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Seasonal and Diurnal CO2 Patterns at Diekirch, LU 2003 - 2005 |
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Francis Massen 1, Antoine Kies 2, Nico Harpes 3 and a group of students of the LCD+ 1 Physics Lab and meteoLCD, Lycée Classique de Diekirch, francis.,massen@education.lu |
pdf version 1.02 |
file: co2_patterns.html
History: version 1.0 02 Feb 2007
1.01 11 Feb 2007 correction of some spelling
faults and typing errors
1.02 24 Mar 2007 added addendum 7
Abstract:
The seasonal and diurnal variations of the CO2 mixing ratio measured at meteoLCD, Diekirch, LU from 2003 to 2005 are analysed for typical variation patterns and relationships with environmental parameters. For seasonal and long term mean CO2 levels, it can be shown that sunshine (duration and energy) plays a variable and minor role, whereas the daily amplitude of air temperature and CO2 variations correlate positively over the whole year as well for winter and summer months. Increased wind velocities always lower CO2 levels, whatever the wind direction may be. Storm "Franz" passing over Diekirch the 11th Jan.07 allowed to quantify this relationship by a simple mathematical model, which might be used to compute an asymptotic CO2 level close to the global mixing ratio. Diurnal variability (exceeding 100 ppm) shows up in 3 characteristic pattern due to different atmospheric mixing caused by wind speed disrupting ABL inversions.
Index:
| 1. | How is CO2 measured at meteoLCD? |
| 2. | Geographic location of meteoLCD |
| 3. | Seasonal variations of the CO2 mixing ratio: 3.1. mean and extreme levels 3.2. Relationship between CO2 mixing ratios, temperature and sunshine duration according to season 3.3. Relationship between mean CO2 parameters and mean wind velocity and direction |
| 4. | Diurnal variations: 4.1. The dual peak diurnal CO2 pattern 4.2. The single peak diurnal CO2 pattern 4.3. No peak days and average pattern 4.4. Can day-time biological fixing be detected? |
| 5, | Conclusion |
| 6. | References |
| 7. | Addendum A: A revised model for the relationship between CO2 and windspeed |
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1.
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The instrument is recalibrated about every 3 weeks using span and zero gas (or CO2-free dry air), a general overhaul done by Envitec SA four times a year. The span gas used is from Praxair: bottle concentration is 496 ppmV +/- 2%. The same bottle has been in use since 30 June 2003. Zero drift has been found to be practically inexistant and is in fact not a problem as the sensor is built to make regular zero autocalibrations at night-time. The span-factor varies from check to check and is changed as needed. Besides CO2 many other meteorological parameters and gases are measured at meteoLCD; see http://meteo.lcd.lu/structure/readme.html for details. In this paper, all major calculations are done using DADiSP and Statistica 7; missing data are not interpolated except for very few ones in a row. Impossible low CO2 levels (<330 ppm) are treated as missing data. There remain 52245 valid CO2 measurements for the 3 year period, which represents a fair data availability of 99.3%
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2. Geographic location of meteoLCD |
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3.1.
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The situation is usually quite different in urban areas where patterns are heavily influenced by anthropogenic emissions which often cause strong short-time variations, but less visible seasonal patterns over the year. Nasralla et al [2] found an annual amplitude in Kuwait City less than 1.5 ppm from the mean monthly concentrations, whereas Idso et al [4] report almost constant daily minima but strong seasonal variations for the daily maxima over one year. We will report the CO2 measurements from 2003 to 2005 taken at the meteoLCD
site. All measurements have been made by the same instrument, Many natural factors influence CO2 mixing ratios: some parameters as wind direction, night or early morning inversions and daily changes in atmosperic boundary layer (ABL) mixing have a typical short time influence; others like mean air temperature, overall sunshine duration and vegetation activity show up as seasonal factors. Fig.2 and fig.3 show the 2003 to 2005 sequence of monthly CO2 means, minima, maxima and the global monthly averages over the 3 years: the average for the 3 years is 405.6 ppm with a standard deviation of 8.9 ppm.
fig.2 Monthly mean CO2 levels; global mean is 405.6 +/- 8.9 ppm; left axis scale: 360 to 440 ppm
fig.3: Averages of the 2003 to 2005 monthly mean CO2 levels Fig. 2 shows that the yearly variations do not repeat in an identical manner even if the periods of low and high mixing rations usually extend over An autocorrelation computed on the daily means over the 3 years gives maxima peaks at 45, 91, 179 and 352 days, i.e. roughly 1.5, 3, 6 months and full year periods; whereas the full year cycle has to be expected, the other periods remain unexplained.
