Solution structures of staphylococcal nuclease from multidimensional, multinuclear NMR: nuclease-H124L and its ternary complex with Ca2+ and thymidine-3',5'-bisphosphate.

The solution structures of staphylococcal nuclease (nuclease) H124L and its ternary complex, (nuclease-H124L).pdTp.Ca2+, were determined by ab initio dynamic simulated annealing using 1925 NOE, 119 phi, 20 chi 1 and 112 hydrogen bond constraints for the free protein, and 2003 NOE, 118 phi, 20 chi 1 and 114 hydrogen bond constraints for the ternary complex. In both cases, the final structures display only small deviations from idealized covalent geometry. In structured regions, the overall root-mean-square deviations from mean atomic coordinates are 0.46 (+/- 0.05) A and 0.41 (+/- 0.05) A for the backbone heavy atoms of nuclease and its ternary complex, respectively. The backbone conformations of residues in the loop formed by Arg81-Gly86, which is adjacent to the active site, are more precisely defined in the ternary complex than in unligated nuclease. Also, the protein side chains that show NOEs and evidence for hydrogen bonds to pdTp (Arg35, Lys84, Tyr85, Arg87, Tyr113, and Tyr115) are better defined in the ternary complex. As has been observed previously in the X-ray structures of nuclease-WT, the binding of pdTp causes the backbone of Tyr113 to change from an extended to a left-handed alpha-helical conformation. The NMR structures reported here were compared with available X-ray structures: nuclease-H124L [Truckses et al. (1996) Protein Sci., 5, 1907-1916] and the ternary complex of wild-type staphylococcal nuclease [Loll and Lattman (1989) Proteins Struct. Funct. Genet., 5, 183-201]. Overall, the solution structures of nuclease-H124L are consistent with these crystal structures, but small differences were observed between the structures in the solution and crystal environments. These included differences in the conformations of certain side chains, a reduction in the extent of helix 1 in solution, and many fewer hydrogen bonds involving side chains in solution.

Coupling between trans/cis proline isomerization and protein stability in staphylococcal nuclease.

The nucleases A produced by two strains of Staphylococcus aureus, which have different stabilities, differ only in the identity of the single amino acid at residue 124. The nuclease from the Foggi strain of S. aureus (by convention nuclease WT), which contains His124, is 1.9 kcal.mol-1 less stable (at pH 5.5 and 20 degrees C) than the nuclease from the V8 strain (by convention nuclease H124L), which contains Leu124. In addition, the population of the trans conformer at the Lys116-Pro117 peptide bond, as observed by NMR spectroscopy, is different for the two variants: about 15% for nuclease WT and 9% for nuclease H124L. In order to improve our understanding of the origin of these differences, we compared the properties of WT and H124L with those of the H124A and H124I variants. We discovered a correlation between effects of different residues at this position on protein stability and on stabilization of the cis configuration of the Lys116-Pro117 peptide bond. In terms of free energy, approximately 17% of the increase in protein stability manifests itself as stabilization of the cis configuration at Lys116-Pro117. This result implies that the differences in stability arise mainly from structural differences between the cis configurational isomers at Pro117 of the different variants at residue 124. We solved the X-ray structure of the cis form of the most stable variant, H124L, and compared it with the published high-resolution X-ray structure of the cis form of the most stable variant, WT (Hynes TR, Fox RO, 1991, Proteins Struct Funct Genet 10:92-105). The two structures are identical within experimental error, except for the side chain at residue 124, which is exposed in the models of both variants. Thus, the increased stability and changes in the trans/cis equilibrium of the Lys116-Pro117 peptide bond observed in H124L relative to WT are due to subtle structural changes that are not observed by current structure determination technique. Residue 124 is located in a helix. However, the stability changes are too large and follow the wrong order of stability to be explained simply by differences in helical propensity. A second site of conformational heterogeneity in native nuclease is found at the His46-Pro47 peptide bond, which is approximately 80% trans in both WT and H124L. Because proline to glycine substitutions at either residue 47 or 117 remove the structural heterogeneity at that position and increase protein stability, we determined the X-ray structures of H124L + P117G and H124L + P47G + P117G and the kinetic parameters of H124L, H124L + P47G, H124L + P117G, and H124L + P47G + P117G. The individual P117G and P47G mutations cause decreases in nuclease activity, with kcat affected more than Km, and their effects are additive. The P117G mutation in nuclease H124L leads to the same local conformational rearrangement described for the P117G mutant of WT (Hynes TR, Hodel A, Fox RO, 1994, Biochemistry 33:5021-5030). In both P117G mutants, the loop formed by residues 112-117 is located closer to the adjacent loop formed by residues 77-85, and residues 115-118 adopt a type I' beta-turn conformation with the Lys116-Gly117 peptide bond in the trans configuration, as compared with the parent protein in which these residues have a typeVIa beta-turn conformation with the Lys116-Pro117 peptide bond in the cis configuration. Addition of the P47G mutation appears not to cause any additional structural changes. However, the electron density for part of the loop containing this peptide bond was not strong enough to be interpreted.

Engineered disulfide bonds in staphylococcal nuclease: effects on the stability and conformation of the folded protein.

