An FT-IR study of DNA and RNA conformational transitions at low temperatures

Fourier Transform Infrared (FT-IR) spectra of solid samples of DNA and RNA obtained from freeze-drying at solid CO2 and liquid nitrogen temperatures, have been recorded and correlation between the conformational transitions and spectral changes is proposed. It is concluded that an equilibrium exists between A, B and Z conformations at low temperatures for the DNA molecule, which is temperature dependent, whereas the RNA molecule exhibits only the A conformation. The results have been compared with the metal-adducts of DNA and RNA, where one of the conformations is predominant. Marker infrared bands for the B conformer have been found to be the strong band at 825 cm-1 (sugar conformer mode) and a band with medium intensity at 690 cm-1 (guanine breathing mode). The A conformation showed characteristic bands at 810 and 675 cm-1. The B to Z conformational transition was characterized by the strong absorption bands near 820-810 cm-1 and at 665-600 cm-1.     

Flexibility of DNA and RNA upon Binding to Different Metal Cations. An Investigation of the B to A to Z Conformational Transition by Fourier Transform Infrared Spectroscopy

Abstract

The interaction of DNA and RNA with Cu(II), Mg(II), [Co(NH₃)₆]³⁺ [Co(NH₃)₅Cl]²⁺ chlorides and, cis- and trans-Pt(NH₃)₂Cl₂ (CIS-DDP, trans-DDP) has been studied by Fourier Transform Infrared (FT-IR) spectroscopy and a correlation between metal-base binding and conformational transitions in the sugar pucker has been established. It has been found that RNA did not change from A-form on complexation with metals, whereas DNA exhibited a B to Z transition. The marker bands for the A-form (C′₃-endo-anti conformation) were found to be near 810–816 cm^?1, while the bands at 825 and 690 cm^?1 are marker bands for the B- conformation (C′₂-endo, anti), The B to Z (C₃′-endo, syn conformation) transition is characterized by the shift of the band at 825 cm^?1 to 810–816 cm^?1 and the shift of the guanine band at 690 cm^?1 to about 600–624 cm^?1.     

A new approach to the characterization of the B and A forms of DNA by I.R. spectroscopy

The RNA conformational changes of B, A and C forms are reflected in the infrared absorption spectra in the region of 800 cm^?1 to 900 cm^?1 and allow one to investigate unoriented samples. The transition to the A form is characterized by the appearence of bands at about 870 cm^?1 and at 813 cm^?1 whereas the B and the C forms exhibit a band at 837 cm^?1, these bands undoubtedly arise from phosphate diester stretching vibrations and yield information about backbone conformation. The presence of these infrared bands provides a criterion for testing the simultaneous presence of two coexisting forms of DNA. It represents a useful method for structural studies of nucleic acid complexes such as protein-DNA for which it is difficult to obtain orientation.     

Laser Raman spectroscopic analysis of angiotensin peptides' conformation

In this study we examined the conformation and side chain environments of angiotensins I, II, III, and [Sar¹-Ile⁵-Ala⁸]angiotensin II using laser Raman spectroscopy. The positions of the amide I bands for all four peptides were found between 1664 and 1673 cm^?1. D₂O exchange studies confirmed the positions of the amide I and amide III bands. The positions of the amide I bands for all the angiotensins were found at approximately 1665 cm^?1 and the amide III bands were all located between 1265 and 1278 cm^?1. From the positions and intensities of the amide I and III bands we concluded that all peptides share the same overall conformation consisting of β-turn structure. Spectral analysis indicated that although the spectra for all the peptides were qualitatively identical there was evidence that the angiotensin conformations were more flexible in the aqueous phase than the solid phase. Examination of the $\text{850}\text{830}$ cm^?1 tyrosine doublet suggested that the tyrosine residue in the peptides is exposed to the solvent environment and becomes more exposed as the peptide length is decreased. Therefore, there are some localized conformational differences among the angiotensins. The conformational data yielded by this study leads us to conclude that the various biological properties ascribed to the angiotensins are not due to different conformations of the peptides. The biological differences could perhaps be attributed to localized interactions of the individual amino acid residues with themselves and with the hormone receptors.     

