Viscosity-molecular weight relationships,intrinsic chain flexibility,and dynamic solution properties of guar galactomannan

Molecular theories of the viscosity of dilute and more concentrated solutions of random-coil polymers have been applied to five molecular-weight fractions of guar galactomannan. The variation in intrinsic viscosity ([η]; dL.g^?1) with molecular weight (M_r) followed the relationship [η] = 3.8 × 10^?4) M_r^0.723, consistent with random-coil behaviour. The intrinsic stiffness of the galactomannan backbone was estimated by evaluating the “characteristic ratio” C_∝, which is ～ 12.6 and agrees well with results for carboxymethylcellulose, which has a closely similar, β-(1→4)-linked polymer backbone. At intermediate concentrations (c), up to specific viscosities of ～ 10, η_sp was proportional to c^1.3, while at higher concentrations, η_sp was ～c^5.1. This exponent is higher than is usually observed for polymers interacting purely by physical entanglement, and is evidence for more specific polymer-polymer interactions (“hyperentanglements”). The concentration dependence and the time-scale of entanglement coupling have been monitored by both steady-shear and oscillatory measurements, and a generality of response has been demonstrated.     

Infinite dilution viscoelastic properties of poly(gamma-benzyl-L-glutamate) in m-cresol.

The real and imaginary parts of complex viscosity, η′ and η″, are measured for dilute solutions of poly(γ-benzyl-L -glutamate) in m-cresol, a helicogenic solvent. The frequency range is 2.2–525 kHz; the concentration range 0.2–5 g/dl; the temperature 30°C, and the molecular weights M_r are 6.4 × 10⁴–17 × 10⁴. The dispersion curve of extrapolated intrinsic dynamic viscosity [η′] of samples with M_r > 10⁵ is interpreted in terms of three mechanisms appearing from low to high frequencies: end-over-end rotation, flexural deformation, and side-chain motion. For a sample with M_r < 10⁵, the flexural relaxation disappears and a plateau of [η′] is distinctly observed between rotational and side-chain relaxations. Rotational relaxation times of all the samples obey the Kirkwood–Auer theory. The strong concentration dependence of rotational relaxation time is explained by collisions of molecules rather than association. Flexural relaxation times calculated from a theory by assuming the persistence length as 1200 Å are consistent with observed dispersion curves of [η′].     

The effect of solvent viscosity and temperature on DNA viscoelastic behavior

The effect of solvent viscosity (η_s) and temperature (T) on the shape of the concentration dependence of the principal and total recoils in creep-recovery viscoelastometry experiments has been studied for T4 DNA solutions. The range of DNA concentration (c) was 2 – 40 μg/ml; glycerol, 70–80% v/v, sucrose, 60% v/v; NaCl, 5 mM – 1M; and T, 275 – 323 K. A linear proportionality between recoil and c was obtained at high η_s/T. At low η_s/T, the c-dependence was nonlinear, approaching saturation at higher c. At low c, the slope of both curves was the same. Transition between “linear” and “nonlinear” values occurred over a narrow range of η_s/T (a width of 1–5 K if η_s/T was changed by varying T). (η_s/T)_tr, the midpoint of the transition, was independent of solvent properties other than viscosity. Also, (η_s/T)_tr increased with c. For a given c, η_s/T values above this transitional value yield linear behavior; below this, nonlinear behavior. The ratio of linear to nonlinear recoil values is a linear function of c with K_c, the slope of this dependence, independent of η_s and T. A kinetic model for the observed nonlinearity of recoil with c is presented. It explains the independence of K_c on η_s and T. An attempt has been made to explain the linear–nonlinear transitions by comparison of τ₁ and T_R, the lifetime of the contact points of the polymer network in the de Gennes theory. The nonlinear values are consistent with a pseudogel that exists when τ₁ < T_R. At τ₁ > T_R, the DNA behavior is similar to that in dilute solutions (linear values). Thus, the condition for transition is τ₁ = T_R. However, some unsolved problems remain.     

