Half model testing is considered a valuable wind tunnel technique that offers many benefits over conventional full span testing. The technique suffers from aerodynamic losses due to flow separations on the model surfaces near the model/floor junction. Computational Fluid Dynamics, employing the Spalart-Allmaras turbulence model, and experimental investigations were carried out to evaluate the losses and to investigate the effect of localised suction on the junction flows. The wind tunnel model used was a rectangular and untwisted wing having a NASA LS(1)-0413 cross section and with a physical aspect ratio of 3. Tests were conducted at 10.00 incidence at a Reynolds number of 0.44 x 106. Aerodynamic performance of the wind tunnel half model was obtained by surface flow visualisation and pressure measurements on the wing surface in the junction region. CFD predictions showed significantly large losses compared to the experimental findings and therefore CFD predicted significant influence and benefits of suction. These were seen as elimination of the model surface separation and also recovery of the wing surface pressure distributions. In contrast to this, experiments showed much smaller separation than CFD without suction and applying suction in experiments, showed only a marginal effect on the flow separations, which also further deteriorated the pressure distributions. Future CFD studies on junction flows should be conducted using more advanced turbulence models such as Large Eddy Simulations (LES). In addition, to validate these CFD studies, velocity and turbulence measurements in the wing/floor junction region are also needed.

No description available.

Junction flows originate from the interaction between a fluid moving over a wall with an obstacle mounted on the same surface. Understanding the physics of such flows is of great interest to engineers responsible for the design of systems consisting of wall-body junctions. From aerodynamics to turbomachinery and electronics to bridge hydraulics, a number of phenomena (drag, heat transfer, scouring) are driven by the behavior of the most prominent feature of junction flows: the horseshoe vortex system (HVS). Focusing on turbulent flows, the complex dynamics of the HVS is established through its unsteadiness and non-uniformity. The fundamentals of this dynamically-rich phenomenon have been described within the body of a rapidly-expanding literature. Nevertheless, important aspects remain inadequately understood and call for further scrutiny. This study emphasized three of them, by investigating the effects of: model scale, wall roughness, and bed geometry. High-resolution experiments were carried out using Particle Image Velocimetry (PIV). Statistical analyses, vortex identification schemes, and Proper Orthogonal decomposition were employed to extract additional information from the large PIV datasets. The time-averaged topology of junction flows developing over a smooth and impermeable wall was independent of the flow Reynolds number, Re (parameter that expresses the effects of scale). On the contrary, time-resolved analysis revealed a trend of increasing vorticity, momentum, and eruptions of near-wall fluid with Re. New insights on the modal dynamics of the HVS were also documented in a modified flow mechanism. Wall roughness (modeled with a permeable layer of crushed stones) diffused turbulence and vorticity throughout the domain. This effect manifested with high levels of intermittency and spatial irregularity for the HVS. Energetic flow structures were also identified away from the typical footprint of the HVS. Finally, a novel implementation of PIV allowed for unique velocity measurements over an erodible bed. It was demonstrated that, during the initial stages of scouring, the downflow at the face of the obstacle becomes the dominant flow characteristic in the absence of the HVS. Notwithstanding modeling limitations, the physical insight contributed here could be used to enhance the design of systems with similar flow and geometrical characteristics. / Ph. D.

Local scour around bridge foundations has been recognized as one of the main causes of bridge failures. The objective of this study is to investigate the relationships among field, laboratory, and numerical data for the purpose of improving scour prediction methods for complex bridge piers. In this study, three field sites in Georgia were selected for continuous monitoring and associated laboratory models were fabricated with physical scale ratios that modeled the full river and bridge cross sections to consider the effect of river bathymetry and bridge geometry. Three different sizes of sediment and several geometric scales of the bridge pier models were used in this study to investigate the scaling effect of relative sediment size, which is defined as the ratio of the pier width to the median sediment size. The velocity field for each bridge model was measured by the acoustic Doppler velocimeter (ADV) to explain the complicated hydrodynamics of the flow field around bridge piers as guided by the results from a numerical model. In each physical model with river bathymetry, the comparison between the results of laboratory experiments and the measurements of prototype bridge pier scour showed good agreement for the maximum pier scour depth at the nose of the pier as well as for the velocity distribution upstream of each bridge pier bent. Accepted scour prediction formulae were evaluated by comparison with extensive laboratory and field data. The effect of relative sediment size on the local pier scour depth was examined and a modified relationship between the local pier scour depth and the relative sediment size was presented. A useful methodology for designing physical models was developed to reproduce and predict local scour depth around complex piers considering Froude number similarity, flow intensity, and relative sediment size.

