Analysis of stress in the active site of myosin accompanied by conformational changes in transient state intermediate complexes using photoaffinity labeling and 19F-NMR spectroscopy

Asymmetry of the GroEL-GroES complex under physiological conditions as revealed by small-angle x-ray scattering

Despite the well-known functional importance of GroEL-GroES complex formation during the chaperonin cycle, the stoichiometry of the complex has not been clarified. The complex can occur either as an asymmetric 1:1 GroEL-GroES complex or as a symmetric 1:2 GroEL-GroES complex, although it remains uncertain which type is predominant under physiological conditions. To resolve this question, we studied the structure of the GroEL-GroES complex under physiological conditions by small-angle x-ray scattering, which is a powerful technique to directly observe the structure of the protein complex in solution. We evaluated molecular structural parameters, the radius of gyration and the maximum dimension of the complex, from the x-ray scattering patterns under various nucleotide conditions (3 mM ADP, 3 mM ATP gamma S, and 3 mM ATP in 10 mM MgCl(2) and 100 mM KCl) at three different temperatures (10 degrees C, 25 degrees C, and 37 degrees C). We then compared the experimentally observed scattering patterns with those calculated from the known x-ray crystallographic structures of the GroEL-GroES complex. The results clearly demonstrated that the asymmetric complex must be the major species stably present in solution under physiological conditions. On the other hand, in the presence of ATP (3 mM) and beryllium fluoride (10 mM NaF and 300 microM BeCl(2)), we observed the formation of a stable symmetric complex, suggesting the existence of a transiently formed symmetric complex during the chaperonin cycle.

Trinitrophenylated reactive lysine residue in myosin detects lever arm movement during the consecutive steps of ATP hydrolysis

Trinitrophenylation of the reactive lysine (Lys84) in skeletal myosin subfragment 1 (S1) introduces a chiral probe (TNP) into an interface of the catalytic and lever arm domains of S1 [Muhlrad (1977) Biochim. Biophys. Acta 493, 154-166]. Characteristics of the TNP absorption and circular dichroism (CD) spectra in TNP-modified S1 (TNP-Lys84-S1), and the Lys84 trinitrophenylation rate in native S1, indicate a one-to-one correspondence between ATPase transients and trapped phosphate analogues. Phosphate analogue-induced structures of TNP-Lys84-S1 were modeled using the crystallographic coordinates of S1 [Rayment et al. (1993) Science 261, 50-58] with swivels at Gly699 and Gly710 to approximate conformational changes during ATPase. The CD and absorption spectral characteristics of the model structures were compared to those observed for analogue-induced structures. The model calculations, first tested on a trinitrophenylated hexapeptide with known structure, were applied to TNP-Lys84-S1. They showed that ATP binding initiates swiveling at Gly699 and that swiveling at both Gly710 and Gly699 accompanied ATP splitting just prior to product release. The computed lever arm trajectory during ATPase suggests (i) a plausible mechanism for the nucleotide-induced inhibition of Lys84 trinitrophenylation, and (ii) trinitrophenylation-induced changes in S1 Mg2+- and K+-EDTA ATPase are from collision of the lever arm with TNP at Lys84. TNP is a site-specific structural perturbant of S1 and a chiral reporter group for the effect of Lys84 modification on dynamic S1 structure. As such, TNP-Lys84-S1 is equivalent to a genetically engineered mutant with intrinsic sensitivity to structure local to the modified residue.