Substrate-specific inhibition of RecQ helicase

The RecQ helicases constitute a small but highly conserved helicase family. Proteins in this family are of particular interest because they are critical to maintenance of genomic stability in prokaryotes and eukaryotes. Eukaryotic RecQ helicase family members have been shown to unwind not only DNA duplexes but also DNAs with alternative structures, including structures stabilized by G quartets (G4 DNAs). We report that Escherichia coli RecQ can also unwind G4 DNAs, and that unwinding requires ATP and divalent cation. RecQ helicase is comparably active on duplex and G4 DNA substrates, as measured by direct comparison of protein activity and by competition assays. The porphyrin derivative, N-methyl mesoporphyrin IX (NMM), is a highly specific inhibitor of RecQ unwinding activity on G4 DNA but not duplex DNA: the inhibition constant (K_i) for NMM inhibition of G4 DNA unwinding is 1.7 µM, approximately two orders of magnitude below the K_i for inhibition of duplex DNA unwinding (>100 µM). NMM may therefore prove to be a valuable compound for substrate-specific inhibition of other RecQ family helicases in vitro and in vivo.     

Helix-coil dynamics of a Z-helix hairpin

The helix–coil transition of a Z-helix hairpin formed from d(C-G)₅T₄(C-G)₅ has been characterized by equilibrium melting and temperature jump experiments in 5M NaClO₄ and 10 mM Na₂HPO₄, pH 7.0. The melting curve can be represented by a simple all-or-none transition with a midpoint at 81.6 ± 0.4°C and an enthalpy change of 287 ± 15 kJ/mole. The temperature jump relaxation can be described by single exponentials at a reasonable accuracy. Amplitudes measured as a function of temperature provide equilibrium parameters consistent with those derived from equilibrium melting curves. The rate constants of Z-helix formation are found in the range from 1800 s^?1 at 70°C to 800 s^?1 at 90°C and are associated with an activation enthalpy of ?(50 ± 10) kJ/mole, whereas the rate constants of helix dissociation are found in the range from 200 s^?1 at 70°C to 4500 s^?1 at 90°C with an activation enthalpy +235 kJ/mole. These parameters are consistent with a requirement of 3–4 base pairs for helix nucleation. Apparently nucleation occurs in the Z-helix conformation, because a separate slow step corresponding to a B to Z transition has not been observed. In summary, the dynamics of the Z-helix–coil transition is very similar to that of previously investigated right-handed double helices.     

Theory of friction-limited DNA unwinding

The theory of friction-limited DNA unwinding is developed explicitly for moderate tind large perturbations. This extension of the earlier theory of the relaxation kinetics is necessary because of the complex nature of the rate limitation for small perturbations. The assumption of the theory that is violated under relaxation conditions is that base pairing reactions occurring at a constant local degree of twist of the strands are fast compared to the net unwinding of the molecule. However, these reactions that are slow for small perturbations have a large activation energy, and become faster than friction-limited un winding for large enough temperature jumps and sufficiently large DXA molecules. Thus only the rate for moderate and large perturbations is clearly limited by frictional resistance to turning the molecule in solution. The model used is a diffusional unwinding of the two strands, driven by the accompanying decrease in free energy. For large perturbations a numerical solution of the diffusion equation is required, since the diffusion coefficient is not constant. Two new parameters must be introduced into the equilibrium statistical theory to describe friction-limited unwinding kinetics. These are the force constant b, for winding up coil regions and the frictional coefficient per base pair β_cfor rotating coil regions in solution. We find by fitting the theory to experiment that b = 1.8 × 10^?13 ergs/ rad²- and β_c = 3.5 × 10^?21 erg see/base pair, both for DNA melted in alkali at 0.4.M Na ⁺ and ～30 °C. The latter value is in agreement with predictions based on the viscosity of single stranded DNA in alkali. The quoted value of bcan be interpreted to mean that the number of conformational states of a nucleolide is reduced by an average factor of 1.55 when it is wound around another strand to the degree of twist in a double helix, but without forming a base pair.     

