Krzysztof Olendrzynski EMEP/MSC
Transcription
Krzysztof Olendrzynski EMEP/MSC
EMEP /MSC-W Date: Note 4/99 July 1999 DET NORSKE METEOROLOGISKE INSTITUTT Norwegian Meteorological Institute Research Note no. 29 Operational EMEP Eulerian Acid Deposition Model Krzysztof Olendrzynski EMEP/MSC-W 1999 ISSN 0332-9879 -1- CONTENTS Preface and Acknowledgements...................................................................... 3 Introduction ..................................................................................................... 4 1. Recent updates to the model ......................................................................... 4 1.1 Extension of the model domain ......................................................... 5 1.2 PARLAM-PS meteorology ............................................................... 5 1.3 Modifications in the code .................................................................. 6 1.4 New countries in the budget and source-receptor computations ....... 7 2. Measurement database for 1997 .................................................................. 8 3. Annual scatter plots for 1997 ..................................................................... 11 3.1 Concentrations in air ........................................................................ 11 3.2 Concentrations in precipitation ........................................................ 14 3.3 Wet depositions ............................................................................... 18 4. Comparison of computed and measured daily time series in 1997 ............ 21 5. Maps of computed concentration and deposition fields for 1997 ............. 28 Conclusions ................................................................................................... 33 References ..................................................................................................... 35 -2- Preface This report was prepared for the twenty third session of the Steering Body of EMEP (Co-operative Programme for Monitoring and Evaluation of the Long Range Transmission of Air Pollutants in Europe). EMEP is one of the scientific programs of the UN Convention on Longrange Transboundary Air Pollution (LRTAP Convention). The main objective of this report is to present the status of the development of the EMEP Eulerian Acid Deposition model, which is run operationally for the first time this year. The report provides a detailed description of the model performance with regard to 1997 meteorological and measurement data. The application of the model with regard to source-receptor matrix computations and country budgets is described in Bartnicki (1999, EMEP/MSC-W Note 5/99). Acknowledgements The author would like to acknowledge his current and former colleagues from the EMEP modelling group at MSC-W who helped in preparation of this report through numerous discussions on the model, its implementation and its post-processing tools. In particular I would like to thank: Jan-Eiof Jonson, Erik Berge, Hugo Jakobsen, and Jerzy Bartnicki. I would also like to thank Egil Stoeren for his valuable contributions in various parts of this work, and Leonor Tarrason for reviewing the manuscript and inspiring comments. The work would not be completed without support from: the DNMI’s meteorological section, CCC/NILU, and staff of the computer department at the Technical University in Trondheim, on which CRAY T3E computer, the model has been developed and run operationally. -3- Introduction The main objective of Meteorological Synthesizing Centre - West (MSC-W) of the EMEP Programme is computation of atmospheric transboundary transport and deposition of air pollutants (sulfur, nitrogen compounds and tropospheric ozone) in Europe. The computations of annual concentration and deposition fields, as well as country-to-grid matrices for acidifying species, have been performed routinely for 20 and 13 years respectively for sulfur and nitrogen compounds. Two-dimensional (2-D) Lagrangian model (Eliassen and Saltbones, 1983; Barret and Berge, 1996) had been successfully used for routine computations up till 1998. However, one important limitation of the 2-D Lagrangian model is its simplified vertical structure, which makes it is very difficult to parameterize atmospheric transport of pollutants above the mixing height. In order to overcome this limitation, a 3-D Eulerian transport/deposition model has been developed at MSC-W since 1993 (Berge, 1993; Jakobsen et al., 1995; Jonson and Berge, 1995; Jakobsen et al., 1996; Jakobsen et al., 1997; Berge, 1997; Berge and Jakobsen, 1998, Jonson et al., 1998a, 1998b, Olendrzynski et al., 1998a, 1998b, 1999). This year - for the first time - the model was applied to operational computations. The results of routine calculations: country budgets and country-to-country pollution exchange, are presented in Bartnicki (1999). The current status of the model and its performance with respect to 1996 data was extensively described in EMEP 1997 Report (Bartnicki et al., 1998, Olendrzynski et al., 1998), and is available at: http://www.emep.int. Therefore, only the recent updates to the model are presented here (Section 1) together with the analysis of the model performance for 1997. The model was run for 1997 meteorological and emission data. EMEP measurement database for 1997 - used for model validation - is described in Section 2. In Section 3 annual scatter plots are presented and discussed. Examples of daily time series are given in Section 4, while computed maps of annual concentration and deposition fields are presented in Section 5 followed by conclusions and references. 1. Recent updates to the model This section documents significant changes introduced in the model during 1998 and early 1999. The most important development was a rather detailed analysis of pollutant mass conservation, which led to the modifications in the chemistry scheme and to the debugging of the model “book keeping”. The overall outcome was an updated code which produces annual or monthly results with mass conservation error below 1%. Also, the comparison of the model performance with respect to the EMEP Lagrangian model (Bartnicki and Tarrason, 1998), showed that the Eulerian model performs comparably or better in most tests. Some of the tests for 1996 data were repeated with the updated Eulerian model (not discussed here). They showed that the conclusions reached in 1998 are still valid. These developments made the EMEP Eulerian acid deposition model ready for operational use. The individual developments with respect to the model are discussed in detail below. The following modifications were made in the model compared to the 1998 version: - extension of the model domain to 170 x 133 grid - application of the PARLAM-PS meteorological model for producing meteorological data - modifications in the physical routines imposed by the new meteorological data; mass conservation analysis - introduction of new countries/Parties to the CRLTAP Convention in the budget and source receptor computations -4- 1.1 Extension of the model domain The model domain has been extended from [1:151] x [1:133] to [1:170] x [1:133] in the EMEP 50km grid. The description of the EMEP 50km grid system is given e.g. in the Appendix of EMEP/MSC-W Report 1/98 (see also Figure 1.1 below). The extension of the model domain in the x direction from [1:151] to [1:170] grid cells, enabled the inclusion of Cyprus and Armenia (Parties to the LRTAP Convention), as well as the entire Mediterranean Sea, entire Turkey, Armenia, Azerbaijan, the Caspian Sea, Syria, and parts of Iran and Irak. At the same time, the deposition calculation area increased from ([6:38] x [2:36]) used by the EMEP Lagrangian model to ([1:44] x [1:37]). This corresponds to grid cells: ([36:167] x [12:122]) in the 50km notation (Figure 1.1). The extension of the domain required extra input data for the parts not covered by the model so far. These data included - among others - anthropogenic emissions, natural marine emissions from eastern part of the Mediterranean Sea, landuse and surface roughness. The extended emission and meteorological data are discussed in other EMEP/ MSC-W Notes: Mylona (1999), and Tsyro and Støren (1999). The landuse data were processed - aggregated to the classes of the original RIVM formulation - by David Simpson based on the database developed at Stockholm Environment Institute (Simpson - private communication, 1999). 