dc.contributor.author |
Μαγουλάς, Αναστάσιος
|
el |
dc.contributor.author |
Magoulas, Anastasios
|
en |
dc.date.accessioned |
2020-10-28T21:21:21Z |
|
dc.date.available |
2020-10-28T21:21:21Z |
|
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/51649 |
|
dc.identifier.uri |
http://dx.doi.org/10.26240/heal.ntua.19347 |
|
dc.rights |
Default License |
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dc.subject |
Fluid |
en |
dc.subject |
CFD |
en |
dc.subject |
Transition |
en |
dc.subject |
MaPflow |
en |
dc.subject |
Incompressible |
en |
dc.subject |
Ρευστά |
el |
dc.subject |
Ασυμπίεστο |
el |
dc.subject |
Μετάβαση |
el |
dc.subject |
Τυρβώδη |
el |
dc.subject |
Υπολογιστική |
el |
dc.title |
Εφαρμογή μοντέλων μετάβασης σε τυρβώδη ροή σε ασυμπίεστο επιλύτη |
el |
dc.title |
Implementation of transition modelling on an incompressible solver |
en |
heal.type |
bachelorThesis |
|
heal.classification |
Ρευστομηχανική |
el |
heal.classification |
Fluid mechanics |
en |
heal.language |
en |
|
heal.access |
free |
|
heal.recordProvider |
ntua |
el |
heal.publicationDate |
2020-10-09 |
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heal.abstract |
The aim of the present work was to asses the performance of the modelling of transition from laminar to turbulent flow. For this purpose an incompressible solver was utilized, where the velocity and pressure fields were linked with the aid of the Artificial Compressibility Method. From all the transition models available in the literature, the Langtry and Menter Re model was selected, which is a two-equation model and belongs to the family of Local Correlation Based Transition Models. For validation purposes, simulations were performed on two dimensions for two airfoils typically used in the wind power generation industry, as well as a three-dimensional propeller. The results were then compared to experiments available in the literature in order to assess how well the solver captures the complicated phenomenon of transition. The simulation for the two-dimensional airfoils indicated that the results are in good agreement with the experimental ones only for small angles of attack, while in higher angles of attack, the effect of strong three dimensional phenomena lead to discrepancies between the results of the solver and the experimental ones. For the case of the three dimensional propeller, the solver managed to capture the correct slope for the curves on the Open Water Diagram, while a corresponding Fully Turbulent Solver failed to capture them. |
en |
heal.advisorName |
Παπαδάκης, Γεώργιος |
el |
heal.committeeMemberName |
Γρηγορόπουλος, Γρηγόρης |
el |
heal.committeeMemberName |
Τριανταφύλλου, Γεώργιος |
el |
heal.academicPublisher |
Εθνικό Μετσόβιο Πολυτεχνείο. Σχολή Ναυπηγών Μηχανολόγων Μηχανικών. Τομέας Ναυτικής και Θαλάσσιας Υδροδυναμικής. Εργαστήριο Ναυτικής και Θαλάσσιας Υδροδυναμικής |
el |
heal.academicPublisherID |
ntua |
|
heal.numberOfPages |
68 σ. |
el |
heal.fullTextAvailability |
false |
|