PulseExploreJournal ClubDebatesTrendingResearchersJournals
Instagram
HomeExploreJournal ClubTrending
Synapse
⌘+K
Synapse
November 11, 2003Journal of Fluid Mechanics131 citations

Tidal conversion at a very steep ridge

View Full Paper
SSStefan G. Llewellyn SmithWYW. R. Young

Key Points

Key points are not available for this paper at this time.

Abstract

We obtain an analytic solution for the generation of internal gravity waves by tidal flow past a vertical barrier of height b in a uniformly stratified ocean of depth h\, >\, b and buoyancy frequency N. The radiated power (watts per metre of barrier) is 14 ₀ b² U² N 1- (f/) ²M (b/h), where ₀ is the mean density of seawater, U (t) the tidal velocity, and f the Coriolis frequency. The function M (b/h) increases monotonically with M (0) \, =\, 1, M (0. 92) \, =\, 2 and M (1) \, =\,. As b/h \, \, 1, M diverges logarithmically and consequently the radiated power grows as (h-b) /b. We also calculate the conversion in a realistically stratified ocean with strongly non-uniform buoyancy frequency, N (z). A rough approximation to the radiated power in this case is 14 ₀ b² U² N (b) 1- (f/) ² M (B/), where N (b) is the buoyancy frequency at the tip of the ridge and B is the height of the ridge in WKB coordinates. (The WKB coordinate is normalized so that the total depth of the ocean is. ) The approximation above is an over-estimate of the actual radiation by as much as 20% when B/ \, \, 0. 8. But the formula correctly indicates the strong dependence of conversion on stratification through the factor N (b).

Ask AI
Helpful
Bookmark
Share
View Full Paper

Cite This Study

Smith et al. (2003) studied this question.

synapsesocial.com/papers/6a86d0c3ddd5671cb07cb5b9https://doi.org/10.1017/s0022112003006098
Ask AI
Helpful
Bookmark
Share
View Full Paper