122 120 110 100 90 80 70 60 50 40 30 20 12 36 40 50 60 70 80 90 100 110 120 130 140 150 160 167 Figure 1.1 Extended EMEP 50km grid deposition area. It corresponds to [1:44] x [1:37] of the EMEP 150km grid. 1.2 PARLAM-PS meteorology In 1998 computations, the meteorological data for 1996 were derived from the output of the LAM50E meteorological model. This year, however, for the first time the PARLAM-PS model was applied to produce the meteorological data for use in the EMEP Eulerian model. PAR- -5- LAM-PS is a dedicated version of the HIRLAM model - operational weather forecast system of the Norwegian Meteorological Service. In PARLAM-PS the σ-coordinates replaced HIRLAM’s hybrid η−coordinates, and polar stereographic projection replaced rotated spherical horizontal grid. The detailed description of the PARLAM-PS model and its output is given by Tsyro and Støren (1999). Here, only the basics are given. The domain of the PARLAM-PS model covers the entire domain of the EMEP Eulerian model. The horizontal and vertical grids of both model are identical. The temporal resolution of the meteorological data increased from 6 hours in the LAM50E model to 3 hours for PARLAMPS. For the purposes of the EMEP Eulerian model eight 3-D and four 2-D fields of data are needed. The 3-D fields are: - wind u-component [m/s] - wind v-component [m/s] - specific humidity [kg/kg] - potential temperature. [K] - cloud water [(kg water)/(kg air)] - cloud cover [%] - precipitation at each vertical level accumulated over 3-hours [mm] - vertical velocity [1/s] Compared to the LAM50E data, 3-D cloud cover data were added. Previously, the cloud cover was given for two layers: above and below the normalized sigma level 0.85 (~850hPa). The 2D surface fields include: - air pressure [hPa] - temperature at 2m [K] - surface flux of sensible heat [W/m2] - surface stress [N/m2] Because of the increased temporal resolution, extension of the grid and adding 3-D cloud data, the size of the meteorological data files increased to the total of 21 900 MB required for one year of meteorological data. This figure is the product of: 365days times eight 3-hour intervals per day, times 7.5MB - the size of an individual binary file. The size of the meteorological data together with enormously abundant model output (annual, monthly and daily data from runs for individual countries) determines the disk space requirements for the Eulerian model. As in 1998, the model is run on parallel computer CRAY T3E at the Technical University in Trondheim (Norway). Depending on the load at particular time, the model is run on 8-to-16 processors out of the total number of ca. 88 processors available to users. A run for entire year takes (16 processors) about 11 hours of real time. The computation time is practically inversely proportional to the number of used processors. 1.3 Modifications in the code Several modifications in the code were made to account for the changes in the meteorological and other input data. The main temporal loop now is 3 hours (previously 6 hours). At the beginning of the 3-hour loop new set of meteorological data is read from input files. The basic time step is 10 minutes. It is reduced to 200s for chemistry calculations. By increasing the temporal resolution of the basic meteorological data, it became possible to more accurately simulate meteorological conditions in the model. Especially, the diurnal course of basic meteorological variables can be simulated more precisely. Every 10 minutes, there is a linear -6- interpolation of wind, humidity and temperature data within each 3-hour interval. Cloud cover is now given at all twenty vertical layers. It is a an arithmetic mean of 15-minute intervals over the 3-hour period. The 3-D cloud cover data are used directly when computing in-cloud SO2 oxidation and in-cloud scavenging. The maximum cloud cover above the given layer (including the surface layer) is used in computing NO2 dissociation and in computing the wet part of grid cells in the dry deposition scheme. Precipitation is taken as a 3-hour cumulative value. It was found in the original PARLAM-PS data that there are common occasions when there is net evaporation for a given vertical layer. Physically, it means that rain water formed in cloud layers evaporates below the clouds before reaching the surface. Precipitation reaching the ground is thus the difference between the rain water and evaporation. The latter process is not taken into account in the present parameterization of cloud scavenging. Instead, wet scavenging is parameterized in terms of the actual precipitation reaching the surface. The code was modified accordingly to neglect the evaporation process. A detailed parameterization of cloud process in PARLAM-PS provides a good basis for a review of the cloud scavenging processes in the EMEP Eulerian model. The introduction of the evaporation into the pollutant scavenging parameterization, is intended to begin next fall. Horizontal velocities (u and v) are now defined for the staggered grid. The first value at the left boundary is given at the node x = 1+1/2. Similarly the first the value in the y direction is given at y=1+1/2. Previously, in the model version with LAME50e meteorology, the horizontal velocities were given at the centers of grid cells. They were interpolated linearly to grid cell boundaries when computing horizontal advection. Vertical velocities - on the other hand - are now given at the grid centers. The values at the “half-grids” between vertical layers are “recovered” precisely through interpolation and by setting to zero velocities at the surface and at the top of the atmosphere. A reverse calculation is done in PARLAM-PS, when vertical velocities are stored for output. Previously with LAM50e, the situation was just the opposite. Equilibrium chemical reactions leading to the production of ammonium sulfate and ammonium nitrate were taken outside of the iteration within the TWOSTEP method. This modification in the numerical scheme for solving the chemistry, helped to maintain the mass balance especially for reduced nitrogen. It should be noted that, in general, the TWOSTEP conserves mass only if a sufficient number of iterations is performed. In the current implementation only single iteration is used with a time step of 200s. This was found sufficient for practical applications. Pollutant mass conservation is an important and desired feature of an operational air pollution model. It is especially important in case of budget computations and transboundary exchange. For the annual runs with all emissions accounted for, the total mass of pollutants is conserved in the model domain within 1% range for total sulfur, total oxidized nitrogen and reduced nitrogen. Similar accuracy is achieved in runs for individual countries. 1.4 New countries in the budget and source-receptor computations. Due to the extension of the computational domain described in paragraph 1.1, several new countries - Parties to the LRTAP Convention - could be included in the budget calculations. -7- These include: Armenia, Cyprus, Malta and Turkey. For each of these countries as well as for all countries and seas added to the computational domain, it was necessary to determine the fraction of the grid cell area belonging to the respective country or sea (Caspian or Mediterranean). This was done based on the geographical coordinates of coastlines and the country borders. In the following sections, results from model validation against 1997 data are presented. But first comes the basic information about the measurement database for 1997. 