A note on sequence-dependence of DNA structure

A circular dichroism study was conducted on the solution structure of several different oligonucleotides, whose X-ray structures have been solved. It is suggested that in aqueous solution the oligonucleotides can form structures that maintain geometrical elements which are typical of B-DNA, A-DNA, and their intermediate forms. It is shown that 5'GGATGGGAG:5'CTCCCATCC, which forms an A-DNA helix in the crystal state (McCall et al. 1986), in aqueous solution maintains an A-DNA like structure at temperatures below 10 degrees C. At temperatures between 10 degrees C and 25 degrees C it shows a tendency to form an intermediate structure between A-DNA and B-DNA. Also, it is shown that TFE does not cause a transition from B-DNA to A-DNA helix in short DNA fragments, but instead disrupts the helix.     

Interactions of DNA with divalent metal ions. I. 31P-nmr studies

³¹P-nmr has been used to investigate the specific interaction of three divalent metal ions, Mg²⁺, Mn²⁺, and Co⁺², with the phosphate groups of DNA. Mg²⁺ is found to have no significant effect on any of the ³¹P-nmr parameters (chemical shift, line-width, T₁, T₂, and NOE) over a concentration range extending from 20 to 160 mM. The two paramagnetic ions, Mn²⁺ and Co²⁺, on the other hand, significantly change the ³¹P relaxation rates even at very low levels. From an analysis of the paramagnetic contributions to the spin–lattice and spin–spin relaxation rates, the effective internuclear metal–phosphorus distances are found to be 4.5 ± 0.5 and 4.1 ± 0.5 Å for Mn²⁺ and Co²⁺, respectively, corresponding to only 15 ± 5% of the total bound Mn²⁺ and Co²⁺ being directly coordinated to the phosphate groups (inner-sphere complexes). This result is independent of any assumptions regarding the location of the remaining metal ions which may be bound either as outer-sphere complexes relative to the phosphate groups or elsewhere on the DNA, possibly to the bases. Studies of the temperature effects on the ³¹P relaxation rates of DNA in the absence and presence of Mn²⁺ and Co²⁺ yielded kinetic and thermodynamic parameters which characterize the association and dissociation of the metal ions from the phosphate groups. A two-step model was used in the analysis of the kinetic data. The lifetimes of the inner-sphere complexes are 3 × 10^?7 and 1.4 × 10^?5 s for Mn²⁺ and Co²⁺, respectively. The rates of formation of the inner-sphere complexes with the phosphate are found to be about two orders of magnitude slower than the rate of the exchange of the water of hydration of the metal ions, suggesting that expulsion of water is not the rate-determining step in the formation of the inner-sphere complexes. Competition experiments demonstrate that the binding of Mg²⁺ ions is 3–4 times weaker than the binding of either Mn²⁺ or Co²⁺. Since the contribution from direct phosphate coordination to the total binding strength of these metal ion complexes is small (～15%), the higher binding strength of Mn²⁺ and Co²⁺ may be attributed either to base binding or to formation of stronger outer-sphere metal–phosphate complexes. At high levels of divalent metal ions, and when the metal ion concentration exceeds the DNA–phosphate concentration, the fraction of inner-sphere phosphate binding increases. In the presence of very high levels of Mg²⁺ (e.g., 3.1M), the inner-sphere ? outer-sphere equilibrium is shifted toward ～100% inner-sphere binding. A comparison of our DNA results and previous results obtained with tRNA indicates that tRNA and DNA have very similar divalent metal ion binding properties. A comparison of the present results with the predictions of polyelectrolyte theories is presented.     

Solution secondary structure of calcium-saturated troponin C monomer determined by multidimensional heteronuclear NMR spectroscopy.

