H. Peters et al., THE DIURNAL CYCLE OF THE UPPER EQUATORIAL OCEAN - TURBULENCE, FINE-SCALE SHEAR, AND MEAN SHEAR, J GEO RES-O, 99(C4), 1994, pp. 7707-7723
Physical processes within the diurnal cycle of the upper ocean in the
Pacific Equatorial Undercurrent are investigated based on observations
at 0-degrees/14-degrees-W of April 1987. The cycle extended below the
surface mixed layer into the pycnocline, where nighttime maxima and d
aytime minima occurred in turbulent dissipation rates epsilon, fine-sc
ale shear variance, and in ''large-scale,'' low-frequency zonal shear,
buoyancy frequency, and gradient Froude number. The time-of-day avera
ge epsilon varied by a factor of 40 at 20 m, near the base of the mixe
d layer. Its night/day ratio decreased with increasing depth, the diur
nal signal extending to 45-60 m, compared to nighttime mixed layer dep
ths of 10-25 m. The daily variation of epsilon extended throughout the
layer of high shear and high gradient Froude number Fr, above the Und
ercurrent core, being cut off where the large-scale Fr dropped below 1
. The diurnal cycle of epsilon remained unaffected by changes in the l
arge-scale shear and stratification. The nighttime fine-scale shear va
riance in the 5-10 m vertical wavelength band exceeded daytime minima
by a factor of 2 on average, the daily variation decaying rapidly with
increasing depth. Turbulent overturns were smaller than 5 m, so that
we suspect that the fine-scale shear was related to internal waves. Fi
ne-scale shear was large enough to be a factor in local shear instabil
ity. A zone some 20 m thick below the mixed layer showed weak nighttim
e maxima in the large-scale, low-frequency zonal shear, stratification
, and Froude number. We suspect that these variations were a product o
f turbulent mixing. They could become a discriminative tool in a futur
e comparison of our observations with upper ocean models. The applicat
ion of such models encouraged by indications of a local control of the
upper ocean heat budget by the surface heat flux. In apparent respons
e to a weaker Undercurrent, stronger stratification, and weaker trade
winds, mean and nighttime dissipation rates were lower in 1987 than in
November 1984, The night/day ratio, however, was larger in 1987 owing
to the absence of daytime high-epsilon events.