Equilibrium and kinetics of thermal unfolding of yeast 5.8S ribosomal RNA in aqueous salt solutions

Equilibrium and kinetics of thermal melting of yeast 5.8S ribosomal RNA in aqueous NaCl were investigated by differential thermal melting and temperature jump methods. Two peaks were observed in each of the melting curves at 1 mM-1 M Na⁺ and linearity between each melting temperature T_m and log[Na⁺] was found at [Na⁺> 10 mM. From the difference spectrum ratio, $\text{d}\text{A}{}_{280}\text{d}\text{A}{}_{260}$, the G-C content in the local structures was calculated to be 91 and 56%. The temperature jump to 70–85°C in aqueous 30 mM Na⁺ of the RNA solution induced first-order kinetics, from which the kinetically determined melting curve was calculated. The curve could be approximately described in a Gaussian form with a T_m which agrees well with the high T_m in the static melting curve at 30 mM Na⁺. The kinetic properties of the reaction indicated a double helix-coil transition. However, the temperature jump to 20–60°C did not induce monophasic kinetics. The kinetic amplitude of the slow component showed a T_m which corresponded to the low T_m in the static melting curve at 30 mM Na⁺. The slow relaxation had the characteristics of a double helix-to-coil transition. However, contributions from very fast processes including single strand unstacking, were most noticeable in the low temperature melting region of the static curve. The thermodynamic parameters of both transitions from double helix to coil were analysed in detail. Both activation energies for helix formation were negative, and the nucleation is thought to follow a process similar to that in oligonucleotides. Values of T_m and enthalpy change of both helix-coil transitions indicated the cloverleaf model as the most plausible one for some limited regions of yeast 5.8S RNA among the previously proposed models: burp gun, cloverleaf and Rubin's models.     

Dynamic studies of the unwinding of a DNA-like strand

Following Simon and Zimm's recent work, both molecular dynamic and Monte Carlo methods are used to simulate on a computer the unwinding of a DNA-like (N + 1)-unit helical strand. The strand unwinding is assumed to obey (N + 1)-coupled Langevin equations of motion (N = 10–50). The present computer “experiment” was done to elaborate dependence of unwinding behavior of the helix upon (i) configurations of its complementary strand [represented here by a square cylinder (Simon-Zimm model), a circular cylinder, and a fixed helix (double-helical model)]; (ii) interstrand potentials (a hard-cylinder potential, an inverse twelfth-power soft repulsion with or without an inverse third-power attractive tail); (iii) amplitudes of the Brownian motions, and (iv) the molecular weights of the unwinding strand. We found that (i) the Brownian motions strongly couple with the interstrand potentials to produce a shorter “unwinding time” (τ₀) (which characterizes an expotential decay of the unwinding) for a longer renged repulsive potential (without the Brownian motions, no such effect was present); (ii) addition of an attractive tail to the repulsive potentials further reinforces the unwinding, thereby giving a reduced value of τ₀; (iii) τ₀ can be expressed as a product of two factors–unwinding time for a one-dimensional spring-bead model, which mostly accounts for the N ²-dependence in τ₀, and a factor which depends on the Brownian motions and the interstrand potentials; (iv) among the three models described above, under similar situations, the three-dimensional double-helical model has the smallest τ₀; and (v) unless the maximum Brownian displacement exceeds a certain value, the unwinding around a square cylinder takes place in a (unrealistic) stair-step manner whose τ₀ decreases with increase in the Brownian displacements. The N ²-dependence of τ₀ agrees with the Simon and Zimm's machine results as well as Crother's experimental data on T2 DNA; however, it contradicts experimental data of Massie and Zimm, and others. Further possible improvements in connection with the computer simulation are suggested.     

