Recent neutron scattering studies of muscle contraction and its control

We have presented two applications of the method of neutron scattering utilizing selective deuteration of actin. In these experiments the actin was rendered effectively invisible to neutrons by matching the scattering-length densities of deuterated actin and the solvent. The scattering of neutrons by myosin S1 and by Tm bound to this actin was studied. For free chymotrypsin-generated S1 it was found that Rg = 4.0 +/- 0.15 nm, while for papain-generated S1 it was found that Rg = 4.6 +/- 0.2 nm. Upon binding of papain-generated S1 to actin at low NS1/N actin ratios, the change in Rg in difference experiments was delta Rg = 0.05 +/- 0.15 nm. This lack of significant change in Rg in the very low-s domain confirms and extends our earlier neutron scattering work in the higher-s domain. The longest chords of S1, as well as shorter ones, are not significantly altered upon actin binding. These results indicate that muscle contraction does not occur as a result of large-scale changes in S1 structure. In actin-Tm complexes, a measurement of the mean cross-helix separation, d, of Tm molecules has been made using neutron scattering. With deuterated actin matched out in 93% D2O buffer, it was found that d = 7.9 +/- 0.3 nm. This value is in good agreement with a model based on Tm crystallography and also with recent electron microscopy results. These experiments demonstrate the feasibility and value of neutron diffraction and scattering techniques in the study of muscle contraction and its control. One can expect that the further employment of emerging cell biology techniques for generating deuterated proteins will aid our understanding of muscle in the future.

The sequence location of the actin metal

We have incorporated Fe2+ into the high-affinity metal-ion-binding site of actin. By supplying the system with oxygen from air and a reductant (dithiothreitol or ascorbate), we have induced free-radical generation, with the intent of causing peptide cleavage at the metal-ion-binding site. By analysis of the resulting fragments from actin in the F-form, we have deduced that cuts occurred at positions 159-160 and 301-302 (at the latter location we could not be sure if more than one cut occurred). We considered that these two cuts occurred in the chain strand coursing from the outer to the inner domain and vice-versa. Our results harmonize very well with the recently reported atomic structure of actin [Kabsch, W., Mannherz, H.G., Suck, D., Pai, E.F. & Holmes, K.C. (1990) Nature 347, 37-44] and remove ambiguities that had remained in the structure. The results partly bear out the homology-based prediction of Strzelecka-Golaszewska et al. [Strzelecka-Golaszewska, H., Boguta, G., Zmorzynshi, S. & Moraczcwska, J. (1989) Eur. J. Biochem. 182, 299-305].