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25th International Meeting on Organic Geochemistry IMOG 2011

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P-091<br />

Investigati<strong>on</strong> of oil stability under geological c<strong>on</strong>diti<strong>on</strong>s using<br />

kinetics of C8 hydrocarb<strong>on</strong>s cracking derived from MSSV<br />

pyrolysis<br />

Regina Binotto 1 , Rosane F<strong>on</strong>tes 1 , Henrique Penteado 1 , Denise Bohrer 2<br />

1 Petrobras Research Center, Rio de Janeiro, Brazil, 2 Federal University of Santa Maria, Santa Maria, Brazil<br />

(corresp<strong>on</strong>ding author:binotto@petrobras.com.br)<br />

One of the most fundamental problems in<br />

petroleum systems modeling for deep offshore<br />

prospects is to determine the spatial (depth) and<br />

temperature limits of oil occurrence [1]. Reservoirs<br />

that were originally filled with oil might be subjected to<br />

further burial, and liquid petroleum may be cracked to<br />

gas. Oil-to-gas cracking is governed by a large<br />

number of chemical reacti<strong>on</strong>s that are not known in<br />

detail, but are recognized as being irreversible firstorder<br />

reacti<strong>on</strong>s following the Arrhenius law.<br />

Oil-to-gas cracking kinetics applied to petroleum<br />

systems modeling were derived from cracking<br />

experiments using different pyrolysis techniques [2].<br />

Whole oils, light fracti<strong>on</strong>s or individual compounds<br />

have been submitted to artificial cracking using<br />

different methods, thus making a comparis<strong>on</strong> of their<br />

relative kinetic behavior not straightforward.<br />

The objective of this study was to improve the<br />

understanding of oil-to-gas cracking and the extreme<br />

geological c<strong>on</strong>diti<strong>on</strong>s for oil preservati<strong>on</strong> by deriving<br />

kinetics through experimental cracking of compounds<br />

present in the light fracti<strong>on</strong> of petroleum. A<br />

methodology was developed using MSSV (microscale<br />

sealed vessel) coupled with gas<br />

chromatography with flame i<strong>on</strong>izati<strong>on</strong> detector<br />

(MSSV-GC-FID) to assess the thermal degradati<strong>on</strong> of<br />

C8 pure hydrocarb<strong>on</strong>s that occur am<strong>on</strong>g the lightest<br />

and most stable compounds in natural oils.<br />

The selected compounds are representative of<br />

each class of light hydrocarb<strong>on</strong>s: a normal-chain<br />

alkane (n-octane), a branched alkane (2,3,4trimethylpentane),<br />

a cyclic alkane (ethylcyclohexane),<br />

and an aromatic (o-xylene).<br />

By performing the same analytical protocol in these<br />

pyrolysis experiments, kinetic parameters were<br />

obtained (Ea, activati<strong>on</strong> energy, and the frequency<br />

factor A) for the thermal degradati<strong>on</strong> of the four<br />

selected C8 compounds. This approach allows a<br />

direct comparis<strong>on</strong> of the derived kinetics, since<br />

differences due to various analytical setups were<br />

avoided. MSSV Pyrolysis experiments were carried<br />

out in an anhydrous closed system under isothermal<br />

c<strong>on</strong>diti<strong>on</strong>s from 0 to 7 hours (470-530°C). The global<br />

rate c<strong>on</strong>stants were determined based <strong>on</strong> the reactant<br />

c<strong>on</strong>versi<strong>on</strong>s obtained at various temperatures. For all<br />

temperatures, bulk decompositi<strong>on</strong> of the studied<br />

substances obeys first-order kinetics and the resulting<br />

apparent activati<strong>on</strong> energy (Ea, kcal/mol) and the<br />

corresp<strong>on</strong>ding frequency factor (A, s -1 ) derived from<br />

the Arrhenius diagram are: n-octane (57; 5.62x10 12 ),<br />

2,3,4-trimethylpentane (54; 6.71x10 11 ),<br />

ethylcyclohexane (49; 1.76x10 10 ) and o-xylene (40;<br />

3.96x10 6 ).<br />

These kinetic parameters were used to<br />

extrapolate the behavior of compounds at low<br />

temperatures over geologic time. First, the<br />

extrapolati<strong>on</strong> of laboratory cracking rate c<strong>on</strong>stants<br />

showed that the Arrhenius plots cross at 200-300°C<br />

(Fig. 1). This means that o-xylene, which is more<br />

stable than the other compounds at higher<br />

temperatures, becomes the most labile below 200-<br />

300°C. This reverse behavior, i.e. the lower stability of<br />

aromatics under geological c<strong>on</strong>diti<strong>on</strong>s, explains why<br />

oils found in deep reservoirs are more depleted in<br />

aromatics and c<strong>on</strong>sequently enriched in n-alkanes [3].<br />

ln k (s -1 )<br />

0<br />

-10<br />

-20<br />

-30<br />

-40<br />

Lab<br />

C<strong>on</strong>diti<strong>on</strong>s<br />

(470-530°C)<br />

~300°C<br />

~200°C<br />

n-octane ethylcyclohexane<br />

2,3,4-trim ethylpentane o-xilene<br />

-50<br />

0,6 0,7 0,8 0,9 1 1,1 1,2 1,3 1,4<br />

1/RT (kcal/mol)<br />

Natural<br />

C<strong>on</strong>diti<strong>on</strong>s<br />

(120-200°C)<br />

Fig. 1. Comparis<strong>on</strong> of the Arrhenius diagram obtained for noctane,<br />

2,3,4-trimethylpentane, ethylcyclohexane and oxylene<br />

degradati<strong>on</strong>.<br />

Geological simulati<strong>on</strong>s using the acquired<br />

kinetics and a c<strong>on</strong>stant heating rate of 1°C/ milli<strong>on</strong><br />

years indicated that the temperature ―windows‖ of<br />

compound cracking (between 10% and 90%<br />

c<strong>on</strong>versi<strong>on</strong>) are: n-octane 171-202°C, 2,3,4trimethylpentane<br />

163-195°C, ethylcyclohexane 144-<br />

177°C, and o-xylene 126-164°C.<br />

References<br />

[1] Welte, et al., Springer-Verlag, 1997.<br />

[2] Waples, D.W., Org. <strong>Geochemistry</strong>, 31, 553-575, 2000.<br />

[3] Behar et al., Energy & Fuels, 13, 471-481, 1999.<br />

234

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