Sedimentation and viscosity of bacteriophage T7 DNA in presence of CH3HgOH

The effects of increasing concentartions of methylmercuric hydroxide (CH₃HgOH) on the rate of sedimentation, S⁰, and intrinsic viscosity, [η], of T7 DNA have been studied at 20°C in 0.005, 0.05, and 0.5M Na₂SO₄, respectively, whereby each salt solvent conatined, in addition, 0.005M sodium borate, pH 9.18, as a buffer. Both S⁰ and [η] are independent of organomercurial concentration as long as DNA remains native. Denaturation, brought about by the complexing of CH₃HgOH with the polymer, produces large changes in S⁰ as wll as [η]. The sedimentation coefficient increases strongly with increasing oragnomercurial concentration once strand separation has occured. Experimental difficulties prevented measuring of [η] in the posttransition region. The data on S⁰ have been used, in combination with available information on the so-called density increment (?ρ/?c₂), to obtain information on the frictional properties of single-stranded and methylmercurated T7 DNA. The frictional coefficient, defined as f′₂ = M₂(?p/?c₂)/S⁰ηN_A, where M₂ is the molecular wieght of T7 DNA, c₂ is the concentration of DNA in g/ml of solution, η_r the realtive viscosity of the salt solvents, and N_A is Avogadro's number, was evaluated for all three salt media as a function of organomercurial concentration. f′₂ of native T7 DNA was found not to be sensitive to changes in ionic strngth; but f′₂ of single-stranded and methylmercurated T7 DNA varied strongly with salt concentration. Since f′₂ of single-stranded T7 DNA was barely affected by organomercurial concentration at a given ionic strength, it is concluded that the dramatic variations of S⁰ with pM (pM ≡ -log[CH₃HgOH]) observed in the posttransition zone reflect only changes in the thermodynamic interactions (“preferential interactions”) existing between DNA and the vatious other solution components, but not changes in the coil dimensions of the polymer.     

The LiCl effect on the conformation of lentinan in DMSO

Lentinan (β‐(1→3)‐D ‐glucan) was found to be successfully fractionated by the mixture of dimethyl sulfoxide (DMSO) and lithium chloride (LiCl) as a solvent and acetone as a precipitant. Light scattering and viscosity measurements were made on solutions of fractionated samples in pure DMSO and 0.2M LiCl/DMSO in the range of the molecular weight M_w from 21.7 × 10⁴ to 84.7 × 10⁴. The values of M_w in both solvents were almost the same, but the remarkable difference between the values of intrinsic viscosity [η] demonstrated that the LiCl/DMSO solvent greatly enhances the stiffness of the lentinan backbone. The observed intrinsic viscosity [η] was analyzed by the Yoshizaki‐Nitta‐Yamakawa theory of a worm‐like chain, and the persistence length q and molecular weight per unit contour length M_L were determined roughly as 6.0 nm and 890 g nm^?1 in 0.2M LiCl/DMSO, and 5.1 nm and 890 g nm^?1 in pure DMSO, respectively. This slightly larger persistent length in 0.2M LiCl/DMSO also confirmed the higher stiffness of lentinan enhanced by the LiCl/DMSO solvent. The enhancement of the chain stiffness was ascribed to the electrostatic repulsion because of the hydrogen bonding of the hydroxyl protons of lentinan with the chloride ion, which is in turn associated with the Li⁺(DMSO)_n macrocation complex. © 2012 Wiley Periodicals, Inc. Biopolymers 97: 840–845, 2012.     

