1H, 7Li and 133Cs multicomponent self-diffusion NMR study on ion binding of Li+ and Cs+ to nucleotides and aggregation of nucleotides in aqueous solution

The Fourier transform NMR pulsed-gradient spin-echo self-diffusion technique was used for studies of nucleotides (AMP, CMP, GMP and UMP) with Li+ or Cs+ added, in 2H2O. 1H-, 7Li- and 133Cs-NMR-based self-diffusion data on the constituents provide a picture of both the degree of ion binding to nucleotides and the self-association of nucleotides in aqueous solution. Self-diffusion coefficients were investigated in a concentration range up to 0.3 molal nucleotide in 2H2O, while keeping the metal ion concentration of Li+ or Cs+ at twice the nucleotide concentration throughout the investigations. The self-association studies reveal that the aggregation constants of the Li salts differ only slightly from the corresponding constants for the disodium salts of the mononucleotides. Within a two-site bound-free model for the counterions and a cooperative indefinite aggregation model for the nucleotides one finds that the degree of ion binding for all these nucleotide systems remains approximately constant, in spite of increasing aggregate concentration. This corresponds to the well-known polyelectrolyte ion condensation behaviour, indicating that large aggregates are formed, supporting previous findings by the present authors on the aggregation behaviour of nucleotides. An observed large effect on the 17O relaxation of water in nucleotide systems can only be reconciled with the presence of relatively large aggregates in solution.     

Preferential counterion binding to A-tract DNA oligomers

The free solution mobility of four 20 bp DNA oligomers, with and without A-tracts, has been measured by capillary electrophoresis in Tris-acetate buffer, to test the hypothesis that site-specific binding of monovalent counterions can occur in the narrow minor groove of A-tract DNAs. Preferential counterion binding has been proposed to cause A-tract bending because of asymmetric charge neutralization and collapse of the helix backbone toward the minor groove. Preferential counterion binding in A-tract DNAs should be manifested by a decrease in the electrophoretic mobility observed in free solution, compared to that of non-A-tract DNAs of the same size. Of the four sequences studied here, the slowest absolute mobility, indicative of the greatest counterion binding, was observed for a 20 bp oligomer containing two runs of A3T3 in phase with the helix repeat. A 20-mer containing phased CACA sequences migrated with the fastest mobility; 20-mers containing phased A5 tracts or phased runs of T3A3 migrated with intermediate mobilities. Very similar mobility differences were observed when 1-20 mM NaCl was added to the buffer. The results suggest that preferential counterion binding occurs in A-tract DNAs, especially those containing the AnTn sequence motif.     

Gel electrophoresis measurement of counterion condensation on DNA

We used agarose gel electrophoresis to measure the effective charge neutralization of DNA by counterions of different structure and valence, including Na⁺, Mg²⁺, Co(NH₃), and sperinidine³⁺, which competed for binding with an excess of Tris acetate buffer. Linear DNA molecules ranged in size from 1 to 5 kilobases, and supercoiled plasmid pUC18 was also measured. In all cases, the results were in good agreement with theoretical predict ions from counterion condensation theory for two-counterion mixtures. © 1995 John Wiley & Sons, Inc.     

Charge structure and counterion distribution in hexagonal DNA liquid crystal

A hexagonal liquid crystal of DNA fragments (double-stranded, 150 basepairs) with tetramethylammonium (TMA) counterions was investigated with small angle neutron scattering (SANS). We obtained the structure factors pertaining to the DNA and counterion density correlations with contrast matching in the water. Molecular dynamics (MD) computer simulation of a hexagonal assembly of nine DNA molecules showed that the inter-DNA distance fluctuates with a correlation time around 2 ns and a standard deviation of 8.5% of the interaxial spacing. The MD simulation also showed a minimal effect of the fluctuations in inter-DNA distance on the radial counterion density profile and significant penetration of the grooves by TMA. The radial density profile of the counterions was also obtained from a Monte Carlo (MC) computer simulation of a hexagonal array of charged rods with fixed interaxial spacing. Strong ordering of the counterions between the DNA molecules and the absence of charge fluctuations at longer wavelengths was shown by the SANS number and charge structure factors. The DNA-counterion and counterion structure factors are interpreted with the correlation functions derived from the Poisson-Boltzmann equation, MD, and MC simulation. Best agreement is observed between the experimental structure factors and the prediction based on the Poisson-Boltzmann equation and/or MC simulation. The SANS results show that TMA is too large to penetrate the grooves to a significant extent, in contrast to what is shown by MD simulation.     

