A generalized model to predict the liquid–liquid equilibrium in the systems furfural+lubricating oils

A generalized model to predict the liquid–liquid equilibrium in the systems furfural+lubricating oils

Chemical Engineering Science 61 (2006) 8028 – 8039 www.elsevier.com/locate/ces A generalized model to predict the liquid–liquid equilibrium in the sy...

200KB Sizes 0 Downloads 52 Views

Chemical Engineering Science 61 (2006) 8028 – 8039 www.elsevier.com/locate/ces

A generalized model to predict the liquid–liquid equilibrium in the systems furfural + lubricating oils Baudilio Coto ∗ , Rafael van Grieken, José L. Peña1 , Juan J. Espada Department of Environmental and Chemical Technology, School of Experimental Sciences and Technology (ESCET), Rey Juan Carlos University, c/Tulipán s/n, 28933, Móstoles (Madrid), Spain Received 22 May 2006; received in revised form 13 September 2006; accepted 14 September 2006 Available online 23 September 2006

Abstract In the lubricating oil manufacturing process, the aromatic content of vacuum distillates is reduced by solvent extraction, frequently with furfural. These mixtures present very complex composition which makes difficult the description of the liquid–liquid equilibrium involved. In previous studies, the possibility to describe such equilibrium by using a reduced number of pseudo-components and the NRTL model has been stated. In this work, a generalized model to describe the liquid–liquid equilibrium in the systems furfural + lubricating oils is presented. The generalized model is based on a correlation of pseudo-component properties (specific gravity, density, refractive index and sulfur content) and NRTL parameters with the oil average boiling temperature which has been developed from the model description for SPD and HND mixtures. This method allows to set up a suitable thermodynamic model for any lubricant oil cut by using as experimental information only the average boiling point and three physical properties (density, refractive index and sulfur content) of the distillate used as feed. The accuracy of the model was checked by simulating single-stage extractions carried out with different lube oil cuts within the range SPD–HND in different experimental conditions. Calculated and experimental yields, furfural content and physical properties of the raffinates and extracts were compared and a good agreement was obtained. 䉷 2006 Elsevier Ltd. All rights reserved. Keywords: Aromatic extraction; Furfural; Lubricating oils; Liquid–liquid equilibrium

1. Introduction In the process of manufacturing lubricating oil base stocks, removal of aromatic hydrocarbons from vacuum distillates is required to improve several lubricating properties (Singh and Kishore, 1978; Sequeira Jr., 1994). The residue from the crude oil atmospheric distillation (long residue) is transferred to a vacuum distillation column and separated into different lube oil cuts, characterized by their boiling range and viscosity. Five raw cuts are commonly obtained, called spindle distillate (SPD), light neutral distillate (LND), medium neutral distillate (MND), heavy neutral distillate (HND) and bright stock distillate (BSD).

∗ Corresponding author. Tel.: +34 91 4887089; fax: +34 91 4887068.

E-mail address: [email protected] (B. Coto). 1 Alfonso Cortina Technology Centre, REPSOL-YPF, 28933, Móstoles

(Madrid), Spain. 0009-2509/$ - see front matter 䉷 2006 Elsevier Ltd. All rights reserved. doi:10.1016/j.ces.2006.09.037

The aromatic extraction process requires a good solvent which maximize differences in properties between the liquid phases. Furfural is one of the most widely used solvents. Its selectivity towards aromatic compounds is high enough, it decreases slowly when increasing temperature and it is acceptable for both light and heavy vacuum distillates as reported by different authors (Nelson, 1978; Mcketta, 1989; De Lucas et al., 1993). The design and simulation of solvent extraction processes have been done mostly by fully empirical methods (Rahman et al., 1984) that require wide experimental determination. The application of such approach is limited because the experimental information is not usually available. A more rigorous modeling of the extraction process would be a suitable tool to simulate changes in operating conditions or feed quality. To properly describe the liquid–liquid equilibrium (LLE) established in the extraction operation, a consistent thermodynamic model should be based on the equilibrium data of the studied

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

systems. Solvent + lubricating oils are especially difficult systems because the high number of components in these mixtures, and therefore, simplified methods of calculations are needed. The pseudo-components approach based on distillation curves, which is widely used to represent the complex composition of petroleum fractions in the vapor–liquid equilibrium calculations, is not effective in LLE modeling because the chemical structure of the compound has much bigger effect than boiling temperatures. De Lucas et al. (1993) have successfully applied the pseudo-component approach to predict the LLE for the systems furfural+lubricating oils. Recently, Briesen and Marquardt (2004) have reported an adaptive multi-grid strategy based on a discretization to construct correction terms using composition representation. The obtained model, based on molecular information, can be used to describe the LLE. The composition of such complex mixtures is frequently determined by standard test methods, such as ASTM D2007 (Annual Book of Standards, 2003). However, these methods are time and money consuming and, therefore, composition data are not usually available. For that reason, the composition of petroleum mixtures is related with their physical properties, few of them experimentally determined while the remaining are estimated by known correlations. Different authors have proposed accurate relations to calculate the composition of paraffins, naphthenes and aromatics from the refractive index and the viscosity of the mixture (Riazi and Daubert, 1986). However, the use of most of the developed correlations is limited and, therefore, new methods are needed especially for heavy petroleum fractions. Specific gravity (SG), density (D), refractive index (RI) and sulfur content (S%) were selected in this work, since these properties can be successfully correlated with the composition of the lubricant mixtures, obtaining good results for light and heavy lubricant oils (Van Grieken et al., 2005; Coto et al., 2006). In order to describe the LLE in the system solvent+lubricating oils, different thermodynamic models can be used (Poling et al., 2001; Prausnitz et al., 2000; Raal and Mühlbauer, 1998). NRTL (Renon and Prausnitz, 1968) and UNIQUAC (Abrams and Prausnitz, 1975) methods have been used to correlate LLE data for the system furfural + hydrocarbon systems (Letcher et al., 2003; Morawski et al., 2003). Recently, a method based on three pseudo-components (saturates, aromatics and polars) together with the NRTL model has been reported to describe LLE in the systems furfural+light (SPD) and furfural+heavy (HND) lubricating oils (Coto et al., 2006; Van Grieken et al., 2005). The application of such model to describe the extraction operation and to predict properties of petroleum fractions (feed, raffinates and extracts) was also reported. The results obtained in the prediction of several physical properties showed similar or even higher accuracy than those calculated by other methods reported in the literature. However, the application of such models is limited to extraction experiments carried out with light or heavy lubricating oils. In this work, a generalized model was developed from the studies reported for HND and SPD (Coto et al., 2006; Van Grieken et al., 2005). Such generalization is based on the rela-

