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DYNA

versão impressa ISSN 0012-7353

Dyna rev.fac.nac.minas vol.82 no.191 Medellín maio/jun. 2015

http://dx.doi.org/10.15446/dyna.v82n191.42308 

DOI: http://dx.doi.org/10.15446/dyna.v82n191.42308

Modeling of CO2 vapor-liquid equilibrium in Colombian heavy oil using SARA analysis

Modelado del equilibrio líquido-vapor CO2-crudo pesado colombiano con análisis SARA

 

Oscar Ramirez a, Carolina Betancur b, Bibian Hoyos c & Carlos Naranjo d

 

a Facultad de Minas, Universidad Nacional de Colombia, Medellín, Colombia. ojramirezo@unal.edu.co
b Facultad de Minas, Universidad Nacional de Colombia, Medellín, Colombia. cbetancurg@unal.edu.co
c Facultad de Minas, Universidad Nacional de Colombia, Medellín, Colombia. bahoyos@unal.edu.co
d Instituto Colombiano del Petróleo, Ecopetrol S.A., Bogotá, Colombia. carlosed.naranjo@ecopetrol.com.co

 

Received: February 26th, 2014. Received in revised form: October 30th, 2014. Accepted: November 15th, 2015

 

This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License.


Abstract
The solubility of CO2 in Colombian heavy oil was calculated using the Peng-Robinson cubic equation of state and the Lee-Kesler correlations. The crude was represented as a mixture of pseudo-components and for each one of them, the thermodynamic and critical properties were estimated. The results obtained in representing the oil with four, five and six pseudo-components show that all these representations produce similar results and therefore the use of four pseudo-components is sufficient and has a lower computational cost. Excellent results were obtained by comparing the experimental and calculated data. For this system, it is enough to have a complete characterization of the SARA analysis and to use four pseudo-components to adequately model the vapor-liquid equilibrium of CO2 -heavy oil.

Keywords: Equation of state; pseudo-component; SARA analysis; crude; solvent; phase equilibrium.

Resumen
La solubilidad del CO2 en un crudo pesado colombiano fue calculada usando la ecuación cúbica de estado de Peng-Robinson y la correlación de Lee-Kesler. El crudo fue representado como una mezcla de pseudo-componentes y para cada uno de ellos se calcularon las propiedades termodinámicas y críticas. Los resultados obtenidos en la representación del crudo con cuatro, cinco y seis pseudo-componentes muestran que todas las representaciones producen resultados similares y por lo tanto el uso de cuatro pseudo-componentes es suficiente y tiene un costo computacional más bajo. Fueron obtenidos excelentes resultados al comparar los datos experimentales y calculados. Para este sistema es suficiente tener una completa caracterización del análisis SARA y usar cuatro pseudo-componentes para modelar adecuadamente el equilibrio líquido-vapor de CO2-crudo pesado.

Palabras clave: Ecuación de estado; pseudo-componente; análisis SARA; crudo; solvente; equilibrio de fases.


 

1. Introduction

Oil is a complex mixture of hydrocarbons produced from sedimentary rocks in gas form (natural gas), liquid (crude oil), semisolid (bitumen) or solids (wax or asphaltite) [1].

Most of the world's oil resources correspond to viscous and heavy hydrocarbons, which are difficult and expensive to produce and refine. Heavy oil, extra heavy oil and bitumen make up 70% of the world's total oil resources oscillating between 9 and13 trillion barrels [2].

A significant number of laboratory studies have been undertaken to identify technologies that can be applied as a solution to the phenomena that negatively affect the performance of implemented secondary recovery processes. These methods focus mainly on increasing oil mobility and thus increase the production thereof. The goal is to reduce its viscosity so that oil can flow easily. Enhanced Oil Recovery (EOR) can be achieved through technologies such as gas injection, chemical injection, microbial injection, or thermal recovery [3].

The implementation of EOR methods plays a key role as a technology to increase the recovery factor of Colombian fields, and to refurbish them in the implementation of other technologies designed to increase well productivity [4].

The main advantage of gas injection is its microscopic sweep. The gases used to EOR are mostly methane, butane, propane, nitrogen and carbon dioxide. Many of the aforementioned gases have the advantage of being produced in-situ, i.e. large volumes are available in the wellbore for injection. The choice of a particular gas is strongly linked to its availability and to the increased recovery generated. Thus, CO2 appears as one of the most promising gases for use in EOR.

It is therefore important to have a thermodynamic model to adequately characterize the phase behavior of CO2 - heavy oil mixtures. Such models can provide judgment elements for decision-making regarding production, transportation, refining and upgrading oil.

The experimental data reported in the literature to characterize the phase equilibrium for CO2 - heavy oil systems are generally few and so the difficulties in establishing appropriate thermodynamic models are high. Therefore, tools allowing phase equilibrium calculations of such systems with little experimental data are required.