Conformational dependence of the Raman scattering intensities from polynucleotides. 3. Order-disorder changes in helical structures

Raman spectra are presented on ordered and presumably helical structures of DNA and RNA as well as the poly A·poly U helical complex, polydAT, and the helical aggregates of 5′-GMP and 3′-GMP. The changes in the frequency and the intensity of the Raman bands as these structures undergo order-disorder transitions have been measured. In general the changes we have found can be placed into three categories: (1) A reduction in the intensities of certain ring vibrations of the polynucleotide bases is observed when stacking or ordering occurs (Raman hypochromism). Since the ring vibrational frequencies are different for each type of base, we have been able to obtain some estimate of average amount of order of each type of base in partially ordered helical systems. (2) A very large increase in the intensity of a sharp, strongly polarized band at about 815 cm^?1 is observed when polyriboA and polyriboU are formed into a helical complex. Although this band is not present in the separated chains at high temperature, a broad diffuse band at about 800 cm^?1 is present. The 815 cm^?1 band undoubtedly arises from the vibrations of the phosphate-sugar portions of the molecule and provides a sensitive handle to the back-bone conformation of the polymer. This band also appears upon ordering of RNA, formation of the helical aggregate of 5′-riboGMP, and to some extent in the selfstacking of the polyribonucleotides polyA, polyU in the presence of Mg⁺⁺, PolyC, and polyG. No such intense, polarized band is found, however, in ordered DNA, polydAT, or the 3′-riboGMP aggregate, although there is a conformationally independent band at about 795 cm^?1 in DNA and polydAT. (3) Numerous frequency changes occur during Conformational changes. In particular the 1600–1700 cm^?1 region in D₂O shows significant conformationally dependent changes in the C?O stretching region analogous to the changes in this region which have been observed in these substances in the infrared. Thus, Raman scattering appears to provide a technique for simultaneously observing the effects of base stacking, backbone conformation and carbonyl hydrogen bonding in nucleic acids in moderately dilute (10–25 mg/ml) aqueous solutions.     

The conformation of polycytidylic acid, polyguanylic acid, polyinosinic acid, and their helical complexes in aqueous solution from laser Raman scattering

The Raman spectra of the double helical complexes of poly C–poly G and poly I–poly C at neutral p^H are presented and compared with the spectra of the constituent homopolymers. When a completely double-helical structure is formed in solution a strong sharp band at 810–814 cm^?1 appears which has previously been shown to be due to the A-type conformation of the sugar–phosphate backbone chain. By taking the ratio of the intensity of the 810–814 cm^?1 band to the intensity of the 1090–1100 cm^?1 phosphate vibration, one can obtain an estimate of the fraction of the backbone chain in the A-type conformation for both double-stranded helices and self-stacked single chains. This type of information can apparently only be obtained by Raman spectroscopy. In addition, other significant changes in Raman intensities and frequencies have been observed and tabulated: (1) the Raman intensity of certain of the ring vibrations of guanine and hypoxanthine bases decrease as these bases become increasingly stacked (Raman hypochromism), (2) the Raman band at 1464 cm^?1 in poly I is asigned to the amide II band of the cis-amide group of the hypoxanthine base. It shifts in frequency upon base pairing to 1484 cm^?1, thus permitting the determination of the fraction of I–C pairs formed.     

Interpretation of DNA Vibration Modes: III - The Behaviour of the Sugar Pucker Vibration Modes as a Function of its Pseudorotation Parameters

Abstract

A systematic study of the sugar pucker characteristic vibration modes as a function of its geometrical conformations, has been performed. The present investigation is based on the Wilson GF method and a non-redundant valence force field. The calculated results allow to assign the modes arising mainly from the sugar motions and present in quasi whole vibrational spectra related to the right or left-handed double-helices (i.e., 1050 cm^?1,960 cm^?1 and 890 cm^?1). Moreover, the conformation dependent modes as those at 860 cm^?1 and around 810 cm^?1 (A form) as well as the one located around 830 cm^?1 (B form) are interpreted by the present investigation. The possibility of the interaction of the latter modes with the phosphate group motions along the DNA double-helical chains are also discussed.     

Far-infrared spectra of polyalanines with alpha-helical and beta-form structures

Far-infrared spectra of poly-L -alanines having the α-helical conformation and the β-form structure were measured. The spectra of glycine–L -alanine copolymer, silk fibroin, and copoly-D ,L -alanines with different D :L compositions were also measured. In addition to the bands so far reported, four bands at 190, 107, 120, and 90 cm^?1were found for the α-helix conformation and the two bands at 442 and 247 cm^?1 were found for the β form. The 442 cm^?1 band consists of the parallel 432 cm^?1 and perpendicular 445 cm^?1 bands. The 247 cm^?1 band is well defined and has strong dichroism parallel to the direction of stretching. These two bands appear also for silk fibroin and glycine–L -alanine copolymer. All the far-infrared bands of copoly-D ,L -alanines can be interpreted as α-helix bands, the three peaks at 580, 478, and 420 cm^?1 being ascribed to the D -residue incorporated into the right-handed α-helix or to the L -residue in the left-handed α-helix.     

