long-term simulations of photo oxidant pollution over portugal using the chimere model
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Atmospheric Environment 39 (2005) 3089–3101
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Long-term simulations of photo oxidant pollution overPortugal using the CHIMERE model
A. Monteiroa,�, R. Vautardb, C. Borregoa, A.I. Mirandaa
aDepartamento de Ambiente e Ordenamento, Universidade de Aveiro, Aveiro 3810-193, PortugalbLaboratoire de Meteorologie Dynamique, Ecole Polytechnique, F-91128 Palaiseau cedex, France
Received 5 August 2004; received in revised form 12 January 2005; accepted 19 January 2005
Abstract
This work examines the performance of the CHIMERE photochemical model in simulating ozone and nitrogen
dioxide in Portugal over a long-term summer period. The analysis focuses on comparisons against the available
measurements during the 2001 summer season. The meteorological forcing of the model is given by the European
Centre for Medium-Range Weather Forecasts (ECMWF), and the emission inventory used was obtained with a top-
down methodology updated for the simulation year.
Despite the coarse resolution of the meteorological data, the complex topography and coastal location of Portugal,
the results obtained show that the modelling system is able to reproduce the nitrogen dioxide and ozone episodes that
occurred during the simulated summer period. Mean error and correlation improve when considering the sum of photo
oxidant instead of individual pollutants, indicating that a significant part of the model error is due to either the lack of
representativeness of monitoring stations or to inaccuracies in the emission inventory.
r 2005 Elsevier Ltd. All rights reserved.
Keywords: Regional; Modelling; Validation; Ozone; Nitrogen dioxide
1. Introduction
Measured concentrations available at given monitor-
ing sites are generally not numerous enough to describe
the spatial distribution of ozone and other pollutants
over wide areas, whereas this information is a crucial
factor to evaluate the impact of photochemical pollution
on human health and natural ecosystems. Numerical
modelling systems can represent suitable tools for these
purposes, allowing both the study of photochemical
pollution with an adequate spatial detail and the
assessment of appropriate emission reduction strategies.
e front matter r 2005 Elsevier Ltd. All rights reserve
mosenv.2005.01.045
ing author. Tel.: +351 234370200;
29290.
ess: [email protected] (A. Monteiro).
In order to assess the comprehensive effects of
photochemical pollution, not only ozone peak concen-
trations need to be examined, but also ozone exposure
on the ‘‘seasonal’’ scale needs to be quantified. Recent
works (Sistla et al., 2001) point out the importance to
perform policies analysis on a ‘‘climatological’’ basis
rather than focusing on a single critical episode; this
approach allows to better evaluate model performances
(Hogrefe et al., 2001) and to quantify policies effects
with respect to long-term air quality standards. Several
ozone modelling studies were already performed for
Portugal, for b-mesoscale domains and during some
specific and episode days (Barros et al., 2003; Borrego et
al., 2000, 2002). Large scale simulations including
Portugal have also been done, but with a coarse grid
resolution. The present work represents an important air
d.
ARTICLE IN PRESSA. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–31013090
quality modelling study for Portugal, since it aims to
assess the quality of photo oxidant pollution simulations
over the whole continental region of Portugal and
during a long time period, the summer season of 2001.
The paper is organized as follows: Section 2 is devoted
to a brief and general model description. Section 3
describes the model experiment performed over Portu-
gal. Section 4 contains the results, and Section 5 a
conclusive summary.
2. Model description
CHIMERE is a three-dimensional chemistry-trans-
port model (CTM), based on the integration of the mass
continuity equation for the concentrations of several
chemical species in each cell of a given grid (Schmidt et
al., 2001). CHIMERE has been used for several research
applications, among which include sensitivity to anthro-
pogenic or biogenic emissions (Beekmann and Derog-
nat, 2003; Menut, 2003; Sillman et al., 2003; Derognat et
al., 2003; Schmidt and Martin, 2003), emission diag-
nostics (Vautard et al., 2003) or photo-oxidant forecast-
ing over Europe and the Paris region (Vautard et al.,
2001). From the year 2000–2003, a web server displayed
these real-time forecasts together with surface observa-
tions for verification (http://euler.lmd.polytechnique.fr/
pioneer). Results showed reasonable skill for ozone daily
maxima forecasts with average root mean square (RMS)
error of about 10 ppb and 0.8 of correlation, which is in
agreement with the ozone forecast model intercompar-
ison experiment described by Tilmes et al. (2002).
Let us first briefly recall the physical and chemical
processes included in the model. The model version used
here is primarily described by Schmidt et al. (2001), and
further updates, especially for the smaller-scale version,
can be found in the work by Vautard et al. (2003) and on
the web site http://euler.lmd.polytechnique.fr/chimere,
where the model can be downloaded with some
documentation. Horizontal transport is taken into
account by calculating pollutant flux convergence from
the boundaries of each model cell. The numerical
scheme used to interpolate fluxes at cell boundaries is
the Parabolic Piecewise Method (Collela and Wood-
ward, 1984), for slow species (ozone and precursors),
and a first-order scheme is used for the other species.
Vertical transport is assumed to balance horizontal mass
divergence/convergence. Turbulent mixing is calculated
using a Kz formulation, following Troen and Mahrt
(1986) without a counter gradient term for chemical
species.
The chemical mechanism uses 44 species and 116
reactions and was derived from the original complete
scheme MELCHIOR (Lattuati, 1997). In order to
reduce the computing time it follows the formalism of
‘‘chemical operators’’ (Aumont et al., 1997). The
hydrocarbon degradation is fairly similar to the EMEP
gas phase mechanism (Simpson, 1993). Adaptations are
made in particular for low NOx conditions and NO3
nitrate chemistry. All rate constants are updated
according to Atkinson et al. (1997) and DeMore et al.
