The Z-Conformation of Poly(dA-dT) · Poly(dA-dT) in Solution as Studied by Ultraviolet Resonance Raman Spectroscopy

Abstract

Poly(dA-dT) poly(dA-dT) structures in aqueous solutions with high NaCl concentrations and in the presence of Ni²⁺ ions have been studied with resonance Raman spectroscopy (RRS). In low water activity the effects of added 95 mM NiCl₂ in solution stabilize the syn geometry of the purines and reorganize the water distribution via local interactions of Ni-water charged complexes with the adenine N7 position. It is shown that RRS provides good marker bands for a left-handed helix: i) a purine ring breathing mode around 630 cm″^?1coupled to the deoxyribose vibration in the syn geometry, ii) a 1300-1340 cm^?1 region characterizing local chemical interactions of the Ni²⁺ ions with the adenien N7 position, iii) lines at about 1483-and 1582 cm^?1 correlated to the anti/syn reorientation of the adenine residues on B-Z structure transition, iv) marker bands of the thymidine carbonyl group couplings at 1680-and 1733 cm^?1 due to the disposition of the thymidine residues in the Z helix specific geometry. Hence poly(dA-dT) poly(dA-dT) can adopt a Z form in solution. The Z form observed in alternate purine-pyrimidine sequences does not require G-C base pairs.     

Structure of Poly (dT)·Poly (dA)·Poly (dT)

Abstract

The molecular structure of poly (dT)·poly (dA)·poly (dT) has been determined and refined using the continuous x-ray intensity data on layer lines in the diffraction pattern obtained from an oriented fiber of the DNA. The final R-value for the preferred structure is 0.29 significantly lower than that for plausible alternatives. The molecule forms a 12-fold right- handed triple-helix of pitch 38.4 Å and each base triplet is stabilized by a set of four Crick-Watson-Hoogsteen hydrogen bonds. The deoxyribose rings in all the three strands have C2′-endo conformations. The grooveless cylindrical shape of the triple-helix is consistent with the lack of lateral organization in the fiber.     

The Structure of 5-Cyclohexyl-2′-Deoxyuridine as Studied by X-Ray Crystallography and NMR Spectroscopy

Abstract

5-Cyclohexyl-2′-deoxyuridine (I) is an example of a 5-substituted pyrimidine 2′-deoxynucleoside which exhibits no antiviral activity and which is not a substrate for either cellular or viral (herpes) kinases. Despite the fact that a cursory inspection of NMR spectra of the compound, taken in DMSO-d ₆ solution, suggested that the compound had a normal conformation, we here show that in the crystal and in aqueous solution (analysed by 2D NMR techniques), the conformation of this nucleoside has a syn-glycosidic and C4′-exo (₄E) sugar pucker conformation.     

The Structure of Poly(dA)· poly(dT) as Revealed by an X-ray Fibre Diffraction

Abstract

X-ray diffraction in fibres revealed that the calcium salt of poly(dA) · poly(dT) is a 10-fold double helix with a pitch of 3.23 nm. The opposite sugar-phosphate chains in the refined model are characterized by a complete conformational equivalence and contain sugars in a conformation close to C2′-endo.

As a result a new model of the sodium salt of poly(dA) · poly(dT)has been constructed, which is different from the Heteronomous DNA proposed earlier (S. Arnott et al., Nucl. Acids Res. 11, 4141 (1983)). The new model of Na-poly(dA) · poly(dT) has conformationally similar opposite chains; it is a structure of the B-type, rather like that of Ca-poty(dA) · poly(dT).     

Existence of the C Structure in Poly(dA-dC) · Poly(dG-dT)

Abstract

We show that the lithium salt of calf-thymus DNA can assume the C structure in nonoriented, hydrated gels. The transitions between the B and C structures showed little hysteresis and none of the metastable structural states which occur in oriented gels. Therefore crystal-lattice forces are not needed to stabilize the C structure.