No description available.

Hydraulically induced scour of the streambed at the base of bridge piers is the leading cause of bridge failures. Despite the significant scientific efforts towards the solution of this challenging engineering problem, there are still no reliable tools for the prediction and mitigation of bridge scour. This shortcoming is attributed to the lack of understanding of the physics behind this phenomenon. The experimental studies that attempted the physical investigation of bridge scour in the past have faced two main limitations: i) The characterization of the dynamic interaction between the flow and the evolving bed that is known to drive scour, was not possible due to the limitations in the available instrumentation and the significant experimental difficulties; ii) Most of the existing literature studies are based on the findings of laboratory experiments whose scale is orders of magnitudes smaller compared to bridges in the field, while the scale effects on the scour depth have never been quantified. The objective of this research was to enhance the existing understanding of the phenomenon by tackling the aforementioned experimental challenges. To accomplish this, the first part of this work involved the development of a new underwater photogrammetric technique for the monitoring of evolving sediment beds. This technique is able to obtain very high resolution measurements of evolving beds, thus allowing the characterization of their dynamic properties (i.e. evolving topography and scour rates) and overcoming existing experimental limitations. Secondly, the underwater photogrammetric technique was applied on a bridge scour experiment, of simple geometry, and the dynamic morphological characteristics of the phenomenon were measured. The detailed measurements along with reasonable comparisons with descriptions of the flow, from past studies, were used to provide insight on the interaction between the flow and the bed and describe quantitatively the mechanisms of scour. Finally, the scale effects on scour were studied via the performance of two experiments under near-prototype conditions. In these experiments the effects of the Reynolds number on the flow and the scour were quantified and implications concerning existing small-scale studies were discussed. / Ph. D.

This research work investigates the thermal performance of a film-cooled gas turbine endwall under two different mainstream flow conditions. In the first part of the research investigation, the effect of unsteady passing wakes on a film-cooled pitchwise-curved surface (representing an endwall without airfoils) was experimentally studied for heat transfer characteristics on a time-averaged basis. The temperature sensitive paint technique was used to obtain the local temperatures on the test surface. The required heat flux input was provided using foil heaters. Discrete film injection was implemented on the test surface using cylindrical holes with a streamwise inclination angle of 35? and no compound angle relative to the mean approach velocity vector. The passing wakes increased the heat transfer coefficients at both the wake passing frequencies that were experimented. Due to the increasing film cooling jet turbulence and strong jet-mainstream interaction at higher blowing ratios, the heat transfer coefficients were amplified. A combination of film injection and unsteady passing wakes resulted in a maximum pitch-averaged and centerline heat transfer augmentation of ? 28% and 31.7% relative to the no wake and no film injection case. The second part of the research study involves an experimental and numerical analysis of secondary flow and coolant film interaction in a high subsonic annular cascade with a maximum isentropic throat Mach number of ? 0.68. Endwall (platform) thermal protection is provided using discrete cylindrical holes with a streamwise inclination angle of 30? and no compound angle relative to the mean approach velocity vector. The surface flow visualization on the inner endwall provided the location of the saddle point and the three-dimensional separation lines. Computational predictions showed that the leading-edge horseshoe vortex was confined to approximately 1.5% of the airfoil span for the no film injection case and intensified with low momentum film injection. At the highest blowing ratio, the film cooling jet weakened the horseshoe vortex at the leading-edge plane. The passage vortex was intensified with coolant injection at all blowing ratios. It was seen that increasing average blowing ratio improved the film effectiveness on the endwall. The discharge coefficients calculated for each film cooling hole indicated significant non-uniformity in the coolant discharge at lower blowing ratios and the strong dependence of discharge coefficients on the mainstream static pressure and the location of three-dimensional separation lines. Near the airfoil suction side, a region of coalesced film cooling jets providing close to uniform film coverage was observed, indicative of the mainstream acceleration and the influence of three-dimensional separation lines.

