MétaCan
Menu
Retour à la cohorte
Enregistrement W2065482358 · doi:10.2118/68885-jpt

Foamy-Oil Flow

2001· article· en· W2065482358 sur OpenAlex

Pourquoi ce travail est dans la base

Une base qui oublie comment elle a trouvé un travail ne peut pas être vérifiée. Voici les voies qui ont admis celui-ci.

affAu moins un auteur déclare une institution canadienne dans l'instantané OpenAlex épinglé.
aboutLe titre ou le résumé porte un signal canadien du lexique géographique.

Notice bibliographique

RevueJournal of Petroleum Technology · 2001
Typearticle
Langueen
DomaineEngineering
ThématiqueEnhanced Oil Recovery Techniques
Établissements canadiensUniversity of Calgary
Organismes subventionnairesnon disponible
Mots-clésWellheadPetroleum engineeringFlow (mathematics)Scope (computer science)Scale (ratio)PetroleumComputer scienceOperations researchGeologyEngineeringMechanicsGeographyPhysics

Résumé

récupéré en direct d'OpenAlex

Distinguished Author Series articles are general, descriptive representations that summarize the state of the art in an area of technology by describing recent developments for readers who are not specialists in the topics discussed. Written by individuals recognized to be experts in the area, these articles provide key references to more definitive work and present specific details only to illustrate the technology. Purpose: to inform the general readership of recent advances in various areas of petroleum engineering. Summary Foamy-oil flow is a non-Darcy form of two-phase flow of gas and oil encountered in many Canadian and Venezuelan heavy-oil reservoirs during production under solution-gas drive. Unlike normal two-phase flow, which requires a fluid phase to become continuous before it can flow, it involves flow of dispersed gas bubbles. This paper is aimed at acquainting the readers with this type of flow and its role in heavy-oil production. The paper starts with a discussion of what the term "foamy-oil flow" means and how it evolved. Then a brief review of the Canadian field practices is presented. This is followed by a discussion of the pore-scale mechanisms involved and the interplay between capillary and viscous forces. A discussion of the strengths and weaknesses of various mathematical models proposed for numerical simulation of this type of flow is also included. The paper ends with a brief discussion of issues that remain unresolved. Introduction The term "foamy oil" originated from observations of stable foams in samples collected at the wellhead from many Canadian and Venezuelan heavy-oil wells that produce under solution-gas drive. The oil produced from these wells was in the form of thick oil-continuous foam. It was noticed that, very often, a sample container that was overflowing with oil at the time of collection at the wellhead was nearly empty; less than 20% of its volume was filled with oil when opened in the laboratory a few days later, by which time the foam had collapsed. Many of these reservoirs also exhibit anomalous production behavior, both in terms of higher-than-expected well productivity and remarkably high primary recovery factors,1 and this observation was not the result of metering errors caused by foam. Over the years, this anomalous production behavior became closely associated with the foamy nature of the produced oil, and it was suggested that perhaps the two-phase flow behavior of this type of oil in a reservoir rock is different from that of a normal oil/gas mixture. The term "foamy-oil flow" was coined to distinguish the two-phase oil/gas flow in a porous medium of such heavy oils from the normal two-phase behavior. This overview attempts to acquaint the reader with recent developments related to this topic, then provides some insight into the mechanisms involved. Smith1 appears to be the first to publish a detailed analysis of such unusual production behavior. He attributed it to the flow characteristics of heavy oil containing a large volume fraction of very small gas bubbles. He suggested that the mobility of a dispersion of very small bubbles in the heavy oil could be several-fold higher than the single-phase oil mobility. Maini et al.2 attempted to verify this assertion of high dispersion mobility in the laboratory but found that the presence of freshly nucleated gas bubbles actually decreased the oil mobility. However, they found that the dispersed flow of gas was indeed possible under solution-gas-drive conditions. Since then, the flow behavior of such gas-in-oil dispersions has become a subject of several investigations3–15 and considerable speculation, but it remains controversial and poorly understood. Nonetheless, it is well accepted that solution-gas drive in foamy-oil reservoirs involves some unusual effects. It should be mentioned that such dispersed flow of gas under solution-gas-drive conditions in the laboratory was noted by Handy16 in 1958 in high decline rate experiments. However, he concluded that, at the low pressure decline rates in the field, the dispersed flow would not be a significant factor. Although there is still debate on the suitability of the phrase "foamy-oil flow" to describe the anomalous flow of the oil/gas mixtures in cold production of heavy oil, the expression has become a part of petroleum engineering terminology. To some, the term "foamy-oil flow" suggests two-phase flow in the form of oil-continuous foam, and they find it to be a misnomer because the actual microstructure may not resemble foam. To others, including this author, it only denotes the flow of a gas-in-oil dispersion, which is what appears to be involved. However, the full meaning of the term is still evolving, and for now it can be treated as a catchall phrase for representing the contribution of nonequilibrium processes in solution-gas drive in heavy-oil systems. There are two types of nonequilibrium processes involved in solution-gas drive in heavy oils. There is the nonequilibrium between solution gas and free gas that leads to a possibility of significant supersaturation of dissolved gas in the oil phase. The ramifications are delayed release of solution gas and an apparent bubblepoint that is lower than the true thermodynamic bubblepoint. This nonequilibrium process is affected by the kinetics of bubble nucleation and gas diffusivity. Because bubble nucleation is a stochastic process driven by supersaturation, the degree of supersaturation required before nucleation occurs depends on the time available for nucleation. Therefore, this type of nonequilibrium is likely to be more significant in laboratory experiments, which are run on a much smaller time scale compared with the field case.

