A two-dimensional NMR study of the solution structure of a DNA dodecamer comprising the concensus sequence for the specific DNA-binding sites of the glucocorticoid receptor protein

NMR analysis of duplex d(CGCGATCGCG)2 modified by Λ- and Δ-[Ru(bpy)2(m-GHK)]Cl2 and DNA photocleavage study

The interaction of the diastereomeric complexes Lambda-[Ru(bpy)2(m-GHK)]Cl2 and Delta-[Ru(bpy)2(m-GHK)]Cl2 (bpy is 2,2'-bipyridine, GHK is glycine-L-histidine-L-lysine) with the deoxynucleotide duplex d(5'-CGCGATCGCG)2 was studied by means of 1H NMR spectroscopy. At a Delta-isomer to DNA ratio of 1:1, significant shifts for the metal complex are observed, whereas there is negligible effect on the oligonucleotide protons and only one intermolecular nuclear Overhauser effect (NOE) is present at the 2D nuclear Overhauser enhancement spectroscopy spectrum. The 1Eta NMR spectrum at ratio 2:1 is characterized by a slight shift for the Delta-isomer's bpy aromatic protons as well as significant shifts for the decanucleotide G4 H1' and Eta2'', A5 H2, G10 H1', T6 NH and G2 NH protons. Furthermore, at ratio 2:1, 11 intermolecular NOEs are observed. The majority of the NOEs involve the sugar Eta2' and Eta2'' protons sited in the major groove of the decanucleotide. Increasing the Delta-isomer to d(CGCGATCGCG)2 ratio to 5:1 results in noteworthy spectral changes. The Delta-isomer's proton shifts are reduced, whereas significant shifts are observed for the decanucleotide protons, especially the sugar protons, as well as for the exchangeable protons. Interaction is characterized by the presence of only one intermolecular NOE. Furthermore, there is significant broadening of the imino proton signals as the ratio of the Delta-isomer to DNuAlpha increases, which is attributed to the opening of the two strands of the duplex. The Lambda-isomer, on the other hand, approaches the minor groove of the oligonucleotide and interacts only weakly, possibly by electrostatic interactions. Photocleavage studies were also conducted with the plasmid pUC19 and a 158-bp restriction fragment, showing that both diastereomers cleave DNA with similar efficiency, attacking mainly the guanines of the sequence probably by generating active oxygen species.

Formation of sheared G:A base pairs in an RNA duplex modelled after ribozymes, as revealed by NMR

The thermal stability and structure of an RNA duplex, r(GGACGAGUCC)2, the base sequence of which was modelled after both a hammerhead ribozyme and a lead ribozyme, were studied by CD and NMR. We previously demonstrated that the corresponding DNA duplex, d(GGACGAGTCC)2, formed unique 'sheared' G:A base pairs, where an amino proton, instead of an imino proton, of G is involved in the hydrogen bonding, and G and A bases are arranged 'side by side' instead of 'head to head' (Nucleic Acids Res. (1993) 21, 5418-5424). CD melting profiles showed that the RNA duplex is thermally more stable than the corresponding DNA duplex. NMR studies revealed that sheared G:A base pairs are formed in the RNA duplex, too, although the overall structure of the RNA is the A form, which differs from the B form taken on by the corresponding DNA. A model building study confirmed that sheared G:A base pairs can be accommodated in the double helical structure of the A form. A difference between the RNA and DNA duplexes in the stacking interaction involving G:A mismatch bases is also suggested. The demonstration that sheared G:A base pairs can be formed not only in DNA but also in RNA suggests that this base pairing plays an important role regarding the RNA structure.

