Ray J.
Yang
,
Adam G.
Xia
,
Diane V.
Michelangeli
*,
David A.
Plummer
,
Lori
Neary
,
Jacek W.
Kaminski
and
John C.
McConnell
Department of Earth and Atmospheric Science, York University, Toronto, ON, Canada M3J 1P3. E-mail: dvm@yorku.ca; Fax: +1-416-736-5817
First published on 26th September 2002
The simulated concentrations from a numerical 3-dimensional regional air quality model (MC2AQ) are compared to those of ground-based observations in north-eastern Canada and the United States. The model has oxidant chemistry for both inorganic and organic species and deposition routines driven online by a mesoscale compressible community meteorological model (MC2). A standard emission inventory of anthropogenic, natural and biogenic sources for the year 1990 for 21 atmospheric trace species was used in the simulation. The model was run for July 1999, because of the occurrence of a high ozone episode and the availability of the monitoring data for surface O3, SO2, NO, NO2 and NOx. The comparisons during the episode show that the model performs quite well for predicting concentrations and diurnal variations of the surface ozone. The predictions for other gaseous species show some discrepancies with observations, but they are consistent with the results from other models evaluated in the literature. The uncertainties in the emission inventory for these species might be the main causes of the discrepancies. Further studies are needed to improve the predictability of SO2 and NOx, especially as the model is developed to include particulate matter formation as a result of these gaseous precursors.
Usually it is difficult to quantify the direct contribution of precursor species to the pollutant concentrations. Chemical species, after being directly emitted into the atmosphere from anthropogenic and natural sources, undergo complex non-linear physical-chemical transformations, in which new species can be formed from their precursors.4 Moreover, meteorology can also play important roles in the pollution formation processes. Biswas and Rao5 and Hogrefe et al.6 pointed out that photochemical models can be very sensitive to meteorological inputs after they examined the variability in the predictions of the Urban Airshed Model (UAM-V) when the meteorological input was derived from two different meteorological models, namely, RAMS (or RAMS3b) and MM5. Hogrefe et al.6 found that such a variability can be decomposed into intra-day, diurnal, synoptic and long-term meteorological effects. The observed concentrations at a given site are therefore the comprehensive result of emissions, chemical transformations, microphysical processes and meteorological actions.
Many regional air quality models have been developed so far to study ozone, and more recently particulate matter (PM). Jacobson et al.7 developed the model GATOR for modelling ozone and PM in the Los Angeles metropolitan area.8–10 Other air quality models include CIT,11 URM12 UAM-V,13 CAMx,14 SAQM,15 MAQSIP,16,17 SMRAQ18 and Models-3.19 Comparison studies for many air quality models can be found in Russell and Dennis.20 In Canada, two air quality models have been developed: ADOM (Acid Deposition and Oxidant Model)21 and CHRONOS (Canadian Hemispheric and Regional Ozone and NOx system).22
Until now, pre-calculated meteorological fields were used to drive the transport of chemical species in most of the regional air quality models mentioned above. Such “off-line” models often include differences between the vertical and horizontal grids and sub-grid scale parameterizations can be inconsistent for temporal resolution.23 An online chemistry modeling system, in which the meteorological fields are computed concurrently with the chemistry, will have significant advantages. In this paper, we present comparisons of results obtained from the online regional air quality modeling system MC2AQ to observation data from the routine ground-based monitoring network in Canada and the United States.
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Forty-seven inorganic and organic chemical species are involved in 98 chemical reactions and 16 photolysis reactions. The gas phase chemistry mechanism is that of Version II of ADOM.21 An operator-splitting approach is used to solve the system. Initial and boundary conditions for the chemical fields in the simulation were derived from global Chemical Transport Model (CTM) results.24 Those species, which are only middle products of chemical reactions and do not appear in the CTM chemistry, were assigned near-zero values for their initial and boundary conditions.
