Vibrational circular dichroism of A-, B-, and Z-form nucleic acids in the PO2-stretching region.

Vibrational circular dichroism (VCD) spectra were measured for H2O solutions of several natural and model DNAs (single and double strands, oligomers and polymers) in the B-form, poly(dG-dC)-poly(dG-dC) in the Z-form, and various duplex RNAs in an A-form over the PO2-stretching region. Only the symmetric PO2 stretch at approximately 1075 cm-1 yields a significant intensity VCD signal. Differences of the PO2-stretching VCD spectra found for these conformational types are consistent with the spectral changes seen in the base region, but no sequence dependence was seen in contrast to VCD for base modes. The B to Z transition is accompanied by an inversion of the PO2- VCD spectra, which is characteristic of the change in the helical sense of the nucleic acid backbone. A-RNAs give rise to the same sense of couplet VCD as do B-DNAs but have a somewhat different shape because of overlapping ribose modes. These PO2- VCD spectral characteristics have been successfully modeled using simple dipole coupling calculations. The invariability of the symmetric PO2- stretching mode VCD spectra to the base sequence as opposed to that found for the C = O stretching and base deformation modes is evidence that this mode will provide a stable indication of the DNA helical sense.     

Intercalation of daunomycin into d(CG)4 oligomer duplex containing G x T mismatches by vibrational circular dichroism and infrared absorption spectroscopy

The vibrational circular dichroism (VCD) and infrared absorption (IR) spectra of the mismatched octamer oligonucleotides d(CGTGCGCG)(2) (CGT) and d(CGCGTGCG)(2) (CGC) and their complexes with the antitumor drug daunomycin were measured in D(2)O, interpreted, and compared to the octamer d(CGCGCGCG)(2) (CG). The IR spectra of the mismatched octamers in the carbonyl-stretching region are similar to those of the parent CG, whereas the VCD spectra differ in several respects between each other. The main VCD feature due to carbonyl stretching is informative for the mismatches and CG. Vibrational modes in the sugar-phosphate region remain essentially unchanged especially for PO(2) (-) symmetric stretching. Differences between the free and complexed mismatch octamers occurred mainly in the carbonyl-stretching region (1,700-1,600 cm(-1)). The absorption intensity of the C==O peak of G is more prominent for CGC than CGT and resembles CG in this respect. The detailed composition of this doublet is clearly visible, indicating the geometric rearrangement of the base pairs in the presence of the mismatch and upon forming the daunomycin complex.     

Vibrational CD study of the thermal denaturation of poly(rA) · poly(rU)

The vibrational cd (VCD) of a double-stranded RNA, poly(rA) - poly(rU), at pH 7 and moderate added salt concentration (0.1M) has been measured in both the base-stretching and phosphate-stretching regions of the ir as a function of temperature. The data in both cases show two distinct phase transitions. The first is from double- to a triple-stranded form, and the second is from triple- to single-stranded forms, which still retain substantial local order even up to 80°C. The nature of these transitions has been identified by comparison of the VCD and ir absorption spectra of the initially double-stranded samples with those of single-stranded poly(rA) and poly(rU) and with triple-stranded poly-(rA) -poly-(rU) poly (rU). The large differences in the VCD band shapes allows positive identification of the intermediate and final states. Thus under VCD-concentration conditions, a simple helix-to-coil transition can be eliminated for poly (rA ) - poly (rU) while such a two-step transition can be seen at low salt conditions. All of these observations are consistent with previous studies of the phase transitions of poly (rA) - poly (rU) under various salt conditions. Additionally, the VCD is indicative of premelting for all the triple-, double-, and single-strand complexes studied. The triple-strand complex did not show disproportionation to double strand on heating under these added salt conditions. The unusual VCD pattern for low temperature poly (rA) - poly (rU), as compared to high G? C content RNAs and DNAs, is qualitatively, but not quantitatively, explained using exciton coupling of localized dipolar transitions in each type of base within the strand. © 1993 John Wiley & Sons, Inc.     

