We compared the effects of human filamin A (FLNa) and the activated human Arp2/3 complex on mechanical properties of actin filaments. As little as 1 FLNa to 800 polymerizing actin monomers induces a sharp concentration-dependent increase in the apparent viscosity of 24 M actin, a parameter classically defined as a gel point. The activated Arp2/3 complex, at concentrations up to 1:25 actins had no detectable actin gelation activity, even in the presence of phalloidin, to stabilize actin filaments against debranching. Increasing the activated Arp2/3 complex to actin ratio raises the FLNa concentration required to induce actin gelation, an effect ascribable to Arp2/3-mediated actin nucleation resulting in actin filament length diminution. Time lapse video microscopy of microparticles attached to actin filaments or photoactivation of fluorescence revealed actin filament immobilization by FLNa in contrast to diffusion of Arp2/3-branched actin filaments. The experimental results support theories predicting that polymer branching absent cross-linking does not lead to polymer gelation and are consistent with the observation that cells deficient in actin filament cross-linking activity have unstable surfaces. They suggest complementary roles for actin branching and cross-linking in cellular actin mechanics in vivo.The major ingredient of living cells is water, but unlike water, cells exhibit elastic as well as viscous properties. The elasticity of cells, historically designated as gel-like, results from the interactions of intracellular solute, principally cytoskeletal polymers. One of these polymers, actin, dominates the periphery of motile non-muscle cells and accounts for their ability to protrude against resistance as they spread and crawl and to resist surface deformations. A basic prerequisite for this material property is solute cohesion (1, 2).Pure actin filaments in the absence of chemical cross-linking form a relatively soft material (3, 4), a finding predicted by recent theories for the rheological behavior of semi-flexible rods (5-7). Moreover, estimates of the actin polymer concentration (ϳ1 mM) (8) and of the average actin filament length (less than 1 m in actively protruding cells (9, 10)) predict that the actin filaments would disperse unless tethered and that, therefore, cross-linking of these filaments is necessary to provide sufficient coherence to account for the protrusive activity and deformation resistance of cells. Cells contain many actin filament-cross-linking proteins to accomplish this task (11).A phase transition that marks the cross-linking of actin filaments into a cohesive structure is an easily discernable abrupt consistency increase inducible by imposing a critical number of actin filament-cross-linking molecules (12). At this transition point, the system converts from predominantly overlapping linear chains into a giant continuously linked molecular structure, operationally defined as a gel (13). As with other polymers (1), the length of actin filaments is directly proportional to their...