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COMPONENT PARTITIONING IN COg-HYDROCARBON SYSTEMS:
THE EFFECTS OF CHEMICAL TYPE
A THESIS
SUBMITTED TO THE FACULTY OF THE GRADUATE SCHOOL
OF THE NEW MEXICO INSTITUTE OF MINING AND TECHNOLOGY
by
Matthew Silva
IN PARTIAL FULFILLMENT OF THE REQUIREMENTS
FOR THE DEGREE OF
MASTER OF SCIENCE
IN PETROLEUM ENGINEERING
May 1984
PRRCUBRARYCOPy
(m)
ACKNOWLEDGEMENTS
I wish to thank Lynn Orr for sharing his insight into the subject
of CO2 flooding and providing encouragement throughout this effort.
I also wish to thank the members of my committee, Joe Taber, John
Heller and Charles Nathan, for their support.
In addition, Joe Franklin, Chris Lien, Kent Wainwright, and Mickey
Pelletier deserve recognition for their special contributions to this
project.
I also wish to thank Dileep Dandge with x^hom I had a number of
discussions about the extraction of organic compounds by carbon dioxide.
A note of thanks also goes to Kathy Grattan for typing this thesis,
to Paula Bradley for her very helpful advice in the area of technical
writing, and to Jessica McKinnis for drafting the figures.
The support that made this research effort possible was provided by
the U.S. Department of Energy, the New Mexico Energy Research and
Development Institute and a consortium of companies and foundations
including the Abu Dhabi Reservoir Research Foundation, American
Cyanamid, the Amoco Foundation, ARCO Oil and Gas, Conoco, Marathon,
Mobil, Shell Development, Sohio, Sun Exploration and Production, and
Tenneco. That support is gratefully acknowledged. In addition, support
was provided by the Petroleum Recovery Research Center.
Crude oil samples were provided by Mobil Research and Development
Corporation, Conoco, Inc., and Pennzoil Exploration and Production
Company.
i
TABLE OF CONTENTS
PAGE
NO.
LIST OF TABLES ii
LIST OF FIGURES iii
ABSTRACT 1
1. INTRODUCTION 2
Role of Phase Behavior in the Development ofMiscibility 4
Slim Tubes and "Minimum Miscibility Pressure" 8
Effects of Oil Composition on MMP 13
Binary C02-Hydrocarbon Systems 16
Multicomponent Systems 26
2. PHASE BEHAVIOR AND FLUID PROPERTY MEASUREMENTS 32
Experimental Procedure 32
C02-Crude Oil Systems 35
C02-Synthetic Oil Systems 46
3. INTERPRETATION OF EXPERIMENTAL RESULTS 58
4. IMPROVEMENT OF CORRELATIONS FOR MINIMUM MISCIBILITY
PRESSURES • 66
Correlating Parameter 66
Preliminary Tests of Correlation Accuracy 69
5. SUMMARY AND CONCLUSIONS 78
REFERENCES 81
ii
LIST OF TABLES
PAGE
NO.
Table 1.1 Extraction of Hydrocarbons by CO2 in BinarySystems 23
Table 1.2 Extraction of Hydrocarbons by CO2 in BinarySystems 25
Table 1.3 Synthetic Oil Compositions for Phase BehaviorStudies Conducted by Monger 28
Table 1.4 Physical Properties of Hydrocarbons Used inSynthetic Oils 30
Table 2.1 Compositions of Gas and Liquid Samples from CMCExperiment for Maljamar Crude Oil at 1400 psiaand 90°F 36
Table 2.2 Comparison of Oil Properties and Run Conditionsfor Continuous Multiple Contact Experiments forMaljamar and Rock Creek Crude Oils 40
Table 2.3 Composition of Mixture of Aromatic HydrocarbonsAdded to Rock Creek Crude Oil 40
Table 2.4 Composition of Rock Creek Crude Oil Mixed withSelected Aromatic Hydrocarbons 40
Table 2.5 Compositions and Molecular Weights of FourSynthetic Oils 49
Table 3.1 Hydrocarbon Components for SyntheticBlend 60
Table 4.1 Experimental Data with Weighted C2+ FractionParameter 70
Table 4.2 Composition of Recombined ReservoirOils 73
Table 4.3 Comparison of Predicted and MeasuredMMPs 76
iii
LIST OF FIGURES
PAGE
NO.