The occurrence of the alternative structures of the Li, Na and K salts of poly(dA-dC) · poly(dG-dT) was measured as a function of hydration for nonoriented gels. Poly(dA-dC) · poly(dG-dT) · Li exists in the B structure at high hydrations and in the C structure at moderate hydrations with no A or Z structure at any hydration tested. The Na salt of poly(dA-dC) · poly(dG-dT) exists in the B structure at high hydration, as mixtures of B and C at moderate hydrations and in the A structure at lower hydrations. The potassium salt behaves similarly except that mixtures of the C and A structures exist at lower hydrations.

ZnCl₂ and NaNO₃, which promote the Z structure in duplex poly(dG-dC), promote the C structure in poly(dA-dC) · poly(dG-dT). Information contained in the sequence of base pairs and not specific ionic interactions appear to determine the stability of the alternative structures of polynucleotides as hydration is changed.     

Structure of Poly(dA)·Poly(dT) is not Identical to the AT Rich Regions of the Single Crystal Structure of CGCGAATTBrCGCG. The Consequence of this to Netropsin Binding to Poly(dA)·Poly(dT)

Abstract

The basic assumption of Dickerson and Kopka (J. Biomole. Str. Dyns. 2, 423, 1985) that the conformation of poly(dA)·poly(dT) in solution is identical to the AT rich region of the single crystal structure of the Dickerson dodecamer is not supported by any experimental data. In poly(dA)·poly(dT), NOE and Raman studies indicate that the dA and dT units are conformationally equivalent and display the (anti-S-type sugar)-conformation; incorporation of this nucleotide geometry into a double helix leads to a conventional regular B-helix in which the width of the minor groove is 8A. The derived structure is consistent with all available experimental data on poly(dA)·poly(dT) obtained under solution conditions. In the crystal structure of the dodecamer, the dA and dT units have distinctly different conformations—dA residues adopt (anti, S-type sugar pucker), while dT residues belong to (low anti, N-type sugar pucker). These different conformations of the dA and dT units along with the large propeller twist can be accommodated in a double helix in which the minor groove is shrunk from 8A to less than 4A. In the conventional right handed B-form of poly(dA)·poly(dT) with the 8A wide minor groove, netropsin has to bind asymmetrically along the dA strand to account for the NOE and chemical shift data and to generate a stereochemically sound structure (Sarma et al, J. Biomole. Str. Dyns. 2, 1085, 1985).     

Characteristics of Relationships Between Structure of Gluten Proteins and Dough Rheology – Influence of Dietary Fibres Studied by FT-Raman Spectroscopy

The aim of this research was to study which kind of conformational changes in gluten proteins were induced by addition of four dietary fibre (apple-cranberry, cacao, carob and oat) by using FT-Raman spectroscopy and to find relationships between conformational changes and rheological behaviour of bread dough in mixing and extensional tests. Structural studies showed that all fibres induced formation of β-like structures between two protein molecules (pseudo-β-sheets) with the band at 1616 cm^?1 in the Raman spectrum. According to Principal Component Analysis, the strongest dependence was between changes in gluten structure and two extensographic parameters (resistance to extension and extensibility). Resistance to extension was positively correlated with content of α-helix and pseudo-β-sheets, while a negative correlation was observed between the parameter and content of β-sheets and β-turns. Gauche-gauche-gauche conformation of disulphide bridges and ability of tyrosine residues to hydrogen bonds creation improved mixing properties as stability of dough.     