Testing the vibrational exciton and the local mode models on the instructive cases of dicarvone,dipinocarvone, and dimenthol vibrational circular dichroism spectra

The vibrational circular dichroism (VCD) spectra of dicarvone ( 1 ), dipinocarvone ( 2 ), and dimenthol ( 3 ) have been recorded in the range 900–3200 cm⁻¹, encompassing the mid-infrared (mid-IR), the CO stretching, and the CH-stretching regions. For compound 3 also, the fundamental and the first overtone OH stretching regions have been investigated by IR/NIR absorption and VCD. Density functional theory (DFT) calculations allow one to interpret the IR and VCD spectra and to confirm the configuration/conformational studies previously conducted by X-ray diffraction. The most intense VCD signals are associated with the vibrational normal modes involving symmetry-related groups close to the CC bond connecting covalently the two molecular units. The vibrational exciton (VCDEC) model is fruitfully tested on the VCD data of compounds 1 and 2 for the spectroscopic regions at ~1700 cm⁻¹, and the local mode model is tested on compound 3 at ~3500 and ~6500 cm⁻¹. For compounds 1 and 2 also, ECD spectra are reported, and the exciton mechanism is tested also there, and connections to the VCDEC model are examined.     

Cisplatin adducts of d(CCTCTG*G*TCTCC).d(GGAGACCAGAGG) in aqueous solution by vibrational circular dichroism spectroscopy

The vibrational circular dichroism (VCD) and IR absorption spectra of a dodecamer d(CCTCTGGTCTCC).d(GGAGACCAGAGG) coordinated with cisplatin are distinct compared to those of the dodecamer without cisplatin. Although the intensity of PO(2)/deoxyribose absorptions (1150-850 cm(-1)) increases noticeably relative to those of the carbonyl and ring deformations of the bases (1750-1500 cm(-1)), the VCD spectra differ to a much greater extent. Overlapping positive and negative bands can be assigned relatively easily to individual vibrational modes. The effect of platination on the dodecamer duplex is expressed most prominently in VCD arising solely from the vibrations of the guanines bound to the platinum atom. The effect on the VCD features of other bases leads to minute wavenumber shifts at most. These observations are in agreement with previous NMR and X-ray experiments on the same oligonucleotide. The assignment of the absorption and VCD bands strongly resembles those of the octamer duplex d(CCTGGTCC).d(GGACCAGG) when coordinated with platinum. The spectra of the dodecamer did not indicate any isomerization of the complex with time, as is clearly the case for the octamer.     

Comparison of the conformation of poly(dI-dC) with poly(dI-dbr5C) and the B and Z forms of poly(dG-dC). One- and two-dimensional NMR studies

One- and two-dimensional nuclear Overhauser effects (2D NOE) have been used to compare the conformational properties of 60-80 base pair long duplexes of the synthetic DNA polymer poly(dI-dC) with those of poly(dI-dbr5C) and poly(dG-dC) in the B and Z conformations. Cross peaks in the 2D NOE spectra arising from proton-proton dipolar interactions which are more or less independent of the DNA conformation are used to assign the spectra of these molecules. Other cross peaks are sensitive to the conformational details, and these are used to make deductions about the average conformation in solution. The proton-proton interactions that give rise to the cross peaks in the 2D NOE spectrum of poly(dI-dC) are indicative of a B family conformation and rule out the possibility of some alternative conformations, including A, Z, alternating B, and left-handed B-DNA. The spectra are similar to those obtained from B-form poly(dI-dbr5C) and poly(dG-dC) but different from Z-form poly(dG-dC). Taken together, these results indicate that the solution conformation of poly(dI-dC) is not unusual but more closely resembles that of other B-form DNAs.     