The emissions of 1985 and 1990 have been extensively tested and proven to be a reliable dataset for regional modelling studies within the Canadian modelling community.25 Whilst the new emission inventory is now under construction, this 1990 inventory is up to now the best available data for this application.
United States | Canada | |
---|---|---|
O3 | 194 | 70 |
NO2 | 62 | 46 |
NO | 35 | 46 |
NOx | 43 | 28 |
SO2 | 148 | 38 |
Wind | 40 | 78 |
Another reason we chose observation data for July 1999 is that an occurrence of high ozone concentration at ground level is found in this month. Ozone episode formation is strongly influenced by meteorology.1 Light surface winds, a strong subsidence inversion, sunny and warm weather associated with a high pressure system will minimize the dispersion of pollutants and provide favourable conditions for the photochemical generation of ozone.1 Ozone episodes in southern Ontario occur predominately when a stationary high-pressure ridge lies to the east of the Great Lakes region. Under this condition, synoptic flow is from the south or southwest direction, placing southern Ontario downwind from regions with significant anthropogenic emissions in the American Midwest and Ohio valley. The ozone episode case in July 1999 was formed under similar conditions.
The model was run for the entire month of July 1999 during a high ozone episode in this month, with concentrations above the national standards in both Canada and the United States. The results for the period from July 10 to 22 are presented to cover three four-days states: ‘before’, ‘during’ and ‘after’ the high ozone episode. The simulated ozone concentration was obtained by using bilinear interpolation. The comparison between observations and simulations in this period will help evaluate the model performance under pre-episodic, episodic and post-episodic conditions.
Fig. 1 shows simulated ozone mixing ratios (in ppbv) at the peak of the episode, which corresponds to 2 pm Eastern Daylight Time (EDT) in eastern North America on July 17, 1999. The factors driving this ozone episode have been mentioned above. The maximum ozone level can be found along the eastern seaboard, in western Pennsylvania and in West Virginia. Ozone concentrations in the areas east of Sarnia and north of Lake Ontario exceed the 82 ppbv national standard in Canada. Fig. 2 shows the wind direction over the model domain corresponding to the conditions for Fig. 1. The prevailing winds are from the west over most of the model domain, from the southwest in southern Ontario and along the Saint Lawrence River, and from the south over the eastern seaboard. A stable high-pressure system off the eastern coast was responsible for this episode. These winds bring ozone and other chemical species into far-distance transport, which can contribute to the ‘base’ loadings of these species in downwind areas as shown in Fig. 3.
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Fig. 2 Simulated surface wind vectors (in Knots) at 2 pm (EDT) on July 17, 1999. |
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Fig. 3 Time series of ozone mixing ratios from the ground-based observations (black curve) and simulations with emissions of 1985 (red curve) and 1990 (blue curve) for selected sites in Canada and the United States in July 1999 (EDT). The vertical lines correspond to midnight every second day of the simulation. |
Fig. 3 shows the time series of ozone mixing ratios predicted with the 1985 and 1990 emission inventories and observed for eight sites among all those in the model domain. Four of them are in Canada. They are London, Toronto, Peterborough and Montreal, extending from the south-west to the north-east, representing the airshed upwind, within and downwind of major metropolitan areas. The other four sites are in the United States: New York City, Ohio Warren, Pennsylvania Centre and Pennsylvania Lawrence. These sites were selected due to their spread-out geographical extent and their high ozone levels. The comparison between the predicted and the measured mixing ratios shows that the qualitative agreements in all cases are quite good. During afternoons, ozone reaches its maximum concentration because of high photochemical production resulting from the emissions of NOx and volatile organic compounds (VOCs) in urban air. The titration process of ozone by NOx results in the decrease of ozone concentration within the areas of high NOx emissions. This is illustrated by the lower ozone concentrations in the urban regions, as shown in Fig. 1. During nights, high O3 is seldom observed because of low ozone production, net deposition, and the titration of ozone in the urban plume. The diurnal variations are well captured by the model, which suggests the ozone production and removal processes in the boundary layer are well characterized by the model.
