Changes

First, we create [[Image:ff settings.png|thumb|left|150px|Adding an RCS observable with 1 degree increments in both phi and theta directions. Although increasing for the angular resolution of our farfield can increase simulation time, The RCS of electrically large structures tend to have very narrow peaks and nulls, so the resolution is required.Mirage project]]

We also First, we create two field sensors -- one an RCS observable with a z-normal underneath the aircraft, 1 degree increments in both phi and another with an x-normal along theta directions. Although increasing the length angular resolution of our farfield will significantly increase simulation time, The RCS of electrically large structures tend to have very narrow peaks and nulls, so the aircraftresolution is required.

[[Image:ff settings.png|thumb|left|150px|Figure 1: Geometry of We also create two field sensors -- one with a z-normal underneath the periodic unit cell aircraft, and another with an x-normal along the length of the dispersive water slab in EMaircraft.Tempo.]][[Image:ff settings.png|thumb|left|150px|Figure 1: Geometry of The nearfields are not the periodic unit cell of prime observable for this project, but they may add insight into the dispersive water slab in EM.Temposimulation, and do not add much overhead to the simulation.]]