Récupéré en direct depuis OpenAlex et désinversé. Les résumés ne sont pas conservés dans cette base de données : les index inversés représentent 8,6 Go des 9,3 Go de texte de la base, et le serveur dispose de 13 Go libres.

Prédiction distillée sur la base complète

Imitation des enseignants

Ni prévalence calibrée, ni vérité terrain. Validation humaine à venir. Apprise à partir de 10 348 étiquettes directes de Codex et de 10 348 étiquettes directes de Gemma. Le mode candidate est l'union des têtes enseignantes seuillées; le consensus est leur intersection. Ces sorties portent le statut machine_predicted_unvalidated et ne sont ni des étiquettes humaines ni des étiquettes directes de modèles de pointe.

score de la tête « metaresearch » (Codex)0,000
score de la tête « metaresearch » (Gemma)0,000
Version: codex-gemma-dda1882f352aStatut de validation: machine_predicted_unvalidated
Catégories candidatesaucune
Catégories consensuellesaucune
DomaineSignal candidat: aucune · Signal consensuel: aucune
Devis d'étudeSignal candidat: Autre devis · Signal consensuel: aucune
GenreSignal candidat: Empirique · Signal consensuel: Empirique
Score de désaccord entre enseignants0,825
Score d'incertitude au seuil0,557

Scores Codex et Gemma par catégorie

CatégorieCodexGemma
Métarecherche0,0000,000
Méta-épidémiologie (sens strict)0,0000,000
Méta-épidémiologie (sens large)0,0000,000
Bibliométrie0,0010,000
Études des sciences et des technologies0,0000,000
Communication savante0,0000,000
Science ouverte0,0000,000
Intégrité de la recherche0,0000,001
Charge utile insuffisante (le modèle a refusé de juger)0,0000,000

Scores machine (provisoires)

Les deux têtes enseignantes du modèle étudiant, lues sur ce travail. Un score ordonne la base pour la relecture; il n'affirme jamais une catégorie, et le statut de validation accompagne chaque rangée tel quel.

Scores de référence d'un modèle non mature (critères de maturité non atteints, 7 itérations). Un score ordonne; il n'affirme jamais une catégorie.

Tête enseignante Opus0,004
Tête enseignante GPT0,208
Écart entre enseignants0,203 · la distance entre les deux têtes enseignantes sur ce seul travail
Statut de validationscore_only:v0-immature-baseline · tel quel depuis la passe de notation : score_only signifie que le nombre peut ordonner les travaux, et qu'aucune étiquette de catégorie n'en découle