8029

tion between the pseudo-components properties and the NRTL parameters with the average boiling point of the mixture used as feed. The relations between pseudo-component properties and average boiling point can be used to calculate the composition of the lubricant oil, if it is not experimentally available, by means of an iterative method based on the pseudo-components properties, and developed in this work. Thus, the LLE can be described by means of a reduced number of parameters and using as experimental information only the characterization of the lube oil cut used as feed. To check the accuracy of the proposed model, single-stage extraction experiments carried out with lubricating oil cuts (obtained from light Arabia crude oil and within the range SPD–HND) were simulated with Aspen Plus, using the generalized model. Good results were obtained for the prediction of yields and furfural content of the involved mixtures. The predictions of physical properties (SG, D, RI and S%) calculated by using the generalized model showed a good agreement with the experimental values. 2. Experimental section SPD, LND and MND were provided by REPSOL-YPF from their refinery in Cartagena (Spain). Such mixtures were obtained from light Arabia crude oil. Furfural was also supplied by REPSOL-YPF and distilled before use to remove the oxidation products formed due to air contact. Experimental results for the single-stage extraction experiments were obtained by using a 2L cylindrical stirred glass reactor following the procedure reported by Van Grieken et al. (2005). Temperature was set by recirculating silicone oil from a thermostatic bath, and controlled within ±0.1 ◦ C. A gentle stream of nitrogen was passed to prevent furfural decomposition. Agitation at 430 rpm was maintained for 1 h, followed by settling for another hour to achieve a good separation of the two phases. Furfural was removed from extracts and raffinates by vacuum distillation. Table 1 shows the temperature at which 50% of the lubricating oil is distilled (T50% ) following ASTM D-1160. (SG) and D at 343 K (D343 ) (ASTM D1298), RI at 343 K (RI 343 ) (ASTM D1747) and S% (ASTM D4294) of feed, raffinates and extracts were determined by means of the mentioned ASTM procedures (Annual Book of Standards, 2003). Each mixture is denoted by a letter (R, raffinate; E, extract), followed by the corresponding number of the experiment. From the results shown in Table 1, for experiments at the same temperature, lower yields of extract were obtained when decreasing the furfural/feed ratio: species undergo less dissolution in furfural, and therefore, the efficiency of the extraction is lower. Consequently, the yield of raffinate is higher. When experiments with the same furfural/feed ratio and different temperature are compared, higher temperatures increase not only aromatic extraction, but also other compounds, reducing the selectivity of the process. 3. Generalized model A generalized model to describe the extraction operation was developed from the models previously reported for SPD and

8030

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

Table 1 Experimental results for the extractions carried out with SPD, LND and MND T (K)

Yield (wt%)

Furfural (wt%)

SG

D343 (g/ml)

RI 343

%S (wt%)

SPD (T50% = 651 K) Feed – R-1 1 E-1 1 R-2 4 E-2 4 R-3 7 E-3 7 R-4 1 E-4 1 R-5 4 E-5 4 R-6 7 E-6 7 R-7 1 E-7 1 R-8 4 E-8 4 R-9 7 E-9 7

– 328 328 328 328 328 328 348 348 348 348 348 348 368 368 368 368 368 368

– 74.1 25.9 53.3 46.7 43.8 56.2 67.9 32.1 41.6 58.4 28.0 72.0 53.8 46.2 20.7 79.3 0.8 99.2

– 10.7 82.5 9.0 91.7 7.4 94.2 16.0 78.8 11.4 89.8 10.4 92.7 10.4 92.7 14.3 86.6 – 90.1

0.9123 0.8829 1.0104 0.8599 0.9839 0.8518 0.9676 0.8834 0.9839 0.8572 0.9566 0.8482 0.9342 – 0.9456 0.8545 0.9286 – 0.9215

0.8745 0.8447 0.9738 0.8214 0.947 0.8132 0.9305 0.8452 0.9470 0.8187 0.9195 0.8095 0.9020 – 0.9082 0.8159 0.8910 – 0.8747

1.4889 1.4694 1.5558 1.4550 1.5356 1.4496 1.525 1.4693 1.5363 1.4531 1.5185 1.4481 1.5070 – 1.5118 1.4521 1.5002 1.4509 1.4934

2.76 1.75 5.58 0.88 4.98 0.59 4.49 1.75 4.97 0.76 4.25 0.56 3.90 – 3.90 0.76 3.34 – 2.77

LND (T50% = 717 K) Feed – R-1 1 E-1 1 R-2 4 E-2 4 R-3 7 E-3 7 R-4 1 E-4 1 R-5 4 E-5 4 R-6 7 E-6 7 R-7 1 E-7 1 R-8 4 E-8 4 R-9 7 E-9 7