The solution secondary structure of calcium-saturated skeletal troponin C (TnC) in the presence of 15% (v/v) trifluoroethanol (TFE), which has been shown to exist predominantly as a monomer (Slupsky CM, Kay CM, Reinach FC, Smillie LB, Sykes BD, 1995, Biochemistry 34, forthcoming), has been investigated using multidimensional heteronuclear nuclear magnetic resonance spectroscopy. The 1H, 15N, and 13C NMR chemical shift values for TnC in the presence of TFE are very similar to values obtained for calcium-saturated NTnC (residues 1-90 of skeletal TnC), calmodulin, and synthetic peptide homodimers. Moreover, the secondary structure elements of TnC are virtually identical to those obtained for calcium-saturated NTnC, calmodulin, and the synthetic peptide homodimers, suggesting that 15% (v/v) TFE minimally perturbs the secondary and tertiary structure of this stably folded protein. Comparison of the solution structure of calcium-saturated TnC with the X-ray crystal structure of half-saturated TnC reveals differences in the phi/psi angles of residue Glu 41 and in the linker between the two domains. Glu 41 has irregular phi/psi angles in the crystal structure, producing a kink in the B helix, whereas in calcium-saturated TnC, Glu 41 has helical phi/psi angles, resulting in a straight B helix. The linker between the N and C domains of calcium-saturated TnC is flexible in the solution structure.     

Solution structure of the DNA complex with a quinacrine-netropsin hybrid molecule by NMR spectroscopy.

The solution structures of 1:1 complexes of a quinacrine-netropsin hybrid molecule with the self-complementary DNA duplexes, d(CGCGAATTCGCG)2 and d(CGAATTCG)2, have been studied by one- and two-dimensional 1H NMR spectroscopy. The NOE data indicate that the acridine ring of the hybrid intercalates into the 5'-GpA step and its netropsin moiety spans the minor groove of the central AATT region.     

Understanding the sequence-dependence of DNA groove dimensions: implications for DNA interactions

Background

The B-DNA major and minor groove dimensions are crucial for DNA-protein interactions. It has long been thought that the groove dimensions depend on the DNA sequence, however this relationship has remained elusive. Here, our aim is to elucidate how the DNA sequence intrinsically shapes the grooves.

Methodology/Principal Findings

The present study is based on the analysis of datasets of free and protein-bound DNA crystal structures, and from a compilation of NMR ³¹P chemical shifts measured on free DNA in solution on a broad range of representative sequences. The ³¹P chemical shifts can be interpreted in terms of the BI↔BII backbone conformations and dynamics. The grooves width and depth of free and protein-bound DNA are found to be clearly related to the BI/BII backbone conformational states. The DNA propensity to undergo BI↔BII backbone transitions is highly sequence-dependent and can be quantified at the dinucleotide level. This dual relationship, between DNA sequence and backbone behavior on one hand, and backbone behavior and groove dimensions on the other hand, allows to decipher the link between DNA sequence and groove dimensions. It also firmly establishes that proteins take advantage of the intrinsic DNA groove properties.

Conclusions/Significance

The study provides a general framework explaining how the DNA sequence shapes the groove dimensions in free and protein-bound DNA, with far-reaching implications for DNA-protein indirect readout in both specific and non specific interactions.     

Solution structure of neuronal bungarotoxin determined by two-dimensional NMR spectroscopy: sequence-specific assignments, secondary structure, and dimer formation

The solution structure of neuronal bungarotoxin (nBgt) has been studied by using two-dimensional 1H NMR spectroscopy. Sequence-specific assignments for over 95% of the backbone resonances and 85% of the side-chain resonances have been made by using a series of two-dimensional spectra at four temperatures. From these assignments over 75% of the NOESY spectrum has been assigned, which has in turn provided 582 distance constraints. Twenty-seven coupling constants (NH-alpha CH) were determined from the COSY spectra, which have provided dihedral angle constraints. In addition, hydrogen exchange experiments have suggested the probable position of hydrogen bonds. The NOE constraints, dihedral angle constraints, and the rates of amide proton exchange suggest that a triple-stranded antiparallel beta sheet is the major component of secondary structure, which includes 25% of the amino acid residues. A number of NOE peaks were observed that were inconsistent with the antiparallel beta-sheet structure. Because we have confirmed by sedimentation equilibrium that nBgt exists as a dimer, we have reinterpreted these NOE constraints as intermolecular interactions. These constraints suggest that the dimer consists of a six-stranded antiparallel beta sheet (three from each monomer), with residues 55-59 forming the dimer interface.     

