Why Structured Water Causes Sharp Absorption by DNA at Microwave Frequencies

Abstract

Aqueous solutions of oligopolymer DNA have been observed by G.S. Edwards, C.C. Davis, M.L. Swicord and J.D. Saffer, Phys. Rev. Lett. 53, 1284(1984) to show structured absorption of microwave energy in the region of several gigahertz, characteristic of an ordered series of compressional normal mode vibrations propagating on the polymer chain. Although hydrodynamic coupling of such vibrations to the surrounding solvent would preclude the existence of sharp resonances, the molecular nature of the solvent in the near neighborhood of the polymer and - paradoxically- the strong water/polymer interactions provide a means for effectively decoupling the polymer motion from the dissipation of the liquid. Recent measurements of DNA/water relaxation times allow estimating numerical values in a parameterization of the decoupling effect. The resulting predicted frequency dependence explains many of the smaller features of Edwards' experiment as well as theoverall anomaly. A simple model gives a surprisingly complete account of the features of the data using only values determined from other experiments.     

Theory of the anomalous resonant absorption of DNA at microwave frequencies

Aqueous solutions of oligopolymer DNA have been observed by Edwards, Davis, Swicord & Saffer to show structured absorption of microwave energy in the region of several gigahertz characteristic of an ordered series of compressional normal mode vibrations propagating on the polymer chain. Hydrodynamic coupling of such vibrations to the surrounding solvent would preclude the existence of sharp resonances. The inclusion of electromagnetic interactions with surrounding counter ions yields a richer space of possibilities for complex behavior of the combined system. A well defined resonant absorption peak appears when the molecular motion and the nearby solvent motion are even slightly decoupled. The microwave electric fields in the vicinity of the molecule provide a mechanism for such a decoupling not present for the case of electrically neutral solvent.     

Theory of the Anomalous Resonant Absorption of DNA at Microwave Frequencies−

Abstract

Aqueous solutions of oligopolymer DNA have been observed by Edwards, Davis, Swicord & Saffer to show structured absorption of microwave energy in the region of several gigahertz characteristic of an ordered series of compressional normal mode vibrations propagating on the polymer chain. Hydrodynamic coupling of such vibrations to the surrounding solvent would preclude the existence of sharp resonances. The inclusion of electromagnetic interactions with surrounding counter ions yields a richer space of possibilities for complex behavior of the combined system. A well defined resonant absorption peak appears when the molecular motion and the nearby solvent motion are even slightly decoupled. The microwave electric fields in the vicinity of the molecule provide a mechanism for such a decoupling not present for the case of electrically neutral solvent.     

Local compressibilities of proteins: comparison of optical experiments and simulations for horse heart cytochrome-c

Spectroscopy with probe molecules yields local information on the environment of the probe. In this article we compare local compressibilities of cytochrome-c as obtained from molecular dynamics simulations with experimental results as obtained from spectroscopic measurements. The simulations show that the protein-core around the heme is much less compressible in a glycerol/water solvent than in pure water. The pocket is also much less compressible than the protein as a whole, although the compressibility of the water inside the rather incompressible protein-core is almost liquidlike. We show that the local compressibility values capture the collective correlations of local volume fluctuations with volume fluctuations in the surrounding protein-solvent system. The decoupling of the volume fluctuations of the core from the solvent shell explains the reduction of the heme-core-compressibility in glycerol/water solvent. This decoupling could be traced back to the suppression of the exchange between pocket-water and hydration-shell-water upon addition of glycerol as co-solvent.     

The denaturation transition of DNA in mixed solvents

The helix-to-coil denaturation transition in DNA has been investigated in mixed solvents at high concentration using ultraviolet light absorption spectroscopy and small-angle neutron scattering. Two solvents have been used: water and ethylene glycol. The "melting" transition temperature was found to be 94 degrees C for 4% mass fraction DNA/d-water and 38 degrees C for 4% mass fraction DNA/d-ethylene glycol. The DNA melting transition temperature was found to vary linearly with the solvent fraction in the mixed solvents case. Deuterated solvents (d-water and d-ethylene glycol) were used to enhance the small-angle neutron scattering signal and 0.1M NaCl (or 0.0058 g/g mass fraction) salt concentration was added to screen charge interactions in all cases. DNA structural information was obtained by small-angle neutron scattering, including a correlation length characteristic of the inter-distance between the hydrogen-containing (desoxyribose sugar-amine base) groups. This correlation length was found to increase from 8.5 to 12.3 A across the melting transition. Ethylene glycol and water mixed solvents were found to mix randomly in the solvation region in the helix phase, but nonideal solvent mixing was found in the melted coil phase. In the coil phase, solvent mixtures are more effective solvating agents than either of the individual solvents. Once melted, DNA coils behave like swollen water-soluble synthetic polymer chains.     