Hydrodynamic properties of a rigid molecule: Rotational and linear diffusion and fluorescence anisotropy

The fluorescence anisotropy of a general rigid body is formally the sum of five exponentials. We show that, to a high degree of approximation, there are relationships between the five time constants. As we define the time constants here, τ₁ ? τ₅, τ₂ ? τ₃, and τ₁^?1 + 3τ₄^?1 ? 4τ₂^?1. In practical cases, at most only three exponentials will be observed, and, of these, only two are independent. Using a numerical integration procedure, Perrin's equations for the rotational and translational diffusion of a general ellipsoid are solved. Rotational friction coefficients, frictional ratio, rotational relaxation times, and the five exponential terms in the fluorescence anisotropy are tabulated as functions of the axial ratios of the ellipsoid. In principle, the three axes of a general ellipsoid may be determined by a simultaneous measurement of the anisotropy and the linear diffusion constant. We examine, and illustrate, the effect of experimental error on such a determination.     

Syn–anti equilibrium of purine bases in dinucleoside monophosphates as studied by proton longitudinal relaxation

The preferential orientations of the purine bases in dinucleoside monophosphates such as ApA, ApG, and GpA in 10^?2M neutral aqueous solutions have been investigated by proton relaxation at 250 MHz. These orientations are deduced from computer simulations of the magnetization recovery curves following a 180° nonselective pulse. The distances between the H(8) proton of a base and the ribose ring protons which are used in these calculations are obtained by minimization as a function of the glycosyl torsion angle ? of the standard deviation between the isotropic reorientation correlation times τ_R derived from the relaxation rates of these protons. The average H(1′) – H(8) distance obtained by this procedure may be readily verified from the reduction of the H(1′) relaxation rate when H(8) is substituted by a deuteron. The limits of validity of the assumption of a single correlation time τ_R governing the proton relaxation have been estimated, taking into account several possible internal motions, e.g., the rotation of the base, of the methylene exocyclic group and the N ? S interconversion of the ribose ring. For 10^?10 < τ_R < 2 × 10^?10 sec, it appears that the influence of these motions on the proton relaxation becomes perceptible when the jump rates among equilibrium positions exceed ca. 10⁹ sec^?1. The whole of the experimental results show that for the ribose ring N conformer, the orientation of the bases is found in the ranges 60° < ? < 80° (syn) and 180° < ? < 210° (anti). For ribose S conformer, it is observed that this orientation is mainly syn with 5° < ? < 90°. The average H(1′) – H(8) distance provides semiquantitative information on the overall syn or anti orientations of the base in each nucleoside moiety. At 298 K the population of the anti conformer is found to increase in the order A- pG < Ap -G ～ Gp -A < Ap -A < A-pA < G-pA . A more detailed analysis of relaxation data shows that the maximum possible fraction of the stacked form of dinucleotides, due to the occurrence of N-anti conformers in both nucleoside moieties, is in the order ApG < GpA < ApA, in agreement with previous works, with however smaller values. Lastly the deuteron linewidth in position 8 of the bases indicates a syn–anti transition rate of the order of 10⁹ sec^?1 at room temperature, without noticeable effects therefore on the proton relaxation.     

Mg2+-dependent unwinding of DNA by nonhistone chromosomal protein HMG(1 + 2) from pig thymus as determined by DNA melting temperature analysis

In the previous studies with endonucleases specific for single-stranded DNA, we have indicated that the nonhistone chromosomal protein HMG(1 + 2) prepared from pig thymus has an activity to unwind DNA partially at low protein-to-DNA weight ratios (Yoshida, M. & Shimura, K. (1984) J. Biochem. 95, 117-124). In the present work, we have pursued the unwinding reaction by HMG(1 + 2) by thermal melting temperature analysis of DNA, and by investigating the effect of Mg2+ on the reaction. The melting temperature of DNA in the presence of HMG(1 + 2) at low protein weight ratios decreased in 2 mM Tris-HCl, pH 7.8, whereas it increased at higher ratios. The depressions of melting temperature by HMG(1 + 2) at low ratios were not observed either in the system of 2 mM Tris-HCl, pH 7.8, containing EDTA or in the system containing samples treated in advance with EDTA. An addition of Mg2+ to the system reproduced the depression of melting temperature at low protein-to-DNA ratios as well as the increase at higher ratios. Analysis by Mg2+-equilibrated gel filtration revealed that HMG(1 + 2) is a Mg2+-binding protein. However, the depression of melting temperature at low protein-to-DNA ratios was not due to removal of Mg2+ from DNA by HMG(1 + 2). From these results, it is concluded that HMG(1 + 2) causes a partial DNA unwinding detectable by thermal melting temperature analysis of DNA, and that Mg2+ is necessary for the unwinding reaction.     