Coexistence of G-quadruplex and duplex domains within the secondary structure of 31-mer DNA thrombin-binding aptamer

A number of thrombin-binding DNA aptamers have been developed during recent years. So far the structure of just a single one, 15-mer thrombin-binding aptamer (15TBA), has been solved as G-quadruplex. Structures of others, showing variable anticoagulation activities, are still not known yet. In this paper, we applied the circular dichroism and UV spectroscopy to characterize the temperature unfolding and conformational features of 31-mer thrombin-binding aptamer (31TBA), whose sequence has a potential to form G-quadruplex and duplex domains. Both structural domains were monitored independently in 31TBA and in several control oligonucleotides unable to form either the duplex region or the G-quadruplex region. The major findings are as follows: (1) both duplex and G-quadruplex domains coexist in intramolecular structure of 31TBA, (2) the formation of duplex domain does not change the fold of G-quadruplex, which is very similar to that of 15TBA, and (3) the whole 31TBA structure disrupts if either of two domains is not formed: the absence of duplex structure in 31TBA abolishes G-quadruplex, and vice versa, the lack of G-quadruplex folding results in disallowing the duplex domain.     

Coexistence of G-quadruplex and duplex domains within the secondary structure of 31-mer DNA thrombin-binding aptamer

A number of thrombin-binding DNA aptamers have been developed during recent years. So far the structure of just a single one, 15-mer thrombin-binding aptamer (15TBA), has been solved as G-quadruplex. Structures of others, showing variable anticoagulation activities, are still not known yet. In this paper, we applied the circular dichroism and UV spectroscopy to characterize the temperature unfolding and conformational features of 31-mer thrombin-binding aptamer (31TBA), whose sequence has a potential to form G-quadruplex and duplex domains. Both structural domains were monitored independently in 31TBA and in several control oligonucleotides unable to form either the duplex region or the G-quadruplex region. The major findings are as follows: (1) both duplex and G-quadruplex domains coexist in intramolecular structure of 31TBA, (2) the formation of duplex domain does not change the fold of G-quadruplex, which is very similar to that of 15TBA, and (3) the whole 31TBA structure disrupts if either of two domains is not formed: the absence of duplex structure in 31TBA abolishes G-quadruplex, and vice versa, the lack of G-quadruplex folding results in disallowing the duplex domain.     

Solvation effects on the 31P-nmr chemical shifts and infrared spectra of phosphate diesters

The effects of organic solvents on the ³¹P-mr chemical shifts of various phosphate diesters have been investigated in water and mixed-organic solvent systems. The addition of organic solvents to cyclic phosphates and to diethyl phosphate causes large upfield shifts of the phosphorus resonance which are attributed to solvent-induced changes in the local hydration of the phosphodiester group. This is consistent with the fact that there is an inverse correlation between the hydrogen-bond-donating ability of the solvents and the magnitude of the shifts they induce. Other possible interpretations, such as solvent-induced ion pairing and solvent-induced conformational changes, appear to be eliminated. Fourier-transform ir study of the cyclic nucletides reveals that there are also large solvent-induced shifts in the frequency of the antisymmetric OPO stretching frequency, and a comparison of the two types of measurements indicates that there is a linear correlation between shifts observed in the ir and in the ³¹P-nmr spectra. With UpU, the solvent-induced ³¹P-nmr shifts are ～3 times smaller than those observed with the cyclic phosphates and the solvent-induced shift of the OPO band is reduced (factor of ～1.7) as compared with the cyclic phosphates. With the single-stranded polynuclotides, poly(C) and poly(U), the solvent-induced shifts in both the nmr and ir are quite small (～0.1 ppm and ～1 cm^?1). The very small solvent effects observed with poly(U) and poly(C) are attributed to a combination of steric effects and a polyelectrolyte effect which maintains a high density of counterions with waters of hydration in the vicinity of the charged backbone and makes the phosphates much less susceptible to solvent-induced changes in hydration.     

Investigation of the cAMP receptor protein secondary structure by Raman spectroscopy

