Mechanisms for flexibility in DNA sequence recognition and VP16-induced complex formation by the Oct-1 POU domain.

DNA binding by the Oct-1 protein is directed by its POU domain, a bipartite DNA-binding domain made up of a POU-specific (POUS) domain and a POU-homeo (POUH) domain, two helix-turn-helix-containing DNA-binding modules that cooperate in DNA recognition. Although the best-characterized DNA target for Oct-1 binding is the octamer sequence ATGCAAAT, Oct-1 also binds a number of different DNA sequence elements. For example, Oct-1 recognizes a form of the herpes simplex virus VP16-responsive TAATGARAT element, called the (OCTA-)TAATGARAT site, that lacks octamer site similarity. Our studies suggest two mechanisms by which Oct-1 achieves flexible DNA sequence recognition. First, an important arginine found in the Oct-1 POUS domain tolerates substitutions of its base contacts within the octamer site. Second, on the (OCTA-)TAATGARAT site, the POUS domain is located on the side of the POUH domain opposite from where it is located on an octamer site. This flexibility of the Oct-1 POU domain in DNA binding also has an impact on its participation in a multiprotein-DNA complex with VP16. We show that Oct-1 POUS domain residues that contact DNA have different effects on VP16-induced complex formation depending on whether the VP16-responsive element involved has overlapping octamer similarity or not.     

Influence of the R823W mutation on the interaction of the ANKS6–ANKS3: insights from molecular dynamics simulation and free energy analysis

The sterile alpha motif (SAM) domain of the protein ANKS6, a protein–protein interaction domain, is responsible for autosomal dominant polycystic kidney disease. Although the disease is the result of the R823W point mutation in the SAM domain of the protein ANKS6, the molecular details are still unclear. We applied molecular dynamics simulations, the principal component analysis, and the molecular mechanics Poisson–Boltzmann surface area binding free energy calculation to explore the structural and dynamic effects of the R823W point mutation on the complex ANKS6–ANKS3 (PDB ID: 4NL9) in comparison to the wild proteins. The energetic analysis presents that the wild type has a more stable structure than the mutant. The R823W point mutation not only disrupts the structure of the ANKS6 SAM domain but also negatively affects the interaction of the ANKS6–ANKS3. These results further clarify the previous experiments to understand the ANKS6–ANKS3 interaction comprehensively. In summary, this study would provide useful suggestions to understand the interaction of these proteins and their fatal action on mediating kidney function.     

DNA recognition and nucleosome organization

The affinity of a DNA sequence for the histone octamer in a core nucleosome depends on the intrinsic flexibility of the DNA. This parameter can be affected both by the sequence-dependent conformational preferences of individual base steps and by the nature and location of the exocyclic groups of the DNA bases. By adopting highly preferred conformations particular types of base step can influence the rotational positioning of the DNA on the surface of the histone octamer. The asymmetry of the next higher order of chromatin structure is determined in part by the asymmetric binding of the globular domain of histone H5 to the core nucleosome. © 1998 John Wiley & Sons, Inc. Biopoly 44: 423–433 1997     

Structural biochemistry of a bacterial checkpoint protein reveals diadenylate cyclase activity regulated by DNA recombination intermediates

To reveal mechanisms of DNA damage checkpoint initiation, we structurally and biochemically analyzed DisA, a protein that controls a Bacillus subtilis sporulation checkpoint in response to DNA double-strand breaks. We find that DisA forms a large octamer that consists of an array of an uncharacterized type of nucleotide-binding domain along with two DNA-binding regions related to the Holliday junction recognition protein RuvA. Remarkably, the nucleotide-binding domains possess diadenylate cyclase activity. The resulting cyclic diadenosine phosphate, c-di-AMP, is reminiscent but distinct from c-di-GMP, an emerging prokaryotic regulator of complex cellular processes. Diadenylate cyclase activity is unaffected by linear DNA or DNA ends but strongly suppressed by branched nucleic acids such as Holliday junctions. Our data indicate that DisA signals DNA structures that interfere with chromosome segregation via c-di-AMP. Identification of the diadenylate cyclase domain in other eubacterial and archaeal proteins implies a more general role for c-di-AMP in prokaryotes.     

