Organized structures in subsurface bubble clouds: Langmuir circulation in the open ocean

Len Zedel, David M. Farmer

Journal of Geophysical Research Atmospheres · 1991 · 135 citations · 19 references

Concepts

TL;DR

Subsurface bubble distributions reveal coherent motions near the ocean surface. Measurements were collected in the open ocean using a freely drifting, self‑contained acoustic platform equipped with side‑scan sonar, dual‑frequency echo sounders, and ambient sound recorders. Bubble clouds form long, narrow wind‑aligned plumes 3–5 m wide and up to 100 m long, with mean spacing increasing from ~5 m at wind speeds below 5 m s⁻¹ to ~10 m above 10 m s⁻¹, penetrating to a maximum depth of 12 m at the highest winds but averaging only 6 m when winds exceed 5 m s⁻¹, and exhibiting downward velocities of ~0.06 m s⁻¹ at 8 m depth that taper to zero near the surface and plume edges.

Abstract

Observations of the movement and distribution of subsurface bubbles reveal the structure of coherent motions near the ocean surface. The measurements were obtained in the open ocean from a freely drifting, self‐contained acoustical instrument equipped with side scan sonar, dual‐frequency echo sounders, and ambient sound recording systems. The bubble clouds are organized into long, narrow plumes aligned with the wind, consistent with windrows caused by Langmuir circulations. They have widths of about 3 to 5 m and lengths up to 100 m, with multiple scales coexisting. Their mean separation depends upon wind speed: below 5 m s −1 , mean spacings were about 5 m, increasing to 10 m when winds exceeded 10 m s −1 The maximum depth to which the plumes were observed to penetrate depended to some extent on wind speed, with the greatest penetrations of 12 m occurring at the highest wind speeds (13 m s −1 ). However, the time‐averaged depth of observed bubble plume penetration bears only a weak dependence on wind speed. Whenever winds exceeded 5 m s −1 , a mean penetration depth of 6 m was observed. Associated with these bubble plumes were maximum downward velocities of about 0.06 m s −1 . These speeds were detected at 8 m depth in the center of the plumes; magnitudes decreased to zero near the surface and horizontally toward the boundaries of the plumes.

References

19