Quasi-elastic light scattering study of salt induced conformational transitions of chromatin subunit

The translational diffusion coefficient D_T of monodisperse solutions of 146 base pairs (bp) core particles was studied by the quasi-elastic light scattering technique. When the salinity was raised a change of D_T from 1.9 × 10^?7 cm² s^?1 to 3.2 × 10^?7 cm² s^?1 was detected at about 2 mM NaCl, followed by a smooth decrease of D_T beyond 0.6 M NaCl. The measurements of particle concentration and scattering vector effects on the D_T showed that the influence of interactions between particles can be disregarded. The interaction between particles and counterions is also discussed and does not appear to be the origin of the actual changes in D_T. These transitions of D_T are hence related to changes of shape and size of the particles. It is shown that the single transition at low salinity corresponds to a conformational change while the variation of D_T at high salinity can be interpreted by a destabilization of the edifice. In different regions of salinities, the observed values of D_T can lead to reasonable hydrodynamic models.     

Dynamic light scattering of the bacteriophage T4B: determination of translational diffusion coefficients and centres of rotation

Using dynamic light scattering, the translational diffusion coefficient (D_T) and the distance between the hydrodynamic centre and the centre of the head (r₀) of the bacteriophage T4B have been determined. For a particle with retracted tail fibres we found D_T20.w =2.88 (2.88 ± 0.02) × 10^?8cm²s^?1 and r₀ = 52 ± 1 nm. For a phage with fully extended tail fibres D_T20w = (.210 ± 0.02) × 10^?8cm²s^?1 and r₀ = 112 ± nm. These data were obtained by interpreting the correlation function using a theory which takes into account the influence of the lollipop shape of the phage. In the literature this influence has not been taken into account, which has led to erroneous values of diffusion coefficients for T4B and other phages. The sedimentation coefficient of T4B phage is 1040 ± 5 S (fibres retracted) or 829 ± 4 S (fibres extended). With the above mentioned diffusion coefficients, these values correspond to a molecular weight of 236 × 10⁶ ± 3 × 10⁶. Finally, the theory used in this study is applied to other bacterial viruses, to correct reported values of the translational diffusion coefficients and of the corresponding molecular weights of these viruses.     

Translational and rotational diffusion of tobacco mosaic virus from polarized and depolarized light scattering

The translational and rotational dynamics of tobacco mosaic virus in sodium phosphate buffer (pH =7.5) solutions has been investigated by polarized and depolarized light scattering Rayleigh linewidth studies. For concentrations ranging from 1.75 × 10^?4 g ml^?1 to 0.25 × 10^?4 g ml^?1 the translational diffusion coefficient (D_T) has been found to be slightly concentration dependent and extrapolation to zero concentration gives D₀^20°C = 0.34 ± 0.01 × 10^?7 cm²S^?1. A full analysis of the polarized spectra obtained at high and low scattering angles and the depolarized spectra at near zero scattering angles has enabled these techniques to be compared and the rotational diffusion constant D_R to be determined. At a solution concentration of 1.75 × 10^?4 g ml^?1 a mean value is found to be D_R^20°C = 350 ± 30s^?1. These values of D_T and D_R are in approximate agreement with calculations based on models of the tobacco mosaic virus molecule as a cylindrical rod.     

Studies on the reactivity of malondialdehyde. I. Effects of acid concentration and solvent composition on deuterium exchange reactions

The rates of deuterium exchange reactions of malondialdehyde (MDA) and deuterated malondialdehyde (MDAd) have been studied as a function of acidity and the content of dimethyl sulfoxide (DMSO) in binary mixtures with D₂O . MDA incorporates deuterium from D₂O solutions in a first-order reaction with a rate constant (k_obs) that depends on the acid concentration. From this dependence, a catalytic constant, k_cat, can be derived (k_cat^MDA = 2.25 × 10⁵M^?s^?1). Similar kinetic behavior was found for MDAd in H₂O solutions, and in this case, k_cat^MDA = 1.56 × 10⁵M^?1s^?1. Results from reactions of MDA and MDAd in identical H₂OD₂O mixtures show that primary and secondary isotope effects are small (k_H/k_D = 1.13) and that solvent isotope effects cause most of the differences found between reactions in D₂O and H₂O. Reactions in binary DMSOd₆D₂O mixtures show a six-fold rate increase as the proportion of DMSOd₆ increases from 50% to 90%. These results also illustrate the relatively high reactivity of MDA at pH values well above its pK_a and the importance of medium composition on its reaction rate.     

