Solution

ID: past-exam-of-the-physics-of-atmospheres-and-oceans-course-of-the-university-of-oxford/2022/6/d/solution

Coastal Kelvin-wave radiation of long Rossby waves requires a common phase convention to match the two waves. The supplied Rossby wave formula conventionally multiplies , while the coastal expression uses . Since physical fields are real, matching may use the complex-conjugate representative; in either convention the boundary forcing fixes the absolute frequency and alongshore wavenumber. Thus and .
For , the shallow-water Rossby-wave dispersion relation reduces to
Choosing recovers the printed magnitude relation. Both the zonal phase velocity and zonal group velocity are approximately , so the long Rossby waves carry the coastal signal westwards into the basin.
The coastal condition alone does not guarantee a long zonal wavelength. Since , matching requires and hence the stronger consistency condition
For example, at a coastal wavenumber with gives , which is not asymptotically small even though the meridional wavelength is long. Thus the source's proposed excitation is possible at sufficiently low frequency; it is not an automatic consequence of its meridional long-wave assumption.
At N or S the beta plane parameter is
Taking a representative Pacific basin width m gives
A width of – m gives roughly – years. This is propagation near latitude, not an equatorial calculation. Slow Rossby wave adjustment supplies a basin-scale delay relevant to El Niño–Southern Oscillation: changing thermocline depth can affect later sea surface temperature and coupled wind forcing. Reflection and coupling may help produce interannual memory, but this travel-time estimate alone does not establish a climate oscillation or its period.

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