“…These floccumittivity e* tot (v) calculated from the Fourier transform of lated aggregates give rise to a higher static permittivity and the pulse shapes will, in addition to the dielectric part e*(v), longer relaxation time than can be expected from the simple include a contribution from d.c conductivity, s; i.e., models of noninteracting spherical inclusions. This has resulted in the development of new models taking into account flocculation and elongation of aggregates, which are repree* tot Å e*(v) 0 is ve 0 , [6] sented by a shape factor. This shape factor depends on the axial ratios of the aggregates and is 1 3 for spheres and 1 50 for where e 0 is the permittivity of free space.…”