A vitrational study of poly (L-proline) I and II in the far infrared.

The far infrared spectra of poly(L -proline) I (190–35 cm^?1) and II (400–35 cm^?1) were obtained in the solid state at both 300° and 110°K. A significant difference in the region below 100 cm^?1 was observed. A very intense band located at 60 cm^?1 in the infrared spectrum of form II has no counterpart in form I. This indicates the sensitivity of low-frequency vibrations to the difference in conformation assumed by both forms in the solid state. Additional bands observed in this study are correlated with ir and Raman data previously reported and tentative assignments are made using the results of normal mode calculations (in the single-chain approximation) which have been reported.     

Raman Spectroscopy Study of the B-Z Transition in (dG-dC)n · (dG-dC)n and a DNA Restriction Fragment

Abstract

The B to Z conformational transition of (dG-dC)_n·(dG-dC)_n and a 157 bp DNA restriction fragment were followed using Raman spectroscopy. The 157 bp DNA has a 95 bp segment from the E. coli lactose operon sandwiched between 26 and 32 bp of (dC-dG) sequences. Raman spectra of the DNAs were obtained at varying sodium chloride concentrations through the region of the transition. A data analysis procedure was developed to subtract the background curves and quantify Raman vibrational bands. Profiles of relative intensity vs. sodium chloride concentration are shown for bands at 626, 682, 831–833 and 1093 cm^?1. Both (dG-dC)_n·(dG-dC)_n and the 157 bp DNA show changes in the guanine vibration at 682 cm^?1 and backbone band at 831–3 cm^?1 preceeding a highly cooperative change in the 1093 cm^?1 PO 7 vibration. This result indicates that there are at least two conformational steps in the B to Z conformational pathway.

We review the effect of the (dC-dG) portion of the 157 bp DNA on the 95 bp segment. Comparison of Raman spectra of the 157 bp DNA, the 95 bp fragment and (dG-dC)_n·(dG- dC)_n indicate that in 4.5 M NaC/the (dC-dG) segments are in a Z-conformation. Base stacking in the 95 bp portion of the 157 bp DNA appears to maintain a B-type conformation. However, a substantial portion of this region no longer has a B-type backbone vibration.     

FT-IR spectroscopic evidence of sugar ring conformational changes in GpC and CpG on platination and intercalation

An FT-IR spectroscopic study concerning changes in the conformation of sugar in the dinucleotides; GpC and CpG, on platination and intercalation is presented. The results are compared with the FT-IR spectral data of 5′-CMP, 5′-GMP, 3′-GMP and their metal adducts. The spectra of free GpC, free CpG, proflavine-GpC, proflavine-CpG, and cis-[Pt(NH₃)₂(GpC)₂]²⁺ exhibit the diagnostic band at 800 cm⁻¹ which was assigned to a sugar phosphate vibrational mode and diagnostic of C3′-endo sugar pucker. In the case of 9-aminoacridine-GpC and cis-[Pt(NH₃)₂(CpG]⁺ the diagnostic bands of the C2′-endo and C3′-endo conformations are observed at 810–820 cm⁻¹ and near 800 cm⁻¹ respectively. The results are in good agreement with X-ray data. The infrared diagnostic bands are important for distinguishing the sugar pucker conformational changes.     

Changes in Raman vibrational bands of calf thymus DNA during the B-to-A transition

The B -to-A conformational transition of calf thymus DNA fibers was followed employing Raman spectroscopy. The transition was induced by soaking DNA fibers in water/ethanol mixtures increasing from 60 to 85% ethanol (v/v). Intensity changes of 17 Raman vibrational bands were quantified in the region from 400 to 860 cm^?1. Two bands at 500 and 784 cm^?1 were employed as internal standards. These bands do not appear to change in intensity with ethanol concentration. Large intensity changes relative to these two bands are observed between 70 and 74% ethanol for backbone vibrations at 708, 808, and 835 cm^?1, and base vibrations at 682, 730, and 750 cm^?1. These results indicate that a highly cooperative conformational change takes place between different portions of DNA in the B -to-A transition. Relative intensity changes preceding the onset of the major transition are observed in only two bands; at 835 cm^?1, assigned to a ribose–phosphate vibration, and at 750 cm^?1, assigned to thymine. The implications of these pretransition changes are discussed.     