Η θερμοδυναμική ανάλυση του κύκλου Brayton υποδεικνύει ότι η θερμική απόδοση και το ειδικό έργο εξόδου ενός αεριοστρόβιλου μπορούν να βελτιωθούν με την αύξηση της θερμοκρασίας εισόδου των αεριών της καύσης στον στρόβιλο. Επιπλέον, οι αυξημένες θερμοκρασίες εισόδου στον στρόβιλο συνοδεύονται και από μείωση της κατανάλωσης καυσίμου, ενώ σε αεροπορικές εφαρμογές οι υψηλότερες θερμοκρασίες έχουν ώς αποτέλεσμα την αύξηση της ώσης του κινητήρα. Δυστυχώς όμως, οι υψηλές αυτές θερμοκρασίες θέτουν σε κίνδυνο την ακεραιότητα των εξαρτημάτων του στροβίλου υψηλής πίεσης και ειδικότερα τα πτερύγια (blades) του στροβίλου και το δάπεδο (endwall) στο οποίο τα πτερύγια αυτά είναι προσκολλημένα. Στους μοντέρνους κινητήρες, η θερμοκρασία εισόδου στον στρόβιλο μπορεί να φτάνει και στα επίπεδα των 1900Κ, θερμοκρασία η οποία υπερβαίνει το σημείο τήξης των υλικών από τα οποία είναι κατασκευασμένα τα εξαρτήματα του στροβίλου. Αυτό έχει ως αποτέλεσμα τα εξαρτήματα του στροβίλου να λειτουργούν σε πολύ σκληρότερο περιβάλλον απ' ότι στο παρελθόν. Η διατήρηση επαρκούς διάρκειας ζωής στις υψηλές αυτές θερμοκρασίες απαιτεί την ανάπτυξη νέων υλικών κατασκευής και αποτελεσματικών μεθόδων ψύξης για τα εξαρτήματα του στροβίλου. Για την αντιμετώπιση και την αποφυγή της αστοχίας των πτερυγίων (blades) και των δάπεδων (endwall) των πτερυγικών διακένων στους στροβίλους, η μέθοδος του "film cooling" έχει ενσωματωθεί στον σχεδιασμό τους. Κατά την διεργασία της ψύξης των εξαρτημάτων με την μέθοδο αυτή, ψυχρός αέρας αφαιμάσσεται από το στάδιο του συμπιεστή, διοχετεύεται μέσω εσωτερικών θαλάμων του κινητήρα στα εξαρτήματα του στροβίλου και εγχέεται μέσω διακριτών οπών στα τοιχώματα των πτερυγίων και των δαπεδικών τοιχωμάτων. Μετά την έξοδο του από τις οπές, ο ψυκτικός αέρας σχηματίζει ένα λεπτό, προστατευτικό στρώμα-φιλμ μεταξύ των θερμών αερίων της καύσης και της μεταλλικής επιφάνειας των εξαρτημάτων. Μια εκ των κρίσιμων περιοχών οι οποίες υποβάλλονται σε αυξημένους ρυθμούς μετάδοσης θερμότητας είναι και η περιοχή γύρω από την περιφέρεια σύνδεσης των πτερυγίων (blades) με τα δάπεδα (endwalls) του στροβίλου. Η περιοχή αυτή κυριαρχείται από την παρουσία ισχυρών τρισδιάστατων δευτερογενών ροών (γνωστές και ώς junction flows) οι οποίες προκαλούν αύξηση των τοπικών ρυθμών μετάδοσης θερμότητας στην περιοχή της τάξης του 350%. Επιπλέον, οι ροές αυτές, εμποδίζουν την διείσδυση ψυκτικού ρευστού στην προβληματική περιοχή εκτοπίζοντας το μακριά από την επιφάνεια του δαπέδου πριν αυτό προλάβει να παράσχει ικανοποιητική ψύξη. Αντικείμενο της παρούσας διδακτορικής διατριβής, είναι η μελέτη, ανάπτυξη και δοκιμή (τόσο πειραματικά όσο και υπολογιστικά) μιας πρωτότυπης γεωμετρίας ψύξης (με την μέθοδο του film cooling), για την αποτελεσματική αντιμετώπιση του προβλήματος της υπερθέρμανσης της περιοχής σύνδεσης του πτερυγίου – δαπέδου κυρίως γύρω από το επίπεδο του χείλους προσβολής. Το κύριο χαρακτηριστικό της πρωτότυπης μεθόδου έγχυσης είναι ότι το ψυκτικό εκχέεται κατά τέτοιο τρόπο έτσι ώστε οι ροϊκές γραμμές του ψυκτικού να υποβοηθούνται από την περιστροφική κίνηση των τοπικών τρισδιάστατων ροών. Η πολυπλοκότητα του προβλήματος ψύξης της συγκεκριμένης περιοχής προκύπτει από δύο στοιχεία. Πρώτον, όπως αναφέρθηκε και προηγουμένως, η ροή στην περιοχή σύνδεσης κοντά στο τοίχωμα χαρακτηρίζεται από πολύπλοκη τρισδιάστατη δομή. Δεύτερον, το πρόβλημα χαρακτηρίζεται από τρείς θερμοκρασίες: την θερμοκρασία της κύριας ροής, την θερμοκρασία του τοιχώματος και την θερμοκρασία του ψυκτικού αέρα. Για την πλήρη διερεύνηση των χαρακτηριστικών της προτεινόμενης μεθόδου ψύξης η εργασία περιλαμβάνει τόσο πειραματικό όσο και υπολογιστικό σκέλος: Υπολογιστικό Σκέλος (Computational part): Ο επιτυχής σχεδιασμός μιας πιθανής γεωμετρίας ψύξης για την συγκεκριμένη περιοχή του δαπέδου (endwall) απαιτεί την γνώση και κατανόηση της τοπικής ροής μέσα στην οποία το τζετ του ψυκτικού πρόκειται να εισέλθει. Επιπλέον, είναι σημαντική η κατανόηση της αλληλεπίδρασης που αναμένεται μεταξύ του ψυκτικού αέρα με την τοπική