– 333 333 333 333 333 333 353 353 353 353 353 353 373 373 373 373 373 373

– 80.0 20.0 60.3 39.7 51.5 48.5 75.3 24.7 51.4 48.6 39.5 60.5 66.6 33.4 34.1 65.9 16.5 83.5

10.4 85.2 7.9 92.5 7.1 – 15.4 81.8 11.5 91.0 9.9 93.4 23.4 75.7 15.6 88.1 12.7 91.2

0.9236 0.9009 1.0304 0.8805 0.9991 0.8710 – 0.8991 1.0060 0.8772 0.9791 – – 0.8994 0.9729 0.8738 0.9520 – –

0.8857 0.8694 0.9872 0.8498 0.9634 0.8414 – 0.8647 0.9677 0.8422 0.9394 0.8277 0.9277 0.8630 0.9444 0.8377 0.9149 0.8243 0.8982

1.4960 1.4800 1.5710 1.4670 1.5460 1.4620 – 1.4800 1.5530 1.4650 1.5340 1.4600 1.5235 1.4800 1.5310 1.4630 1.5140 1.4580 1.5047

2.48 1.80 5.31 1.11 4.63 0.74 – 1.71 4.74 0.98 4.07 0.68 3.65 1.71 3.87 0.85 3.35 – 2.84

MND (T50% = 745K) Feed – R-1 1 E-1 1 R-2 4 E-2 4 R-3 7 E-3 7 R-4 1 E-4 1 R-5 4 E-5 4 R-6 7 E-6 7 R-7 1 E-7 1 R-8 4 E-8 4 R-9 7 E-9 7

– 333 333 333 333 333 333 353 353 353 353 353 353 373 373 373 373 373 373

– 83.2 16.8 66.3 33.7 57.8 42.2 78.7 21.3 57.0 43.0 45.8 54.2 72.1 27.9 42.4 57.6 28.3 71.7

– 10.3 87.2 8.6 93.6 8.0 95.3 14.4 83.8 10.9 91.9 10.3 94.1 21.6 78.7 15.7 89.4 12.9 92.3

0.9341 0.9135 1.0494 0.8949 1.0235 0.8868 1.0092 0.9122 1.0247 0.8919 0.9987 0.9128 0.9956 – – – – – –

0.8947 0.8738 1.0112 0.8550 0.9850 0.8468 0.9706 0.8725 0.9863 0.8520 0.9600 0.8419 0.9463 0.8731 0.9568 0.8468 0.9336 0.8372 0.9205

1.4992 1.4843 1.5800 1.4723 1.5601 1.4666 1.5488 1.4838 1.5631 1.4698 1.5432 1.4682 1.5369 1.4842 1.5410 1.4722 1.5287 1.4663 1.5192

2.46 1.88 5.31 1.29 4.77 1.04 4.48 1.83 4.75 1.21 4.18 0.85 3.74 1.85 4.10 1.04 3.50 0.74 3.10

Fraction

Furfural/feed (v/v)

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

P = A · T50% + B,

(1)

where P denotes a pseudo-component property or a NRTL binary interaction parameter, and A and B are linearly adjustable parameters. Fig. 1 shows, as an example, the assumed linear dependence between pseudo-component SG (for saturates, aromatics and polars) and T50% of the lubricant oil. In such figure it is possible to check how the T50% range between the previously studies for HND and SPD is covered.

Table 2 Pseudo-component properties previously reported for SPD (Coto et al., 2006) and HND (Van Grieken et al., 2005)

3.1. Pseudo-component properties The parameters of Eq. (1) for the different properties (SG, D343 , RI 343 and %S) of each pseudo-component are shown in Table 4. According to such correlations, the pseudocomponents properties of any vacuum distillate lubricating oil with T50% within the range SPD–HND (640–801 K) can be easily calculated. The following mixing rule was assumed to relate the physical properties of any lubricating oil mixture to the properties and composition of pseudo-components:   XS XA XP Pi,calc = (2) P i,S + P i,A + P i,P , 100 100 100 2.0

1.6

SG

HND lubricating oil cuts (Coto et al., 2006; Van Grieken et al., 2005). Such models were based on the pseudo-component properties and the NRTL model. The pseudo-component properties for SPD and HND lubricating oil cuts previously reported are shown in Table 2. NRTL parameters calculated for such lubricating oil cuts are presented in Table 3. In this work, both pseudo-component and NRTL parameters for SPD and HND were linearly correlated with T50% as follows:

8031

1.2

Saturates

Aromatics

Polars

SPD T50% (K) SG D343 (g/ml) RI 343 %S (wt%)

640 0.8050 1.4110 0.7670 0

640 1.0212 1.5860 1.0000 4.6

640 1.9300 1.6000 1.3000 20.0

HND T50% (K) SG D343 (g/ml) RI 343 %S (wt%)

801 0.8361 0.7930 1.4311 0

801 0.9764 0.9900 1.5816 2.10

801 1.9228 1.2232 1.5830 23.3

0.8

640

680

720

760

800

T50% / K

Fig. 1. Relation between SG and T50% for the studied lubricant oils. Line: —– Saturates, ..... Aromatics, - - - - Polars; Symbols:  SPD (Coto et al., 2006) and HND (Van Grieken et al., 2005),  SPD,  LND, 䊉 MND, this work.

