The purpose of this appendix is to present a derivation of MOM's discretized horizontal friction operator. Much here follows the functional approach used for the isoneutral diffusion discretization in Appendix C. However, the present discussion is considerably simpler because of the need to only discretize a two dimensional (x-y plane) operator, and because there are no subtleties associated with neutral directions. The approach here is therefore a straightforward application of the functional formalism outlined in Section 9.7 for the continuum friction, and Appendix C for the diffusion operator.
Brief history of this method in MOM: