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I Rouzina

Publications and source records attributed to I Rouzina.

12 recordsLinked to original sources
PubMed2001

Mechanism for nucleic acid chaperone activity of HIV-1 nucleocapsid protein revealed by single molecule stretching.

The nucleocapsid protein (NC) of HIV type 1 is a nucleic acid chaperone that facilitates the rearrangement of nucleic acids into conformations containing the maximum number of complementary base pairs. We use an optical tweezers instrument to stretch single DNA molecules from the helix to coil state at room temperature in the presence of NC and a mutant form (SSHS NC) that lacks the two zinc finger structures present in NC. Although both NC and SSHS NC facilitate annealing of complementary strands through electrostatic attraction, only NC destabilizes the helical form of DNA and reduces the cooperativity of the helix-coil transition. In particular, we find that the helix-coil transition free energy at room temperature is significantly reduced in the presence of NC. Thus, upon NC binding, it is likely that thermodynamic fluctuations cause continuous melting and reannealing of base pairs so that DNA strands are able to rapidly sample configurations to find the lowest energy state. The reduced cooperativity allows these fluctuations to occur in the middle of complex double-stranded structures. The reduced stability and cooperativity, coupled with the electrostatic attraction generated by the high charge density of NC, is responsible for the nucleic acid chaperone activity of this protein.

DNA, Viral↗
PubMed2001

Effect of pH on the overstretching transition of double-stranded DNA: evidence of force-induced DNA melting.

When a single molecule of double-stranded DNA is stretched beyond its B-form contour length, the measured force shows a highly cooperative overstretching transition. We have investigated the source of this transition by altering helix stability with solution pH. As solution pH was increased from pH 6.0 to pH 10.6 in 250 mM NaCl, the overstretching transition force decreased from 67.0 +/- 0.8 pN to 56.2 +/- 0.8 pN, whereas the transition width remained nearly constant. As the pH was lowered from pH 6.0 to pH 3.1, the overstretching force decreased from 67.0 +/- 0.8 pN to 47.0 +/- 1.0 pN, but the transition width increased from 3.0 +/- 0.6 pN to 16.0 +/- 3 pN. These results quantitatively agree with a model that asserts that DNA strand dissociation, or melting, occurs during the overstretching transition.

Biophysical Phenomena↗
PubMed2001

Force-induced melting of the DNA double helix 1. Thermodynamic analysis.

The highly cooperative elongation of a single B-DNA molecule to almost twice its contour length upon application of a stretching force is interpreted as force-induced DNA melting. This interpretation is based on the similarity between experimental and calculated stretching profiles, when the force-dependent free energy of melting is obtained directly from the experimental force versus extension curves of double- and single-stranded DNA. The high cooperativity of the overstretching transition is consistent with a melting interpretation. The ability of nicked DNA to withstand forces greater than that at the transition midpoint is explained as a result of the one-dimensional nature of the melting transition, which leads to alternating zones of melted and unmelted DNA even substantially above the melting midpoint. We discuss the relationship between force-induced melting and the B-to-S transition suggested by other authors. The recently measured effect on T7 DNA polymerase activity of the force applied to a ssDNA template is interpreted in terms of preferential stabilization of dsDNA by weak forces approximately equal to 7 pN.

Biophysical Phenomena↗
PubMed2001

Force-induced melting of the DNA double helix. 2. Effect of solution conditions.

In this paper, we consider the implications of the general theory developed in the accompanying paper, to interpret experiments on DNA overstretching that involve variables such as solution temperature, pH, and ionic strength. We find the DNA helix-coil phase boundary in the force-temperature space. At temperatures significantly below the regular (zero force) DNA melting temperature, the overstretching force, f(ov)(T), is predicted to decrease nearly linearly with temperature. We calculate the slope of this dependence as a function of entropy and heat-capacity changes upon DNA melting. Fitting of the experimental f(ov)(T) dependence allows determination of both of these quantities in very good agreement with their calorimetric values. At temperatures slightly above the regular DNA melting temperature, we predict stabilization of dsDNA by moderate forces, and destabilization by higher forces. Thus the DNA stretching curves, f(b), should exhibit two rather than one overstretching transitions: from single stranded (ss) to double stranded (ds) and then back at the higher force. We also predict that any change in DNA solution conditions that affects its melting temperature should have a similar effect on DNA overstretching force. This result is used to calculate the dependence of DNA overstretching force on solution pH, f(ov)(pH), from the known dependence of DNA melting temperature on pH. The calculated f(ov)(pH) is in excellent agreement with its experimental determination (M. C. Williams, J. R. Wenner, I. Rouzina, and V. A. Bloomfield, Biophys. J., accepted for publication). Finally, we quantitatively explain the measured dependence of DNA overstretching force on solution ionic strength for crosslinked and noncrosslinked DNA. The much stronger salt dependence of f(ov) in noncrosslinked DNA results from its lower linear charge density in the melted state, compared to crosslinked or double-stranded overstretched S-DNA.

