In the time mean, the basic circulation is understood as follows: As the inflow reaches topography and the flow moves upslope, a western anticyclonic boundary current develops due to Rossby wave energy concentrating towards the western wall, or equivalently due to bottom pressure torque acting on the mean streamlines. The boundary current induces a local acceleration along the mean streamline, resulting in a reduction of the Bernoulli potential in the along-stream direction and thus a net cross-stream frictional vorticity flux from the wall. A similar situation occurs as the flow moves downslope. The reversed topographic slope now promotes a cyclonic boundary current at the eastern wall. The resulting local acceleration of the flow along the streamline results in a cross-stream vorticity flux towards wall, balancing the advective vorticity flux along the ridge.
Along the ridge, barotropic eddies separate from the western boundary current, extracting and advecting large cyclonic relative vorticity from the wall. As they move towards the eastern boundary current along topographic contours, these eddies experience dissipation due to bottom friction. Frictional vorticity production, which can be written as the integral of the Bernoulli potential along solid boundaries, allows for the examination of the role of eddies on the mean flow. In addition, we present a complementary analysis comparing our results at different spatial resolutions that allow eddies to develop, as well as contrasting the choice of free slip and no-slip boundary conditions.