On the compact form of linear duplex DNA: globular states of the uniform elastic (persistent) macromolecule

A theory of collapse of DNA considered as unifilar homopolymer is suggested. The collapse is interpreted as the coil-globule transition. Three reasons of the collapse such as the confinement in a microcavity, the influence of poor low-molecular-weight solvent and the influence of polymeric solvent were studied. The results are summed up by the stage diagrams in variables: DNA length versus the characteristics of the compaction factor (the cavity volume, the energy of attraction of DNA segments in poor low-molecular-weight solvent and the concentration of polymer added). It is shown that a sufficiently long DNA forms the spherical compact particle while the relatively short DNA forms the toroidal one. More delicate features of the tertiary structure are determined by the relative role of the bending stiffness and steric repulsions in preventing further collapse. As the compaction occurs in polymeric solvent almost all added polymer is forced out from the globule. Thus, the internal structure of the compact DNA particle in polymeric solvent is similar to that in the model of microcavity.     

Nuclear magnetic resonance studies on a cyclic dodecapeptide analogue of a repeat hexapeptide of tropoelastin: evaluation of secondary structure.

The cyclododecapeptide, (Ala1-Pro2-Gly3-Val4-Gly5-Val6)2, was synthesized and its secondary structure was evaluated from extensive studies in dimethyl sulphoxide, trifluoroethanol and water using NMR methods. A selective decoupling technique in 13C-NMR has been utilized in order to assign the C=O carbon resonances. Temperature dependence of the peptide NH protons and the solvent perturbation of the peptide NH and C=O resonances show the occurrence in all solvents of a beta-turn (a 10-membered H-bond between the Val4 NH and Ala1 C=O) and a gamma-turn, an 11-membered H-bond between the Gly3 NH and the Gly5 C=O; and a possible 14-membered H-bond between the Ala1 NH and the Val4 C=O in dimethyl sulphoxide and trifluoroethanol. These secondary structural features are compared with the linear polyhexapeptide and found the the beta-turn and the gamma-turn are the common conformational features of these peptide systems.     

The temperature-dependent swelling of elastin

It is suggested that the temperature-dependent swelling behavior of water-swollen elastin is due entirely to the interaction of the numerous nonpolar groups in the elastin protein wiht the aqueous swelling solvent (i.e., ahydrophobic interaction). Flory-Rehner theory for network swelling was used to test this hypothesis. Calculated values for the solvent–polymer interaction parameter, χ1, derived from swelling data indicate that water is a very poor solvent for elastin at all temperatures over the range 0–70° C. Comparison of the calculated _χ1 values with theoretical values for the free energy of interaction of nonpolar solutes and water strongly suggests that the swelling behavior of elastin can be attributed quantitatively to hydrophobic interactions. The implications of these results for the structure and elastic mechanism of elastin are discussed.     

Temperature and concentration behavior of anomalous microwave resonances in DNA

We have calculated the expected absorption of microwave radiation in the gigaHertz frequency range by fixed-length DNA polymer molecules dissolved in saline solution. While the effects of counterions and solvent dynamics have been accounted for in detail, the features of the absorption are completely dominated by the interaction between the charged polymer and the so-called first hydration layer, that is, the nearest layer of solvent water molecules not actually bonded to the polymer. The relevant parameters of the interaction are the strength of the water-to-polymer coupling and the average persistence time of the individual water-to-polymer bonds. These are presumably hydrogen bonds to the oxygen atoms of the backbone phosphate structure. Using a given parameterization we can obtain the structured absorption corresponding to compressional wave phonon excitations on the polymer, "organ pipe" modes, such as have been claimed to be seen by Edwards, Davis, Swicord, and Saffer. While further studies have not confirmed these resonances, at some frequency and hydration these modes must become visible because of the high relaxation time measured by Lindsay, the existence of the resonances in relatively dry fibers and films of DNA, and the existence of underdamped modes in the ir spectrum of DNA in solution. We have examined the effects of varying salt concentration and the system temperature.(ABSTRACT TRUNCATED AT 250 WORDS)     