Quasielastic light scattering: Effect of ionic strength on the internal dynamics of DNA

Quasielastic light scattering is used to study the effect of ionic strength on the dynamic behaviour of DNA. In a first approach the spectrum of scattered light is analyzed in terms of a single relaxation process. The large difference between the observed behaviour and that expected according to a pure diffusional process reflects the contribution associated with internal modes, which increases with decreasing ionic strength. Such behaviour is better analyzed in terms of a double relaxation process by using two relaxation times, the reciprocals of which are equal to DK² and DK² + τ_i^?1 (K), respectively, where τ_i (K) is an average value describing the set of modes observed at a given K value. Relative intensity and relaxation times, which are the more accurate parameters, were used to interpret the results. The observed increase of the relative contribution of internal modes with decreasing ionic strength is actually a relative decrease of the diffusional contribution induced by a corresponding increase of the radius of gyration R_G. On the other hand, the reciprocal τ_i^?1 (K) of the relaxation time is a linear function of K² in the analyzed KR_G range and is insensitive to ionic strength between 10^?2M and 1M. These results, when discussed according to Rouse's model, lead to define for each value of τ_i^?1 (K) a corresponding mean-squared equilibrium length 〈μ〉 which is found to be a linear function of K^?2.     

Dda helicase tightly couples translocation on single-stranded DNA to unwinding of duplex DNA: Dda is an optimally active helicase

Helicases utilize the energy of ATP hydrolysis to unwind double-stranded DNA while translocating on the DNA. Mechanisms for melting the duplex have been characterized as active or passive, depending on whether the enzyme actively separates the base pairs or simply sequesters single-stranded DNA (ssDNA) that forms due to thermal fraying. Here, we show that Dda translocates unidirectionally on ssDNA at the same rate at which it unwinds double-stranded DNA in both ensemble and single-molecule experiments. Further, the unwinding rate is largely insensitive to the duplex stability and to the applied force. Thus, Dda transduces all of its translocase activity into DNA unwinding activity so that the rate of unwinding is limited by the rate of translocation and that the enzyme actively separates the duplex. Active and passive helicases have been characterized by dividing the velocity of DNA unwinding in base pairs per second (V_un) by the velocity of translocation on ssDNA in nucleotides per second (V_trans). If the resulting fraction is 0.25, then a helicase is considered to be at the lower end of the “active” range. In the case of Dda, the average DNA unwinding velocity was 257 ± 42 bp/s, and the average translocation velocity was 267 ± 15 nt/s. The V_un/V_trans value of 0.96 places Dda in a unique category of being an essentially “perfectly” active helicase.     

The influence of single-strand breaks on the kinetics of denaturation of DNA

The influence of single-strand breaks on the kinetics of the relaxation of DNA in a solution of low ionic strength has been investigated by a temperature jump method. The relaxation of DNA after a jump of 0.7 °C in the melting region has been monitored by measuring the extinction at 260 nm. For essentially monodisperse T4 DNA (M = 130 × 10⁶) two distinct relaxation times have been observed, that depend markedly on the initial extent of denaturation 1 ? θ. The larger relaxation time decreases from 450 sec to about 300 sec, the smaller one from 55 see to 30 when 1 ? θ increases from 0.03 to about 0.8. The dependence of these relaxation times on the average number of single-strand breaks per molecule (p) appears to be very small up to p = 100. However, the relative contribution of the slow process decreases sharply when p increases from 0.6 to 30 and remains nearly constant for larger p. The observations are discussed in the light recent theories of the kinetics of denaturation.     

