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    Effects of petroleum resins on asphaltene aggregation andwater-in-oil emulsion formation

    P. Matthew Spiecker a , Keith L. Gawrys b , Chad B. Trail c,Peter K. Kilpatrick b, *

    aExxonMobil Upstream Research Company, Houston, TX 77027, USAb Department of Chemical Engineering, North Carolina State Uni v ersity, Raleigh, NC 27695, USA

    c Uni v ersity of Kentucky, Lexington, KY 40506, USA

    Recei ved 22 July 2002; accepted 30 December 2002

    Abstract

    Asphaltenes from four crude oils were fractionated by precipitation in mixtures of heptane and toluene. Solubilityprofiles generated in the presence of resins (1:1 mass ratio) indicated the onset of asphaltene precipitation occurred atlower toluene volume fractions (0.1 /0.2) than without resins. Small-angle neutron scattering (SANS) was performed onsolutions of asphaltene fractions in mixtures of heptane and toluene with added resins to determine aggregate sizes.Water-in-oil emulsions of asphaltene /resin solutions were prepared and separated by a centrifuge method to determinethe vol.% water resol ved. In general, the addition of resins to asphaltenes reduced the aggregate size by disrupting thep /p and polar bonding interactions between asphaltene monomers. Interaction of resins with asphaltenic aggregatesrendered the aggregates less interfacially acti ve and thus reduced emulsion stability. The smallest aggregate sizesobser ved and the weakest emulsion stability at high resin to asphaltene (R/A) ratios presumably corresponded toasphaltenic monomers or small oligomers strongly interacting with resin molecules. It was often obser ved that, in theabsence of resins, the more polar or higher molecular weight asphaltenes were insoluble in solutions of heptane andtoluene. The addition of resins dissol ved these insolubles and aggregate size by SANS increased until the solubility limitwas reached. This corresponded approximately to the point of maximum emulsion stability. Asphaltene chemistry playsa vital role in dictating emulsion stability. The most polar species typically required significantly higher resinconcentrations to disrupt asphaltene interactions and completely destabilize emulsions. Aggregation and film formation

    are likely dri ven by polar heteroatom interactions, such as hydrogen bonding, which allow asphaltenes to absorb,consolidate, and form cohesi ve films at the oil /water interface.# 2003 Else vier Science B.V. All rights reserved.

    Keywords: Asphaltenes; Resins; Emulsion stability; Small-angle neutron scattering

    1. Introduction

    Emulsion challenges during petroleum reco veryha ve been attributed to colloidal aggregation of

    * Corresponding author. Tel.: ' /1-919-515-7121; fax: ' /1-919-515-3465.

    E-mail address: [email protected] (P.K. Kilpatrick).

    Colloids and Surfaces A: Physicochem. Eng. Aspects 220 (2003) 9 /27

    www.else vier.com/locate/colsurfa

    0927-7757/03/$ - see front matter # 2003 Else vier Science B.V. All rights reserved.doi:10.1016/S0927-7757(03)00079-7

    mailto:[email protected]:[email protected]
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    asphaltenes and waxes [1 /6]. Many early studieswere performed on the film forming and emulsify-ing beha vior of crude oil /water systems [1,7 /15].These and later studies often pointed to theasphaltenic constituents in crude oil as beingresponsible for film formation and stabilization[10,11,16,17] .

    Asphaltenes, or n -heptane insolubles and tolu-ene solubles, are the most refractory compoundspresent in crude oil and are generally distinguishedby a fused aromatic core with polar heteroatomfunctionality [18,19]. Studies indicate the presenceof carboxylic acids, carbonyls, phenols, pyrrolesand pyridinic functional groups capable of accept-

    ing or donating protons [20 /24]. Vapor pressureosmometry measurements suggest number a veragemolecular weights range from approximately 800to 3000 Da [25 /32]. Even lower asphaltenemolecular weights are obser ved in hot, polarsolvents suggesting that aggregates formedthrough stacking interactions between asphaltenemonomers. The most plausible mechanisms of asphaltene aggregation in volve p /p overlap be-tween aromatic sheets, hydrogen bonding betweenfunctional groups and other charge transfer inter-

    actions.Small-angle neutron scattering (SANS) has beenapplied to probe sol vent and temperature effectson asphaltene aggregation [33 /44]. Proper analy-sis of the scattering intensity cur ves can pro videaggregate size, shape, molecular weight, andfractal dimension. Asphaltenic aggregates arecomprised of cofacial stacks of planar, fusedaromatic ring moieties connected by aliphaticchains and rings. Recent structural and molecularmodeling seem to confirm the so-called archipe-lago model of asphaltenes, as opposed to the morewidely implied and in voked island model [45]. Inthe archipelago model, indi vidual asphaltenemonomers are comprised of aromatic and fusedaromatic ring moieties, some with polar functionalgroups, connected to each other by aliphaticpolymethylene chains and rings that likely containsome sulfide and carbonyl functional groups (seeFig. 1 ). Asphaltenic aggregates ha ve been modeledas mono- and polydisperse spheres [35,46], flatdisks [37,47,48] , and prolate cylinders [38]. As-phaltene polydispersity, howe ver, makes the pre-

    cise shape difficult to discriminate. With thearchipelago-like structure of Fig. 1 , it seemsprobable that asphaltenic aggregates possess aporous reticulated microstructure.

    While the effects of temperature, sol vent aro-maticity, and polarity ha ve received much atten-tion, the sol vation of asphaltene aggregates byresins has not been fully explored. What we meanhere by the expression sol vation is the stronglocal interaction of asphaltenic aggregates by resinmolecules, a phenomenon referred to in pre viousstudies by the curious term peptized; we do notmean by sol vation the swelling of asphaltenicaggregates, although as we show in a subsequent

    publication, resins definitely fill in sol vent voids inasphaltenic aggregates created by the reticulatedstructure of asphaltenes. Espinat et al. measuredneutron and X-ray scattering intensities fromasphaltenic aggregates in se veral sol vents, at lowand high temperatures and with added resins [37].The scattering cur ves were fit using a thin discform factor model. In toluene, 2 wt.% Boscanasphaltene solutions formed larger aggregates atroom temperature (234 A diameter) than at 76 8 C(175 A ). At room temperature, aggregate sizes

    were two to four times smaller in high polaritysolvents such as pyridine and tetrahydrofuran thanin benzene. They also found that resin /asphalteneratios of 2:1 by mass reduced the scatteringintensity at low Q suggesting the formation of smaller aggregates. Howe ver, the effect of resinsolvation on asphaltene aggregate size was notexplicitly reported. Bardon et al. obser ved resinsolvation of Safaniya asphaltenes using SANS andSAXS [47]. Weight a verage molecular weights of 2wt.% asphaltene solutions in toluene with R/Aratios of 2, 4, and 8:1 were reduced by factors of 2.6, 4.6, and 7.5, respecti vely.