Pullulan and dextran: uncommon composition dependent Flory-Huggins interaction parameters of their aqueous solutions

Vapor pressure measurements were performed for aqueous solutions of pullulan ( M w 280 kg/mol) and dextran ( M w 60 and 2100 kg/mol, respectively) at 25, 37.5, and 50 degrees C. The Flory-Huggins interaction parameters obtained from these measurements, plus information on dilute solutions taken from the literature, show that water is a better solvent for pullulan than for dextran. Furthermore, they evince uncommon composition dependencies, including the concurrent appearance of two extrema, a minimum at moderate polymer concentration and a maximum at high polymer concentration. To model these findings, a previously established approach, subdividing the mixing process into two clearly separable steps, was generalized to account for specific interactions between water and polysaccharide segments. Three adjustable parameters suffice to describe the results quantitatively; according to their numerical values, the reasons for the solubility of polysaccharides in water, as compared with that of synthetic polymers in organic solvents, differ in a principal manner. In the former case, the main driving force comes from the first step (contact formation between the components), whereas it is the second step (conformational relaxation) that is advantageous in the latter case.     

Theory of acoustic mode vibrations of DNA fibers

A previous model for acoustic mode vibrations of a DNA molecule in water is extended to the case of an array of many DNA molecules, as occurs in the fibers studied in most experimental work on DNA. The acoustic modes of this system are found to consist of coupled modes of water sound vibrations and DNA acoustic modes. This model is used to study the electrostatic coupling of acoustic vibrations to the relaxational modes of the orientational degrees of freedom of the water molecules. It is found that the long-range or macroscopic electric field generated by the acoustic mode vibrations of the water-DNA system gives too small a damping and frequency shift of the acoustic modes to account for the observations on DNA fibers. Therefore, the observed damping and frequency shifts are most likely due to either friction between the surrounding water and the vibrating DNA, or coupling to the water orientation degrees of freedom resulting from the short range (i.e., screened) Coulomb interaction. The latter explanation (which is most likely the correct one) implies that the relaxation time of the hydration shell water is longer than the observed relaxation time by a factor of the static dielectric constant of the hydration water.     

Polymerase-Tailored Variations in the Water-Mediated and Substrate-Assisted Mechanism for Nucleotidyl Transfer: Insights from a Study of T7 DNA Polymerase

The nucleotidyl transfer reaction catalyzed by DNA polymerases is the critical step governing the accurate transfer of genetic information during DNA replication, and its malfunctioning can cause mutations leading to human diseases, including cancer. Here, utilizing ab initio quantum mechanical/molecular mechanical calculations with free-energy perturbation, we carried out an extensive investigation of the nucleotidyl transfer reaction mechanism in the well-characterized high-fidelity replicative DNA polymerase from phage T7. Our defined mechanism entails an initial concerted deprotonation of a conserved crystal water molecule with protonation of the γ-phosphate of the deoxynucleotide triphosphate(dNTP) via a solvent water molecule, and then the proton on the primer 3′-terminus is transferred to the resulting hydroxide ion. Subsequently, the nucleophilic attack takes place, with the formation of a metastable pentacovalent phosphorane intermediate. Finally, the pyrophosphate leaves, facilitated by the relay of the proton on the γ-phosphate to the α-β bridging oxygen via solvent water. The computed activation free-energy barrier is consistent with kinetic data for the chemistry step with correct nucleotide incorporation in T7 DNA polymerase. This variant of the water-mediated and substrate-assisted mechanism has features tailored to the structure of the T7 DNA polymerase. However, a unifying theme in the water-mediated and substrate-assisted mechanism is the cycling through crystal and solvent water molecules of the proton originating from the primer 3′-terminus to the α-β bridging oxygen of the deoxynucleotide triphosphate; this neutralizes the evolving negative charge as pyrophosphate leaves and restores the polymerase to its pre-chemistry state. These unifying features are likely requisite elements for nucleotidyl transfer reactions.     