The counterion influence on cationic lipid-mediated transfection of plasmid DNA

A panel of DOTAP analogs was prepared by altering the anionic counterion that accompanies the trimethylammonium polar domain. The transfection of plasmid DNA into NIH3T3 cells and mouse lung was examined using the counterion analogs. The in vitro transfection activity decreased as follows: DOTAP · bisulfate > trifluoromethanesulfonate ∼ iodide ∼ bromide > dihydrogenphosphate ∼ chloride ∼ acetate > sulfate. A similar activity trend was observed in vivo.     

Trivalent counterion condensation on DNA measured by pulse gel electrophoresis

Pulse gel electrophoresis was used to measure the reduction of mobilities of λ-DNA-Hind III fragments ranging from 23.130 to 2.027 kilobase pairs in Tris borate buffer solutions mixed with either hexammine cobalt(III), or spermidine³⁺ trivalent counterions that competed with Tris⁺ and Na⁺ for binding onto polyion DNA. The normalized titration curves of mobility were well fit by the two-variable counterion condensation theory. The agreement between measured charge fraction neutralized and counterion condensation prediction was good over a relatively wide range of trivalent cation concentrations at several solution conditions (pH, ionic strength). The effect of ionic strength, trivalent cation concentration, counterion structure, and DNA length on the binding were discussed based on the experimental measurements and the counterion condensation theory. © 1996 John Wiley & Sons, Inc.     

Effect of ions on counterion fluctuation in low-molecular weight DNA dielectric dispersions

The dielectric permittivity of aqueous solutions of low-molecular weight DNA (Mr = 3.2 X 10(5) ) in the presence of MgCl2 and AgNO3 has been measured in the frequency range from 5 kHz to 30 MHz, at a temperature of 25 degrees C. The DNA concentration was 3.5 X 10(-4) M in terms of phosphate and the salt concentration was varied from 1 X 10(-5) to 2 X 10(-4) M. The dielectric results have been analyzed in terms of two contiguous dielectric dispersions, and characteristic parameters have been discussed on the basis of polyelectrolyte theories which deal with counterion fluctuation. Some molecular parameters of the DNA molecule in electrolyte solutions are estimated.     

23Na-NMR investigations of counterion exchange reactions of helical DNA

Changes in Δν_½, the nmr linewidth of ²³Na, have been determined during titrations of helical DNA with polyamines (divalent putrescine and trivalent spermidine) and with inorganic cations (Mg²⁺ and Co(NH₃)). In each case additions of a multivalent cation (M^z+) to a solution containing NaDNA and NaCl cause decreases in Δν_½, which is a population-weighted average of contributions from nuclei in bound and free environments. Thus, the binding of M^z+ to DNA displaces sodium ions from regions where the quadrupolar relaxation of ²³Na is relatively efficient. At a given extent of titration, the binding of a polyamine produces a smaller decrease in Δν_½ than does the binding of an inorganic ion of the same valence. The concentration dependence of Δν_½ during the course of a titration can be interpreted most simply as a two-state ion-exchange reaction by assuming that the binding of M^z does not alter R_B, the average relaxation rate of sodium nuclei that remain bound. On the basis of this assumption, the initial linear portions of titration curves can be analyzed to determine upper bounds for r°, the number of sodium ions bound per DNA phosphate in the absence of any competing counterion. Analyzing the titration curves for the four multivalent competitors leads to a range of upper-bound estimates for r°: 0.5–0.8. The differences in these estimates could indicate that polyamines displace fewer sodium ions from DNA than do their smaller inorganic counterparts. Alternatively, the range in upper-bound estimates for r° could also reflect specific differences in the effects of the various multivalent cations on R_B, if this relaxation rate does change during titration.     