    Pre viously [44,49] we examined the aggregationand emulsion stabilizing beha vior of asphaltenesand their more and less soluble fractions inmixtures of heptane and toluene (so-called hep-tol). Gra vimetric solubility measurements indi-cated that asphaltenes start to precipitate atconcentrations between 45 and 52% ( v/v) toluenein heptol. Precipitation concentrated the mostaromatic and polar constituents as measured byH/C ratio and nitrogen content. In addition,

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    SANS indicated that the less soluble fractionformed the largest aggregates in heptol while themore soluble fraction formed considerably smalleraggregates. Asphaltenes and their various sub-fractions are well known to stabilize water-in-oilemulsions near the point of incipient flocculation[50]. The degree of aggregation and proximity tothe solubility limit go verns the stability of emul-

    sions prepared in heptol.In this study, we ha ve taken another steptowards understanding the mechanisms of asphal-tene aggregation and emulsion formation in pet-roleum and petroleum-deri ved systems throughthe addition of sol vating molecules. Crude oils areusually characterized by SARA fractionationwhere asphaltenes are remo ved by precipitationwith a paraffinic sol vent and the deasphalted oil(DAO or maltenes) is separated into saturates,aromatics and resins by chromatographic separa-

    tion [51 /55]. Resins are the most polar andaromatic species present in deasphalted oil and,it has been suggested, contribute to the enhancedsolubility of asphaltenes in crude oil by sol vatingthe polar and aromatic portions of the asphaltenicmolecules and aggregates [25,56,57] . The solubilityof asphaltenes in crude oil is mediated largely byresin sol vation and thus resins play a critical role

    in precipitation, and emulsion stabilization phe-nomena [37,40,58 /60]. Resins, although quitesurface-acti ve, ha ve not been found to stabilizesignificantly water-in-oil emulsions by themsel vesin model systems, a fact that mitigates somewhatagainst the notion that resins and asphaltenes forma simple continuum of molecular structures andfunctions [61,62]. Howe ver, the presence of resinsin solution can destabilize emulsions via asphal-tene sol vation and/or replacement at the oil /waterinterface [62 /66].

    Fig. 1. Schematic illustration of archipelago model of asphaltene monomers, asphaltenic aggregate in absence of resins, andasphaltenic aggregate in presence of resins.

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    Here we probe the effects of resins on asphalteneaggregation and emulsion formation. Aggregationis likely controlled by the ability of asphaltenemonomers to interact through aromatic and polarforces. By fractionating asphaltenes into solubilityclasses, the most polar and aromatic species can beconcentrated. The effecti veness of sol vating resinson these more and less soluble asphaltenes aids inelucidating the mechanisms of colloid formationand emulsion stabilization in petroleum deri vedfluids.

    2. Experimental

    2.1. Asphaltene precipitation and fractionation

    Asphaltenes were precipitated from four crudeoils in a 40:1 excess of n -heptane. The crude oilswere obtained from se veral locations around theworld: B6 and Hondo (off-shore California), ArabHea vy (Safaniya), and Canadon Seco (Argentina).For bre vity the following abbre viations will beused to describe the asphaltenes generated fromHondo, Arab Hea vy, and Canadon Seco crudeoils, respecti vely: HO, AH, and CS. These crudeoils are asphaltene rich and vary in viscosity, resincontent and asphaltene H/C ratio. Basic crude oiland asphaltene properties can be found in Table 1 .Resin content was determined by sequential elu-tion chromatography (discussed in the next sec-tion), H/C ratios were calculated from combustionelemental analysis (Perkin Elmer Series IICHNSO), and viscosity measurements were per-formed on a Rheometrics Dynamic Stress Rhe-ometer with concentric cylinder geometry.

    Asphaltenes precipitated from the crude oils wereseparated into more and less soluble fractions by

    dissol ving in toluene and inducing partial precipi-tation through heptane addition. Enough heptanewas added during fractionation to generate ap-proximately 33% (w/w) insoluble asphaltenes froma 0.75% (w/ v) asphaltene solution in toluene. Allsolvents were HPLC grade and obtained fromFisher Scientific. Details of the precipitation andfractionation procedures can be found in anotherpublication [44]. A summary of the elementalcomposition of the asphaltene fractions is pro-vided in Table 2 .

    2.2. SARA fractionation

    Petroleum resins were isolated via the SARAtechnique where DAO is charged to silica gel andextracted with sol vents of increasing polarity [51 /53,67] . After a two stage filtration to ensurecomplete remo val of the asphaltenes, the hep-tane-diluted crude oil was rotary e vaporated untildry. The DAO was dissol ved in methylene chloride(Fisher-HPLC grade) and adsorbed to acti vatedsilica gel (Chromatographic silica gel, 35 /60 mesh,Fisher). Silica gel acti vation proceeded undervacuum at 120 8 C for 48 h. The silica gel /DAOslurry was shaken for 24 h then rotary e vaporateduntil dry and placed in a nitrogen flushed vacuumoven at 50 8 C for 24 h.

    Chromatography columns (2 ) /100 cm with 250ml sol vent reser voir) were initially filled with amixture of 68:32 heptane /toluene ( v/v). Cleanacti vated silica gel was added until the depthreached /20 cm. Finally, silica gel with adsorbedDAO was transferred to the column until full. Asolvent mixture containing 68% ( v/v) heptane and32% (v/v) toluene eluted saturates, mono-, di-, and

    triaromatics from the silica gel. Once the saturatesand aromatics were extracted, a more polar

    Table 1Crude oil properties

    Crude wt.% Asph R/A ratio H/C Asph Viscosity (cP) 100 8 F

    AH 6.7 1.12 1.14 33.8B6 13.1 0.92 1.24 2030CS 7.5 1.19 1.11 70HO 14.8 1.39 1.29 363

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    solvent (40:30:30 acetone:toluene:methylene chlo-ride) was applied to elute the resins. The resin-solvent mixture was filtered to remo ve any silica

    gel fines and rotary e vaporated until dry. Theresins were transferred to jars and placed in anitrogen flushed vacuum o ven at 60 8 C for 48 h oruntil completely dry. Combustion elemental ana-lyses of the resins appear in Table 3 .