Structural basis for SRY-dependent 46-X,Y sex reversal: modulation of DNA bending by a naturally occurring point mutation

The HMG-box domain of the human male sex-determining factor SRY, hSRY(HMG) (comprising residues 57-140 of the full-length sequence), binds DNA sequence-specifically in the minor groove, resulting in substantial DNA bending. The majority of point mutations resulting in 46X,Y sex reversal are located within this domain. One clinical de novo mutation, M64I in the full-length hSRY sequence, which corresponds to M9I in the present hSRY(HMG) construct, acts principally by reducing the extent of DNA bending. To elucidate the structural consequences of the M9I mutation, we have solved the 3D solution structures of wild-type and M9I hSRY(HMG) complexed to a DNA 14mer by NMR, including the use of residual dipolar couplings to derive long-range orientational information. We show that the average bend angle (derived from an ensemble of 400 simulated annealing structures for each complex) is reduced by approximately 13 degrees from 54(+/-2) degrees in the wild-type complex to 41(+/-2) degrees in the M9I complex. The difference in DNA bending can be localized directly to changes in roll and tilt angles in the ApA base-pair step involved in interactions with residue 9 and partial intercalation of Ile13. The larger bend angle in the wild-type complex arises as a direct consequence of steric repulsion of the sugar of the second adenine by the bulky S(delta) atom of Met9, whose position is fixed by a hydrogen bond with the guanidino group of Arg17. In the M9I mutant, this hydrogen bond can no longer occur, and the less bulky C(gamma)m methyl group of Ile9 braces the sugar moieties of the two adenine residues, thereby decreasing the roll and tilt angles at the ApA step by approximately 8 degrees and approximately 5 degrees, respectively, and resulting in an overall difference in bend angle of approximately 13 degrees between the two complexes. To our knowledge, this is one of the first examples where the effects of a clinical mutation involving a protein-DNA complex have been visualized at the atomic level.     

Investigation of the Interaction Between Human Serum Albumin and Antitumor Palladium(II) Complex Containing 1,10-Phenanthroline and Dithiocarbamate Ligands

The interaction between [Pd(But-dtc)(phen)]NO₃ (where But-dtc = butyldithiocarbamate and phen = 1,10-phenanthroline) with HSA (Human Serum Albumin) was investigated by applying fluorescence, UV–Vis and circular dichroism techniques under physiological conditions. The results of fluorescence spectra indicated that the Pd(II) complex could effectively quench the fluorescence intensity of HSA molecules via static mechanism. The number of binding sites and binding constant of HSA–Pd(II) complex were calculated. Analysis of absorption titration data on the interaction between Pd(II) complex and HSA revealed the formation of HSA–Pd(II) complex with high-binding affinity. Thermodynamic parameters indicated that hydrophobic forces play a major role in this interaction. Furthermore, CD measurements were taken to explore changes in HSA secondary structure induced by the Pd(II) complex.     

Three-dimensional structure of the KChIP1-Kv4.3 T1 complex reveals a cross-shaped octamer

Brain I(A) and cardiac I(to) currents arise from complexes containing Kv4 voltage-gated potassium channels and cytoplasmic calcium-sensor proteins (KChIPs). Here, we present X-ray crystallographic and small-angle X-ray scattering data that show that the KChIP1-Kv4.3 N-terminal cytoplasmic domain complex is a cross-shaped octamer bearing two principal interaction sites. Site 1 comprises interactions between a unique Kv4 channel N-terminal hydrophobic segment and a hydrophobic pocket formed by displacement of the KChIP H10 helix. Site 2 comprises interactions between a T1 assembly domain loop and the KChIP H2 helix. Functional and biochemical studies indicate that site 1 influences channel trafficking, whereas site 2 affects channel gating, and that calcium binding is intimately linked to KChIP folding and complex formation. Together, the data resolve how Kv4 channels and KChIPs interact and provide a framework for understanding how KChIPs modulate Kv4 function.     