Efforts to enhance the stability of proteins by introducing engineered disulfide bonds have resulted in mixed success. Most approaches to the prediction of the energetic consequences of disulfide bond formation in proteins have considered only the destabilizing effects of cross-links on the unfolded state (chain entropy model) [Pace, C. N., Grimsley, G. R., Thomson, J. A., & Barnett, B. J. (1988) J. Biol. Chem. 263, 11820-11825: Doig, A. J., & Williams, D. H. (1991) J. Mol. Biol. 217, 389-398]. It seems clear, however, that disulfide bridges also can influence the stability of the native state. In order to assess the importance of the latter effect, we have studied four variants of staphylococcal nuclease (V8 strain) each containing one potential disulfide bridge created by changing two wild-type residues to cysteines by site-directed mutagenesis. In each case, one of the introduced cysteines was within the type VIa beta turn containing cis Pro117, and the other was located in the adjacent extended loop containing Gly79. In all four cases, the overall loop size was kept nearly constant (the number of residues in the loop between the two cysteines varied from 37 to 42) so as to minimize differences from chain entropy effects. The objective was to create variants in which a change in the reduction state of the disulfide would be coupled to a change in the position of the equilibrium between the cis and trans forms of the Xxx116-Pro117 peptide bond in the folded state of the protein. The position of this equilibrium, which can be detected by NMR spectroscopy, has been shown previously to correlate with the stability of the native protein. Its determination provides a measure of strain in the folded state. The thermal stabilities and free energies for unfolding by elevated temperature and guanidinium chloride were measured for each of the four mutants under conditions in which the introduced cysteines were cross-linked (oxidized) and unlinked (reduced). In addition, reduction potentials were determined for each mutant. Formation of the different disulfide bridges was found to induce varying levels of folded state strain. The stabilization energy of a given disulfide bridge could be predicted from the measured perturbation energy for the peptide bond isomerization, provided that energetic effects on the unfolded state were calculated according to the chain entropy model. Undiagnosed strain in native states of proteins may explain the variability observed in the stabilization provided by engineered disulfide bridges.

High-pressure denaturation of staphylococcal nuclease proline-to-glycine substitution mutants.

Our recently reported pressure-jump relaxation kinetics experiments on staphylococcal nuclease folding and unfolding [Vidugiris et al. (1995) Biochemistry 34, 4909] demonstrated that both transitions exhibit positive activation volumes, with that of folding being much larger than that of unfolding. Thus high pressure denatures proteins by slowing the rate of folding more than that of unfolding. In the present work, we take advantage of the very slow folding and unfolding rates under pressure to examine the kinetics and volume changes along the reaction coordinate for protein folding-unfolding for an interesting set of mutants of staphylococcal nuclease: P42G, P47G, P117G, and the double mutant, P47G+P117G. Previous studies have shown that replacement of an individual proline residue at position 42, 47, or 117 by glycine leads to paradoxical protein stabilization against denaturation by guanidine chloride, high temperature, or high pressure. In order to observe unfolding over an attainable pressure range, guanidine hydrochloride was employed. Within experimental error, the activation volumes and equilibrium volume changes were independent of the concentration of this denaturant and our analysis of the rate constants is consistent with the generally accepted hypothesis that this denaturant acts both by increasing the rate of unfolding and decreasing the rate of folding. We show that the stabilization resulting from each of the proline-to-glycine substitutions arises primarily from a decrease in the unfolding rate, and to a small degree, from an increase in the folding rate. The changes in rate constants upon proline-to-glycine substitution can be modeled in terms of small stabilization of the unfolded state, a greater stabilization of the transition state, and a still greater stabilization of the folded state. Although the rates were found to change for all of the mutants in the set, no changes greater than experimental error were found in the corresponding equilibrium volume changes and activation volumes for folding and unfolding. At low pressures (well below the onset of unfolding) the pressure-jump relaxation profiles for wild type proteins (both Foggi and V8) showed kinetic complexity. Although the effect was attenuated somewhat in pressure-jump profiles of one proline-to-glycine mutant (P42G), its persistence in data from all the mutants studied leads us to conclude that its origin is not cis/trans peptide bond isomerization at proline 117, 47, or 42.

Holographic methods in X-ray crystallography. IV. A fast algorithm and its application to macromolecular crystallography.

The holographic method makes use of partially modeled electron density and experimentally measured structure-factor amplitudes to recover electron density corresponding to the unmodeled part of a crystal structure. This paper describes a fast algorithm that makes it possible to apply the holographic method to sizable crystallographic problems. The algorithm uses positivity constraints on the electron density and can incorporate a 'target' electron density, making it similar to solvent flattening. The potential for applying the holographic method to macromolecular X-ray crystallography is assessed using both synthetic and experimental data.

Helix propagation in trifluoroethanol solutions.

Helix propagation of the S-peptide sequence (residues 1-19 of ribonuclease A) in 2,2,2-trifluoroethanol (TFE) solutions has been investigated with CD and nmr Overhauser effect spectroscopies. In this study, the S-peptide helix is covalently initiated at the N-terminus through disulfide bonds to a helix scaffold derived from the N-terminal sequence of the bee venom peptide apamin. The entire S-peptide sequence of this hybrid sequence peptide becomes helical at high proportions of TFE. Residues 14-19 of the S-peptide are not helical in the free peptide in TFE, nor are they helical in ribonuclease A. The "helix stop" signal encoded by the S-peptide sequence near residue 13 does not persist at high TFE with this hybrid sequence peptide. The helix-stabilizing effects of TFE are due at least in part to facilitated propagation of an extant helix. This stabilizing effect appears to be a general solvation effect and not due to specific interaction of the helical peptide with TFE. Specifically these data support the idea that TFE destabilizes the coil state by less effective hydrogen bonding of the peptide amide to the solvent.