Comparison of alpha-lactalbumin and lysozyme using vibrational circular dichroism. Evidence for a difference in crystal and solution structures

The conformation of the milk protein alpha-lactalbumin has been studied using vibrational circular dichroism (VCD) and compared to parallel studies on lysozyme. These proteins have been shown by Acharya et al. [(1989) J. Mol. Biol. 208, 99-127] to have very similar three-dimensional crystal structures. However, their VCD spectra in D2O solution are quite different. The VCD of lysozyme in D2O more resembles that of alpha-lactalbumin in 33% propanol/D2O, under which conditions alpha-lactalbumin has conformationally transformed to a structure with increased helical fraction. These results can be seen to be consistent with UVCD and resolution-enhanced FTIR spectra of alpha-lactalbumin and lysozyme in both D2O and H2O environments. The solvent sensitivity of the alpha-lactalbumin spectra and hence of its conformation contrasted with the lack of such sensitivity for lysozyme suggest that the alpha-lactalbumin crystal structure represents a conformation different from that which is dominant in aqueous solution.     

Mammalian DNA methyltransferases prefer poly(dI-dC) as substrate

The synthetic duplex DNA, poly(dI-dC).poly(dI-dC), is methylated in vitro by human or murine DNA methyltransferases at 20-100 times the rate of other nonmethylated DNAs. Preparation of the hemimethylated derivative, poly(dI-dMeC).poly(dI-dC), of this polymer increases its effectiveness as a substrate by 2-fold, making it 4-10 times more effective as a substrate for mammalian DNA methyltransferases than any other hemimethylated DNA so far reported. However, the apparent slower rate of de novo methylation of poly(dI-dC).poly(dI-dC) as compared to the hemimethylated derivative is due to substrate inhibition, unique to the unmethylated polymer, as the rates of de novo and maintenance methylation are identical at low substrate concentrations.     

Conformational analysis of melittin in solution phase: vibrational circular dichroism study

The vibrational absorption and vibrational circular dichroism (VCD) spectra of melittin in D(2)O solutions at different pH values, different salt concentrations, or different 2,2,2-trifluoroethanol (TFE) concentrations are recorded in the amide I' (1850-1600 cm(-1)) region. Two models are used to simulate this peptide in different conditions, and a coupled oscillator program is used to obtain the calculated absorption and VCD spectra. This study indicates that melittin adopts a mixed structure in D(2)O solution at low pH, low salt concentration, or low TFE concentration. With an increase in pH, salt concentration, or TFE concentration, the structure changes to alpha-helix and further increases lead to aggregation. These results demonstrate the versatility of VCD in probing the conformations of peptides under different environmental perturbations.     

The hydrogen-bonding structure in parallel-stranded duplex DNA is reverse Watson-Crick

Raman spectra of the parallel-stranded duplex formed from the deoxyoligonucleotides 5'-d-[(A)10TAATTTTAAATATTT]-3' (D1) and 5'-d[(T)10ATTAAAATTTATAAA]-3' (D2) in H2O and D2O have been acquired. The spectra of the parallel-stranded DNA are then compared to the spectra of the antiparallel double helix formed from the deoxyoligonucleotides D1 and 5'-d(AAATATTTAAAATTA-(T)10]-3' (D3). The Raman spectra of the antiparallel-stranded (aps) duplex are reminiscent of the spectra of poly[d(A)].poly[d(T)] and a B-form structure similar to that adopted by the homopolymer duplex is assigned to the antiparallel double helix. The spectra of the parallel-stranded (ps) and antiparallel-stranded duplexes differ significantly due to changes in helical organization, i.e., base pairing, base stacking, and backbone conformation. Large changes observed in the carbonyl stretching region (1600-1700 cm-1) implicate the involvement of the C(2) carbonyl of thymine in base pairing. The interaction of adenine with the C(2) carbonyl of thymine is consistent wtih formation of reverse Watson-Crick base pairing in parallel-stranded DNA. Phosphate-furanose vibrations similar to those observed for B-form DNA of heterogenous sequence and high A,T content are observed at 843 and 1092 cm-1 in the spectra of the parallel-stranded duplex. The 843-cm-1 band is due to the presence of a sizable population of furanose rings in the C2'-endo conformation. Significant changes observed in the regions from 1150 to 1250 cm-1 and from 1340 to 1400 cm-1 in the spectra of the parallel-stranded duplex are attributed to variations in backbone torsional and glycosidic angles and base stacking.     

