Interaction of chloroquine with linear and supercoiled DNAs. Effect on the torsional dynamics, rigidity, and twist energy parameter

The magnitude and uniformity of the torsion elastic constant (alpha) of linear pBR322 DNA and supercoiled pBR322 DNAs with high-twist (sigma = -0.083) and normal-twist (sigma = -0.48) are measured in 0.1 M NaCl as a function of added chloroquine/base-pair ratio (chl/bp) by studying the fluorescence polarization anisotrophy (FPA) of intercalated ethidium dye. The time-resolved FPA is measured by using a picosecond dye laser for excitation and time-correlated single-photon counting detection. A general theory is developed for the binding of ligands that unwind superhelical DNAs, and the simultaneous binding of two different intercalators is treated in detail. The equilibrium constant (K) for binding chloroquine to linear pBR322 DNA and the number (r) of bound chloroquines per base pair are determined from the relative amplitude ratio of the slow (normally intercalated) and fast (free) components in the decay of the (probe) ethidium fluorescence intensity as a function of chl/bp. For chloroquine binding to supercoiled pBR322 DNAs, the intrinsic binding constant is assumed to be the same as for the linear DNA, but the twist energy parameter ET (N times the free energy to change the linking number from 0 to 1 in units of kBT) is regarded as adjustable. Using the best-fit ET, the binding ratios r are calculated for each chl/bp ratio. Twist energy parameters are also determined for ethidium binding to these supercoiled DNAs by competitive dialysis. For chloroquine binding, we obtain ET = 360 and 460 respectively for the normal-twist and high-twist supercoiled DNAs. For ethidium binding the corresponding values are ET = 280 +/- 70 and 347 +/- 50. Like other dye-binding values, these are substantially lower than those obtained by ligation methods. In the absence of chloroquine, the torsion constants of all three DNAs are virtually identical, alpha = (5.0 +/- 0.4) x 10(-12) dyn.cm. For linear pBR322 DNA, the magnitude and uniformity of alpha remain unaltered by intercalated chloroquine up to r = 0.19. This finding argues that the FPA is not significantly relaxed by diffusion of any kinks or solitons. If alpha d denotes the torsion constant between a dye and a base pair and alpha 0 that between two base pairs, then our data imply that alpha d/alpha 0 lies in the range 0.65-1.64, with a most probable value of 1.0.(ABSTRACT TRUNCATED AT 400 WORDS)     

Monte Carlo simulations of locally melted supercoiled DNAs in 20 mM ionic strength

Mesoscopic models of unmelted and locally melted supercoiled DNAs in 20 mM ionic strength are simulated over a range of linking difference from deltal = 0 to -26 turns, or superhelix density from sigma = 0 to -0.062. A domain containing m = 0, 28, or 56 melted basepairs (out of 4349 total) is modeled simply by a region of suitable length with substantially reduced torsion and bending elastic constants. Average structural properties are calculated from the saved configurations, and a reversible work protocol is used to calculate the supercoiling free energy, The cross-writhe between duplex and melted regions (defined herein) is found to be negligibly small. The total writhe, radius of gyration, and ordered elements of the diagonalized inertial tensor are found to be nearly universal functions of the residual linking difference (deltal(r)) associated with the duplex region, independent of m. However, deformability of the tertiary structure, as manifested by the variance of those same properties, is not a universal function of deltal(r)), but depends upon m.delta (SC) varies with deltal(r)) more strongly than deltal(r)) (2)due to the low ionic strength. The twist energy parameter, E (T) obtained from the simulated delta G(SC), deltal(r)), and net twisting strain of the melted region T (D), is found to be independent of m, hence also of the torsion and bending elastic constants of the melted region. However, E(T) increases linearly with -deltalr), which leads to 1). a small overestimation of E (T) for any given deltal(r)) when E(T) is determined from the observed deltal and deltal (r) by the protocol of Bauer and Benham; and 2). a significant enhancement of the apparent slope, -dE(T)/d(T), obtained via the protocol of Bauer and Benham, relative to the actual slope at fixed delta l(r). After taking these two effects into account, the theoretical and experimental values E(T) and -dE(T)/d(T) values agree rather well. For the larger deltal the melted regions are found preferentially in the linker domains between interwound arms, rather than in the apical regions at the ends of interwound arms.     

Effect of ethidium on the torsion constants of linear and supercoiled DNAs.

