Matches in SemOpenAlex for { <https://semopenalex.org/work/W1988617999> ?p ?o ?g. }
Showing items 1 to 96 of
96
with 100 items per page.
- W1988617999 abstract "Flow in annular geometries, i.e., flow through the gap between two cylindrical pipes, occurs in many different engineering professions, such as petroleum engineering, chemical engineering, mechanical engineering, food engineering, etc. Analysis of the flow characteristics through annular geometries is more challenging when compared with circular pipes, not only due to the uneven stress distribution on the walls but also due to secondary flows and tangential velocity components, especially when the inner pipe is rotated. In this paper, a mathematical model for predicting flow characteristics of Newtonian fluids in concentric horizontal annulus with drill pipe rotation is proposed. A numerical solution including pipe rotation is developed for calculating frictional pressure loss in concentric annuli for laminar and turbulent regimes. Navier-Stokes equations for turbulent conditions are numerically solved using the finite differences technique to obtain velocity profiles and frictional pressure losses. To verify the proposed model, estimated frictional pressure losses are compared with experimental data which were available in the literature and gathered at Middle East Technical University, Petroleum & Natural Gas Engineering Flow Loop (METU-PETE Flow Loop) as well as Computational Fluid Dynamics (CFD) software. The proposed model predicts frictional pressure losses with an error less than ± 10% in most cases, more accurately than the CFD software models depending on the flow conditions. Also, pipe rotation effects on frictional pressure loss and tangential velocity is investigated using CFD simulations for concentric and fully eccentric annulus. It has been observed that pipe rotation has no noticeable effects on frictional pressure loss for concentric annuli, but it significantly increases frictional pressure losses in an eccentric annulus, especially at low flow rates. For concentric annulus, pipe rotation improves the tangential velocity component, which does not depend on axial velocity. It is also noticed that, as the pipe rotation and axial velocity are increased, tangential velocity drastically increases for an eccentric annulus. The proposed model and the critical analysis conducted on velocity components and stress distributions make it possible to understand the concept of hydro transport and hole cleaning in field applications." @default.
- W1988617999 created "2016-06-24" @default.
- W1988617999 creator A5000459775 @default.
- W1988617999 creator A5021885965 @default.
- W1988617999 creator A5048947308 @default.
- W1988617999 creator A5064367718 @default.
- W1988617999 date "2010-01-01" @default.
- W1988617999 modified "2023-09-25" @default.
- W1988617999 title "Modeling of Newtonian Fluids in Annular Geometries With Inner Pipe Rotation" @default.
- W1988617999 doi "https://doi.org/10.1115/fedsm-icnmm2010-31176" @default.
- W1988617999 hasPublicationYear "2010" @default.
- W1988617999 type Work @default.
- W1988617999 sameAs 1988617999 @default.
- W1988617999 citedByCount "2" @default.
- W1988617999 countsByYear W19886179992013 @default.
- W1988617999 countsByYear W19886179992015 @default.
- W1988617999 crossrefType "proceedings-article" @default.
- W1988617999 hasAuthorship W1988617999A5000459775 @default.
- W1988617999 hasAuthorship W1988617999A5021885965 @default.
- W1988617999 hasAuthorship W1988617999A5048947308 @default.
- W1988617999 hasAuthorship W1988617999A5064367718 @default.
- W1988617999 hasConcept C114088122 @default.
- W1988617999 hasConcept C121332964 @default.
- W1988617999 hasConcept C127413603 @default.
- W1988617999 hasConcept C150936888 @default.
- W1988617999 hasConcept C159985019 @default.
- W1988617999 hasConcept C1633027 @default.
- W1988617999 hasConcept C173736775 @default.
- W1988617999 hasConcept C182748727 @default.
- W1988617999 hasConcept C191545125 @default.
- W1988617999 hasConcept C192562407 @default.
- W1988617999 hasConcept C196558001 @default.
- W1988617999 hasConcept C204561356 @default.
