Interaction of human SRY protein with DNA: a molecular dynamics study

Molecular dynamics simulations have been conducted to study the interaction of human sex-determining region Y (hSRY) protein with DNA. For this purpose, simulations of the hSRY high mobility group (HMG) domain (hSRY-HMG) with and without its DNA target site, a DNA octamer, and the DNA octamer alone have been carried out, employing the NMR solution structure of hSRY-HMG-DNA complex as a starting model. Analyses of the simulation results demonstrated that the interaction between hSRY and DNA was hydrophobic, just a few hydrogen bonds and only one water molecule as hydrogen-bonding bridge were observed at the protein-DNA interface. These two hydrophobic cores in the hSRY-HMG domain were the physical basis of hSRY-HMG-DNA specific interaction. They not only maintained the stability of the complex, but also primarily caused the DNA deformation. The salt bridges formed between the positive-charged residues of hSRY and phosphate groups of DNA made the phosphate electroneutral, which was advantageous for the deformation of DNA and the formation of a stable complex. We predicted the structure of hSRY-HMG domain in the free state and found that both hSRY and DNA changed their conformations to achieve greater complementarity of geometries and properties during the binding process; that is, the protein increased the angle between its long and short arms to accommodate the DNA, and the DNA became bent severely to adapt to the protein, although the conformational change of DNA was more severe than that of the hSRY-HMG domain. The sequence specificity and the role of residue Met9 are also discussed.     

DNA structure and fluctuations sensed from a 1.1ns molecular dynamics trajectory of a fully charged Zif268-DNA complex in water

The microcystin-RR structures are compared with the structures of microcystin-LR in solution as well as in the crystal structure of the complex with protein phosphatase. The gross structures of the two peptides are similar, but with a more accentuated and compact saddle structure for microcystin-RR. The structural differences affect the hydrogen-bond pattern in the peptides and the location of the side chain of N-methyldehydroalanine, both of which are important for the ability of the peptide to form a tight complex with protein phosphatase. These structural differences may contribute to the observed differences in toxicity of microcystin-RR and microcystin-LR.     

Motional dynamics of residues in a beta-hairpin peptide measured by 13C-NMR relaxation

Structurally characterizing partially folded peptides is problematic given the nature of their transient conformational states. 13C-NMR relaxation data can provide information on the geometry of bond rotations, motional restrictions, and correlated bond rotations of the backbone and side chains and, therefore, is one approach that is useful to assess the presence of folded structure within a conformational ensemble. A peptide 12mer, R1GITVNG7KTYGR12, has been shown to partially fold in a relatively stable beta-hairpin conformation centered at NG. Here, five residues, G2, V5, G7, Y10, G11, were selectively 13C-enriched, and 13C-NMR relaxation experiments were performed to obtain auto- and cross-correlation motional order parameters, correlation times, bond rotation angular variances, and bond rotational correlation coefficients. Our results indicate that, of the three glycines, G7 within the hairpin beta-turn displays the most correlated phi(t),psi(t) rotations with its axis of rotation bisecting the angle defined by the H-C-H bonds. These positively correlated bond rotations give rise to "twisting" type motions of the HCH group. V5 and Y10 phi,psi bond rotations are also positively correlated, with their CbetaCalphaH groups undergoing similar "twisting" type motions. Motions of near-terminal residues G2 and G11 are less restricted and less correlated and are best described as wobbling-in-a-cone. V5 and Y10 side-chain motions, aside from being highly restricted, were found to be correlated with phi,psi bond rotations. At 303 K, where the hairpin is considered "unfolded," the peptide exists in a transient, collapsed state because backbone and side-chain motions of V5, G7, and Y10 remain relatively restricted, unlike their counterparts in GXG-based tripeptides. These results provide unique information toward understanding conformational variability in the unfolded state of proteins, which is necessary to solve the protein folding problem.