Low frequency and diffusive motion in aligned phospholipid multilayers studied by pulsed NMR

Measurements of T₁, T_1?, T_1D and the FID are reported for protons in aligned stacks of Egg Yolk Lecithin (EYL)-D₂O multilayers. From the ω₁ dependence of T_1? and the ω₀ dependence of T₁ the two dispersive regions of the spectral density function were identified. The lower frequency region has a centre angular frequency of 2.2 × 10⁵ rad/s and the upper frequency region a centre angular frequency of 4 × 10⁷ rad/s.From the orientation dependence of T_1?, T_1D and the FID, the lower frequency dispersion is assigned to fluctuations in the packing density of the hydrocarbon chains in the plane of the bilayer, and the upper frequency region to the translational diffusion of the lipid molecules. Based on a similar approach to one previously described, a diffusion coefficient of 1.4 × 10^?8 cm²/s is calculated for the EYL molecules in the bilayers.     

Hydrolysis of p-nitrotrifluoroacetanilide catalyzed by water and imidazole

The hydrolyses of p-nitrotrifluoroacetanilide catalyzed by water and imidazole were examined at 70°C. The pH-rate constant profile of the hydrolysis in H₂O was examined in the pH range 0.0–11.4. The hydrolysis was independent of pH in the region from pH 1.0 to 4.5, presumably a water-catalyzed reaction. The rate constant and the D₂O solvent isotope effect for this reaction were 1.0 × 10^?4 sec^?1 and 3.7, respectively. Both natural imidazole and imidazolium cation catalyzed hydrolysis. The rate constant of the hydrolysis catalyzed by neutral imidazole was determined to be 5.4 × 10^?3M^?1 sec^?1 and the D₂O solvent isotope effect was 1.8.     

A quasi-elastic laser light scattering study of tubulin and microtubule protein from bovine brain

Quasi-elastic light scattering has been used to characterize the oligomeric properties of solutions of glycerol-cycled bovine microtubule protein, and the properties of the 30 S oligomeric species and 6 S tubulin heterodimer prepared by gel filtration on Sepharose 6B. It is shown that in dimer preparations, as little as 0.04% by number of 30 S rings would account for the difference between an observed mean diffusion coefficient D_{20, W} = 3.1 × 10^?7 cm² s^?1 and the value of D_{20, W} = 5.1 × 10^?7 cm² s^?1 calculated for tubulin dimer of M_rel 100,000. The 30 S ring has an observed diffusion coefficient of D_{20, W} = 0.49 × 10^?7 cm² s^?1. These values are not changed significantly by the presence of 4 m-glycerol, indicating the persistence of 6 S and 30 S forms for dimer and ring, respectively.Mixtures of ring and dimer components of this preparation behave as a non-interacting two-component system, indicating the absence of substantial re-equilibration between the species at 5 °C and pH 6.5.The effect of salt on ring and microtubule protein samples indicates partial dissociation, consistent with the formation of additional intermediate oligomeric forms.In quasi-elastic light scattering measurements adapted to kinetic studies, changes in the oligomeric composition of microtubule protein are detected in the early stages of the reversible assembly process at pH 6.5. A 25% decrease in scattered light intensity, without significant change in mean diffusion coefficient, indicates the lability of the ring oligomeric structures, which undergo partial transformation to alternative oligomeric species under these assembly conditions.     

Histone-induced conformational changes in DNA as probed by quasi-elastic light scattering.