By comparing two model predictions associated with two emission inventories, we can find that ozone levels predicted by using the emission inventory of 1985 (red curves) are in slightly better agreement with observations than those of the 1990 emission inventory (blue curve) at Canadian monitoring sites. While at monitoring sites in the United States, the 1990 emission inventory predicts better results than the 1985 emission. The old emissions lead to higher ozone predictions at high ozone levels. It should be noted that different emission processing methods are used in Canada and the United States. Although results with the two inventories underestimate ozone at peak levels, the general predicted geographical distributions and patterns for ozone agree well.
As mentioned above, mesoscale long-range transport can play an important role in determining the level of surface ozone.5,6 Such transport effects are clearly indicated at the four Canadian sites, as shown in Fig. 3. During nights, high ozone is seldom observed because of few ozone productions, net deposition, and the titration of ozone in urban plume. The only contribution to high ozone at night is from transport. Ozone levels don’t drop to low levels at night in Canadian sites compared with the four sites in the United States, especially for the period between July 16 and July 18. It is also evident that ozone transport effects at Montreal and Peterborough are greater than at Toronto and London. The north-eastward wind, as shown in Fig. 2, brings pollutants from high concentration areas in the American Midwest and Ohio valley, and therefore, increases the ‘base’ level in downwind areas during this period.
Fig. 4 shows the correlation coefficients between the simulated and the observed ozone on an-hourly basis for the eight sites of Fig. 3. The coefficients were computed for four days ‘before’, ‘during’ and ‘after’ the episode, as well as for the total period, at each location. The overall correlations are quite good for the eight sites, with total period correlations between 0.85 and 0.92 for the United States and between 0.79 and 0.86 for Canada (Fig. 4). In the United States, the best correlation seems to be during the peak in the episode when the maximum ozone concentration occurs. The correlations for the sites in the United States are in general better than those of the four Canadian locations. There is also a trend of decreasing correlation as time progresses ‘before’, ‘during’ and ‘after’ the episode in Canada. Fig. 5 shows the correlation coefficient for each site in the model domain over the total period. Most of the sites have satisfied values larger than 0.70, and many even larger than 0.8, which suggests the model has dynamically and chemically captured the main features of the oxidant chemistry. It is also interesting to note that the further a site is from the source region, for example in Quebec at the north-eastern region of the model domain, the worse the correlation. This is probably due to the meteorological uncertainties in the long-range transport of trace species as indicated by Biswas and Rao5 and Hogrefe et al.6 The wind and other meteorological fields are usually not predicted as well in the surface layer as in upper layers of the model.
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Fig. 4 Correlation coefficients calculated during four-day periods ‘before’, ‘during’ and ‘after’ the ozone episode, and for the total period in July 1999 for the eight selected sites of Fig. 3. |
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Fig. 5 Correlation coefficient for O3 from July 10 to 21, 1999. |
In addition to the correlation coefficient, the index of agreement is also introduced complementarily to evaluate the model performance.34 It is expressed as:
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To statistically evaluate model performance, two other parameters are calculated: the normalized gross error G and the normalized bias B. They are defined as
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Fig. 6 shows the geographical distribution of G in the entire domain for ozone evaluated with a cut-off of 60 ppbv. Observation–prediction pairs are often excluded if the observations are below a cut-off, typically chosen to be 60 ppbv for ozone20 based on the US EPA-recommended criteria for evaluating ozone performance.33 All sites but one have values smaller than 35%. When the cut-off is reduced to 30 ppbv, which is much lower than usually selected, there are only 9 sites with G larger than 35%, but still smaller than 40%.