    2.3. Asphaltene and resin solubility

    The solubility of asphaltenes and their sub-fractions were determined in heptol with addedresins. Resins from the crude oil were only addedto their complementary asphaltenes. Solubilityprofiles of the asphaltenes without resins wereobtained in another study [44] and will be used forcomparison. Resin /asphaltene solutions were pre-pared in various mixtures of heptane and toluene.The asphaltene concentration was 0.75% w/ v ( /1wt.%) in 15 mL sol vent and the resin /asphalteneratio was 1:1 by mass. Resins and asphaltenes weredissol ved together in toluene and allowed to shakefor 12 h prior to heptane addition. After anadditional 12 h, the solutions were vacuum filtered

    through 1.5 mm Whatman 934 AH filter paper tocollect precipitates and rinsed with 7.5 ml of heptol

    at the same toluene volume fraction. To ensure allof the resins were remo ved, the precipitate wasrinsed with neat heptane prior to dissolution in

    methylene chloride. The % precipitated was deter-mined from the mass ratio of precipitated asphal-tenes to the original asphaltene mass.

    2.4. Small-angle neutron scattering

    Neutron scattering of asphaltenic aggregatessolvated by resins was performed on the NG7and NG1 small angle spectrometers at the NISTCenter for Neutron Research (Gaithersburg, MD)or on the Small Angle Neutron Diffractometer(SAND) at Argonne National Laboratory (IPNS,Argonne, IL). Samples were measured in cylind-rical quartz cells (NSG Precision Cells) with a pathlength of 5 mm (all NG7 samples) or 2 mm (allSAND samples).

    Mixtures of asphaltenes and resins were pre-pared at resin:asphaltene (R/A) ratios between0.25:1 and 10:1. Asphaltene solutions (1 wt.%)were prepared in perdeuterated heptane andtoluene solutions (CDN Isotopes, Canada) andstudied at 25 and 80 8 C. Scattering intensity versus

    scattering angle (I(Q) vs. Q) data were fit toLorentzian line shapes using a non-linear leastsquares regression to determine the aggregatecorrelation lengths. Following Ornstein /Zernikeformalism the scattering intensity, I, can be relatedto the scattering vector, Q, by:

    I(Q) 0I0

    1 ' (Q j )2(1)

    where j is the correlation length, I 0 is the scatter-ing intensity at Q 0 /0 [42,68]. In some asphaltene

    Table 2Asphaltene fraction composition in wt.%, except H/C

    Asphaltene H/C Nitrogen SulfurSol Whole Ppt Sol Whole Ppt Sol Whole Ppt

    AH 1.17 1.14 1.13 0.92 1.02 1.08 8.06 8.32 7.66B6 1.30 1.24 1.22 1.81 1.87 1.93 7.25 6.68 6.33CS 1.12 1.11 1.09 1.32 1.32 1.39 0.52 0.52 0.48HO 1.30 1.29 1.24 1.95 1.99 2.11 8.42 8.53 8.48

    Table 3Resin composition in wt.%, except H/C (O by difference)

    Resin source H/C N S O

    AH 1.31 0.81 6.49 1.53B6 1.51 1.48 6.91 1.98CS 1.39 1.52 0.88 2.77HO 1.51

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    systems, a Porod upturn was obser ved at low Qwhere the scattering intensity increased monoto-nically with decreasing Q. Furthermore, incoher-ent scattering of all nuclei in the sol vent and solutewith non-zero spin was manifested in the scatter-ing cur ves at large Q values (typically Q ! /0.1) asan isotropic background signal. The Q values thatmarked the transition from the Guinier regime tothe Porod or incoherent scattering regimes weredetermined from inflection points in the scatteringcur ves. The Lorentzian line shape described in Eq.(1) was applied o ver the intermediate range of Qvalues between the inflection points.

    In the absence of a significant low Q upturn,

    Guinier analysis was also performed to calculatethe radius of gyration, R g, which is defined as themean squared distance from the center of gra vityof the scatterer. The Guinier approximation ap-plies to aggregates in dilute solution and is strictlyvalid in the low Q range where QR g is less than 1.The Guinier approximation has the form:

    I(Q) 0 I0e(( Q2 R 2g=3) (2)

    where

    I0 0 N p Vp (Dr )2

    (3)

    and N p is the number of scatterers, V p is thescatterer volume, and Dr 2 is the coherent scatter-ing contrast between the sol vent and solute. Gi venthat elemental compositions of the asphaltenesand resins are a vailable, it is possible to calculatethe scattering contrast terms and subsequently, theweight-a verage molecular weight of the aggregatesin the Guinier regime. These analyses will beaddressed in a future paper.

    Comparing the analytical form of the Guinierapproximation and Lorentzian lineshapes predictsthat R g should be proportional to j by a scalefactor of 3 (or /1.73). A comparison of the R gand j values obtained from experiments onasphaltene and resin mixtures in heptol pro videsthe relation R g 0 /1.71 j . This suggests that Guinieranalysis and Lorentzian fits are equally suitablefor extracting rele vant aggregation beha vior fromscattering cur ves. Further details concerning theSANS instruments, experimental conditions, anddata analysis methods are pro vided elsewhere [44].

    2.5. Resin / asphaltene emulsions

    Water-in-oil emulsions were prepared by homo-genizing water and model oil solutions containingasphaltenes and resins. Asphaltenes and resinswere dissol ved together in toluene for approxi-mately 12 h followed by heptane addition. A 4 mLaliquot of this solution with an asphaltene con-centration of 0.37% w/ v ( /0.5% w/w) was homo-genized with a 6 ml aliquot of deionized water. AVirtis Virtishear Cyclone I.Q. homogenizer with a6 mm rotor /stator emulsion generator assemblywas lowered into the oil /water system and run at15 000 rpm for 3 min.

    After aging 24 h, the emulsions were centrifugedfor 1 h at 15 000 rpm. The stability of theemulsions was calculated from the volume of water resol ved:

    % Water resolved 0Volume resolved

    Initial volume) 100 (4)

    Complete details on solution preparation andhomogenization can be found elsewhere [49].

