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Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in...

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www.pol.ac.uk Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U. Liverpool)
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Page 1: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

www.pol.ac.uk

Internal waves and slope mixing in the Faroe-Shetland Channel

Rob Hall (POL) John Huthnance (POL)

Ric Williams (U. Liverpool)

Page 2: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Internal waves

Page 3: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Internal waves

Page 4: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Internal wave reflection

Page 5: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Faroe-Shetland Channel

Page 6: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Faroe-Shetland Channel

Page 7: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Internal Tide

Page 8: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Internal Tide

Page 9: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Internal Tide

Page 10: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Near-bed, non-linear internal waves

Page 11: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Near-bed, non-linear internal waves

Page 12: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

TKE dissipation rate

Page 13: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Internal wave energy dissipation

Page 14: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Numerical model

Page 15: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Numerical model

Page 16: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Conclusions

•  Mixing on the slope enhanced above background levels (ε = 5 × 10-8 W kg-1 κρ = 2 × 10-4 m2 s-1)

•  Can be accounted for by internal wave energy fluxes –  Internal tides, 150 W m-2 (100 W m-2 in pycnocline)

–  Near-bed, non-linear internal waves, up to 200 W m-2

•  Up to 68% of incident internal tide energy reflected •  Modal structure maintained upon reflection cannot

be explained simply by critical slope theory •  Non-linear internal waves must dissipate or break

locally because near-bed N < ω further up the slope •  Up-slope of the intersection with pycnocline, internal

wave energy cannot progress onto the shelf

Page 17: Internal waves and slope mixing in the Faroe-Shetland Channel · Internal waves and slope mixing in the Faroe-Shetland Channel Rob Hall (POL) John Huthnance (POL) Ric Williams (U.

Slope mixing processes


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