(1997). The impact of cloud on photolytic reaction rates
is included in a highly parameterized fashion: in the
presence of clouds a radiation attenuation coefficient is
taken into account throughout the model layers. Dry
deposition is parameterized as a downward flux from the
lowest model layer. The deposition velocity is described
through a resistance analogy (Wesely and Hicks, 1977).
The numerical method for the time solution of the stiff
system of partial differential equations is the second-
order TWOSTEP algorithm originally proposed by
Verwer (1994).
3. Model application
3.1. Simulation domain and resolution
The model is applied to the Continental region of
Portugal, as shown in Fig. 1, with a horizontal domain
of 290� 580 km and a 10 km horizontal resolution, and
during the entire ozone season of 2001, from 1 May to
31 August. Vertical grid consists in six hybrid sigma-
pressure layers with a model top at 700 hPa. The top
altitudes of the layers vary with time, but their
approximate values are, from bottom to top: 50, 250,
600, 1200, 2000 and 3000m.
An attempt is made to differentiate concentrations
near the emission sources (like for traffic monitoring
station) and ‘‘background’’ concentrations. The model
surface layer (the lowest layer), in each horizontal cell, is
divided into two disjoint volumes: an emission volume
and a background volume. The ‘‘emission volume’’ is
assumed to occupy 10% of the total volume of the total
surface cell. All surface emissions are sent into the
emission volume while no emission is sent in the
background volume. Emissions from high (450m)
point sources are sent into Layer 2 of the model. The
emission volume exchanges air and pollutants with the
background volume, with a constant mixing time scale
of 15min, which enables the mixing of fresh emissions
with background air. This time scale was empirically
tuned over the Paris area in a previous study, in such a
way that the model average concentrations over traffic
monitoring stations match the observed ones. In the
emission layer no horizontal transport takes place. This
parameterization of the exchange is rather crude but
allows a clear distinction between background and near-
source concentrations. Sensitivity tests showed that
background concentrations are not very sensitive to
the mixing time scale. By contrast, concentrations in the
emission layer are sensitive to the mixing time scale,
ARTICLE IN PRESS
Fig. 1. Simulated domain for Continental Portugal (290� 580km) and the location of the air quality stations with available data for
the simulated time period, with a zoom into the Lisbon and Porto urban areas.
A. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–3101 3091
since mixing is the only process driving dispersion in this
volume (no transport assumed).
3.2. Meteorological data
The meteorological input variables are taken, as by
Schmidt et al. (2001), from ECMWF 3-hourly short-
term forecasts: 3D-dimensional fields of horizontal wind
(u and v), temperature, specific humidity, cloud liquid
water content, and two-dimensional fields of surface
pressure, heat fluxes, 2m temperature and cloud cover.
The ECMWF operational short-term forecasts are
extracted on a 14degree grid but have a T511 resolution,
that is, structures with total spherical wavenumbers
larger than 511 are not represented (effective resolution
of about 12degree). Forecast fields are linearly inter-
polated to the CHIMERE grid and linear time inter-
polation is also applied to obtain hourly values.
3.3. Boundary and initial concentrations
The Portugal model run is nested within a continen-
tal-scale run, using the same physics and a simple one-
way technique: the coarse grid long-term simulation is
performed with CHIMERE over a regional area from
10.5 W to 22.5 E and from 35 N to 57.5 N. Monthly
climatologies of O3, NO2, CO, PAN, CH4, C2H6,
HCHO and HNO3 taken from the MOZART second-
generation model (Horowitz et al., 2003) are forcing this
continental-scale simulation at the lateral and top
boundaries. The comparison between the monitoring
background data and the climatotological MOZART
values, shows that these values used as boundary
conditions are on average 1.6 times superior to the
observed ozone data and 3% of the NO2 monitored
data, which indicates the importance of the emissions
input and the dispersion photochemical processes
simulated by the CTM. Therefore, the large-scale run
concentrations of 22 slow species including ozone and
precursors (VOC and reactive nitrogen species) are
passed as lateral boundary values to the small-scale run.
As the Portugal model top is as high as the continental
version, its top boundary concentrations used are also
the MOZART monthly climatological values. The
simulation is continuous in time and a spin-up period
of 10 days is considered before any statistics on the
results are calculated. The spin-up period is also
initialized with the MOZART climatological values.
ARTICLE IN PRESS
Fig. 2. Spatial distribution of NMVOC industrial and NOx
traffic emissions, respectively, resulting from the top-down
methodology applied to the national EMEP inventory.
A. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–31013092
3.4. Emission data
The CHIMERE model requires the input of emission
for 15 primary compounds: NO, NO2, HONO, SO2,
CO, Ethane, n-Butane, Ethene, Propene, Isoprene, a-pinene, o-xylene, Formaldehyde, Acetaldehyde, Methyl
ethyl Ketone. At European scale, emissions were derived
from the annual totals of the EMEP database for 1999,
through a methodology similar to that described by
Schmidt et al. (2001). Over the Portuguese domain, area-
source annual emission data for the four anthropogenic
species NOx, SO2, CO and NMVOC are obtained from
the Portuguese EMEP database for the reference
simulation year (2001) for each pollutant activity
(traffic, solvents, industrial and residential combustion
and others) and then spatially disaggregated in order to
obtain the resolution required by the small-scale model.
The disaggregation is made in two steps. First, emissions
are estimated at municipality level using adequate
statistical indicators for each pollutant activity (types
of fuel consumption) and then processed applying
Census data in order to obtain sub-municipal resolution
(Borrego et al., 2002). Examples of the emissions spatial
distribution estimated from this approach are showed in
Fig. 2.
Both maps show that most of the emissions are
concentrated along the western coast of Portugal, where
the two main urban centres of Lisbon and Porto are
easily located. The traffic sector represents, compared to
industrial activities, a major source of air pollution
(Borrego et al., 2002).