fig 4. Autocorrelation confirms long-time periodicities in daily mean CO2 pattern
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Table 1 shows the relevant correlations for the full year, the JF and JA months, the red ones being significative at p<0.05
table 1 For the full year comparison the highest positive correlation exists between daily CO2 amplitude ( amplitude = maximum - minimum readings) and the corresponding daily temperature amplitude: regardless of season all coefficients are positive and significant at p<0.05; the correlations are better during the summer season. The next figure 5 gives the corresponding graphs:
One would expect that mean CO2 concentrations and mean daily
temperature vary in opposite sense as higher (summer) temperatures
usually happen during days with maximum photosynthesis which lowers the CO2 mixing
ratios: actually the data show a clear negative correlation for the winter
months and surprisingly a clear high positive correlation for the summer season.
A computation of 18 linear regression slopes for every couple of months
gives essentially negative slopes for the months of November to February and
positive slopes for the remaining months (with only 2 exceptions): fig 6 gives
Idso et al. [4] report a negative slope for the regression between maximum daily
CO2 and minimum daily air temperature; the Diekirch data do Table 2 gives a mixed picture for the correlations between CO2 and sunshine:
the full year correlations are slightly negative, the winter JF and summer
table 2 Even if the daily mean CO2 and daily solar energy antiregress for the full
3 year period they do not, contrary to what one would expect, antiregress
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fig. 7: Histogram of wind direction; total sample size is 51516 (windspeed > 0).
Let us limit the main directions to the ranges [50°-120°] and [200°-270°] for the easterly and westerly winds; the statistics are the following:
table 3 The table shows that the higher the wind speed, the lower the CO2 level.
Actually, the highest wind speeds correpond to a maximum mixing of the
atmospheric boundary layer, and should be close to the global baseline CO2
mixing ratio. Fig. 8 gives the plot of CO2 versus wind speed, and points
fig. 9: CO2 and wind speed during storm "Franz"
The same model applied to the complete 2003-2005 data points gives a bad fit
(R=0.22). The modified model There are virtually no industries in the easterly direction, whereas the main potential emitters are located upwind to the west: nevertheless the corresponding mean CO2 levels are lower. This suggests that the higher levels especially noticeable during calm wind conditions are not caused by CO2 plumes from industrial emitters, but by slower wind speeds which do not mix up the boundary layer as well as the higher westerly winds do. When wind speeds are higher than 2 m/s the CO2 levels are similar, regardless the wind direction (with and without upwind factories); this confirms the hypothesis:
As a reminder: the overal mean CO2 level computed from the 52445 measurements is 405.1 +/- 28.7 ppm for the period 2003-2005; Mauna Loa's average mixing ratio is 376 ppm for the same period.
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Despite great variabilty in day to day CO2 levels, a few typical diurnal patterns can be found. As shown in the preceeding chapter, wind speed is a dominant cause in lowering CO2, and a stable atmosphere (often found at night and during morning hours) is an efficient trap of natural and anthropogenic CO2 emissions, . Three typical diurnal CO2 patterns can be found: dual peak, single peak and no peak
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4.1. The dual peak diurnal CO2 pattern |
Lets us first show in detail the situation from Saturday 8th toTuesday 11th July 2006. These 4 days are dry, with only one small rain-fall of 1.8mm during 30 minutes at Tuesday; the night wind speeds are low ( <0.5 m/s), but have daily maxima from 3 to 7 m/s; Monday is a blue sky day, all the others have intermittent moderate or heavy (Sunday) cloud cover, as shown by the variablitiy of the UVB and solar irradiance. All 3 nights display 2 peaks, the first at 00:00 and the second at 06:00 UTC; there is far less morning traffic during Sunday compared to Monday and Tuesday: NO peaks at 50 ug/m3 on Sunday and 60 ug/m3 on Monday.
