A Thorpe scale analysis of the overturns yields a time-averaged dissipation near the bottom of
, 10 to 100 times higher than at similar depths in the ocean interior
from the ridge at the south mooring. The dissipation at the north mooring is estimated to be an order of magnitude smaller at
. At the south mooring, dissipation events much larger than the overall mean (up to
) occur predominantly during two phases of the semidiurnal tide: 1) during peak downslope flows when the tidally modulated stratification is minimum (
), and 2) when the flow reverses from down to upslope flow as the tidally modulated stratification is ordinarily increasing (
). Shear instabilities, particularly due to tidal and near-inertial strain enhancements, appear to trigger downslope flow mixing at the south mooring. Convective instabilities are proposed as the cause for flow reversal mixing at the south mooring, owing to the oblique propagation of an internal tidal beam down the slope.
At the north mooring, dissipation occurs predominantly during periods of high strain at the maximum upward displacement of the semidiurnal tide. Overturns are particularly prevalent when the tidal strain is enhanced by near-inertial wave driven downwelling near the slope. The intermittency of near-inertial waves at the north mooring limits the predictability of mixing events.