    3. Results and discussion

    3.1. Asphaltene / resin solubility

    The effect of adding resins (1:1 mass ratio) onasphaltene solubility is shown in Fig. 2 (a /d). Thehalf filled markers represent solubility data deter-mined for asphaltenes in neat heptol while thefilled markers represent asphaltene solubility withresins. As mentioned before, the solubility limits of the whole asphaltene fractions were approximately50% toluene. The more soluble fraction or Solu-ble asphaltenes precipitated at toluene volumefractions between 0.3 and 0.4 while the less solubleor Precipitate asphaltenes precipitated at consid-erably higher aromaticity (0.6 /0.8). This indicatesthat the Soluble fraction cooperati vely sol vates thePrecipitate fraction in solution.

    The process of fractionation generated uniqueasphaltene classes distinguished by their solubilitybeha vior. The Precipitate fractions were character-ized by higher aromaticity, polarity, molecular

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    weight, and aggregate size than the Whole orSoluble asphaltene fractions. Their beha vior in thepresence of resins should help elucidate themolecular mechanisms of sol vation and aggrega-tion.

    The asphaltene solubility limit, after resin addi-tion, was reduced as much as 10% ( v/v) toluene. Inthe precipitated regime, resins were capable of enhancing asphaltene solubility (reducing the per-centage of precipitates) between 10 and 50%.Resins appear to enhance the solubility of themore polar and aromatic Precipitate asphaltenesmore so than the Soluble asphaltenes. Solubleasphaltenes are less polar and aromatic and do notrespond as fa vorably to resin addition in highlyaliphatic sol vents. Of note is the considerablesolvating effect of CS resins on CS Whole and

    Precipitate fractions. These interactions suggestthat CS resins play a significant role in asphaltenesolvation in the crude oil.

    Asphaltenes form aggregates in solutionthrough intermolecular p-p and hydrogen bondsbetween asphaltene monomers. Resins reduce thetendency for asphaltenes to aggregate by disrupt-ing these intermolecular interactions. From Table3 we see that resins contain polar heteroatomswithin a mixed aromatic /aliphatic carbon matrix.Similar to asphaltenes, resins are polydisperse andonly a verage chemical properties can be measured.Polar functional groups gi ve resins the capacity todisrupt the electron donor /acceptor interactionspartly responsible for asphaltene aggregation.Resins, howe ver, are less aromatic than asphal-tenes as gauged by H/C ratios between 1.31 and

    Fig. 2. Solubility of 0.75% (w/ v) Whole asphaltenes and their more and less soluble subfractions in heptol with and without resins.Half lled markers denote systems without resins. R/A ratio was xed at 1:1 by mass. a) AH, b) B6, c) CS, d) HO.

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    1.51. Due to decreased aromaticity, their solubilityin more strongly aliphatic sol vents is considerablyhigher than asphaltenes. Aromatic moieties inresins likely sol vate the fused ring portion of theasphaltenes, producing a sol vated, stabilized, re-sin /asphaltene aggregate. The ability of resins todissociate intermolecular asphaltene bonds resultsin reduced aggregate sizes.

    3.2. SANS: asphaltenes and resins in heptol

    SANS allows us to probe the effects of resins onasphaltene aggregation. In another SANS study,

    we found that asphaltene Precipitate fractionsformed larger aggregates than the unfractionatedor more soluble fractions [44]. Scattering cur veswere fit with Lorentzian lineshapes to determinethe solute correlation lengths. Fig. 3 shows typicalI(Q) versus Q neutron scattering cur ves for CSWhole asphaltenes with added B6 resins in 60%toluene at 25 8 C. The solid lines represent the non-

    linear least squares fit of the Lorentzian lineshapeto the data. Based on the shape of the neutronscattering cur ve alone, one can readily distinguishtwo length scales of aggregate sizes in typicalasphaltene solutions. For example, the scatteringcur ve for CS Whole asphaltenes with no addedresins in 60% toluene ( Fig. 3 (a)) is a superpositionof a Guinier plateau at intermediate Q and anintense power law feature at low Q. The Guinierplateau region indicated scattering from soluble,non-flocculating aggregates on the order of ap-proximately 20 /100 A . The presence of a low Qfeature indicated flocculation of a portion of thesoluble aggregates. The absence of a secondplateau region in the lowest Q range suggeststhat the largest flocs had a size greater than theorder of 1/Q min (or ] /200 A ). The decrease inintensity of the low Q feature with increasing resincontent indicated that resins were effecti ve atdissol ving the larger flocs into non-interactingaggregates. A reduction in the correlation length

    Fig. 3. SANS ts (2 mm path length) using Lorentzian lineshapes. Canadon Seco Whole asphaltenes at 25 8 C in 60% toluene with: (a)No Resins: I 0: 11.7 9 /0.4, j : 1019 /3, R

    2: 0.9958. (b) 0.5 wt.% B6 Resins: I 0: 6.99 /0.1, j : 709 /1, R2: 0.9962. (c) 2 wt.% B6 Resins: I 0:

    4.56 9 /0.06, j : 48.59 /0.8, R 2: 0.9967. (d) 4 wt.% B6 Resins: I 0: 3.809 /0.03, j : 36.99 /0.5, R 2: 0.9970. (e) 6 wt.% B6 Resins: I 0: 4.029 /0.05,j : 31.19 /0.6, R 2: 0.9940. (f) 10 wt.% B6 Resins: I 0: 3.309 /0.04, j : 22.59 /0.4, R

    2: 0.9922. Note: E very 2nd data point plotted abo ve Q 0 /0.006. Units of I. and j are cm

    ( 1 A respecti vely.

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    from 101 A (no resins) to 23 A (10% resin)indicated that resins were also effecti ve at solubi-lizing the indi vidual asphaltene aggregates.

    One tri vial explanation for the decrease inSANS scattering intensity with increasing resincontent is the notion that resins themsel ves formsmall aggregates similar to asphaltenes. Uponmixing the asphaltene aggregates with an increas-ing number of smaller resin aggregates the a verageparticle size is expected to decrease. While resinaggregation is certainly a plausible explanation forreduced correlation lengths, asphaltene /resin in-teraction in solution cannot be fully discounted.The solubility studies discussed pre viously ha ve

    shown that resins play a role in enhancingasphaltene solubility in solution. We will alsoshow that resins are capable of modifying thesurface-acti vity of asphaltenes, thus affecting theirability to stabilize emulsions. The resins used inthis study were incapable of forming stable emul-sions at any concentration or sol vent condition.

