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thermal cracking of ethylene, propylene and light hydrocarbon

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The selectivity <strong>of</strong> a component I in the <strong>cracking</strong> <strong>of</strong> a mixture<br />

A-B is defined as :<br />

mol9 <strong>of</strong> I from A + mols <strong>of</strong> I from B<br />

YI = mols <strong>of</strong> A cracked + mois <strong>of</strong> B cracked<br />

When there is no interaction, Froment et (7) showed that<br />

equation 1 is identical with :<br />

This predicted value <strong>of</strong> the selectivity will be called the non-<br />

interaction selectivity. *<br />

The pure additivity selectivity : yI = yI,*YA + yI,Bph 3), used<br />

in the literature so far, is obviously a very special case <strong>of</strong> 2)<br />

valid only for xA,jJ = x ~ , ~ ~ .<br />

It is clear from Fig.rce 12 that 2) allows a far better prediction<br />

<strong>of</strong> the experimental results than 3). Analogous figures were plotted<br />

for different conversions <strong>and</strong> for all binary mixtures mentioned in<br />

the experimental program. From all these curves, the following<br />

rule can be deduced : "The experimental selectivities deviate from<br />

the pure additivity lines in the same direction as the non-interaction<br />

selectivitiesll. This means that the effect <strong>of</strong> interaction<br />

can be predicted when the selectivities from the individual<br />

Conponents <strong>and</strong> the relative rates <strong>of</strong> <strong>cracking</strong> are Icno~m.<br />

The selectivities for <strong>cracking</strong> <strong>of</strong> ternary mixtures may be represented<br />

in diagrams <strong>of</strong> the type shown in figure 13,. In this figure<br />

the <strong>ethylene</strong> selectivity at conversions ~~,]\,~=40 F, $ ;<br />

x ,-88 $ is plotted with respect to the ternary feed composition.<br />

i'ttfi-ternary mixtures the pure additivity, non interaction <strong>and</strong><br />

experimental lines <strong>of</strong> Pig. 12 become surfaces. Here too the experimental<br />

selectivities deviate from the pure additivity surface<br />

in the same sense as the non-interaction surface.<br />

4. Kinetics<br />

The kinetics <strong>of</strong> the <strong>cracking</strong> <strong>of</strong> a component X, are derived from<br />

the experiments by means <strong>of</strong> its continuity equation. For ethane<br />

in a binary mixture ethane-<strong>propylene</strong> e.g., cracked in a tubular<br />

reactor with plug flow conditions, the continuity equation may be<br />

written :<br />

n<br />

E<br />

FE,OdxE,p = A e d - m ) . ( C E , p ) dV 4)<br />

E =expansion=<br />

(total molar flow rate)exj-t-(mols G 2II 6 +molsC<br />

mols C kI cracked + iiiols C3F16 cracked<br />

2 6<br />

6 = molar ratio <strong>propylene</strong>/etilylene<br />

= dilation factor : mols 112O/mol <strong>hydrocarbon</strong><br />

In 4) the experimental temperature <strong>and</strong> total preswwe pr<strong>of</strong>ile<br />

are also accounted for.<br />

Tlie kinetics can now be derived froin 4) as such or by inaking use<br />

<strong>of</strong> the equivalent reactoz volume concept.<br />

137

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