Oxidation of NADH by plant mitochondria: Kinetics and effects of calcium ions

The kinetics of NADH oxidation by the outer membrane electron transport system of intact beetroot (Beta vulgaris L.) mitochondria were investigated. Very different values for V_max and the K_m for NADH were obtained when either antimycin A-insensitive NADH-cytochrome c activity (V_max= 31 ± 2.5 nmol cytochrome c (mg protein)^?1 min^?1; K_m= 3.1 ± 0.8 μM) or antimycin A-insensitive NADH-ferricyanide activity (V_max= 1.7 ± 0.7 μmol ferricyanide (mg protein)^?1 min^?1; K_m= 83 ± 20 μM) were measured. As ferricyanide is believed to accept electrons closer to the NADH binding site than cytochrome c, it was concluded that 83 ± 20 μM NADH represented a more accurate estimate of the binding affinity of the outer membrane dehydrogenase for NADH. The low K_m determined with NADH-cytochrome c activity may be due to a limitation in electron flow through the components of the outer membrane electron transport chain. The K_m for NADH of the externally-facing inner membrane NADH dehydrogenase of pea leaf (Pisum sativum L. cv. Massey Gem) mitochondria was 26.7 ± 4.3 μM when oxygen was the electron acceptor. At an NADH concentration at which the inner membrane dehydrogenase should predominate, the Ca²⁺ chelator, ethyleneglycol-(β-aminoethylether)-N,N,-tetraacetic acid (EGTA), inhibited the oxidation of NADH through to oxygen and to the ubiquinone-10 analogues, duroquinone and ubiquinone-1, but had no effect on the antimycin A-insensitive ferricyanide reduction. It is concluded that the site of action of Ca²⁺ involves the interaction of the enzyme with ubiquinone and not with NADH.     

Effect of the cations sodium,potassium and calcium on the interaction of hyaluronate chains: a light scattering and viscometric study

Light scattering and viscometric studies have been carried out on two preparations, A and B, of rooster comb hyaluronate. Sedimentation rate studies have also been performed with A. Light scattering measurements in 0.2 m KCl for preparation A gave a molecular weight of 3.3 × 10⁶ and for B, 1.0 × 10⁶. In (0.1–0.3) M NaCl similar measurements gave a particle weight for A of (4.4–6.4 × 10⁶ and for B (1.7–2.8 × 10⁶. In 0.066 m CaCl₂ molecular weight values of 9.5 × 10⁶ for A and 1.7 × 10⁶ for B were obtained. Thus in the presence of Na⁺ and Ca²⁺ ions aggregates of chains persisted into dilute solution. Measurements by light scattering on A and B in 4 m guanidinium chloride gave values in the same range as those obtained in 0.2 m KCl. Sedimentation rate studies on A gave values of 10.3 Svedbergs in 0.2 m KCl and 12.2 Svedbergs in 0.2 m NaCl and 0.066m CaCl₂. The shear dependence of the viscosity was studied using a conicylindrical viscometer at shear rates between 0.5 and 20 s^?1. Preparation A in 0.2 m KCl and NaCl yielded values for (ν_sp/cc→0 of 5000 and 7100 ml g^?1 respectively in keeping with the tendency to aggregate. The behaviour for preparation B was similar. In 0.066 m CaCl₂ there was a marked dependence of viscosity on shear speed below 10 s^?1 for all concentrations and the value of (ν_sp/c)→0 at 0 s^?1 for preparation A was 7700 ml g^?1 while at a shear rate of 8 s^?1 (ν_sp/c)c→0 ? 5000 ml g ^?1. Similar effects were found for preparation B and the data suggest associations of chains disruptable by weak shear forces. The increase in viscosity with concentration in the presence of 0.066 m CaCl₂ was much less than in the presence of KCl or NaCl, suggesting that the Ca²⁺ had a marked effect on the ”rigidity’ of the molecules in solution. A viscometric titration experiment with Ca^2? showed that a level of 0.02 m CaCl₂ in 0.2 m NaCl was sufficient to produce the change in viscosity presented above and that significant perturbations of the viscosity were present at 0.005?0.01 m CaCl₂.     

