Scattering of flexural-gravity waves by a crack in a floating ice sheet due to mode conversion during blocking

• Published in: Journal of fluid mechanics 2021-04, Vol.916, Article A11
• Main Authors: Barman, S.C., Das, S., Sahoo, T., Meylan, M.H.
• Format: Article
• Language: English
• Subjects: Boundary value problems; Coefficients; Compression; Conversion; Dispersion; Energy; Enforcement; Floating ice; Floating structures; Glaciation; Gravity waves; Group velocity; Ice sheets; JFM Papers; Longitudinal waves; Mathematical problems; Modes; Propagation modes; Radiation; S matrix theory; Scaling; Velocity; Wave propagation; Wave scattering; Wavelengths
• ISSN: 0022-1120; 1469-7645
• DOI: 10.1017/jfm.2021.200

The scattering of flexural-gravity waves in a thin floating plate is investigated in the presence of compression. In this case, wave blocking occurs, which is associated with both a zero in the group velocity and coalition of two or more roots of the related dispersion relation. There exists a region in the frequency space in which there are three real roots of the dispersion equation and hence three propagating modes. This multiplicity leads to mode conversion when scattering occurs. In one of these modes, the energy propagation direction is opposite to the wavenumber, making enforcement of the Sommerfeld radiation condition challenging. The focus here is on a canonical problem in flexural-gravity wave scattering, the scattering of waves by a crack. Formulae are developed that apply uniformly at all frequencies, including through the blocking frequencies. This solution is developed by tracking the movement of the dispersion relation roots carefully in the complex plane. The mode conversion is verified by the scattering matrix of the process and through an energy identity. This energy identity for the case of more than one progressive modes is established using Green's theorem and later applied in the scattering matrix to identify the incident and transmitted waves in the scattering process and derive the radiation condition. Appropriate scaling of the reflection and transmission coefficients are provided with the energy identity. The solution method is illustrated with numerical examples.