Observations from the central North Sea show that, as soon as thermal strat
ification becomes established by solar insolation in the spring, the vertic
al smoothly varying horizontal current structure observed in winter becomes
distorted, with strongest vertical shear coincident with the strongest buo
yancy gradients (thermoclines). This shear is predominant at the local iner
tial frequency following strong wind-forcing or when the thermocline thickn
ess is relatively large, and the semidiurnal tidal frequency otherwise. Alt
hough the currents at these frequencies have a completely different charact
er, being circularly polarized and mode-1 at the inertial frequency and alm
ost rectilinear and barotropic at the tidal frequency, their shear vectors
are both anticyclonically polarized. While this is understood for near-iner
tial motions, it is less obvious for vertically varying tidal currents, in
the absence of internal tides.
Viscous flows are distinguished from those governed by inviscid physics by
inspection of their vertical current structures. It is demonstrated that th
e tidal frictional bottom boundary layer not only determines the depth and
'thickness' of the thermocline in shelf seas, but also the fate of shear ac
ross the stratification. This shear is dominated by the change in phase of
the anticyclonic rotary current component. The circular polarization of the
shear vector implies that the shear magnitude varies much slower with time
than its components, providing justification for the use of slowly varying
exchange parameters in models. As stratification also varies with time muc
h slower than the inertial period, a 'constant' eddy diffusivity is rendere
d through a marginal stability equilibrium relating shear and stratificatio
n and turbulent diapycnal exchange, irrespective of the generating frequenc
y.