NMR studies of G:A mismatches in oligodeoxyribonucleotide duplexes modelled after ribozymes

The structures of two oligodeoxyribonucleotide duplexes, the base sequences of which were modelled after both a hammerhead ribozyme and a small metalloribozyme, were studied by NMR. Both duplexes contain adjacent G:A mismatches; one has a PyGAPu:PyGAPu sequence and the other a PyGAPy:PuGAPu sequence. It is concluded on the basis of many characteristic NOEs that in both duplexes G:A base pairs are formed in the unique 'sheared' form, where an amino proton instead of an imino proton of G is involved in the hydrogen bonding, and G and A bases are arranged 'side by side' instead of 'head to head'. A photo-CIDNP experiment, which gives unique and independent information on the solvent accessibility of nucleotide bases, also supports G:A base pairing rather than a bulged-out structure of G and A residues. This is the first demonstration that not only the PyGAPu:PyGAPu sequence but also the PyGAPy:PuGAPu sequence can form the unique sheared G:A base pairs. Taking the previous studies on G:A mismatches into account, the idea is suggested that a PyGA:GAPu sequence is a minimum and essential element for the formation of the sheared G:A base pairs. The sheared G:A base pairs in the PyGAPu:PyGAPu sequence are suggested to be more stable than those in the PyGAPy:PuGAPu sequence. This is explained rationally by the idea proposed above.

A new model for the bending of DNAs containing the oligo(dA) tracts based on NMR observations

The conformations of double-stranded d(GGAAATTTCC) x 2, d(GGTTTAAACC) x 2, d(CGCAAAAAAGCG)d(CGCTTTTTTGCG) and d(GCATTTTGAAACG)d(CGTTTCAAAATGC) have been studied by NMR spectroscopy. Analyses of cross peaks in NOESY spectra between the H2 of an adenine and the H1' of a deoxyribose in the 3'-neighbouring residue on the complementary strand revealed that the minor groove of the oligo(dA) tract is compressed gradually from 5' to 3' in each duplex. In view of this gradual compression of the minor groove along the oligo(dA) tract, it can be understood clearly why d(GGAAATTTCC)n x 2 and d(GAAAATTTTC)n x 2 are bent, and d(GGTTTAAACC)n x 2 and d(GTTTTAAAAC)n x 2 are not bent. The relative extents of bending of a series of d(AjN10-j)nd(N10-jTj)n sequences can also be understood systematically. Additionally, it was found that the TA step disturbed the compression of the minor groove of the oligo(dA) tract to some extent.

A Monte Carlo simulation study of the influence of internal motions on the molecular conformation deduced from two-dimensional NMR experiments

Monte Carlo methods have been used to simulate internal motions of aromatic protons of an oligonucleotide at the nanosecond time scale. Each proton is allowed to fluctuate about its equilibrium position. The longitudinal cross-relaxation rates of such a system of spins have been determined by computing the appropriate correlation functions. Then the interproton distances have been deduced according to the procedure generally used in two-dimensional nmr techniques (nuclear Overhauser effect spectroscopy--NOESY) and compared to the true values. The influence of the amplitude A and of the internal rotational diffusion constant Dint characterizing the dynamics of the system has been checked for in-phase and for uncorrelated motions. It is shown that for the investigated models the distances deduced from NOESY experiments may be under- or overestimated, depending strongly on the values of A and Dint. Furthermore, the cross-relaxation rate of a couple of protons is very sensitive to the correlation level of the motions of both protons.

One- and two-dimensional NMR studies on the conformation of DNA containing the oligo(dA)oligo(dT) tract

The resonances of the imino protons and all of the non-exchangeable protons (except for H5'/H5'') of d(CGCAAAAAAGCG)d(CGCTTTTTTGCG) have been assigned by means of one- and two-dimensional NMR spectroscopies. Qualitative analyses showed that the overall structure is of the B-form, but local conformational deviations exist. The NOEs between the imino protons of thymines and H2 of adenines suggest that the A-T base pairs are propeller-twisted to almost the same degree as in crystals. A remarkable chemical shift of H1' was observed for the residue located just before the oligo(dA)oligo(dT) tract, suggesting the presence of conformational discontinuity at the junctions between the oligo(dA)oligo(dT) tract and the other portions. Analyses of cross peaks in NOESY spectra between H2 of adenines and H1' of the 3'-neighbouring residues on the complementary strand revealed that the minor groove of the oligo(dA)oligo(dT) tract is narrow and compressed gradually, from 5' to 3', along the tract.