Raman spectroscopy was employed to examine the secondary structure of the cAMP receptor protein (CRP). Spectra were obtained over the range 400-1900 cm-1 from solutions of CRP and from CRP-cAMP cocrystals. The spectra of CRP dissolved in 30 mM sodium phosphate and 0.15 M NaCl buffered at either pH 6 or pH 8 or dissolved in 0.15-0.2 M NaCl at protein concentrations of 5, 15, and 30 mg/mL were examined. Estimates of the secondary structure distribution were made by analyzing the amide I region of the spectra (1630-1700 cm-1). CRP secondary structure distributions were essentially the same in either pH and at all protein concentrations examined. The amide I analyses indicated a structural distribution of 44% alpha-helix, 28% beta-strand, 18% turn, and 10% undefined for CRP in solution. Raman spectra of CRP-cAMP cocrystals differed from the spectra of CRP in solution. Some differences were assigned to interfering background bands, whereas other spectral differences were attributed to changes in CRP structure. Differences in the amide III region and in the intensity at 935 cm-1 were consistent with alterations in secondary structure. Analysis of the amide I region of the CRP-cAMP cocrystal spectrum indicated a secondary structure distribution of 37% alpha-helix, 33% beta-strand, 17% turn, and 12% undefined. This result is in agreement with a published secondary structure distribution derived from X-ray analysis of CRP-cAMP cocrystals (37% alpha-helix and 36% beta-strand).(ABSTRACT TRUNCATED AT 250 WORDS)     

Solution and membrane structure of enkephalins as studied by infrared spectroscopy

The backbone conformation of the two opioid pentapeptides Leu5-enkephalin and Met5-enkephalin was studied by the technique of resolution-enhanced infrared spectroscopy. In aqueous solution, the conformation-sensitive amide I bands of the two peptides are identical. The positions of these bands are consistent with the view that in aqueous solution both enkephalins exist as an ensemble of largely unfolded conformers. Interaction of Leu5- and Met5-enkephalins with bilayer membranes of ditetradecylphosphatidylcholine results in a substantial refolding of the peptide backbones. The conformation stabilized by the membrane environment is a hydrogen-bonded turn structure. Conformational transitions in enkephalins induced by a lipid environment may play a role in the specific interactions between these hormones and their receptor sites.     

Quantitation of secondary structure in ATR infrared spectroscopy

Polarized attenuated total reflection infrared spectroscopy of aligned membranes provides essential information on the secondary structure content and orientation of the associated membrane proteins. Quantitation of the relative content of different secondary structures, however, requires allowance for geometric relations of the electric field components (E(x), E(y), E(z)) of the evanescent wave, and of the components of the infrared transition moments, in combining absorbances (A() and A( perpendicular)) measured with radiation polarized parallel with and perpendicular to, respectively, the plane of incidence. This has hitherto not been done. The appropriate combination for exact evaluation of relative integrated absorbances is A() + (2E(z)(2)/E(y)(2) - E(x)(2)/E(y)(2))A( perpendicular), where z is the axis of ordering that is normal to the membrane plane, and the x-axis lies in the membrane plane within the plane of incidence. This combination can take values in the range approximately from A() - 0.4A( perpendicular) to A() + 2.7A( perpendicular), depending on experimental conditions and the attenuated total reflection crystal used. With unpolarized radiation, this correction is not possible. Similar considerations apply to the dichroic ratios of multicomponent bands, which are also treated.     

The secondary structure of bacteriorhodopsin determined by Raman and circular dichroism spectroscopy

The secondary structure of bacterio-opsin (BO), the retinal free protein-component of bacteriorhodopsin (BR), has been determined by Raman spectroscopy. Additional circular dichroism (CD) measurements have revealed only negligible conformational differences between BO in apomembranes and BR in purple membranes. Therefore, the secondary structure of BR was derived from the Raman data of BO. The protein conformation was determined to consist of 72-82% helices, 2-11% beta-strands, and 11-17% beta-turns. Only about half of the helical structures correspond to alpha 1-helices, the other half possess non-alpha 1-helical structures. According to the analysis of the Raman data, the derived secondary structure of BR was obtained with high reliability for all structure classes which can be distinguished by this method within the given uncertainty range. This is a remarkable difference from recently published secondary structural data derived from CD measurements where the helix content was reported to be between 50 and 80%. The inherent experimental and methodological uncertainties of the CD-technique leading to such a range of variation are critically discussed in comparison to the method of Raman spectroscopy. The combined application of Raman and CD spectroscopy, as performed here, is demonstrated to be a substantial improvement in the secondary structure determination of retinal-containing membrane proteins. On the basis of our results, some of the recently proposed structural models of BR with a beta-strand content of more than 11% can be ruled out.     

Solution structure of duplex DNA containing an extrahelical abasic site analog determined by NMR spectroscopy and molecular dynamics.