Fig. 1.1 Typical pseudo-ternary representation of a crudeoil with carbon dioxide 6
Fig. 1.2 Pseudo-ternary representation of compositionaleffects in the displacement of oil by CO2 7
Fig. 1.3 Effect of pressure on the size of the region oftie line extensions 10
Fig. 1.4 Schematic of a slim tube experiment 12
Fig. 1.5 Qualitative representation of phase behaviorfor binary systems containing CO2 and lightnormal alkanes 18
Fig. 1.6 Qualitative representation of phase behaviorfor binary systems containing CO2 and heavyalkanes 18
Fig. 1.7 PT projection of the critical loci of CO2-tetralin and C02-decalin binary mixtures 21
Fig. 1.8 Critical loci of C02-hydrocarbon binary mixtures ... 22
Fig. 2.1 Continuous multiple contact apparatus 34
Fig. 2.2 Pseudo-ternary representation of phase compositionsof mixtures of CO2 with Maljamar separator oilat 1400 psia and 90°F 37
Fig. 2.3 Pseudo-ternary representation of phase compositionsof mixtures of CO2 with Maljamar separator oilat 1200 psia and 90°F 38
Fig. 2.4 Pseudo-ternary representation of phase compositionsof mixtures of CO2 with Rock Creek separator oilat 1300 psia and 75°F 39
Fig. 2.5 Comparison of partition coefficients for RockCreek and Maljamar crude oils mixed with CO2 41
Fig. 2.6 Pseudo-ternary representation of phase compositionsof mixtures of CO2 with Rock Creek oil containingadded aromatic components at 1300 psia and 75®F .... 43
IV
PAGE
NO.
Fig. 2.7 Comparison of partition coefficients for Rock Creekoil and Rock Creek oil with aromatics added 44
Fig. 2.8 Comparison of extraction of hydrocarbons by denseCO2 for Rock Creek crude oil and Rock Creek oilwith added aromatic components 47
Fig. 2.9 Measured densities for C02-synthetic oil mixtures ... 50
Fig. 2.10 Pseudo-ternary representations of phase compositionsof CO2-hydrocarbon mixtures 51
Fig. 2.11 Partition coefficients in C02-synthetic oilmixtures 53
Fig. 2.12 Effects of changes in tie line slope, solubility ofcomponent, and extraction of component 3 onpartition coefficients 55
Fig. 4.1 Hydrocarbon equilibrium values (with CO2 removed fromthe calculation) for C02-Maljamar crude oil mixturesat 1200 psia and 90°F 68
Fig. 4.2 CO2 density required for miscible type displacementvs. C5-C3Q content 71
Fig. 4.3 CO2 density required for miscible type displacementvs. Z Wi kj 72
1
ABSTRACT
This thesis reviews the relationship between phase behavior and the
development of a miscible type displacement to determine the effects of
hydrocarbon molecular type on phase behavior for C02-hydrocarbon
systems. The continuous multiple contact experiment is used to generate
detailed phase composition and density information for C02-crude oil
systems and four distinctly different C02-synthetic oil systems
(n-alkanes, iso-alkanes, naphthenes, and aromatics). The experimental
results are compared with published data for clues to relate phase
behavior to displacement results observed for systems containing crude
oils. An experiment to resolve unanswered questions about the role of
attached alkyl groups commonly found in reservoir oils is outlined as
well as an improved correlation for predicting displacement pressures
required to achieve miscibility.
1. INTRODUCTION
To date, research into the mechanisms by Xi/hich carbon dioxide
recovers crude oil from a reservoir has established a number of key
relationships. For instance, the efficient recovery of oil relies
directly on the efficient extraction of hydrocarbon components into a
C02-rich phase. Furthermore, the level of hydrocarbon extraction has
been directly related to the density of carbon dioxide. At least one
study, that of Holm and Josendal (1982), produced very strong evidence
that, in addition to CO2 density, the size and chemical type of the
hydrocarbons found in crude oils also influences to some extent the
efficiency of hydrocarbon extraction. This thesis focuses on the
relationship between hydrocarbon molecular type and phase behavior as
part of a larger research effort aimed at developing an improved
correlation for predicting the displacement pressures required to
recover oil efficiently from reservoirs targeted for CO2 floods.
