| dc.contributor.author | Amini-Afshar, Mostafa | |
| dc.date.accessioned | 2022-12-27T23:20:01Z | |
| dc.date.available | 2022-12-27T23:20:01Z | |
| dc.date.copyright | 9/1/2022 12:00:00 AM | |
| dc.date.issued | 2022 | |
| dc.identifier.issn | 0892-7219 | |
| dc.identifier.other | omae_144_6_067001.pdf | |
| dc.identifier.uri | http://yetl.yabesh.ir/yetl1/handle/yetl/4288397 | |
| dc.description.abstract | In this article, the correct form of Eq. (18) for the weak-scatterer contribution is(18)F¯xϕB=−14ρℜ{∫L(∫Cx[W(M−R)*−NQ*]dl)dx}where the term R was missing from the originally published version and is defined byR=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). | |
| dc.publisher | The American Society of Mechanical Engineers (ASME) | |
| dc.title | Erratum: “Salvesen’s Method for Added Resistance Revisited” [ASME J. Offshore Mech. Arct. Eng., 143(5), p. 051902; DOI: 10.1115/1.4050213] | |
| dc.type | Journal Paper | |
| dc.journal.volume | 144 | |
| dc.journal.issue | 6 | |
| dc.journal.title | Journal of Offshore Mechanics and Arctic Engineering | |
| dc.identifier.doi | 10.1115/1.4055234 | |
| dc.journal.fristpage | 67001 | |
| dc.journal.lastpage | 67001_1 | |
| dc.page | 1 | |
| dc.tree | Journal of Offshore Mechanics and Arctic Engineering:;2022:;volume( 144 ):;issue: 006 | |
| dc.contenttype | Fulltext | |