The contribution of transient counterion imbalances to DNA bending fluctuations

A two-sided model for DNA is employed to analyze fluctuations of the spatial distribution of condensed counterions and the effect of these fluctuations on transient bending. We analyze two classes of fluctuations. In the first, the number of condensed counterions on one side of the DNA remains at its average value, while on the other side, counterions are lost to bulk solution or gained from it. The second class of fluctuations is characterized by movement of some counterions from one side of the DNA to the other. The root-mean-square fluctuation for each class is calculated from counterion condensation theory. The amplitude of the root-mean-square fluctuation depends on the ionic strength as well as the length of the segment considered and is of the order 5-10%. Both classes of fluctuation result in transient bends toward the side of greater counterion density. The bending amplitudes are approximately 15% of the total root-mean-square bends associated with the persistence length of DNA. We are thus led to suggest that asymmetric fluctuations of counterion density contribute modestly but significantly toward the aggregate of thermalized solvent fluctuations that cause bending deformations of DNA free in solution. The calculations support the idea that counterions may exert some modulating influence on the fine structure of DNA.     

Formation of ordered domains in membrane-bound DNA.

The interactions between DNA molecules adsorbed on fluid membranes are calculated. The adsorbing DNA perturbs the equilibrium packing of the lipids, thereby giving rise to membrane-induced, attractive interactions. These balance the direct repulsive interactions between DNA molecules. As a result, DNA adsorbed on membranes is predicted to form ordered domains characterized by a finite spacing, which varies with the membrane characteristics and the solution Debye screening length. Comparing the model predictions to recent experiments (Yang et al. 1996) yields excellent agreement with only one free (i.e., experimentally unknown) parameter.     

Similarities and differences in interaction of K+ and Na+ with condensed ordered DNA. A molecular dynamics computer simulation study

Four 20 ns molecular dynamics simulations have been performed with two counterions, K⁺ or Na⁺, at two water contents, 15 or 20 H₂O per nucleotide. A hexagonal simulation cell comprised of three identical DNA decamers [d(5′-ATGCAGTCAG) × d(5′-TGACTGCATC)] with periodic boundary condition along the DNA helix was used. The simulation setup mimics the DNA state in oriented DNA fibers or in crystals of DNA oligomers. Variation of counterion nature and water content do not alter averaged DNA structure. K⁺ and Na⁺ binding to DNA are different. K⁺ binds to the electronegative sites of DNA bases in the major and the minor grooves, while Na⁺ interacts preferentially with the phosphate groups. Increase of water causes a shift of both K⁺ and Na⁺ from the first hydration shell of O1P/O2P and of the DNA bases in the minor groove with lesser influence for the cation binding to the bases in the major groove. Mobility of both water and cations in the K–DNA systems is faster than in the Na–DNA systems: Na⁺ organizes and immobilizes water structure around itself and near DNA while for K⁺ water is less organized and more dynamic.     

Nanomechanical behaviors of microcantilever-based single-stranded DNA chips induced by counterion osmotic effects

Experiments show that deflections of microcantilever-DNA chip can be induced by many factors, such as grafting density, hybridization efficiency, concentration, length and sequence of DNA molecules, buffer salt concentration, time, and temperature variation. However, there are few theoretical works on microcantilever-DNA chips. The present paper is aimed to study the influence of counterion effects of single-stranded DNA (ssDNA) polyelectrolyte solution on the nanomechanical behaviors of microcantilever-based ssDNA chips during packing process. First, the effect of osmotic pressure induced by ingress of counterions into DNA brush structures is studied with Hagan’s model for a cylindrical polyelectrolyte brush system on the basis of Poisson-Boltzmann distribution hypothesis. Second, Zhang’s two-variable method for a laminated cantilever is used to formulate a four-layer energy model for ssDNA chips with weak interactions. Third, the influence of grafting density, ssDNA chain length, and salt concentration on packing deflection is investigated using the principle of minimum energy. The predictive tendency is qualitatively similar to those observed in some related ssDNA chip experiments. The difference between the four-layer model and the simplified two-layer model for ssDNA chips is also discussed.     