Table 3 NRTL binary interaction parameters previously reported for SPD (Coto et al., 2006) and HND (Van Grieken et al., 2005) Component i Component j SPD aij aj i bij bj i

ij

HND aij aj i bij bj i

ij

Furfural Saturate

Furfural Aromatic

Saturate Aromatic

Saturate Polar

Aromatic Polar

Polar Furfural

0.70 −3.85 1310 1421.75 0.23

−1.65 110.00 755 −644 0.10

11.13 −6.39 −4472.87 1900 0.30

67.00 9.47 −26000 −4000 0.13

9.50 −7.27 −3110 3030 0.30

6.62 −17.00 1315 −2300 0.20

0.77 −4.81 1361.55 1707.14 0.29

0.17 11.15 −592.67 4646.93 0.30

10.49 −7.7 −6070.78 1937.2 0.20

−125.49 −4.01 46708.69 −627.88 0.20

−33.84 −0.1 13210.45 −3012.05 0.20

−10.19 −2.92 2266.9 −1446.52 0.20

8032

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

Table 4 Correlation between pseudo-component properties and T50% a Saturates A × 10 SG D (g/ml) RI %S (w%) aP

4

1.9 1.6 1.3 –

Aromatics B

A × 10

0.6814 0.6637 1.3311 –

2.8 0.6 −0.3 −152

4

Polars B

A × 104

B

1.1991 1.0398 1.6035 14.29

−0.5 −4.8 −1.1 205

1.9586 1.6052 1.6676 6.88

= A · T50% + B.

where Pi,calc is the calculated value of property i; Pi,S , Pi,A and Pi,P the calculated values of the property i for saturate, aromatic and polar pseudo-component, respectively, and XS , XA and XP the values of composition in saturates, aromatics and polars. In this work Eq. (2) was used straightforward to calculate physical properties of any lubricating oil mixture from calculated pseudo-component properties and composition. In addition, such equation was used in a reversed way in order to calculate the composition values in saturates, aromatics and polars for any lubricating oil cut used as feed in the extraction operation. The calculation procedure to obtain the composition of the feed involves only three properties, D343 , RI 343 and %S. For a given unknown lubricating oil cut, the pseudo-component properties are obtained from Eq. (1) and values for Xs , XA and XP are those which minimize the following objective function:  F= |Pi,exp − Pi,calc |, (3) i

where Pi,exp is the experimental value for the considered property, i, and Pi,calc is the corresponding one calculated from Eq. (2). The sum is extended over the three above-mentioned properties (D343 , RI 343 and %S). Fig. 2 shows, as an example, the comparison between the experimental and predicted values of D343 for the distillates considered in this work. As it can be observed, no deviation was found, and therefore the calculated values of composition can be successfully considered. 3.2. NRTL model The NRTL equation is based on the local composition concept and considers only binary interactions. The NRTL expression for activity coefficient is given by Raal and Mühlbauer (1998), Prausnitz et al. (2000), Poling et al. (2001): c j =1 xj j i Gj i ln i = c k=1 xk Gki +

c   j =1

xj Gij c k=1 xk Gkj



c  m=1 xm mj Gmj ij −  , c k=1 xk Gkj (4)

Gij = exp(−ij ij ),

(5)

Calculated D343 / gml-1

Property (P )

0.90

0.88

0.86 0.86

0.88 Experimental D343 /

0.90 gml-1

Fig. 2. Experimental and calculated D343 for the lubricant oils used in this work. Symbols:  SPD,  LND, 䊉 MND.

Table 5 Correlation between ij and T50% a Interactionb

A × 104

B × 102

f-s f-a f-p s-a s-p a-p

4.3 13 −0.2 −6.2 4.6 −6.2

−4.9 −70.6 21.5 69.7 −16.8 69.7

a = A · T ij 50% + B. b f, Furfural; s, Saturate;

ij = aij +

bij , Text

a, Aromatic; p, Polar.

(6)

where xi is the molar fraction of component i; ij is a model parameter related with the tendency of species i and j to be randomly distributed, and ij is the model parameter which must be considered for the interaction between pairs of molecules i and j. ij is assumed to be temperature dependent (Text ) according to Eq. (6), for which two binary parameters, aij and bij , are defined (Demirel and Gecegörmez, 1991). As ii = 0, aij = aj i , bij  = bj i and ij = j i , five binary parameters should be considered to characterize each binary interaction. NRTL parameters for SPD and HND shown in Table 3 were used to obtain a T50% -dependent generalized model. Thus, ij parameters, previously calculated for SPD and HND were correlated with T50% by means of expression (1) and shown in Table 5. According to expression (6), temperature-dependent parameters ij and j i were estimated for SPD and HND at different temperatures, in this work values of 323, 343 and 363 K were selected for Text as usual temperatures for the extraction operation. Eq. (1) was used to correlate ij and j i at fixed Text

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

8033

Pseudo-components properties T50% of the lube oil used as feed

Single-stage extractions

NRTL parameters Composition of the lubricating oil used as feed

Simulation by AspenPlus®

Fig. 3. Scheme for the application of the generalized model.