Conformation of poly-L-tyrosine in aqueous solution

The conformational transition of poly-L -tyrosine in 0.1M KCl was investigated by ORD and infrared spectroscopy, potentiometric titration, and sedimentation velocity experiments. It is shown that the fully ordered conformer is obtained by slow titration of the random coil with 0.1N HCl at 25°C. The charge-induced transition, at variance with other poly-α-amino acids, is completed in a narrow range of α. An aggregation process was detected both by potentiometric titration and sedimentation velocity. The polyamino acid aggregates around α = 0.7 at 25°C when the conformational transition is almost complete. Infrared spectra, in the region of the amide I band (1650 cm^?1) showed that the transition is a random coil → antiparallel β one. Evidence exists that the form is of the intramolecular type. The foregoing interpretations of ORD and CD spectra in terms of the α-helix conformation are discussed.     

Observation of small conformational changes in the sperm-whale myoglobin by the far-infrared spectra

Small conformational changes in a molecule of sperm-whale myoglobin in its native solid state for different pH values at room temperature as well as during heat denaturation in alkali medium at different stages of unfolding of the globule were observed by using far-infrared spectroscopy in the region from 30 to 600 cm^?1. The changes appeared in the absorption bands near 420 and 470 cm^?1 ascribed to the side-chain vibrations of helical segments of the myoglobin molecule. For the first time the high structural sensitivity of the far-infrared region of the skeletal vibrations has been confirmed experimentally and the applicability of this technique to globular proteins demonstrated.     

Absolute configuration determination and conformational analysis of (−)‐(3S,6S)‐3α,6β‐diacetoxytropane using vibrational circular dichroism and DFT techniques

The absolute configuration of semisynthetic (?)‐3α,6β‐acetoxytropane 1 , prepared from (?)‐6β‐hydroxyhyoscyamine 2 , has been determined using vibrational circular dichroism (VCD) spectroscopy. The vibrational spectra (IR and VCD) were calculated using DFT at the B3LYP/DGDZVP level of theory for the eight more stable conformers which account for 99.97% of the total relative abundance in the first 10 kcal/mol range. The calculated VCD spectra of all considered conformations showed two distinctive spectral ranges, one between 1300 and 1200 cm^?1, and the other one in the 1150–950 cm^?1 region. When compared with the experimental VCD spectrum, the first spectral region confirmed the calculated conformational preferences, whereas the second region showed little change with conformation, thus allowing the determination of the absolute configuration of 1 as (3S,6S)‐3α,6β‐diacetoxytropane. Also, the bands in the second region showed similarities between 1 and 2 in both the experimental and calculated VCD spectra, suggesting that these bands are mainly related to the absolute configuration of the rigid tropane ring system, since they show conformational independency, no variations with the nature of the substituent, and are composed by closely related vibrational modes. Chirality, 2010. © 2009 Wiley‐Liss, Inc.     

Structural investigation of poly d(BrU-A) by ultraviolet resonance raman spectroscopy

The resonance Raman spectra of a DNA containing bromodeoxy-uridine (BrdUrd), the poly d(BrU-A), are reported, using U.V. laser as a source of excitation. The conformational change from the ordered, base paired form of poly d(BrU-A) (at 25°C) to the melted form at high temperature (63°C) is reflected in a pronounced hyperchromism of Raman bands at 1627 cm^?1, 1352 cm^?1 and 1230 cm^?1. Particularly the band at 1627 cm^?1 assigned to the vibrations of C4 carbonyl which is hydrogen bonded to adenine increases strongly its intensity upon melting. This represents a new approach for a detection of base unpairing and of modifications in geometry of selective molecules (BrdUrd) in a DNA chain in dilute solutions (10^?4 M).     