Kinetics of conformational changes in tRNAPhe (yeast) as studied by the fluorescence of the y-base and of formycin substituted for the 3'-terminal adenine

The kinetics of the melting transitions of tRNA^phe (yeast) were followed by the fluorescence of the Y-base and of formycin substituted for the 3'-terminal adenine. As judged from differential UV absorbance melting cutves the formycin label had virtually no influence on the conformation of the tRNA. A temperature jump apparatus was modified to allow the simultaneous observation of transmission and fluorescence intensities by two independent optical channels. The design of a temperature jump cell with an all quartz center piece is given. The cell is resistant to temperatures up to 90°C; it provides high optical sensitivity, low stray light intensity and the possibility of measuring fluorescence polarization. The T-jump experiments allowed to discriminate between fast unspecific fluorescence quenching (τ <5 μsec) and slow co-operative conformational changes. In the central part of the temperature range of UV-melung (midpoint temperature 30°C in 0.01 M Na⁺ and 39°C in 0.03 M Na⁺, pH 6.8) two resolvable relaxation processes were observed. The coirssponding relaxation times were 20 msec and 800 msec at 30°C in 0.01 M Na⁺, and 4 msec and 120 msec at 39°C in 0.03 M Na⁺. The Y-base fluorescence shows both of the relaxation effects, which almost cancel in equilibrium fluorescence melting, because their amplitudes have opposite signs. From this finding the existence of some residual tertiary structure is inferred which persists after the unfolding of the main part of tertiary structure durirg early melting (midpoint temperature 24°C in 0.03 M Na⁺). In the fluorescence sigXXX of the formycin also the two relaxation effects appear. Both of them are connected with a decrease of the fluorescence intensity. From the results a coupled opening of the anticodon and acceptor branches is concluded.Enzymes: phenylalanyl-tRNA synthetase, PRS (EC 6.1.1.-20); ATP (CTP) tRNA nucleotidyl transferase, NT (EC 2.7.7.-20); alkaline phosphatase (EC 3-1-3.1).     

Detecting base pair substitutions in DNA fragments by temperature-gradient gel electrophoresis.

A vertical gel electrophoresis apparatus is described which can distinguish DNA fragments differing by single base pair substitutions. The system employs a homogenous polyacrylamide gel containing urea-formamide and a temperature gradient which runs either perpendicular or parallel to the direction of electrophoresis. The temperature-gradient system simplifies several features of the denaturant-gradient system (1) and is relatively inexpensive to construct. Eight homologous 373 bp DNAs differing by one, two, or nine base pair substitutions were examined. DNA electrophoretic mobility changed abruptly with the temperature induced unwinding of DNA domains. GC to AT substitutions at different locations within the first melting domain, as well as an AT to TA transversion were separated with temperature gradients parallel to the electrophoretic direction. The relative stabilities of the DNAs observed in the gels were compared to predictions of DNA melting theory. General agreement was observed however complete correspondence was not obtained.     

Frequency dependence of the proton magnetic relaxation in aqueous solutions iof haemoproteins

The longitudinal proton magnetic relaxation times T₁ were measured for ferri (met)-and carbonmonoxy-bovine haemoglobin and equine myoglobin in 0.1 M KH₂PO₄ aqueous solutions near pH 6 at 5°C and 35°C from 1.5- to 60-MHz Larmor frequencies. It is concluded that the correlation time τ_C for the dipole–dipole interaction of electron and nuclear spins is in fact the electron (ferric) spin relaxation time τ_S being close to 1.5 × 10^?10 sec for both metHb and metMb at 5°C. At 35°C the paramagnetic relaxation rates are not determined solely by the relaxation of protons exchanging from the haem pocket with bulk solvent. Hence, τC at 35°C cannot be calculated from the dispersion data obtained at this temperature. The relevance of this for the determination of interspin distances r is discussed.     