    Results from both the solubility and emulsionstudies suggest that some interactions with resinsmodify the asphaltene aggregates to some extent.Bardon et al. compared the scattering cur ve of an

    asphaltene /

    resin mixture to the sum of the scat-tering intensities from pure asphaltenes and pureresins [47]. Since the sum of the indi vidualscatterers was larger than the scattering by themixture, they concluded that asphaltenes weresolvated by resins. Furthermore, they assumedthe pure asphaltene scattering intensity was thedifference between the mixed asphaltene /resin andpure resin (same concentration) scattering pat-terns. The correlation lengths reported in thisstudy were calculated using scattering cur vesfrom the mixed asphaltene /resin solutions, assum-ing that the scattering from resin-only aggregatesin negligible.

    The effect of resins from B6 and AH crude oilson asphaltene aggregation is shown in Fig. 4 . B6Whole asphaltenes in pure toluene and 60% ( v/v)toluene in heptol were combined with AH and B6resins at 80 8 C. As shown in the figure, correlationlengths of B6 Whole asphaltenes sol vated by resinsin pure toluene were identical with either AH orB6 resins. In the mixed sol vent, AH resins maysolubilize B6 asphaltenes slightly more effecti vely

    than B6 resins. Abo ve a 4:1 R/A ratio, thecorrelation lengths obtained for the asphaltene /resin systems were within 10%, regardless of theresin type. This suggests that resins from differentsources may be approximately equal in effecti ve-ness at sol vating asphaltenic aggregates. Modestdifferences in resin aromaticity and polarity (seeTable 3 ) are secondary to differences in asphaltenechemistry and sol vent conditions for dictatingaggregate size in crude oil systems. The aggrega-tion beha vior of B6 Whole asphaltene /resin solu-tions shown in Fig. 4 is typical of the other Wholeasphaltenes as well. In the absence of resins,Whole asphaltene correlation lengths followedthe trend: CS ! /B6 ! /HO ! /AH. Resin additionwas effecti ve at disrupting the intermolecularbonding and aggregation of each asphaltene to asimilar extent. The greatest decrease in aggregatesize occurred between 0.5 and 2:1 R/A suggestingresins strongly sol vate asphaltenes at ratios closeto those found in crude oil ( Table 1 ). As the R/Aratio approached 10:1 the Whole asphaltenecorrelation lengths neared a common value of approximately 11 /14 A , suggesting this may beclose to a sol vated monomer or irreducible oligo-mer.

    In less aromatic sol vents, asphaltenes formlarger aggregates due to sol vent /solute incompat-ibility. Heptane /toluene mixtures of increasingaliphaticity sol vent possess a lower degree of p-bond sol vating capability and polarity than a puretoluene sol vent. As a result, asphaltenes withoutresins in 60% ( v/v) toluene ha ve larger correlationlengths than in pure toluene. For example, B6Whole asphaltenic aggregates ha ve correlationlengths of 79 A at a toluene volume fraction of

    0.6 as compared with 43 A in pure toluene.Howe ver, at a R/A ratio of 10:1 the B6 Wholecorrelation length appears to plateau at similarvalues ( /14 /18 A ) regardless of the sol ventaromaticity. This indicates that high resin concen-trations are apparently more effecti ve at reducingaggregate size than sol vent alone. This comes as nosurprise since resins are more chemically similar toasphaltenes and ha ve been linked to asphaltenesolubility in a variety of systems including crudeoil.

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    3.3. Asphaltene / resin emulsion stability: effect of v aried R/A ratio

    Asphaltene emulsions were prepared in thepresence of resins at R/A ratios from 0.5 to 10and their stabilities were gauged by measuring vol.% water resol ved after centrifugation. Theseemulsion stabilities were compared with aggregatecorrelation lengths determined by SANS ( Figs. 5 /7). As shown in Fig. 5 , resin addition decreasedboth the aggregate correlation length and stabilityof emulsions formed by CS Whole asphaltenes in60% toluene. This trend was also obser ved for B6

    and HO Whole asphaltenes, although CS Wholeasphaltenes formed much weaker emulsions thanboth B6 and HO Whole at similar sol vent condi-tions. CS asphaltenic aggregates were the mostaromatic and least polar of the Whole asphaltenesstudied. The lack of polarity and possible inabilityto form a network of hydrogen bonds likelyreduced interfacial film strength. Resin additionup to R/A ratios of 2:1 effecti vely sol vated theaggregates and further reduced their emulsionstabilizing ability.

    Con versely, B6 Whole aggregates in 60%toluene were sufficiently surface-acti ve (due to

    high polarity), e ven at R/A ratios approaching 5:1,to adsorb at oil /water interfaces and formemulsion-stabilizing films with 72% waterresol ved. Correlation lengths obser ved for B6Whole asphaltenes in 60% toluene at 80 8 Cdecreased with resin addition from 47 A (0.5:1 R/Aratio) to 18 A (10:1 R/A ratio). Correlation lengthsobser ved for HO Whole asphaltenes in 60%toluene at 80 8 C decreased slightly with resinaddition from 38 A (0.5:1 R/A ratio) to 14 A (10:1R/A ratio). Both B6 and HO Whole asphaltenes

    were high in polarity but HO Whole lacked thesurface acti vity to maintain a cohesi ve oil /waterinterfacial film at R/A ratios greater than 2:1 (92%water resol ved). Howe ver, emulsions formed byHO Whole asphaltenes were still more stable thanthose formed by CS Whole asphaltenes undersimilar conditions. Based on the emulsion stabilityresults of the Whole asphaltenes, it is apparentthat higher resin concentrations are needed todestabilize emulsions when asphaltenes are morepolar.

    Fig. 4. Aggregate j of 1 wt.% B6 Whole asphaltenic aggregates with AH and B6 Resins in pure toluene and 60% toluene at 80 8 Cdetermined from SANS (5 mm path length). Legend displayed as (resin type, % toluene).

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    B6 Precipitate emulsions prepared in puretoluene remained very stable in systems containingup to 2:1 resins ( Fig. 6 ). This was due primarily tothe high proportion of film forming species in B6Precipitate. The fractionation process concen-

    trated the most aromatic and polar asphaltenesin the Precipitate fraction and, as a result, theytended to aggregate, adsorb and consolidate intoelastic films at oil /water interfaces. As the R/Aratio approached 2:1, the film forming portion of

    Fig. 5. Emulsion stability (% water resol ved) and aggregate j of CS Whole asphaltenes in 60% toluene with added resins. R/Arepresents mass ratio of resins to asphaltenes. Emulsions tested using CS resins, 0.5 wt.% asphaltenes. SANS j measured at 25 8 C usingB6 resins, 1 wt.% asphaltenes, 2 mm path length.