Table 6 Correlation between ij and T50% a Interactionb

T = 323 K A × 10

f-s f-a f-p s-a s-p a-p s-f a-p p-f a-s p-s p-a a

3

1.5 −15 104 −35 202 44 −0.4 −512 −86 −7.4 −19 −72

Table 7 Pseudo-component properties for the selected lubricating oils T = 343 K

B

A × 10

3.8 10.0 −90.6 19.0 −142.7 −28.6 0.8 435.9 65.8 4.2 9.2 47.9

1.4 −13 103 −33 120 26 −0.8 −520 −87 −7.5 −23 −65

3

T = 363 K B

A × 10

3.6 8.9 −89.5 19.2 −85.9 −16.4 0.8 439.8 66.2 3.9 12.3 43.1

1.3 −12 102 −31 48 9.9 −1.1 −520 −88 −7.5 −26 −59

3

B 3.5 7.9 −88.6 18.8 −35.3 −5.4 0.7 443.2 66.6 3.6 15.1 38.7

= A · T50% + B. b f, Furfural; s, Saturate; a, Aromatic; p, Polar. ij

values with T50% . Obtained values are shown in Table 6. From the dependence of ij against 1/Text according to Eq. (6), values for aij and bij can be obtained. Such procedure was also applicable to j i . These relations allow calculate NRTL parameters for any lubricant oil using as experimental information only the T50% . The range of application is for lubricating oils with T50% values within the range SPD–HND (640–801 K). Fig. 3 summarizes the scheme of application of the generalized model. 4. Results and discussion In order to check the quality of the generalized model described before, several experiments were carried out with the lubricating oil cuts (within the range SPD–HND) presented in Table 1. Pseudo-components properties and NRTL parameters of such lubricating oil cuts were calculated from their T50% (Table 1) according to the coefficients listed in Tables 4, 5 and 6. Calculated properties of each pseudo-component for SPD, LND and MND lubricating oil are shown in Table 7. Calculated NRTL parameters for such cuts are shown in Table 8. Experi-

Saturates

Aromatics

Polars

SPD T50% (K) SG D343 (g/ml) RI 343 S% (wt%)

651 0.8071 0.7688 1.4124 0

651 1.0181 0.9993 1.5857 4.39

651 1.9295 1.2947 1.5989 20.23

LND T50% (K) SG D343 (g/ml) RI 343 S % (wt%)

717 0.8199 0.7794 1.4206 0

717 0.9997 0.9952 1.5839 3.39

717 1.9265 1.2633 1.5919 21.58

MND T50% (K) SG D343 (g/ml) RI 343 S% (wt%)

745 0.8253 0.7840 1.4291 0

745 0.9920 0.9935 1.5832 3.0

745 1.9253 1.2499 1.5890 22.1

mental conditions given in Table 1 were simulated by means of Aspen Plus䉸 using the generalized model and the results for all extraction experiments are shown in Table 9. The composition of each cut used as feed was estimated following the method described above from the pseudo-components properties and physical properties of the different lubricating oils (SPD, LND and MND). In order to determine the accuracy of the different predictions, absolute average deviation () was calculated as follows:   |Pexp − Pcalc | i = = , (7) N N where N represents the number of mixtures considered, Pexp is the experimental value of a property and Pcalc the calculated one. Table 10 lists the values of  for different properties related with the single-stage extractions for SPD, LND and MND. Experimental and predicted yields for all lubricating oil cuts are compared in Fig. 4. As it can be observed, no systematic

8034

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

Table 8 NRTL parameters calculated for the selected lubricating oils Component i Component j SPD aij aj i bij bj i

ij

LND aij aj i bij bj i

ij

MND aij aj i bij bj i

ij

Furfural Saturate

Furfural Aromatic

Saturate Aromatic

Saturate Polar

Aromatic Polar

Polar Furfural

0.70 −3.92 1313.60 1441.20 0.23

−1.52 103.24 661.84 −282.96 0.10

11.10 −6.48 −4584.83 1902.50 0.30

53.84 8.55 −21029.00 −3769.50 0.10

6.54 −6.77 −1995.90 2615.80 0.30

5.47 −16.05 1380.80 −2237.90 0.20

0.74 −4.31 1334.70 1558.20 0.26

−0.78 62.72 109.21 1885.70 0.20

10.83 −7.01 −5239.88 1917.8 0.25

−25.07 3.02 8776.9 −2387.2 0.16

−11.22 −3.84 4694.40 138.87 0.25

−1.42 −10.28 1771.0 −1887.40 0.20

0.75 −4.47 1343.70 1607.80 0.27

−0.46 45.50 −125.20 2805.70 0.23

10.72 −7.24 −5517.78 1924.30 0.23

−58.54 0.68 21422 −1800.8 0.17

−18.76 −2.59 7532.8 −911.95 0.23

−4.35 −7.83 1936.50 −1738.70 0.20

deviations were found in any case, obtaining the expected distribution of phases. Thus, at the lowest temperature and furfural/feed ratio 79.5%, 84.5% and 85.7% in raffinate was predicted for SPD, LND and MND, respectively, which is in good concordance with 74.1%, 80.0% and 83.2% experimentally determined for such cuts. When increasing the temperature or the solvent/feed ratio, the yield becomes lower as stated before. Thus, at the same temperature and highest solvent/feed ratio a raffinate yield of 44.0%, 54.1% and 58.1% was calculated for SPD, LND and MND, respectively, showing again a good agreement with the 43.8%, 51.5% and 57.8% experimentally obtained. Absolute average deviations of 2.6%, 3.0% and 1.2%, were obtained for the prediction of extraction yields for SPD, LND and MND, respectively. The comparison between experimental and predicted content of furfural for raffinates and extracts is shown in Fig. 5. The model exhibits good accuracy in all experimental conditions, even at the higher values of temperature or furfural/feed ratio. For instance, the predicted values for furfural content in raffinate for MND was 9.1% at the lowest temperature and furfural/feed = 7 and 19.2% at higher temperature and furfural/feed ratio = 1, which fit well with the experimental ones, 8.0% and 21.6%, respectively. Absolute average deviations of 0.6%, 1.5% and 1.1% were obtained for the prediction of furfural content in raffinate for SPD, LND and MND, respectively. Physical properties (SG, D, RI and S%) of each mixture (feed, raffinates and extracts) for SPD, LND and MND were calculated according to expression (2), using the pseudo-components properties shown in Table 7 and the compositions in saturates, aromatics and polars (XS , XA and XP ) obtained by simulation presented in Table 9. As an example, experimental and calcu-