Micro-Heterogeneity and Micro-Rheological Properties of High-Viscosity Barley β-Glucan Solutions Studied by Diffusing Wave Spectroscopy (DWS)

Soluble fiber β-glucan is one of the key dietary materials in healthy food products known for reducing serum cholesterol levels. The micro-structural heterogeneity and micro-rheology of high-viscosity barley β-glucan solutions were investigated by the diffusing wave spectroscopy (DWS) technology. By comparing the mean-square displacement (MSD) of the microspheres imbedded in eight concentrations of β-glucan solutions, we found that the solutions exhibited nearly homogeneous behavior at ≤0.1 %, but the material showed a clear degree of heterogeneity at ≥0.25 %. Micro-rheology investigation revealed that β-glucan solutions displayed nearly perfect viscous behavior at ≤0.1 %, but the property changed into viscoelastic one at ≥0.25 %. The magnitude of high-frequency viscoelastic moduli for the 0.25 % - 0.75 % β-glucan solutions can be characterized by ?G*? ∝ ω^3/4, which is the semi-flexible polymer behavior. However, the magnitude of high-frequency viscoelastic moduli (?G*?) for the 1.0 % - 1.25 % β-glucan solutions is proportional to ω^1/2, which is the flexible polymer behavior. All micro-structural heterogeneity and micro-rheological property shifts occurred in relatively small concentration ranges.     

Comparative Studies of the Electronic Structure of 2-Chloro-2′-Deoxyadenosine Studied by 35CI-NQR Spectroscopy and Quantum Chemical Calculations

Abstract

Chlorine-35 NQR spectroscopy and quantum chemical calculations have been applied to provide detailed information on the structure and conformation of 2-chloro- 2′-deoxyadenosine and 2-chloroadenosine. The Gaussian package was used and the calculations were performed at the B3LYP level of the theory in the 6-31G? basis set.     

Membrane Curvature Revisited—the Archetype of Rhodopsin Studied by Time-Resolved Electronic Spectroscopy

G-protein-coupled receptors (GPCRs) comprise the largest and most pharmacologically targeted membrane protein family. Here, we used the visual receptor rhodopsin as an archetype for understanding membrane lipid influences on conformational changes involved in GPCR activation. Visual rhodopsin was recombined with lipids varying in their degree of acyl chain unsaturation and polar headgroup size using 1-palmitoyl-2-oleoyl-sn-glycero- and 1,2-dioleoyl-sn-glycerophospholipids with phosphocholine (PC) or phosphoethanolamine (PE) substituents. The receptor activation profile after light excitation was measured using time-resolved ultraviolet-visible spectroscopy. We discovered that more saturated POPC lipids back shifted the equilibrium to the inactive state, whereas the small-headgroup, highly unsaturated DOPE lipids favored the active state. Increasing unsaturation and decreasing headgroup size have similar effects that combine to yield control of rhodopsin activation, and necessitate factors beyond proteolipid solvation energy and bilayer surface electrostatics. Hence, we consider a balance of curvature free energy with hydrophobic matching and demonstrate how our data support a flexible surface model (FSM) for the coupling between proteins and lipids. The FSM is based on the Helfrich formulation of membrane bending energy as we previously first applied to lipid-protein interactions. Membrane elasticity and curvature strain are induced by lateral pressure imbalances between the constituent lipids and drive key physiological processes at the membrane level. Spontaneous negative monolayer curvature toward water is mediated by unsaturated, small-headgroup lipids and couples directly to GPCR activation upon light absorption by rhodopsin. For the first time to our knowledge, we demonstrate this modulation in both the equilibrium and pre-equilibrium evolving states using a time-resolved approach.     

Solution Structure of Poly(dA-dT)· Poly(dA-dT) in Low and High Salt: A 500 MHz 1H NMR Study Using One-Dimensional NOE

