AGAndrea Del Gaudio

Andrea Del Gaudio

*This is an algorithmically generated author record based on publicly available information.

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Andrea Del Gaudio has a total of 20 co-authors. Here are the top co-authors by number of shared publications:


Latest Publications

  • Open Access

    Drag forces and flow structure around and inside a square array of emerged cylinders in an open channel

    by Andrea Del Gaudio, George Constantinescu, Francesco De Paola

    Eddy resolving simulations are used to describe the mean flow and turbulence structure inside and around a square array of width D containing emerged (i.e., cylinder extending up, or above, the free surface), rigid cylinders of width d . The array is placed at the centre of a long open channel of width W . The study describes how the structure of the wake and shear layers forming along the lateral sides of the array, the wake spectral content and shedding modes, the bleeding velocity, the lengths of the steady and total wake regions, the coherence of the horseshoe vortices forming around the frontal face of the array, the bed shear stresses and the sediment entrainment capacity of the flow inside and outside the array change with the main geometrical parameters defining the array (i.e. the solid volume fraction, SVF, the non-dimensional frontal area per unit volume of the array, italic aD aD $\textit{aD}$ , the shape of the cylinders and d divided by upper D d / D $d/D$ ) and the blockage ratio, upper W divided by upper D W / D $W/D$ . The effects of varying the same geometrical parameters on the total non-dimensional streamwise drag force acting on the array and on the streamwise distribution of the drag force inside the array are quantified. The mean flow and turbulence inside the array are analysed based on the streamwise distributions of the double-averaged (i.e. over time, D and the flow depth, H ) streamwise velocity, upper U overbar overbar U ¯ ¯ $\overline{\overline{U}}$ , and turbulent kinetic energy. Contrary to wakes generated behind circular arrays of emerged cylinders, several streamwise-oriented vortices are generated inside the wake of square arrays for a limited range of italic aD aD $\textit{aD}$ . These vortices increase flow three-dimensionality and vertical transport behind square arrays. Despite the relatively large values of the array and channel Reynolds numbers (i.e. Re D = 40 000, Re H = 14 000), the mean (time and spanwise-averaged) cylinder drag coefficient, upper C prime Subscript d C d ′ ${C}_{d}^{\prime}$ ( x ), defined with d , H and upper U overbar overbar U ¯ ¯ $\overline{\overline{U}}$ is not close to constant over the whole length of the array in some of the dense array simulations. In these cases, upper C prime Subscript d C d ′ ${C}_{d}^{\prime}$ starts increasing monotonically over the downstream part of the array, as the flow transitions from the quadratic drag regime to the linear drag regime. When plotted versus the cylinder Reynolds number ModifyingAbove italic Re Subscript d Baseline With bar equals upper U overbar overbar d slash Re d ¯ = U ¯ ¯ d / $\overline{\textit{Re}_{d}} = \overline{\overline{U}}d/$ ν ( ν is the viscosity), upper C prime Subscript d C d ′ ${C}_{d}^{\prime}$ = 2 α 0 / ModifyingAbove italic Re Subscript d Baseline With bar Re d ¯ $\overline{\textit{Re}_{d}}$ over the linear drag regime. The parameter α 0 and the critical value of ModifyingAbove italic Re Subscript d Baseline With bar Re d ¯ $\overline{\textit{Re}_{d}}$ corresponding to the start of the linear drag regime are strongly influenced by the main geometrical parameters of the array and the blockage ratio. Simulation results show that the close-to-constant value of the cylinder drag coefficient characterising the quadratic drag regime, upper C prime Subscript d Baseline overbar comma C d ′ ¯ , $\overline{{C}_{d}^{\prime}},$ increases with italic SVF SVF $\textit{SVF}$ and italic aD aD $\textit{aD}$ for constant d divided by upper D d / D $d/D$ , cylinder shape and upper W divided by upper D W / D $W/D$ . Moreover, upper C prime Subscript d Baseline overbar C d ′ ¯ $\overline{{C}_{d}^{\prime}}$ increases with d divided by upper D d / D $d/D$ for constant italic aD aD $\textit{aD}$ , cylinder shape and upper W divided by upper D W / D $W/D$ , and decreases with upper W divided by upper D W / D $W/D$ for constant italic aD aD $\textit{aD}$ , cylinder shape and d divided by upper D d / ...

  • Influence of emergent and submerged plants on local hydrodynamics and turbulence anisotropy in vegetated rivers

    by Giuseppe Francesco Cesare Lama, Andrea Del Gaudio, Jyotirmoy Barman, Anurag Handique, Francesco De Paola, Giovanni Battista Chirico, Donatella Termini

  • Detached Eddy Simulation Model to Evaluate Design of Pump Stations

    by Andrea Del Gaudio, George Constantinescu, Francesco De Paola, Jie Zeng, Matahel Ansar


  • Open Access

    Turbulent dam-break waves of Newtonian and non-Newtonian fluids

    by Andrea Del Gaudio, George Constantinescu, Francesco De Paola, Cristiana Di Cristo, Andrea Vacca

