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the coking properties of coal at elevated pressures. - Argonne ...

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t<br />

5360-096pj<br />

There is an interaction between feed gas composition and apparent<br />

temper<strong>at</strong>ure dependence because <strong>the</strong> mini-reactor is an integral reactor. For<br />

example, when pure steam is introduced <strong>at</strong> <strong>the</strong> bottom <strong>of</strong> <strong>the</strong> bed <strong>of</strong> char,<br />

a mixture <strong>of</strong> H20 + Hp issues from <strong>the</strong> top <strong>of</strong> <strong>the</strong> bed. As <strong>the</strong> r<strong>at</strong>e <strong>of</strong> reaction<br />

changes, <strong>the</strong> gas composition <strong>at</strong> various loc<strong>at</strong>ions in <strong>the</strong> reactor changes even<br />

though <strong>the</strong> feed gas remains <strong>the</strong> same. Therefore, as temper<strong>at</strong>ure changes,<br />

some <strong>of</strong> <strong>the</strong> change in r<strong>at</strong>e is due to activ<strong>at</strong>ion energy, but some <strong>of</strong> <strong>the</strong> change<br />

is due to gas composition. A reactor model which performs an integr<strong>at</strong>ion over<br />

<strong>the</strong> bed is required to account for both effects.<br />

Our modeling work discussed<br />

in <strong>the</strong> next section <strong>of</strong> this report has identified <strong>the</strong> true activ<strong>at</strong>ion energy<br />

as about 50 kcal/g mole.<br />

Gasific<strong>at</strong>ion R<strong>at</strong>e Expression<br />

During an earlier phase <strong>of</strong> research on <strong>the</strong> CCG process, a screening<br />

<strong>of</strong> gasific<strong>at</strong>ion reaction r<strong>at</strong>e models was reported by Vadovic and Eakman<br />

(5). In this screening, all combin<strong>at</strong>ions <strong>of</strong> from one to four inhibition terms<br />

involving <strong>the</strong> partial <strong>pressures</strong> <strong>of</strong> H2, CO, H20, and <strong>the</strong> cross products <strong>of</strong><br />

<strong>the</strong> partial <strong>pressures</strong> <strong>of</strong> H2and CO, and Hp and H 0 were tested in <strong>the</strong> denomin<strong>at</strong>or<br />

<strong>of</strong> <strong>the</strong> gasific<strong>at</strong>ion r<strong>at</strong>e expression. In ali, <strong>the</strong>y tested thirty models.<br />

Those models which gave neg<strong>at</strong>ive coefficients on regression were discarded as<br />

being physically unreal. Four additional models were discarded because <strong>the</strong>y<br />

gave an infinite r<strong>at</strong>e for a pure stem environment.<br />

Of <strong>the</strong> thirty models<br />

These<br />

tested, three models remained which gave good fit to <strong>the</strong>ir d<strong>at</strong>a.<br />

three are listed below.<br />

For <strong>the</strong>ir screening <strong>of</strong> gasific<strong>at</strong>ion r<strong>at</strong>e models, Vadovic and Eakman used<br />

d<strong>at</strong>a from runs in which only pure steam was fed to <strong>the</strong> bed <strong>of</strong> <strong>coal</strong> char.<br />

Mixtures <strong>of</strong> HpO and H2 or H20, H2, and CO were introduced and studied in <strong>the</strong><br />

present program.<br />

89

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