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Enregistrement W1589256923 · doi:10.5772/15096

Mixed Convection Heat and Mass Transfer with Phase Change and Flow Reversal in Channels

2011· book-chapter· en· W1589256923 sur OpenAlexaff
Brahim Benhamou, Othmane Oulaid, Mohamed Aboudou, Nicolas Galanis

Notice bibliographique

RevueInTech eBooks · 2011
Typebook-chapter
Langueen
DomaineEngineering
ThématiqueNanofluid Flow and Heat Transfer
Établissements canadiensUniversité de Sherbrooke
Organismes subventionnairesnon disponible
Mots-clésNusselt numberSherwood numberMechanicsThermodynamicsCondenser (optics)Natural convectionMass transferForced convectionHeat transferAirflowMaterials scienceGrashof numberChemistryReynolds numberPhysicsOpticsTurbulence

Résumé

récupéré en direct d'OpenAlex

Due to its widespread applications, heat and mass transfer in an air stream with liquid film evaporation or condensation in open channels has received considerable attention in the literature. This kind of flows is present in many natural and engineering processes, such as human transpiration, desalination, film cooling, liquid film evaporator, cooling of microelectronic equipments and air conditioning. Since the original theory for flow of a mixture of vapour and a non-condensable gas by These studies deal with different geometric configurations such as a flat plate, parallel-plate channel and rectangular or circular-section ducts. Heat and mass transfer convection over a flat plate wetted by a liquid film has been investigated by He performed an analytical and experimental study of the evaporation of a liquid film streaming along a porous flat plate into a naturally driven airflow. This author established correlations for Nusselt and Sherwood numbers in connection with a combined Grashof number. Ben The solutions of the governing equation have been obtained by means of semi-analytical and finite difference methods. The authors present their results in term of expressions of the wall temperature and mass fraction as well as the local Nusselt and Sherwood numbers. A numerical and experimental analysis has been carried out by Tsay et al. (1990) to explore the detailed heat transfer characteristics for a falling liquid film along a vertical insulated flat plate. Free stream air temperature was set at 30C and inlet liquid film temperature was taken equal to 30C or 35C. The results show that latent heat transfer connected with vaporization is the main cause for cooling of the liquid film. The authors affirm that when the inlet liquid temperature is equal to the ambient one, latent heat transfer due to the film vaporization initiates heat transfer in the film and gas flow. Aguanoun et al (1994; 1998) studied numerically the evaporation of a falling film on an inclined plate heated www.intechopen.com Mass Transfer in Multiphase Systems and its Applications 180 at a constant temperature in a humid air stream. They considered forced A boundary layer type model was adopted. The authors stated that the liquid film-gas interface has approximately the same temperature as the plate in the case of forced convection. Yan & Soong (1995) considered turbulent heat and mass transfer convection over a wetted inclined plate. The liquid film flow is turbulent and waves less. Their results pointed out that the plate and the gas-liquid interface temperatures are reduced consequently to the increase of the plate's inclination angle, the inlet film thickness or the air velocity. The plate is insulated or heated by a constant heat flux. The main result of this study was that the enthalpy diffusion term in the energy equation does not influence the film temperature. This term represents the effect of the species diffusion on enthalpy of the humid air mixture. Volchkov et al. ( The authors aim to establish the validity of the heat-mass transfer analogy. The steam in the humid airflow may condense on the plate whose temperature is lower than that of the airflow. The authors made a major simplification by neglecting the effect of the condensate film. This assumption is justified by the experimental data in the literature which indicate that measurements of the liquid film-air interface temperature in humid-air flows show that it is close to the saturation temperature corresponding to the vapour concentration at the plate. This point is addressed hereafter. Recently, Maurya et al. ( Their results show that the evaporation process begins only after the growing thermal boundary layer reaches the interface. Heat and mass transfer in a vertical heated tube with a liquid film falling on its inside walls was treated by They considered co-current downward flows of liquid water and humid air. The airflow is turbulent while the liquid one is laminar and without surface waves. The authors concluded that better cooling of the liquid film is obtained for higher heat flux or lower inlet liquid flow. Their results show that large film evaporation rates are obtained for larger tube wall temperature. Convective instability of heat and mass transfer for laminar forced convection in the thermal entrance region of a horizontal rectangular channel has been examined by The rectangular channel is thermally insulated except for the bottom wall. The latter is maintained at a constant temperature and covered by a thin liquid water film. The thickness of this film is neglected, thus it is treated as a boundary condition for heat and mass transfer. Inlet air temperature was fixed at 20C. The effects of changes of bottom wall temperature, relative humidity of air at the entrance and the channel aspect ratio are examined. The results show that the convective instability is affected by changes in inlet air relative humidity and temperature and also the channel aspect ratio. Huang et al. ( Two of the duct walls were wetted by a thin liquid water film and maintained at different constant temperatures. The other walls are insulated. Air entered the duct with a constant temperature lower than that of the walls. The authors established that vapour condensation occurred on the wall with lower temperature. They used a boundary-layer approximation model to derive a www.intechopen.com

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.

Comment cette classification a été obtenuedéplier

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 candidatesMéta-épidémiologie (sens strict)
Catégories consensuellesaucune
DomaineSignal candidat: aucune · Signal consensuel: aucune
Devis d'étudeSignal candidat: Expérimental (laboratoire) · Signal consensuel: Expérimental (laboratoire)
GenreSignal candidat: Empirique · Signal consensuel: aucune
Score de désaccord entre enseignants0,923
Score d'incertitude au seuil1,000

Scores Codex et Gemma par catégorie

CatégorieCodexGemma
Métarecherche0,0000,000
Méta-épidémiologie (sens strict)0,0000,000
Méta-épidémiologie (sens large)0,0000,000
Bibliométrie0,0000,000
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 Opus0,041
Tête enseignante GPT0,209
Écart entre enseignants0,168 · 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

Classification

machine, non validée

Prédiction automatique; un appel candidat d’une seule tête enseignante, pas un consensus.

Devis d'étudeExpérimental (laboratoire)
Domainenon disponible
GenreEmpirique

Le détail, modèle par modèle et score par score, se trouve en fin de page sous « Comment cette classification a été obtenue ».

En bref

Citations1
Publié2011
Routes d'admission1
Résumé présentoui

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