    The paper uses three-dimensional large eddy simulation (LES) to investigate the structure and propagation of dam break waves of non-Newtonian fluids described by a power-law rheology. Simulations are also conducted for the limiting case of a dam-break wave of Newtonian fluid (water). Turbulent dam-break waves are found to have a two-layer structure and to generate velocity streaks beneath the region in which the flow is strongly turbulent and lobes at the front. The bottom part of the wave resembles a boundary layer and contains a log-law sublayer, while the streamwise velocity is close to constant inside the top layer. The value of the von Kármán constant is found to reach the standard value (i.e. $\kappa$ ≈ 0.4) associated with turbulent boundary layers of Newtonian fluids only inside the strongly turbulent region near the front of Newtonian dam-break waves. Much higher values of the slope of the log law are predicted for non-Newtonian dam-break waves (i.e. $\kappa$ ≈ 0.28) and in the regions of weak turbulence of Newtonian waves. LES shows that a power-law relationship can well describe the temporal evolution of the front position during the acceleration and deceleration phases, and that increasing the shear-thinning behaviour of the fluid increases the speed of the front. The numerical experiments are then used to investigate the predictive abilities of shallow water equation (SWE) models. The paper also proposes a novel one-dimensional (1-D) SWE model which accounts for the bottom friction by employing a friction coefficient regression valid for power-law fluids in the turbulent regime. An analytical approximate solution is provided by splitting the current into an outer region, where the flow is considered inviscid and friction is neglected, and an inner turbulent flow region, close to the wave front. The SWE numerical and analytical solutions using a turbulent friction factor are found to be in better agreement with LES compared with the agreement shown by an SWE numerical model using a laminar friction coefficient. The paper shows that inclusion of turbulence effects in SWE models used to predict high-Reynolds-number Newtonian and non-Newtonian dam break flows results is more accurate predictions.


  • Dam-Break waves over mobile bed

    by Andrea Del Gaudio, Giovanni La Forgia, Francesco De Paola, Cristiana Di Cristo, Michele Iervolino, Angelo Leopardi, Andrea Vacca


  • Large eddy simulation of power-law fluid dam break wave impacting against a vertical wall

    by Andrea Del Gaudio, George Constantinescu, Cristiana Di Cristo, Francesco De Paola, Andrea Vacca

    The study investigates the evolution of a dam break wave of a mixture of clay and water in turbulent flow conditions and its interaction with a vertical rigid wall. The phenomenon reproduction, important for planning risk mitigation strategies and designing protective structures, is performed by means of three-dimensional large eddy simulations. The dynamical Smagorinsky model is employed and the volume-of-fluid technique is used to calculate the free surface evolution with time. A power-law model is considered to represent the mixture rheology. With reference to a small-scale setup, the paper analyzes the influence of the clay concentration and of initial fluid depth upstream of the lock gate on the temporal evolution of the front, the bed shear stresses, and the force acting on the vertical endwall. Moreover, the presence of three-dimensional effects and the turbulence role are also investigated. The occurrence of scale effects for the non-Newtonian dam break wave is finally examined by performing an additional test with a larger-scale setup. Results indicate that lobelike structures develop near the front of the current and near-bed streaks of low and high velocity are present behind the front. The variation of the wave front position with time is described by a power-law function, independently of both clay concentration and initial fluid depth. Over the body of the current, the nondimensional bed shear stress values in the simulations performed with non-Newtonian fluids are about two times larger than the ones in the clear water case. Moreover, the peak value of the nondimensional impact force, slightly lower than the one in clear water, decreases when clay concentration is increased. Comparing large- and small-scale tests, higher nondimensional propagation speeds and bed shear stress values in the front region are observed in the former one. Conversely, the nondimensional peak force is not affected by scale effects, suggesting that small-scale tests can be used to provide reliable predictions of this critical variable for engineering design.


  • Open Access

    Modelling the impact of a dam‐break wave on a vertical wall

    by Andrea Del Gaudio, Giovanni La Forgia, George Constantinescu, Francesco De Paola, Cristiana Di Cristo, Michele Iervolino, Angelo Leopardi, Andrea Vacca

    Summary: Dam‐Break waves arise from the sudden release of the water stored behind a wall, and they cause destruction and losses on nearby areas. Characterisation of the impact force on obstacles is very important for risk assessment. In this work, we performed a series of lock‐release experiments to evaluate the wave‐induced impact force on a vertical end wall situated some distance from the lock. Laboratory data were used to evaluate the performance of several types of numerical models to predict the wave‐induced force on the vertical end wall. The selected models were as follows: the hydrostatic 1D De Saint‐Venant model, the multi‐layer hydrostatic model and the Navier–Stokes two‐phase flow. For the latter two models, both 2D (in the ‐ plane) and 3D simulations were performed. The results show that, independently of the hydrostatic assumption, the 2‐D simulations generate nonphysical oscillations which are not present in the measured temporal histories of the pressure and force values. By contrast, the predictions of both 3D numerical models better reproduce the temporal variation of the pressure forces on the end wall. The present study also shows that from a practical point of view, the 1D De Saint‐Venant model predicts with sufficient accuracy the impact time and the magnitude of the peak value of the impact force. Therefore, if the use of a fully 3D models is not a feasible option, in terms of a trade‐off between computation cost and accuracy, the use of a simple hydrostatic 1D De Saint‐Venant model is preferable to a 2D model.


  • Open Access

    Experimental Investigation and Numerical Evaluation of the Free Surface of a Dam Break Wave in the Presence of an Obstacle

    by Andrea Del Gaudio, Francesco De Paola, Cristiana Di Cristo, Giovanni La Forgia, Angelo Leopardi, Andrea Vacca

    Tsunamis, impulse waves, and dam break waves have a high impact on nearby areas. Scaled experiments allow us to deeply understand the hydrodynamic features of these unsteady flows and, equally, to validate numerical models. The study shows the experimental set-up and the preliminary results of the tests performed at the Hydraulic Engineering Laboratory of the University of Naples “Federico II”. We set up a 3 m long Perspex tank in order to generate dam break waves by a pneumatic gate removal. Two high-speed CCD (charge-coupled device) cameras were used to characterize the wavefront celerity and the free surface profile. Five pressure transducers were installed on a vertical wall, located at the end of the channel, in order to sample the force extent of the surge. The results of the numerical simulations realized through the depth-integrated model were compared with experimental data.