The annual emissions of large point sources were
obtained directly from the available monitoring data of
each industrial plant.
Time disaggregation is obtained by the application of
monthly, weekly and hourly profiles from the University
of Stuttgart (GENEMIS, 1994). The NMVOCs are
disaggregated into 227 individual VOCs according to the
UK speciation (Passant, 2000) for each activity sector
above referred, before being grouped into the model
VOCs using the standard procedure of Middleton et al.
(1990).
The methodology for biogenic emissions of isoprene
and terpenes is described by Schmidt et al. (2001). The
land use database comes from the Global Land Cover
Facility (Hansen et al., 2000), which after some
processing provides the cell by cell coverage of
coniferous and broadleaf forests. The spatial distribu-
tion of tree species within these classes is established
following the methodology outlined by Simpson et al.
(1999). The Stohl et al. (1996) methodology is used for
biogenic emissions of NO from fertilized soils.
3.5. Observations
The Portuguese national air quality network includes
32 stations, of which 14 are background, 13 traffic and
five are industrial stations, according to the European
Environment Agency criteria. However, for the simu-
lated period, only 21 stations had uninterrupted
monitored data. These stations are mainly concentrated
in the two main coastal urban areas (Fig. 1): Lisbon
(eight stations) and Porto (six stations).
4. Results and discussion
As in previous ozone model evaluations (Simpson,
1993), daily maximum ozone values were used as the
basis of statistical evaluation. The comparison is made
using time series, scatter plots and the calculation of
RMS errors and correlation coefficients for each
observation site.
Besides that, the original time series was split into
different spectral components allowing the identification
of the time scales that are responsible for the correlation
structure in the original data, determining which
processes are poorly represented and helping further
model developments. The observed O3 hourly excee-
dances (to the standards settled in the 2002/3/EC
Daughter Directive) were also compared to the model
predictions in order to identify and analyze the origin of
these ozone episodes. During Summer 2001, the thresh-
old for public information (180mgm�3 hourly average)
that can cause health risks for short time exposure of
groups particularity sensitive, was exceeded 64 times.
Also the threshold for public alert (240mgm�3 for three
consecutive hourly averages), above which health risks
for short time exposure of the population are expected
was exceeded two times at Teixugueira station.
ARTICLE IN PRESS
Table 1
Mean values, RMS error and the correlation coefficient for each station, for the NO2, O3 and Ox species
Station Name Type Mean values (mgm�3) RMS error (mgm�3) r correlation
O3 NO2 Ox O3 NO2 Ox O3 NO2 Ox
Lavradio Industrial 46.2 30.8 39.2 27.9 34.7 17.9 0.6 0.4 0.6
Teixugueira Industrial 49.0 13.4 31.5 33.0 31.4 18.0 0.8 0.1 0.8
Monte chaos Industrial 43.8 6.4 25.3 36.4 11.0 21.3 0.5 0.2 0.5
Santiago cacem Industrial 59.5 3.1 31.4 39.1 13.8 21.6 0.5 0.0 0.6
Lec-a Rural 45.0 21.4 34.2 18.7 43.2 16.2 0.8 0.4 0.7
Avanca Rural 52.0 13.9 33.3 23.1 15.5 10.9 0.8 0.2 0.8
Monte velho Rural 75.5 3.6 39.1 32.4 12.3 16.8 0.5 0.1 0.5
Ermesinde Suburban 50.7 28.8 40.4 21.2 27.0 13.0 0.8 0.6 0.8
Vila nova Telha Suburban 45.7 16.7 31.0 23.1 36.9 16.2 0.7 0.6 0.8
Beato Suburban 61.3 14.3 38.2 26.9 55.4 16.4 0.8 0.7 0.8
Custoias Suburban 37.1 19.3 27.5 29.0 48.7 25.6 0.7 0.6 0.8
Reboleira Suburban 65.4 14.1 39.4 33.6 54.1 14.3 0.7 0.8 0.8
Alfragide Suburban 71.0 33.6 53.2 37.7 37.6 19.0 0.6 0.7 0.7
Loures Urban 59.7 8.0 34.1 18.1 31.3 10.4 0.8 0.7 0.8
Paio pires Urban 56.1 20.0 38.4 23.0 41.7 14.4 0.8 0.6 0.8
Laranjeiro Urban 53.0 29.6 42.0 30.4 41.1 15.9 0.7 0.6 0.7
Entrecampos Traffic 36.1 22.0 29.6 13.2 42.7 22.4 0.8 0.7 0.8
Hospital velho Traffic 39.8 22.1 31.6 15.4 61.4 29.2 0.8 0.0 0.3
Feup Traffic 33.5 n.a. n.a. 19.4 n.a. n.a. 0.6 n.a. n.a.
Formosa Traffic 38.6 42.1 40.8 21.5 34.4 17.7 0.7 0.6 0.8
Coimbra Traffic 27.8 50.7 38.9 45.2 56.9 14.6 0.5 0.1 0.7
Average 54.4 17.3 36.1 28.3 33.5 16.7 0.7 0.5 0.7
n.a.:not available.
0
0.2
0.4
0.6
0.8
1
0 30
Nor
mal
ized
err
or 12/07
13/0729/07
27/08
days1209060
Average Error for all the stations
07/08
Fig. 3. Normalized absolute bias for the daily ozone peak,
average for all the stations, during the simulated period.
A. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–3101 3093
4.1. Error statistics
The RMS error and the correlation coefficients (r-
values), calculated from the daily maximum ozone
concentrations, for each station and for NO2, O3 and
Ox (sum of O3 and NO2) species are listed in Table 1.