B-Z DNA conformational transition in 1:1 electrolytes: dependence upon counterion size

We have studied the B-Z transition of poly[d(G-C)] in the presence of alkali metal, tetramethylammonium and tetraethylammonium chlorides at room temperature. The measured critical salt concentrations increase in the order Na, K, Rb, TMA, Cs and are in good agreement with the theoretical values predicted from a statistical-mechanical treatment of the transition.     

Brownian dynamics simulations of probe and self-diffusion in concentrated protein and DNA solutions.

We have developed a Brownian dynamics algorithm for simulating probe and self-diffusion in concentrated solutions of DNA and protein. In these simulations, proteins are represented as spheres with radii given by their hydrodynamic radii, while DNA is modeled as a wormlike chain of hydrodynamically equivalent spherical frictional elements. The molecular interaction potentials employed by the program allow for intramolecular stretching and bending motions of the DNA chains, short-range Lennard-Jones interactions, and long-range electrostatic interactions. To test the program, we have carried out simulations of bovine serum albumin (BSA) probe diffusion and DNA self-diffusion in solutions of short-chain DNA as a function of both DNA concentration and solution ionic strength. In addition, we report on simulations of BSA self-diffusion as a function of BSA concentration and ionic strength. Based on a comparison to available experimental data, we find that our simulations accurately predict these transport properties under conditions of physiological salt concentration and predict the stronger concentration dependence observed at lower salt concentrations. These results are discussed in light of the nature of the intermolecular interactions in such systems and the approximations and limitations of the simulation algorithm.     

Effects of Li+ transport and intracellular binding on Li+/Mg2+ competition in bovine chromaffin cells

Li(+) transport, intracellular immobilisation and Li(+)/Mg(2+) competition were studied in Li(+)-loaded bovine chromaffin cells. Li(+) influx rate constants, k(i), obtained by atomic absorption (AA) spectrophotometry, in control (without and with ouabain) and depolarising (without and with nitrendipine) conditions, showed that L-type voltage-sensitive Ca(2+) channels have an important role in Li(+) uptake under depolarising conditions. The Li(+) influx apparent rate constant, k(iapp), determined under control conditions by (7)Li NMR spectroscopy with the cells immobilised and perfused, was much lower than the AA-determined value for the cells in suspension. Loading of cell suspensions with 15 mmol l(-1) LiCl led, within 90 min, to a AA-measured total intracellular Li(+) concentration, [Li(+)](iT)=11.39+/-0.56 mmol (l cells)(-1), very close to the steady state value. The intracellular Li(+) T(1)/T(2) ratio of (7)Li NMR relaxation times of the Li(+)-loaded cells reflected a high degree of Li(+) immobilisation in bovine chromaffin cells, similar to neuroblastoma, but larger than for lymphoblastoma and erythrocyte cells. A 52% increase in the intracellular free Mg(2+) concentration, Delta[Mg(2+)](f)=0.27+/-0.05 mmol (l cells)(-1) was measured for chromaffin cells loaded with the Mg(2+)-specific fluorescent probe furaptra, after 90-min loading with 15 mmol l(-1) LiCl, using fluorescence spectroscopy, indicating significant displacement of Mg(2+) by Li(+) from its intracellular binding sites. Comparison with other cell types showed that the extent of intracellular Li(+)/Mg(2+) competition at the same Li(+) loading level depends on intracellular Li(+) transport and immobilisation in a cell-specific manner, being maximal for neuroblastoma cells.     

Interaction of glutathione and other low-molecular-weight thiols with DNA: evidence for counterion condensation and coion depletion near DNA

The interaction of low-molecular-weight thiols with sonicated DNA was examined using spin filtration to concentrate the DNA. Cationic thiols (WR 1065 and cysteamine) behaved as counterions and were found to have increased concentrations in the DNA retentate relative to the filtrate. Anionic thiols (GSH, 2-mercaptoethanesulfonate, mercaptosuccinate) behaved as coions and were decreased in concentration in the DNA fraction. Concentrations of the uncharged thiol 2-mercaptoethanol were little influenced by DNA. The results demonstrate the importance of counterion condensation and coion depletion in determining the concentrations of charged species near DNA. They provide a rationale for enhanced effectiveness of WR 1065 and cysteamine as radioprotectors compared to neutral and anionic thiols and suggest that anionic thiols such as GSH should be poor radioprotectors of DNA.