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recent results on the kinetics of coal pyrolysis and hydropyrolysis ...

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A characteristic result using <strong>the</strong> <strong>the</strong>rmobalance is given in fig. 1,<br />

showing <strong>the</strong> formati<strong>on</strong> rates <strong>of</strong> <strong>the</strong> main products. The mass loss<br />

depicts <strong>the</strong> overall reacti<strong>on</strong> <strong>and</strong> <strong>the</strong>reby <strong>the</strong> formati<strong>on</strong> <strong>of</strong> <strong>the</strong><br />

char <strong>and</strong> occurs in two steps. The volatile matter - tar <strong>and</strong> gaseous<br />

products - are liberated in <strong>on</strong>e or a few single reacti<strong>on</strong>s for<br />

each comp<strong>on</strong>ent. Fig. 2 shows <strong>the</strong> gas formati<strong>on</strong> for a wide rank<br />

Of German <strong>coal</strong>. In all cases - with <strong>the</strong> excepti<strong>on</strong> <strong>of</strong> C02 <strong>and</strong> <strong>the</strong><br />

hydrogen (not given in <strong>the</strong> figure) - <strong>the</strong> curves show a systematic<br />

degradati<strong>on</strong> by <strong>coal</strong>ificati<strong>on</strong> <strong>of</strong> those groups, which have a weaker<br />

b<strong>on</strong>ding <strong>and</strong> are <strong>the</strong>refore liberated at lower temperature during<br />

<strong>pyrolysis</strong>.<br />

Course <strong>of</strong> product formati<strong>on</strong> <strong>and</strong> yields are c<strong>on</strong>trolled by chemical<br />

reacti<strong>on</strong> <strong>on</strong> <strong>the</strong> <strong>on</strong>e h<strong>and</strong> <strong>and</strong> transport phenomena inside <strong>the</strong> particle<br />

<strong>on</strong> <strong>the</strong> o<strong>the</strong>r. The latter gains in influence, if particle diameter,<br />

heating rate <strong>and</strong> pressure increase. An example for quantitative<br />

measurements <strong>and</strong> relevant calculati<strong>on</strong>s is given in fig. 3. As<br />

a functi<strong>on</strong> <strong>of</strong> particle diameter <strong>and</strong> heating rate a curve has been<br />

established separating areas where - depending <strong>on</strong> diameter <strong>and</strong><br />

heating rate - transport phenomena or chemical reacgi<strong>on</strong> c<strong>on</strong>trols<br />

<strong>the</strong> overall process. With higher pressure it is shifted to lower<br />

values for diameter <strong>and</strong> heating rate. The regi<strong>on</strong>, in which <strong>the</strong><br />

chemical reacti<strong>on</strong> is rate determining, meets to a high degree<br />

<strong>the</strong> c<strong>on</strong>diti<strong>on</strong>s in technical reactors regarding pressure, particle<br />

size <strong>and</strong> rate <strong>of</strong> heating. Thus <strong>kinetics</strong> <strong>the</strong>mselves are not influenced<br />

by transport processes, however by <strong>the</strong> different residence times<br />

<strong>of</strong> <strong>the</strong> product inside <strong>the</strong> particle sec<strong>on</strong>dary reacti<strong>on</strong>s may c<strong>on</strong>trol<br />

yields. This is especially true for <strong>the</strong> liquid volatile matter<br />

as can be seen by <strong>the</strong> formati<strong>on</strong> <strong>of</strong> <strong>the</strong> tar <strong>and</strong> - as an example<br />

<strong>of</strong> <strong>the</strong> BTX aromatics - <strong>the</strong> benzene (fig. 5 ), whereby pressure<br />

favours obviously <strong>the</strong> cracking <strong>of</strong> <strong>the</strong> liquids. This is true for<br />

<strong>the</strong> whole rank /lo/. Fig. 7 gives quantitative data for two rates<br />