Abstract

CD spectra of poly(dA-dT)· poly(dA-dT) in low salt (10–100 mM NaCl) and high salt (4–6 M CsF) are different i.e. 275 nm band gets inverted in going from low to high salt (Vorhickova et. al.MarJ. Mol. Biol. 166, 85, 1983). However, from CD spectra alone it is not possible to decipher any structural differences that might exist between the low and high salt forms of poly(dA-dT)? poly(dA-dT). Hence, we took recourse to high resolution NMR spectroscopy to understand the structural properties of poly(dA-dT)? poly(dA-dT) in low and high salt. A detailed analysis of shielding constants and extensive use of NOE studies under minimum spin diffusion conditions using C(8)-deuterated poly(dA-dT)? poly(dA-dT) enabled us to come up with the following conclusions (i) base-pairing is Watson-Crick under low and high salt conditions, (ii) under both the conditions of salt the experimental data can be explained in terms of an equilibrium blend of right and left-handed B-DNA duplexes with the left-handed form 70% and the right-handed 30%. In a 400 base pairs long poly(dA-dT)? polyidA-dT) (as used in this study), equilibrium between right and left-handed helices can also mean the existence of both helical domains in the same molecule with fast interchange between these domains or/and unhindered motion/propagation of these domains along the helix axis, (iii) However, there are other structural differences between the low and high salt forms of poly(dA-dT) ? poly(dA-dT); under the low salt condition, right-and left-handed B-DNA duplexes have mononucleotide as a structural repeat while under the high salt conditions, right-and left-handed B-DNA duplexes have dinucleotide as a structural repeat. In the text we provide the listing of torsion angles for the low and high salt structural forms, (iv) Salt (CsF) induced structural transition in poly(dA-dT)? poly(dA-dT) occurs without any breakage of Watson- Crick pairing, (v) The high salt form of poly(dA-dT)? poly(dA-dT) is not the left-handed Z-helix.

Although the results above from NMR data are quite unambiguous, a question still remains i.e. what does the salt (CsF) induced change in the CD spectra of poly(dA-dT)? poly(dA-dT) really indicate? Interestingly, we could show that the salt (CsF) induced change in poly(dA-dT)? poly(dA-dT) is quite similar to that caused by a basic polypeptide viz. poly-L(Lys₂-Ala)_n i.e. both the agents induced a ψ-structure in DNA. And it was also demonstrated that the changes in poly(dA-dT)? poly(dA-dT) as caused by CsF and poly-L-(Lys₂-Ala)_n could be reverted back by ethidium bromide-a relaxing agent.

To minimize complications from spin diffusion in this study we have used very small presaturation pulse lengths and C(8)-deuterated poly(dA-dT)? poly(dA-dT) of 400 ± 150 bp long. Even though deuteration of a primary site of diffusion such as C(8)H substantially decreases diffusion, in order to make sure that our conclusions are not compromised by possible diffusion in such a long fragment under small presaturation times, we have repeated our experiments using the six base pair long duplex of d(A-T-A-T-A-T) and found the results to be strikingly similar to that from the polymer.     

The Preparation of Poly(A)±mRNA from the Hagfish Slime Gland

The isolation of translatable poly(A)^±mRNA from the slime glands of the Pacific hagfish, Eptatretus stouti, is not possible by the commonly used procedures because of the viscous slime that is formed when the contents of the glands are hydrated. This paper reports on a procedure developed to overcome this problem. Briefly, the tissue was powdered in liquid nitrogen, mixed with sodium lauroylsarcosine and proteinase K and lyophilized. The lyophilized powder was then mixed with 0.3 mm diameter glass beads, thoroughly ground and wetted with buffer and digested at 37°C. The RNA from the digest was recovered by ultracentrifugation through a CsCl cushion. Further purification of the RNA was accomplished by the usual methods with slight modifications.     

The Complex of Poly(dG) · Poly(dC) with Arginine: Stabilization of the B Form and Transition to Multistranded Structures

Abstract

We have studied by X-ray diffraction fibers of complexes of poly(dG)·poly(dC) with N-α-acetyl-L-arginine ethylamide. Although these polynucleotides favour the A form of DNA, in this complex it is never found, thus confirming that arginine prevents the appearance of this form of DNA At high relative humidity the B form is present. Upon dehydration two new structures appear. One of them is a triple helix, most likely formed by poly(dC⁺) · poly(dG) · poly(dC). The other structure found also has features which indicate a multistranded conformation.     

