2014
DOI: 10.1017/jfm.2013.589
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The wake of a two-dimensional ship in the low-speed limit: results for multi-cornered hulls

Abstract: In the Dagan & Tulin (J. Fluid Mech., vol. 51, 1972, pp. 529-543) model of ship waves, a blunt ship moving at low speeds can be modelled as a two-dimensional semiinfinite body. A central question for these reduced models is whether a particular ship design can minimize, or indeed eliminate, the wave resistance. In the previous part of our work (Trinh et al., J. Fluid Mech., vol. 685, 2011, pp. 413-439), we demonstrated why a single corner can never be made waveless. In this accompanying paper, we continue our… Show more

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Cited by 13 publications
(26 citation statements)
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“…Origin of the low-Froude paradox Ogilvie (1968) Two-dimensional and three-dimensional linearizations Dagan & Tulin (1972), Keller (1979), Ogilvie & Chen (1982), Doctors & Dagan (1980), Tulin (1984), Brandsma & Hermans (1985) On numerical solutions Vanden-Broeck & Tuck (1977), Vanden-Broeck et al (1978), Madurasinghe & Tuck (1986), Farrow & Tuck (1995) On exponential asymptotics applied to water waves Chapman & Vanden-Broeck (2002, 2006, Trinh et al (2011), Trinh & Chapman (2013a, Lustri et al (2013); Lustri & Chapman (2014), Trinh & Chapman (2014) Review articles Tuck (1991a), Tulin (2005) …”
Section: Historical Significance Papersmentioning
confidence: 99%
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“…Origin of the low-Froude paradox Ogilvie (1968) Two-dimensional and three-dimensional linearizations Dagan & Tulin (1972), Keller (1979), Ogilvie & Chen (1982), Doctors & Dagan (1980), Tulin (1984), Brandsma & Hermans (1985) On numerical solutions Vanden-Broeck & Tuck (1977), Vanden-Broeck et al (1978), Madurasinghe & Tuck (1986), Farrow & Tuck (1995) On exponential asymptotics applied to water waves Chapman & Vanden-Broeck (2002, 2006, Trinh et al (2011), Trinh & Chapman (2013a, Lustri et al (2013); Lustri & Chapman (2014), Trinh & Chapman (2014) Review articles Tuck (1991a), Tulin (2005) …”
Section: Historical Significance Papersmentioning
confidence: 99%
“…For flows past a semi-infinite surface piercing body, we can choose the length scale to be L " K{U , where K is a representative scale of the potential along the body (see (2.3) in Trinh & Chapman (2014) for further details). We assume that the free surface attaches to the body at a stagnation point, chosen without loss of generality to be φ " 0.…”
Section: Boundary Integral Formulation and Geometrical Examplesmentioning
confidence: 99%
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