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

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samples during this pyrolysis were <strong>of</strong> <strong>the</strong> order <strong>of</strong> 30 percent. In o<strong>the</strong>r cases <strong>the</strong> c<strong>at</strong>alysts were<br />

added after charring <strong>at</strong> 7OO0C by mixing weighed amounts <strong>of</strong> salts and chgr toge<strong>the</strong>r in a Fisher<br />

Minimill. The char samples had surface areas <strong>of</strong> approxim<strong>at</strong>ely 280 m /g., as determined by<br />

C02 adsorption <strong>at</strong> 195'K.<br />

Spectroscopic grade graphite powder (-325 mesh, Type UCP-ZR, highest 9urity) was obtained<br />

from Ultra Carbon Corp. This m<strong>at</strong>erial had an initial surface area <strong>of</strong> 7.5 m /g., as determined<br />

by nitrogen adsorption <strong>at</strong> -195OC.<br />

The salt additives were Analytical Reagent or Certified ACS Grade m<strong>at</strong>erials and were<br />

used without fur<strong>the</strong>r tre<strong>at</strong>ment. The gaseous <strong>at</strong>mospheres used included Linde Instrument<br />

Grade carbon dioxide and Linde Ultra-High Purity Grade helium. For experiments in steam<br />

(w<strong>at</strong>er vapor), <strong>the</strong> helium was passed through a distilled w<strong>at</strong>er bubbler <strong>at</strong> 25OC to give a w<strong>at</strong>er<br />

vapor pressure <strong>of</strong> 23 mm. (3.1 kPa) in <strong>the</strong> gas stream.<br />

Procedure<br />

Proxim<strong>at</strong>e Analysis<br />

% Moisture % Vol<strong>at</strong>iles % Fixed C BTU/lb<br />

As Received 0.72 9.68 39.45 50.15 12979<br />

Dry Basis 9.75 39.74 50.51 13073<br />

Ultim<strong>at</strong>e Analysis<br />

Free Swelling Index = 5<br />

% Moisture %c 'j%J % 0 (diff.)<br />

As Received 0.72 73.06 5.04 1.68 0.39 1.20 8.23<br />

Dry Basis 73.59 5.08 1.69 0.39 1.21 8.29<br />

Table I: Analyses <strong>of</strong> Illinois #6 Coal Sample<br />

Thermogravimetric studies and measurements <strong>of</strong> <strong>the</strong> iso<strong>the</strong>rmal kinetics <strong>of</strong> <strong>the</strong> c<strong>at</strong>alyzed<br />

gasific<strong>at</strong>ion <strong>of</strong> char and graphite in CO and w<strong>at</strong>er vapor were carried in <strong>the</strong> Mettler<br />

Thermoanalyzer-2 autom<strong>at</strong>ically recordin% balance as previously described?Y') Kinetic measurements<br />

<strong>at</strong> a series <strong>of</strong> constant temper<strong>at</strong>ures between 600 and 1000°$ were made on 200 rng.<br />

samples <strong>of</strong>-re doped carbons, using flowing C02 <strong>at</strong> 1 <strong>at</strong>m. (1.02 x 10 kPa) and a flow r<strong>at</strong>e <strong>of</strong><br />

200 ml.min . Gasific<strong>at</strong>ion in w<strong>at</strong>er vapor was accomplished in p w<strong>at</strong>er vapor-s<strong>at</strong>ur<strong>at</strong>ed helium<br />

stream (23 mm. H20, 3.1 kPa) <strong>at</strong> a flow r<strong>at</strong>e <strong>of</strong> 300 ml.min- . Kinetic d<strong>at</strong>a were generally<br />

plotted in <strong>the</strong> form <strong>of</strong> Arrhenius plots (r<strong>at</strong>es vs. I/T°K), <strong>the</strong> gasific<strong>at</strong>ion r<strong>at</strong>es <strong>at</strong> each<br />

temper<strong>at</strong>ure being derived experimentally from <strong>the</strong> rel<strong>at</strong>ion,<br />

R<strong>at</strong>e (min-l) = dW/dt<br />

wO<br />

where w is <strong>the</strong> initial weight <strong>of</strong> <strong>the</strong> sample. In all cases, in order to minimize <strong>the</strong> effects <strong>of</strong><br />

changing'surface area and c<strong>at</strong>alyst concentr<strong>at</strong>ion, <strong>the</strong> total wight loss during gasific<strong>at</strong>ion <strong>of</strong><br />

each sample was kept below 15 percent.<br />

75

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