Hysteresis and partial irreversibility of denaturation of DNA as a means of investigating the topology of base distribution constraints: application to a yeast rho- (petite) mitochondrial DNA

Low salt concentrations prevent reassociation of separated single strands of DNA, but not the renaturation of partially melted molecules. Rewinding, however, may be delayed (hysteresis) and/or incomplete (partial irreversibility). Long-range fluctuations in base compositioncould account for these observations: (a) the “zippering-up” of a denatured (G + C)-rich section may have to await that of one of its neighbouring (A + T)-rich sections, hence a temperature lag in rewinding; (b) the removal of intramolecular heterogeneities in base composition by fragmentation will give rise to a dispersal of strand-separation temperatures. Conversely, it is shown how a considerable amount of information about the topology of base distribution constraints could be derived from these phenomena.Some yeast ρ^? (petite) mitochondrial DNAs, the melting of which is quasidiscontinuous, provide an excellent opportunity for testing the applicability of this new approach to denaturation mapping. Alternating partial denaturation and renaturation with a low rate of temperature change were followed by high-frequency recording of absorbance at 260 nm. A typical experiment (counterion concentration 0.015 m-Na⁺) carried out on a low-complexity (length of repetitive unit about 3000 base-pairs) ρ^? DNA is reported in full detail. Analysis of the data disclosed the existence of two relatively (G + C)-rich clusters separated by long homogeneous stretches of high (A + T) content.The rewinding of ρ^? DNAs is a discontinuous process. Both equilibrium and non-equilibrium melting processes were observed. Hysteresis in rewinding, which is restricted to the melting range, increases discontinuously with the extent of unwinding reached prior to cooling. Results are shown to be fully consistent with a model that presupposes that nucleation does not play any part in the renaturation process. They are briefly discussed further in the light of current concepts in the theory of helix-coil transitions of DNA.     

31P nmr spin-lattice relaxation studies of deoxyoligonucleotides

Temperature-dependent conformational transitions of deoxyoligonucleotides have been monitored by measuring ³¹P chemical shifts, spin-lattice relaxation times (T₁), and ³¹P-{H} nuclear Overhauser enhancements (NOEs). The measured NOE ranged from 30 to 80%, compared to the theoretical maximum of 124% for a dipolar relaxation mediated by rapid isotropic rotation. The observed 3′-5′ phosphate diester ³¹P T₁ showed a similar temperature dependence over the range 2–75°C for both double- and single-stranded oligonucleotides, and for dinucleotides. The results show that dipole–dipole interactions dominate the internucleotide phosphate relaxation rate in oligonucleotides. The same is true of terminal phosphate groups at low temperature; but at higher temperature another process, possibly due to contamination by paramagnetic ions, becomes dominant. The rotational correlation time τ_R calculated from the dipole–dipole relaxation rate of the internucleotide phosphate in d(pA)₂ at 16°C is τ_R = 5.0 × 10^?10 sec, implying a Stokes radius for isotropic rotation of 7.6 Å. The T₁ and NOE values for the double-helical octanucleotide d(pA)₃pGpC(pT)₃ are consistent with dominance of dipole–dipole relaxation and isotropic rotation of a sphere of radius 14 Å, a reasonable dimension for the double helix. Activation energies for the rotation of dinucleotides range from 4 to 6 kcal/mol, close to the value of 4 kcal/mol expected for isotropic rotation. In order to test the possible effect of internal motion of correlation time τ_G on the results, we considered a model in which the nucleotide chain rotates about the P-O bonds. Comparison of the calculation with our experimental results shows that internal motion with τ_G ? 10^?9 sec, as found from other studies to be present for large nucleic acids, would not influence out T₁ and NOE values enough to be distinguished from isotropic rotation. However, we can conclude that τ_G cannot be as fast as 10^?10 sec, even for dinucleotides.     