This chapter opens with the development of a few key concepts
needed to understand how CO2 miscibly recovers crude oil. In
particular, the chapter discusses the role of phase behavior in the
development of miscibility and the use of slim tube displacements to
determine what is commonly referred to as the minimum miscibility
pressure. This discussion is followed by a review of some experimental
investigations which used slim tube displacements to delineate the role
of oil composition in the displacement process. The research of Holm
and Josendal (1982) dominates much of this discussion. In addition to
drawing a clear picture of the effects of hydrocarbon molecular size,
their study produced some surprising results which indicated that
aromatic oils require slightly lower pressures than paraffinic oils to
generate raiscibility with C02- A review of the limited amount of
component partitioning data for binary and mul t ic ompo nent
C02-hydrocarbon systems fails to explain their results and raises a few
additional questions about the behavior of these systems. For instance,
how do hydrocarbon components with widely different molecular structures
(paraffins, naphthenes, and aromatics) partition in the presence of CO2?
Do cyclic molecules act as more efficient co-solvents than paraffinic
molecules as suggested by Holm and Josendal? And, does the attachment
of alkyl groups to hydrocarbon molecules influence their extraction in
multicomponent systems? Finally, does an aromatic crude oil exhibit
phase behavior significantly different from that of a paraffinic crude
oil when contacted by carbon dioxide?
Chapter two systematically addresses each of these questions with a
suite of phase behavior experiments designed to provide detailed
component partitioning information. The novel technique used by the
continuous multiple contact apparatus to generate these data is briefly
reviewed. Phase compositions for three crude oils containing differing
amounts of aromatics are compared. Also compared are measurements of
partitioning in four synthetic oil systems of similar overall molecular
weight but composed of n-alkanes, branched allcanes, naphthenes and
aromatics.
Chapter three examines the almost identical phase behaviors of an
aromatic oil and a paraffinic oil. An indication of the effects of
attached alkyl groups couples with an investigation into typical crude
oil compositions to suggest an explanation. However, conclusive
evidence requires an experiment designed to delineate also the role of
allcyl groups in component partitioning. That experiment is briefly
outlined. The discussion also presents explanations to account for the
differences Holm and Josendal observed between displacements with an
aromatic oil and those conducted with a paraffinic oil. This leads to a
reexamination of their correlation which depends on a rudimentary
characterization of oil composition.
Chapter four presents a recently proposed correlation that uses the
type of component partitioning data generated by the continuous multiple
contact experiment as a basis for determining a parameter representing
oil composition. The merits of the method are discussed, results are
compared with other correlations and experimental data, and the
additional work needed to develop the correlation is outlined.
Chapter five summarizes the results of the investigation and lists
the conclusions that can be drawn from the information presented.
Role of Phase Behavior in the Development of Miscibility
The key to understanding how aromaticity might affect recovery
efficiency first requires a clear picture of the phase behavior
mechanism which allows carbon dioxide to recover oil miscibly. The term
"miscible" is used rather loosely throughout the CO2 flooding
literature. Usually carbon dioxide is not completely miscible with
crude oils at typical reservoir conditions. However, the continuous
process of preferential extraction of lighter hydrocarbons into a
C02~rich phase leads to the development of a very efficient
displacement. Hutchinson and Braun (1961) first used ternary
representations of phase behavior to illustrate the development of
miscibility with methane as the displacing solvent. Similar arguments
can be applied to C02-crude oil systems. Of course, crude oils consist
of hundreds of organic compounds, and the use of ternary diagrams
requires that the oil be described by only two pseudo—components as
shown in Figure 1.1. Orr, Silva and Lien (1983) demonstrated that this
simple representation of phase compositions gives enough information to
make fairly accurate quantitative predictions of one-dimensional
displacements. In general, ternary diagrams offer a convenient method
of representing phase compositions for mixtures containing three
components. Tie lines within the two-phase region connect each upper
phase composition with its corresponding lower phase composition. The
series of tie line end points generates a binodal curve with the plait
point dividing the upper and lower phase composition portions of the
curves.
The type of phase behavior shown here represents but one of several
associated with C02-crude oil mixtures (Orr, Yu and Lien 1981). In this
simple representation, the light hydrocarbon component acts as a
co-solvent for the system. A co-solvent serves to promote miscibility
between two immiscible substances. Francis (1955) showed for several
different ternary systems that the solubility of an oil in carbon
dioxide can be enhanced by many different co-solvents. In the case of
crude oils, as shown in Figure 1.1, the crude oil contains its own
co-solvent in the form of lighter hydrocarbons. Thus, miscibility
between the crude oil and CO2 can be promoted by increasing the
concentration of the co-solvent.