lated values for SPD experiments are summarized in Table 11. The comparison between experimental and calculated values of such properties is shown in Figs. 6–8 for SPD, LND and MND extraction experiments, respectively. As it can be seen, a good agreement between predicted and experimental values was obtained in all cases. In all cases absolute average deviations were < 0.015 for SG, < 0.007 for D343 , < 0.005 for RI 343 and < 0.6 for %S. As it can be observed in Figs. 6–8 the prediction of the S% shows systematic deviations. This can be due to a limitation of the model since it is assumed that the S% is zero for saturates, which is true if only tiophenic sulfur (present in aromatic and polar species) is present. It works well for the lightest lube oil cut (SPD). However, for heavier lube oil cuts, other sulfur species present in the saturate compounds should be considered. Although the proportion of this kind of sulfur is not very high, it could affect the predictions obtained by using the proposed model and a new distribution of the S% for the pseudocomponents would be needed. In spite of these limitations, the obtained results reported by Coto et al. (2006) using the simplified distribution of the S% present similar accuracy than those obtained using a method proposed by Riazi et al. (1999). The experiments carried out at highest temperatures and furfural/feed ratio could not be simulated because the system is near the miscibility region. This is a limitation in the application of the model previously indicated (Van Grieken et al., 2005) for the system furfural + HND lubricating oils and also found for the system furfural + SPD lubricating oil (Coto et al., 2006). No accurate predictions are obtained in these conditions; however, this limitation is not a big model lack because in the practice these severe conditions are not very usual.

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

8035

Table 9 Simulation results for the single-stage extraction experiments Furfural/feed (w/w)

T (K)

Yield (wt%)

Furfural (wt%)

XS (wt%)

XA (wt%)

XP (wt%)

SPD Feed R-1 E-1 R-2 E-2 R-3 E-3 R-4 E-4 R-5 E-5 R-7 E-7 R-8 E-8

– 1 1 4 4 7 7 1 1 4 4 1 1 4 4

– 328 328 328 328 328 328 348 348 348 348 368 368 368 368

– 79.5 20.5 57.1 42.9 44.0 56.0 70.8 29.2 42.3 57.7 24.4 75.6 22.7 77.3

– 11.0 85.3 9.0 92.2 8.3 94.1 15.4 79.9 11.8 89.8 10.8 92.2 16.0 86.9

50.4 60.0 13.2 71.4 22.5 76.3 30.1 62.5 21.1 75.4 32.1 80.2 40.8 77.5 42.5

45.8 37.6 77.3 27.2 70.4 22.6 63.9 35.2 71.4 23.3 62.2 18.9 54.5 21.4 52.9

3.8 2.4 9.5 1.4 7.1 1.1 6.0 2.3 7.5 1.3 5.7 0.9 4.7 1.1 4.6

LND Feed R-1 E-1 R-2 E-2 R-3 E-3 R-4 E-4 R-5 E-5 R-7 E-7 R-8 E-8

– 1 1 4 4 7 7 1 1 4 4 1 1 4 4

– 333 333 333 333 333 333 353 353 353 353 373 373 373 373

– 84.5 15.5 65.6 34.4 54.1 45.9 77.7 22.3 52.5 47.5 70.3 29.7 35.7 64.3

– 10.7 88.1 9.7 93.5 9.4 95.0 14.6 83.4 12.7 91.2 20.5 78.1 16.7 88.4

47.6 54.8 8.4 63.9 16.7 68.0 23.7 57.1 14.6 67.7 25.5 58.0 23.1 69.9 35.2

48.5 41.9 84.4 33.4 77.2 29.5 70.8 39.5 79.7 29.7 69.3 38.5 72.1 27.5 60.2

3.9 3.3 7.2 2.7 6.1 2.5 5.5 3.4 5.7 2.6 5.2 3.5 4.8 2.6 4.6

MND Feed R-1 E-1 R-2 E-2 R-3 E-3 R-4 E-4 R-5 E-5 R-7 E-7

– 1 1 4 4 7 7 1 1 4 4 1 1

– 333 333 333 333 333 333 353 353 353 353 373 373

– 85.7 14.3 68.2 31.8 58.1 41.9 79.6 20.4 56.4 43.6 73.0 27.0

– 9.9 89 9.3 93.9 9.1 95.4 13.8 84.6 12.4 91.9 19.2 79.9

45.5 54.8 8.4 63.9 16.7 68.0 23.7 57.1 14.6 67.7 25.5 58.0 23.3

50.1 41.9 84.4 33.4 77.2 29.5 70.8 39.5 79.7 29.7 69.3 38.5 72.0

4.4 3.3 7.2 2.7 6.1 2.5 5.5 3.4 5.7 2.6 5.2 3.5 4.7

Fraction

Table 10 Absolute average deviations for predictions of single-stage extractions

SPD LND MND

Yield

Furf raff

Furf ext

SG × 102

D343 × 102

RI 343 × 102

S%

2.6 3.0 1.2

0.6 1.5 1.1

0.8 1.4 0.7

0.8 0.5 1.4

0.6 0.5 0.7

0.5 0.3 0.3

0.5 0.5 0.6

8036

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039 100 Calculated yield / w %

Calculated yield / w %

100 80 60 40 20 0

80 60 40 20 0

0

(a)

20 40 60 80 Experimental yield / w %

0

100

20 40 60 80 Experimental yield / w %

(b)

100

Calculated yield / w %

100 80 60 40 20 0 0

20

(c)

40

60

80

100

Experimental yield / w %

100 Calculated furfural % / w %

Calculated furfural % / w %

Fig. 4. Comparison between experimental and predicted values for extraction yields for the single-stage extraction experiments: (a) SPD; (b) LND; (c) MND. Symbols:  Raffinates;  Extracts.

