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Apostolos G Gittis

Publications and source records attributed to Apostolos G Gittis.

5 recordsLinked to original sources

High apparent dielectric constant inside a protein reflects structural reorganization coupled to the ionization of an internal Asp.

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.

Aspartic Acid↗

Influence of ions, hydration, and the transcriptional inhibitor P4N on the conformations of the Sp1 binding site.

Three crystal structures containing the entire Sp1 consensus sequence d(GGGGCGGGG) with two or three additional base-pairs on either the 5' or 3' ends and overhangs have been determined. Despite the different lengths of DNA in the pseudo-dodecamers and pseudo-tridecamer, all three structures form A-DNA duplexes that share a common set of crystal contacts, including a T*(G.C) base triplet and a 5'-overhang that flips out and away from the helical axes to form a Hoogsteen base-pair with the 3'-overhang of a symmetry mate. The global conformations of the three structures differ, however, in the widths of their respective major grooves, the lengths of the molecules, and the extent of crystal packing. The structures were determined from crystals grown in an unusual precipitant for A-DNA, polyethylene glycol (PEG) 400, in combination with polyamines or ions; cobalt hexamine for the pseudo-tridecamer, and spermidine for the pseudo-dodecamers. As the Sp1 binding site is a target for antiviral and anticancer drugs, pseudo-dodecamer crystals were soaked with one such antiviral and anticancer compound, P4N. Although P4N was not visualized unambiguously in the electron density maps, the effect of the drug is evident from significant differences in the lattice constants, crystal packing, and overall conformation of the structure.

Base Sequence↗

X-ray and thermodynamic studies of staphylococcal nuclease variants I92E and I92K: insights into polarity of the protein interior.

We have used crystallography and thermodynamic analysis to study nuclease variants I92E and I92K, in which an ionizable side-chain is placed in the hydrophobic core of nuclease. We find that the energetic cost of burying ionizable groups is rather modest. The X-ray determinations show water molecules solvating the buried glutamic acid under cryo conditions, but not at room temperature. The lysine side-chain does not appear solvated in either case. Guanidine hydrochloride (GnHCl) denaturation of I92E and I92K, done as a function of pH and monitored by tryptophan fluorescence, showed that I92E and I92K are folded in the pH range pH 3.5-9.0 and pH 5.5-9.5, respectively. The stability of the parental protein is independent of pH over a broad range. In contrast, the stabilities of I92E and I92K exhibit a pH dependence, which is quantitatively explained by thermodynamic analysis: the PK(a) value of the buried K92 is 5.6, while that of the buried E92 is 8.65. The free energy difference between burying the uncharged and charged forms of the groups is modest, about 6 kcal/mol. We also found that epsilon(app) for I92K and I92E is in the range approximately 10-12, instead of 2-4 commonly used to represent the protein interior. Side-chains 92E and 92K were uncharged under the conditions of the X-ray experiment. Both are buried completely inside the well-defined hydrophobic core of the variant proteins without forming salt-bridges or hydrogen bonds to other functional groups of the proteins. Under cryo conditions 92E shows a chain of four water molecules, which hydrate one oxygen atom of the carboxyl group of the glutamic acid. Two other water molecules, which are present in the wild-type at all temperatures, are also connected to the water ring observed inside the hydrophobic core. The ready burial of water with an uncharged E92 raises the possibility that solvent excursions into the interior also take place in the wild-type protein, but in a random, dynamic way not detectable by crystallography. Such transient excursions could increase the average polarity, and thus epsilon(app), of the protein interior.

Crystallography, X-Ray↗

A compact RNA tertiary structure contains a buried backbone-K+ complex.

The structure of a 58 nucleotide ribosomal RNA fragment buries several phosphate groups of a hairpin loop within a large tertiary core. During refinement of an X-ray crystal structure containing this RNA, a potassium ion was found to be contacted by six oxygen atoms from the buried phosphate groups; the ion is contained completely within the solvent-accessible surface of the RNA. The electrostatic potential at the ion chelation site is unusually large, and more than compensates for the substantial energetic penalties associated with partial dehydration of the ion and displacement of delocalized ions. The very large predicted binding free energy, approximately -30 kcal/mol, implies that the site must be occupied for the RNA to fold. These findings agree with previous studies of the ion-dependent folding of tertiary structure in this RNA, which concluded that a monovalent ion was bound in a partially dehydrated environment where Mg2+ could not easily compete for binding. By compensating the unfavorable free energy of buried phosphate groups with a chelated ion, the RNA is able to create a larger and more complex tertiary fold than would be possible otherwise.

Base Sequence↗