1963
DOI: 10.21236/ad0414680
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On Ships With Zero and Small Wave Resistance

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Cited by 5 publications
(5 citation statements)
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“…(1) + S, Cl) K^cos-^^y dd Namely the amplitude function of the elementary waves from the bow for all angle (' in (28) can be made zero by attaching at the bow a concentrated doublet line which extends to infinite depth. Since the deeply submerged part does not influence too much the surface waves (Yim, 1963) this clarifies the mechanism of the bulb and backs up the approach made by .…”
Section: Ijmentioning
confidence: 70%
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“…(1) + S, Cl) K^cos-^^y dd Namely the amplitude function of the elementary waves from the bow for all angle (' in (28) can be made zero by attaching at the bow a concentrated doublet line which extends to infinite depth. Since the deeply submerged part does not influence too much the surface waves (Yim, 1963) this clarifies the mechanism of the bulb and backs up the approach made by .…”
Section: Ijmentioning
confidence: 70%
“…The optimum distribution of the concentrated singularities at the finite stern line for several given ship source distributions are calculated (Yim 1963) and shown in Figs, 3-7. These indicate that the strength of the singularities at the deepest point (the same level as the keel) is the largest. Especially for the higher Froude numbers, the optimum distributions appear to be almost concentrated at the keel.…”
Section: Appendix 1 Methods Of Evaluation Of Variances Of Relative Motion and Velocity Between Wave And Ship Bowmentioning
confidence: 99%
“…The comparison between total resistance of the forms with bulb and total resistance of the forms without bulb are done via Equation (11). Thus, it is determined that, how much increase (+) or decrease (-) are on the total resistance according to the bulb shapes.…”
Section: Comparison Of Cfd Results With Test Resultsmentioning
confidence: 99%
“…Later, Bragg [4], Inui et al [5], Ferguson [6], and Muntjewerf [7] experimentally conducted experiments on the Δ (delta) type, cylindrical and conical bulbs, which are known as Taylor bulbs, by systematically changing the bulb parameters. Weinblum [8], Wigley [9], Inui [10] and Yim [11] studied on the theory of linearized wave resistance theoretically. Inui [10] presented a method to determine the size of the bulb by matching amplitude functions of bulb in regular waves and stem.…”
Section: Introductionmentioning
confidence: 99%
“…Almost all the experimental studies were done on either Taylor bulbs (bottom heavy or ∆ type bulb) or cylindrical bulbous bows. Theoretically, Wigley (1936), Weinblum (1935), Inui (1962), and Yim (1963) studied the linearized theory of wave resistance in detail. Though the theory gives a better understanding of bulb action it is still difficult to design the bulb for given constraints because of a lack of quantitative guidelines.…”
Section: Review Of Literaturementioning
confidence: 99%