    Fig. 6. Emulsion stability (% water resol ved) and aggregate j of B6 Precipitate asphaltenes in toluene with B6 resins. Emulsions testedat 0.5 wt.% and j determined by SANS at 25 8 C, 1 wt.% asphaltenes, and 2 mm path length.

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    Precipitate asphaltenes were in sufficient supply tomaintain nearly complete emulsion stability. Theslight increase in stability from 0 to 0.25:1 R/A waslikely due to enhanced asphaltene solubility andlability of the aggregates. In the absence of resins,the aggregate size may ha ve been too large forasphaltenes to effecti vely cover water dropletinterfaces and for w/o emulsions to achie ve highstability. As the large aggregates were sol vated byresins, they became more interfacially acti ve andformed a cohesi ve film. Beyond 2:1 R/A theasphaltenic aggregates became increasingly solu-ble, less surface-acti ve, and consequently formedweaker emulsions. The most dramatic decrease inasphaltene correlation length occurred between R/A ratios of 0.5 and 2. A minimum aggregate sizewas approached abo ve 2:1 R/A and the asphal-tenes were sufficiently sol vated that they lost theirinterfacial acti vity.

    B6 Precipitate asphaltenes were beyond the limitof solubility in 30% toluene and the emulsionsprepared without resins were not particularlystable ( Fig. 7 ). The increase in correlation lengthwith addition of resins to a R/A ratio of 10:1indicated that resins facilitated the dissolution of the insoluble asphaltenes. As more interfaciallyacti ve material was dissol ved, the emulsion stabi-

    lity increased. The maximum in correlation lengthdid not coincide with the maximum in emulsionstability, perhaps because different initial asphal-tene concentrations were used for the SANS andemulsions experiements. The emulsions weretested at an asphaltene concentration of 0.5 wt.%and SANS experiments were performed at 1 wt.%.Fewer resins were needed to dissol ve asphaltenesat the lower concentration, thus the maximum inemulsion stability was shifted to a R/A ratio of 5:1.At R/A of 20:1, the additional resins sol vated anddissociated the asphaltenic aggregates renderingthem less surface-acti ve, and reducing the emul-sion stability.

    Similar trends in aggregate size and emulsionstability were obser ved for CS Precipitate asphal-tenes in pure toluene and in 50% toluene. In puretoluene, correlation lengths increased from 101 A (no resins) to 128 A (0.5:1 R/A ratio) as resinaddition dissol ved the insoluble species followedby a monotonic decrease with further resin addi-tion to 26 A (10:1 R/A ratio). CS Precipitateasphaltenes did not form particularly stable emul-sions in pure toluene and the addition of resins hada modest effect on emulsion stability. As expected,CS Precipitate asphaltenes were also partiallyinsoluble in 50% toluene and the addition of resins

    Fig. 7. Emulsion stability (% water resol ved) and aggregate j of B6 Precipitate asphaltenes in 30% toluene with B6 resins. Emulsionstested at 0.5 wt.% and j determined by SANS at 25 8 C, 1 wt.% asphaltenes, and 2 mm path length.

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    up to a R/A ratio of 2:1 aided the dissolution of the insoluble species. Correlation lengths obser vedfor CS Precipitate in 50% toluene increased from98 A (0.5:1 R/A ratio) to 108 A (2:1 R/A ratio)followed by a decrease to 31 A (10:1 R/A ratio). Asmore interfacially acti ve material was dissol ved,the emulsion stability increased markedly from52% water resol ved (no resins) to 25% waterresol ved (5:1 R/A ratio).

    3.4. Asphaltene (Soluble, Whole, Precipitate) / resin emulsion stability

    The stability of emulsions prepared with AHWhole and its fractions at se veral heptol ratios areshown in Fig. 8 (a /c). As with the pre viousexperiments, the asphaltene concentration was0.37% (w/ v), or equi valently 0.5% (w/w), and theresin /asphaltene ratio was varied. The volumefractions of toluene were chosen such that theasphaltenes were either abo ve or below theirsolubility limits. AH Soluble asphaltenes in 60%toluene formed weak emulsions that becameincreasingly unstable as resin concentration in-

    creased ( Fig. 8 (a)). The asphaltenes were verysoluble at these conditions and could not forminterfacial films capable of withstanding rupture.AH Soluble asphaltenes in 30% toluene werepartially precipitated. Resin addition initially sol-vated the flocculated aggregates at R/A ratios of 0.25 and 0.5 resulting in enhanced emulsionstability. Further sol vation by resins completelydestabilized the emulsions at a R/A ratio of 2. AHWhole asphaltenes formed emulsions in 55%toluene with nearly 50% water resol ved (Fig.8(b)). In the insoluble regime, (30% toluene) theemulsions formed were initially weaker due tonon-surface-acti ve, flocculated asphaltenic aggre-gates. Resin addition up to 0.5:1 R/A increased theemulsion stability as insolubles were dissol ved intosolution. At higher R/A ratios, the 30% toluenesystem became highly sol vated and emulsions weredestabilized. Much the same effect was seen withAH Precipitate asphaltenes ( Fig. 8 (c)) where theemulsions containing the most soluble asphaltenesbecame unstable while partially insoluble systemsactually formed stronger emulsions.

    Fig. 8. Emulsion stability (% water resol ved) of AH asphal-tenes in heptol with AH resins. Emulsions tested at 0.5 wt.%,25 8 C. (a) Soluble: 30, 60% toluene. (b) Whole: 30, 55% toluene.(c) Precipitate: 30, 60% toluene.

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    Fig. 9. Emulsion stability (% water resol ved) of CS asphaltenes in heptol with CS resins. Emulsions tested at 0.5 wt.%, 25 8 C. (a)Soluble: 40, 50, 60% toluene. (b) Whole: 30, 45, 60% toluene. (c) Precipitate: 50, 100% toluene.

