The conformation and dynamics of circular polymers is a subject of considerable theoretical and experimental interest. DNA is an important example because it occurs naturally in different topological states, including linear, relaxed circular, and supercoiled circular forms. A fundamental question is how the diffusion coefficients of isolated polymers scale with molecular length and how they vary for different topologies. Here, diffusion coefficients D for relaxed circular, supercoiled, and linear DNA molecules of length L ranging from Ϸ6 to 290 kbp were measured by tracking the Brownian motion of single molecules. A topology-independent scaling law D ϳ L ؊ was observed with L ؍ 0.571 ؎ 0.014, C ؍ 0.589 ؎ 0.018, and S ؍ 0.571 ؎ 0.057 for linear, relaxed circular, and supercoiled DNA, respectively, in good agreement with the scaling exponent of Х 0.588 predicted by renormalization group theory for polymers with significant excluded volume interactions. Our findings thus provide evidence in support of several theories that predict an effective diameter of DNA much greater than the Debye screening length. In addition, the measured ratio DCircular͞ DLinear ؍ 1.32 ؎ 0.014 was closer to the value of 1.45 predicted by using renormalization group theory than the value of 1.18 predicted by classical Kirkwood hydrodynamic theory and agreed well with a value of 1.31 predicted when incorporating a recently proposed expression for the radius of gyration of circular polymers into the Zimm model. circular ͉ polymer ͉ polyelectrolyte ͉ hydrodynamics ͉ excluded volume W hile many eukaryotic genomes are linear, prokaryotic genomes and most cloned DNA constructs are circular (1). Indeed, a commonly stated motivation for theoretical calculations on circular polymers is that they may be applicable to understanding the behavior of DNA. However, four of the five previously reported studies on the diffusion of circular polymers have used synthetic polymers, and only two of these, both using synthetic polymers, examined the dependence of the diffusion coefficient on molecular length. The dependence of D on length for relaxed circular DNA has never been measured. Here, we examine linear, relaxed circular, and supercoiled DNA molecules covering a wide range of lengths (Ϸ6 to 290 kbp).For long linear polymers in a good solvent, where excluded volume effects are appreciable, polymer physics theory (2) predicts D ϳ 1͞R G ϳ L Ϫ with Х 0.588, where R G is radius of gyration. The same scaling exponent has been calculated for both dynamic (D ϳ L Ϫ ) and static (R G ϳ L ) quantities, with nearly identical results determined by using a wide range of methods. Static scaling has been examined by using Monte Carlo simulations (3), bead-rod simulations (4), and cylindrical selfavoiding polygon models (5). Renormalization group theory methods have been used in both static (3, 6) and dynamic (7) calculations, and bond-fluctuation simulations (8) were used to measure and compare both scaling relationships. The predicted scaling exponent is close ...