Despite the RMS error quite high for some stations,
the simulation exhibits a correlation between 0.5 and 0.8
for O3 and Ox at all monitoring sites. Both the RMS
error and correlation coefficient indicate a better model
performance for O3 than for NO2, since this latter
pollutant is generally more sensitive to errors in
emissions and meteorology, especially under stagnant
conditions. Statistical scores are significantly improved
if Ox is considered instead of each pollutant separately.
In fact, Ox is much less sensitive to emissions and their
uncertainties because it is not affected by the fast
photostationary equilibrium between NO, NO2 and O3.
Thus, an error in NO emissions can dramatically change
individual compounds concentrations but not Ox.
Another type of difficulty that can arise is related to
the representativeness of monitoring locations: if for
instance, a station is located close to a NOx source not
representative of the model grid cell, ozone concentra-
tion could be overestimated and NO2 concentration
could be underestimated by the model while Ox should
not be affected by this problem.
The analysis by station type reveals that relatively
large errors exist for industrial stations (namely Monte
Chaos and Santiago Cacem) perhaps due to an incorrect
estimation of point sources emissions or to representa-
tiveness problems. The RMS error is much lower when
considering Ox instead of ozone. However, the correla-
tion is poor even for Ox for three of these four stations.
Traffic stations values are compared with the model’s
emission sub-layer (polluted layer) results. They exhibit
reasonable scores for ozone, both in terms of RMS and
ARTICLE IN PRESSA. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–31013094
correlation, but NO2 is poorly simulated. For two of
these stations the Ox scores are lower than the ozone
scores, mostly because the Ox peak variability is
dominated by NO2 variability. By contrast, the station
of ‘‘Coimbra’’ has the highest RMS error and lowest
correlation for ozone and NO2, but Ox is fairly well
simulated. This station is located on the main avenue of
the City of Coimbra and is affected by the local titration
of ozone by NO emissions. Still the Ox peak variability is
largely due to ozone, hence the behaviour is different to
the above two stations.
There should not be any representativeness problem
for suburban stations. However, large RMS errors for
O3 are found for Reboleira and Alfragide (33.6 and
37.7mgm�3, respectively). These statistics are difficult to
understand and cannot be interpreted without further
information on the observation sites. For these two
stations the Ox simulation has RMS below 20 mgm�3
and reasonable correlations, indicating possible
influences of local NOx sources. These stations also
exhibit a large variability due to occurrences of intense
ozone plumes. When such variability exists, a low
ozone RMS is difficult to obtain because errors are
also large. The complex nature of the flow in
coastal areas, which cannot be taken into account
by the coarse meteorological model grid, could also be
at least in part responsible for the particularly
high RMS. The model performs reasonably well
with ozone and Ox peaks at the three urban stations
and two of the rural stations. For the last rural
station (Monte Velho), the RMS of the Ox errors
is much smaller than the RMS of the ozone errors,
again indicating a possible representativeness problem.
The poor correlations show that this cannot be the
only problem. Again, ozone simulation at this
coastal station could suffer from insufficiently resolved
winds.
In order to analyze the global performance of the
model, the mean normalized absolute bias error
(1=NPN
1¼1jCobs � Csimj=Cobs; considering the N stations
and daily peak ozone concentrations) is plotted versus
time, in Fig. 3. During most of the days, this normalized
error remains below 0.4. However, there are 5 days with
high errors, identified in the graph. A meteorological
analysis shows similar synoptic conditions in all these
days: a low thermal pressure at surface together with an
anticyclone at 500 hPa covering the Iberian Peninsula.
Backtrajectories analysis shows that in all these 5 days
the air was coming from the Atlantic, in agreement with
the air quality background conditions given to the
model. This suggests that the meteorological model
could not simulate correctly these specific conditions or
an insufficient vertical resolution of the CHIMERE
model exists. The use of a more detailed mesoscale
meteorological model will be the focus of future
developments.
In addition to the RMS error and correlation
coefficient other statistical parameters are recommended
by the US Environment Protection Agency (USEPA,
1996) in order to evaluate the performance of photo-
chemical models:
�
Unpaired highest-prediction accuracy (Au )Au ¼coð:; :Þ � cpð:; :Þ
coð:; :Þ100%,
�
Normalized bias test (Dk)Dk ¼1
N t
XN
i¼1
XHi
j¼1
coði; jÞ � cpði; jÞ
coði; jÞ;
�
Gross error of all pairs 4120 mgm�3(Ed)Ed ¼1
N t
XN
i¼1
XHi
j¼1
coði; jÞ � cpði; jÞ
coði; jÞ,
where Coð:; :Þ is the maximum 1-h observed concentra-
tion over all hours and monitoring stations; Cpð:; :Þ is
maximum 1-h predicted concentration over all hours
and surface grid plumes; Coði; jÞ is observed value at
monitoring station i for hour j; Cpði; jÞ is predicted value
at monitoring station i for hour j; N is number of
monitoring stations; Hi is number of hourly predictio-
n–observation pairs for monitoring station i; N t is total
number of station hours.
When considering all stations and simulated hours, Au
has a value of 19.8, Dk a value of �15.7 and E a value of
8.2. Tesche et al. (1990) state that, based on past
photochemical model evaluations acceptable models
produce peak (unpaired) prediction accuracy, overall
bias, and gross error statistics in the approximate ranges
of 715–20, 75–15 and 730–35%, respectively. The
estimated performance indices fall within these ranges
showing that the model behaviour is acceptable for air
quality management. The lower value of the E indice
reveals that the model has a particularly good ability to
predict higher and peak ozone concentrations.
