Abstract
We obtain the equations of motion for the density and phase of a propagating pulse in analogy to the Bohm formulation. We define the group velocity operator and show how it can be used to obtain the fluid-like velocity. We consider propagation with dispersion and attenuation.
Acknowledgments
The author would like to thank one of the referees for the helpful suggestions made. This research was supported by the Office of Naval Research (Grant No. N00014-09-1-0162).