In this article, the correct form of Eq. (18) for the weak-scatterer contribution is
$F¯xϕB=−14ρℜ{∫L(∫Cx[W(M−R)*−NQ*]dl)dx}$
(18)
where the term R was missing from the originally published version and is defined by
$R=N2x[ξ3ψ3y+ξ5ψ3y(U/iω−x)+ψsy]+N3x[ξ3ψ3z+ξ5ψ3z(U/iω−x)+ψsz]$
This term is negligible for the slender hulls like the Wigley I and the DTC. It also has negligible influence on the results of other geometries presented in this article. The only case with a visible influence is the RIOS hull at β = 100 and Fr = 0.18 (Fig. 6, bottom left). This figure is updated with the correct results for Salvesen (new).
Fig. 6
Fig. 6
Close modal