Carbon-13 NMR of glycogen: hydration response studied by using solids methods

The carbon-13 NMR spectra of glycogen are reported by using the methods of magic-angle sample spinning and high-power proton decoupling to provide a dynamic report on the glucose monomer behavior as a function of hydration. Although the glycogen behaves as a typical polymer in the dry state, addition of water makes a significant difference in the spectral appearance. Water addition decreases the carbon spin-lattice relaxation times by 2 orders of magnitude over the range from 7% to 70% water by weight. The proton-carbon dipole-dipole coupling, which broadens the carbon spectrum and permits cross-polarization spectroscopy, is lost with increasing hydration over this range. By 60% water by weight, scalar decoupling methods are sufficient to achieve a reasonably high-resolution spectrum. Further, at this concentration, the carbon spin-lattice relaxation times are near their minimum values at a resonance frequency of 50.3 MHz, making acquisition of carbon spectra relatively insensitive to intensity distortions associated with saturation effects. Though motional averaging places the spectrum in the solution phase limit, the static spectrum shows a residual broader component that would not necessarily be detected readily by using high-resolution liquid-state experiments.     

Electric field effect on the helix–coil transition of poly(L-α,γ-diaminobutyric acid hydrochloride) in methanol/water mixtures

Transient electric birefringence of poly(L -α,γ-diaminobutyric acid hydrochloride) in methanol/water mixtures has been measured over a wide range of field strengths and solvent compositions and at different polymer concentrations and temperatures. The molar ellipticity at 222 nm and the specific Kerr constant underwent an abrupt change between 75 and 80 vol % methanol at 25°C, accompanied by a solvent-induced helix–coil transition. Anomalous birefringence transients were observed between 78 and 80 vol% methanol above threshold field strengths. The double logarithmic plots of the steady-state specific birefringence versus the square of field strength for different solvent compositions and polymer concentrations could be superimposed by shifting them horizontally along the abscissa and vertically along the ordinate except for the range where anomalous transients were observed. The threshold field strength could be estimated from the point at which a downward deviation occurred. It increased with increasing polymer concentration and with increasing methanol content on the verge of the transition region. The results were interpreted as indicating that a conformational change from the charged helix to the charged coil is induced by high fields in this system, as in the case of poly(L -lysine hydrobromide) in methanol/water mixtures.     

Z form of poly d(A-C).poly d(G-T) in solution studied by Raman spectroscopy.

Poly d(A-C).poly d(G-T) structures have been studied in solution by Raman spectroscopy, in presence of Na+, Mn2+ and Ni2+ counterions. Increase of the Na+ concentration or addition of Mn2+ ions up to 1M MnCl2 does not modify the B geometry of the polynucleotide. On the contrary, in conditions of low water activity (4M NaCl), the presence of small amounts of nickel ions (65 mM) induces a left-handed geometry of the DNA. The shift of the guanine line located at 682 cm-1 in B form to 622 cm-1 reflects unambiguously the C2'-endo/anti-greater than C3'-endo/syn reorientation of the deoxyribose-purine entities. Moreover modifications in the phosphate backbone lines indicate that the polymer is in a Z conformation. New or displaced lines corresponding to adenosine vibrations are correlated with the left-handed structure. An interaction of the Ni2+ ions specifically with the N7 site of purines, combined with a low water activity is necessary to promote the B-greater than Z transition.     

Influence of anions on the properties of microbial polysaccharides in solution

The order-disorder transition temperatures of the polysaccharides succinoglycan and xanthan are strongly influenced by the salts present in solution. High concentrations of anions such as bromide or thiocyanate lower the transition temperature, thus decreasing the stability of the polymer and increasing its susceptibility to acid catalysed degradation. Salts such as sulphate and phosphate raise the transition temperature but can cause precipitation, and result in the incompatibility of the polymers with certain brines. The effects are in line with the Hofmeister or lyotropic series. The two polysaccharides seem to fit into a spectrum including other biopolymers such as some proteins, although not DNA even though its behaviour is qualitatively similar. The effects arise from the interaction of the salts, primarily the anions, with the solvent water. The hydropholic nature of carbohydrates enables them to structure the solvent to a higher temperature than proteins. The importance of the effect of the polymer on the solvent in considering structure-property relationships cannot the overstressed.     

Raman spectroscopy of an O(2)-Co(II)bleomycin-calf thymus DNA adduct: alternate polymer conformations.

Bleomycin (Blm) is an antitumor agent which binds to specific sequences of DNA and as HO(2)-Fe(III)Blm causes single and double strand cleavage. In the present investigation, binding of O(2)-Co(II)Blm to a native DNA polymer, calf thymus DNA, was examined using conventional Raman spectroscopy. O(2)-Co(II)Blm is a model for O(2)-Fe(II)Blm, the direct precursor of HO(2)-Fe(III)Blm. Although the DNA polymer retained a predominant B-form structure, Raman spectral evidence was obtained for localized structural changes to A, C and Z-DNA forms. The presence of these alternate DNA forms within B-DNA implied the presence of B/A, B/C and B/Z junctions. The observed changes in DNA secondary structure were attributed to perturbation of structural water resulting from binding of O(2)-Co(II)Blm within the minor groove.     