- W1988617999 hasConcept C2524010 @default.
- W1988617999 hasConcept C2776088076 @default.
- W1988617999 hasConcept C294558 @default.
- W1988617999 hasConcept C33923547 @default.
- W1988617999 hasConcept C38349280 @default.
- W1988617999 hasConcept C57879066 @default.
- W1988617999 hasConcept C74050887 @default.
- W1988617999 hasConcept C76563973 @default.
- W1988617999 hasConcept C78519656 @default.
- W1988617999 hasConcept C90278072 @default.
- W1988617999 hasConcept C90296322 @default.
- W1988617999 hasConcept C92854067 @default.
- W1988617999 hasConceptScore W1988617999C114088122 @default.
- W1988617999 hasConceptScore W1988617999C121332964 @default.
- W1988617999 hasConceptScore W1988617999C127413603 @default.
- W1988617999 hasConceptScore W1988617999C150936888 @default.
- W1988617999 hasConceptScore W1988617999C159985019 @default.
- W1988617999 hasConceptScore W1988617999C1633027 @default.
- W1988617999 hasConceptScore W1988617999C173736775 @default.
- W1988617999 hasConceptScore W1988617999C182748727 @default.
- W1988617999 hasConceptScore W1988617999C191545125 @default.
- W1988617999 hasConceptScore W1988617999C192562407 @default.
- W1988617999 hasConceptScore W1988617999C196558001 @default.
- W1988617999 hasConceptScore W1988617999C204561356 @default.
- W1988617999 hasConceptScore W1988617999C2524010 @default.
- W1988617999 hasConceptScore W1988617999C2776088076 @default.
- W1988617999 hasConceptScore W1988617999C294558 @default.
- W1988617999 hasConceptScore W1988617999C33923547 @default.
- W1988617999 hasConceptScore W1988617999C38349280 @default.
- W1988617999 hasConceptScore W1988617999C57879066 @default.
- W1988617999 hasConceptScore W1988617999C74050887 @default.
- W1988617999 hasConceptScore W1988617999C76563973 @default.
- W1988617999 hasConceptScore W1988617999C78519656 @default.
- W1988617999 hasConceptScore W1988617999C90278072 @default.
- W1988617999 hasConceptScore W1988617999C90296322 @default.
- W1988617999 hasConceptScore W1988617999C92854067 @default.
- W1988617999 hasLocation W19886179991 @default.
- W1988617999 hasOpenAccess W1988617999 @default.
- W1988617999 hasPrimaryLocation W19886179991 @default.
- W1988617999 hasRelatedWork W1267368245 @default.
- W1988617999 hasRelatedWork W1573375290 @default.
- W1988617999 hasRelatedWork W1969379606 @default.
- W1988617999 hasRelatedWork W1982984395 @default.
- W1988617999 hasRelatedWork W2034758128 @default.
- W1988617999 hasRelatedWork W2055326167 @default.
- W1988617999 hasRelatedWork W2101566420 @default.
- W1988617999 hasRelatedWork W2117341894 @default.
- W1988617999 hasRelatedWork W2204871140 @default.
- W1988617999 hasRelatedWork W2364502252 @default.
- W1988617999 hasRelatedWork W2370602368 @default.
- W1988617999 hasRelatedWork W2375945021 @default.
- W1988617999 hasRelatedWork W2387341306 @default.
- W1988617999 hasRelatedWork W2398228150 @default.
- W1988617999 hasRelatedWork W2741044978 @default.
- W1988617999 hasRelatedWork W2758414089 @default.
- W1988617999 hasRelatedWork W2891594988 @default.
- W1988617999 hasRelatedWork W2965287680 @default.
- W1988617999 hasRelatedWork W3083093180 @default.
- W1988617999 hasRelatedWork W3188397897 @default.
- W1988617999 isParatext "false" @default.
- W1988617999 isRetracted "false" @default.
- W1988617999 magId "1988617999" @default.
- W1988617999 workType "article" @default.