Vibrational CD studies of the solution conformation of simple alanyl peptides as a function of pH

The CH-stretching vibrational CD (VCD) spectra of glycyl-L-alanine, L-alanylglycine, and L-alanyl-L-alanine have been studied at neutral, high, and low pH in D2O solution. The intense positive VCD band attributed to the C alpha H stretch of the alanyl residue in glycyl-L-alanine at neutral pH is absent in L-alanylglycine. In contrast to the VCD spectra of L-alanine, the positive methine-stretching VCD band in glycyl-L-alanine and L-alanyl-L-alanine is still present at pH 2. Based on the ring current mechanism, the VCD spectra are consistent with the presence of a five-membered CO...HN intramolecular hydrogen-bonded ring between the C-terminal carboxylate and peptide NH groups at neutral and high pH; and a seven-membered COH...O = C hydrogen-bonded ring between the C-terminal carboxyl OH and peptide C = O groups at low pH. In the N-terminal alanyl residue, the peptide C = O group is hydrogen bonded to the NH trans to the methine bond. The CH-stretching VCD spectra of L-alanyl-L-alanyl-L-alanine at neutral pH are consistent with two intramolecularly hydrogen-bonded conformations for the central alanyl residue.     

Conformational study of linear alternating and mixed D- and L-proline oligomers using electronic and vibrational CD and fourier transform IR

Vibrational CD (VCD) spectra of a series of blocked linear, alternating D - and L -proline containing oligopeptides, dissolved in D₂O and in CDCl₃. are reported. For the Boc-LDL -Pro₃ to Boc-DLDLDLDL-Pro₈ oligomers. The VCD spectra in the amide I band is a positive couplet, opposite in sense to that obtained for (L -Pro)_n oligomers. While this admits the possibility of their favoring a right-handed helical chain conformation, the amide I ir spectra for these dl oligomers in D₂O indicate a mixed, apparently alternate, cis-trans conformation that prevents a simple conclusion. Their VCD in D₂O evidence no narrowing and has a progressive loss in intensity (measured as Δ /A,) with an increase in chain length. In CDCl₃a similar pattern of positive VCD couplets decreasing in intensity with length was seen, but their spectra are narrower. Their electronic CD (ECD) in the uv, also indicates a loss in intensity with increasing length. Oligomers with odd or even numbers of Pro residues have different ECD patterns, indicating that those spectra are strongly influenced by local contributions arising in the N-terminal groups. The VCD arises from dipolar and vibrational coupling of the amides in the helical structure. All the spectra are consistent with the chiral end groups leading to formation of an excess of one helical handedness. With an increase in length, the influence of this selectiveness is less and the overall CD measured decreases. © 1995 John Wiley & Sons, Inc.     

Density functional and Møller–Plesset studies of cyclobutanone⋯HF and ⋯HCl complexes

The molecular structure (hydrogen bonding, bond distances and angles), dipole moment and vibrational spectroscopic data [vibrational frequencies, IR and vibrational circular dichroism (VCD)] of cyclobutanone?HX (X?=?F, Cl) complexes were calculated using density functional theory (DFT) and second order Møller–Plesset perturbation theory (MP2) with basis sets ranging from 6–311G, 6–311G^**, 6–311 + + G^**. The theoretical results are discussed mainly in terms of comparisons with available experimental data. For geometric data, good agreement between theory and experiment is obtained for the MP2 and B3LYP levels with basis sets including diffuse functions. Surface potential energy calculations were carried out with scanning HCl and HF near the oxygen atom. The nonlinear hydrogen bonds of 1.81 Å and 175° for HCl and 1.71 Å and 161° for HF were calculated. In these complexes the C=O and H–X bonds participating in the hydrogen bond are elongated, while others bonds are compressed. The calculated vibrational spectra were interpreted and the band assignments reported are in excellent agreement with experimental IR spectra. The C=O stretching vibrational frequencies of the complexes show red shifts with respect to cyclobutanone.     