The same pattern can sometimes be found when temperatures are colder or
freezing, as shown by fig. 14 for the 10th to 12th Dec. 2005 period; a double peak can be seen Saturday to
Sunday night, and a much more preeminent one from Sunday to Monday. The last peak coincides with a NO maximum,
sign of the Monday morning commuter traffic; the Monday CO2 peak exceeds the Sunday
peak by about 40 ppm. As soon as the air
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fig. 15: Alternating dual and single peak days 10 to 14 July 2005 Inspection shows that the double peak coincides with a small nocturnal dip in air temperature; if we magnify the graph of CO2 and wind velocity, it becomes clear that wind speed is the driver of the dual peak (and causes the small air temperature drop): a small rise of wind around midnight pushes down CO2 levels by disrupting the inversioon layer; low wind nights do not show this.
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A plot of these mean hourly CO2 levels versus wind speed suggests, similar to
figure 8, a baseline CO2 level of about 376 ppm: the applied model
fig. 19: 2003-2005 mean hourly CO2 versus wind speed, with asymptotic baseline level
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Even if the summer daytime wind speeds are lower, the corresponding CO2 levels are not higher, but also lower: this could be seen as a fingerprint of photosynthetic CO2 fixation. But the difference in winter/summer levels could also be caused by higher anthropogenic winter emissions from increased heating. As a consequence, it is difficult or impossible to detect a photosynthesis fingerprint unambiguously in the daytime CO2 signal.
Table 5 resumes some of the influences of environmental factors on CO2 pattern:
table 5
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[1] |
NOAA, Earth Systems Research Laboratory, Global Monitoring Division: http://www.cmdl.noaa.gov/ccgg/trends/ |
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| [2] | Nasrallah et al: Temporal Variations in Atmospheric CO2 Concentrations in Kuwat City. Elsevier, Environment Pollution, 2003, Vol 121 | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| [3] | meteoLCD data archive, 2005 data file (http:meteo.lcd.lu/data/2005_only.xls) | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| [4] | Idso et al: Seasonal and diurnal variations of near-surface atmospheric CO2 concentration within a residential sector of the urban CO2 dome of Phoenix, AZ, USA. Pergamon, Atmospheric Environment, 36 (2002) p.1655-1660 | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| [5] | Burns S.P et al: Measurements of
the Diurnal Cycle of Temperature, Humidity, Wind, and Carbon Dioxide in
a Subalpine Forest during the Carbon in the Mountain Experiment (CME04);
NCAR, Boulder, CO http://www.mmm.ucar.edu/people/burns/files/agf_blt06_110188.pdf |
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| [6] | Parazoo N.: Sources of Synoptic
CO2 Variability in North America; Powerpoint presentation, Colorado
State University, ChEAS June 5, 2006 http://cheas.psu.edu/meeting/2006/meetingtalks/cheas06talks/parazoo.ppt |
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| [7] | Ahrens, C.D.:Meteorology Today. 8th edition.Thomson, Brooks/Cole, 2007 | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| [8] | Henninger S. et al: Mobile
Measurements of Carbon Dioxide wihin the Urban Canopy Layer of Essen,
Germany. http://www.uni-duisburg-essen.de/imperia/md/content/geographie/klimatologie/henninger2004.pdf |
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All data files are available in the data archive of meteoLCD at http://meteo.lcd.lu/data/
+ The following LCD students from the
optional (baccalaureat year) course "CLIMATE" helped in preparing the
preliminary research and calculations:
Dirkse Anne, Fischer Eric, Glaesener Laurent, Gleis Paul, Kobs Daniel, Lavandier
Philippe, Meyer Julien, Miny Christian, Schmit Jonathan
(C) copyright meteoLCD
| 7.
Addendum A A revised relationship between CO2 and windspeed |
The rational function used in chapters 3.3 and 4.3
for fitting CO2
mixing ratios to wind speed may give a good asymptotical base level, but
it lacks a clear physical base and represents nothing more than a mathematical trick. Using
a physical sensible exponential
function of the type
CO2 = a +b*exp(-c*windspeed) [eq. 4] resolves this problem. The horizontal asymptote for infinite windspeeds
is the parameter a.
The cup anemometer has the best goodness of fit R: this might not be surprinsing if one considers the different mounting heights of the air inlet, cup- and ultrasonic anemometers: the cup anemometer is mounted 1.10m, the ultrasonic 2.05m above the air inlet (see fig.20). The higher mountings show up in different mean windspeeds over 2003-2005: 1.58 m/s (cup, lower) and 1.77 m/s (ultrasonic, higher).
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