Model of ribosome translation and mRNA unwinding

A ribosome is an enzyme that catalyzes translation of the genetic information encoded in messenger RNA (mRNA) into proteins. Besides translation through the single-stranded mRNA, the ribosome is also able to translate through the duplex region of mRNA via unwinding the duplex. Here, based on our proposed ribosome translation model, we study analytically the dynamics of Escherichia coli ribosome translation through the duplex region of mRNA, and compare with the available single molecule experimental data. It is shown that the ribosome uses only one active mechanism (mechanical unwinding), rather than two active mechanisms (open-state stabilization and mechanical unwinding), as proposed before, to unwind the duplex. The reduced rate of translation through the duplex region is due to the occurrence of futile transitions, which are induced by the energy barrier from the duplex unwinding to the forward translocation along the single-stranded mRNA. Moreover, we also present predicted results of the average translation rate versus the external force acting on the ribosome translating through the duplex region and through the single-stranded region of mRNA, which can be easily tested by future experiments.     

The DinG protein from Escherichia coli is a structure-specific helicase

The Escherichia coli DinG protein is a DNA damage-inducible member of the helicase superfamily 2. Using a panel of synthetic substrates, we have systematically investigated structural requirements for DNA unwinding by DinG. We have found that the helicase does not unwind blunt-ended DNAs or substrates with 3'-ss tails. On the other hand, the 5'-ss tails of 11-15 nucleotides are sufficient to initiate DNA duplex unwinding; bifurcated substrates further facilitate helicase activity. DinG is active on 5'-flap structures; however, it is unable to unwind 3'-flaps. Similarly to the homologous Saccharomyces cerevisiae Rad3 helicase, DinG unwinds DNA.RNA duplexes. DinG is active on synthetic D-loops and R-loops. The ability of the enzyme to unwind D-loops formed on superhelical plasmid DNA by the E. coli recombinase RecA suggests that D-loops may be natural substrates for DinG. Although the availability of 5'-ssDNA tails is a strict requirement for duplex unwinding by DinG, the unwinding of D-loops can be initiated on substrates without any ss tails. Since DinG is DNA damage-inducible and is active on D-loops and forked structures, which mimic intermediates of homologous recombination and replication, we conclude that this helicase may be involved in recombinational DNA repair and the resumption of replication after DNA damage.     

Embryonic development of the European smelt Osmerus eperlanus eperlanus (L.) (Neva population)

The embryonic development of the European smelt Osmerus eperlanus eperlanus has been described. The whole period of the development has been subdivided into 6 subperiods. More than 80 stages may be described for all of these periods. The development of the European smelt embryo was studied in the 5 different regimes of a constant temperature in the range 9.5–18.3°C. The duration of different stages under different temperature regimes was expressed in the relative units of τ₀ (the time of a single cleavage) and τ_s (the time of formation of a single pair of somites). It was established that the τ_s value had proportionally changed by embryogenesis. Due to this fact, the duration of the stages was expressed only as τ_s. The dependency of the speed of the European smelt embryogenesis on temperature has been shown. This dependence was expressed using the standard interval τ_s and described using the equation log τ_s(t) = 3.22665?0.13876t + 0.00297t ², where t is the temperature.     

Mechanism of DNA denaturation in the presence of manganese ions

The unwinding of DNA strands in the presence of small concentrations of Mn²⁺ ions (2 × 10^?4?4 × 10^?4M) has been studied. The process of unwinding is nonequilibrium; the DNA strands are gradually unwound at a constant temperature corresponding to the beginning of the melting curve. There is no true renaturation in the partially melted DNA. It is shown in the paper that these effects are due to the aggregation of the unwound DNA regions. The Mn²⁺ ions are responsible for the binding of the unwound strands. The aggregation precludes renaturation, shifts the equilibrium towards the melted state, and causes slow unwinding at a constant temperature. The binding of denaturated regions seems to occur through the guanines.