Bh-DNA: Variations of the Poly[d(A)] · Poly[d(T)] Structure within the Framework of the Fibre Diffraction Studies

Abstract

A refinement of the recent results for poly[d(A)] · poly[d(T)] (Alexeev et al., J. Biomol. Struct. Dyn. 4, 989 (1987)) involving additional parameters of the base-pair structure and of the sugar- phosphate backbone expands the conformational potential of this polynucleotide of the B type to include the possibility of bifurcated hydrogen bonds of the kind recently discovered in crystalline deoxyoligonucleotide with lone d(A)_n · d(T)_n stretch (Nelson et al., Nature 330, 221 (1987)).

Still, analysis of the available data and energy calculations do not seem to indicate that the bifurcated H-bonds are a crucial factor responsible for the anomalous structure of the d(A)_n · d(T)_n sequence. The unique structural properties of poly [d(A)] · poly[d(T)] can hardly be explained without taking into account its interactions with the double-layer hydration spine in the minor groove. In view of the hydration mechanism stabilizing poly [d(A)] · poly [d(T)] and of the polynucleotide's heteronomous prehistory (Arnott et al., Nucleic Acids Res. 11, 4141 (1983)) we suggest that this B-type structure be called B_h.     

Description of Base Motion and Role of Excitations in the Melting of Poly(dG) · Poly(dC)

Abstract

We study the contribution of various vibrational modes to the melting of poly(dG) · poly(dC). We find that the principal contribution comes from the H-bond breathing modes that have been observed in Raman scattering and that we have associated with helix melting. We show the softening of these modes on approach to melting in agreement with the observed behavior. We also describe the contribution to melting from base rotation modes that others have suggested are important in melting.     

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.     

Interactions Between Esterified Whey Proteins (α-Lactalbumin and β-Lactoglobulin) and DNA Studied by Differential Spectroscopy

Spectroscopic study of interactions between esterified whey proteins and nucleic acids, at neutral pH, showed positive differential spectra over a range of wavelength between 210 and 340 nm. In contrast, native forms of whey proteins added to DNA did not produce any differential spectra. The positive difference in UV absorption was observed after addition of amounts of proteins as low as 138 molar ratio (MR) of protein/DNA, indicating high sensitivity of the applied method to detect interactions between basic proteins and DNA. UV-absorption differences increased with MR of added whey protein up to saturation. The saturation points were reached at relatively lower MR in the case of methylated forms of the esterified protein as compared to its ethylated form. Saturation of nucleic acid (2996 bp long) was achieved using 850 and 1100 MR of methylated β-lactoglobulin and of methylated α-lactalbumin, respectively. Saturation with ethylated forms of the proteins was reached at MR of 3160 and 2750. Lysozyme, a native basic protein, showed a behavior similar to what was observed in the case of methylated forms of the dairy proteins studied. However, in the case of lysozyme, saturation was achieved at relatively lower MR (700). Methylated β-casein failed to give positive spectra at pH 7 in the presence of DNA. It interacted with DNA only when the pH of the medium was lowered to 6.5, below its pI. Generally, amounts of proteins needed to saturate nucleic acid were much higher than those needed to neutralize it only electrostatically, demonstrating the presence on DNA of protein-binding sites other than the negative charges on the sugar-phosphate DNA backbones. Addition of 0.1% SDS to the medium suppressed totally all spectral differences between 210–340 nm. The presence of 5 M urea in the medium reduced only the spectral differences between 210–340 nm, pointing to the role played by hydrophobic interactions. Peptic hydrolysates of esterified and native proteins or their cationic fractions (pH > 7) produced negative differential spectra when mixed with DNA. The negative differences in UV absorption spectra were the most important in the case of peptic hydrolysates of methylated derivatives of whey proteins.     