80 60 40 20 0 0

40

60

80

80 60 40 20 0 0

100

Experimental furfural % / w % Calculated furfural % / w %

(a)

20

100

20

40

60

80

100

Experimental furfural % / w %

(b)

100 80 60 40 20 0 0

(c)

20

40

60

80

100

Experimental furfural % / w %

Fig. 5. Comparison between experimental and predicted values for the furfural content for the single-stage extraction experiments: (a) SPD; (b) LND; (c) MND. Symbols:  Raffinates; 䊉 Extracts.

According to all the obtained results, it is possible to correlate the pseudo-components properties and NRTL parameters with the T50% of the lubricating oil cut to predict extraction yields, furfural content and physical prop-

erties of the involved mixtures. Therefore, the generalized model can be used to describe the LLE in the systems furfural + lubricating oil cuts with T50% within the range SPD–HND.

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

8037

Table 11 Experimental and calculated values of the studied properties for SPD extraction experiments Fraction

Feed R-1 E-1 R-2 E-2 R-3 E-3 R-4 E-4 R-5 E-5 R-7 E-7 R-8 E-8

Furfural/feed (w/w)

T (K)

– 1 1 4 4 7 7 1 1 4 4 1 1 4 4

D343 (g/ml)

SG

RI 343

Experimental

Calculation

Experimental

Calculation

Experimental

Calculation

Experimental

Calculation

0.9123 0.8829 1.0104 0.8599 0.9839 0.8518 0.9676 0.8834 0.9839 0.8572 0.9566 – 0.9456 0.8545 0.9286

0.9144 0.8888 1.0277 0.8629 0.9922 0.8526 0.9688 0.8836 0.9972 0.8547 0.9629 0.8447 0.9390 0.8505 0.9345

0.8745 0.8447 0.9738 0.8214 0.9470 0.8132 0.9305 0.8452 0.947 0.8187 0.9195 – 0.9082 0.8159 0.891

0.8752 0.8512 0.9814 0.8255 0.9505 0.8151 0.9282 0.8456 0.9548 0.8170 0.9226 0.8070 0.8993 0.8128 0.8949

1.4889 1.4694 1.5558 1.4550 1.5356 1.4496 1.5250 1.4693 1.5363 1.4531 1.5185 – 1.5118 1.4521 1.5002

1.4871 1.4712 1.5576 1.4532 1.5384 1.4458 1.5236 1.4671 1.5411 1.4471 1.5197 1.4400 1.5038 1.4440 1.5007

2.76 1.75 5.58 0.88 4.98 0.59 4.49 1.75 4.97 0.76 4.25 – 3.90 0.76 3.34

2.78 2.13 5.27 1.48 4.49 1.21 3.99 2.01 4.61 1.27 3.87 1.01 3.34 1.17 3.24

1.04 Calculated D343 / g ml-1

1.00

Calculated SG

1.00 0.96 0.92 0.88 0.84 0.84

0.88

0.92

0.96

1.00

1.04

0.96 0.92 0.88 0.84 0.80 0.80

Experimental SG

0.84

0.88

0.92

0.96

1.00

Experimental D343 / g ml-1 6

1.58 Calculated S % / w %

1.56 Calculated RI343

%S (wt%)

1.54 1.52 1.50 1.48 1.46 1.44 1.44 1.46 1.48 1.50 1.52 1.54 1.56 1.58 Experimental RI343

5 4 3 2 1 0 0

1

2

3

4

5

6

Experimental S % / w %

Fig. 6. Comparison between experimental and predicted properties for SPD mixtures (feed, raffinates and extracts).

5. Conclusions A thermodynamic model, previously developed for the description of the LLE established in the extraction operation of lubricating oils with furfural, has been extended to other feeds within the range SPD–HND yielding a generalized model version. Only three pseudo-components (saturates, aromatics and polars) are considered and the NRTL model is used to determine

the activity coefficients. In order to reach a predictive model, a procedure has been developed to determine both the pseudocomponent properties and the NRTL parameters. The T50% value was chosen as representative of the lubricating oil mixture and a linear dependence was established between pseudocomponents properties and NRTL parameters and T50% . The feed composition was estimated from their physical properties and that estimated for the pseudo-components. Involved properties were D343 , RI 343 and %S.

8038

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039 1.00 Calculated D343 / g ml-1

Calculated SG

1.04 1.00 0.96 0.92 0.88

0.96 0.92 0.88 0.84 0.80 0.80

0.84 0.84 0.88 0.92 0.96 1.00 1.04 Experimental SG 1.58

0.88

0.92

0.96

1.00

6 Calculated S % / w %

1.56 Calculated RI343

0.84

Experimental D343 / g ml-1

1.54 1.52 1.50 1.48 1.46 1.44 1.44 1.46 1.48 1.50 1.52 1.54 1.56 1.58 Experimental RI343

5 4 3 2 1 0 0

1

2

3

4

5

6

Experimental S % / w %

Fig. 7. Comparison between experimental and predicted properties for LND mixtures (feed, raffinates and extracts).

1.04 Calculated D343 / gml-1

1.04

Calculated SG

1.00 0.96 0.92 0.88 0.84 0.84

0.88

0.92

0.96

1.00

1.04

1.00 0.96 0.92 0.88 0.84 0.84

6

1.58

5

Calculated S % / w %

Calculated RI343

1.60

1.54 1.52 1.50 1.48 1.46 1.46 1.48 1.50 1.52 1.54 1.56 1.58 1.60 Experimental RI343

0.92

0.96

1.00

Experimental D343 / g

Experimental SG

1.56

0.88

1.04

ml-1

4 3 2 1 0 0

1

2

3

4

5

6

Experimental S % / w %

Fig. 8. Comparison between experimental and predicted properties for MND mixtures (feed, raffinates and extracts).

