“…• The diffusion and sedimentation of microspheres in polymer solutions generally follow "Stokes-Einstein behavior," i.e., f ϭ Ϫ6 * trans a, where f is a modified Stokes friction factor, a is the radius of the sphere, and * trans is the effective viscosity that is dependent on the concentration, molecular weight and morphology of the polymer, the sphere size, and so on (Kluijtmans, et al, 2000;Turner and Hallett, 1976;Yang and Jamieson, 1988;Brown and Rymden, 1988;Phillies et al, 1989;Onyenemezu et al, 1993;Bu and Russo, 1994); • The rotations of bacterial tethered cell in methylcellulose solutions are faster than those in Ficoll solutions at the same viscosities (Berg and Turner, 1979). The measurement of the rotational Brownian motion of globular proteins in dextran solutions indicates that the effective viscosity is expressed as * rot ϭ 0 (/ 0 ) q , where and 0 are the macroviscosities of polymer solution and water as mentioned above, and q is smaller than unity and is distinctly polymer-and protein-dependent (Lavalette et al, 1999).…”