708 378.81 378.81 382.11 30
2006 10 2006.792 379.06 379.06 382.48 26
2006 11 2006.875 380.17 380.17 382.32 30
2006 12 2006.958 381.85 381.85 382.70 31
2007 1 2007.042 382.88 382.88 382.68 23
2007 2 2007.125 383.77 383.77 382.90 21
2007 3 2007.208 384.42 384.42 382.83 29
2007 4 2007.292 386.36 386.36 383.54 27
2007 5 2007.375 386.53 386.53 383.33 30
2007 6 2007.458 386.01 386.01 383.65 30
2007 7 2007.542 384.45 384.45 383.99 31
2007 8 2007.625 381.96 381.96 383.74 30
2007 9 2007.708 380.81 380.81 384.10 26
2007 10 2007.792 381.09 381.09 384.52 30
2007 11 2007.875 382.37 382.37 384.52 30
2007 12 2007.958 383.84 383.84 384.70 28
2008 1 2008.042 385.42 385.42 385.22 30
2008 2 2008.125 385.72 385.72 384.86 28
2008 3 2008.208 385.96 385.96 384.36 30
2008 4 2008.292 387.18 387.18 384.36 28
2008 5 2008.375 388.50 388.50 385.29 26
2008 6 2008.458 387.88 387.88 385.53 24
2008 7 2008.542 386.38 386.38 385.92 10
2008 8 2008.625 384.15 384.15 385.94 26
2008 9 2008.708 383.07 383.07 386.35 30
2008 10 2008.792 382.98 382.98 386.42 24
2008 11 2008.875 384.11 384.11 386.25 29
2008 12 2008.958 385.54 385.54 386.41 30
2009 1 2009.042 386.92 386.92 386.70 31
2009 2 2009.125 387.41 387.41 386.57 28
2009 3 2009.208 388.77 388.77 387.16 30
2009 4 2009.292 389.46 389.46 386.65 28
2009 5 2009.375 390.18 390.18 386.96 31
2009 6 2009.458 389.43 389.43 387.09 29
2009 7 2009.542 387.74 387.74 387.27 31
2009 8 2009.625 385.91 385.91 387.71 30
2009 9 2009.708 384.77 384.77 388.04 27
2009 10 2009.792 384.38 384.38 387.83 31
2009 11 2009.875 385.99 385.99 388.12 30
2009 12 2009.958 387.27 387.27 388.14 21
2010 1 2010.042 388.45 388.45 388.22 28
2010 2 2010.125 389.85 389.85 389.02 23
2010 3 2010.208 391.10 391.10 389.48 29
2010 4 2010.292 392.46 392.46 389.66 28
2010 5 2010.375 392.94 392.94 389.71 30
2010 6 2010.458 392.04 392.04 389.71 29
2010 7 2010.542 390.09 390.09 389.60 31