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    The emulsions formed by CS Whole asphaltenesand its more and less soluble asphaltene fractionswere typically unstable. In the soluble regime, theability of each asphaltene to form stable emulsionsdecreased with resin addition ( Fig. 9 (a /c)). Theemulsion stability of CS Soluble at 40% tolueneappeared to increase slightly up to an R/A of 0.5:1followed by a decrease. CS Whole asphaltenesformed unstable emulsions beyond an R/A of 1:1due to resin sol vation. The beha vior of partiallyinsoluble CS Precipitate at 50% toluene suggeststhat resins were capable of a modest enhancementof emulsion stability. E ven when the systems wererendered more soluble with resins, emulsion stabi-lity did not increase appreciably. High aromaticity,as suggested by low H/C ratios, likely caused theformation of large aggregates through p /p inter-actions between asphaltene monomers and re-duced aggregate lability. These properties suggest

    that CS asphaltenes are inherently weak emulsi-fiers possibly due to large aggregate formation,low polarity and an inability to form hydrogenbonds.

    Unlike the weak emulsions formed by AH andCS asphaltenes o ver a wide range of sol ventconditions, B6 and HO asphaltene-stabilized emul-sions were considerably stronger. The effects of resins on emulsion stability in the soluble andinsoluble regimes are quite apparent. In Fig. 10 (a),resins are shown to destabilize emulsions in thesoluble regime of B6 Soluble. In the insolubleregime (30% toluene), emulsion stability is reducedonly after reaching a 5:1 R/A ratio. Resins initiallydissol ved precipitated asphaltenes and renderedthem interfacially acti ve until the system becametoo soluble and the dri ving force for film forma-tion disappeared. In a highly aliphatic sol vent(10% toluene:90% heptane) B6 Soluble asphaltenes

    Fig. 10. Emulsion stability ( vol.% water resol ved) of B6 asphaltenes in heptol with B6 resins. Emulsions tested at 0.5 wt.%, 258

    C. (a)B6 Soluble: 10, 30, 60% toluene. (b) B6 Whole: 40, 60, 100% toluene. (c) B6 Precipitate: 30, 60, 100% toluene. (d) HO Precipitate: 30,60, 100% toluene.

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    did not form stable emulsions e ven with an R/A of 5:1.

    B6 Whole asphaltenes were studied at threesolvent conditions in the presence of resins ( Fig.10(b)). B6 Whole asphaltenes were completelysoluble at both 60 and 100% toluene. B6 Wholeasphaltenes were very soluble in pure toluene butstill formed stable emulsions up to a R/A of 0.25:1.Beyond this point the emulsion stability rapidlydecreased as a result of enhanced solubility. At60% toluene, B6 Whole asphaltenes approachedtheir limit of solubility in solution and, conse-quently, formed larger aggregates and strongeremulsions than obser ved in pure toluene. As

    discussed in another paper [44], aggregate sizewas obser ved to increase with decreasing sol ventaromaticity up to the asphaltene solubility limit asthe soluble asphaltenes attempted to minimizeinteractions with the increasingly aliphatic sol vent.As shown in Fig. 10 (b), the proximity to thesolubility limit also corresponds to a maximumin emulsion stability. Emulsions of B6 Wholeasphaltenes in 60% toluene e ventually becameunstable at a 10:1 R/A ratio, while a R/A ratioof 5:1 was needed to completely destabilize emul-

    sions in pure toluene. Solutions containing afraction of insoluble asphaltenes (40% toluene)were also able to form very stable emulsions up toa R/A ratio of 5:1. The dissolution of theseinsoluble asphaltenes facilitated strong interfacialfilm formation up to R/A ! /10, at which point theasphaltenes were so strongly sol vated by resinsthat they ceased to be effecti vely surface-acti ve.

    B6 Precipitate asphaltenes were appreciablyinsoluble at both 30 and 60% toluene but solublein pure toluene. B6 Precipitate formed stableemulsions in 60 and 100% toluene; howe ver, at30% toluene, B6 Precipitate asphaltenes were notsufficiently soluble to stabilize emulsions ( Fig.10(c)). The effect of adding resins at 30% toluenewas to effecti vely dissol ve the insoluble asphal-tenes and form strongly stable emulsions abo ve aR/A of 5:1. E ven at 20:1 R/A, there still existed asufficient supply of film forming material to formrelati vely stable emulsions, a remarkable obser va-tion. This le vel of solubility is quite high andsuggests that B6 Precipitate asphaltenes ha veunique molecular structures that allow them to

    stabilize emulsions in the presence of large con-centrations of strongly sol vating resins. In parti-cular, a balance between aromaticity andhydrogen bonding capacity must exist to allowstability in both pure toluene with no resins (higharomaticity, low polarity) and in highly aliphaticsolvents with substantial resin content (low aro-maticity, high polarity).

    The effecti veness of resins at solubilizing as-phaltenes surely depends on asphaltene and resinchemical composition and on the supportingaliphatic and aromatic sol vent. B6 Whole asphal-tenes formed stable emulsions at 40% toluenewithout resins but were only 60% soluble ( Fig.

    2). The amount of precipitated material decreasedbelow 10% at an R/A of 1:1. Abo ve this resincontent, the asphaltenes were soluble and formedstable emulsions up to R/A of 5:1. Furthersolvation by addition of resins e ventually destabi-lized the emulsions. At 30% toluene, B6 Precipitateasphaltenes did not form stable emulsions. Appar-ently, either the amount of soluble material wasinsufficient and/or the soluble material was inaggregates of too large a size to effecti vely coverwater droplet surfaces. Emulsion stability in-

    creased slightly by adding resins of equal massratio to asphaltenes. Solubility measurements in-dicated that the asphaltenes were nearly insolubleat these conditions. Howe ver, at an R/A of 5:1, B6Precipitate solubility increased from essentiallyinsoluble to 55% soluble and emulsion stabilityreached a maximum. Further sol vation with resinsdid not enhance gra vimetric solubility, but emul-sion stability decreased substantially.

    HO Whole and its more and less solublefractions beha ved in a very similar fashion to B6asphaltenes; howe ver, HO Precipitate asphalteneswere obser ved to form e ven stronger emulsionsthan B6 Precipitate fractions ( Fig. 10 (d)). HOPrecipitate asphaltenes were solubilized with resinsat 30% toluene and formed stable emulsions up toR/A ratios of 20:1. Again, in the regime in whichHO Precipitate asphaltenes were soluble, theaddition of resins led to emulsion destabilization.