The aim of this work is to develop a model for the calculation of vapor-liquid equilibrium for CO2 - Colombian heavy oil (called here UnalMed), using the representation of pseudo-components and to estimate the critical and thermodynamic properties of those components. Additionally, we seek here to establish the right number of components to be used for a good representation of the system, with little experimental information and at low computational cost. This information may be useful for developing appropriate thermodynamic models for the Colombian oil industry. To our knowledge, data on thermodynamic properties of pseudo-components to represent Colombian heavy oils have not been previously published.

 

2. Model

Based on the nature of the mixture of oil, there are several ways to express its composition. Some of the most important types of composition [1,5,6] are PONA analysis (paraffins, olefins, aromatics and Naphthenes), PNA (paraffins, Naphthenes and Aromatics), PIONA (paraffins, Isoparaffins, Olefins, Naphthenes and Aromatics), elemental (C, H, S, N, O) and SARA analysis (Saturates, Aromatics, Resins and Asphaltenes) [7].

PNA and PINA analyses are useful for petroleum products in a range of low boiling temperatures, such as distillates of atmospheric distillation units for crude. However, the SARA analysis is useful for heavy oil fractions, residues and fossil fuels (i.e., coal liquids) that have a high content of aromatics, resins and asphaltenes.

The above analyses are ways to represent oil as a mixture of pseudo components (several components represented in a single fraction), given the complexity of the composition of this. With SARA analysis, for example, oil can be represented in four pseudo components, which are the saturates, aromatics, resins and asphaltenes, and each of them has its properties such as the boiling point, specific gravity, density, molecular weight, among others. In addition, each pseudo component can be modeled as a pure substance.

The critical properties, molecular weight and acentric factor of each pseudo component can be calculated by correlations reported in the literature for heavy oil fractions.

In this work, the critical temperature, critical pressure and acentric factor of each pseudo component were calculated using the Lee-Kesler correlations [8], as shown in (eq.1-6); the molecular weight was calculated with the Daubert-Riazi correlation (eq. 7) and the critical volume with the Hall-Yarborough correlation (eq. 8). These correlations were selected by considering the good results that have been obtained with respect to experimental data along its applications [9,10]. The input parameters of these correlations are the boiling point (Tb) and the specific gravity (SG).

Kesler and Lee [11] proposed the following correlation for

Where y are in K and in bar and is the reduced boiling point defined as,

is the Watson characterization factor [1], given by

Where is in Kelvin and the molecular weight, is in g/mol.

In 1976, Peng and Robinson proposed a modification to the Soave-Redlich-Kwong equation of state (EOS) that has been well received internationally [26]. This equation of state is well accepted in technical publications, research and simulators to predict the behavior of natural hydrocarbon systems. PVT variables are related to predict the thermodynamic behavior of a system [12-14].

Where is the system pressure, is the system temperature, is a parameter of attraction, is a parameter of repulsion, is the molar volume and R is the ideal gas constant.

In terms of the compressibility factor,

Where

The constants and b are related to the critical pressure, critical temperature and acentric factor by:

Where,

is the interaction coefficient between components i and j. These parameters have no theoretical basis but are empirical, and their role is to help overcome the deficiencies of the theorem of corresponding states [15].

The fugacity coefficient can be calculated from EOS (eq. 9) [13],

In this manner, the expression for the fugacity coefficient of a pure component is:

The functional form of was determined by using the values of vapor pressure in the literature and the Newton method to find the values of a to be used in (eq. 10, 25) in a way that the equilibrium condition

is satisfied along the curve of vapor pressure [13]. Where y are the fugacity in the liquid and vapor phase, respectively.

The fugacity coefficient of a k component in a mixture can be calculated by:

Calculating fugacity coefficients for each component in both, liquid and gas phase with (eq. 27), the vapor-liquid distribution ratio can be calculated by (eq. 28):

The relationships described by (eq. 28) (one for each pseudo component) provide the main equations for VLE calculations using EOS.

For the development of this work, the heavy oil (UnalMed) was modeled with three different fractions groups: four, five and six pseudo components and CO2 solubility with UnalMed oil was calculated, in order to determine the amount of pseudo components that should be used to obtain an acceptable thermodynamic model.

 

3. Results

To model the CO2 - UnalMed oil system, the crude was initially characterized with four pseudo components, using the SARA analysis. The initial parameters for the calculation of the solubility of CO2 in oil at different conditions, such as boiling temperature (Tb) and specific gravity (SG) were assumed following some tips outlined in the work of Kariznovi et al., [9]:

  • Boiling temperature of the distillable fraction (saturates and aromatics) is less than 600 °C.
  • Boiling temperature of the non-distillable fraction (resins) is greater than 600 °C.
  • Boiling temperature of the asphaltenes is greater than the boiling temperature of the non-distillable fraction.

Table 1 shows the final parameters for each input of pseudo components that compose the UnalMed crude. These parameters were calculated iteratively within the developed algorithm.

UnalMed crude characterization shown in Table 1 is described by the following order: the first pseudo component corresponds to saturate fraction, aromatics is represented by PSC 2, the third and fourth pseudo components correspond to resins and asphaltenes, respectively. UnalMed oil composition and CO2 solubility curve derived from experimental measurements performed by the Colombian Petroleum Institute (ICP).