Direct evidence for the presence of a rotenone-resistant NADH dehydrogenase on the inner surface of the inner membrane of plant mitochondria

Submitochondrial particles (SMP) were produced from Jerusalem artichoke (Helianthus tuberosus L.) mitochondria by sonication and differential centrifugation. The SMP were about 50% inside-out as measured by the access of reduced cytochrome c to cytochrome c oxidase. Uncoupled NADH oxidation (1 mM NADH) by the SMP was 120 nmol O₂ min^?1mg^?1, which was reduced to 98 nmol O₂ min^?1 (mg mitochondrial protein)^?1 in the presence of EGTA. In contrast, the oxidation of NADH by intact mitochondria was completely inhibited by EGTA (from 182 to 14 nmol O₂ min^?1mg^?1). The EGTA-resistant NADH oxidation by the SMP is ascribed to the NADH dehydrogenase(s) on the inside of the inner membrane and exposed to the medium in the inside-out SMP. In the presence of EGTA it could be shown that two NADH dehydrogenase activities were present in the SMP. One had an apparent K_m of 7 μM for NADH, a V_max of 80 nmol NADH min^?1mg^?1, and was rotenone-sensitive. This dehydrogenase is equivalent to the mammalian Complex I NADH dehydrogenase. The other dehydrogenase, which was rotenone-resistant, had a K_m of 80 μM and a V_max of 131 nmol NADH min^?1mg^?1; it is probably responsible for the rotenone-resistant oxidation of organic acids often observed in plant mitochondria. The redox poise of the pyridine nucleotides had only a small effect on the relative rates of the two internal dehydrogenases. Electron flow through these dehydrogenases appears, therefore, to be regulated mainly by the concentration of NADH in the matrix of the mitochondria.     

Immobilized glucose dehydrogenase for cofactor regeneration in heme-catalyzed demethylation and hydroxylation reactions

Glucose dehydrogenase (E.C. 1.1.1.47) from B. megaterium M 1286 was immobilized together with mutarotase (E.C. 5.1.3.3) on several organic carriers and by different methods. The storage stability of the enzyme at pH-values > 6 is slightly improved by immobilization and the pH-optimum is shifted from 8.3 to 8.0. Kinetic constants of the immobilized enzyme are: K′_M(NAD⁺) = 5.36 × 10^?4 mol/l K′_M(glucose) = 3.76 · 10^?2 mol/l and V′_max = 5.54 · 10^?5 mol/(l min g carrier) for the most active preparation (2.16 mg enzyme/g carrier). In reactor experiments the immobilized glucose dehydrogenase was used with glucose to regenerate NADPH in NADPH-dependent iron-III-protoporphyrin-IX-imidazole catalyzed hydroxylation and demethylation of model substrates of cytochrome P-450. The advantages of the coupling of both reactions with cofactor recycling are shown and discussed.     

Dynamic viscoelastic properties of solutions of shear-degraded deoxyribonucleic acid

Calf thymus and salmon sperm deoxyribouncleie acid were degraded by high-shear stirring to molecular weights M in the range of 1.3–3.2 × 10⁶ and purified by chromatography on methylated bovine serum albumin. Dynamic viscoelastic properties of the fragmented products, in aqueous glycerol solutions in the concentration range of c = 0.003–0.01 g./ml., were investigated with the apparatus of Birnboim and Ferry. At values of the product cM higher than 4 × 10³, the frequency dependence of the components of the complex shear modulus, G′ and G″, displayed a plateau region in which G′ > G″ – ων₁η_S, similar to that observed in concentrated solutions of coiling polymers where it is attributed to an entanglement network (ω is radian frequency, ν₁ volume fraction of solvent, and η₈, solvent viscosity). The width of this plateau region on the logarithmic frequency scale is given by Δ = 3.8 (log cM – 3.56). At lower values of cM, the frequency dependence is intermediate between those predicted by the theory of Zimm for flexible coiled macromolecules and by the theory of Kirkwood and Auer for rods. Fitting to the Zimm theory gives highly discrepant values for molecular weights, while fitting the low-frequency end of the dispersion to the Kirkwood-Auer theory gives reasonable agreement for both molecular weight and rotary diffusion coefficient. It is concluded that the helical fragments appear as nearly rigid rods in their behavior at very low frequencies, but at higher frequencies reveal substantial bending flexibility.     