τρισδιάστατη ροή. Για τον σκοπό αυτό, χρησιμοποιήθηκε η μέθοδος της υπολογιστικής ρευστοδυναμικής (Computational Fluid Dynamics) για την πρόβλεψη του σχετικού τρισδιάστατου βασικού πεδίου ροής στην περιοχή σύνδεσης του πτερυγίου (blade) - δαπέδου (endwall). Έγιναν προσομοιώσεις τόσο για την βασική γεωμετρία απουσία έγχυσης (οι οποίες χρησιμοποιήθηκαν ως πεδίο αναφοράς) όσο και προσομοιώσεις παρουσία της πρωτότυπης έγχυσης οι οποίες αφορούσαν την επίδραση διαφόρων παραμέτρων στην αποτελεσματικότητα της ψύξης της προβληματικής περιοχής. Στις προσομοιώσεις υιοθετήθηκε η εξής θερμοκρασιακή κατανομή: Θερμό δάπεδο (endwall) - Θερμότερη κύρια ροή (mainstream) - Ψυχρός αέρας έγχυσης, η οποία είναι και αντίστοιχη με αυτήν που εμφανίζεται σε πραγματικές εφαρμογές. Τα αποτελέσματα των προσομοιώσεων βοήθησαν στην κατανόηση του ροϊκού πεδίου στην περιοχή σύνδεσης τόσο ποιοτικά όσο και ποσοτικά σε ότι αφορά τα σχετικά μεγέθη των ροϊκών δομών και των αεροδυναμικών χαρακτηριστικών τις περιοχής. Αυτό είχε ώς αποτέλεσμα τον αποτελεσματικό σχεδιασμό της πρωτότυπης γεωμετρίας έγχυσης. Επιπλέον, οι υπολογιστικές προβλέψεις ήταν πολύ βοηθητικές προς την κατεύθυνση κατανόησης και ερμηνείας των πειραματικών αποτελεσμάτων, αφού παρείχαν την δυνατότητα συσχέτισης της προκύπτουσας κατανομής της θερμοκρασίας στο δάπεδο (endwall) με τις τοπικές τρισδιάστατες ροές. Πειραματικό Σκέλος (Experimental part): Για την πειραματική διερεύνηση της αποτελεσματικότητας της προτεινόμενης μεθόδου ψύξης, χρησιμοποιήθηκε μια νέα τεχνική η οποία αναπτύχθηκε ως μέρος της παρούσας εργασίας, υιοθετώντας θερμοκρασιακή κατανομή αντίστροφη από αυτήν που χρησιμοποιήθηκε για τις υπολογιστικές προβλέψεις, π.χ. Ψυχρή κύρια ροή (mainstream) - Θερμό πλαϊνό τοίχωμα (endwall) - Θερμότερος αέρας έγχυσης. Χρησιμοποιώντας την μέθοδο αυτή και με την χρήση υπέρυθρης θερμογραφίας (infrared thermography), ποσοτικοποιείται η αποτελεσματικότητα στην ψύξη του πλαϊνού τοιχώματος και προσδιορίζεται η περιοχή στην οποία η ψύξη είναι αποτελεσματική. Επιπλέον της ποιοτικής και ποσοτικής αποτίμησης της αποτελεσματικότητας της ψύξης, ήταν αναγκαίες αεροδυναμικές μετρήσεις για τον καθορισμό του αεροδυναμικού κόστους της προτεινόμενης μεθόδου ψύξης. Οι μετρήσεις αυτές, δίνουν μια ένδειξη του κατά πόσον η μέθοδος επηρεάζει την μεγέθυνση και ένταση των δευτερογενών ροών (π.χ. δίνη διακένου (passage vortex)) στην περιοχή κατάντη της ζώνης αλληλεπίδρασης του ψυκτικού τζετ με την τοπική τρισδιάστατη ροή. / The thermodynamic analysis of the Brayton cycle designates that the thermal efficiency and the specific work output of a Gas Turbine can be improved by increasing the Turbine Inlet Temperatures. Furthermore, increment of the turbine inlet temperatures also results into lower fuel consumption rates, while, if the gas turbine is meant for propulsion purposes, increment of the turbine inlet temperatures also results into increased engine thrust. Unfortunately, these high gas temperatures jeopardize the integrity of the high pressure turbine components and more particular, the turbine blades and the endwall on which the blades are attached. In modern turbines, the turbine inlet temperature may reach the level of 1900K, exceeding by far the melting temperature of the metal walls. As a result, the turbine components operate at much harsher environments than in the past. Maintaining adequate life in these high temperatures requires the development of new materials and manufacturing processes, as well as efficient cooling methods for the components of the turbine. In order to address and avoid the failure of the blades and endwall of a turbine cascade, the method of "film cooling" has been incorporated as part of the components design process. In the latter method, air is bled from the compressor stage, passed through internal chambers of the engine to the turbine components and is injected through discrete holes in the walls of the blades and the endwall, forming a thin protective layer film between the hot