Computational simulation of turbulent flows around a marine propeller by solving the partially averaged Navier–Stokes equation. (September 2019)

• Record Type: Journal Article
• Authors: Seok, Woochan; Lee, Sang Bong; Rhee, Shin Hyung
• Is Part Of: Proceedings of the Institution of Mechanical Engineers. Volume 233:Number 18(2019)
• Page Start: 6357
• Page End: 6366
• Publication Date: 2019-09
• Subjects: Partially averaged Navier–Stokes -- marine propeller -- turbulence model -- Open-source Field Operation And Manipulation -- vortical structure; Mechanical engineering -- Periodicals; 621.05
• DOI: 10.1177/0954406219848021
• Languages: English
• ISSNs: 0954-4062

Abstract

This study concerns the characteristics of the partially averaged Navier–Stokes method for local flow analysis around a rotating propeller. Partially averaged Navier–Stokes, resolving crucial large-scale structures of turbulent flow at a given computational grid resolution, is a bridging turbulence closure model between the Reynolds-averaged Navier–Stokes equation and the direct numerical simulation. A detailed comparison between partially averaged Navier–Stokes and Reynolds-averaged Navier–Stokes models is made to achieve a better understanding of partially averaged Navier–Stokes characteristics for predicting the coherent structures in turbulent flow. The two-equation k-ω shear stress transport model and the seven-equation Reynolds stress model are selected for Reynolds-averaged Navier–Stokes computations. The problem of interest is the flow around a rotating KP505 propeller in open water conditions at an advance ratio of 0.7. Near the leading edge, the partially averaged Navier–Stokes results are similar to those of Reynolds stress model in terms of the vortical structures. Vorticity predicted by different turbulence models, however, shows significant differences. For a more detailed analysis, the velocity gradient constituting the vorticity is identified at the leading edge. It is proven that partially averaged Navier–Stokes is able to capture the anisotropic characteristics of the flow at the leading edge, where both the geometric and flow characteristics change abruptly.