Light scattering and viscosity study of heat aggregation of insulin

Aggregation behavior and hydrodynamic parameters of insulin have been determined from static and dynamic light scattering experiments and intrinsic viscosity measurements carried out at pH 4.0, 7.5, and 9.0 in the temperature range 20–40°C in aqueous solutions. The protein aggregated extensively at elevated temperatures in the acidic solutions. Intermolecular interactions were found to be attractive and to increase with temperature. The measured intrinsic viscosity [η], diffusion coefficient D₀, molecular weight M, and radius of gyration R_g exhibited the universal behavior: M[η] = (2.4 ± 02) × 10⁻²⁷ (R_e,η/R_e,D)³(D_0η/T)⁻³ and (D₀√n)₋₁ ≃ (√6 πη₀ζβ/k_BT) [1 + 0.201)(v/β³)√n], where n is the number of segments in the polypeptide. The effective hydrodynamic radii deduced from [η], (R_e, η) and the same deduced from D₀, (R_e,D) showed a constant ratio, (R_e,η/R_e,D = 1.1 ± 0.1). R_e,D/R_g = ξ was found to be (0.76 ± 0.07). From the known solvent viscosity η₀, the segment length β was deduced to be (10 ± 1) Å. The excluded volume was deduced to be (5 Å)³ regardless of pH. The Flory-Huggins interaction parameter was found to be χ = 0.45 ± 0.04, independent of pH and temperature. © 1998 John Wiley & Sons, Inc. Biopoly 45: 1–8, 1998     

Measurement of plasma uracil using gas chromatography–mass spectrometry in normal individuals and in patients receiving inhibitors of dihydropyrimidine dehydrogenase

A sensitive gas chromatographic–mass spectrometric method is described for reliably measuring endogenous uracil in 100 μl of human plasma. Validation of this assay over a wide concentration range, 0.025 μM to 250 μM (0.0028 μg/ml to 28 μg/ml), allowed for the determination of plasma uracil in patients treated with agents such as eniluracil, an inhibitor of the pyrimidine catabolic enzyme, dihydropyrimidine dehydrogenase. Calibration standards were prepared in human plasma using the stable isotope, [¹⁵N₂]uracil, to avoid interference from endogenous uracil and 10 μM 5-chlorouracil was added as the internal standard.     

Characterization and Regulatory Properties of Glucose-6-Phosphate Dehydrogenase from Black Gram (Phaseolus mungo)

Glucose-6-phosphate dehydrogenase (E.C. 1.1.1.49) was partially purified by fractionation with ammonium sulfate and phosphocellulose chromatography. The K_m value for glucose-6-phosphate is 1.6 × 10^?4 and 6.3 × 10^?4M at low (1.0–6.0 × 10^?4M) and high (6.0–30.0 × 10^?4M) concentrations of the substrate, respectively. The K_m value for NADP⁺ is 1.4 × 10^?5M. The enzyme is inhibited by NADPH, 5-phosphoribosyl-1-pyrophosphate, and ATP, and it is activated by Mg²⁺, and Mn²⁺. In the presence of NADPH, the plot of activity vs. NADP⁺ concentration gave a sigmoidal curve. Inhibition of 5-phosphoribosyl-1-pyrophosphate and ATP is reversed by Mg²⁺ or a high pH. It is suggested that black gram glucose-6-phosphate dehydrogenase is a regulatory enzyme of the pentose phosphate pathway.     

