Abstract
The influence of anharmonic elastic terms on the hydrodynamics of discotic liquid crystals is examined. These terms generate a nonlinear coupling between the velocity field and thermally excited undulation modes which, it is shown, causes four of the five viscosities in these systems to diverge as ω12 at small frequencies ω. This implies that the attenuation of sound in these systems should scale as ω32 (not ω2 as in conventional materials). A simple relation between three of the diverging viscosities is found. Various experimental tests of these predictions are suggested.