2. Measurement database for 1997 The Eulerian model has been run with meteorological and emission data refer for 1997. Computed concentrations and depositions have been compared with available measurements in the model domain. Altogether, 87 EMEP stations have been used for the model validation (89 stations in 1996). These stations reported daily values of air concentrations and concentrations in precipitation. The number of days in 1997 for which measurements were performed varied form one station to another as well as the number of measured species at each station. The list of the stations used for the Eulerian model validation is given in Table 2.1. Geographical positions of these stations in the model domain are shown in Figure 2.1. The density of the EMEP measurement network is quite high in Central and Western Europe (Germany, France, UK, Switzerland, Poland, Czech Republic, Slovakia) and Scandinavia (Finland, Norway, Sweden and Denmark). The spatial coverage is less satisfactory in Southern Europe (Italy, Greece, Spain, the Balkans), where in general the quality of measurements is lower than in Central and Northern Europe. Figure 2.1 Geographical locations of the EMEP stations in the Eulerian model domain. The stations marked by black circles have been used for the model validation. -8- Table 2.1. List of EMEP stations used for the model validation. Station No Code 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 AT2 AT4 AT5 CH1 CH2 CH3 CH4 CH5 CS1 CS3 DE1 DE2 DE3 DE4 DE5 DE7 DE8 DE9 DK3 DK5 DK8 EE9 EE11 FI4 FI9 FI17 FI22 FI37 FR3 FR5 FR8 FR9 FR10 FR11 FR12 GB2 GB4 GB6 GB7 GB13 GB14 GB15 GB16 GR1 HU2 Position Name Illmitz St. Koloman Vorhegg Jungfraujoch Payerne Tönikon Chaumont Rigi Svratouch Kosetice Westerland Langenbrügge Schauinsland Deuselbach Brotjacklriegel Neuglobsow Schmücke Zingst Tange Keldsnor Anholt Lahemaa Vilsandy Ähtari Utö Virolahti II Oulanka Ähtari II La Crouzille La Hague Donon Revin Morvan Bonnevaux Iraty Eskdalemuir Stoke Ferry Lough Navar Barcombe Mills Yarner Wood High Muffles Strath Vaich D. Glen Dye Aliartos K-puszta Lat. N EMEP grid Lon. E 47°46’ 47°39’ 46°40’ 46°33’ 46°48’ 47°29’ 47°03’ 47°04’ 49°44’ 49°35’ 54°55’ 52°48’ 47°55’ 49°46’ 48°49’ 53°09’ 50°39’ 54°26’ 56°21’ 54°44’ 56°43’ 59°30’ 58°23’ 62°33’ 59°47’ 60°31’ 66°19’ 62°35’ 45°50’ 49°37’ 48°30’ 49°54’ 47°16’ 46°49’ 43°02’ 55°19’ 52°34’ 54°26’ 50°52’ 50°36’ 54°20’ 57°44’ 56°58’ 38°22’ 46°58’ 16°46’ 13°12’ 12°58’ 7°59’ 6°57’ 8°54’ 6°58’ 8°27’ 16°02’ 15°05’ 8°18’ 10°45’ 7°54’ 7°03’ 13°13’ 13°02’ 10°46’ 12°44’ 9°36’ 10°44’ 11°31’ 25°54’ 21°49’ 24°13’ 21°23’ 27°41’ 29°24’ 24°11’ 1°16’ -1°50’ 7°08’ 4°38’ 4°05’ 6°11’ -1°05’ -3°12’ 0°30’ -7°54’ -0°02’ -3°43’ -0°48’ -4°46’ -2°25’ 23°05’ 19°35’ -9- i-50 112.05 108.34 109.74 103.87 102.17 103.56 101.82 103.65 107.80 107.09 91.60 97.31 101.66 97.86 106.40 99.03 100.72 96.67 90.73 94.28 91.93 97.90 97.33 91.26 94.52 21.00 17.59 91.18 95.91 86.93 99.84 94.77 21.26 22.39 20.69 78.76 86.28 74.14 87.73 16.44 16.21 13.49 14.60 137.31 116.43 Altitude j-50 60.48 56.11 54.18 48.42 47.80 51.09 48.28 49.86 62.72 61.41 63.69 62.25 50.84 53.38 58.08 65.03 58.60 66.83 67.24 65.50 69.47 86.56 81.26 88.71 82.72 89.42 97.14 88.73 40.35 45.41 51.14 51.38 45.84 47.05 32.39 55.95 53.07 51.40 49.32 46.04 55.58 59.86 59.70 55.17 62.76 (m) 117 851 1020 3573 510 540 1130 1028 737 633 12 74 1205 480 1016 62 937 1 13 9 40 32 6 162 7 4 310 180 497 133 775 390 620 836 1300 243 15 126 8 119 267 270 85 110 125 Table 2.1. List of EMEP stations used for the model validation. Station No Code 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 IE1 IE2 IE3 IS2 IT1 IT4 LT15 LV10 LV16 NL9 NL10 NO1 NO8 NO15 NO39 NO41 NO42 NO55 PL2 PL3 PL4 PL5 PT1 PT3 PT4 RU1 RU13 RU16 SE2 SE5 SE8 SE11 SE12 SE13 SI8 SK2 SK4 SK5 SK6 TR1 YU5 YU8 Position Name Valentia Obs. Turlough Hill The Burren Irafoss Montelibretti Ispra Preila Rucava Zoseni Kollumerwaard Vreedepeel Birkenes Skreådalen Tustervatn Kårvatn Osen Spitzbergen, Z Karasjok Jarczew Sniezka Leba Diabla Gora Braganca V. d. Castelo Monte Velho Janiskoski Pinega Shepeljovo Rörvik Bredkälen Hoburg Vavihill Aspvreten Esrange Iskrba Chopok Stará Lesná Liesek Starina Cubuk11 Kamenicki vis Zabljak Lat. N EMEP grid Lon. E 51°56’ 53°02’ 52°59’ 64°05’ 42°06’ 45°48’ 55°21’ 56°13’ 57°08’ 52°20’ 51°32’ 58°23’ 58°49’ 65°50’ 62°47’ 61°15’ 78°54’ 69°28’ 51°19’ 50°44’ 54°45’ 54°09’ 41°49’ 41°42’ 38°05’ 68°56’ 64°42’ 59°58’ 57°25’ 63°51’ 56°55’ 56°01’ 58°48’ 67°53’ 45°34’ 48°56’ 49°09’ 49°22’ 49°03’ 40°30’ 43°24’ 43°09’ - 10 - -10°15’ 13°11’ -9°06’ -21°01’ 12°38’ 8°38’ 21°04’ 21°13’ 25°55’ 6°17’ 5°51’ 8°15’ 6°43’ 13°55’ 8°53’ 11°47’ 11°53’ 25°13’ 21°59’ 15°44’ 17°32’ 22°04’ -6°46’ -8°48’ -8°48’ 28°51’ 43°24’ 29°07’ 11°56’ 15°20’ 18°09’ 13°09’ 17°23’ 21°04’ 14°52’ 19°35’ 20°17’ 19°41’ 22°16’ 33°00’ 21°57’ 19°08’ i-50 13.13 77.34 73.97 6.47 117.19 105.86 22.76 22.27 22.80 91.81 93.89 86.49 84.49 15.19 15.56 17.05 59.01 79.20 110.50 105.76 100.46 105.27 88.32 84.99 88.59 81.61 20.21 21.61 91.21 83.60 97.21 20.17 19.79 15.38 113.86 112.77 113.03 112.06 115.06 142.33 125.78 123.20 Altitude j-50 44.83 49.33 47.69 67.30 45.86 47.74 76.44 77.77 83.76 59.16 55.51 69.63 69.24 85.59 77.49 77.01 104.35 97.68 71.93 63.96 71.98 75.87 24.84 23.03 14.62 99.47 107.55 90.20 70.96 83.58 75.76 69.77 77.79 93.08 54.61 65.67 66.84 66.43 69.16 74.68 60.75 56.37 (m) 9 420 100 61 48 209 5 18 183 1 28 190 475 439 210 440 474 474 180 1604 2 157 691 16 43 118 28 4 10 404 58 172 20 475 520 2008 808 892 345 1169 813 1450 3. Annual scatter plots for 1997 3.1 Concentrations in air We begin the model validation by comparing measured and computed annual concentrations in air and in precipitation. For the comparison of air concentrations, only those stations from Table 2.1 were selected which reported measurements for at least 274 days in 1997, i.e. 75% of days. The number of stations that fulfil the requirement varied between 25 for nitric acid and nitrate, and 60 for sulfate. The same requirement had been applied in previous years in case of EMEP Lagrangian acid deposition model. A new element this year are the quality classes updated recently by CCC/NILU. The results of the comparison are presented in the form of scatter plots. Scatter plots illustrate the differences between calculated and measured annual concentrations and depositions for all selected stations available for a given compound. Five stations (DE3, FR12, PL3, SK2 and NO42) have been excluded from the comparison due to either their location on mountain tops, or due to influence of local emission sources (Hjellbrekke, 1998). For annual average concentrations of sulfur dioxide in air, the scatter plot is shown in Figure 3.1. Calculated, mean concentration over 56 stations (2.88 µg(S)m-3) is 91% higher than the mean concentration from the observations (1.51 µg(S)m-3). The difference is much larger for sulfur dioxide than for all other compounds both in air and in precipitation. In general, model overestimates high concentrations above 1.5 µg(S)m-3, and underestimates those below 0.6 µg(S)m-3. The ‘factor of two’ agreement between computed and measured annual concentrations lies between external dotted lines in Figures: 3.1 - 3.12. When the station is located in the factor of two zone in the scatter plots, annual average computed value for this station must be no more than two times higher or no less than two times lower than the measured value. Logarithmic scale is applied in order to better display stations with low concentration or deposition values. In case of linear plots, those stations typically are grouped together in the lower left corner of the plot, thus making station identification difficult. SO2 in air [ug S/m3] in 1997 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 4.0 PL2 6.0 CS1 10.0 DE8 IT1 10.0 CS3 SK6 8.0 SK4 NL10 6.0 DE7 SI8 DE4 FR9 DE2 PL5 4.0 HU2 SK5 GB4 8.0 6.0 8.0 10.0 AT2 4.0 FR8 DE5 IT4 FR10 2.0 GB13 2.0 GB2 SE11 IE3 IE2 DK3 LV10 LV16 CH3RU16 EULERIAN GB6 CH5 1.0 1.0 CH4 0.8 CH2 FI17 0.8 PL4 0.6 0.6 TR1 DE9 GB7 SE13 DK5 FI22 0.4 SE12 0.4 LT15 GB16 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 1.51 2.88 0.74 56 SE2 DK8 NO1 FI9 DE1 0.2 0.2 SE8 FR5 0.1 0.08 0.1 SE5 0.08 IE1 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 4.0 OBSERVED 6.0 8.0 10.0 Figure 3.1 Computed versus measured annual average sulfur dioxide concentrations in air in 1997. Units: µg(S)m-3. - 11 - Figure 3.1 and all other scatter plots (Figures 3.2 - 3.13) include EMEP stations of quality classes ranging between A (best quality; within +/- 10%) to D (lowest quality; worse than 30%). The quality classes for all station/component combinations have been determined by EMEP Chemical Coordinating Centre (CCC) at the Norwegian Institute for Air Research (NILU). CCC arrived at the quality ranking through inter-laboratory comparisons and analysis of various measurement and analytical methods. The tables with quality classes are included in the Appendix of EMEP/MSC-W Report 1/99. Correlation coefficient shown in Figure 3.1, between measured and computed annual concentrations, is 0.74. If only those stations with quality class A are considered (not shown here), the correlation coefficient increases to 0.81. This increase occurs also for other components. However, in general, no major improvement of the annual model performance (scatter and bias) is noted when only class A stations are taken into account. This is partly because there are relatively few stations ranked B-D for components other than SO2. The performance of the EMEP Eulerian model for SO2 concentrations is not satisfactory. The model generally overestimates concentrations in source areas (Central and Western Europe) and underestimates concentrations in remote locations (Scandinavia). There are two possible reasons for this. On one hand, EMEP stations have been designed to monitor air pollution levels in relatively remote and clean areas. Measurements at such point locations are not usually