GV

Guilherme Vaz

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8 records found

Journal article (2022) - Maarten Klapwijk, Thomas Lloyd, Guilherme Vaz
A new partially averaged Navier-Stokes (PANS) closure is derived based on the k-kL (KSKL) model. The aim of this new model is to incorporate the desirable features of the KSKL model, compared to the k-ω shear stress transport model, into the PANS framework. These features include reduced eddy-viscosity levels, a lower dependency on the cell height at the wall, well-defined boundary conditions, and improved iterative convergence. As well as the new model derivation, the paper demonstrates that these desirable features are indeed maintained, for a range of modeled-to-total turbulence kinetic energy ratios (fk), and even for multiphase flow. ...
Journal article (2022) - Manuel Rentschler, Pranav Chandramouli, Guilherme Vaz, Axelle Viré, Rodolfo T. Gonçalves
With the advancement of high-performance computation capabilities in recent years, high-fidelity modelling tools such as computational fluid dynamics are becoming increasingly popular in the offshore renewable sector. To justify the credibility of the numerical simulations, thorough verification and validation is essential. In this work, preparatory heave decay tests for a freely floating single cylinder are modelled. Subsequently, the surge and sway decays of a linearly moored floating offshore wind turbine model of the OC4 (Offshore Code Comparison Collaboration Continuation) phase II semi-submersible platform are simulated. Two different viscous-flow CFD codes are used: OpenFOAM (open-source), and ReFRESCO (community-based open-usage). Their results are compared against each other and with water tank experiments. For the single-cylinder decay simulations, it is found that the natural period is accurately modelled compared to the experimental results. Regarding the damping, both CFD codes are overly dissipative. Differences and their potential explanations become apparent in the analysis of the flow field data. Meanwhile, large numerical uncertainties especially in later oscillations make a distinct conclusion difficult. For the OC4 semi-submersible decay simulations, a better agreement in damping can be achieved, however discrepancies in results are observed when restricting the degrees of freedom of the platform. Flow field data again reveals differences between the CFD codes. Meanwhile, through the effort to use similar numerical settings and quantify the numerical uncertainties of the CFD simulations, this work represents a stepping stone towards fairer and more accurate comparison between CFD and experimental results. ...
Journal article (2021) - S.L. Lovato, Serge Leon Toxopeus, Just W. Settels, G.H. Keetels, Guilherme Vaz
The presence of complex fluids in nature and industrial applications combined with the rapid growth of computer power over the past decades has led to an increasing number of numerical studies of non-Newtonian flows. In most cases, non-Newtonian models can be implemented in existing Newtonian solvers by relatively simple modifications of the viscosity. However, due to the scarcity of analytical solutions for non-Newtonian fluid flows and the widespread use of regularization methods, performing rigorous code verification is a challenging task. The method of manufactured solutions (MMS) is a powerful tool to generate analytical solutions for code verification. In this article, we present and discuss the results of three verification exercises based on MMS: (i) steady single-phase flow; (ii) unsteady two-phase flow with a smooth interface; (iii) unsteady two-phase flow with a free surface. The first and second exercises showed that rigorous verification of non-Newtonian fluid solvers is possible both on single- and two-phase flows. The third exercise revealed that “spurious velocities” typical of free-surface calculations with the Volume-of-Fluid model lead to “spurious viscosities” in the non-Newtonian fluid. The procedure is illustrated herein on a second-order finite volume flow solver, using the regularized Herschel-Bulkley fluid model as an example. The same methodology is however applicable to any flow solver and to all the rheological models falling under the class of generalized Newtonian fluid models. ...
Journal article (2021) - Rens Liebrand, Maarten Klapwijk, Thomas Lloyd, Guilherme Vaz
This study evaluates the influence of transition and turbulence modeling on the prediction of wetted and cavitating tip vortices for an elliptical wing, while investigating the numerical errors. Transition modeling increases the quality of numerical predictions since the assumption of a fully turbulent boundary layer, commonly found in literature, contributes to underprediction of the tip vortex cavity size. By applying the local correlation-based transition model (LCTM) and controlling the boundary layer thickness using different turbulent inflow conditions, the pressure in the vortex was found to reduce by 20% for an Angle of Attack (AoA) of 5 deg. The consequent increase in cavity size was found to be of a similar order of magnitude. At 9 deg AoA, transition always occurs just downstream of the leading edge, making this AoA more suitable to investigate the effect of different turbulence modeling approaches. Azimuthal and axial velocity fields are validated against stereographic-particle image velocimetry (S-PIV) measurements. The time-averaged velocity profiles predicted by delayed detached-eddy simulation (DDES) and improved delayed detached-eddy simulation (IDDES) are close to the experiments; however, no velocity fluctuations and vortex dynamics are observed around the vortex. A comparison of wetted and cavitating simulations shows that the cavity leads to a change in the balance between production and destruction of turbulence kinetic energy, which reduces the turbulent diffusion in and around the cavity compared to wetted flow conditions. Consequently, the vapor flow exhibits the characteristics of a potential flow. Whether this is physically plausible remains to be investigated. ...

Low versus high Reynolds number approach

Conference paper (2019) - Maarten Klapwijk, Thomas Lloyd, Guilherme Vaz, T.J.C. van Terwisga
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Conference paper (2019) - Rens Liebrand, Maarten Klapwijk, Thomas Lloyd, Guilherme Vaz, Rui Lopes
A sensitivity analysis of the transitional flow over a NACA662 - 415 foil and the elliptical Arndt wing is carried out. The SST turbulence model is complemented with the ? - Re ~?t transition model to determine the effect of varying turbulence intensity and eddy-viscosity ratio on the integral quantities and transition locations. Local grid refinement at the transition location is used to improve convergence. The skin friction drag coefficient is found to be more sensitive to the inflow conditions for 5? angle of attack compared to 9?. The movement of the transition location on the suction side is found to be responsible for this. The transition model captures a laminar separation bubble at the pressure side for both angles of attack, causing the lift coefficient to drop slightly. 3D calculations for the Arndt wing with the same foil section show that applying a transition model can decrease the boundary layer thickness by a factor of three, which is expected to influence the viscous core radius and consequently the minimum pressure in the tip vortex. ...
Conference paper (2015) - Oleksandr Zverkhovskyi, Maarten Kerkvliet, Arjan Lampe, Guilherme Vaz, Thomas van Terwisga
One of the most promising viscous drag reduction techniques for ships is so-called air lubrication. Particularly, a stable air layer created on the bottom reduces the wetted area and therefore reduces the resistance of a ship due to the negligibly small viscous drag of air compared to water. The air cavity and air chamber concepts are considered as the most effective and practical ways to form a stable air layer on the bottom capable to reduce the total drag by 10-20% for cargo ships ([1], [2]). These concepts are shown in Figure 1. The air cavity concept is based on injecting air behind a small obstruction that separates the flow which is called a cavitator. The cavitator is extended in the span-wise direction and typically has a rectangular or triangular cross section with a sharp edge. In the developed stage the length of an air cavity is limited to the length of a half the gravity-wave length and it should be restricted by skegs/keels on the sides. The air chamber is created by injecting air into a recess formed in the bottom. Provided the recess has sufficient depth, the free surface is not limited by the wave length and can have a multi-wave profile. The shape of the free-surface at different flow conditions and air injection rates is of interest. ...