Integral Analysis of Turbulent Natural Convection with Condensation in the Presence of a Noncondensable Gas

dc.contributor.advisorJames Selgrade, Committee Memberen_US
dc.contributor.advisorTiegang Fang, Committee Memberen_US
dc.contributor.advisorHerbert Eckerlin, Committee Co-Chairen_US
dc.contributor.advisorJames Leach, Committee Chairen_US
dc.contributor.authorMatar, Walid Omaren_US
dc.date.accessioned2010-04-02T18:12:06Z
dc.date.available2010-04-02T18:12:06Z
dc.date.issued2010-03-08en_US
dc.degree.disciplineMechanical Engineeringen_US
dc.degree.levelthesisen_US
dc.degree.nameMSen_US
dc.descriptionNorth Carolina State University Theses Mechanical and Aerospace Engineering.;North Carolina State University Theses Mechanical and Aerospace Engineering.
dc.description.abstractAn approximate model is presented for turbulent natural convection flow of a two-component mixture in which condensate forms along a vertical wall. The integral method is employed as the scheme for the analysis of the gas boundary layer. By incorporating empirical correlations and profiles for temperature, velocity, and density, the compressible Navier-Stokes equations are solved for boundary layer thickness and maximum velocity. Eventually, the desired physical characteristics of heat flux and condensation rate are determined. The major constraint enforced in the model is that the water within the boundary layer is either saturated vapor or slightly superheated. Local condensation away from the wall is not considered. A diverse range of mixtures were studied to examine the effects of noncondensable gas concentration on the heat transfer and condensation rates. It is shown in the results how the presence of air is a hindrance to the diffusion of vapor through the gas boundary layer. The results are compared to a previous empirical model. The results showed reasonable agreement with the previous experimental study discussed. For very large and often times more applicable temperature differences, the model predicts volumetric condensation within the gas boundary layer. A semi-empirical one-equation turbulence model was introduced, and although the turbulent impact on effective properties was determined to be small, it was included nonetheless for flexibility. Code logic and methodology are presented to automate this problem, as the solution is obtained through the iteration on both the turbulent viscosity and the interface temperature.en_US
dc.formatThesis (M.S.)--North Carolina State University.
dc.identifier.otheretd-03022010-171030en_US
dc.identifier.urihttp://www.lib.ncsu.edu/resolver/1840.16/2301
dc.rightsI hereby certify that, if appropriate, I have obtained and attached hereto a written permission statement from the owner(s) of each third party copyrighted matter to be included in my thesis, dis sertation, or project report, allowing distribution as specified below. I certify that the version I submitted is the same as that approved by my advisory committee. I hereby grant to NC State University or its agents the non-exclusive license to archive and make accessible, under the conditions specified below, my thesis, dissertation, or project report in whole or in part in all forms of media, now or hereafter known. I retain all other ownership rights to the copyright of the thesis, dissertation or project report. I also retain the right to use in future works (such as articles or books) all or part of this thesis, dissertation, or project report.en_US
dc.subjectcondensationen_US
dc.subjectnatural convectionen_US
dc.subjectintegral analysisen_US
dc.titleIntegral Analysis of Turbulent Natural Convection with Condensation in the Presence of a Noncondensable Gasen_US
dcterms.abstractKeywords: condensation, natural convection, integral analysis.
dcterms.extentviii, 55 pages : illustrations (some color)

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