Ammonia assimilation and glutamate incorporation in coenzyme F420 derivatives ofMethanosarcina barkeri

Methanosarcina barkeri was able to grow on L-alanine and L-glutamate as sole nitrogen sources. Cell yields were 0.5 g/l and 0.7 g/l (wet wt), respectively. The mechanism of ammonia assimilation inMethanosarcina barkeri strain MS was studied by analysis of enzyme activities. Activity levels of nitrogen-assimilating enzymes in extracts of cells grown on different nitrogen sources (ammonia, 0.05–100 mM; L-alanine, 10 mM; L-glutamate, 10 mM) were compared. Activities of glutamate dehydrogenase, glutamate synthase, glutamine synthetase, glutamate oxaloacetate transaminase and glutamate pyruvate transaminase could be measured in cells grown on these three nitrogen sources. Alanine dehydrogenase was not detected under the growth conditions used. None of the measured enzyme activities varied significantly in response to the NH₄ ⁺ concentration. The length of the poly--glutamyl side chain of F₄₂₀ derivatives turned out to be independent of the concentration of ammonia in the culture medium.Abbreviations ADH alanine dehydrogenase - FO 7,8-didemethyl-8-hydroxy-5-deazariboflavin - GDH glutamate dehydrogenase - GOGAT glutamate synthase - GOT glutamate oxaloacetate transaminase - GPT glutamate pyruvate transaminase - GS glutamine synthetase - H₄MPT tetrahydromethanopterin     

Solution properties and chain flexibility of pullulan in aqueous solution

Molecular characteristics for pullulan, a polysaccharide produced by a fungus Aureobasidium pullulans, were measured by light scattering, viscometry, and gel-permeation chromatography. From the experimental data the Mark-Houwink-Sakurada viscosity equation in water at 25°C was determined for samples having the molecular weight M ranging from 48 × 10³ to 2.18 × 10⁶ g mol^?1 as [η] = (1.91 ± 0.02) × 10^?2M_w^0.67±0.01 (in cm³ g^?1); and as molecular weight decreased, the slope of the viscosity equation decreased, although the molecular weight values below 30 × 10³ g mol^?1 evaluated by gel-permeation chromatography were somewhat unreliable. The unperturbed dimensions 〈R²〉₀^1/2 of pullulan were estimated by determining the expansion factor α_s, from the theoretical combination of theories for the interpenetration function Ψ and those for α_s. The 〈R²〉₀/M value estimated from this procedure in 6.7 × 10^?17 cm² mol g^?1. We concluded that the polysaccharide chain that is linked by the α-1,6-glucosidic linkage behaves like a flexible chain in aqueous solution.     

Immobilization of oxyreductases on inorganic supports based on alumina. Immobilization of lactate dehydrogenase on alumina by adsorption

Lactate dehydrogenase (LDH) was adsorbed on low-(γ, η) and high -(θ, α) temperature forms of alumina. θ-Al₂O₃ exhibited the greatest adsorption ability. The maximum adsorption value was 30 mg LDH/g of a carrier. The conditions for irreversible adsorption have been determined. An adsorption isotherm on θ-Al₂O₃ for pH 6.0 has been obtained; the LDH_ads surface area and the carrier surface portion accessible to the enzyme molecules have been calculated. The reaction kinetic parameter were determined by taking into account the reaction proceeding in the intradiffusional region. The specific catalytic activity (A_spec) of LDH_ads at small surface coverage of θ-Al₂O₃ is five times less than A_spec of the native enzyme and K_M^imm with respect to NADH exceeds K_M^nat by two orders or magnitude. The is evidence for a strong LDH–Al₂O₃ interaction and a considerable deformation of the enzyme globule. A_spec and K_M decrease as the amount of the enzyme attached to the carrier increases. Due to adsorption. LDH becomes thermostable and durable. The LDH_ads samples conserve 20–40% of their activity at room temperature during a year.     