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Fig. 6 Mean normalized gross error G for O3 from July 10 to 21, 1999. |
Fig. 7 gives the normalized bias B for ozone over the model domain. Most sites have B within ±15%. Russell and Dennis20 presented overall bias and gross error from seven air quality models. The biases ranged from −24% to +7.4%, and the gross errors ranged from 15% to 36%. The California Air Resources Board31 and the US EPA have established acceptable ranges for G and B for model performance evaluation, which are <35% for G and within ±15% for B. Over the entire MC2AQ domain, the values of 18.5% for G and −10.9% for B are within the acceptable ranges. It is clear that the MC2AQ performs quite well for surface ozone, especially in the regions of southern Ontario, Ohio, Pennsylvania and the New York City area.
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Fig. 7 Mean normalized bias B for O3 from July 10 to 21, 1999. |
While the primary focus of this paper is to investigate the model’s performance with respect to ozone, it is interesting to look at the predictions of other gaseous concentrations. Fig. 8 presents a summary of the correlation coefficients for NO, NO2, NOx, and SO2 over the model domain. NOx was evaluated separately from NO and NO2, because certain monitoring locations only record total NOx, and because there are possible uncertainties in the ratio of NO/NO2 in the emissions from each source. The correlation extends up to 0.8 for NO, 0.65 for NO2, 0.7 for NOx and 0.6 for SO2. The best correlations occur in the Greater Toronto Area, northern Virginia and Pennsylvania for NO2, in eastern Pennsylvania and central New York for SO2, in Toronto and New York City for NO.
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Fig. 8 Histograms of correlation coefficients for NO, NO2, NOx, SO2, wind speed and wind angle agreement within 30 degrees between the observations and the model results from July 10 to 21, 1999. |
While the correlations for these gases seem not as good compared to those for ozone, they nevertheless are within the ranges obtained by others. For example, Biswas et al.32 obtained a correlation of about 0.2 with a maximum of 0.4 for NOx in their unfiltered data in the RAMS/UAM-V model evaluation. Russell and Dennis20 showed a systematic under-prediction of NOx by the models and indicated that there seems to be a tendency of the models to convert NOx too rapidly to NOy. The correlation value of this work is quantitatively similar to their results at most of the sites, except for the over-predictions of NOx for the sites around New York City. Compared with the 1985 emission inventory, predictions of NOx have been improved around the Great Toronto Area, and the SO2 predictions have been improved around Montreal.
The reason that modelled NOx deviates from observations is that measurements are made near the sources where the model emission schemes will never be able to reproduce small-scale fluctuations observed. Diurnal temporal variations of NOx and SO2 emissions can also account for the poor predication of these species.32 Sub-grid scale variability in emissions will have a major impact on the comparison between the model and observations. When only observations between 2 and 6 pm are considered, the correlation coefficients for NOx improve, with 18 stations having values between 0.5 and 0.7, compared to only 8 when the entire day is analyzed. This is a reflection of the fact that in the afternoon, the lower atmosphere is well mixed, which minimises the uncertainties in sub-grid scale variability. Further work to improve the predication for these species is necessary in order to model accurately the secondary formation of nitrate and sulfate with the regional air quality model. If the precursor emissions are not adequately represented in the model, or the precursor chemistry is not correctly simulated, the predictive capability of the model for PM will be reduced significantly.
The meteorological prediction of the model has been extensively studied by the original MC2 group.27 The purpose here is to provide a level of confidence in the predictions of wind speed and direction as they relate to the gas phase concentrations predicted by the model. Thus Fig. 8 presents a histogram of the correlation coefficient of the wind speed over the entire domain. The correlation extends to 0.75, with a maximum between 0.2 and 0.6. Fig. 8 also presents a histogram of the fraction of hours at each site where the difference between the observed wind direction and that predicted by the model is less than 30 degrees. The poorest correlations for winds occur around the Great Lakes. This is likely due to poorly resolved lake breeze circulation in that region, which would require much higher horizontal spatial resolution (e.g. Plummer24). The study of the effects of the lake breeze circulation at high resolution with MC2AQ is underway.
This journal is © The Royal Society of Chemistry 2003 |