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MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...

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the surface rate coefficient may produce “apparent” kinetics, just as absorbing the effects<br />

of internal combustion into the global n-th order rate coefficient k s (see Eq. 2.16) does.<br />

In contrast to the approach of Sun and Hurt (1999), Charpenay et al. (1992)<br />

neglected the molecular diffusion mechanism and used only the Knudsen diffusivity to<br />

calculate the effective diffusivity:<br />

D e = D K / (5.19)<br />

Although both groups used the tortuosity factor to convert the diffusivity into effective<br />

diffusivity, the selections of diffusion mechanism seemed somewhat arbitrary. In this<br />

study the relative importances of these two diffusion mechanisms were compared, and<br />

the situations where one of these mechanism may be neglected were explored.<br />

In general, both bulk diffusion (also called molecular diffusion) and Knudsen<br />

diffusion may contribute to the mass transport rate within the porous structure of the<br />

char. The combined effects of these two diffusion mechanisms can be described by the<br />

combined diffusivity D (Smith, 1981):<br />

1<br />

D =<br />

1/ DAB + 1/ DK 54<br />

(5.20)<br />

The combined diffusivity can be controlled by molecular diffusion, Knudsen diffusion or<br />

both of them, depending on the ratio of the size of pore to the mean free path (Knudsen,<br />

1950). The Knudsen diffusivity can be calculated from classical kinetic theory (Smith,<br />

1981):<br />

DK = 9.70 ×10 3 ⎛<br />

rp ⎝<br />

⎜<br />

T p<br />

M A<br />

1/2<br />

⎟<br />

⎞<br />

⎠<br />

(5.21)

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