Infrared and Raman studies show that poly(dA).poly(dT) and d(AAAAATTTTT)2 exhibit a heteronomous conformation in films at 75% relative humidity and a B-type conformation at high humidities and in solution

The decadeoxynucleotide d(AAAAATTTTT)2 in duplex form and the double-helical polynucleotide poly(dA).poly(dT) have been studied by Raman and infrared (IR) spectroscopy under a variety of environmental conditions. The IR spectra have been taken of cast films and compared to the IR spectra of the alternating poly(dA-dT), which shows clear B-genus and A-genus vibrational spectra under conditions of high (greater than 92%) and low (75%) relative humidity (RH). From the IR data, it is shown that d-(AAAAATTTTT)2 and poly(dA).poly(dT) adopt a B-genus conformation in films with high water content. When the relative humidity of the film is decreased, the IR spectra reflect a gradual evolution of the geometry of both d(AAAAATTTTT)2 and poly(dA).poly(dT) into a form intermediate between the B genus and A genus, but the IR spectrum of a pure A genus has not been obtained. In these DNAs at 75% RH, the IR bands of adenosine have the same frequencies as those found in poly(dA-dT) at 75% RH where the local furanose conformation is C3' endo/anti, but the thymidine frequencies do not resemble those of poly(dA-dT) at 75% RH but rather those of poly(dA-dT) at high humidities. It is concluded that both poly(dA).poly(dT) and d(AAAAATTTTT)2 adopt a fully heteronomous duplex geometry in cast films at low humidity. For studies in aqueous solution the Raman effect was employed. As a model for the heteronomous conformation in solution, the duplex poly(rA).poly(dT) was used.(ABSTRACT TRUNCATED AT 250 WORDS)     

Poly(rA).poly(rU) with Ni(2+) ions at different temperatures: infrared absorption and vibrational circular dichroism spectroscopy

Phase transitions were studied of the sodium salt of poly(rA).poly(rU) induced by elevated temperature without Ni(2+) and with Ni(2+) in 0.07 M concentration in D(2)O (approximately 0.4 [Ni]/[P]). The temperature was varied from 20 degrees C to 90 degrees C. The double-stranded conformation of poly(rA).poly(rU) was observed at room temperature (20 degrees C-23 degrees C) with and without Ni(2+) ions. In the absence of Ni(2+) ions, partial double- to triple-strand transition of poly(rA).poly(rU) occurred at 58 degrees C, whereas only single- stranded molecules existed at 70 degrees C. While poly(rU) did not display significant helical structure, poly(rA) still maintained some helicity at this temperature. Ni(2+) ions significantly stabilized the triple-helical structure. The temperature range of the stable triple-helix was between 45 degrees C and 70 degrees C with maximum stability around 53 degrees C. Triple- to single-stranded transition of poly(rA).poly(rU) occurred around 72 degrees C with loss of base stacking in single-stranded molecules. Stacked or aggregated structures of poly(rA) formed around 86 degrees C. Hysteresis took place in the presence of Ni(2+) during the reverse transition from the triple-stranded to the double-stranded form upon cooling. Reverse Hoogsteen type of hydrogen-bonding of the third strand in the triplex was suggested to be the most probable model for the triple-helical structure. VCD spectroscopy demonstrated significant advantages over infrared absorption or the related electronic CD spectroscopy.     

Nucleic acid vibrational circular dichroism, absorption, and linear dichroism spectra. II. A DeVoe theory approach.

The DeVoe polarizability theory is used to calculate vibrational circular dichroism (VCD) and infrared (IR) absorption spectra of four polyribonucleotides: poly(rA) x poly(rU), poly(rU) x poly(rA) x poly(rU), poly(rG) x poly(rC), and poly(rC+) x poly(rI) x poly(rC). This is the first report on the use of the DeVoe theory to calculate VCD, oriented VCD, IR absorption, and IR linear dichroism (LD) spectra of double- and triple-stranded polyribonucleotides. Results are reported for DeVoe theory calculations--within the base-stretching 1750-1550 cm(-1) spectral region--on several proposed multistranded polyribonucleotide geometries. The calculated spectra obtained from these proposed geometries are compared with previously reported measured and calculated VCD and IR spectral results. Base-base hydrogen-bonding effects on the frequencies and magnitudes of the base carbonyl stretching modes are explicitly considered. The good agreements found between calculated and measured spectra are proposed to be further evidence of the usefulness of the DeVoe theory in drawing three-dimensional structural conclusions from measured polyribonucleotide VCD and IR spectra.     

