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Asphaltene precipitation in crude oils: Theory and experiments

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Table 9. Model Parameters Fitted Us<strong>in</strong>g Sutherl<strong>and</strong> <strong>and</strong> SW Potential Models for Tank-Oil C1*<br />

s A H A /k (K) H R /k (K) AA RR AA /k (K) AR /k (K)<br />

Sutherl<strong>and</strong> 3 11270.01 1891.03 4.130 4.200 2036.54 2383.34<br />

SW 3 11270.01 1891.03 1.596 1.564 2036.54 2383.34<br />

*k 1.381 10 23 J/K (Boltzman constant). ij ( i i j j )/( i j ).<br />

dures, fixed by model assumptions, or calculated through specific<br />

physical relationships or recent theoretical results (Ortega-<br />

Rodriguez et al., 2004). Only seven parameters (H A , H R , AA ,<br />

RR , AA , AR , <strong>and</strong> s A ) need to be determ<strong>in</strong>ed from experimental<br />

data of the particular oil of <strong>in</strong>terest.<br />

<strong>Asphaltene</strong> Precipitation as a Liquid–Liquid<br />

Separation<br />

The conditions for liquid–liquid isothermal equilibrium are<br />

obta<strong>in</strong>ed by impos<strong>in</strong>g the equality of <strong>in</strong>tensive thermodynamic<br />

functions <strong>in</strong> both phases:<br />

A A (12)<br />

R R (13)<br />

(14)<br />

where superscripts <strong>and</strong> refer to the two equilibrated phases<br />

(the higher-density liquid phase corresponds to the precipitated<br />

phase); is the chemical potential; A <strong>and</strong> R denote asphaltenes<br />

<strong>and</strong> res<strong>in</strong>s, respectively; <strong>and</strong> denotes the osmotic pressure,<br />

recall<strong>in</strong>g that, accord<strong>in</strong>g to the McMillan–Mayer theory, the<br />

pressure to be considered must be the osmotic pressure, where<br />

only the solutes are <strong>in</strong>volved <strong>in</strong> an explicit way <strong>in</strong> the thermodynamic<br />

expressions. As <strong>in</strong> the case of electrolyte solutions,<br />

the chemical potentials of the solutes <strong>and</strong> the osmotic pressure<br />

for each phase <strong>in</strong> the asphaltene–res<strong>in</strong>–oil mixture depend only<br />

on the solutes concentration (asphaltene <strong>and</strong> res<strong>in</strong>) <strong>in</strong> the solvent<br />

(oil). The osmotic pressure is obta<strong>in</strong>ed from the thermodynamic<br />

relationship<br />

V<br />

2<br />

NkT<br />

<br />

i<br />

x i<br />

kT <br />

A<br />

<br />

i1 NkT<br />

(15)<br />

where the chemical potential is calculated from the free energy<br />

A<br />

i A<br />

N i i A, R (16)<br />

T,V,N ji<br />

where V is the total volume of the phase. The thermodynamic<br />

properties are written <strong>in</strong> terms of effective values of composition<br />

<strong>and</strong> density, xˆ i <strong>and</strong> , respectively, which depend only on<br />

the solutes properties,<br />

Nˆ N A N R (17)<br />

xi N i / N i A, R (18)<br />

A R (19)<br />

The total values for the molar fractions <strong>and</strong> densities are given<br />

by<br />

x i <br />

N i<br />

N A N R N m<br />

(20)<br />

i x i /v i A, R (21)<br />

Figure 6. Fitt<strong>in</strong>g of experimental n-heptane titration data us<strong>in</strong>g Sutherl<strong>and</strong> <strong>and</strong> SW potential models.<br />

AIChE Journal October 2004 Vol. 50, No. 10<br />

2561

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