Translesional DNA synthesis past abasic sites proceeds with the preferential incorporation of dAMP opposite the lesion and, depending on the sequence context, one or two base deletions. High-resolution NMR spectroscopy and molecular dynamics simulations were used to determine the three-dimensional structure of a DNA heteroduplex containing a synthetic abasic site (tetrahydrofuran) residue positioned in a sequence that promotes one base deletions. Analysis of NMR spectra indicates that the stem region of the duplex adopts a right-handed helical structure and the glycosidic torsion angle is in anti orientation for all residues. NOE interactions establish Watson-Crick alignments for all canonical base pairs of the duplex. Measurement of distance interactions at the lesion site shows the abasic residue excluded from the helix. Restrained molecular dynamics simulations generated three-dimensional models in excellent agreement with the spectroscopic data. These structures show a regular duplex region and a slight bend at the lesion site. The tetrahydrofuran residue extrudes from the helix and is highly flexible. The model reported here, in conjunction with a previous study performed on abasic sites, explains the structural bias of one-base deletion mutations.     

Periodicity in DNA primary structure is defined by secondary structure of the coded protein.

A 10.5-base periodicity found earlier is inherent in both eu- and prokaryotic coding nucleotide sequences. In the case of noncoding eukaryotic sequences no periodicity is found, so the 10.5-base oscillation seemingly does not correlate with the nucleosomal organization of DNA. It is shown that the DNA fragments, coding the alpha-helical protein segments, manifest the pronounced 10.5-base periodicity, while those regions of DNA which code the beta-structure have a 6-base oscillation. The repeating pattern of nucleotide sequences can be used for comparison of the DNA segments with low degree of homology.     

Determination of the secondary structure of interleukin-8 by nuclear magnetic resonance spectroscopy

The solution conformation of interleukin-8 (IL-8), a small protein of 72 residues with a wide range of proinflammatory activities, has been investigated by two-dimensional NMR spectroscopy. The 1H-NMR spectrum of IL-8 is assigned in a sequential manner and regular elements of secondary structure are identified on the basis of a qualitative interpretation of the nuclear Overhauser, coupling constant and amide exchange data. The IL-8 monomer contains a triple stranded anti-parallel beta-sheet arranged in a Greek key and a long C-terminal helix (residues 57-72). It is shown that IL-8 is a dimer in solution in which the interface is principally formed by six backbone hydrogen bonds between residues 25, 27, and 29 of one monomer and residues 29, 27, and 25, respectively, of the other. As a result, the two units of the dimer form a contiguous six-stranded anti-parallel beta-sheet. The secondary structure of IL-8 is similar to that found in the crystal structure of the sequence related protein platelet factor 4.     

Determination of the secondary structure of proteins in different environments by FTIR-ATR spectroscopy and PLS regression

The secondary structures of proteins (alpha-helical, beta-sheet, beta-turn, and random coil) in the solid state and when bound to polymer beads, containing immobilized phenyl and butyl ligands such as those as commonly employed in hydrophobic interaction chromatography, have been investigated using FTIR-ATR spectroscopy and partial least squares (PLS) methods. Proteins with known structural features were used as models, including 12 proteins in the solid state and 7 proteins adsorbed onto the hydrophobic surfaces. A strong PLS correlation was achieved between predictions derived from the experimental data for 4 proteins adsorbed onto the phenyl-modified beads and reference data obtained from the X-ray crystallographic structures with r(2) values of 0.9974, 0.9864, 0.9924, and 0.9743 for alpha-helical, beta-sheet, beta-turn, and random coiled structures, respectively. On the other hand, proteins adsorbed onto the butyl sorbent underwent greater secondary structural changes compared to the phenyl sorbent as evidenced from the poorer PLS r(2) values (r(2) are 0.9658, 0.9106, 0.9571, and 0.9340). The results thus indicate that the secondary structures for these proteins were more affected by the butyl sorbent, whereas the secondary structure remains relatively unchanged for the proteins adsorbed onto the phenyl sorbent. This study has important ramifications for understanding the nature of protein secondary structural changes following adsorption onto hydrophobic sorbent surfaces. This knowledge could also enable the development of useful protocols for enhancing the chromatographic purification of proteins in their native bioactive states. (c) 2008 Wiley Periodicals, Inc. Biopolymers 89: 895-905, 2008.This article was originally published online as an accepted preprint. The "Published Online" date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com.