Assimilation of ammonia inParacoccus denitrificans

Two pathways serve for assimilation of ammonia inParacoccus denitrificans. Glutamate dehydrogenase (NADP⁺) catalyzes the assimilation at a high NH₄ ⁺ concentration. If nitrate serves as the nitrogen source, glutamate is synthesized by glutamate-ammonia ligase and glutamate synthase (NADPH). At a very low NH₄ ⁺ concentration, all three enzymes are synthesized simultaneously. No direct relationship exists between glutamate dehydrogenase (NADP⁺) and glutamate-ammonia ligase inP. denitrificans, while the glutamate synthase (NADPH) activity changes in parallel with that of the latter enzyme. Ammonia does not influence the induction or repression of glutamate dehydrogenase (NADP⁺). The inner concentration of metabolites indicates a possible repression of glutamate dehydrogenase (NADP⁺) by the high concentration of glutamine or its metabolic products as in the case when NH₄ ⁺ is formed by assimilative nitrate reduction. No direct effect of the intermediates of nitrate assimilation on the synthesis of glutamate dehydrogenase (NADP⁺) was observed.     

A circular channel crucible oscillating viscometer: Detection of DNA damage induced in vivo by exceedingly small doses of dimethylnitrosamine

A new oscillating crucible viscometer, having a U-shaped circular channel, is described. The damping coefficient δ is lowered by an increase of the viscosity η. The instrument described here allows the solution to come in contact with inert plastic only. At all steps of its preparation and during viscosity measurements, giant DNA from rat liver nuclei was maintained at shear stresses around 10^?4 dynes cm^?2. Viscosity was studied as a function of surface tension, DNA concentration and shear stress. It was found that under our experimental conditions it was possible to obtain meaningful values for reduced viscosity, η_red, practically identical to intrinsic viscosity [η]. Rat liver nuclei are incubated in an alkaline lysing solution (pH 12.5; 22 °C): they are lysed immediately and the released DNA starts to uncoil. The viscosity of solutions of this giant DNA increases very slowly with time, reaching a maximum only after about ten hours. The process was accelerated by single-stranded breaks arising from methylation of DNA in vivo with dimethylnitrosamine. It was found that the time of DNA disentanglement was sensitive to an exceedingly small number of breaks. We think that we were able to measure molecular weights around the length of the single strand of an average chromosome (M_n 5 × 10¹⁰). An empirical relation between molecular weight and reduced viscosity after complete disentanglement was also established, as a linear log-log plot, covering a molecular weight range between 10⁸ and 2.5 × 10¹⁰. It is suggested that the viscosimetric evaluation of DNA disentanglement is probably the most sensitive method for studying DNA damage induced “in vivo” by chemical carcinogens.     

Transient electric birefringence of T-even bacteriophages. II. T4B in the presence of tryptophan and T4D.

Measurements of electric birefringence, sedimentation velocity, and biological adsorption rate are used to study the properties of bacteriophage T4B in the presence of excess tryptophan. The adsorption rate determined in borate buffer pH 9 (at 25°C) increases from 0.003 × 10^?8 ml min^?1 (0.025 M) to 0.130 × 10^?8 ml min^?1 (0.150 M). The Kerr coefficient, rotational diffusion coefficient, and the sedimentation coefficient of the phage are also dependent on buffer concentration and reach plateau values above 0.12 M given by K_sp = ?(275 ± 18) × 10^?9 OD^?1 cm² statvolt^?2, D_25,w = 133 ± 4 sec^?1, and s_20,w = 818 ± 11 S. From a comparison of electric birefringence measurements of T4B and T4D it is concluded that T4D and T4B (in the presence of excess tryptophan) exhibit a similar hydrodynamic behavior. The change in physical parameters is solely due to a shift in fiber configuration. At high buffer concentrations the fibers make an angle of approximately 3π/4 with the sheath and the permanent dipole moment is about 200,000 D. This dipole moment is roughly ten times as large as that of a phage particle with nonextended fibers. This difference may be due to a change in hydrodynamic center upon fiber extension or to the presence of positive charges on the fiber tips, or both. At intermediate buffer concentrations the phage population behaves as if it were monodisperse. Probably not all six fibers are extended under such conditions.