The generalized model was applied to a single-stage extraction experiments carried out with vacuum distillates SPD, MND and LND, all of them within the range SPD–HND. Accurate predictions were obtained for yields and furfural content in the

extraction experiments as well as for the physical properties (SG, D343 , RI 343 and %S) of the involved mixtures (raffinates and extracts). Absolute average deviations were always lower than 3.0% for the yields and lower than 1.5% for the furfural

B. Coto et al. / Chemical Engineering Science 61 (2006) 8028 – 8039

content in raffinates and extracts. Likewise, absolute average deviations for the studied properties were lower than 0.014 for SG, around 0.006 for D343 , lower than 0.005 for RI 343 and around 0.5 for the %S. S% predictions show systematic deviations revealing that it is necessary to obtain a new distribution of the S% for the pseudo-components. No systematic deviations were obtained for the predictions of the other properties in the application of the model to the different feeds, thus concluding that the differences between these feeds can be well established through the different physical properties involved and the T50% value. Notation a A b B Comp. D343 E f F HND LND p P P R RI 343 s SG SPD S% T T50% v/v x X

NRTL interaction parameter parameter of linear correlation NRTL interaction parameter parameter of linear correlation compound liquid density at 343 K, g/ml extract furfural objective function heavy neutral distillate light neutral distillate polar studied property such as D, SG, RI or S% average property of pseudo-component raffinate refractive index at 343 K saturate specific gravity spindle distillate sulfur content, wt% temperature of extraction, K average temperature of the feed lubricating oil, K volume/volume mole fraction composition of each mixture, wt%

Greek letters  

NRTL interaction parameter NRTL interaction parameter given by Eq. (4)

Subscripts A i, j P S

aromatics component i, j polars saturates

Acknowledgments The authors thank REPSOL-YPF for providing the lubricant oil samples used in this work and for the financial support

8039

through the project “Desarrollo de modelos de simulación de procesos de refino”. References Abrams, D., Prausnitz, J.M., 1975. Statistical thermodynamics of liquid mixtures: a new expression for the excess Gibbs energy of partly or completely miscible systems. A.I.Ch.E. Journal 21, 116–128. ASTM Annual Book of Standards, 2003. American Society for Testing and Materials, vol. 5. West Conshohocken, Pennsylvania. Briesen, H., Marquardt, W., 2004. New approach to refinery process simulation with adaptive composition representation. A.I.Ch.E. Journal 50, 633–645. Coto, B., Van Grieken, R., Peña, J.L., Espada, J.J., 2006. A model to predict physical properties for light lubricating oils and its application to the extraction process by furfural. Chemical Engineering Science 61, 4381–4392. De Lucas, A., Rodríguez, L., Sánchez, P., Carnicer, A., 1993. Extraction of aromatic compounds from heavy neutral distillate lubricating oils by using furfural. Separation Science and Technology 28, 2465–2477. Demirel, Y., Gecegörmez, H., 1991. Simultaneous representation of excess enthalpy and vapor–liquid equilibrium data by the NRTL and UNIQUAC models. Fluid Phase Equilibria 65, 111–133. Letcher, T.M., Zondi, S., Naicker, K., 2003. Liquid–liquid equilibria for mixtures of (Furfural + an aromatic hydrocarbon + an alkane) at T = 298.15 K. Journal of Chemical and Engineering Data 48, 23–28. Mcketta, J.J., 1989. Encyclopedia of Chemical Processing and Design. Marcel Dekker, New York. Morawski, P., Letcher, T.M., Naicker, P.K., Domanska, U., 2003. Liquid–liquid equilibria for mixtures of (furfural+a chlorinated aromatic compound +an alkane) at T = 298.15 K. Journal of Chemical and Engineering Data 48, 822–826. Nelson, W.L., 1978. Petroleum Refining Engineering. fourth ed. McGrawHill, New York. Poling, B.E., Prausnitz, J.M., O‘Connell, J.P., 2001. The Properties of Gases and Liquids. McGraw-Hill, New York. Prausnitz, J.M., Lichtenthaler, R.N., De Azevedo, E.G., 2000. Molecular Thermodynamics of Fluid-Phase Equilibria. Prentice-Hall, New Jersey. Raal, J.D., Mühlbauer, A.L., 1998. Phase Equilibria. Measurement and Computation. Taylor and Francis, Washington. Rahman, M., Mikitenko, P., Asselineau, L., 1984. Solvent extraction of aromatics from middle distillates. Chemical Engineering Science 39, 1543–1558. Renon, H., Prausnitz, J.M., 1968. Local compositions in thermodynamic excess functions for liquid mixtures. A.I.Ch.E. Journal 14, 135–144. Riazi, M.R., Daubert, T.E., 1986. Prediction of molecular-type analysis of petroleum fractions and coal liquids. Industrial and Engineering Chemistry Process Design and Development 25, 1009–1015. Riazi, M.R., Nasimi, N., Roomi, Y.A., 1999. Estimation of sulfur content of petroleum Products and crude oils. Industrial and Engineering Chemistry Research 38, 4507–4512. Sequeira Jr, A., 1994. Lubricant Base Oil and Wax Processing. Marcel Dekker, New York. pp. 81–82. Singh, H., Kishore, K., 1978. Solvent refining of medium viscosity distillate and changes in group chemical composition. Journal of Applied of Chemistry and Biotechnology 28, 617–625. Van Grieken, R., Coto, B., Romero, E., Espada, J.J., 2005. Liquid–liquid equilibrium in the system furfural + heavy neutral distillate. Industrial and Engineering Chemistry Research 44 (21), 8106–8112.