Figure 1.2, first presented by Orr (1983), combines a ternary
representation of phase behavior with a simple model of a porous medium
to show how this is accomplished. This explanation of the diagram
TWO PHASE
REGION
LOWER PHASE
COMPOSITIONS
HEAVY
HYDROCARBONS
CO.
SINGLE
PHASE
REGION
UPPER PHASE
COMPOSITIONS
PLAIT
POINT
LIGHT
HYDROCARBONS
(Cg-C,^)
Figure 1.1 Typical pseudo-ternary representation of acrude oil with carbon dioxide.
HEAVY lightHYDROCARBONS HYDROCARBONS
a. PSEUDO-TERNARY DIAGRAM
STEP
1 I
2 I
3 I
0 0 0 0 0 0
V,L|
0—
0— 0 0
— 0
VR,
LR|—
V2
L20 0 — 0 0
VRg ^2 V2 +0 0 0 n
, LR2 L3\J
b. SEQUENCE OF MIXING CELLS
Figure 1.2 Pseudo-ternary representation of compositional effectsin the displacement of oil by CO2.
closely follows that given by Orr. Time step 0 shows that prior to CO2
injection the cells contain only crude oil. In the first time step
carbon dioxide is injected into the first mixing cell until the
resulting overall composition lies at point A. The equilibrated mixture
splits into tv7o phases with compositions and The C02-rich phase,
has a significantly lower viscosity than L|̂ because has a higher
concentration of CO2 and preferentially-extracted lighter hydrocarbons.
In an actual porous medium the less viscous phase, would be expected
to travel to the front of the transition zone and contact more fresh
oil. This simple model, composed of a series of discrete mixing cells,
assumes that only the less viscous phase is mobile. As more CO2 is
injected into the first cell, the upper phase, Vj^, proceeds to the
second cell and combines with fresh oil to form phases V2 and L2.
Meanwhile, the components in the first cell have partitioned into an
upper phase richer in carbon dioxide and light hydrocarbon, VR^, and a
lower phase, LRj^, which contains the residual heavier hydrocarbons and
some dissolved carbon dioxide. With continued CO2 injection, phase V2,
which is now directly miscible with the original reservoir oil, moves to
the leading edge of the transition zone to contact more fresh oil. The
molecular weight of the residual hydrocarbons continues to increase at
the trailing edge as the lighter components are preferentially extracted
and carried away.
Slim Tubes and "Minimum Miscibility Pressure"
Clearly, phase behavior determines whether or not miscibility
develops. Factors which can influence phase behavior include
temperature, pressure, and oil composition. The temperature and oil
composition are, of course, reservoir characteristics that cannot easily
be changed. Figure 1.3 couples two ternary diagrams to illustrate
qualitatively the effects of pressure on phase behavior and consequently
displacement efficiency. In both diagrams the complex composition of
the reservoir oil is again represented as two pseudo-components. The
top diagram is at a lower pressure than the bottom one. The extended
critical tie line in each passes through the plait point adjacent to the
binodal curve. In the top diagram the critical tie line intersects the
baseline to the right of the original oil composition so that the
original oil composition lies within the region of tie line extensions.
As the displacement proceeds, the composition at the front of the
transition zone again travels down the binodal curve, but in this case
it encounters a limiting tie line before miscibility develops. The
upper phase composition remains fixed as it contacts additional fresh
oil. Thus, the displacement remains immiscible. Increasing the
pressure as shown in the bottom figure alters the component
partitioning. The increase in hydrocarbon extraction into the C02-rich
phase combines with the increase in CO2 solubility in the oil-rich phase
to decrease the size of the binodal curve and to shift the tie line
slopes in a favorable way. In this case, the region of tie line
extensions does not include the original oil composition and, hence, oil
can be "miscibly" recovered by the same mechanism described for Figure
1.2.
Rather than measure phase behavior directly, the studies of Holm
and Josendal (1982) and Yellig and Metcalfe (1980) relied on slim tube
displacements to measure the effects of temperature and oil composition
on recovery efficiency. Slim tube displacements are usually conducted