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Journal Articles
Accepted Manuscript
Article Type: Research Papers
J. Offshore Mech. Arct. Eng.
Paper No: OMAE-22-1168
Published Online: March 20, 2023
Journal Articles
Article Type: Research Papers
J. Offshore Mech. Arct. Eng. December 2023, 145(6): 061901.
Paper No: OMAE-22-1155
Published Online: March 16, 2023
Journal Articles
Article Type: Research Papers
J. Offshore Mech. Arct. Eng. December 2023, 145(6): 061902.
Paper No: OMAE-22-1087
Published Online: March 16, 2023
Image
in Turbulent Anisotropy and Length Scale Variation Over Multiple Shaped Structure
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 1 Schematic of the experimental setup for flow over sharp-corner cubical shape body, angled cubical-shaped body, and rounded-corner cubical-shaped body in water channel facility More
Image
in Turbulent Anisotropy and Length Scale Variation Over Multiple Shaped Structure
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 2 Variation of normalized stream-wise mean velocity profiles. Here, the vertical solid line represents log-law (Eq. (2) ) for the undisturbed flow condition (case 0), and the dotted horizontal line denotes the obstacle height. More
Image
in Turbulent Anisotropy and Length Scale Variation Over Multiple Shaped Structure
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 3 Lumley triangle plotted in ξ − η plane at the upstream and downstream locations for case 1, case 2, and case 3, respectively. The black dotted circle represents the large eddy simulation data over the smooth surfaces for free surface flow [ 35 ]. More
Image
in Turbulent Anisotropy and Length Scale Variation Over Multiple Shaped Structure
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 4 ( a – b ) The mean dissipation rate using the spectrum method at the elevation z / h = 0.5, for the flat surface More
Image
in Turbulent Anisotropy and Length Scale Variation Over Multiple Shaped Structure
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 5 Variation of the integral length scales ( L xx ) against z / h for case 1, case 2, and case 3, respectively More
Image
in Turbulent Anisotropy and Length Scale Variation Over Multiple Shaped Structure
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 6 Variation of Taylor's length scales ( λ ) against z / h for case 1, case 2, and case 3, respectively More
Image
in Turbulent Anisotropy and Length Scale Variation Over Multiple Shaped Structure
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 7 Variation of the Kolmogorov length scales ( η κ ) against z / h for case 1, case 2, and case 3, respectively More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 1 Illustration of the numerical domain used in the study demonstrating the FNPF and CFD models, coupling and cylinder placement in the case of the 3-h steady-state simulation case More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 2 Part of the numerical domain of REEF3D::FNPF simulation at t = 25 s demonstrating the free surface elevation due to a regular wave on a σ -grid More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 3 Grid convergence for REEF3D::FNPF using the 3-h sea state simulation: ( a ) free surface at x = 15.281 m, at the location of cylinder and ( b ) force on the cylinder More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 4 Grid convergence for REEF3D::CFD using the 3-h sea state simulation: ( a ) free surface at x = 15.281 m, at the location of cylinder close to the wall and ( b ) force on the cylinder More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 5 Calculated and measured free surface in front of the cylinder and wave forces due to incident nonbreaking regular waves: ( a ) free surface at x = 5.0 m, in front of the cylinder and ( b ) force on the cylinder More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 6 Part of the numerical domain of REEF3D::FNPF simulation at t = 22.5 s between x = 13 and 18 m More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 7 Calculated and measured free surface in front of the cylinder and wave forces due to irregular waves generated using a Jonswap spectrum with γ = 3.2, H = 0.1720 m, T = 1.5556 s for different time intervals: ( a ) free surface at x = 15.281 m for t = 500–520 s, ( b ) calculated for... More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 8 Hydrodynamic coupled CFD domain with wave incidence on a vertical cylinder at t = 1.73 s in the CFD simulation, corresponding to crest incidence at t = 811.73 s in the initial simulation More
Image
in Identification and Investigation of Extreme Events Using an Arbitrary Lagrangian–Eulerian Approach With a Laplace Equation Solver and Coupling to a Navier–Stokes Solver
> Journal of Offshore Mechanics and Arctic Engineering
Published Online: March 16, 2023
Fig. 9 Measured free surface in front of the cylinder and wave forces along with calculations from a coupled CFD simulation with a limited domain corresponding to t = 0.5–2.8 s in the coupled CFD simulation, which is t = 810.5–812.8 s in the initial simulation: ( a ) free surface at x = 15.2... More
Journal Articles
Article Type: Research Papers
J. Offshore Mech. Arct. Eng. December 2023, 145(6): 062001.
Paper No: OMAE-22-1097
Published Online: March 16, 2023