<strong>of</strong> heating. However, by comparis<strong>on</strong> <strong>of</strong> low <strong>and</strong> high heating rate<br />

<strong>the</strong> latter exhibits a higher yield <strong>of</strong> liquids as <strong>the</strong> residence<br />

time <strong>of</strong> <strong>the</strong> products inside <strong>the</strong> particle is c<strong>on</strong>siderably smaller.<br />

The effect <strong>of</strong> hydrogen exists mainly in an increase <strong>of</strong> <strong>the</strong> formati<strong>on</strong><br />

<strong>of</strong> liquid products, which are now formed in a two reacti<strong>on</strong>s (fig. 6 ).<br />

The peak between 350 <strong>and</strong> about 480 OC is slightly affected mainly<br />

by <strong>the</strong> influence <strong>of</strong> <strong>the</strong> pressure as discussed before <strong>and</strong> can be<br />

ascribed to <strong>pyrolysis</strong>. However with rising pressures <strong>the</strong> sec<strong>on</strong>d<br />

reacti<strong>on</strong> becomes more <strong>and</strong> more important. The enhancing influence<br />

<strong>of</strong> hydrogen pressure <strong>on</strong> <strong>the</strong> yield <strong>of</strong> tar as well as <strong>on</strong> BTX aromatics<br />

is dem<strong>on</strong>strated in fig. 9 for three different high volatile <strong>coal</strong>s.<br />

It is remarkable that up to 40 % <strong>of</strong> <strong>the</strong> <strong>coal</strong> can be c<strong>on</strong>verted<br />

into liquids ultimately at 100 bar under low heating rates. The<br />

BTX aromatics have a share <strong>of</strong> about 10 % <strong>of</strong> <strong>the</strong> total tar. Fig. 10<br />

summarizes <str<strong>on</strong>g>results</str<strong>on</strong>g> <strong>of</strong> <strong>the</strong> characterizati<strong>on</strong> <strong>of</strong> tar samples, taken<br />

at different temperatures during hydro<strong>pyrolysis</strong>. It shows that<br />

<strong>the</strong> c<strong>on</strong>centrati<strong>on</strong> <strong>of</strong> <strong>the</strong> aromatics in <strong>the</strong> tar increases with rising<br />

temperature <strong>and</strong> that <strong>the</strong> BTX aromatics are mainly formed at <strong>the</strong><br />

end <strong>of</strong> <strong>the</strong> tar formati<strong>on</strong>. The sec<strong>on</strong>d reacti<strong>on</strong> <strong>of</strong> tar formati<strong>on</strong><br />

mainly can be ascribed to hydrogenati<strong>on</strong> <strong>and</strong> <strong>the</strong> formati<strong>on</strong> <strong>of</strong> <strong>the</strong><br />

BTX to hydrocracking.<br />

3. Kinetics <strong>and</strong> Mechanism<br />

A derivati<strong>on</strong> <strong>of</strong> ma<strong>the</strong>matical equati<strong>on</strong>s to describe product formati<strong>on</strong><br />

curves for Coal <strong>pyrolysis</strong> is given in fig. 9, left side. They<br />

have been achieved under <strong>the</strong> asumpti<strong>on</strong> that <strong>the</strong> rate <strong>of</strong> <strong>the</strong> for-<br />

mati<strong>on</strong> <strong>of</strong> a particular product is dependent <strong>on</strong> <strong>the</strong> c<strong>on</strong>centrati<strong>on</strong><br />

<strong>of</strong> functi<strong>on</strong>al groups in <strong>the</strong> <strong>coal</strong>, <strong>the</strong> degradati<strong>on</strong> <strong>of</strong> which <str<strong>on</strong>g>results</str<strong>on</strong>g><br />

in this product /3/. With <strong>the</strong>se equati<strong>on</strong>s <strong>the</strong> measured curves<br />

can be described excellently as <strong>the</strong> examples <strong>on</strong> <strong>the</strong> right h<strong>and</strong><br />

3

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