4.2. Time series and scatter plots
Time series and scatter plots belong to the standard
methods for the comparison of model results with
observations. Time series for a selection of four
‘‘representative’’ sites, chosen to cover the different type
of monitoring stations, are presented in Fig. 4. The
model is in general able to simulate the daily maximum
ozone variability. It reproduces the episodic events of
high ozone mixing ratios. This holds in particular for the
remote sites with rural and suburban background
stations like Avanca and Ermesinde, and also for traffic
ARTICLE IN PRESS
FORMOSA(traffic)
0 30 60 90 1200
50
100
150
200
250
0
50
100
150
200
250observedmodeled
LAVRADIO(industrial) observed
modeled
AVANCA(rural background)
0
50
100
150
200
250
0
50
100
150
200
250observedmodeled
ERMESINDE(suburban background)
observedmodeled
NO
2 (�
g. m
-3)
NO
2 (�
g. m
-3)
days0 30 60 90 120
0 30 60 90 120 0 30 60 90 120
days
Fig. 5. Observed and modelled maximum daily NO2 concentration for different types of monitoring stations.
AVANCA(rural background)
0 30 60 90 120
0 30 60 90 120
0 30 60 90 1200
50
100
150
200
250observedsimulated
ERMESINDE(suburban background) observed
simulated
FORMOSA(traffic)
0
50
100
150
200
250observedsimulated
LAVRADIO(industrial)
0
50
100
150
200
250
0
50
100
150
200
250
observedsimulated
O3
(�g.
m-3
)O
3 (�
g. m
-3)
days0 30 60 90 120
days
Fig. 4. Observed and modelled maximum daily ozone concentration for different types of monitoring stations.
A. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–3101 3095
stations located in urban areas with lower ozone
concentrations. Monitoring sites close to larger indus-
trial sites like Lavradio exhibit larger differences
between observed and modelled ozone peak values.
The time series point out differences in the model
performance for each episode. During the two large
episodes around 29 May and 1 August, there is an
overall tendency to overestimate the ozone peak.
Conversely, around 20 June the model underestimates
the O3 episode values.
In Fig. 5 the same analysis for the NO2 species is
presented. Simulations show a reasonable agreement
with the observed data for all the different station types.
The mean, variability, and the differences of variability
ARTICLE IN PRESS
FORMOSA(traffic)
0 30 60 900
50
100
150
200
250
0
50
100
150
200
250
0
50
100
150
200
250
observedmodeled
LAVRADIO(industrial) observed
modeled
AVANCA(rural background) observed
modeled
ERMESINDE(suburban background) observed
modeled
Ox
(ppb
)
0
50
100
150
200
250
Ox
(ppb
)
days
120 0 30 60 90days
120
0 30 60 90 120 0 30 60 90 120
Fig. 6. Observed and modelled maximum daily Ox concentration for different types of monitoring stations.
A. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–31013096
of simulated maxima are coherent with that observed,
even though there may be strong errors in individual
daily maxima simulated amplitudes. As in the previous
ozone plots, the industrial site of Lavradio exhibits the
highest departures between observed and modelled
maximum NO2 concentration values.
Fig. 6 presents the time series plots for the Ox daily
maxima. The improvement of the results is clear, as
compared to the O3 and NO2 daily maxima plots. The
correspondence between observed and modelled values
is much closer even for the industrial site, where the O3
and NO2 plots show significant errors. It is interesting to
notice that, in the Ox time series, the relatively large
errors on the ozone ‘‘background level’’ given by the
lowest daily maxima, disappear. This could be an
indication of the lack of representativeness of the
station, which may be influenced by local sources.
The scatter plots for some of the ‘‘representative’’
stations (Fig. 7) reveal perhaps the most important
feature of model errors: despite the spread of points
around the diagonal, there is a general tendency to
overestimate the ozone concentrations, which could be
due to a model bias or an overestimation of boundary
concentrations. However, an opposite behaviour exists
for O3 at the urban and traffic stations, like Beato and
Formosa. The corresponding scatter plots show a
general slight underestimation of the ozone values
mainly for the extreme values, so the model variability
is smaller than the observed one. This can be due to the
horizontal model grid size, insufficient to resolve city
plumes. Once again, the scattered plots examples of Fig.
7 confirm the clear improvement of the model perfor-
mance when considering Ox correlation results ðr40:70Þinstead of ozone or nitrogen dioxide individually. The
worst performance is obtained for NO2 ðr40:41Þ; for allmonitoring stations types, where in general NO2 is
overestimated.
4.3. Time series spectral decomposition
Since this is a longer-term modelling application, it is
advisable to split and evaluate the model performance
(accuracy) at different time scales with specific frequen-
cies ranges and fluctuations. Following the methodology
presented by Hogrefe et al. (2001), ozone hourly time
series were spectrally decomposed into four specific time
series periods with characteristic processes affecting
ozone concentration, namely intra-day component
(ID), diurnal component (DI), synoptic component
(SY) and the longer-term (baseline) component (BL),
which are related to the log-transformation (P) of the
original time series by: PðtÞ ¼ eIDðtÞeDIðtÞeSYðtÞeBLðtÞ:InTable 2, the distribution of the variance between the
time series components for both observation and model
results (considering all the monitoring stations) are
presented. The model predicts a variance distribution
that is very close to the observations. In both cases the
DI is the largest contributor to the overall variance (as it
was expected, since this DI includes the day and
nighttime differences), followed by the synoptic, baseline
ARTICLE IN PRESS
O3BEATO
(suburban background)r = 0.76
NO2BEATOr = 0.73
OxBEATOr = 0.75
O3FORMOSA
r = 0.69
NO2FORMOSA
0
50
100
150
200
250
r = 0.58
OxFORMOSA
0
50
100
150
200
250
r = 0.79
O3LAVRADIO(industrial)r = 0.59
NO2LAVRADIO
0 50 100 150 200 2500 50 100 150 200 250 0 50 100 150 200 250
0 50 100 150 200 250
0 50 100 150 200 2500 50 100 150 200 2500 50 100 150 200 250
0 50 100 150 200 2500 50 100 150 200 250
0
50
100
150
200
250
r = 0.41
OxLAVRADIO
0
50
100
150
200
250
r = 0.63
O3LEÇA
(rural background)
0
50
100
150
200
250
r = 0.78
NO2LEÇA
0
50
100
150
200
250
r = 0.42
OxLEÇA
0 50 100 250
Mod
eled
dat
a
Mod
eled
dat
a
Mod
eled
dat
a
0
50
100
150
200
250
Mod
eled
dat
a
0
50
100
150
200
250
Mod
eled
dat
a
0
50
100
150
200
250
Mod
eled
dat
a
0
50
100
150
200
250
Mod
eled
dat
a
0
50
100
150
200
250
Mod
eled
dat
a
Mod
eled
dat
a
Mod
eled
dat
a
Mod
eled
dat
a
Mod
eled
dat
a
0
50
100
150
200
250
r = 0.73
Observed data150 2000 50 100 250
Observed data150 2000 50 100 250
Observed data150 200
(traffic)
Fig. 7. Scatter plots for simulated versus observed daily maxima of O3, NO2 and Ox mixing ratios in mgm�3 for the period from 1 May
to 30 August 2001.