Yeast DNA recombination and repair proteins Rad 1 and Radio constitute a complex in vivo mediated by localized hydrophobic domains

The Saccharomyces cerevisiae Rad 1 and Rad 10 proteins are required for damage-specific incision during nucleotide excision repair and also for certain mitotic recombination events between repeated sequences. Previously we have demonstrated that Rad1 and Rad10 form a specific complex in vitro. Using the ‘two-hybrid’ genetic assay system we now report that Rad1 and Rad10 proteins are subunits of a specific complex in the cell nucleus. The Rad10-binding domain of Rad1 protein maps to a localized region between amino acids 809–997. The Rad1 -binding domain of Radio protein maps between amino acids 90–210. These domains are evolutionarily conserved and are hydrophobic in character. Although significant homology exists between Rad10 and the human-DNA-repair protein Ercc1 in this region, we were unable to detect any interaction between Ercc1 and Rad1 proteins. We conclude that Rad1 and Rad10 operate in DNA repair and mitotic recombination as a constitutive complex.     

Exploring CRD mobility during RAS/RAF engagement at the membrane

During the activation of mitogen-activated protein kinase (MAPK) signaling, the RAS-binding domain (RBD) and cysteine-rich domain (CRD) of RAF bind to active RAS at the plasma membrane. The orientation of RAS at the membrane may be critical for formation of the RAS-RBDCRD complex and subsequent signaling. To explore how RAS membrane orientation relates to the protein dynamics within the RAS-RBDCRD complex, we perform multiscale coarse-grained and all-atom molecular dynamics (MD) simulations of KRAS4b bound to the RBD and CRD domains of RAF-1, both in solution and anchored to a model plasma membrane. Solution MD simulations describe dynamic KRAS4b-CRD conformations, suggesting that the CRD has sufficient flexibility in this environment to substantially change its binding interface with KRAS4b. In contrast, when the ternary complex is anchored to the membrane, the mobility of the CRD relative to KRAS4b is restricted, resulting in fewer distinct KRAS4b-CRD conformations. These simulations implicate membrane orientations of the ternary complex that are consistent with NMR measurements. While a crystal structure-like conformation is observed in both solution and membrane simulations, a particular intermolecular rearrangement of the ternary complex is observed only when it is anchored to the membrane. This configuration emerges when the CRD hydrophobic loops are inserted into the membrane and helices α3–5 of KRAS4b are solvent exposed. This membrane-specific configuration is stabilized by KRAS4b-CRD contacts that are not observed in the crystal structure. These results suggest modulatory interplay between the CRD and plasma membrane that correlate with RAS/RAF complex structure and dynamics, and potentially influence subsequent steps in the activation of MAPK signaling.     

Structure prediction of a complex between the chromosomal protein HMG-D and DNA

Non-histone chromosomal proteins are an important part of nuclear structure and function due to their ability to interact with DNA to form and modulate chromatin structure and regulate gene expression. However, the understanding of the function of chromosomal proteins at the molecular level has been hampered by the lack of structures of chromosomal protein–DNA complexes. We have carried out a molecular dynamics modeling study to provide insight into the mode of DNA binding to the chromosomal HMG-domain protein, HMG-D. Three models of a complex of HMG-D bound to DNA were derived through docking the protein to two different DNA fragments of known structure. Molecular dynamics simulations of the complexes provided data indicating the most favorable model. This model was further refined by molecular dynamics simulation and extensively analyzed. The structure of the corresponding HMG-D-DNA complex exhibits many features seen in the NMR structures of the sequence-specific HMG-domain-DNA complexes, lymphoid enhancer factor 1 (LEF-1) and testis determining factor (SRY). The model reveals differences from these known structures that suggest how chromosomal proteins bind to many different DNA sequences with comparable affinity. Proteins 30:113–135, 1998. © 1998 Wiley-Liss, Inc.     

