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A glutamic acid was buried in the hydrophobic core of staphylococcal nuclease by replacement of Val-66. Its pK(a) was measured with equilibrium thermodynamic methods. It was 4.3 units higher than the pK(a) of Glu in water. This increase was comparable to the DeltapK(a) of 4.9 units measured previously for a lysine buried at the same location. According to the Born formalism these DeltapK(a) are energetically equivalent to the transfer of a charged group from water to a medium of dielectric constant of 12. In contrast, the static dielectric constants of dry protein powders range from 2 to 4. In the crystallographic structure of the V66E mutant, a chain of water molecules was seen that hydrates the buried Glu-66 and links it with bulk solvent. The buried water molecules have never previously been detected in >20 structures of nuclease. The structure and the measured energetics constitute compelling and unprecedented experimental evidence that solvent penetration can contribute significantly to the high apparent polarizability inside proteins. To improve structure-based calculations of electrostatic effects with continuum methods, it will be necessary to learn to account quantitatively for the contributions by solvent penetration to dielectric effects in the protein interior.

To quantitate the contributions of the large hydrophobic residues in staphylococcal nuclease to the stability of its native state, single alanine and glycine substitutions were constructed by site-directed mutagenesis for each of the 11 leucine, 9 valine, 7 tyrosine, 5 isoleucine, 4 methionine, and 3 phenylalanine residues. In addition, each isoleucine was also mutated to valine. The resulting collection of 83 mutant nucleases was submitted to guanidine hydrochloride denaturation using intrinsic tryptophan fluorescence to monitor the equilibrium constant between the native and denatured states. From analysis of these data, each mutant protein's stability to reversible denaturation (delta GH2O) and sensitivity to guanidine hydrochloride (mGuHCl or d(delta G)/d[GuHCl]) were obtained. Four unexpected trends were observed. (1) A striking bipartite distribution was found for sites of mutations that altered mGuHCl: mutations that increased this parameter only involved residues that contribute side chains to the major hydrophobic core centered around a five-strand beta-barrel, whereas mutations that caused mGuHCl to decrease clustered around a second, smaller and less well-defined hydrophobic core. (2) The average stability loss for mutants in each of the six residue classes was 2-3 times greater than that estimated on the basis of the free energy of transfer of the hydrophobic side chain from water to n-octanol. (3) The magnitude of the stability loss on substituting Ala or Gly for a particular type of amino acid varied extensively among the different sites of its occurrence in nuclease, indicating that the environment surrounding a specific residue determines how large a stability contribution its side chain will make.(ABSTRACT TRUNCATED AT 250 WORDS)

Lys-66 and Glu-66, buried in the hydrophobic interior of staphylococcal nuclease by mutagenesis, titrate with pK(a) values of 5.7 and 8.8, respectively (Dwyer et al., Biophys. J. 79:1610-1620; García-Moreno E. et al., Biophys. Chem. 64:211-224). Continuum calculations with static structures reproduced the pK(a) values when the protein interior was treated with a dielectric constant (epsilon(in)) of 10. This high apparent polarizability can be rationalized in the case of Glu-66 in terms of internal water molecules, visible in crystallographic structures, hydrogen bonded to Glu-66. The water molecules are absent in structures with Lys-66; the high polarizability cannot be reconciled with the hydrophobic environment surrounding Lys-66. Equilibrium thermodynamic experiments showed that the Lys-66 mutant remained folded and native-like after ionization of the buried lysine. The high polarizability must therefore reflect water penetration, minor local structural rearrangement, or both. When in pK(a) calculations with continuum methods, the internal water molecules were treated explicitly, and allowed to relax in the field of the buried charged group, the pK(a) values of buried residues were reproduced with epsilon(in) in the range 4-5. The calculations show that internal waters can modulate pK(a) values of buried residues effectively, and they support the hypothesis that the buried Lys-66 is in contact with internal waters even though these are not seen crystallographically. When only the one or two innermost water molecules were treated explicitly, epsilon(in) of 5-7 reproduced the pK(a) values. These values of epsilon(in) > 4 imply that some conformational reorganization occurs concomitant with the ionization of the buried groups.