Table 2
Relative contribution (%) of the components time series
variances to the total variance for observations and model
predictions, the sum of the components variances and the
original time series variance
Observations Model prediction
ID DI SY BL Sum Original ID DI SY BL Sum Original
10 46 27 17 0.99 0.82 8 51 26 14 1.25 1.00
Table 3
Correlation coefficient and ratio of variances (modelled to
observed) for the different time series components (original
time series and intra-day, diurnal, synoptic and baseline
components)
Correlation coefficient Ratio of variances (model/observed)
Original ID DI SY BL Original ID DI SY BL
0.60 0.38 0.69 0.55 0.59 1.23 0.96 1.42 1.29 1.02
A. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–3101 3097
ARTICLE IN PRESSA. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–31013098
and ID. However, there is a slight underestimation of
the ID and a more significant overestimation of the
diurnal time scales.
Table 3 lists the correlation coefficient and ratios of
the variances of the modelled to observed for each time
series component (for all the monitoring stations and for
the entire simulation length), in order to compare the
absolute amount of energy at the different time scales
between observations and model predictions. It can be
seen that the model overestimates the variance of the
original, diurnal and synoptic time series, but slightly
underestimates the intra-day time scale. The baseline
variance (its amount of energy) is the best captured by
the model. The variability of the DI (the largest
contributor to the overall variance) is the most over-
Fig. 8. Ozone concentration fields for the episode days occurred dur
name, the time and the registered exceedance value.
estimated, suggesting that the model does not properly
capture all processes that characterize the diurnal cycle
and that are associated with the diurnal variation of the
solar flux (differences between daytime photochemical
production and nightime consumption of ozone, as well
as the diurnal cycle of boundary layer evolution and
decay).
The correlation for the ID is less than 0.4, suggesting
that despite the good variance agreement, the processes
contributing to the high-frequency fluctuations (hori-
zontal turbulence and vertical mixing, local titration by
fresh emissions of NO and ozone response to fast-
changing emission patterns during the rush traffic hours)
in the ID are not captured by the model. The high
correlations for the DI are due to the inherent diurnal
ing the simulated period. In each map are indicate the station
ARTICLE IN PRESSA. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–3101 3099
cycle caused by the day and night differences. However,
when the night and day period are evaluated separately,
the correlation factor is significantly low for the night
period (0.43 for the night and 0.73 for the day). The
synoptic and baseline components display similar
correlations higher than 0.55. These results combined
with the variance analysis suggest that the longer time
scales are represented quite well by the model, which
means that the model is able to reproduce the changing
synoptic conditions and capture the seasonal variation
of the solar flux, changing large-scale flow patterns and
changes in vegetation coverage and biogenic emissions.
4.4. Concentration fields patterns
In Fig. 8 is displayed the spatial ozone concentration
fields at some specific hours of episodic days where
ozone exceedances occurred during the simulated
period. In almost all cases the ozone exceedances are
well reproduced by the model. However, there are large
areas of inland Portugal where the simulated ozone
exceedances cannot be verified due to the absence of
monitoring sites. The concentration patterns show that
there is a potential advection and transport of the
pollutants emitted from the major urban centres (Porto
and Lisbon) to the coast and to some inland parts of
Portugal. This can be confirmed and more deeply
analyzed with mesoscale meteorological simulations
performed in this specific regions (Barros et al., 2003;
Borrego et al., 2000).
5. Summary and conclusions
The results of a long-term simulation of photo
oxidant pollution over Continental Portugal are pre-
sented. The CHIMERE CTM is used and forced by
ECMWF weather forecasts, which is a considerable
simplification with respect to using a mesoscale meteor-
ological model, especially for the Portuguese area where
topographic and coastal effects are important.
The validation procedure consists in comparing the
simulation results with observation values obtained
from ground-based monitoring stations over the whole
summer season of 2001, from 1 May to 31 August, using
error statistics such as root mean square error, correla-
tion coefficients and the EPA statistical parameters, and
qualitative comparisons with time series and scatter
plots. Both the RMS error and correlation coefficients
indicate that the differences between observed and
modelled values are considerably lower when analysing
the sum of photo-oxidants, Ox, than when analysing O3
and NO2. This indicates that a large part of the error in
ozone simulation could be due to the representativeness
of stations in the model grid cells or to emissions
estimation errors. In all cases, the errors deal with the
rapid conversion between ozone and NO2. The ozone
RMS errors range from 13.2 to 45.2mgm�3, with an
average value of 28mgm�3, which is translatable in 60%
of representative stations. Nevertheless the remaining
uncertainties regarding the representativeness of stations
and inhomogeneous data, this preliminary long-term
modelling approach seems to have acceptable results,
given the coarse resolution grid of the meteorological
data used (that should be, at least in part, responsible for
some errors). The background ozone prediction could
also be another factor of bias. Almost all the excee-
dances are well simulated, but the model also predicts
ozone standard exceedances in large areas of Portugal,
located mostly in the inland part of the country.