combustion gases and the metal surfaces of the parts. A critical region that is subjected into increased thermal stresses is the area around the leading edge - endwall juncture, which is inherently dominated by the presence of strong three dimensional secondary flows (also known as juncture flows) responsible for the increment of the local heat transfer rates to the order of 350%. Moreover, these flows, prevent the penetration of the fluid in the problematic area, displacing the coolant mass flux away from the surface of the endwall before providing adequate cooling. The subject of the current thesis, is the design, development and testing (both experimental and computational) of a prototype cooling scheme (with the method of film cooling), in order to effectively address the endwall overheating problem around the leading edge - endwall juncture, especially around the stagnation plane area. The main feature of the novel injection method is that the coolant air is ejected in such a way that the cooling effectiveness in the area is assisted by the rotational sense of local three-dimensional flows. The complexity of film cooling for the problematic area arises from two facts. Firstly, as mentioned previously the flow around the leading edge junction is characterized by complex three dimensional flows. Secondly, the problem is characterized by three temperatures: the temperature of the main flow, the endwall temperature and the temperature of the coolant air. In order to fully investigate the features and characteristics of the proposed cooling method, the work of the current thesis includes both, an experimental and a computational part: Computational part: The successful design of a possible cooling scheme for the particular region of the endwall requires the knowledge and understanding of local flow in which the coolant jet is to be entrained. Furthermore, it is important to understand the expected interaction between the coolant air and the local three-dimensional flow. For this purpose, the method of Computational Fluid Dynamics was employed for predicting the relevant three-dimensional flow field around the blade-endwall junction area. Simulations were made for both, the basic geometry in the absence of any coolant injection (which were used as a reference point) and simulations during the employment of the proposed coolant injection method which concerned the effect of various parameters on the cooling efficiency of the problematic area. For the simulations, the following temperature step was adopted: Warm endwall - Warmer main flow (mainstream) - Cold air injection, which is similar to that seen in real applications. The CFD predictions were very helpful towards understanding the relevant flow field in the junction area, both qualitatively and quantitatively in terms of the relative magnitudes of the flow structures and the aerodynamic characteristics of the flow in the region. Experimental part: For the experimental investigation regarding the effectiveness of the proposed cooling method, a new experimental technique was employed which was developed as part of the current thesis. In the latter technique, a reversed temperature step is adopted (when compared to the relevant temperature step adopted for the numerical simulations), e.g. Cold main flow (mainstream) - Warm endwall - Warmer air injection. Along with the use of infrared thermography, the endwall film cooling effectiveness is quantified and the region that the injection is effective is determined. In addition to the qualitative and quantitative evaluation of the cooling effectiveness, extensive aerodynamic measurements were necessary in order to evaluate the aerodynamic costs of the proposed cooling method. These measurements provide an indication of whether the cooling process affects the growth and intensity of secondary flows (e.g. passage vortex) in the region downstream of the coolant jet-local three-dimensional flow interaction.

No description available.