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The dielectric properties of proteins are poorly understood and difficult to describe quantitatively. This limits the accuracy of methods for structure-based calculation of electrostatic energies and pK(a) values. The pK(a) values of many internal groups report apparent protein dielectric constants of 10 or higher. These values are substantially higher than the dielectric constants of 2-4 measured experimentally with dry proteins. The structural origins of these high apparent dielectric constants are not well understood. Here we report on structural and equilibrium thermodynamic studies of the effects of pH on the V66D variant of staphylococcal nuclease. In a crystal structure of this protein the neutral side chain of Asp-66 is buried in the hydrophobic core of the protein and hydrated by internal water molecules. Asp-66 titrates with a pK(a) value near 9. A decrease in the far UV-CD signal was observed, concomitant with ionization of this aspartic acid, and consistent with the loss of 1.5 turns of alpha-helix. These data suggest that the protein dielectric constant needed to reproduce the pK(a) value of Asp-66 with continuum electrostatics calculations is high because the dielectric constant has to capture, implicitly, the energetic consequences of the structural reorganization that are not treated explicitly in continuum calculations with static structures.

Water motion at protein surfaces is fundamental to protein structure, stability, dynamics, and function. By using intrinsic tryptophans as local optical probes, and with femtosecond resolution, it is possible to probe surface-water motions in the hydration layer. Here, we report our studies of local hydration dynamics at the surface of the enzyme Staphylococcus nuclease using site-specific mutations. From these studies of the WT and four related mutants, which change local charge distribution and structure, we are able to ascertain the contribution to solvation by protein side chains as relatively insignificant. We determined the time scales of hydration to be 3-5 ps and 100 -150 ps. The former is the result of local librational͞rotational motions of water near the surface; the latter is a direct measure of surface hydration assisted by fluctuations of the protein. Experimentally, these hydration dynamics of the WT and the four mutants are also consistent with results of the total dynamic Stokes shifts and fluorescence emission maxima and are correlated with their local charge distribution and structure. We discuss the role of protein fluctuation on the time scale of labile hydration and suggest reexamination of recent molecular dynamics simulations.protein hydration ͉ femtosecond dynamics ͉ protein fluctuation ͉ selective mutation F rom the laboratories of the senior authors of this study (A.H.Z. and D.Z.) (1-11), there has been a series of reports regarding the time and length scales of the water layer around protein surfaces. These studies were for proteins subtilisin Carlsberg (2), monellin (3), phospholipase A 2 (5), melittin (9), and human serum albumin (8, 10). A theoretical model was developed to take into account the exchange with bulk water (4, 12), and the dynamics are consistent with molecular dynamics (MD) simulations of residence times (13-16) on time scales from femtoseconds to picoseconds. Earlier NMR studies have reported hydration dynamics (residence times) in the subnanosecond regime (17-20), but, more recently, a claim has been made that water motions at protein surfaces are ultrafast compared with bulk water, only slowing down by a factor of two to three (21,22). This Ͻ10-ps range would imply that the observed long-time hydration dynamics in tens of picoseconds are due to protein side-chain relaxation (22, 23). In our earlier studies (6), we addressed in detail this issue and the reasons for dominance of hydration dynamics. To quantify the contribution of sidechain motions to total solvation on the time scale of hydration, we must carefully alter the local structure while maintaining the same tryptophan site.In this contribution, we report the effect of mutation (four mutants on three site selections and the WT) on hydration of the enzyme Staphylococcus nuclease (SNase). Fig. 1 shows the x-ray structure of the protein, consisting of three ␣-helices and a five-stranded ␤-barrel with a total of 149 amino acids (24). The only single tryptophan residue (W140) has one edge exposed to the surface ...

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