Eduard Egusquiza

Prof. Eduard Egusquiza


Research Focus & Metrics

Academic Career Length

34Years (1993-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 May 2006 in Mechanical Systems and Signal Processing
Verified
Journal Article
Closed access
Xavier EscalerXavier Escaler
Xavier Escaler
EEEduard Egusquiza
Eduard Egusquiza
MFMohamed Farhat
Mohamed Farhat
FAFrançois Avellan
François Avellan
MCMiguel Coussirat
Miguel Coussirat

1 July 2012 in Engineering Failure Analysis
Verified
Journal Article
Open access
EEEduard Egusquiza
Eduard Egusquiza
CVCarme Valero
Carme Valero
Xingxing HuangXingxing Huang
Xingxing Huang
EJEsteve Jou
Esteve Jou
Alfredo GuardoAlfredo Guardo
Alfredo Guardo
Cristian RodriguezCristian Rodriguez
Cristian Rodriguez

26 May 2007 in Journal of Fluids Engineering
Verified
Journal Article
Closed access
PDF file
Cristian RodriguezCristian Rodriguez
Cristian Rodriguez
EEEduard Egusquiza
Eduard Egusquiza
ISIlmar Santos
Ilmar Santos
The highest vibration levels in large pump turbines are, in general, originated in the rotor stator interaction (RSI). This vibration has specific characteristics that can be clearly observed in the frequency domain: harmonics of the moving blade passing frequency and a particular relationship among their amplitudes. It is valuable for the design and condition monitoring to count on these characteristics. A CFD model is an appropriate tool to determine the force and its characteristics. However, it is time consuming and needs highly qualified human resources while usually these results are needed immediately and in situ. Then, it is useful to determine these characteristics in a simple, quick, and accurate method. At present, the most suitable method indicates a large amount of possible harmonics to appear, without indicating the relative importance of them. This paper carries out a theoretical analysis to predict and explain in a qualitative way these frequencies and amplitudes. The theoretical analysis incorporates the number of blades, the number of guide vanes, the RSI nonuniform fluid force, and the sequence of interaction. This analysis is compared with the method currently in use, and both methods are applied to a practical case. The theoretical analysis gives a resulting force over the pump turbine, which corresponds well to the measured behavior of a pump turbine in terms of its frequencies and the relationship between their amplitudes. A corrective action is proposed as a result of the analysis and after it is carried out in one of the units, the vibration levels are reduced. The vibration induced by the RSI is predicted considering the sequence of interaction and different amplitudes in the interactions between the same moving blade and different stationary blades, giving a different and original interpretation about the source of the vibration characteristics. A successful corrective action is proposed as a consequence of this new interpretation.

1 March 2005 in Chemical Engineering Science
Verified
Journal Article
Closed access
Alfredo GuardoAlfredo Guardo
Alfredo Guardo
MCM. Coussirat
M. Coussirat
MLM.A. Larrayoz
M.A. Larrayoz
FRF. Recasens
F. Recasens
EEEduard Egusquiza
Eduard Egusquiza

16 March 2007 in Journal of Fluids Engineering
Verified
Journal Article
Closed access
PDF file
PAPhilippe Ausoni
Philippe Ausoni
MFMohamed Farhat
Mohamed Farhat
Xavier EscalerXavier Escaler
Xavier Escaler
EEEduard Egusquiza
Eduard Egusquiza
FAFrançois Avellan
François Avellan
The present study deals with the shedding process of the von Kármán vortices at the trailing edge of a 2D hydrofoil at high Reynolds number Reh=25×103–65×103. This research focuses mainly on the effects of cavitation and fluid-structure interaction on the mechanism of the vortex generation. The vortex shedding frequency, derived from the flow-induced vibration measurement, is found to follow the Strouhal law provided that no hydrofoil resonance frequencies are excited, i.e., lock-off. For such a regime, the von Kármán vortices exhibit strong spanwise 3D instabilities and the cavitation inception index is linearly dependent on the square root of the Reynolds number. In the case of resonance, the vortex shedding frequency is locked onto the hydrofoil eigenfrequency and the spatial coherence is enhanced with a quasi-2D shape. The measurements of the hydrofoil wall velocity amplitude and phase reveal the first torsion eigenmotion. In this case, the cavitation inception index is found to be significantly increased compared to lock-off conditions. It makes clear that the vortex roll-up is amplified by the phase locked vibrations of the trailing edge. For the cavitation inception index, a new correlation relationship that encompasses the entire range of Reynolds numbers, including both the lock-off and the lock-in cases, is proposed and validated. In contrast to the earlier models, the new correlation takes into account the trailing edge displacement velocity. In addition, it is found that the transverse velocity of the trailing edge increases the vortex strength linearly. This effect is important in the context of the fluid-structure interaction, since it implies that the velocity of the hydrofoil trailing edge increases the fluctuating forces on the body. It is also demonstrated that cavitation developing in the vortex street cannot be considered as a passive agent for the turbulent wake flow. In fact, for fully developed cavitation, the vortex shedding frequency increases up to 15%, which is accompanied by the increase of the vortex advection velocity and reduction of the streamwise vortex spacing. In addition, a significant increase of the vortex-induced vibration level is found at cavitation onset. These effects are addressed and thought to be a result of the increase of the vorticity by cavitation.

1 July 2007 in Computers & Fluids
Verified
Journal Article
Closed access
QLQ.W. Liang
Q.W. Liang
Cristian RodriguezCristian Rodriguez
Cristian Rodriguez
EEEduard Egusquiza
Eduard Egusquiza
Xavier EscalerXavier Escaler
Xavier Escaler
MFM. Farhat
M. Farhat
FAFrançois Avellan
François Avellan