In addition, the original season time series was
spectrally decomposed into intra-day, diurnal, synoptic
and baseline time scales. This analysis reveal that the
model approximately captures the relative contributions
of all components, with a slightly underestimation of the
ID variability and a small overestimation of the relative
strength of the diurnal fluctuations. Correlations be-
tween model predictions and observations are weak for
the ID and high for the inherent diurnal cycle and long-
term components. The poor performance on the intra-
day time scale is at least partially related to the
horizontal grid resolution dimension used in the model
and to the inability of the input fields (meteorology,
emissions, landuse, etc) to capture this scale in time and
space. The better performance of the model on longer
time scales suggest that modelling periods should be
longer than the duration of a single episode to increase
confidence in the regulatory modelling applications.
Nevertheless, the results of this validation experiment
calls for improving the modelling system in several
aspects. Future model developments would have to
focus on the intra-day and diurnal cycle processes,
improving vertical mixing and dry deposition, which are
only very crudely represented. The meteorological
parameters need to be better simulated, with a numerical
model able to simulate the mesoscale thermal circula-
tions, like sea and valley breezes.
Ozone concentration predictions are the main subject
discussed in this work, but the model also simulates
nitrogen dioxide, which can be especially in winter, of
major concern for the air quality managers in urban
areas. During Summer 2001, the NO2 concentrations
were also modelled and a fair correspondence between
observed and simulated peaks was found. However, the
concentrations are often overestimated. The experiment
is being carried on for the winter season, and will be
discussed in a subsequent paper. Another future task
will be the evaluation of this modelling system in
forecast mode, one of the requirements of the new Air
Quality Framework Directive (96/62/CE), and a reliable
tool for the air quality management in Portugal, in
reducing and protecting the population exposure more
ARTICLE IN PRESSA. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–31013100
efficiently and enabling real-time emission abatement
measures.
Acknowledgements
This work is partially financed by the Portuguese
Environment Institute and CRUP. Additional support is
provided by the Portuguese Ministerio da Ciencia,
Inovac- ao e Ensino Superior, for the PhD Grant of A.
Monteiro (SFRH/BD/10922/2002). The authors would
like to thank R. Friedrich and B. Wickert (University of
Stuttgart) for making available VOC profiles and the
temporal variability of annual emissions. The authors
are also grateful to ACCENT European Network of
Excellence.
References
Atkinson, R., Baulsch, l., Cox, R.A., Hampton, R.F., Kerr,
I.A., Rossi, J., Troe, J., 1997. Evaluated kinetics, photo-
chemical and heterogeneous data. Journal of Physical and
Chemical Reference Data 26 (3), 521–1012.
Aumont, B., Jaecker-voirol, A., Martin, B., Toupance, G.,
1997. Tests of some reduction hypotheses made in photo-
chemical mechanisms. Atmospheric Environment 30,
2061–2077.
Barros, N., Borrego, C., Toll, I., Soriano, C., Jimenez, P.,
Balsasano, J.M., 2003. Urban photochemical pollution in
the Iberian Peninsula: Lisboa and Barcelona airsheds. Air
and Waste Management Association 53, 347–359.
Beekmann, M., Derognat, C., 2003. Monte Carlo uncertainty
analysis of a regional-scale transport chemistry model
constrained by measurements from the Atmospheric Pollu-
tion Over the Paris Area (ESQUIF) campaign. Journal of
Geophysical Research 108 (D17), 8559.
Borrego, C., Barros, N., Miranda, A.I., Carvalho, A.C.,
Valinhas, M.J., 2000. Validation of two photochemical
numerical systems under complex mesoscale circulations.
In: Gryning, S., Batchvarova, E. (Eds.), Air Pollution
Modeling and its Application, vol. XIII. Kluwer Academic/
Plenum Publishers, New York, pp. 597–604.
Borrego, C., Tchepel, O., Monteiro, A., Barros, N., Miranda,
A., 2002. Influence of traffic emissions estimation variability
on urban air quality modelling. Water, Air and Soil
Pollution: Focus, vol. 2 (5–6). Kluwer Publishers, Dor-
drecht, pp. 487–499.
Collela, P., Woodward, P.R., 1984. The piecewise parabolic
method (PPM) for gas-dynamical simulations. Journal of
Computational Physics 54, 174–201.
DeMore, W.P., Sander, S.P., Howard, C.J., Ravishankara,
A.R., Golden, D.M., Kolb, C.E., Hampson, R.F., Kurylo,
M.J., Molina, M.J., 1997. Chemical kinetics and photo-
chemical data for use in stratospheric modeling, JPL
Publications, 97-4.
Derognat, C., Beekmann, M., Baeumle, M., Martin, D.,
Schmidt, H., 2003. Effect of biogenic volatile organic
compound emissions on tropospheric chemistry during the
atmospheric pollution over the Paris Area (ESQUIF)
campaign in the Ile-de-France region. Journal of Geophy-
sical Research 108 (D17), 8560.
GENEMIS (Generation of European Emission Data for
Episodes) Project, 1994. EUROTRAC Annual Report
1993, Part 5. EUROTRAC International Scientific Secre-
tariat, Garmisch-Partenkirchen.
Hansen, M., DeFries, R., Townshend, J.R.G., Sohlberg, R.,
2000. Global land cover classification at 1 km resolution
using a decision tree classifier. International Journal of
Remote Sensing 21, 1331–1365.