    The power of resins to sol vate asphaltenes of varied chemical composition is e vident fromSANS, solubility, and emulsion stability measure-ments. In addition, the ability to dissol ve insoluble

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    asphaltenes and render them capable of emulsionstabilization is remarkable. Howe ver, this resin /asphaltene interaction appears to act primarilywith HO and B6 Precipitate, and CS to a lesserdegree, and must be linked significantly to themolecular structure of these asphaltenes. HO andB6 Precipitate fractions ha ve the highest polarityof any of the fractions pre viously prepared (seeTable 2 ). The H/C ratio of these fractions is alsolower than B6 or HO Whole but not as low as AHor CS asphaltenes, indicating a moderate le vel of aromaticity. These chemical properties suggestthat aggregation and film formation may be dri venmore so by polar heteroatom interactions such as

    hydrogen bonding than by p /p bonding betweenasphaltenic aromatic moieties. AH and CS asphal-tenes contain low concentrations of polar nitrogenand likely aggregate via aromatic stacking. With-out sufficient proton donor /acceptor sites, theasphaltenes cannot adsorb and form a cohesi vefilm at the oil /water interface.

    4. Conclusions

    In this study, resins isolated by SARA fractio-nation had a strong sol vating effect on asphaltenesand their more and less soluble subfractions * /so-called Soluble and Precipitate asphaltenes. Atan R/A ratio of 1:1, the toluene concentration atwhich asphaltenes began to precipitate in heptolwas reduced by as much as 10%. The sizes of asphaltenic aggregates, as gauged by correlationlengths from neutron scattering, were obser ved todecrease significantly upon addition of resins. Atroom temperature, the correlation lengths of Whole asphaltenes approached a value of approxi-mately 14 /18 A at high resin concentrations (R/Aof 10:1) regardless of asphaltene, resin type, or %toluene (in the soluble regime). Furthermore, thegreatest decreases in aggregate size occurred atconditions found in typical crude oils (i.e. R/Aratios between 0.5 and 2:1). It is not known towhat extent the aggregates can be dissociated byresin addition. The presumed minimum would be asingle asphaltene monomer sol vated completely byresins. In the portion of the phase diagram inwhich asphaltenes were insoluble, aggregate sizes

    increased with resin addition up to the solubilitylimit as the more polar, insoluble asphaltenes weredissol ved into solution. Once the insolubles weredissol ved, additional resins sol vated the largest of the soluble aggregates as obser ved by a decrease inthe correlation length.

    Asphaltene stabilized emulsions were susceptibleto the effects of resin sol vation. Soluble asphal-tenes typically formed the weakest emulsionsbecause the aggregates were small, well sol vated,less aromatic, and less polar than the Whole andPrecipitate fractions, and consequently, less inter-facially acti ve. Soluble and Whole asphaltenes attoluene concentrations in the insoluble regime

    could be sol vated by resin addition to produceslightly more stable emulsions. Resins completelydestabilized emulsions of Whole and Solubleasphaltenes in the portion of phase space at whichthese asphaltenes were soluble at a R/A of 2:1,except in the case of B6 Whole, which formedstable emulsions up to a R/A of 10:1.

    AH and CS Precipitate asphaltenes were pooremulsion formers without resins and their emul-sions were only modestly more stable with resins.Their lack of polarity, e ven when sol vated to

    become more labile, pre vented them from inter-acting strongly at oil /water interfaces. B6 and HOPrecipitate, howe ver, formed very stable emulsionsin their soluble regime that were resistant to thesolvating effects of resins. Both approached com-plete instability near a R/A of 10:1. At 60% tolueneB6 and HO Precipitate asphaltenes were partiallyinsoluble but formed very stable emulsions due totheir highly polar and H-bonding nature. Resinsadded to these systems dissol ved the insolubleasphaltenic flocs, rendering them interfaciallyacti ve. Once B6 Precipitate asphaltenes weresolubilized, emulsions remained stable e ven at aR/A of 20:1. In highly aliphatic sol vents (30%toluene), B6 and HO Precipitate asphaltenes werelargely insoluble and did not form stable emul-sions. Resins were able to sol vate these systems toa considerable extent and led to stable emulsionsat R/A ratios of 20:1.

    Comparisons between aggregate sizes and thestability of oil-in-water emulsions formed at var-ious R/A ratios suggested that the most stableemulsions formed from soluble aggregates of

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    maximum size and greatest interfacial acti vity.These aggregates in variably formed at the limitof asphaltene solubility. Modest differences inresin aromaticity and polarity are secondary toasphaltene chemistry and sol vent conditions fordictating aggregate size and emulsion stability inasphaltene solutions.

    The remarkable ability of resins to sol vateasphaltenes can be attributed to the polar anddispersi ve nature of the resin molecules. In highlyaromatic sol vents, where p /p interactions betweenasphaltenic aggregates are largely mitigated, resinsserve to further disrupt polar and hydrogen-bonding interactions within asphaltene aggregates.

    At low sol vent aromaticity, resin sol vation aids tobreak flocs by disruption of dispersion and hydro-gen bonding interactions between aggregates. Forsystems containing asphaltenes with high polarityand surface acti vity (e.g. B6 and HO Whole andPrecipitate), resin sol vation is sometimes insuffi-cient to induce complete emulsion destabilization.Weak emulsion formers and Soluble asphaltenespossessing a lower polarity and aromaticity areeasily destabilized in the presence of resins. Ag-gregation and film formation in petroleum fluids

    are likely dri ven by polar heteroatom interactions,such as hydrogen bonding. The most polarasphaltenes, typically concentrated in the leastsoluble fraction, require the largest concentrationof resins to completely destabilize asphalteneemulsions and likely cause many petroleum pro-duction problems such as pipeline deposition andwater-in-crude oil emulsion stabilization.

    Acknowledgements

    This work was supported by grants from theNational Science Foundation (CTS-981727),PERF (97-07), and shared consortium fundingfrom ExxonMobil, Ondeo-Nalco Energy Systems,Shell Oil Company and Texaco. Special thanks goto George Blankenship and Semaj McI ver whoassisted with the experimental work. We wouldlike to thank Eric Sirota of ExxonMobil Corpo-rate Research for acquiring the SANS beam timeat NIST and Min Lin for his assistance on theNG-7 and NG-1 beamlines. We are grateful to the

    Department of Energy, Argonne National La-boratory, and particularly to Pappannan Thiya-garajan and Denis Wozniak for their assistance onthe SAND instrument. We also want to thankMarit-Helen Ese and Jihong Tong for helping withthe SANS data collection.

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