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Health Assessment Document for Diesel Emissions - NSCEP | US ...

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1 C.l. INTRODUCTION<br />

2 As discussed in Chapter 4 the lung burden of diesel exhaust particles (DEPs) during<br />

3 exposure is determined by both the amount and site of particle deposition in the lung and,<br />

4 subsequently, by rates of translocation and clearance from the deposition sites. Mathematical<br />

5 models have often been used to complement experimental studies in estimating the lung burdens<br />

6 of inhaled particles in different species under different exposure conditions. This section<br />

7 presents a mathematical model that simulates the deposition and clearance of DEPs in the lungs<br />

8 of rats and humans.<br />

9 . <strong>Diesel</strong> particles are aggregates <strong>for</strong>med from primary spheres of 15 to 30 nm in diameter.<br />

1 0 The aggregates are irregularly shaped and range in size from a few molecular diameters to tens of<br />

11 microns. The mass median aerodynamic diameter (MMAD) of the aggregates is approximately<br />

12 0.2 J..Lm. The primary sphere consists of a carbonaceous core (soot) on which numerous kinds of<br />

13 organic compounds are adsorbed. The organics normally account <strong>for</strong> 10 to 30% ofthe particle<br />

14 mass. However, the exact size distribution ofDEPs and the specific composition of the adsorbed<br />

15 organics depend upon many factors, including engine design, fuels used, engine operating<br />

16 conditions, and the thermodynamic process of exhaust. The _physical and chemical<br />

17 characteristics of DEPs have been reviewed extensively by Amann and Siegla (1982) and<br />

18 Schuetzle (1983).<br />

19 Four mechanisms deposit diesel particles within the respiratory tract during exposure:<br />

20 impaction, sedimentation, interception, and ·diffusion. The contribution from each mechanism to<br />

21 deposition, however, depends upon lung structure and size, the breathing condition of the<br />

22 subject, and particle size distribution. Under normal breathing conditions, diffusion js found to<br />

23 . be the most dominant mechanism. The other three mechanisms play only a minor role.<br />

24 Once DEPs are deposited in the respiratory tract, both the carbonaceous cores and the<br />

25 adsorbed organics ofthe particles will be removed from the deposition sites as described in<br />

26 Chapter 4. There are two mechanisms which facilitate this removal: (a) mechanical clearance,<br />

27 provided by mucocilliary transport in the ciliated conducting airways as well as macrophage<br />

28 phagocytosis and migration in the nonciliated airways, and (b) clearance by dissolution. Siqce<br />

29 the carbonaceous soot ofDEPs is insoluble, it is removed from the lung primarily by mechanical<br />

30 clearance, whereas the adsorbed organics are removed principally by dissolution.<br />

31<br />

32 C.2. PARTICLE MODEL<br />

· 33 To develop a mathematical model which simulates the deposition and clearance ofDEPs<br />

34 in the lung, an appropriate particle model characterizing a diesel particle must first be introduced.<br />

35 For the deposition study, we employed an' equivalent sphere model <strong>for</strong> the diesel particle<br />

36 developed by Yu and Xu (1987)to simulate the dynamics and deposition ofDEPs in the<br />

2/1/98 C-2 DRAFT--DO NOT CITE OR QUOTE

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