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Amino acid selective isotope labeling is an important nuclear magnetic resonance technique, especially for larger proteins, providing strong bases for the unambiguous resonance assignments and information concerning the structure, dynamics, and intermolecular interactions. Amino acid selective 15N labeling suffers from isotope dilution caused by metabolic interconversion of the amino acids, resulting in isotope scrambling within the target protein. Carbonyl 13C atoms experience less isotope scrambling than the main-chain 15N atoms do. However, little is known about the side-chain 13C atoms. Here, the 13C scrambling profiles of the Cα and side-chain carbons were investigated for 15N scrambling-prone amino acids, such as Leu, Ile, Tyr, Phe, Thr, Val, and Ala. The level of isotope scrambling was substantially lower in 13Cα and 13C side-chain labeling than in 15N labeling. We utilized this reduced scrambling-prone character of 13C as a simple and efficient method for amino acid selective 13C labeling using an Escherichia coli cold-shock expression system and high-cell density fermentation. Using this method, the 13C labeling efficiency was >80% for Leu and Ile, ∼60% for Tyr and Phe, ∼50% for Thr, ∼40% for Val, and 30-40% for Ala. 1H-15N heteronuclear single-quantum coherence signals of the 15N scrambling-prone amino acid were also easily filtered using 15N-{13Cα} spin-echo difference experiments. Our method could be applied to the assignment of the 55 kDa protein.

The Escherichia coli Orf135 protein, a MutT-type enzyme, hydrolyzes mutagenic 2-hydroxy-dATP (2-OH-dATP) and 8-hydroxy-dGTP, in addition to dCTP and 5-methyl-dCTP, and its deficiency causes increases in both the spontaneous and H(2)O(2)-induced mutation frequencies. To identify the amino acid residues that interact with these nucleotides, the Glu-33, Arg-72, Arg-77, and Asp-118 residues of Orf135, which are candidates for residues interacting with the base, were substituted, and the enzymatic activities of these mutant proteins were examined. The mutant proteins with a substitution at the 33rd, 72nd, and 118th amino acid residues displayed activities affected to various degrees for each substrate, suggesting the involvement of these residues in substrate binding. On the other hand, the mutant protein with a substitution at the 77th Arg residue had activitiy similar to that of the wild-type protein, excluding the possibility that this Arg side chain is involved in base recognition. In addition, the expression of some Orf135 mutants in orf135(-) E. coli reduced the level of formation of rpoB mutants elicited by H(2)O(2). These results reveal the residues involved in the substrate binding of the E. coli Orf135 protein.

High Mobility Group Box 1 (HMGB1) protein, a potential therapeutic target, binds bent DNAs structure-specifically. Here we report on a crucial structural feature of the bent DNA required for strong binding to HMGB1. NMR structures of two bent DNA oligomers, only one of which binds strongly to HMGB1, revealed that the presence of a pocket structure on the minor groove is crucial for strong binding through penetration of a phenylalanine residue.

In DNA duplexes, pyrimidine-purine steps are believed to be flexible or conformationally unstable. Indeed, several DNA crystal structures exhibit a multitude of conformations for CpA*TpG steps. The question arises of whether this structural flexibility is accompanied by dynamical flexibility, i.e., a question pertaining to the energy barrier between conformations. Except for TpA steps, slow motions on the microsecond-to-millisecond time scale have not been detected in duplexes until now. In the present study, such slow motion was investigated by 1H, 13C, and 15N NMR relaxation measurements on a DNA decamer d(CATTTGCATC)*d(GATGCAAATG). The DNA decamer was enriched with 15% 13C and 98% 15N isotopes for each adenosine and guanosine residue. Three lines of evidence support the notion of slow motion in the CAA*TTG moiety. Analysis of (15)N relaxation showed that the order parameter, S2, of guanosine imino NH groups was about 0.8, similar to that of CH groups for this oligomer. The strong temperature dependence of guanosine NH S2 in the CAA*TTG sequence indicated the presence of a large-amplitude motion. Signals of adenosine H8 protons in the CAA*TTG sequence were broadened in 2D 1H NOESY spectra, which also suggested the existence of slow motion. As well as being smaller than for other adenine residues, the 1H T2 values exhibited a magnetic field strength dependence for all adenosine H8 signals in the ATTTG*CAAAT region, suggesting slow motions more pronounced at the first adenosine in the CAA*TTG sequence but extending over the CAAAT*ATTTG region. This phenomenon was further examined by the pulse field strength dependence of the 1H, 13C, and 15N T1rho values. 1H and 13C T1rho values showed a pulse field strength dependence, but 15N T1rho did not. Assuming a two-site exchange process, an exchange time constant of 20-300 micros was estimated for the first adenosine in the CAA sequence. The exact nature of this motion remains unknown.

The formation of the C-U base pair in a duplex was observed in solution by means of the temperature profile of (15)N chemical shifts, and the precise geometry of the C-U base pair was also determined by NOE-based structure calculation. From the solution structure of the RNA oligomer, r[CGACUCAGG].r[CCUGCGUCG], it was found that a single C-U mismatch preferred being stacked in the duplex rather than being flipped-out even in solution. Moreover, it adopts an irregular geometry, where the amino nitrogen (N4) of the cytidine and keto-oxygen (O4) of the uridine are within hydrogen-bonding distance, as seen in crystals. To further prove the presence of a hydrogen bond in the C-U pair, we employed a point-labeled cytidine at the exocyclic amino nitrogen of the cytidine in the C-U pair. The temperature profile of its (15)N chemical shift showed a sigmoidal transition curve, indicating the presence of a hydrogen bond in the C-U pair in the duplex.

The solution structures of two DNA duplexes containing a DNA*RNA hybrid region at different sites, d(GG)r(AGAU)d(GAC) x d(GTCATCTCC) (DHD, where D and H represent the DNA and DNA x RNA hybrid segments, respectively) and d(GGAGA)r(UGAC) x d(GTCATCTCC) (DDH), were determined by nuclear magnetic resonance spectroscopy to clarify the structural features of the D-H and H-D junctions. All proton-proton distances were derived from the NOESY spectra, with mixing times of 45 ms, and the restrained molecular dynamics were carried out starting from the typical A- and B-form conformations. Both duplexes were converged from the respective initial structures into structures with RMSD values of less than 1.0 angstrom. These structures were subjected to full relaxation matrix refinement to produce the final structures. In the case of the D-H junction, where the ribonucleotide was linked to the 3'-end of the DNA, the H2' and H2" signals of the deoxynucleotide overlapped completely, and the ribonucleotide had a H1'-H2' coupling constant larger than that of the normal C3'-endo sugar pucker. The dihedral angles, the pseudorotation phase angles, and the helical parameters changed at the H-D junction, but not at the D-H junction. A detailed comparison of the two duplexes revealed the structural heterogeneity between the DNA segment and the DNA x RNA hybrid region and the transitions at the junctions.

N−N J-coupling across a metal center (2JNN) was clearly detected in a biological macromolecule (DNA duplex) for the first time. By using 2JNN, the base pairing mode of mercury-mediated T−T pairs (T−HgII−T) was definitely determined. This pairing mode was found to be a novel metal ion-binding mode for DNA and RNA molecules, in which imino proton−metal exchange processes are included. Accordingly, 2JNN is highly important for the determination of the chemical structures of metal-mediated base pairs.