Frequency analysis of infrared absorption and vibrational circular dichroism of proteins in D2O solution.

The IR absorption frequencies as derived from second derivatives of the Fourier transform IR spectra of the amide I' bands of globular proteins in D2O are compared to those obtained from band fitting of the vibrational circular dichroism (VCD) spectra. The two sets of frequencies are in very good agreement, yielding consistent ranges where amide I' VCD and IR features occur. Use of VCD to complement the IR allows one to add sign information to the frequency information so that features occurring in the overlapping frequency ranges that might arise from different secondary structures can be better discriminated. From this comparison, it is clear that correlation just of the frequency of a given IR transition to secondary structure can lead to a nonunique solution. Different sign patterns were identified for correlated groups of globular proteins in restricted frequency ranges that have been previously assigned to defined secondary structural elements. Hence, different secondary structural elements must contribute band components to a given frequency range.     

The structure of triple helical poly(U).poly(A).poly(U) studied by Raman spectroscopy

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U).poly(A).poly(U) triple helix. We compared the Raman spectra of poly(U).poly(A).poly(U) in H2O and D2O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A).poly(U). The presence of a Raman band at 863 cm-1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3' endo; that of the second poly(U) chain may be C2' endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A).poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.     

Reassessment of the random coil conformation: vibrational CD study of proline oligopeptides and related polypeptides.

The "random coil" conformational problem is examined by comparison of vibrational CD (VCD) spectra of various polypeptide model systems with that of proline oligomers [(Pro)n] and poly(L-proline). VCD, ir and uv CD spectra of blocked L-proline oligopeptides [(Pro)n, n = 2-12] in different solvents are reported and compared to the spectra of poly(L-proline) II, poly(L-glutamic acid), and unblocked proline oligomers. Based on the chain-length dependence of the VCD and electronic CD (ECD) spectra of proline oligomers, it is established that VCD spectra are dominated by short-range interactions. The VCD of random coil model polypeptides is shown to be identical in shape but smaller in magnitude than poly(L-proline) II and of similar magnitude to that of (Pro)n (n = 3, 4). Based on the spectral evidence, it is concluded that the "random coil" conformation has a large fraction of helical regions, conformationally similar to the left-handed, 3(1) polyproline II helix, as was previously suggested by Krimm and co-workers. This conclusion is further supported by studies of effects of salt (CaCl2, LiBr, LiClO4), temperature (5-75 degrees C), and pH on the VCD spectra of L-proline oligomers, poly(L-proline) II, and poly(L-glutamic acid). These show that, after each of these perturbations, a significant local ordering remains in the oligomers and polymers studied, and that charged polypeptides such as poly(L-glutamic acid) are more flexible than are polyproline or even L-proline oligomers.     

Vibrational circular dichroism signature of hemiprotonated intercalated four-stranded i-DNA

The four-stranded intercalated DNA structure exemplified by the oligonucleotide 5'-d(CCCCCCCCCCCC) (d(C)12) was studied at acidic pH by infrared absorption (IR) and vibrational circular dichroism (VCD) spectroscopy and compared with spectra of the same oligonucleotide at neutral pH to establish distinct VCD markers for the intercalation motif. The most striking feature is a new absorption at 1694 cm(-1) and its corresponding VCD couplet with reversed sign. These are unique for the intercalated structure and have not been observed for other parallel stranded duplexes. Significant characteristic features resulting from the spatial arrangement of the sugar-phosphate backbone are also clearly present for d(C)12 at acidic pH. An extensive network of CH...O bonds twists the backbone such that multiple through-space vibrational coupling occurs among neighbouring sugar-phosphate residues resulting in unusual VCD signals.