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SUSTAINABLE IN-SITU HEAVY OIL AND BITUMEN RECOVERY TECHNIQUES, CASE STUDIES, AND ENVIRONMENTAL CONSIDERATIONS MOHAMMADALI AHMADI Department of Chemical and Petroleum Engineering, University of Calgary, Canada
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Contents 1. Heavy oil and bitumen characterization 1.1 1.2
Introduction Bitumen classification 1.2.1 SARA analysis 1.2.1.1 Asphaltenes 1.2.1.2 Maltenes 1.2.1.3 Resins 1.2.1.4 Oildsaturates and aromatics 1.2.2 PONA analysis 1.3 Bitumen reserves 1.4 Bitumen properties 1.4.1 Density 1.4.1.1 Density models for bitumenesolvent mixtures 1.4.2 Viscosity 1.4.2.1 Viscosity models for bitumen versus thermodynamic conditions 1.4.2.2 Models for the viscosity of the mixture of solvents and bitumen 1.4.2.3 Models based on mixing rules 1.4.2.4 Direct regression model 1.4.2.5 Expanded fluid viscosity correlation 1.4.2.6 Corresponding states equations 1.4.2.7 Model based on NMR for mixture of bitumen and solvent References
2. Fundamentals of heavy oil and bitumen recovery 2.1 2.2
Introduction Bitumen recovery techniques 2.2.1 Thermal recovery methods 2.2.1.1 Steam flooding 2.2.1.2 Hot water injection 2.2.1.3 Cyclic steam stimulation 2.2.1.4 Steam-assisted gravity drainage 2.2.2 Solvent-based recovery methods 2.2.2.1 Cyclic solvent injection
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2.2.3
2.2.4
2.2.2.2 Vapor extraction process 2.2.2.3 N-Solv Solvent-assisted thermal methods 2.2.3.1 Expanded solvent steam-assisted gravity drainage 2.2.3.2 Liquid addition to steam for enhancing recovery 2.2.3.3 Steam alternating solvent Steam-additive coinjection methods 2.2.4.1 Chemical-steam coinjection 2.2.4.2 Noncondensable gas-steam coinjection
References
3. Nonthermal heavy oil recovery 3.1 3.2
Introduction Background 3.2.1 Solvent-based recovery methods 3.2.1.1 Cyclic solvent injection 3.2.1.2 Vapor extraction process (VAPEX) 3.2.1.3 N-Solv 3.3 Phase behavior of bitumenesolvent systems 3.4 Solvent diffusivity in bitumen 3.5 Calculation of solvent diffusion coefficient in bitumen 3.6 Scaling-up criteria of the heavy oil production References
4. In-situ thermal heavy oil recovery 4.1 4.2 4.3
Introduction Background Conventional steam-based recovery processes 4.3.1 Cyclic steam stimulation 4.3.2 Steam flooding 4.3.3 Steam-assisted gravity drainage 4.4 Heat transfer theory 4.5 Mathematical modeling of in-situ thermal recovery methods 4.6 Transient convective heat transfer References
5. In-situ upgrading 5.1 5.2 5.3
Introduction Background Catalysts for in-situ upgrading
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5.3.1 Water-soluble catalysts 5.3.2 Oil-soluble catalysts 5.3.3 Amphiphilic catalysts 5.3.4 Minerals, zeolites, and solid superacids 5.3.5 Ionic liquids 5.3.6 Dispersed catalysts 5.3.7 Metallic NPs 5.4 Mechanism 5.5 Technical challenges 5.5.1 Formation damage 5.5.2 Cost 5.5.3 Environmental footprint 5.5.4 Recoverability References
6. Solvent-steam coinjection 6.1 6.2 6.3 6.4 6.5
Introduction Background Mechanisms involved in solvent-based heavy oil recovery methods Relative permeability Solvent-assisted thermal recovery methods 6.5.1 Solvents in steam flooding 6.5.2 Steam-alternating solvent 6.5.3 Solvents in CSS 6.5.4 Solvent in SAGD 6.6 Mathematical modeling of solvent-steam coinjection 6.7 Steam-bitumen-solvent phase behavior 6.7.1 Gibbs phase rule and phase equilibrium 6.7.2 Steam-bitumen binary system 6.7.3 Water-solvent binary system 6.7.4 Water-bitumen-solvent ternary system 6.8 Field trials of solvent-steam Coinjection technique 6.9 Technical challenges References
7. Noncondensable gas-steam coinjection 7.1 7.2 7.3 7.4
Introduction Background Mechanisms of NCG-steam coinjection Mathematical modeling of NCG-steam coinjection
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7.5 Phase equilibrium of bitumen/water/noncondensable gas 7.6 Field trials of NCG-steam coinjection technique References
8. Chemical-steam coinjection 8.1 8.2 8.3
Introduction Background Surfactant screening 8.3.1 Surfactant types 8.3.2 Critical micelle concentration 8.3.3 Hydrophilicelipophilic balance 8.3.3.1 Empirical models 8.3.3.2 Water dispersibility 8.3.3.3 Experimental estimation 8.3.3.4 Group contribution approach 8.4 Adsorption of chemicals 8.4.1 Adsorption models 8.4.2 Adsorption kinetic 8.4.3 Adsorption thermodynamics 8.5 Thermal stability of chemicals 8.6 IFT reduction and wettability alteration 8.7 Foam generation 8.8 Emulsion generation 8.9 Surfactant applications in thermal recovery methods 8.9.1 Surfactants in hot waterflooding 8.9.2 Surfactants in steam flooding 8.9.3 Surfactants in CSS 8.9.4 Surfactants in SAGD 8.10 Molecular mechanisms of surfactant-assisted bitumen recovery 8.11 Field trials of surfactant-steam coinjection technique 8.12 Technical challenges References