Biophysical Phenomena↗
PubMed2001

Entropy and heat capacity of DNA melting from temperature dependence of single molecule stretching.

When a single molecule of double-stranded DNA is stretched beyond its B-form contour length, the measured force shows a highly cooperative overstretching transition. We have measured the force at which this transition occurs as a function of temperature. To do this, single molecules of DNA were captured between two polystyrene beads in an optical tweezers apparatus. As the temperature of the solution surrounding a captured molecule was increased from 11 degrees C to 52 degrees C in 500 mM NaCl, the overstretching transition force decreased from 69 pN to 50 pN. This reduction is attributed to a decrease in the stability of the DNA double helix with increasing temperature. These results quantitatively agree with a model that asserts that DNA melting occurs during the overstretching transition. With this model, the data may be analyzed to obtain the change in the melting entropy DeltaS of DNA with temperature. The observed nonlinear temperature dependence of DeltaS is a result of the positive change in heat capacity of DNA upon melting, which we determine from our stretching measurements to be DeltaC(p) = 60 +/- 10 cal/mol K bp, in agreement with calorimetric measurements.

Calorimetry↗
PubMed2000

Thermodynamics of DNA binding and condensation: isothermal titration calorimetry and electrostatic mechanism.

The thermodynamics of binding of the trivalent cations cobalt hexammine and spermidine to plasmid DNA was studied by isothermal titration calorimetry. Two stages were observed in the course of titration, the first attributed to cation binding and the second to DNA condensation. A standard calorimetric data analysis was extended by applying an electrostatic binding model, which accounted for most of the observed data. Both the binding and condensation reactions were entropically driven (TDeltaS approximately +10 kcal/mol cation) and enthalpically opposed (DeltaH approximately +1 kcal/mol cation). As predicted from their relative sizes, the binding constants of the cations were indistinguishable, but cobalt hexammine had a much greater DNA condensing capacity because it is more compact than spermidine. The dependence of both the free energy of cobalt hexammine binding and the critical cobalt hexammine concentration for DNA condensation on temperature and monovalent cation concentration followed the electrostatic model quite precisely. The heat capacity changes of both stages were positive, perhaps reflecting both the temperature dependence of the dielectric constant of water and the burial of polar surfaces. DNA condensation occurred when about 67 % of the DNA phosphate charge was neutralized by cobalt hexammine and 87 % by spermidine. During condensation, the remaining DNA charge was neutralized.

Binding, Competitive↗
PubMed1999

Heat capacity effects on the melting of DNA. 1. General aspects.

In this paper we analyze published data on DeltaH and DeltaS values for the DNA melting transition under various conditions. We show that there is a significant heat capacity increase DeltaC(p) associated with DNA melting, in the range of 40-100 cal/mol K per base pair. This is larger than the transition entropy per base pair, DeltaS(0) approximately 25 cal/mol K. The ratio of DeltaC(p)/DeltaS(0) determines the importance of heat capacity effects on melting. For DNA this ratio is 2-4, larger than for many proteins. We discuss how DeltaC(p) values can be extracted from experimental data on the dependence of DeltaH and DeltaS on the melting temperature T(m). We consider studies of DNA melting as a function of ionic strength and show that while polyelectrolyte theory provides a good description of the dependence of T(m) on salt, electrostatics alone cannot explain the accompanying strong variation of DeltaH and DeltaS. While T(m) is only weakly affected by DeltaC(p), its dependence on one parameter (e.g., salt) as a function of another (e.g., DNA composition) is determined by DeltaC(p). We show how this accounts for the stronger stabilization of AT relative to GC base pairs with increasing ionic strength. We analyze the source of discrepancies in DeltaH as determined by calorimetry and van't Hoff analysis and discuss ways of analyzing data that yield valid van't Hoff DeltaH. Finally, we define a standard state for DNA melting, the temperature at which thermal contributions to DeltaH and DeltaS vanish, by analyzing experimental data over a broad range of stabilities.

Base Pairing↗
PubMed1999

Heat capacity effects on the melting of DNA. 2. Analysis of nearest-neighbor base pair effects.

