Coastal Engineering 1966 1967
DOI: 10.1061/9780872620087.016
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Wave Decaying Due to Breaking

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Cited by 7 publications
(8 citation statements)
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“…2 which shows the relative change in wave height H/H versus the distance from the breaking point measured in units of h. . Horikawa & Kuo (1966) and by Nakamura et al (1966) on a similar slope (1 in 30 against ours 1 in 34) though the above mentioned conjecture implies that the effect of the slope is insignificant. It is worth noticing that the wide range of wave parameters in Fig.…”
Section: Run-up Regionsupporting
confidence: 76%
“…2 which shows the relative change in wave height H/H versus the distance from the breaking point measured in units of h. . Horikawa & Kuo (1966) and by Nakamura et al (1966) on a similar slope (1 in 30 against ours 1 in 34) though the above mentioned conjecture implies that the effect of the slope is insignificant. It is worth noticing that the wide range of wave parameters in Fig.…”
Section: Run-up Regionsupporting
confidence: 76%
“…Specifically, wave height and its spatial gradients generate or have direct impact on sediment mobilization and suspension, littoral currents in both the alongshore and onshore/offshore directions, waveinduced set-down/set-up in the mean water level, and forces on coastal structures. While the "0.78" criterion (ratio of breaker height to water depth equals 0.78) appears to provide a reasonable prediction of incipient breaking on mildly sloping beaches, data show that this criterion does not hold farther into the surf zone [Horikawa and Kuo, 1966;Nakamura et al, 1966;Street and Camfield, 1966;Divoky et al, 1970]. In fact, these data show that such a similarity model is especially inappropriate on mild slopes, just where many coastal scientists assume that it is most valid.…”
Section: Introductionmentioning
confidence: 99%
“…The transformation of a breaking wave over a slope is a problem of obvious concern in the design and planning of coastal facilities A number of investigators have considered this topic, including Freeman and LeMe'haute' (1964), Horikawa and Kuo (1966), LeMehaute* (1962), Divoky, LeMehaute", and Lin (1970), Nakamura, Shiraishi, and Sasaki (1966), and Street and Camfield (1966) The present contribution considers an essential aspect neglected m previous studies, the phenomenon of "wave set-up " Set-up, while negligible seaward of the breaking point, becomes dominant with respect to still-water depth as the shore is approached It is apparent, then that any analysis of breaking wave height transformation should account for the set-up Experimental investigations of set-up have been made by Saville (1961) and by Bowen, Inman, and Simmons (1968) with the result that the maximum elevation may be a significant fraction (~ 50%) of the breaking wave height Additionally, measurements obtained during the Mono Lake explosion-wave tests indicated a set-up value equalling the maximum height of the superposed dispersive wave train (Van Dorn, et al, 1968) Hwang (1970 also investigated dispersive wave trains and found a fluctuating set-up of roughly half the peak wave height Wave set-up has been investigated extensively in a series of papers by 61,62,64) from an analytical approach The difficulty m applying their results to the Tetra Tech, Inc , Pasadena, California surf zone, arises from the problem of finding an adequate description of the waves after breaking Bowen, Inman, and Simmons (1968) assumed that the wave height remains a constant fraction of mean water depth after breaking and found, from a momentum balance, a linear set-up variation…”
Section: Introductionmentioning
confidence: 99%