9. Hybrid of in-situ combustion and steam-based heavy oil recovery 9.1 9.2
Introduction Fundamentals of ISC 9.2.1 Dry combustion 9.2.2 Wet combustion 9.2.3 Chemical reactions associated with in-situ combustion
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9.2.3.1 LTO reactions 9.2.3.2 Negative temperature gradient region 9.2.3.3 MTO reactions 9.2.3.4 HTO reactions 9.3 Drawbacks of in-situ combustions 9.4 Models for in-situ combustion reactions 9.5 Hybrid ISC and steam-based bitumen recovery 9.6 Field applications References
10. Electromagnetic heating processes for heavy oil and bitumen recovery 10.1 Introduction 10.2 Background 10.3 Electrical heating techniques 10.3.1 Electric heater 10.3.2 Electrical resistance heating 10.3.3 Inductive heating 10.3.4 Electrocarbonization 10.3.5 Laser heating 10.3.6 Electroosmosis 10.3.7 Electromagnetic heating 10.4 Electrothermal dynamic stripping process 10.5 Thermal-assisted gravity drainage 10.6 Low-pressure electrothermally assisted drainage 10.7 High-frequency techniques 10.8 Hybrid of EM and SAGD 10.9 Heating start-up models 10.9.1 SAGD process 10.9.2 Ohmic heating (with electric heaters) 10.9.3 Electrothermal heating with conduction only 10.9.4 Electrothermal heating with convective heating 10.9.5 Inductive heating 10.9.6 RF heating or the ESEIEH process 10.10 Field trials 10.11 Techno-economic modeling of ESEIEH process 10.11.1 Capital cost 10.11.2 Operational cost References
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11. Practical challenges in reservoir simulation of in-situ thermal heavy oil recovery 11.1 Introduction 11.2 Mathematical description 11.2.1 Mass conservation 11.2.2 Energy conservation 11.2.3 Simulation constraints 11.3 Thermal simulation 11.4 Critical parameters and mechanisms involving in numerical simulation of thermal bitumen recovery processes 11.4.1 Heterogeneity effect on SAGD and solvent-assisted coinjection process 11.4.2 Effect of operational parameters on solvent and water-assisted electrical heating process 11.4.3 Impact of aqueous phase solubility on noncondensable gas-steam coinjection simulation 11.4.4 Numerical simulation of surfactant-steam coinjection under SAGD configuration 11.4.5 Numerical simulation of undulating shale breaking with SAGD 11.4.6 Numerical modeling of in-situ combustion and SAGD 11.4.7 Effect of operating pressure on the efficiency of toe-to-heel air injection in-situ combustion 11.4.8 THAI in-situ combustion operation in heavy oil reservoirs with bottom aquifer 11.4.9 Steam injection and bitumen production time scales during SAGD operation 11.4.10 Comparison of performance of thermal recovery methods 11.4.11 Numerical simulation of multilateral wells with dynamic gridding in SAGD operation 11.5 Summary References Index
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CHAPTER ONE
Heavy oil and bitumen characterization 1.1 Introduction Petroleum is a mixture of various hydrocarbon compounds that can contain varying amounts of elements such as oxygen, nitrogen, sulfur, hydrogen, and trace metals like nickel and vanadium. Table 1-1 reported that crude oils are classed as conventional light to medium crude oil, heavy oil, extra-heavy oil, or bitumen, depending on their viscosity and American Petroleum Institute (API) gravity. Bitumen is a term used to describe an extra-heavy oil immobile under reservoir conditions (Fig. 1-1). The viscosity of extra-heavy and heavy crude oils deviates from that of conventional light oils, with the primary distinction being their ability to flow to a wellbore via natural driving energy of the reservoir. On the other hand, bitumen is too viscous to flow to the wellbore without artificial stimulation at reservoir temperature and pressure. With an API gravity of 10 degrees to 22.3 degrees (1 g/cc to 0.92 g/cc) and a viscosity of 100 cP to 10,000 cP, heavy oil has a specific gravity close to water (See Fig. 1-1). Bitumen, a dense hydrocarbon material, has a viscosity that is similar to that of honey or molasses when it is in its minimum state. Additionally, it has a viscosity greater than 10,000 centipoise (cP) when it is free of gas and an API gravity of 10 degrees. The viscosity of heavy oil and bitumen can be affected by a range of parameters, including the length and composition of the molecular chains, the amount of natural dissolved gas present, and reservoir temperature and pressure; hence, there is no direct relation between oil viscosity and density [2,4e7]. Table 1-1 Properties of liquid petroleum under standard conditions [1]. Density (kg/m3) Viscosity (mPa.s) Type of oil Gravity (oAPI)
Bitumen Extra-heavy oil Heavy oil Medium crude oil Light crude oil
1000 900e1000 855e900 815e855
>105