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Observations and Modelling of Fronts and Frontogenesis

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temperature variations, but again presumably mostly on scales<br />

larger than 10 km.<br />

Over 900-km space <strong>and</strong> two-week time scales <strong>and</strong> despite<br />

variable atmospheric conditions, the spectral shapes were<br />

roughly constant. This suggests that processes that<br />

contribute substantially to the variance must be<br />

statistically homogeneous over these scales. Near-inertial<br />

currents, which respond strongly to storms, would appear not<br />

to meet this criterion.<br />

Finally, we note that the -3 power law temperature<br />

spectrum differs from that predicted for a passively advected<br />

scalar in a turbulent flow. In that case the scalar<br />

spectrum, not the gradient spectrum, is inversely<br />

proportional to wavenumber (atchelor, 1959).<br />

11.6 Summary<br />

The thermistor tows yield a detailed two-dimensional<br />

description <strong>of</strong> surface layer temperature along 1400 km <strong>of</strong> tow<br />

tracks in the Eastern North Pacific Subtropical Frontal Zone<br />

during January 1980. In brief, we find:<br />

(1) The dominant features have wavelengths <strong>of</strong> 10-100 km,<br />

amplitudes <strong>of</strong> 0.2 to 1.0 °C, <strong>and</strong> no preferred orientation<br />

with respect to the mean meridional gradient (Figure 11.4).<br />

These features, which could be created from the<br />

climatological mean sea surface temperature field by<br />

26

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