representative for pollution levels in larger areas, to which model results should be compared - due to its grid cell area of ca. 2000-2500 km2. Similar situation was in the case of EMEP Lagrangian acid deposition model, which - in addition - had grid cell area ca. nine times larger than the EMEP Eulerian model. SO2 in air [ug S/m3] in 1997 0.04 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 4.0 PL2 4.0 CS1 IT1 GB7 SK4 SK6 0.8 GB6 CH5 0.6 SE8 0.4 SE12 FI9 IE3 2.0 NL10 DE7 DE4 SI8 IT4 FR9 DE2 GB16 FR8 GB13 PL4 PL5 SE11 DE9 DK3 GB2 DK8 SE2 DK5 DE5 CH4 CH2 IE2 RU16 CH3 FR5 FR10 LV10 FI17 1.0 EULERIAN CS3 GB4 DE8 2.0 4.0 SK5 HU2 AT2 1.0 0.8 0.6 DE1 LT15 LV16 0.4 IE1 NO1 SE13 0.2 FI22 0.2 TR1 0.1 0.1 0.08 0.08 0.06 0.06 0.04 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 1.51 1.25 0.78 56 0.04 SE5 0.04 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 4.0 OBSERVED Figure 3.2 Computed versus measured annual average sulfur dioxide concentrations in air in 1997. Test with fixed vd for SO2. Units: µg(S)m-3. - 12 - Another reason for relatively poor performance with respect to SO2 air concentrations, is the unsatisfactory performance of the dry deposition scheme applied in the Eulerian model. Figure 3.2 presents analogous results for a test run in which the SO2 dry deposition velocity at 1m was fixed at 0.008 m/s for all meteorological conditions and all surface types. The computed mean of SO2 concentrations decreased to 1.25 µg(S)m-3. Now, both the underestimations and overestimations seen in Figure 3.1 have been significantly reduced. The results of this model version for other than SO2 components (not shown here), are only slightly affected. This tests shows that most probably the computed by the model sum of the surface and laminar resistances is on the average - overestimated in the source regions and underestimated in remote areas. That results in the opposite estimation for the respective dry deposition velocities for SO2. Dry deposition parameterization for SO2 has to be, therefore, re-evaluated. It is intended to start with this task is in the coming months. The scatter plot for annual average concentrations of sulfate in air is shown in Figure 3.3. Calculated mean concentration over 60 stations (0.73 µg(S)m-3) is 12% lower than the mean concentration from the observations (0.83 µg(S)m-3). Model underestimates low concentrations below 0.60 µg(S)m-3, especially very low values measured at Norwegian and Swedish stations. However, for sulfate in air, 82% of the stations can be found in the factor of two area. Correlation between measured and computed concentrations (0.87) is better in this case than for sulfur dioxide. The scatter plot for annual average concentrations of nitrogen dioxide in air is shown in Figure 3.4. Calculated mean concentration over 47 stations (2.06 µg(N)m-3) is almost identical (1% difference) to the mean concentration from the observations (2.04 µg(N)m-3). The agreement between model results and measurements is best for NO2 among all components. For nitrogen dioxide, 87% of the stations can be found in the factor of two area. Correlation between measured and computed concentrations (0.80) is also good in this case. SO4-- in air [ug s/m3] in 1997 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 PL2 HU2 2.0 2.0 CS1 CS3 SK6 SK5 GB4 SK4 IT1 NL10 SI8 GB7 DE8 DE7 DE4 DE2 1.0 0.9 DE5 DE9 FR9 NL9 PL5 FR8 0.8 0.7 IE3 0.6 EULERIAN 0.5 0.4 1.0 0.9 PL4 IT4 0.8 FR5 DK5 FR10GB13 DE1 FR11 SE11DK8 CH2 DK3 GB16 LV10 CH5 GB2SE2 IE2SE8 LV16 RU16 FI17 GB6 FI9 SE12 0.3 0.7 0.6 0.5 0.4 IE1 0.3 GB15 NO8 NO1 FI22 0.2 0.2 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 0.83 0.73 0.87 60 NO41 NO55 SE13 0.1 0.1 0.09 0.09 SE5 IS2 0.08 0.07 NO15 0.06 0.06 0.08 NO39 0.07 0.08 0.1 0.2 0.06 0.4 0.6 0.8 1.0 2.0 OBSERVED Figure 3.3 Computed versus measured annual average sulfate concentrations in air in 1997. Units: µg(S)m-3. - 13 - NO2 in air [ug N/m3] in 1997 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 4.0 6.0 8.0 NL10 8.0 8.0 6.0 6.0 DE4 4.0 IT4 PL2 HU2 SE2CS3 DE2 IT1 SE11 DE8 DK8 DE5 CH4 SK5 DE7 DE9 CH5 SK6 PL4 2.0 4.0 CH3 CH2 2.0 DE1 SE12 PL5 SE8 SK4 FI17 FI9 LT15 EE11 EE9 EULERIAN 1.0 RU16 LV10 1.0 NO1 NO8 0.8 0.8 LV16 0.6 0.6 IE1 NO41 YU8 YU5 0.4 0.4 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 2.04 2.06 0.80 47 FI22 SE5 TR1 NO39 0.2 0.2 NO15 0.1 0.1 NO55 0.08 0.08 0.1 0.2 0.08 0.4 0.6 0.8 1.0 2.0 4.0 6.0 8.0 OBSERVED Figure 3.4 Computed versus measured annual average nitrogen dioxide concentrations in air in 1997. Units: µg(N)m-3. The scatter plot for annual average concentrations of nitric acid plus nitrate in air is shown in Figure 3.5. Calculated mean concentration over 25 stations (0.62 µg(N)m-3) is in good agreement (only 13% higher) with than the mean concentration from the observations (0.55 µg(N)m-3). In general, model reproduces measured concentrations well, but there is underestimation of the concentrations in the range below 0.2 µg(N)m-3. For nitric acid plus nitrate, 88% of the stations can be found in the factor of two area. Correlation between measured and computed concentrations is 0.69. The scatter plot for annual average concentrations of ammonia plus ammonium nitrate in air is shown in Figure 3.6. Calculated mean concentration over 26 stations considered (1.25 µg(N)m-3) is 8% lower than the mean concentration from the observations (1.36 µg(N)m-3. For ammonia plus ammonium nitrate, 85% of the stations can be found in the factor of two area. Correlation between measured and computed concentrations is 0.80. 3.2 Concentrations in precipitation In case of concentrations in precipitation a different temporal coverage requirement is applied. For a station to be included in the comparison, there must be at least 25% of common days with measured concentrations between the model and the station. The same requirement has been used so far, when analyzing the results of the EMEP Lagrangian model. Figure 3.7 shows the differences between measured and computed total annual precipitation. It should be noted here that the computed value refers to the grid cell mean while the measured one is a point measurement. - 14 - HNO3 and NO3- in air [ug N/m3] in 1997 0.01 0.02 0.04 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 GB14 2.0 2.0 2.0 DK5 HU2 PL2 DK8 DK3 1.0 SE11 SE2 PL4 GB2 0.8 FI9 SI8 0.6 1.0 0.8 CH2 PL5 0.6 LT15 LV10 0.4 0.4 FI17 SE12 LV16 0.2 0.2 EULERIAN NO8 NO1 0.1 0.1 0.08 0.08 0.06 0.06 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 0.55 0.62 0.69 25 NO41 0.04 0.04 0.02 0.02 FI22 SE5 0.01 0.01 0.02 0.04 0.06 NO39 0.01 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 OBSERVED Figure 3.5 Computed versus measured annual average nitric acid plus nitrate concentrations in air in 1997. Units: µg (N)m-3. NH3 and NH4+ in air [ug N/m3] in 1997 0.04 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 2.0 4.0 PL2 4.0 4.0 DK3 CH2 GB14 PL5 SI8 2.0 GB2 DK5 SE11 2.0 DK8 PL4 SE2 LV10 1.0 1.0 LV16 LT15 0.8 0.8 SE12 0.6 0.6 EULERIAN FI17 NO8 0.4 0.4 FI9 NO1 NO41 0.2 0.2 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 1.36 1.25 0.80 26 FI22 SE5 NO55 0.1 0.1 NO39 0.08 0.08 0.06 0.06 NO15 0.04 0.04 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 0.04 2.0 4.0 OBSERVED Figure 3.6 Computed versus measured annual average ammonia plus ammonium concentration in air in 1997. Units: µg(N)m-3. - 15 - In case of precipitation no individual point is a good measure for an area equivalent to the grid cell area cell (ca. 2000 to 2500km2). It should be noted that the computed mean (574 mm) is significantly lower (29%) than the observation mean (808 mm). As it is discussed below, it has consequences for wet deposition. The scatter plot for annual mean sulfate concentration in precipitation is shown in Figure 3.8. Calculated, mean concentration over 50 stations (0.72 mg(S)l-1) is 43% higher than the mean concentration from the observations (0.51 mg(S)l-1), which means significant overestimation. In this case, still 87% of the stations can be found in the factor of two area. Correlation (0.64) between measured and computed concentrations in precipitation of sulfate is not so good as in the case of air concentrations (0.87). The scatter plot for annual mean concentration of nitrate in precipitation is shown in Figure 3.9. There is little difference (3%) between calculated mean over 52 stations (0.36 mg(N)l-1yr-) and the observation mean (0.35 mg(N)l-1yr-). In general, model slightly underestimates measured mean concentrations in the range below 0.1 mg(N)l-1yr-1. For concentration in precipitation of nitrate, 90% of the stations can be found in the factor of two area. Correlation between measured and computed