Table 2 shows the properties of the four pseudo components calculated using correlations presented in Section 2. The binary interaction coefficients between CO2 and UnalMed crude were tuned to give a closer approximation to the experimental data.

Fig. 1 shows the results obtained by applying four pseudo components to the model. This figure shows the solubility of CO2 in the crude at 80°F and different pressures, the x-axis corresponds to the saturation pressure and the y-axis corresponds to the molar composition of the solvent in terms of mole fraction of CO2. It can be seen that having a relatively low operating temperature, and increasing the saturation pressure, CO2 is more highly compressed, increasing its solubility in UnalMed crude.

For oil represented by five pseudo components, the same methodology as for the crude representation with four pseudo components was used. The additional pseudo component results from separation of the non-distillable oil fraction, namely resins, as these resins were separated into the asphaltene-free and resins containing asphaltenes. With this as mentioned, the order of pseudo components is as follows: the first two pseudo components represent UnalMed crude distillable fraction, third and fourth represent the non-distillable fraction of resins (resins 1 and 2), and the fifth pseudo component represents asphaltenes.

Table 3 shows the final input parameters of UnalMed crude represented by five pseudo components.

Table 4 presents the properties of the five pseudo components calculated by the model, as well as the binary interaction coefficient between CO2 and UnalMed crude, which were tuned to provide a closer approximation to the experimental data.

Fig. 2 shows the results obtained by applying the model of VLE of CO2 - UnalMed crude represented with five pseudo components. This figure shows the solubility of CO2 in the oil at 80 ° F and different pressures.

The results are practically the same to those shown in Fig. 1, which is an indication that modelling the CO2 - UnalMed crude VLE with four pseudo components is appropriate.

Now, for oil represented by six pseudo components, the same methodology as for the four and five pseudo components was used. In this case, the additional pseudo component represents a portion of the non-distillable fraction with a portion of the asphaltenes fraction, i.e. the resins and asphaltenes. This pseudo component is called transition pseudo component. The pseudo components order is as follows: The first two represent the distillable fraction, the third and fourth pseudo components represent the non-distillable fraction (resins 1 and 2), the fifth represents the transition between the resins and asphaltenes and the sixth pseudo component corresponds to asphaltenes.

Table 5 shows the final input parameters of UnalMed crude represented by six pseudo components, and Table 6 shows the properties calculated for the six pseudo components as well as the binary interaction coefficients between CO2 and UnalMed crude.

Fig. 3 shows again the same behavior as shown in Fig. 1, 2. In general, results show a high level of agreement with the UnalMed crude experimental data, which indicates that it is possible to model the CO2 - UnalMed crude VLE through four pseudo components, which can be commonly obtained with SARA analysis.

 

4. Conclusions

For the calculation of CO2 - UnalMed crude VLE, the crude representation was tested with different amounts of pseudo components to compare the model results with experimental data.

All crude representations showed very similar results and it is important to note that it is sufficient to have a complete characterization of the SARA analysis and use these four pseudo components to model the VLE.

Having specific data, such as boiling point and specific gravity of each pseudo component, is useful for further reducing the uncertainty of the results.

Binary interaction coefficients, required in the parameters of the cubic EOS are a key element in the study of the solubility of CO2 in the oil, because the saturation pressure proved to be highly sensitive to the values of binary interaction parameters, thus had to be tuned to obtain a better approximation of the experimental data.

We observed that with a relatively low operating temperature, the solubility of CO2 in the oil is favored when the system is at high pressures, which is an important factor in the recovery of oil, because this could decrease the viscosity thereof without needing too much energy to heat the contents of the fields.

Crude representation using four pseudo components and the model used were suitable for the analysis of phase behavior in these kinds of systems.

 

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O.J. Ramirez, completed a BSc. degree in Chemical Engineering in 2013 from the Universidad Nacional de Colombia and worked in Process Safety in Ecopetrol S.A during the traineeship.

C. Betancur, completed a BSc. degree in Chemical Engineering in 2013 from the Universidad Nacional de Colombia and worked in Process Technology in Ecopetrol S.A during the traineeship.

B.A. Hoyos, completed BSc. in 1994 and MSc. in 2003 degrees both in Chemical Engineering and a PhD degree in Energy Systems in 2010, all of them from the Universidad Nacional de Colombia campus Medellín, Colombia. Currently he is a full professor in the Departamento de Procesos y Energía, Facultad de Minas, Universidad Nacional de Colombia, campus Medellín, Colombia. His research interests include molecular simulation, modeling asphaltene aggregation and viscosity, modelling wettability alteration by surfactants and specific adsorption.

C. E. Naranjo, completed a BSc. degree in Petroleum Engineering in 1993 from the Universidad Industrial de Santander, Colombia and a MSc. degree in Hydrocarbon Engineering in 2010. He has over fourteen years of experience as a reservoir engineer in the area of secondary and Enhanced Oil Recovery with emphasis on water injection and thermal recovery processes. Two (2) applications for invention patents in Republic of Colombia, coauthor of six (6) Declaration technology products in Ecopetrol S.A., co-directed research projects through Labor and Jobs Master's Degree, and several academic and national and international technical recognitions and achievements.