Reversible helix/coil transitions of left-handed Z-DNA structures. Comparison of the thermodynamic properties of poly(dG).poly(dC), poly[d(G-C)].poly[d(G-C)], and poly(dG-m5dC).poly(dG-m5dC)

In contrast to poly(dG).poly(dC), which remains in the B-DNA conformation under all experimental conditions the polynucleotides with the strictly alternating guanine/cytosine or guanine/5'-methylcytosine sequences can change from the classical right-handed B-DNA structure to the left-handed Z-DNA structure when certain experimental conditions such as ionic strength or solvent composition are fulfilled. Up to now the investigation of the helix/coil transition of left-handed DNA structures was not possible because the transition temperature exceeds 98 degrees C. By applying moderate external pressure to the surface of the aqueous polymer solution in the sample cell the boiling point of the solvent water is shifted up the temperature scale without shifting the transition temperature, so that we can measure the helix/coil transition of the polynucleotides at all experimental conditions applied. It can thus be shown that the Z-DNA/coil transition is cooperative and reversible. The Tm is 125 degrees C for poly(dG-m5dC).poly(dG-m5dC) in 2mM Mg2+, 50mM Na+, pH 7.2 and 115 degrees c for poly[d(G-C)].poly[d(G-C)] in 3.04M Na+. The transition enthalpy per base pair was determined by the help of an adiabatic scanning microcalorimeter.     

IR spectroscopic studies of major cellular components. III. Hydration of protein,nucleic acid,and phospholipid films

The IR absorption spectra of protein, DNA, RNA, and phospholipid films as a function of the water content are reported. We find that the hydration of protein films affects the peak intensity of amide I and amide II bands and the shape of the amide III band. For nucleic acids, the symmetric (nu(S) PO(2) (-)) and antisymmetric (nu(AS) PO(2) (-)) stretching vibrations of the phosphate linkage are the most affected by hydration, because both intensity changes and frequency shifts are observed. The spectra of phospholipid films are also sensitive to hydration, and they exhibit changes in the peak intensities and frequencies of both nu(S) PO(2) (-) and nu(AS) PO(2) (-) vibrations. We interpret the spectral differences between water saturated and dried films both in terms of structural changes and the change in the local dielectric in the vicinity of the polar and solvent exposed groups. In addition, we observe that the most significant change in the absorption intensity, frequency, and shape of the water sensitive vibrations occurs at high hydration levels. The principal component analysis of hydration results and the kinetics of water removal from sample films are also discussed. In addition, protein spectra acquired using film and KBr pellet sampling techniques are compared.     

1H nuclear magnetic resonance double resonance study of oxytocin in aqueous solution.

Peptide NH resonances in the 250 MHZ 1H nuclear magnetic resonance (NMR) spectrum of oxytocin in H2O were assigned to specific amino acid residues by the "underwater decoupling" technique (i.e., decoupling from corresponding CalphaH resonances, which are buried beneath the intense water peak). These experiments confirm previous assignments of A. I. Brewster an V. J. Hruby ((1973), Proc. Natl. Acad. Sci. U.S.A. 70, 3806) and A. F. Bradbury et al. ((1974), FEBS Lett. 42, 179). Three methods of assigning NH resonances of peptides--solvent titration, underwater decoupling, and isotopic labeling--are compared. As the solvet composition is gradually changed from dimethyl sulfoxide to H2O, oxytocin undergoes a conformational change at 70-90 mol % of H2O. Exposure to solvent of specific hydrogens of oxytocin in H2O was studied by monitoring intensity changes of solute resonances when the solvent peak was saturated. Positive nuclear Overhauser effects (NOE's) of 14 +/- 5 were observed for the Tyr ortho CH and meta CH resonances, respectively. Comparative studies with deamino-oxytocin indicate that these effects result predominantly from intermolecular dipoledipole interaction between aromatic side chain CH protons and protons of the solvent. The NOE's therefore indicate intimate contact between water and the aromatic CH hydrogens of the Tyr side chain. The extent of saturation transferred by proton exchange between water and NH group varies with Ph in a manner which appears to reflect the acid-base catalysis of the protolysis reaction. There is no indication that any NH protons are substantially shiedled from the solvent.