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Receptor Modelling Fugitive dust emission rate estimates by reverse-dispersion
modelling
2.1 Short-term monitoring The dispersion of emitted matter is influenced by the location and geometry of the source, weather conditions and terrain roughness. The dispersion factor a is the contribution of a local source i with emission rate e = 1 g/s to the concentration c at a receptor site r downwind of the source. For dust particles, the dispersion factor also depends on the aerodynamic particle size d. cird = aird eid 2.2 Long-term monitoring In many cases, different sources contribute to the concentration at the measuring site. To distinguish the contributions of these sources, a network of receptor sites is needed. Furthermore, accuracy will increase by using time-series of measurements.
The necessary input variables for calculating the dispersion factors
are:
In order to use reverse-dispersion modelling, the emitted component must disperse over some distance, at least 30 m or more. Therefore, it is not applicable for leak detection which takes place at a much smaller distance from the source. To distinguish local sources, the measurements should be performed within several kilometers of the source. At larger distances, the contribution of the local source may be mixed up with the background concentration and the meteorological conditions may require a trajectory analysis instead of a dispersion model. Distinguishing different sources Contributions of different sources can be distinguished when their sets
of dispersion factors are not correlated. For instance, when a receptor
site is located in between two sources one sources is located downwind
(a =0) and the other one upwind (a > 0). With the wind blowing from
the opposite direction, it is the reversed. Then, the dispersion factors
are not correlated.
5 Requirements of the measuring devices Time resolution Reverse-dispersion modelling requires a time resolution of at least one hour. The main reason is the constantly changing weather conditions. To calculate dispersion factors accurately, they must be calculated for every hour. Another reason is the ability to analyse the temporal characteristics of sources. Fine and coarse dust When measuring dust, fine and coarse dust must be distinguished because of their different dispersion chracteristics, their different effects and (partly) their different origin. Particle size resolution When measuring coarse dust, the particle size distribution must be assessed while particle size is very important in calculating the dispersion factor. For fine dust, particle size is of minor importance. Available measuring devices For long-term fine dust measurements, several samplers are commercially
available. The most well-known samplers are the TEOM and the Beta-dust
sampler. A slight disadvantage of the Beta dust sampler is the lower time
resolution which is three hours or more. Samplers based on light scattering
need a calibration for the dust source under investigation. On the other
hand, these samplers can simultaneously assess both PM2.5 and PM10, like
the Osiris sampler. For short-term measurements of coarse dust, a rotary impactor is used:
the dust is sampled on a rotating strip by inertial impaction. There are
several rotary impactors commercially avail-able. Commonly used are the
R--otorod sampler and the Dustviewer. The advantage of the Dustviewer
is the practical use at field locations without any facilities. For long-term measurements of coarse dust, the Coarse Dust Recorder is
used. The Coarse Dust Recorder consists of a tube, a fan, and a cassette
containing a long sticky strip. The fan draws air through the tube at
a rate of 8.8 m.s-1. The tube is 0.3 m wide and is continuously aligned
towards the wind by means of a weather vane. Inside the tube, a small
part of a long strip is exposed to the airflow. Fugitive dust is collected
on the sticky strip by inertial impaction. The lower cut-off diameter
is 14 µm. The strip is moved little by little, so that success-ively
new parts are exposed. After a period of one week, the cassette containing
the strip is removed and analysed by means of image analysis. The result
is the hourly course of the dust concentration and the particle size distribution.
6.1 Standard error and coefficient of multiple determination The standard error of the emission rate is a measure of the accuracy
of the emission rate estimate, assuming that the errors are normally and
independently distributed. The method described above calculates mean fugitive
emissions of the local dust sources. In many cases, however, the emission
will vary, due to weather conditions and industrial activities. These
variations are investigated by creating subsets based on relevant parameters.
The emission rate is calculated for every subset. 6.3 Residual analysis The residuals from the multiple regression model being
the difference between measured and predicted concentration play an important
role in evaluating model adequacy, just as they do in simple linear regression.
Residual plots are used for investigating normality, the possible neglect
of regressors, autocorrelation and outliers.
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