Quasi-elastic light scattering as measured by intensity fluctuation (self-beat) spectroscopy in the time domain can be profitably used to follow both the translational diffusion D and the dominant internal flexing mode τ_int of DNA and its complexes with various histones in aqueous salt solutions. Without histones, DNA is found to have D = 1.6 × 10^?8 cm²/sec and τ_int ? 5 × 10^?4 sec in 0.8 M NaCl, 2 M urea at 20°C. Total histone as well as fraction F2A induce supercoiling (D = 2.6 × 10^?8 cm²/sec, τ_int ? 2.8 × 10^?4 sec) whereas fraction F1 induces uncoiling (D = 1.0 × 10^?8 cm²/sec, τ_int ? 9.4 × 10^?4 sec). Upon increasing the salt concentration to 1.5 M the DNA–histone complex dissociates (D = 1.8 × 10^?8 cm²/sec). Upon decreasing the salt concentration to far below 0.8 M, the DNA–histone complex eventually precipitates as a chromatin gel.     

Resonance coherent anti-Stokes Raman scattering (CARS) spectra of flavin adenine dinucleotide,riboflavin binding protein and glucose oxidase

Coherent anti-Stokes Raman scattering spectra, in resonance with the isoalloxazine visible electronic transition, have been obtained down to 300 cm^?1 for flavin adenine dinucleotide, riboflavin binding protein and glucose oxidase, in H₂O and D₂O. Several isoalloxazine vibrational modes can be identified by analogy with those of uracil. Of particular interest is a band at ～1255 cm^?1 in H₂O, which is replaced by another at ～1295 cm^?1, in D₂O. The H₂O band appears to be a sensitive monitor of H-bonding of the N3 isoalloxazine proton to a protein acceptor group. It shifts down by 10 cm^?1 in riboflavin binding protein, and disappears altogether in glucose oxidase. Other band shifts, of 3–5 cm^?1, are similar for the two flavoproteins, and may reflect environmental changes between aqueous solution and the protein binding pockets.     

Physical studies on proteins L3 and L24 from the 50 S subunit of the Escherichia coli ribosome.

Proteins L3 and L24, purified by a nondenaturing method from the 50 S ribosomal subunit of Escherichia coli A19, have been characterized. Both proteins were studied under conditions which resemble those used for reconstitution experiments. They were soluble at approximately 2–3 mg/ml and showed little or no aggregation. These proteins have s⁰_20,w values of 2.0 and 1.5 S, and D_20,w values of 7.6 × 10^?7 and 11.0 × 10^?7 cm² s^?1. Partial specific volumes at 20 °C are 0.730 and 0.740 ml g^?1 for the two proteins. The respective molecular weights determined by sedimentation equilibrium are 24,500 and 12,000. The intrinsic viscosity values for the two proteins are 6.0 and 4.0 ml g^?1. From these hydrodynamic parameters an elongated shape for L3 and a globular shape for L24 have been inferred.     

An investigation into possible quantum chaos in the H<Subscript>2</Subscript> molecule under intense laser fields via Ehrenfest phase space (EPS) trajectories

By employing the Ehrenfest "phase space" trajectory method for studying quantum chaos, developed in our laboratory, the present study reveals that the H₂ molecule under intense laser fields of three different intensities, I?=?1?×?10¹⁴ W/cm², 5?×?10¹⁴ W/cm², and 1?×?10¹⁵ W/cm², does not show quantum chaos. A similar conclusion is also reached through the Loschmidt echo (also called quantum fidelity) calculations reported here for the first time for a real molecule under intense laser fields. Thus, a long-standing conjecture about the possible existence of quantum chaos in atoms and molecules under intense laser fields has finally been tested and not found to be valid in the present case.     

Coordination chemistry of 7,9-disubstituted 6-oxopurine metal compounds. 4. Platinum(II) coordination at N(1). Molecular and crystal structure of [(ethylenediamine)bis(7,9-dimethylhypoxanthine)platinum(II)] hexafluorophosphate