depositions (0.59) is, however, worse than in the case of sulfate. The scatter plot for annual mean concentration of ammonium in precipitation is shown in Figure 3.10. Calculated mean concentration in precipitation (0.48 mg(N)l-1yr-1) over 54 stations, is 14% higher than the mean over observations (0.42 mg(N)l-1yr-1). In general, model reproduces measured concentrations well except for high values above 0.5 mg(N)l-1yr-1 which tend to be overestimated. For nitrate concentration in precipitation, 74% of the stations can be found in the factor of two area. Correlation between measured and computed depositions is 0.55. Although, agreement between mean computed and measured values, as well as correlation are good, the scatter of the stations within a factor of two area is larger than for air concentrations. The same remarks applies to concentrations of sulfate and nitrate in precipitation. Accumulated precipitation in 1997 200 300 400 500 600 700 800 900 1000 2000 2000 2000 YU8 NO8 NO39 SK4 NO15 IE2 SK5 1000 GB15 900 1000 FR10 IE3 GB13 GB2 GB6 800 LV16 900 IS2 800 NO1 700 700 RU16 600 FI22 TR1 RU13 SE12 EE11 FI17 EE9 500 FI9 400 600 PL5 DK3 SE2 DE1 FI4 NO41 SE11 SK6 GB14 DE4 DK5 LT15 AT2 SE5 NL9 FR11 LV10 CH5 DE5 500 FR9 FR5 DE8 DK8 NO55 AT4 AT5 CS1 CH4 YU5 CH2 PL2 PL4 400 CH3 FR8 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 808.12 574.51 0.53 67 DE2 RU1 DE7 300 IT4 HU2 DE9 300 CS3 200 200 IT1 200 300 400 500 600 700 800 900 1000 OBSERVED 2000 Figure 3.7 Computed model versus measured mean annual precipitation in 1997. Units: mm yr-1. - 16 - Conc. in prec. of SO4-- corr. [mg S/l/year] in 1997 0.08 0.1 0.2 0.4 0.6 0.8 1.0 SK6 YU5 IT4 PL2 CS3 SK5 CH3 AT5 AT4 1.0 0.9 FR8 0.8 0.7 0.6 EULERIAN 0.9 DE9 DK5 YU8 FI17 NL9 DK3 LV16 FI9 SE2 DE1 NO1 EE9 RU16 FR11 0.5 1.0 DE2 0.8 CH4 CH2 CH5 FR9 LV10 SK4 DE8 DE7 DE4 PL4DE5 PL5 0.7 0.6 0.5 FR10 NO41FI4 0.4 FR5 0.4 GB2 NO8 0.3 0.3 RU13 FI22 IE2 0.2 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 0.51 0.72 0.64 50 0.2 IE3 0.1 0.1 NO39 0.09 IS2 0.09 0.08 0.08 NO15 0.08 0.1 0.2 0.4 0.6 0.8 1.0 OBSERVED Figure 3.8 Computed model versus measured mean annual sulfate (corrected for sea spray) concentrations in precipitation in 1997. Units: mg(S)l-1 yr-1. Conc. in prec. of NO3- [mg N/l/year] in 1997 0.04 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 1.0 1.0 0.9 0.9 0.8 0.8 CH3 0.7 AT5 0.6 FR8 FR9 SK6 0.5 LV10 0.4 FR11 0.3 CH4 CH2 FR5 NO8 GB2 0.5 SE2 0.4 YU5 0.3 FI9 SK4 YU8 EULERIAN 0.6 DE9 FI17 GB13 IE2 GB6 0.7 DE5 CS3 DE7 NL9 DE8 DE1 DK5 DE4 DK3 PL2 PL4 NO1 GB14PL5 CH5 SK5 FR10 0.2 DE2 AT4 LV16 0.2 EE9 RU16 IE3 FI4 NO41 GB15 0.1 0.1 0.09 0.09 0.08 0.08 0.07 0.07 0.06 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 0.35 0.36 0.59 52 0.06 FI22 0.05 0.05 RU13 0.04 0.04 NO15 NO39 0.03 0.04 0.06 0.08 0.03 0.1 0.2 0.4 0.6 0.8 1.0 OBSERVED Figure 3.9 Computed versus measured mean annual nitrate concentrations in precipitation in 1997. Units: mg (N)l-1 yr-1. - 17 - Conc. in prec. of NH4+ [mg N/l/year] in 1997 0.02 0.04 0.06 0.08 0.1 0.2 0.4 CH3 1.0 CH4 0.8 FR11 0.6 LV10 0.6 AT4 0.8 1.0 DE5 CH5 IT4 DE2 SK6 CH2 PL2 AT5 DE8CS3 FR8 DE7 SK5 FR9 DE4 YU5 DK5 DE1 NL9 DE9 SK4 DK3 PL5 PL4 0.4 0.8 0.6 0.4 SE2 FR10 1.0 NO1 GB2 LV16 FR5 GB14 FI17 YU8 FI9 GB13 IE2 0.2 0.2 EE9 EULERIAN GB6 NO8 RU16 NO41 FI4 IE3 0.1 0.1 GB15 0.08 0.08 0.06 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 0.42 0.48 0.55 54 0.06 FI22 RU13 0.04 0.04 NO39 NO55 0.02 0.02 NO15 0.02 0.04 0.06 0.08 0.1 0.2 0.4 0.6 0.8 1.0 OBSERVED Figure 3.10 Computed versus measured mean annual ammonium concentrations in precipitation in 1997. Units: mg(N)l-1 yr-1. 3.2 Wet depositions The scatter plot for annual wet deposition of sulfate is shown in Figure 3.11. Calculated, mean concentration over 50 stations (385.4 mg(S)m-2yr-1) is merely 3% higher than the mean concentration from the observations (395.8 µg(S)m-2yr-1), which means very good agreement. In this case, 90% of the stations can be found in the factor of two area. Correlation between measured and computed concentrations in precipitation of sulfate is good (0.63) but not so good as in the case of respective air concentrations(0.87; see Figure 3.3). The same conclusion applies to nitrate, and the sum of ammonia and ammonium (see below and Figures 3.5 and 3.6). The scatter plot for annual wet deposition of nitrate is shown in Figure 3.12. Calculated mean over 52 stations (189.12 mg(N)m-2yr-1) is 30% higher than the mean concentration from the observations (268.80 mg(N)m-2yr-1). In general, model underestimates measured values, especially for the range above 100.0 mg(N)m-2yr-1. However, despite the significant underestimation, still 83% of the stations can be found in the factor of two area. Correlation between measured and computed depositions (0.64) is similar to the one in case of sulfate. It can be noticed that although, the model on the average computes reasonable values for concentration in precipitation (Figures 3.8-3.10), the respective computed wet depositions are on the average underestimated. A reason for that can be the underestimation of modelled total precipitation at model grid cells where the measurement stations are located. That means that although the concentrations in precipitation are on the average correct, insufficient amount of precipitation makes the total mass deposited to be underestimated. - 18 - Wet deposition of SO4-- corr. [mg S/m2/year] in 1997 80 100 200 400 600 800 1000 SK5 SK4 YU8 1000 1000 900 900 SK6 800 800 700 700 YU5 600 600 AT5 500 AT4 PL2 LV16 PL5 500 FR10 DE8NO8 DE5 DE4 400 CH3 DK3 CH5 FR11 FR9 LV10 DK5 FI9 IT4 400 CS3 FR8 DE2RU16 SE2 GB2 DE1 FI17 CH2 CH4 DE7 EE9 300 NO1 PL4 IE2 300 DE9 NL9 NO41 200 200 FI4 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 395.80 385.40 0.63 50 FR5 IE3 FI22 RU13 NO39 100 100 NO15 90 90 80 80 IS2 80 100 200 400 600 800 1000 OBSERVED Figure 3.11 Computed versus measured annual wet deposition of sulfate in 1997. Units: mg(S)m-2 yr-1. Wet deposition of NO3- [mg N/m2/year] in 1997 30 40 50 60 70 80 90 100 200 300 400 500 600 600 600 500 500 SK5 400 400 NO8 SK4 AT5 300 DE5 SK6 LV10 200 EULERIAN YU8 AT4 FI9 GB15 100 300 NO1 CH3 DE8 DE1 FR9 DK3 DE2 FR10 GB13 DE4GB2 IE2 FR11CH5 FR8 SE2 PL5 NL9 DK5 DE7 GB14 LV16 CS3 CH2 CH4 PL2 PL4 DE9 YU5 IE3 FR5 FI17 200 GB6 EE9 100 RU16 90 90 80 80 NO41 70 70 FI4 60 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 268.80 189.12 0.64 52 60 50 50 40 30 40 NO39 NO15 30 FI22 RU13 30 40 50 60 70 80 90 100 200 300 400 500 600 OBSERVED Figure 3.12 Computed versus measured annual wet deposition of nitrate in 1997. Units: mg(N)m-2 yr-1. - 19 - The scatter plot for annual wet deposition of mean of ammonia and ammonium is shown in Figure 3.13. There is a large difference (28%) between calculated mean (243.98 mg(N)m-1yr1) over 54 stations and the mean from the observations (338.27 mg(N)m-1yr-1). As in the case of nitrate, the model underestimates measured depositions, especially for the range above 100.0 mg(N)m-2yr-1. For wet deposition of ammonia and ammonium nitrate, 72% of the stations can be found in the factor of two area. Correlation between measured and computed depositions is 0.58. Wet deposition of NH4+ [mg N/m2/year] in 1997 10 20 40 60 80 100 200 400 800 600 800 800 SK5 AT4 SK4 600 600 CH5 DE5 CH3 SK6 AT5 YU8 DE8 FR10 CH4 CH2 FR11 PL2 FR9 DE2 DE4 FR8 GB2 PL5 NO1 DK3 DE1 NO8 IE2 YU5 DE7 LV10 LV16 CS3 GB13 400 DK5 200 SE2 400 IT4 200 NL9 PL4 GB6 DE9 FR5 FI17 EULERIAN 100 EE9 GB14 IE3 100 RU16 FI9 NO41 80 GB15 80 60 FI4 60 NO39 40 40 OBSERVED mean = EULERIAN mean = correlation = no. of stations = 338.27 243.98 0.58 54 FI22 NO15 RU13 20 20 10 10 NO55 10 20 40 60 80 100 200 400 600 800 OBSERVED Figure 3.13 Computed versus measured annual wet deposition of ammonium in 1997. Units: mg(N)m-2 yr-1. - 20 - 4. Comparison of measured and computed daily results In this section, computed daily concentrations are compared with daily measurements at EMEP stations in Europe. To present all available graphs - several hundreds - would be a formidable task. Therefore, a reasonable selection must be made. Below, we give examples which we think are typical for describing model behavior for a given component/location combination. For each of the combinations, there are stations for which model performs better than in the displayed graphs, and there are stations where the model performance is poorer. Five components are included in the analysis: sulfur dioxide, nitrogen dioxide, sulfate, sum of nitric acid and nitrate, and sum of ammonia and ammonium. The first two components are gases while the last two are measured as gases plus aerosols. Sulfate is measured as aerosol. In all graphs the units are: µgS(or