the coking properties of coal at elevated pressures. - Argonne ...
the coking properties of coal at elevated pressures. - Argonne ...
the coking properties of coal at elevated pressures. - Argonne ...
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from Figure 5, due to <strong>the</strong> scale, is th<strong>at</strong> <strong>the</strong> time for total burnaway is <strong>the</strong> same<br />
for each distribution since <strong>the</strong>y all have <strong>the</strong> same maximum particle size <strong>of</strong> 3m.<br />
Evalu<strong>at</strong>ion <strong>of</strong> C<br />
P<br />
Equ<strong>at</strong>ion 27) was numeric<strong>at</strong>ly integr<strong>at</strong>ed to give <strong>the</strong> particul<strong>at</strong>e oxygen<br />
concentr<strong>at</strong>ion C for <strong>the</strong> three distributions. The results are shown in<br />
Figure 6. An igteresting fe<strong>at</strong>ure <strong>of</strong> <strong>the</strong>se results is <strong>the</strong> value <strong>of</strong> Cp <strong>at</strong> t=o.<br />
According to Avedesian and Davidson 17) <strong>the</strong> value <strong>of</strong> 5 should be almost zero<br />
for <strong>the</strong> b<strong>at</strong>ch fed system but it is clear from Figure 6 th<strong>at</strong> this is not <strong>the</strong> case.<br />
Equ<strong>at</strong>ions 25), 26) and 27) are valid only for constant temper<strong>at</strong>ure and<br />
pressure. These conditions are usually met in FBC's except th<strong>at</strong> <strong>the</strong> particle<br />
temper<strong>at</strong>ure Tp can vary during burnaway and can be appreciably higher than<br />
<strong>the</strong> bed temper<strong>at</strong>ure (4,5,6). The effect <strong>of</strong> increasing Tp would be to increase<br />
<strong>the</strong> value <strong>of</strong> k2 rel<strong>at</strong>ive to kl and <strong>the</strong> controlling mechanism would tend<br />
towards th<strong>at</strong> <strong>of</strong> diffusion. Increasing <strong>the</strong> pressure <strong>of</strong> <strong>the</strong> system would only<br />
have a significant effect if <strong>the</strong> combustion r<strong>at</strong>e was initially domin<strong>at</strong>ed by<br />
chemical kinetics.<br />
Conclusions<br />
A <strong>the</strong>oretical model has been developed which predicts <strong>the</strong> change in size<br />
distribution during burnaway, burn-out times and particul<strong>at</strong>e phase oxygen<br />
concentr<strong>at</strong>ions as a function <strong>of</strong> original particle size distribution in a b<strong>at</strong>ch<br />
fed fluidised bed.<br />
b<strong>at</strong>ch fed experiment could be devised to determine <strong>the</strong> role <strong>of</strong> chemical kinetics<br />
for a given type <strong>of</strong> <strong>coal</strong> and would thus be an aid to modelling <strong>of</strong> fluidised bed<br />
combus tion.<br />
Acknowledgements<br />
If <strong>the</strong> original size distribution is accur<strong>at</strong>ely known a<br />
The work described here form part <strong>of</strong> <strong>the</strong> activities <strong>of</strong> <strong>the</strong> Sheffield<br />
Coal Research Unit sponsored by Shell Coal Intern<strong>at</strong>ional and <strong>the</strong> N.C.B.. The<br />
authors are gr<strong>at</strong>eful for <strong>the</strong> financial assistance <strong>of</strong> <strong>the</strong> Sponsors and wish to<br />
point out th<strong>at</strong> <strong>the</strong> views expressed here are those <strong>of</strong> <strong>the</strong> authors and not<br />
necessarily those <strong>of</strong> <strong>the</strong> Sponsors. We are also gr<strong>at</strong>eful to Dr. R.G. Siddall and<br />
Dr. P.J. Foster for many illumin<strong>at</strong>ing discussions.<br />
Nomencl<strong>at</strong>ure<br />
Constant defined by equ<strong>at</strong>ion 24)<br />
Area <strong>of</strong> fluidised bed (m2)<br />
Rosin-Rammler constant - equ<strong>at</strong>ion 21)<br />
Oxygen exchange parameter - equ<strong>at</strong>ion 12)<br />
Oxygen concentr<strong>at</strong>ion <strong>of</strong> fluidising air (mole/m 3 )<br />
3<br />
Particul<strong>at</strong>e phase oxygen concentr<strong>at</strong>ion (mole/rn )<br />
Gas diffusion coefficient (m2/s)<br />
constant (= l/k2)<br />
constant (= l/kl)<br />
Defined by equ<strong>at</strong>ion 12)<br />
Function <strong>of</strong> Oxygen concentr<strong>at</strong>ion (= 2M C /~p)<br />
O P<br />
302