treasure valley road dust study: final report - ResearchGate
treasure valley road dust study: final report - ResearchGate
treasure valley road dust study: final report - ResearchGate
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6.3 Discussion<br />
The depletion of PM 10 in the proximity of the emissions source has important implications<br />
for the use of <strong>road</strong> <strong>dust</strong> emissions in air quality models. PM 10 <strong>dust</strong> emissions used to estimate<br />
emissions factors are measured within 5 to 50 m of a <strong>road</strong>. Emissions calculated based on those<br />
factors do not account for the depletion of PM 10 as the plume travels further downwind. Many of<br />
the frequently used urban and regional scale air quality models assume that ground level emissions<br />
are initially uniformly mixed over a certain height, typically the distance from the ground to the<br />
first node in the numerical grid (20 – 40 m). This assumption does not adequately allow for the<br />
removal by deposition of the larger particles in the PM 10 size range. Consequently, air quality<br />
models that use <strong>road</strong> <strong>dust</strong> emissions as input without accommodation for near-source removal of<br />
particles will likely overestimate the ambient concentrations of <strong>road</strong> <strong>dust</strong> PM 10 .<br />
Table 6-4 shows how changes in the parameters used in the model can affect the fraction<br />
of PM 10 that remains suspended after 60 seconds. The model is sensitiveto some of the<br />
parameter values and fairly insensitive to others. For example, varying the roughness length under<br />
neutral conditions over several orders of magnitude has only a modest effect on the fraction of<br />
particles remaining in suspension. On the other hand, the value used for deposition rate due to<br />
impaction can have substantial consequences. If impaction is not accounted for at all (V i = 0) and<br />
particles were only allowed to deposit by gravitational settling, then the fraction that remains in<br />
suspension is 95%, considerably higher than the 65% achieved with the model assumptions here.<br />
Another important parameter is the assumption for the initial distribution of particles in the<br />
vertical direction. A factor of two increase or decrease in the initial pulse height can vary the<br />
fraction remaining between 45% and 80%.<br />
Table 6-4. The effects of perturbation of model inputs on fraction of particles remaining in<br />
suspension at t = 60 seconds.<br />
Parameter Stability Baseline value<br />
Baseline<br />
fraction<br />
remaining<br />
Perturbed value<br />
Fraction<br />
remaining<br />
z 0, u * Neutral 0.01 m, 0.058 m/s 65% 1 m, 0.17 m/s 60%<br />
z 0, u * Neutral 0.01 m, 0.058 m/s 65% 0.1 m, 0.087 m/s 62%<br />
z 0, u * Neutral 0.01 m, 0.058 m/s 65% 0.001 m, 0.043 m/s 67%<br />
V i Neutral 0.08 m/s 65% 0.16 m/s 63%<br />
V i Neutral 0.08 m/s 65% 0.04 m/s 68%<br />
V i Neutral 0.08 m/s 65% 0 m/s 95%<br />
L Stable 10 m 64% 1 m 70%<br />
L Stable 10 m 64% 1000 m 64%<br />
Initial distribution Neutral 0-2 m 65% 0-4 m 80%<br />
Initial distribution Neutral 0-2 m 65% 0-1 m 46%<br />
Z i Neutral 200 m 65% 400 m 65%<br />
Z i Neutral 200 m 65% 100 m 65%<br />
The model presented here is useful for demonstration of the behavior of <strong>road</strong> <strong>dust</strong><br />
emissions near the point of origin. However, several simplifying assumptions have been made in<br />
the formulation of this model and many of the parameters only represent approximations. In<br />
future work, and in keeping with the suggestions of both Watson and Chow (2000) and Countess<br />
(2001), it is important to better estimate the conditions under which emissions from <strong>road</strong>s are<br />
transported. Most notably, better field measurements of the impaction term V i and the initial<br />
plume distribution should be obtained under neutral and stable atmospheric conditions.<br />
6-7