N) m-3. Before we turn to the computed daily values, one important limitation has to be revoked. EMEP Eulerian acid deposition model has not been designed to simulate day-to-day variations. Its main objective is to compute long-term (monthly, annual) mean concentrations and accumulated depositions. Long-term transboundary fluxes and country budgets constitute another important part of model output. To model daily concentrations more precisely, one would need much better input data (e.g. daily variations of emissions on a grid cell basis) and finer horizontal resolution. The former is very difficult or almost impossible to obtain. Introduction of the latter would result in a very complicated model. Then, the required computation time would make long-term calculations practically impossible, at least in the operational mode. Point measurements at stations are compared with the grid cell values in the model (roughly 50 km × 50 km, in the horizontal direction). For gases the computed values are scaled from the lowest model layer (approximately 45 m) to the height of 1m. Measurements can vary significantly even for locations close to each other. Local topographical effects and local emission sources may influence measurements and result in poor representativeness of a given station. For each component we selected three different stations: one located in northern part of Europe, one in middle latitudes, and one in southern Europe. One possibility would be to take the same locations for presentation of various pollutants. However, while there are stations fulfilling this requirement in the northern and Central Europe, no such station exists in the South. Therefore, to better illustrate the model performance different stations have been selected for different components. For both Virolahti II and Cubuk 11 (Figure 4.1), there is a fairly good agreement between calculated and measured SO2 concentrations. The seasonal variations in the observations are well captured by the model, especially at Virolahti II. As one could expect not all peaks are well simulated, but the model dynamics and its response to rapid concentration changes in winter and spring looks satisfactory. For Neuglobsow in Germany the agreement is not good. Model overestimates concentrations throughout the year. As discussed in Section 3, this is typical model behavior in Central and Western Europe, where calculated SO2 concentrations are usually overestimated. - 21 - ___ EMEP measurements ...... EMEP Eulerian model Virolahti II- FI17: SO2 in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 5 5 4 4 3 3 2 SO2 in air [ug S/m3] DE 7 : Neuglobsow ( 62m a.s.l.) 2 1 0 1 ___ 20 ...... EMEP measurements 40 60 80 100 120 0 140 160 180 200 220 240 260 280 300 320 340 360 260 280 300 320 340 360 1997 EMEP Eulerian model Neuglobsow- DE 7: SO2 in air 20 40 60 80 100 120 140 160 180 200 220 240 25 25 20 20 15 15 10 SO2 in air [ug S/m3] TR 1 : Cubuk11 (1169m a.s.l.) 10 5 0 5 ___ 20 ...... EMEP measurements 40 60 80 100 120 0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 260 280 300 320 340 360 1997 Cubuk11- TR1: SO2 in air 20 40 60 80 100 120 140 160 180 200 220 240 8 8 7 7 6 6 5 5 4 4 3 3 2 2 1 1 0 0 20 40 60 80 100 120 140 160 180 200 1997 220 240 260 280 300 320 340 360 Figure 4.1 Comparison of measured and computed SO2 concentrations in air at Virolahti II, Neuglobsow and Cubuk11. Solid line - observations, dotted line - model results. Units: µg(S) m-3. - 22 - ___ EMEP measurements ...... EMEP Eulerian model Vavihill - SE11: SO4 in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 3.5 3.5 3.0 3.0 2.5 2.5 2.0 2.0 1.5 1.0 SO4-- in air [ug S/m3] CH 2 : Payerne ( 510m a.s.l.) 1.5 1.0 0.5 0.0 0.5 ___ 20 ...... EMEP measurements 40 60 80 100 120 0.0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 260 280 300 320 340 360 1997 Payerne - CH2: SO4 in air 20 40 60 80 100 120 140 160 180 200 220 240 6 6 5 5 4 4 3 2 3 SO4-- in air [ug S/m3] GR 1 : Aliartos ( 110m a.s.l.) 2 1 0 1 ___ 20 ...... EMEP measurements 40 60 80 100 120 0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 260 280 300 320 340 360 1997 Aliartos - GR1: SO4 in air 20 40 60 80 100 120 140 160 180 200 220 240 10 10 8 8 6 6 4 4 2 2 0 0 20 40 60 80 100 120 140 160 180 200 1997 220 240 260 280 300 320 340 360 Figure 4.2 Comparison of measured and computed SO4 concentrations in air at Vavihill, Payerne and Aliartos. Solid line - observations, dotted line - model results. Units: µg (S) m-3. - 23 - ___ EMEP measurements ...... EMEP Eulerian model Birkenes - NO1: NO2 in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 10 10 8 8 6 4 6 NO2 in air [ug N/m3] IT 1 : Montelibretti ( 48m a.s.l.) 4 2 2 ___ 0 EMEP measurements 20 40 ...... 60 80 100 120 0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 260 280 300 320 340 360 1997 Montelibretti - IT1: NO2 in air 20 40 60 80 100 120 140 160 180 200 220 240 10 10 9 9 8 8 7 7 6 6 5 5 NO2 in air [ug N/m3] DE 1 : Westerland ( 12m a.s.l.) 4 3 4 3 2 2 1 1 ___ 0 20 ...... EMEP measurements 40 60 80 100 120 0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 1997 Westerland - DE 1: NO2 in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 20 20 15 15 10 10 5 5 0 0 20 40 60 80 100 120 140 160 180 200 1997 220 240 260 280 300 320 340 360 Figure 4.3 Comparison of measured and computed NO2 concentrations in air at Birkenes, Montelibretti and Westerland. Solid line - observations, dotted line - model results. Units: µg(N)m-3. - 24 - ___ EMEP measurements ...... EMEP Eulerian model Virolahti II - FI17: HNO3 and NO3- in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 2.0 2.0 1.5 1.5 1.0 HNO3 and NO3- in air [ug N/m3] LT 15 : Preila ( 5m a.s.l.) 1.0 0.5 0.0 0.5 ___ 20 ...... EMEP measurements 40 60 80 100 120 0.0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 1997 Preila - LT15: HNO3 and NO3- in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 6 6 5 5 4 4 HNO3 and NO3- in air [ug N/m3] HU 2 : K-puszta ( 125m a.s.l.) 3 2 3 2 1 1 ___ 0 20 ...... EMEP measurements 40 60 80 100 120 0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 1997 K-puszta - HU2: HNO3 and NO3- in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 7 7 6 6 5 5 4 4 3 3 2 2 1 1 0 0 20 40 60 80 100 120 140 160 180 200 1997 220 240 260 280 300 320 340 360 Figure 4.4 Comparison of measured and computed nitric acid and nitrate concentrations in air at Virolahti II, Preila and K-puszta. Solid line - observations, dotted line - model results. Units: µg(N)m-3. - 25 - ___ EMEP measurements ...... EMEP Eulerian model Oulanka - FI22: Ammonia and ammonium in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 1.0 1.0 0.8 0.8 0.6 0.6 0.4 NH3 and NH4+ in air [ug N/m3] PL 2 : Jarczew ( 180m a.s.l.) 0.4 0.2 0.0 0.2 ___ 20 ...... EMEP measurements 40 60 80 100 120 0.0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 300 320 340 360 1997 Jarczew - PL2: Ammonia and ammonium in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 12 12 10 10 8 8 6 4 NH3 and NH4+ in air [ug N/m3] SI 8 : Iskrba ( 520m a.s.l.) 6 4 2 0 2 ___ 20 ...... EMEP measurements 40 60 80 100 120 0 140 160 EMEP Eulerian model 180 200 220 240 260 280 300 320 340 360 1997 Iskrba - SI8: Ammonia and ammonium in air 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 6 6 5 5 4 4 3 3 2 2 1 1 0 0 20 40 60 80 100 120 140 160 180 200 1997 220 240 260 280 300 320 340 360 Figure 4.5 Comparison of measured and computed ammonia and ammonium concentrations in air at Oulanka, Jarczew Birkenes and Iskrba. Solid line - observations, dotted line - model results. Units: µg(N)m-3. - 26 - In case of SO4 measurements (Figure 4.2), reasonable agreement is seen in all three graphs. At Swedish station Vavihill, the episodes of high concentrations associated with advection from central Europe are well represented. Also at Payerne (Switzerland) the model fairly well captures the day-to-day variations in all seasons except winter, when the computed values are too low. The agreement between measured and computed values is not so good at Aliartos (Greece). The agreement for other stations in southern Europe - not shown here - is generally worse than in central and northern Europe. This can be explained by the gaps and poorer quality of emission data in southern Europe. Also the density of the measurement network is lower as well as the lower - on the average - quality of measurements estimated by NILU during inter-laboratory comparisons (Hjellbrekke, 1998). NO2 concentrations (Figure 4.3).are well reproduced in all three stations: Birkenes (Norway), Montelibretti (Italy) and Westerland (Germany). As in the case of SO4, good agreement is typical for most of Scandinavian stations and