Random walks have been used to describe a wide variety of systems ranging from cell colonies to polymers. Sixty-five years ago, Kuhn [Kuhn, W. (1934) Kolloid-Z. 68, 2-11] made the prediction, backed later by computer simulations, that the overall shape of a random-walk polymer is aspherical, yet no experimental work has directly tested Kuhn's general idea and subsequent computer simulations. By using fluorescence microscopy, we monitored the conformation of individual, long, random-walk polymers (fluorescently labeled DNA molecules) at equilibrium. We found that a polymer most frequently adopts highly extended, nonfractal structures with a strongly anisotropic shape. The ensemble-average ratio of the lengths of the long and short axes of the best-fit ellipse of the polymer was much larger than unity. R andom walks have been extensively used to describe a multitude of phenomena, ranging from cell migration within connective tissues, to Markov processes in DNA sequences, to time series in the stock market, to diffusion in gas, liquids, and solids (1-5). Sixty-five years ago, Kuhn (6) predicted that the shape of a random-walk polymer is not spherically symmetric, i.e., a regular random walk has an overall shape which is anisotropic. The intuitive idea of a spherical shape is based on a flexible polymer (or a random walk) having an isotropic end-to-end vector distribution and on the implicit rotational averaging typically done in polymer theories and experiments (7-10), yet the shape of individual polymers has not been probed directly (5, 9).The lack of direct conformational information has so far prevented a direct test of Kuhn's prediction (6), which is supported by computer simulations (11-16) and analytical calculations (5). Bulk measurements such as light scattering and rheology (17, 18) are inappropriate to probe the behavior of individual polymers in solution. These bulk experimental methods average the orientation, shape, and dynamics of a large ensemble of molecules simultaneously. Here, by monitoring the conformation, orientation, and dynamics of individual flexible polymers in dilute solutions, we directly measure the distributions of conformational parameters. We therefore test Kuhn's central prediction directly.
Materials and MethodsLight microscopy (Nikon) equipped with a ϫ100, n.a. 1.30, oil-immersion lens was used to monitor the conformation of individual, fluorescently labeled DNA molecules at equilibrium. We used monodisperse Coliphage T2-phage DNA (T2-DNA) molecules (19) suspended at a concentration Ϸ20 ng͞ml (much smaller than the overlap concentration Ϸ0.13 mg͞ml) in Tris⅐EDTA buffer and an oxygen-scavenging system to reduce photobleaching (20)(21)(22). DNA molecules were stained with an intercalating dye (YOYO-1, Molecular Probes), which we verified did not affect the overall shape distribution of DNA. T2-DNA is a highly flexible polymer with a contour length of L Ϸ 56 m and a persistence length of l p Ϸ 52 nm. Hence, this polymer is a linear sequence of Ϸ1,075 (ϭ L͞l P Ͼ Ͼ 1) statistical segme...