4.7 Article

Experimental and numerical study of free surface effect on the ventilated cavitating flow around a surface vehicle model

Journal

OCEAN ENGINEERING
Volume 268, Issue -, Pages -

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.oceaneng.2022.113413

Keywords

Cavitating flow; Surface vehicle; Free surface effect; Supercavity size; Drag coefficient

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In this study, the ventilated cavitating flow near the free surface is investigated experimentally and numerically. The experimental observations and numerical predictions show that increasing the Froude number results in an increase in supercavity size and a decrease in drag coefficient. The numerical results also reveal that increasing the submergence depth leads to an increase in drag coefficient due to the existence of a cavitator at the front of the vehicle.
In the current study, the ventilated cavitating flow for a model near the free surface is investigated experimentally and numerically. The experiments are performed in a towing tank equipped with a ventilation system, drag measurement interface and a photography system. The numerical simulation is performed by commercial CFD code ANSYS-CFX with the volume of fluid (VOF) method, the RNG k-e turbulence model, and effectiveness of the gravity. The ventilated supercavity and drag coefficient of the model under free surface effect is studied at different submergence depths and velocities. Both the experimental observations and numerical predictions show that with increasing the Froude number (Fr), the ventilated supercavity size increases and the drag coefficient decreases. The good agreement observed between the numerical predictions and experimental data, in terms of both the supercavity size and drag coefficient, has revealed the accuracy and capability of the applied numerical model. The numerical results reveal that with increasing the submergence depth, the drag coefficient increases due to existence of the cavitator at the front of the vehicle. Also, in the regions near the free surface, the variation of supercavity length with Fr is different from that of the regions away from the free surface.

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