those located in Central and Western Europe. There is a clear seasonal course in the results at Westerland. Higher concentrations are computed for the colder period of the year. This is the result of the seasonal variations of emissions. According to NILU (Hjellbrekke, 1998), the main reason for the relatively large variations of NO2 concentrations at Montelibretti, is the influence of local NOx emission sources. In case of HNO3 and NO3- observations (Figure 4.4), a better agreement is for the Finish station Virolahti II and Lithuanian Preila, than for the Hungarian K-Puszta. The seasonal trend at KPuszta is captured by the model, but its amplitude in winter is underestimated. At Virolahti, the episodes of high concentrations are - on the average - well simulated by the model. It is not the case at Preila. The graphs for the sum of ammonia and ammonium (Figure 4.5), show considerable day to day variations. Model simulates the variations quite well at Oulanka (Finland) and in the second half of the year at Jarczew (Poland). At Iskrba (Slovenia) model simulates significant variations on a daily basis, but the variations do not exactly follow the observed ones. The computed values in the colder part of the year are underestimated. The graphs presented in this section give an insight into the model behaviour on a daily basis. The dynamics of concentration changes is frequently well captured by the model. This is particularly evident at stations in Scandinavia on occasions of long-range transport from the continental Europe. The agreement between model results and observations becomes worse when moving towards southern Europe. This conclusions holds for all five components analysed here. More plots are of this type are presented in the Appendix of the EMEP/MSC-W Report 1/99. Plots for all stations and all components can be found at: http://www.emep.int - 27 - 5. Maps of computed concentration and deposition fields for 1997 The results of the EMEP Eulerian model run for 1997 are presented in this section as concentration and deposition maps. Annual average air concentrations of sulfur dioxide, sulfate, nitrogen dioxide, nitric acid + nitrate, and ammonia + ammonium are shown in Figures 5.1, 5.2, 5.3, 5.4 and 5.5, respectively. Annual depositions of total sulfur, oxidized nitrogen and reduced nitrogen are shown in Figures 5.6, 5.7 and 5.8, respectively. In the map of computed annual mean sulfur dioxide air concentration at the surface (Figure 5.1), one can clearly see the influence of the distribution of emission sources in Europe (Mylona, 1999). Southern Italy around Sicily is the location with the absolute maximum of the computed concentrations, the same where the largest single source of both natural and anthropogenic emissions - Mt. Etna - is. A large area with high concentrations exceeding 10 µg(S)/ m3 is the so called ‘Black Triangle’ region (southern Poland, eastern Germany and northern part of the Czech Republic), where also the largest sources of anthropogenic emissions of sulfur dioxide are. Outside Black triangle, there are several other large emission sources (e.g southern U.K., northern Yugoslavia, Bulgaria, Belgium, Kola Peninsula) which are reflected in the concentration map. Overall concentration pattern computed by the Eulerian model is similar to the concentration pattern produced by the Lagrangian model for 1996 (see Appendix C of the Numerical Addendum to EMEP/MSC-W Report 1/98). However, because of the better spatial resolution of the Eulerian model (50 km instead of 150 km), more details are visible in the map computed by this model. In addition, due to fully three-dimensional structure of the Eulerian model, certain climatological and terrain features appear clearly only in the maps produced by the Eulerian model. For example, the presence of Alps appears as an area with significantly lower concentrations in the Eulerian map. This and other similar features can be seen when comparing all concentration and deposition fields produced by the two models. Computed surface concentration field for sulfates (sum of SO4 and ammonium sulfate) (Figure 5.2) is smoother than the one for sulfur dioxide. This is because unlike SO2 which is emitted, sulfates are mainly produced in the atmosphere - as a result of SO2 oxidation. The influence of emissions is not so pronounced in this case, however, regions with higher sulfate concentrations follow, to some extent, the regions with high emissions of sulfur dioxide. Concentrations exceeding 5 µg(S)/m3 are found in southern Poland, northern Czech Republic, south-western Germany (‘Black Triangle’), northern Yugoslavia, parts of Britain and Bulgaria. Map of computed annual average surface concentrations of nitrogen dioxide is shown in Figure 5.3. Again, as in the case of sulfur dioxide, concentration pattern for nitrogen dioxide is driven by the distribution of NOx emissions in Europe. However, the location of maxima is a bit different compared to maps for SO2 and sulfates. A large area with high concentrations above 5 µg(N)/m3 covers northern Germany, the Netherlands, part of Belgium and southern United Kingdom. Similar concentrations are also found in southern Poland and south-western Germany. Computed annual average surface concentrations of nitric acid + nitrate are shown in Figure 5.4. Here, we note high concentrations exceeding 2 µg(N)/m3 in and around the English Channel. Another large area of high concentrations is in the northern Italy and off the south-western coast of Spain. - 28 - Computed annual average surface concentration of ammonia + ammonium (Figure 5.5) has a very similar pattern to ammonia emissions (Mylona, 1999). Three regional maxima can be distinguished with concentrations exceeding 5 µg(N)/m3: the Netherlands and northern Belgium, southern Germany (Bavaria) and northern Italy. Concentrations above 2 µg(N)/m3 are noted in most of western and Central Europe extending from western France, through Germany, Czech Republic, Poland up to the eastern borders of Lithuania and Ukraine. Total deposition of oxidized sulfur in 1997 is shown in Figure 5.6. There is a large area with depositions above 2000 mg(S)m-2yr-1 which covers large parts of Europe. In this area, scattered local deposition maxima are in the following locations: ‘Black Triangle’, southern and central Poland, Sicily, northern Yugoslavia, Bulgaria, English Channel and central U.K., northern Yugoslavia and eastern Bulgaria. These locations coincide with the locations of the main emissions sources for SO2. Figure 5.7 shows the total deposition of oxidized nitrogen in 1997. Maxima of the deposition exceeding 1000 mg(N)m-2yr-1 can are found in the Benelux countries, western Germany, northern Italy and France, southern and central U.K, northern Czech Republic and southern Poland (Silesia). Annual total (dry + wet) deposition of reduced nitrogen is shown in Figure 5.8. The maxima of total deposition are located in western Europe: the Netherlands, northern Italy, Ireland, northwestern France and southern Germany. These are also the regions with high ammonia emissions in Europe. 120 ’97 SO2 conc. [ug/m3] 110 100 90 80 70 60 50 40 > 10.0 5.0 - 10.0 2.0 - 5.0 1.0 - 2.0 0.5 - 1.0 0.2 - 0.5 0.1 - 0.2 < 0.1 30 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.1. Map of computed annual average sulfur dioxide concentrations in 1997. Units: µg(S)m-3. - 29 - 120 ’97 SO4 conc. [ug/m3] 110 100 90 80 70 60 50 40 > 5.0 2.0 - 5.0 1.0 - 2.0 0.5 - 1.0 0.2 - 0.5 0.1 - 0.2 < 0.1 30 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.2. Map of computed annual average sulfate air concentrations in 1997. Units: µg(S)m-3. 120 ’97 NO2 conc. [ug/m3] 110 100 90 80 70 60 50 40 > 10.0 5.0 - 10.0 2.0 - 5.0 1.0 - 2.0 0.5 - 1.0 0.2 - 0.5 0.1 - 0.2 < 0.1 30 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.3. Map of computed annual average nitrogen dioxide air concentrations in 1997. Units: µg(N)m-3. - 30 - 120 ’97 HNO3 [ug/m3] 110 100 90 80 70 60 50 40 > 5.0 2.0 - 5.0 1.0 - 2.0 0.5 - 1.0 0.2 - 0.5 0.1 - 0.2 < 0.1 30 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.4. Map of computed annual average nitric acid + nitrate air concentrations in 1997. Units: µg(N)m-3. 120 ’97 NH3+NH4 [ug/m3] 110 100 90 80 70 60 50 40 > 5.00 2.00 - 5.00 1.00 - 2.00 0.50 - 1.00 0.20 - 0.50 0.10 - 0.20 < 0.10 30 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.5. Map of computed annual average ammonia + ammonium air concentrations in 1997. Units: µg(N)m-3. - 31 - 120 ’97 S dep. [mg/m2/yr] 110 100 90 80 70 60 50 40 > 2000 1000 - 2000 500 - 1000 200 - 500 100 - 200 50 - 100 < 50 30 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.6. Map of computed annual total (dry + wet) deposition of oxidized sulfur in 1997. Units: mg(S)m-2 yr-1. 