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thermal cracking of ethylene, propylene and light hydrocarbon

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acetylene then acetylene.<br />

B. :+Xl_gne crac+g<br />

In CoWete amlogy with <strong>propylene</strong> <strong>cracking</strong>, the two major initial<br />

reactions are :<br />

%<br />

C2fijo+C 2FI 4 -+ C~EI?O -+ c 4M 6 +HO<br />

~ ( rno1-lsec-l) 1<br />

7 107<br />

~(~ccal/mol)<br />

7.3 8)<br />

c 2H 3 o+i:l--tC k 9 2H 2 +Ho+l,i 5 loq1 31.5 9)<br />

The vinylradical acts as a p radical. in 8) <strong>and</strong> as a<br />

9). The kinetic parameters <strong>of</strong> Z;'nese reactions were<br />

extensive literature survey ( 1 1,15,16,17).<br />

The border line between the two zrea's is now given hy :<br />

k8(C21130)(C2H4) = k (C H O )(l.i)<br />

9 2 3<br />

This line is the flit1 line in Figure 18. ';;itti a second orcier<br />

initiation 1i.ke 2C H 422I.i- "+C21150 <strong>and</strong> a teir;iinatj.on involving<br />

two vinylradicals ;i2&Ii3 -+ .? , !C4Hg), an order <strong>of</strong> 2 is predicted<br />

for Conditions in the polymerization zone <strong>and</strong> a.n order <strong>of</strong> 1 for<br />

conditions in the dccoi~iposition zone.<br />

Si1:lon <strong>and</strong> Iijaclc (1 5) <strong>and</strong> Silcocks (1 8) observed seconci order<br />

kinetics, while l.:olera <strong>and</strong> Stuhbs (16) found second order 1cineti.c.s<br />

in the region 5 <strong>of</strong> Fi,mre 18 <strong>and</strong> first order kinetics in region TI,<br />

in agreement with tie proposed border line. R.m.uzi's data (11 )<br />

ivhi.cli arc located in the transition area lead to an order <strong>of</strong> 312<br />

for tiic ~:lolial. disa?xarrr.nc:e reaction.<br />

The pilot plant experiinento cover the transition zone. The order<br />

!ea.s shown in 'I'al:~lea 4 <strong>and</strong> 6 to evolve fron! 1 .6 to 1 .2 as the<br />

temperature is increased <strong>and</strong> the activation eiiergy from 40 to<br />

2.boIit 75 kce?.l/iilol.<br />

I '<br />

J?'Iie pol.yilir~i.iarttion can also lie <strong>of</strong> a J!lOleCILlar nature :<br />

.A(I mol-' sec-l) :,'(1cca,l/rnQl) iter<br />

C,ii +I ,'jC I L ---> polymer<br />

r 4 4<br />

3 107 27 19 IC)<br />

Th.e ratio <strong>of</strong> the ra.c?ica.l. reaction <strong>and</strong> molecular condensation rates<br />

was ca3.cula.ted fron 2.n isotlierraal. non cteady state radi.ca1 siimlation<br />

<strong>of</strong> the <strong>ethylene</strong> experiinents by Sunderan & PToment (IO), to be<br />

71 at 80GV <strong>and</strong> 1.; conversion, 15 at OOO°C <strong>and</strong> 3:~ conversion ana<br />

10 at 825°C <strong>and</strong> 8 ;i conversion.<br />

It follows that molecular condensation cannot be neglected a.t<br />

8CO°C <strong>and</strong> higher. This explains vlhy the experi.inenta1 Cg+ frsction<br />

was SO stroiicly correla.ted aitli the temperature. In <strong>propylene</strong><br />

crrtcitiiie the ratios <strong>of</strong> the rates <strong>of</strong> the radical po1yl;ierisation <strong>and</strong><br />

the moleculcir conderisation at OGCV would Le <strong>of</strong> the ordcr <strong>of</strong> IC00<br />

because the allyl rzdical is hich <strong>and</strong> butadiene is low.<br />

It is clear also froiii Piwre 16 for <strong>ethylene</strong> ax1 from Figure 17<br />

for <strong>propylene</strong> that tile influence <strong>of</strong> the pnr-tial <strong>and</strong> total pressure<br />

on fne order anci activation encrt27 vrill be inore or less pronounced<br />

depending u?on the distance frnrn the border line. The higher acti-<br />

vation enerzies Given in lnbles 6 <strong>and</strong> 7 for the conditions <strong>of</strong> the<br />

classes 2, 4 <strong>and</strong>, 5 may be related to t<br />

Pinally, il; ShOii.ld be added that even<br />

less tila (1.2 wt ,:, in the etiiyleiie feed, the initiation reaction<br />

C 11 i2CI11° cannot lje ne!:lecterl, as concluded already by<br />

2 6<br />

1:m~ugi (I I ) unc~ BY yowell <strong>and</strong> liartin (20) .<br />

141

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