The preparation and molecular and crystal structure of the complex [(ethylenediamine)bis(7,9,-dimethylhypoxanthine)platinum(II)] hexafluorophosphate, [Pt(C₂H₈N₂)(C₇H₈N₄O)₂] (PF₆)₂, are reported. The complex crystallizes in the monoclinic system, space group C2/c, with a = 12.334(2)Å, b = 10.256(2)Å, c = 22.339(3)Å, β = 101.31(1)°, V = 2771.0ų, Z = 4, D_measd = 2.087(3) g cm^?3, D_calc = 2.094 g cm^?3. Intensities for 3992 symmetry-averaged reflections were collected in the θ-2o scan mode on an automated diffractometer employing graphite-monochromatized MoKα radiation. The structure was solved by standard heavy-atom Patterson and Fourier methods. Full matrix least-squares refinement led to a final R value of 0.051. Both the ethylenediamine chelate and the PF₆^? anion are disordered. The primary coordination sphere about the Pt(II) center is approximately square planar with the bidentate ethylenediamine ligand and the N(1) atoms [Pt(II) ? N(1) = 2.020(5)Å] of two 7,9-dimethylhypoxanthine bases (related by a crystallographic twofold axis of symmetry) occupying the four coordination sites. The exocyclic O(6) carbonyl oxygen atoms of the two 7,9-dimethylhypoxanthine ligands participate in intracomplex hydrogen bonding with the amino groups of the ethylenediamine chelate [N(ethylenediamine) ? O(6) = 2.89( )Å]. The observed Pt ? O(6) intramolecular distances of 3.074(6)Å are similar to those found in other Pt(II) N(1)-bound 6-oxopurine complexes and in several Pt(II) N(3)-bound cytosine systems.     

Joining of bacteriophage T4D heads and tails: A kinetic study by inelastic light scattering

We have used inelastic laser light scattering to study the kinetics of the spontaneous assembly of heads and tails of bacteriophage T4D to form noninfectious tail fiberless particles. For interpretation of the kinetics, it was first necessary to determine the physical properties of the strongly scattering phage parts. For heads, these are D_{20,w = 3.60 × 10⁻⁸cm²/s, 820,w = 1025 S, M = 1.76 × 10⁸}. For tail fiberless particles, D_20,w = 3.14 × 10⁻⁸cm²/s, 8_20,w = 968 S, and M = 1.95 × 10⁸. The kinetics of the head-tail joining process was followed by measuring the time variation of the homodyne scattering autocorrelation function. This was interpreted as a sum of exponentials whose decay constants were known from the scattering angle and the diffusion coefficients, and whose amplitudes were related to the concentrations of reactants and products. Scattering experiments at 22 °C gave a bimolecular rate constant of 1.02 × 10⁷m⁻¹ s⁻¹, while infectivity assays at 30 °C gave a rate constant of 1.28 × 10⁷. Adjustment of both rate constants to 20 °C, assuming diffusion controlled reaction, gave 0.97 × 10⁷ and 0.98 × 10⁷m⁻¹ s⁻¹, respectively. This rate is about $\text{1}\text{500}$ that predicted by Smoluchowski theory for a diffusion controlled reaction between two spherical particles; the discrepancy is largely explicable from orientational factors.     

Protein Rotational Dynamics in Aligned Lipid Membranes Probed by Anisotropic T1ρ NMR Relaxation

A membrane-bound form of Pf1 coat protein reconstituted in magnetically aligned DMPC/DHPC bicelles was used as a molecular probe to quantify for the viscosity of the lipid membrane interior by measuring the uniaxial rotational diffusion coefficient of the protein. Orientationally dependent ¹⁵N NMR relaxation times in the rotating frame, or T_1ρ, were determined by fitting individually the decay of the resolved NMR peaks corresponding to the transmembrane helix of Pf1 coat protein as a function of the spin-lock time incorporated into the 2D SAMPI4 pulse sequence. The T_1ρ relaxation mechanism was modeled by uniaxial rotational diffusion on a cone, which yields a linear correlation with respect to the bond factor sin⁴θ_B, where θ_B is the angle that the NH bond forms with respect to the axis of rotation. Importantly, the bond factors can be independently measured from the dipolar couplings in the separated local-field SAMPI4 spectra. From this dependence, the value of the diffusion coefficient D_|| = 8.0 × 10⁵ s^?1 was inferred from linear regression of the experimental T_1ρ data even without any spectroscopic assignment. Alternatively, a close value of D_|| = 7.7 × 10⁵ s^?1 was obtained by fitting the T_1ρ relaxation data for the assigned NMR peaks of the transmembrane domain of Pf1 to a wavelike pattern as a function of residue number. The method illustrates the use of single-helix transmembrane peptides as molecular probes to assess the dynamic parameters of biological membranes by NMR relaxation in oriented lipid bilayers.     