120 ’97 ox.N d. [mg/m2/yr] 110 100 90 80 70 60 50 40 30 > 1000 500 - 1000 200 - 500 100 - 200 50 - 100 < 50 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.7. Map of computed annual total (dry + wet) deposition of oxdized nitrogen in 1997. Units: mg(N)m-2 yr-1. - 32 - 120 ’97 re.N d. [mg/m2/yr] 110 100 90 80 70 60 50 40 > 2000 1000 - 2000 500 - 1000 200 - 500 100 - 200 50 - 100 < 50 30 20 40 50 60 70 80 90 100 110 120 130 140 150 160 Figure 5.7. Map of computed annual total (dry + wet) deposition of reduced nitrogen in 1997. Units: mg(N)m-2 yr-1. Conclusions Several important modifications have been made in the EMEP Eulerian acid deposition model since 1998. The model has been adapted to new meteorological data produced by PARLAMPS - a dedicated meteorological model. Mass conservation properties of the model have been reviewed and updated, leading to pollutant mass conservation within 1% error, for long-term computations as required by EMEP. The model domain has been extended to account for the new countries - Parties to the CLRTAP Convention - located outside the traditional EMEP modelling domain. Moreover, as in 1998 (Olendrzynski et al., 1998), also this year an extensive evaluation of the model performance was carried out. This time, it was based on 1997 meteorological and measurement data. In addition to comparison of modelled and measured annual average concentrations in air and precipitation, model results were also compared with daily measured values. Based upon the recent updates to the model, and upon the analysis of the results of the model validation, the following conclusions can be drawn: • After several years of development, EMEP Eulerian acid deposition model has become ready for operational use. On the average, the model performs comparably or better than the EMEP Lagrangian model with regard to measured values. High precision of mass conservation makes the Eulerian model suitable for the analysis of transboundary exchange and country budgets. Higher, than in the Lagrangian model, horizontal resolution makes the Eulerian model a better tool for applications not only on regional but also on sub-regional - 33 - scales. • Scatter diagrams demonstrate that the computed annual mean air concentrations are generally within a factor of two agreement with observations in most of the EMEP stations in 1997. Only for SO2 the model tends to overestimate high concentrations close to emission sources, and to underestimate low concentrations in remote areas of Europe. • A test with fixed dry deposition velocity at 1m for SO2, showed that the agreement with measurements improves significantly for SO2, while the results for other components are except SO4 - only slightly affected. The possible cause of the inadequate performance of the dry deposition scheme is the computation of surface and quasi-laminar boundary layer resistances. A closer look into this problem is intended in the near future. • For compounds other than SO2, computed annual mean air concentrations are in relatively good agreement with observations. The difference between computed and measured air concentrations, averaged over all stations considered, varies between 1-13% with NO2 and NH3+NH4 having the best agreement. Correlation coefficient between computed and measured concentrations is rather high, varying between 0.69 and 0.87 depending on the compound. Between 82-88% of all stations are within the zone of ‘the factor of two’ difference. • Computed annual concentrations in precipitation are also in fairly good agreement with observations. The difference between computed and measured air concentrations, averaged over all stations is 43%, 3% and 14% for sulfate, nitrate and ammonium, respectively. Correlation coefficient between computed and measured concentrations is lower than for air concentrations, varying between 0.55 and 0.64. Between 74-87% of all stations are within the zone of ‘the factor of two’ difference. A still unresolved problem in the model, is the missing parameterization of the pollutant evaporation from the rain water below the clouds. This task is planned for implementation in the coming months. • Computed wet depositions are also in fairly good agreement with observations. The difference between computed and measured annual values, averaged over all stations is 3%, 30% and 28% for sulfate, nitrate and ammonium, respectively. Correlation coefficient between computed and measured wet depositions varies between 0.58 and 0.64. Between 72-90% of all stations are within the zone of ‘the factor of two’ difference. • Analysis of the daily measured and computed concentrations indicated that the dynamics of the concentration changes is frequently well captured by the model. This is particularly evident at stations in Scandinavia on occasions of long-range transport from continental Europe. Model performance for southern Europe is, in general less satisfactory than for the rest of the continent. • Examination of the concentration and deposition maps computed by the Eulerian model, and their comparison with corresponding maps produced by the Lagrangian model showed that there are more local scale details in the Eulerian maps, mainly due to better spatial resolution and multilayer structure. Lagrangian model produces smoother concentration and deposition fields but general patterns are quite similar for both models. - 34 - References Barret K. and E. Berge (1996) Transboundary Air Pollution in Europe. EMEP/MSC-W Report 1/96. The Norwegian Meteorological Institute, Oslo, Norway. Bartnicki J., Olendrzynski K., Jonson J.-E. and S. Unger (1998) Description of the Eulerian Deposition Model. EMEP/MSC-W Report 1/98. Part 2. The Norwegian Meteorological Institute, Oslo, Norway. Bartnicki J. and L. Tarrason (1998) Comparison of the Lagrangian and the Eulerian model performance. EMEP/MSC-W Report 1/98. Part 1. The Norwegian Meteorological Institute, Oslo, Norway. Bartnicki J., (1999) Computing source-receptor matrices with the EMEP Eulerian acid deposition model. EMEP/MSC-W Note 5/99. The Norwegian Meteorological Institute, Oslo, Norway. Berge E. (1993) Preliminary estimates of sulphur transport and deposition in Europe with a regional scale multi-layer Eulerian model. EMEP/MSC-W Note 1/93. The Norwegian Meteorological Institute, Oslo, Norway. Berge E. (1997) Transboundary Air Pollution in Europe. MSC-W Status Report 1997. Part 1 and 2. EMEP/MSC-W Report 1/97. The Norwegian Meteorological Institute, Oslo, Norway. Berge E. and H.A. Jakobsen (1998) A regional scale multi-layer model for the calculation of long term transport and deposition of air pollution in Europe. Submitted and accepted to Tellus. Eliassen A. and J. Saltbones (1983) Modelling of long-range transport of sulphur over Europe: a two year model run and some model experiments. Atmospheric Environment 17, 14571473. Hjellbrekke A. (1998) Personal communication. Jakobsen H.A., Berge E., Iversen T. and R. Skålin (1995) Status of the development of the multilayer Eulerian model. a) Model description; b) New method for calculating mixing heights; c) model results for sulphur transport and deposition in Europe for 1992 in the 50 km grid. EMEP/MSC-W Note 3/95. The Norwegian Meteorological Institute, Oslo, Norway. Jakobsen H. A., Jonson, J. E., Berge, E. (1996) Transport and deposition calculations of sulphur and nitrogen compounds in Europe for 1992 in the 50 km grid by use of the multi-layer Eulerian model. EMEP/MSC-W Note 2/96. The Norwegian Meteorological Institute, Research Report no 34, The Norwegian Meteorological Institute, Oslo, Norway. Jakobsen H.A., Jonson J.E. and E. Berge (1997) The multi-layer Eulerian model: Model description and evaluation of transboundary fluxes of sulphur and nitrogen for one year. EMEP/MSC-W Note 2/97. 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Performance of the Eulerian Acid Deposition Model. Chapter in MSC-W/EMEP Report 1/98. The Norwegian Meteorological Institute, Oslo, Norway. Olendrzynski K., Jonson J.E., Bartnicki J., H.Jakobsen and E.Berge (1998b). EMEP Eulerian Model for Acid Deposition over Europe. Proceeding of the 5th International Conference on Harmonization within Atmospheric Dispersion Modelling for Regulatory Purposes, Rhodes, Greece, 18-21 May 1998. Olendrzynski K., Berge E., and J. Bartnicki J., (1999). EMEP Eulerian Acid Deposition Model and its applications. European Journal of Operational Research (in print). Tsyro S. and E. Støren (1999) New meteorological model for air pollution transport models. EMEP/MSC-W Note 3/99. The Norwegian Meteorological Institute, Oslo, Norway. - 36 -