Molecular dynamics analysis of the engrailed homeodomain-DNA recognition

Molecular dynamics (MD) simulations were performed for investigating the role of Gln50 in the engrailed homeodomain-DNA recognition. Employing the crystal structure of free engrailed homeodomain and homeodomain-DNA complex as a starting structure, we carried out MD simulations of: (i) the complex between engrailed homeodomain and a 20 base-pair DNA containing TAATTA core sequence; (ii) the free engrailed homeodomain. The simulations show that homeodomain flexibility does not depend on its ligation state. The engrailed homeodomain shows similar flexibility, and the recognition helix-3 shows very similar characteristic of high rigidity and limited conformational space in two complexation states. At the same time, DNA structure has also no obvious conformational fluctuations. These results preclude the possibility of the side chain of Gln50 forming direct hydrogen bonds to the core DNA bases. MD simulations confirm a few well-conserved sites for water-mediated hydrogen bonds from protein to DNA are occupied by water molecules, and Gln50 interacts with corresponding core DNA bases through water-mediated hydrogen bonds. So Gln50 plays a relatively modest role in determining the affinity and specificity of the engrailed homeodomain. In addition, the electrostatic interaction between homeodomain and phosphate backbone of the DNA is a main factor for N- and C-terminal arm becoming ordered upon DNA binding.     

Investigation of cathepsin D–mAb interactions using a combined experimental and computational tool set

Cathepsin D has been identified as a challenge to remove in downstream bioprocessing of monoclonal antibodies (mAbs) due to interactions with some mAbs. This study focused on investigating the mechanisms of interaction between cathepsin D and two industrial mAbs using a combined experimental and computational approach. Surface plasmon resonance was used to study the impact of pH and salt concentration on these protein–protein interactions. While salt had a moderate effect on the interactions with one of the mAbs, the other mAb demonstrated highly salt-dependent association behavior. Cathepsin D binding to the mAbs was also seen to be highly pH dependent, with operation at pH 9 resulting in a significant decrease in the binding affinity. Protein–protein docking simulations identified three interaction sites on both mAbs; near the complementarity determining region (CDR), in the hinge, and in the C_H3 domain. In contrast, only one face of cathepsin D was identified to interact with all the three sites on the mAbs. Surface property analysis revealed that the binding regions on the mAbs contained strong hydrophobic clusters and were predominantly negatively charged. In contrast, the binding site on cathepsin D was determined to be highly positively charged and hydrophobic, indicating that these protein–protein interactions were likely due to a combination of hydrophobic and electrostatic interactions. Finally, covalent crosslinking coupled with mass spectrometry was used to validate the docking predictions and to further investigate the regions of interaction involved in mAb–cathepsin D binding. A strong agreement was observed between the two approaches, and the CDR loops were identified to be important for cathepsin D interactions. This study establishes a combined experimental and computational platform that can be used to probe mAb–host cell protein (HCP) interactions of importance in biomanufacturing.     

Recognition mechanism of Wilms’ tumour suppressor protein and DNA triplets: insights from molecular dynamics simulation and free energy analysis

The Wilms’ tumour suppressor protein (WT1) plays a multifaceted role in human cancer processes. Mutations on its DNA recognition domain could lead to Denys–Drash syndrome, and alternate splicing results in insertion of the tripeptide Lys–Thr–Ser (KTS) between the third and fourth zinc fingers (ZFs), leading to changes in the DNA-binding function. However, detailed recognition mechanisms of the WT1–DNA complex have not been explored. To clarify the mutational effects upon WT1 towards DNA binding at the atomic level, molecular dynamics simulations and the molecular mechanics/Poisson Boltzmann surface area (MM/PBSA) method were employed. The simulation results indicate that mutations in ZF domains (E427Q and Q369H) may weaken the binding affinity, and the statistical analyses of the hydrogen bonds and hydrophobic interactions show that eight residues (Lys351, Arg366, Arg375, Arg376, Lys399, Arg403, Arg424 and Arg430) have a significant influence on recognition and binding to DNA. Insertion of the tripeptide KTS could form an immobilized hydrogen-bonding network with Arg403, affecting the flexibility and angle of the linker between ZF3 and ZF4, thus influencing the recognition between the protein and the DNA triplet at its 5′ terminus. These results represent the first step towards a thorough characterization of the WT1 recognition mechanisms, providing a better understanding of the structure–function relationship of WT1 and its mutants.