Hogrefe, C., Rao, S.T., Kasibhatla, P., Hao, W., Sistla, G.,
Mathur, R., Mchenry, J., 2001. Evaluating the perfor-
mances of regional-scale photochemical modelling systems:
Part II—ozone predictions. Atmospheric Environment 35,
4175–4188.
Horowitz, L.W., Walters, S., Mauzerall, D., Emmons, L.,
Rasch, P., Granier, C., Tie, X., Lamarque, J., Schultz, M.,
Brasseur, G., 2003. A global simulation of tropospheric
ozone and related tracers: description and evaluation of
MOZART. Journal of Geophysical Research 108 (D24),
4784 version 2.
Lattuati, M., 1997. Impact des emissions europeennes sur le
bilan d’ozone tropospherique a l’interface de l’Europe et de
l’Atlantique Nord : apport de la modelisation lagrangienne
et des mesures en altitude. Ph.D. Thesis, Universite Pierre et
Marie Curie, Paris, France.
Menut, L., 2003. Adjoint modeling for atmospheric pollution
process sensitivity at regional scale. Journal of Geophysical
Research 108 (D17), 8562.
Middleton, P., Stockwell, W.R., Carter, W.P.L., 1990. Aggre-
gation and analysis of volatile organic compound emissions
for regional modeling. Atmospheric Environment 24A,
1107–1133.
Passant, N.R., 2000. Speciation of UK emissions of non-
methane VOC. AEA Technology, Report number AEAT/
ENV/R/0545 Issue 1. Available online at www.aeat.co.uk/
netcen/airqual/reports/emfact/AEAT_ENV_0545_fi-
nal_v2.pdf.
Schmidt, H., Martin, D., 2003. Adjoint sensitivity of episodic
ozone in the Paris area, to emissions on the continental
scale. Journal of Geophysical Research 108 (D17), 4313.
Schmidt, H., Derognat, C., Vautard, R., Beekmann, M., 2001.
A comparison of simulated and observed ozone mixing
ratios for the summer of 1998 in Western Europe. Atmo-
spheric Environment 35, 2449–2461.
Sillman, S., Vautard, R., Menut, L., Kley, D., 2003. O3-NOx-
VOC sensitivity and NOx-VOC indicators in Paris: results
from models and atmospheric pollution over the Paris Area
(ESQUIF) measurements. Journal of Geophysical Research
108 (D17), 8563.
Simpson, D., 1993. Photochemical model calculations over
Europe for two extended summer periods: 1985 and 1989.
Model results and comparisons with observations. Atmo-
spheric Environment 27A (6), 921–943.
Simpson, D., Winiwarter, W., Borjesson, G., Cinderby, S.,
Ferreiro, A., Guenther, A., Hewitt, C.N., Janson, R.,
Khalil, M.A.K., Owen, S., Pierce, T.E., Puxbaum, H.,
Shearer, M., Skiba, U., Steinbrecher, R., Tarrason, l.,
Oquist, M.G., 1999. Inventorying emissions from nature in
Europe. Journal of Geophysical Research 104, 8113–8152.
ARTICLE IN PRESSA. Monteiro et al. / Atmospheric Environment 39 (2005) 3089–3101 3101
Sistla, G., Hao, W., Ku, J.-Y., Kallos, G., Lagouvardos, K.,
Papadopoulos, A., Zhang, K.K., Mao, H., Rao, S.T., 2001.
An operational evaluation of two regional-scale ozone air
quality modelling systems over the eastern United States.
Bulletin of the American Meteorological Society 82, 945–964.
Stohl, A., Williams, E., Wotawa, G., Kromp-Kolb, H., 1996. A
European inventory for soil nitric oxide emissions and the
effect of these emissions on the photochemical formation of
ozone. Atmospheric Environment 30, 3741–3755.
Tesche, T.W., Georgopoulos, P., Lurmann, F.L., Roth, P.M.,
1990. Improvement of procedures for evaluating photo-
chemical Models. Draft Final Report. California Air
Resources Board, Sacramento.
Tilmes, S., Brandt, J., Flatfy, F., Bergstrom, R., Flemming, J.,
Langner, J., Christensen, J.H., Frohn, L.M., Hoy, f.,Jacobsen, I., Reimer, E., Stern, R., Zimmermann, J., 2002.
Comparison of five eulerian air pollution forecasting systems
for the summer of 1999 using the German ozone monitoring
data. Journal of Atmospheric Chemistry 42, 91–121.
Troen, I., Mahrt, L., 1986. A simple model of the atmospheric
boundary layer: sensitivity to surface evaporation. Bound-
ary-Layer Meteorology 37, 129–148.
USEPA—US Environmental Protection Agency, 1996. Compi-
lation of Photochemical Model’s Performance Statistics for
11/94 Ozone SIP Applications. EPA-454/R-96-004. USE-
PA, Office of Air Quality Planning and Standards, Research
Triangle Park, NC 27711, 156 pp.
Vautard, R., Beekmann, M., Roux, J., Gombert, D., 2001.
Validation of a deterministic forecasting system for the
ozone concentrations over the Paris area. Atmospheric
Environment 35, 2449–2461.
Vautard, R., Martin, D., Beekmann, M., Drobinski, P.,
Friedrich, R., Jaubertie, A., Kley, D., Lattuati, M., Moral,
P., Neininger, B., Theloke, J., 2003. Paris emission
inventory diagnostics from ESQUIF airborne measure-
ments and a chemistry transport model. Journal of
Geophysical Research 108 (D17), 8564.
Verwer, J.G., 1994. Gauss-Seidel iteration for stiff odes from
chemical kinetics. Journal on Scientific Computing 15,
1243–1250.
Wesely, M.l., Hicks, B.B., 1977. Some factors that affect the
deposition rates of sulfur dioxide and similar gases on
vegetation. Journal of Air Pollution Control Association 27,
1110–1116.