Structure and Dynamics of Netropsin-Poly(dA-dT)· Poly(dA-dT) Complex: 500 MHz 1H NMR Studies

Abstract

Antibiotic netropsin is known to bind specifically to A and T regions in DNA; the mode of binding being non-intercalative. Obviously, H-bonding between the proton donors of netropsin and acceptors N3 of A and 02 of T comes as a strong possibility which might render this specificity. In netropsin there could be 8 proton donors: four terminal amino groups and four internal imino groups. However, methylation of the terminal amino groups does not alter the binding affinity of netropsin to DNA—but the modification of the internal imino groups significantly lowers the binding affinity. Hence, the logical conclusion is that netropsin may specifically interact with A and T through H-bonding and in order to do so, it should approach the helix from the minor groove. The present paper provides experimental data which verify the conclusion mentioned above.

Using poly(dA-dT)? poly(dA-dT) as a model system it was observed following a thorough theoretical stereochemical analysis that netropsin could bind to -(T-A-T) sequence of the polymer in the B-form through the minor groove by forming specific B-bonding. Models could be either right or left-handed B-DNA with a mono or dinucleotide repeat.

By monitoring the ³¹P signals of free poly(dA-dT) ? poly(dA-dT) and netropsin-poly(dA-dT)? poly(dA-dT) complex we show that the drug changes the DNA structure from essentially a mononucleotide repeat to that of very dominant dinucleotide repeat; however the base- pairing in the DNA-drug complex remain to be Watson-Crick. Whether H-bonding is the specific mode of interaction was judged by monitoring the imino protons of netropsin in the presence of poly(dA-dT) ? poly(dA-dT). This experiment was conducted in 90% H₂O + 10% D₂O Using the time-shared long pulse. It was found that exchangeable imino protons of netropsin appear in the drug-DNA complex and disappear upon increasing the D₂O content; thus confirming that H-bonding is indeed the specific mode of interaction. From these and several NOE measurements, we propose a structure for poly(dA-dT)? poly(dA-dT(-netropsin complex.

In summary, experimental data indicate that netropsin binds to poly(dA-dT)? poly(dA-dT) by forming specific hydrogen bonds and that the binding interaction causes the structure to adopt a Watson-Crick paired dinucleotide repeat motif. The proposed hydrogen bonds can form only if the drug approaches the DNA from the minor groove. Within the NMR time scale the interaction between the ligand and DNA is a fast one. From the NOE experimental data, it appears that poly(dA-dT)? poly(dA-dT) in presence of netropsin exists as an equilibrium mixture of right- and left-handed B-DNA duplexes with a dinucleotide repeat—with a predominance of the left-handed form. The last conclusion is a soft one because it was very difficult to make sure the absence of spin diffusion. In a 400 base pairs long DNA duplex- drug complex (as used in this study), equilibrium between right and left-handed helices can also mean the existence of both helical domains in the same molecule with fast interchange between these domains or/and unhindered motion/propagation of these domains along the helix axis.     

Interaction of Pyrylium Dye with Self-Complementary DNA Oligomer as Studied by H NMR Spectroscopy‡

Abstract

Interaction of 2-methyl-4,6-bis-(4-N,N-dimethylaminophenyl) pyrylium salt (P2) with [d(CGACGTCG)]₂ was investigated by H NMR spectroscopy. The aromatic signals of P2 and the oligomer were shifted to the upfield by forming the complex, and intermolecular NOEs were also observed between P2 and the terminal CpG base steps but not between P2 and the central CpG. These results indicate that P2 binds to the weakly stacking CpG steps in an intercalation manner.

     

An Effective Enzyme Interacting with Poly (dT-dA)· Poly (dT-dA): A Dynamic Enhancer-Repressor Action

Abstract

The Green function technique is used to study the open hydrogen bond probability of poly(dT-dA)·poly(dT-dA) when an effective enzyme is attached to the helix. The DNA interstrand hydrogen bond mean motion and probability of fluctuating to an open state depends on the internal vibrational frequency of the enzyme. An enzyme with internal frequency of 80 cm ^?1 reduces hydrogen bond motion and the resulting probability of hydrogen bond fluctuational opening. An enzyme with internal frequency of 72 cm ^?1 increases hydrogen bond motion and the probability of hydrogen bond breaking.