| 1 | 
Bottom Topography as a Control Parameter in an | 
| 2 | 
    Ocean Circulation Model | 
| 3 | 
     | 
| 4 | 
Martin Losch and Carl Wunsch | 
| 5 | 
 | 
| 6 | 
  Bottom topography is a major factor in determining the general | 
| 7 | 
  circulation of the ocean. It is, however, inaccurately known in many | 
| 8 | 
  regions, and even where accurately known, the best way to represent  | 
| 9 | 
  (parameterize) it in models is obscure. To begin to understand the   | 
| 10 | 
  influence of errors in topography and of misrepresentations of both  | 
| 11 | 
  resolved and sub-grid scale structures, a linear barotropic shallow  | 
| 12 | 
  water model and its adjoint are developed in which depth is used as  | 
| 13 | 
  a control variable. Simple basin geometries are employed to explore  | 
| 14 | 
  the extent to which topographic structure determines the sea-surface | 
| 15 | 
  elevation in a steady flow and, more directly, the information | 
| 16 | 
  content about the bottom contained in elevation measurements.  | 
| 17 | 
  Experiments show that even perfect measurements of sea-surface | 
| 18 | 
  elevation in a steady state cannot, by themselves, uniquely | 
| 19 | 
  determine the full structure of the bottom topography. (There is a | 
| 20 | 
  null space.) As in most control problems, a priori knowledge of its | 
| 21 | 
  structure is useful in the best topographic determination. | 
| 22 | 
  Resolution of the bottom topography as a function of position is | 
| 23 | 
  greatest where the flow velocities are greatest. Spatial correlation | 
| 24 | 
  between the resolution of the bottom topography and the flow field   | 
| 25 | 
  is weaker (as expected) when noise with realistically large variance | 
| 26 | 
  is introduced into the data. Ultimately, bottom topography will | 
| 27 | 
  likely be included generally as a control variable in GCMs of   | 
| 28 | 
  arbitrary complexity along with other controls such as friction and | 
| 29 | 
  lateral boundary conditions. | 
| 30 | 
 |