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Record W2003356265 · doi:10.2118/01-03-das

Mechanisms of Solution Gas Drive in Heavy Oil Reservoirs

2001· article· en· W2003356265 on OpenAlexaboutno aff
Abbas Firoozabadi

Bibliographic record

VenueJournal of Canadian Petroleum Technology · 2001
Typearticle
Languageen
FieldEngineering
TopicEnhanced Oil Recovery Techniques
Canadian institutionsnot available
FundersU.S. Department of Energy
KeywordsPetroleum engineeringEnvironmental scienceOil productionGas oil ratioFossil fuelEnhanced oil recoveryProduction (economics)Work (physics)ViscosityProduction rateRange (aeronautics)GeologyWaste managementMaterials scienceEngineeringThermodynamicsProcess engineeringPhysicsMechanical engineering

Abstract

fetched live from OpenAlex

Introduction Solution gas drive in heavy oil reservoirs (with viscosity in the range of 10 to 1,000 poise and API gravity in the range of eight to 15), which is often referred to as cold production, has a long production history in Canada. In a recent review paper, Dusseault et al.(1) presented the information that more than 5,000 wells in Canada have produced heavy oil by cold production. In addition to Canada, cold production from heavy oil reservoirs has been practiced in Venezuela(2), China(3), and Oman(4). Recoveries from some of the heavy oil reservoirs by cold production are estimated to be as high as 20﹪. The high recovery is often associated with a low pressure decline rate in the reservoir and the slow increase of GOR in the two-phase below the bubblepoint, as well as geomechanical effects. Recoveries in the range of 10 to 20﹪ below the bubblepoint pressure are believed unusual for very heavy oils. In this overview, we will briefly review the literature and then provide some insight into the relevant mechanisms for cold production. Literature Review An early paper by Smith(5) set the stage for the understanding of cold production from solution gas drive in heavy oil reservoirs. In his work, Smith provides an analysis of solution gas drive in heavy oil reservoirs from the examination of field data. He attributes the high efficiency of solution gas drive in viscous oils to:a significant reduction (around one order of magnitude) in the oil viscosity due to formation of small gas bubbles in the oil,simultaneous flow of continuous oil phase and discontinuous gas phase in the form of tiny bubbles,an increase in absolute permeability due to sand production, andhigh fluid compressibility due to high gas bubble density in the oil. In order to validate some of the postulations by Smith, the bulk of research has focused on the socalled pseudo-single phase model. In the pseudo-single phase model, a new terminology has evolved to distinguish solution gas drive in heavy oil reservoirs. The so-called foamy oil terminology was introduced in 1992 by Sarma and Maini(6); it was defined as a viscous (heavy) oil containing dispersed gas bubbles. Claridge and Prats(7) used the term " foamy heavy oil" and " foamy crude" mainly to imply drastic reduction in the oil viscosity due to dispersed as bubbles. The term " foamy oil" has had a wide acceptance because the oil samples at the wellhead produced from the reservoirs seem to be in the form of oil-continuous foam, with the appearance of chocolate mousse, and may contain a large volume of dispersed gas bubbles. Hu et al.(3) report that the density of the produced oil from a heavy oil pilot well from the Henan oil field in China is about 0.58 g/cm3, while the density after all the gas has left the oil (which may take several days) is 0.95 g/cm3.

Fetched live from OpenAlex and de-inverted. Abstracts are not stored in this database: the inverted indexes are 8.6 GB of the frame’s 9.3 GB of text, and the host has 13 GB free.

How this classification was reachedexpand

Full frame distilled prediction

Teacher imitation

Not calibrated prevalence, not ground truth. Human validation pending. Learned from the 10,348 direct Codex labels and 10,348 direct Gemma labels. Candidate is the union of thresholded teacher heads; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels or direct frontier model labels.

metaresearch head score (Codex)0.000
metaresearch head score (Gemma)0.000
Version: codex-gemma-dda1882f352aValidation status: machine_predicted_unvalidated
Candidate categoriesnone
Consensus categoriesnone
DomainCandidate signal: none · Consensus signal: none
Study designCandidate signal: Bench or experimental · Consensus signal: Bench or experimental
GenreCandidate signal: Empirical · Consensus signal: Empirical
Teacher disagreement score0.240
Threshold uncertainty score0.769

Codex and Gemma teacher scores by category

CategoryCodexGemma
Metaresearch0.0000.000
Meta-epidemiology (narrow)0.0000.000
Meta-epidemiology (broad)0.0000.000
Bibliometrics0.0050.001
Science and technology studies0.0000.000
Scholarly communication0.0000.000
Open science0.0000.000
Research integrity0.0000.001
Insufficient payload (model declined to judge)0.0000.000

Machine scores (provisional)

The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.

Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.

Opus teacher head0.007
GPT teacher head0.203
Teacher spread0.196 · how far apart the two teachers sit on this one work
Validation statusscore_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it

Classification

machine, unvalidated

Machine predicted; a candidate call from one teacher head, not a consensus.

The models applied no category: nothing in the taxonomy fit this work.
Study designBench or experimental
Domainnot available
GenreEmpirical

How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".

Quick stats

Citations71
Published2001
Admission routes1
Has abstractyes

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