Polarized Raman scattering from oriented single microcrystals of d(A5T5)2 and d(pTpT)

Polarized Raman spectra have been obtained from single microcrystals of the duplex of the decamer d(A₅T₅)₂ using a Raman microscope. This is the first report of Raman spectra from a crystal of a deoxyoligomer that contains only long, nonalternating sequences of adenine and thymine. Sequences containing d(A)_n and d(T)_n are of interest in view of recent suggestions that they induce bends in DNA and that they might exist in a nonstandard B-conformation. Polarized Raman spectra of a crystal of d(pTpT) have also been obtained. Both crystals display Raman bands whose intensities are very sensitive to the orientation of the crystal with respect to the direction of polarization of the incident laser beam. These spectra indicate that the helical axes of the oligonucleotides are parallel to the long axes of the crystals and that the d(A₅T₅)₂ is not appreciably bent in the crystal. The Raman spectrum from the d(pTpT) crystal indicates that all of the furanose ring puckers are in a C2′-endo configuration since only the C2′-endo marker band at 835 ± 5 cm^?1 is present. Crystals of d(A₅T₅)₂ show measurable Raman intensities in both the 838- and 816-cm^?1 bands. This indicates the presence of both the C2′-endo and C3′-endo, or possibly other non-C2′-endo, furanose conformations. The 816-cm^?1 band is weak so that only a small fraction of the residues are estimated to be in the non-C2′-endo conformation. In both the d(pTpT) and d(A₅T₅)₂ crystals the intensity of the bands due to vibrations of the backbone show only a small dependence on orientation of the crystals. This result is explained by the low symmetry of the puckered sugar rings. It is concluded that Raman spectra obtained from oligonucleotide crystals in which the orientation of the crystal axes to the laser polarization is not carefully controlled may contain intensity artifacts that are due to polarization effects.     

Intensity Changes of Base and Backbone Raman Modes in the B to Z Transition of poly(dG-dm5C)

Abstract

Raman spectroscopy was employed to investigate the temperature-induced B to Z transition of poly(dG-dm-⁵C). The transition midpoint was about 37°C for a solvent containing 20 mM Mg²⁺. A 10-fold change in Mg²⁺ concentration altered the transition midpoint by at least 60°C. Raman spectra of the B and Z forms of poly(dG-dm⁵C) exhibited characteristics similar to those observed with poly(dG-dC). The 682 cm^?1 guanine mode and 835 cm^?1 backbone mode were present in the B conformation. In the Z form the intensities of these two bands decrease substantially and new peaks were observed at 621 cm^?1, 805 and 819 cm¹. Several bands unique to poly(dG-dm⁵C) were also observed. Transition profiles of band intensity vs. temperature were determined for fourteen Raman bands. The curves of all of the base vibrations and one backbone mode had the same slope and midpoint. This indicates that conformational changes in the guanine and methycytosine bases occur concurrently.     

Folding of aminosuccinyl peptides: Thermodynamic data from temperature dependent circular dichroism measurements

The conformational equilibrium of aminosuccinyl peptides between extended conformations and an intramolecularly hydrogen bonded type II′ β-turn conformation has been studied on the peptide Boc-L -Asu-Gly-L -Ala-OMe (Asu = aminosuccinyl residue) by means of temperature dependence of circular dichroism spectra. Owing to the peculiar chiroptical and conformational properties of the Asu residue, this technique proved to be very useful for deriving thermodynamic data for the above folding process. The value of ΔH⁰ (?6.6 kJ mol^?1), obtained for the peptide studied in a chloroformacetonitrile mixture, shows that the lower energy of the folded conformer is primarily due to the characteristic intramolecular hydrogen bond of the β turns. © 1995 Wiley-Liss, Inc.     

Conformational flexibility in the molecular structure of rotenone, a naturally occurring insecticide

The crystal and molecular structure of rotenone, a naturally occurring insecticide with mitochondrial and mitotic spindle inhibitory properties, was determined by direct methods. The crystals were orthorhombic, space group, P2_I2_I2_I with two molecules in the asymmetric unit; a = 8.413 (1) Å, b = 19.840(1), c = 23.581(1), V = 3936 ų, Z = 8. The structure was refined by least-squares methods to a final R = 0.067. The two molecules in the asymmetric unit have different conformations about the junction between the nonaromatic rings B and C. Ring B is in a sofa conformation in both molecules, with a slight distortion toward a half-chair in I, but with C8 and C8′ on opposite sides of the planar part of the rings. This difference in conformation results in I having an extended (linear) shape while II is V-shaped. The more elongated conformation of the molecule (I) has not been reported in previous studies. Ring C also has opposite conformations in the two molecules. The angle between the planes formed by rings A and D in molecule I is 64.3°, while in molecule II it is 88.3°. Molecular mechanics techniques were used to determine the energy of the two conformations. These calculations, at room temperature, predict molecule II to be the more stable conformer. The highly flexible site in the B/C ring junction is also chemically very reactive. This flexibility and reactivity are further discussed in terms of rotenone's inhibitory activities.