Arsenazo I and tetramethylmurexide as optical calcium indicators

Calcium-binding stoichiometry, dissociation equilibrium constants at zero ionic strength (K⁰), and molar extinction difference coefficients (Δ?_λ) at the wavelength λ of the metallochromic indicators arsenazo I (ArsI) and tetramethylmurexide (TMX) were reevaluated with a computerized method based on mass conservation and thermodynamic consistency checks. This new method is shown to provide a more critical assessment of the assumed calcium-dye complexing model than is afforded by the commonly used reciprocal-plot method. The analyses of spectrophotometric Ca titrations confirm that both dyes form only 1:1 complexes in aqueous solution. For TMX, K⁰ = 1.3 × 10^?3m and Δ?₄₈₀ = 1.5 × 10⁴m^?1 cm^?1; for ArsI, K⁰ = 5.8 × 10^?3m and Δ?₅₆₂ = 1.8 × 10⁴m^?1 cm^?1 at pH 7.0 and T = 293°K. The discriminatory power of the analytical method is demonstrated by comparison of these results with those found for a different dye, arsenazo III, which complexes Ca in 1:1, 1:2, and 2:1 forms.     

A reaction of the superoxide radical with tetrapyrroles

Bilirubin and biliverdin were bleached during exposure to the aerobic xanthine oxidase reaction. Enzymic scavenging of O₂^?, by Superoxide dismutase, inhibited, whereas enzymic scavenging of H₂O₂, by catalase, did not. Increasing the rate of production of O₂^? without increasing the turnover rate of xanthine oxidase, by increasing pO₂, accelerated the bleaching of the biliverdin. Moreover, a scavenger of OH·, such as benzoate, or an inactivating chelating agent for iron, such as diethylenetriamine pentaacetate or desferrioxamine mesylate, did not inhibit. It follows that O₂^? can directly attack these tetrapyrroles. Kinetic competition between Superoxide dismutase and bilirubin yielded a value for k_{bilirubin, O2^?} = 2.3 × 10⁴ M^?1s^?1 at pH 8.3 and at 23 °C. A similar experiment for biliverdin yielded a value for k_{bilirubin, O2^?} = 7 × 10⁴ M^?1s^?1.     

Solvent effects on the dynamics of (dG-dC)3

The kinetics of the coil-to-helix transition of (dG-dC)₃ in M NaCl, 45 mM sodium cacodylate, pH 7, were measured in H₂O, D₂O, 10 mol % ethanol, 10 mol % urea, and 10 mol % glycerol. At 43°C in H₂O the recombination rate is 1.3 ± 0.2 × 10⁷ M^?1 s^?1; the dissociation rate is 68 ± 10 s^?1. The destabilization of the helix in 10 mol % ethanol and 10 mol % urea relative to water is primarily due to a large increase in the helix-dissociation rate. In 10 mol % glycerol, the destabilization of the helix is due to a decrease in the recombination rate and an increase in the dissociation rate. Above 20°C, two exponential decays longer than 1 μs are observed after a temperature jump. The slower relaxation time is 4–10 times faster than the bimolecular component and is independent of oligomer concentration. We attribute this relaxation to a rapid equilibrium between two helical states. At low temperatures and oligomer concentrations of 1 mM or greater, the helices aggregate in 1M NaCl. Experimental data are presented under conditions where aggregation is unimportant and evidence is given that the ΔH-determined spectroscopically is unaffected by aggregation.     