Resonance assignments of non-exchangeable protons in B type DNA oligomers, an overview

The chemical shifts of 1H resonances of non exchangeable protons (except H5', H5" and adenine H2) of over six hundred nucleotides have been collected. The influence which the base of the nucleotide itself as well as the bases on its 5' and 3' side exert on the chemical shifts of the various resonances has been investigated. Most of the resonances appear to be predominantly influenced by only one base. For H2', H2", H3', H4' and H6/H8 this is the base of the central nucleotide, for H5(C) and CH3(T) it is the one on the 5' side and for H1' it is the one on the 3' side. Chemical shift distribution profiles are presented which allow an estimation of the probability of finding a particular resonance at a particular position in the spectrum.

A two-dimensional 1H-NMR study of the dam methylase site: comparison between the hemimethylated GATC sequence, its unmethylated analogue and a hemimethylated CATG sequence. The sequence dependence of methylation upon base-pair lifetimes

We report two-dimensional NOE (NOESY) spectra on the sequence d(GCGATCATGG).d(CCATGATCGC) which contains the unmethylated dam site. As expected the DNA adopts a B-form conformation but appears to be distorted at the TG step of the second strand. This distorsion, probably bending, is not seen on the opposite strand. When the first strand is methylated on adenine in the GATC or CATG sequence the NOESY spectra indicate little or no change in the conformation. However the single strand-duplex exchange is slowed down to the slow-exchange region on a proton NMR time scale. We have assigned the exchangeable imino and cytidine amino resonances of the three duplexes. From the imino linewidths as a function of temperature, we observe that the unmethylated and the hemimethylated Gm6ATC duplexes melt normally from the ends. However, this is not so for the hemimethylated Cm6ATG duplex which, apart from the terminal base pairs, melts cooperatively and at higher temperature. In spectra recorded in H2O a second duplex is observed, for the Gm6ATC sequence, which we have not been able to identify. It is however unlikely to be a hairpin structure. Ultraviolet-melting curves also indicate the presence of two transitions for this duplex. The effect of methylation upon base-pair lifetimes has been studied by comparing the above three duplexes. Little effect is observed upon methylation in the GATC sequence but a drastic increase in the lifetimes of all base pairs is observed upon methylation in the CATG sequence.

Kinetics of the proton-deuteron exchange at position H8 of adenine and guanine in DNA

Proton-NMR has been used to determine the activation energies and pre-exponential factors for the deuterium exchange of AH8 in poly(dA-dT).poly(dA-dT), and for GH8 in poly(dG-dC).poly(dG-dC). No simple relationship between the kinetic parameters and molecular conformation was found. By addition of 4.5 M NaCl a transition from the B to the Z conformation was induced for poly(dG-dC).poly(dG-dC), and an increased exchange rate was observed. The exchange rate for poly(dA-dT).poly(dA-dT) also increased below 64 degrees C, and a significant decrease in activation energy on addition of 4.5 M NaCl was observed. The exchange rates at T = 55.8 degrees C were also measured for the AH8 and GH8 in random sequence calf thymus DNA. From the difference in exchange rates, a method of preferential labeling of either the AH8 or the GH8 in high molecular weight DNA is evaluated.

Conformational analysis of the octamer d(G-G-C-C-G-G-C-C) in aqueous solution. A one-dimensional and two-dimensional proton NMR study at 300 MHz and 500 MHz

