next up previous contents
Next: Separation of Variables Up: Very Low Frequency Waves Previous: Very Low Frequency Waves

Basic Equations

A considerable simplification and an added flexibility in the analysis occurs if one neglects the vertical acceleration. This is justifiable for gravity modes if tex2html_wrap_inline5813 , and is certainly justifiable for quasi-geostrophic (Rossby) modes for which tex2html_wrap_inline5817 (i.e. subinertial modes). As in the previous analyses, we ignore compressibility and employ the traditional approximation for the Coriolis terms. However, we will now remove the restriction of a rigid lid and thus allow surface (barotropic) gravity modes. Finally, we treat the sea bed as level (D = constant). The hydrostatic approximation (i.e. ( tex2html_wrap_inline5821 ) and the restriction to constant D allow us the completely separate the z dependency of admissible modes from the x, y, t dependency. Stated another way, the equations of motion for the linear, undamped, free disturbances are converted into a set of linearly independent equations controlling the x, y, t dependency of each of the admissible vertical modes.

Thus the equations for which solutions are to be sought are

align2998

plus the boundary conditions

align3010

Here tex2html_wrap_inline5839 and the subscript 1 is dropped for simplicity on all other variables.


next up previous contents
Next: Separation of Variables Up: Very Low Frequency Waves Previous: Very Low Frequency Waves

Steve Baum
Sun May 19 00:59:05 CDT 1996