Anisotropy Decay of Labelled Actin

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Abstract
G actin, labelled presumably on cysteine‐373 with the fluorescent chromophore N‐iodoacetylN′‐(5 sulfo‐1‐naphthyl)‐ethylenediamine and purified by Sephacryl S‐200 gel chromatography, migrated in one band on polyacrylamide gel electrophoresis and had the same polymerizability as unlabelled purified G actin. Anisotropy decays of labelled actin solutions have been studied at different ionic strengths and protein concentrations.It was found that these anisotropy decays could be fitted by a sum of two exponential functions. Under low ionic strength or below the critical concentrations the longer correlation time (45 ns at 3.5°C) was independent of protein concentration and ionic strength. Above the critical concentration, the longer correlation time increased with ionic strength and protein concentration. In order to take into account that, under these conditions, the solutions contained a mixture of F and G actin at the critical concentration, the anisotropy decays were analysed as a sum of three exponential functions in which the longest correlation time characterized F actin. Since F actin correlation time also depended on actin concentration, an analysis with a sum of four exponential functions was performed, in which two fixed correlation times (100 ns and 900 ns at 3.5°C) were introduced in order to characterize the F actin motions. The longer of these correlation times was attributed to regions where two actin filaments interact side by side, while the shorter one was attributed to filament regions free from intermolecular interactions.The small value of the free F actin correlation time indicates that the protomer peptide chain is very flexible around its C terminus, probably involving the motion of a molecular lobe. This flexibility might be an important factor in the interaction of actin with myosin during the muscular contraction.