Proton NMR studies in H2O and 2H2O were carried out on the self-complementary DNA octamer d(G-G-C-C-G-G-C-C) and compared with similar studies on the dimethylated analogue d(G-G-m5C-m5C-G-G-C-C) [Sanderson, M. R., Mellema, J.-R., van der Marel, G. A., Wille, G., van Boom, J. H. & Altona, C. (1983) Nucleic Acids Res. 11, 3333-3346]. Base, H1', H2' and H2" resonances were assigned by means of two-dimensional nuclear Overhauser spectroscopy (NOESY) and correlated spectroscopy (COSY) experiments. Chemical shift vs temperature profiles were used to analyze the temperature-dependent conformational behaviour and to extract thermodynamic parameters for the duplex-to-coil transition. Analysis of proton-proton couplings were used to discriminate between J1'2' and J1'2" and between the H2' and H2" resonances as well as to obtain conformational parameters of the sugar rings. From the NOESY and COSY experiments, the temperature profiles and the analysis of the coupling data it is concluded that: (a) the compound adopts a B-DNA-type helix in solution; (b) the sugar rings in the intact duplex display limited conformational freedom; (c) methylation of the cytosine bases at the C5 position has no measurable effect on the conformational behaviour of the octamer, nor on the conformation of the sugar rings; however, methylation does increase the stability of the duplex in aqueous solution under conditions of low salt concentration.

The effect of the trp repressor from Escherichia coli on the structure and dynamics of dA20dT20

We have determined the effect of the tryptophan (trp) repressor from Escherichia coli on the structure and dynamics of dA20dT20. The structure was determined using time-dependent nuclear Overhauser effects and spin-lattice relaxation times. The deoxyribose conformation is near C3' endo for the thymine residues, and a mixture of about 30% C3' endo and 70% C2' endo for the adenine residues. The glycosidic torsion angles are -50 degrees for T and -60 degrees for A. The roll is 20 degrees and the propellor twist is about 29 degrees. The conformation is consistent with recent calculations (Rao, K. and Kollman, P.A. (1985) J. Am. Chem. Soc. 107, 1507-1511). The rate constant for exchange of the imino protons is similar to that usually found for AT base-pairs, with an activation energy of 20 +/- 2 kcal/mol, and an activation entropy of 17 +/- 7 cal/mol per K. The repressor greatly retards the exchange of imino protons, and the activation energy increases to 38 kcal/mol. There are small changes in the structure of the DNA on forming the complex, with the adenine and thymidine residues becoming more similar in conformation.

Two-dimensional nuclear magnetic resonance spectroscopy

Great spectral simplification can be obtained by spreading the conventional one-dimensional nuclear magnetic resonance (NMR) spectrum in two independent frequency dimensions. This so-called two-dimensional NMR spectroscopy removes spectral overlap, facilitates spectral assignment, and provides a wealth of additional information. For example, conformational information related to interproton distances is available from resonance intensities in certain types of two-dimensional experiments. Another method generates 1H NMR spectra of a preselected fragment of the molecule, suppressing resonances from other regions and greatly simplifying spectral appearance. Two-dimensional NMR spectroscopy can also be applied to the study of 13C and 15N, not only providing valuable connectivity information but also improving sensitivity of 13C and 15N detection by up to two orders of magnitude.

The structure of the double-stranded RNA pentamer 5'(CACAG) . 5'(CUGUG) determined by nuclear Overhauser enhancement measurements: interproton distance determination and structure refinement on the basis of X-ray coordinates

The structure in solution of the duplex RNA pentamer 5'(CACAG) . 5'(CUGUG), comprising the stem of the T psi C loop of yeast tRNAPhe, has been investigated by means of one- and two-dimensional nuclear Overhauser enhancement measurements. All non-exchangeable base and sugar proton resonances with the exception of the H5'/H5" sugar resonances are assigned in a sequential manner. From the relative intensities of the cross-peaks obtained in the pure-phase absorption two-dimensional nuclear Overhauser enhancement spectra at several mixing times, it is deduced that the RNA pentamer adopts an A-type conformation in solution. Cross-relaxation rates and interproton distances are determined from the time dependence of the nuclear Overhauser effects, principally by one-dimensional measurements. The structure of the RNA pentamer is then refined by restrained least-squares minimization on the basis of both distance and planarity restraints using fibre diffraction data as an initial model. The refined structure of the RNA pentamer is of the A type but exhibits local structural variations in glycosidic bond and backbone torsion angles as well as in propeller twist, base roll and base tilt angles.