The dynamic microenvironment of cells depends on macromolecular architecture, equilibrium fluctuations, and nonequilibrium forces generated by cytoskeletal proteins. We studied the influence of these factors on the motions of mitochondria in mating S. cerevisiae using Fourier imaging correlation spectroscopy (FICS). Our measurements provide detailed length-scale dependent information about the dynamic behavior of mitochondria. We investigate the influence of the actin cytoskeleton on mitochondrial motion and make comparisons between conditions in which actin network assembly and disassembly is varied either by using disruptive pharmacological agents or mutations that alter the rates of actin polymerization. Under physiological conditions, nonequilibrium dynamics of the actin cytoskeleton leads to 1.5-fold enhancement of the long-time mitochondrial diffusion coefficient and a transient subdiffusive temporal scaling of the mean-square displacement (MSD ∝ τ α , with α ¼ 2∕3). We find that nonequilibrium forces associated with actin polymerization are a predominant factor in driving mitochondrial transport. Moreover, our results lend support to an existing model in which these forces are directly coupled to mitochondrial membrane surfaces.anomalous diffusion | Arp2/3-mediated actin polymerization | Fourier imaging correlation spectroscopy | intracellular transport | mitochondrial dynamics T he intracellular environment is a dynamic multicomponent fluid with relaxations spanning a broad range of length and time scales. As in ordinary fluids, in cells thermally generated inertial forces give rise to stochastic particle motions, which may be characterized by the particle mean-square displacement (MSD). Under many circumstances, thermal diffusion is a primary mechanism of intracellular transport. However, nonequilibrium forces that are generated by protein polymerization, motor proteins, and gradients in thermodynamic potentials can additionally influence particle motion. A central question in modeling cell transport is whether the cytoplasm may be viewed as a simple extension of a complex fluid at equilibrium or if nonequilibrium effects dominate the motions of intracellular species.For a spatially homogeneous fluid at equilibrium, the MSD scales linearly in time (i.e. MSD ∝ τ α with α ¼ 1). However, microscopic heterogeneity and viscoelasticity of multicomponent fluids results in "anomalous" particle motion (1-5). In the context of cell dynamics the motion of a macromolecule or larger particle may become hindered by obstacles in its immediate environment, leading to subdiffusive scaling of the MSD (i.e. α < 1), over an appreciable time range (4). For example, the motions of small proteins in bacteria appear to be diffusive (6-8), whereas those of larger particles, such as mRNA-protein clusters in E. coli and yolk granules in yeast, appear to be subdiffusive (2, 3). These differences in the dynamics of intracellular species and host organisms may be reconciled by accounting for the relative size of the mobile particles...