The stability of a DNA double helix of any particular sequence is conventionally estimated as the average of the stabilities of the 10 different nearest-neighbor (NN) base pair doublets that it contains. Therefore, much effort has been devoted to the experimental characterization and tabulation of the enthalpy, entropy, and free energy of melting for each of the NN doublets. Although data from different research groups generally agree for the NN free energies and melting temperatures, there are major disagreements for the enthalpies and entropies. The largest differences are between the parameters obtained on oligomeric relative to polymeric DNA. This disagreement interferes with the practical application of NN thermodynamic parameters. It also raises doubts regarding several fundamental assumptions about DNA melting, such as the absence of longer range interactions, the length dependence of DNA melting parameters per base pair, the applicability of polyelectrolyte theory to the description of salt effects on oligomers, and the purely enthalpic difference between NN doublets. Here we show that if one takes into account the significant heat capacity increase associated with DNA melting, all of the above assumptions are self-consistently reconciled with experiment.

Base Pairing↗
PubMed1999

Negative electrostatic contribution to the bending rigidity of charged membranes and polyelectrolytes screened by multivalent counterions.

Bending rigidity of a charged membrane or polyelectrolyte screened by monovalent counterions is known to be enhanced by electrostatic effects. We show that in the case of screening by multivalent counterions the electrostatic effects reduce the bending rigidity. This inversion of the sign of the electrostatic contribution is related to the formation of two-dimensional strongly correlated liquids (SCL) of counterions at the charged surface due to strong lateral repulsion between them. When a membrane or a polyelectrolyte is bent, SCL is compressed on one side and stretched on the other so that thermodynamic properties of SCL contribute to the bending rigidity. Thermodynamic properties of SCL are similar to those of Wigner crystal and are anomalous in the sense that the pressure, compressibility and screening radius of SCL are negative. This brings about substantial negative correction to the bending rigidity. For the case of DNA this effect qualitatively agrees with experiment.

Cations↗
PubMed1998

DNA bending by small, mobile multivalent cations.

We propose a purely electrostatic mechanism by which small, mobile, multivalent cations can induce DNA bending. A multivalent cation binds at the entrance to the B-DNA major groove, between the two phosphate strands, electrostatically repelling sodium counterions from the neighboring phosphates. The unscreened phosphates on both strands are strongly attracted to the groove-bound cation. This leads to groove closure, accompanied by DNA bending toward the cationic ligand. We explicitly treat the dynamic character of the cation-DNA interaction using an adiabatic approximation, noting that DNA bending is much slower than the diffusion of nonspecifically bound, mobile cations. We make semiquantitative estimates of the free energy components of bending-electrostatic (with a sigmoidal distance-dependent dielectric function), elastic, and entropic cation localization-and find that the equilibrium state is bent B-DNA stabilized with a self-localized cation. This is a bending polaron, formation of which should be critically dependent on the strength of electrostatic interaction and the concentration of highly mobile cations available for self-localization. We predict that the resultant bend will be large (approximately 20-40 degrees), smooth (because it is spread over 6 bp), and infrequent. The stability of such a bend can be variable, from transient to highly stable (static) bending, observable with standard curvature-measuring techniques. We further predict that this bending mechanism will have an unusual sequence dependence: sequences with less binding specificity will be more bent, unless the specific binding site is in the major groove.

Base Sequence↗
PubMed1997

Competitive electrostatic binding of charged ligands to polyelectrolytes: practical approach using the non-linear Poisson-Boltzmann equation.

We have developed a practical analytical treatment of the non-linear Poisson-Boltzmann (P-B) equation to characterize the strong but non-specific binding of charged ligands to DNA and other highly charged macromolecules. These reactions are notable for their strong salt dependence and anti-cooperativity, features which the theory fully explains. We summarize analytical results for concentration profiles and ion binding in various regimes of surface curvature and ionic strength, and show how counterion size and charge distribution may influence competitive binding. We present several practical applications of the formalism, showing how to estimate the ligand concentration needed to effectively compete with a given buffer salt, and how to calculate the amounts of counterion species bound at various distances from the DNA surface under given bulk solution conditions. We cast our results into the form of a Scatchard binding isotherm, showing how the apparent binding constant K(obs) and S = -dlog K (obs )d log[M (+)] can be predicted from the basic theory. Anti-cooperativity arises naturally without steric repulsion, and binding curves can be fitted with K(obs) and effective charge as the only free parameters. We extend the analytical P-B analysis to an arbitrary number of counterion species, and apply the results to fit and predict three-ion competition data.

Journal Article↗