D2O-induced ion channel activation in Characeae at low ionic strength

Effects of D₂O were studied on internodal cells of the freshwater alga Nitellopsis obtusa under plasmalemma perfusion (tonoplast-free cells) with voltage clamp, and on Ca²⁺ channels isolated from the alga and reconstituted in bilayer lipid membranes (BLM). External application of artificial pond water (APW) with D₂O as the solvent to the perfused plasmalemma preparation led to an abrupt drop of membrane resistance (R _m = 0.12 ±0.03 kΩ · cm²), thus preventing further voltage clamping. APW with 25% D₂O caused a two-step reduction of R _m : first, down to 2.0 ± 0.8 kΩ · cm², and then further to 200 Ω · cm², in 2 min. It was shown that in the first stage, Ca²⁺ channels are activated, and then, Ca²⁺ ions entering through them activate the Cl^? channels. The Ca²⁺ channels are activated irreversibly. If 100 mm CsCl was substituted for 200 mm sucrose (introduced for isoosmoticity), no effect of D₂O on R _m was observed. Intracellular H₂O/D₂O substitution also did not change R _m . In experiments on single Ca²⁺ channels in BLM H₂O/ D₂O substitution in a solution containing 100 mm KCl (trans side) produced no effect on channel activity, while in 10 mm KCl, at negative voltage, the open channel probability sharply increased. This effect was irreversible. The single channel conductance was not altered after the H₂O/D₂O substitution. The discussion of the possible mechanism of D₂O action on Ca²⁺ and Cl^? channels was based on an osmotic-like stress effect and the phenomenon of higher D-bond energy compared to the H-bond.     

Hemoglobin-water interactions in normal and sickle erythrocytes by proton magnetic resonance T1ϱ measurements

The dependence of the water proton magnetic resonance spin-lattice relaxation rate (T_1?^?1) in the rotating frame on the strength of the spin-locking (H₁) field has been investigated for packed oxy and deoxy normal and sickle erythrocytes at temperatures from 9 to 40 °C. The T_1?^?1 of oxy or deoxy normal erythrocytes shows no dependence on H₁ up to ~7 G at any temperature studied. On the other hand, T_1?^?1 decreases from about 40 s^?1 to 15 s^?1 (H₁ from 0 to ~7 G) for deoxygenated packed sickle cells at 40 °C. The magnitude of this variation of T_1?^?1 with H₁ decreases with decreasing temperature. Oxy packed sickle cells also show a dependence of T_1?^?1 on H₁ but the magnitude is <10% of that of the deoxygenated samples. These results suggest that water proton T_1?^?1 measurements are a sensitive probe of hemoglobin S polymerization and provide a novel technique for the study of slow water motions in these systems. The T_1?^?1 results are compared with low frequency T₁^?1 results of other investigators on hemoglobin S solutions. Analysis of the data suggests that water proton motions with correlation times of the order of 10^?5 s are present in the deoxygenated sickle cell samples at temperatures above 10 °C.     

Translational diffusion in the plasma membrane of sea urchin eggs

Translational diffusion in the plasma membrane of individual egg cells from the sea urchin species Paracentrotus lividus has been studied by fluorescence microphotolysis (FM). In order to probe the lipid phase of the membrane, procedures have been worked out by which the fluorescent analog 3,3′-dioctadecyl-oxatricarbocyanine (C₁₈diO) can be incorporated into the membrane. In the unfertilized egg a fraction R = 0.9 of C₁₈diO was mobile having an apparent diffusion coefficient of D = 6.0 × 10^?9 cm² sec^?1. Fifteen to twenty-five minutes after fertilization R and D were reduced to 0.8 and 2.7 × 10^?9 cm² sec^?1, respectively. In order to study diffusion of membrane proteins, procedures have been worked out by which the cell surface can be labeled with fluorescein-isothiocyanate (FITC). FITC binds to both the plasma membrane and the vitelline layer. Together with the vitelline layer two-thirds of the FITC-fluorescence could be removed from the egg surface. Gel electropherograms of isolated egg cortices showed various protein bands; however, only two of the protein bands were labeled with FITC. In the unfertilized egg a fraction R = 0.9 of the FITC-labeled membrane proteins was mobile having an apparent diffusion coefficient of D = 35 × 10^?11 cm² sem^?1. Fiteen to twenty-five minutes after fertilization R and D were reduced to 0.8 and 7.0 × 10^?11 cm² sec^?1, respectively. FITC-labeled proteins of the fertilization envelope were immobile. Our studies have shown (i) that the egg surface can be fluorescently labeled without blocking fertilization and early development, (ii) that the plasma membrane of unfertilized eggs is a fluid environment permitting a rapid movement of lipids and proteins, and (iii) that after fertilization a substantial degree of lipid and protein mobility is maintained.