The torsion elastic constants (alpha) of linear pBR322 (4363 bp) and pUC8 (2717 bp) DNAs and supercoiled pBR322 and pJMSII (4375 bp) DNAs are measured in 0.1 M NaCl as a function of added ethidium/base-pair (EB/BP) ratio by studying the fluorescence polarization anisotropy (FPA) of the intercalated ethidium. The time-resolved FPA is measured by using a picosecond dye laser for excitation and time-correlated single photon counting detection. Previously developed theory for the emission anisotropy is generalized to incorporate rotations of the transition dipole due to excitation transfer. The excitation transfers are simulated by a Monte Carlo procedure (Genest et al., Biophys. Chem. 1 (1974) 266-278) and the consequent rotations of the transition dipole are superposed on the Brownian rotations. After accounting for excitation transfer, the torsion constants of the linear DNAs are found to be essentially independent of intercalated ethidium up to a binding ratio r = 0.10 dye/bp. Dynamic light scattering measurements on linear pUC8 DNA confirm that the torsion constant is independent of binding ratio up to r = 0.20 dye/bp. If alpha d denotes the torsion constant between ethidium and a base-pair, and alpha 0 that between two base-pairs, then our data imply that alpha d/alpha 0 lies in the range 0.65 to 1.64 with a most probable value of 1.0. The torsion constants of supercoiled DNAs decrease substantially with increasing binding ratio even after accounting for excitation transfer. At the binding ratio r* = 0.064, where the superhelix density vanishes and superhelical strain is completely relaxed, the torsion constant of the supercoiled pBR322 DNA/dye complex lies below that of the corresponding linear DNA/dye complex by about 30%. This contradicts the conventional view according to which linear, nicked circular, and supercoiled DNA/dye complexes with r = r* should coexist with the same concentration of free dye, display the same distribution of bound dye, and exhibit identical secondary structures, twisting and bending rigidities, and FPA dynamics. These and other observations imply the existence of metastable secondary structure in freshly relaxed supercoiled DNAs. A tentative explanation is presented for these and other unexpected observations on supercoiled DNAs.     

Kinetics of nucleosome unfolding at low ionic strength

The kinetics of a conformational change which occurs in nucleosome core particles at about 1 mM ionic strength have been studied by observing changes in the fluorescence of labeled histone H3. The unfolding reaction is intramolecular since no concentration dependence is observed. However, the kinetics are unexpectedly complicated and reveal evidence of at least three relaxation times. It is possible to fit the kinetics observed under several conditions to a consistent four-state cyclic mechanism in which folded and unfolded forms can inter-convert by two parallel pathways, each involving a distinct intermediate. While the data are not sufficient to establish this mechanism as a unique choice, they exclude many simpler possibilities. The cyclic mechanism is quite reasonable in view of what is currently known about the structures of the folded and unfolded forms.     

Nonideal size-exclusion chromatography of proteins: Effects of pH at low ionic strength

Ideal size-exclusion chromatography separates molecules primarily on the basis of hydrodynamic volume. This is achieved only when the chromatographic support is neutral and the polarity nearly equal to that of the mobile phase. When this is not the case, the support surface may begin to play a role in the separation process. As the magnitude of surface contributions becomes larger, the deviation from the ideal increases. Because the separation mechanism is different than that of ideal size-exclusion chromatography, selectivity could be increased in nonideal size-exclusion chromatography. This paper explores the use of size-exclusion chromatography columns with mobile phases that cause proteins to exhibit slight deviations from the ideal size-exclusion mechanism. Although there are many ways to initiate nonideal size-exclusion behavior, the specific variable examined in this study is the influence of pH at low ionic strength. Individual proteins were chromatographed on SynChrom GPC-100, TSK-G2000SW, and TSK-G3000SW columns at low ionic strength. It was found that a protein could be selectively adsorbed, ion excluded, or chromatographed in an ideal size-exclusion mode by varying mobile-phase pH relative to the isoelectric point of the protein. In extreme cases, molecules could be induced either to elute in the void volume or beyond the volume of total permeation. It is postulated that these effects are the result of electrostatic interactions between proteins and surface silanols on the support surface. Optimization of size-exclusion separations relative to protein isoelectric points is discussed.     

Crystallization of tuna ferricytochrome c at low ionic strength

Previous crystallographic studies of tuna ferricytochrome c have employed crystals grown from solutions of ammonium sulfate, corresponding to an ionic strength of 9.5 M (Takano, T., and Dickerson, R. E. (1981) J. Mol. Biol. 153, 95-115). To obtain a structure at a lower ionic strength, the ferric tuna protein was crystallized at neutral pH with polyethylene glycol at an ionic strength of 45 mM, These crystals (space group P2(1), a = 37.11 A, b = 107.66 A, c = 55.75 A, beta = 105.3 degrees) contain four molecules/asymmetric unit and grow to dimensions of 0.2 X 0.4 X 1.0 mm in 2-4 weeks. They diffract to beyond 1.8 A and are stable in the x-ray beam. We have recorded 28,198 unique Bragg reflections (83% of those possible) to a resolution of 1.89 A from a native crystal. We are undertaking a solution of this structure by the molecular replacement method.     

Neutron scattering studies of nucleosome structure at low ionic strength

Ionic strength studies using homogeneous preparations of chicken erythrocyte nucleosomes containing either 146 or 175 base pairs of DNA show a single unfolding transition at about 1.5 mM ionic strength as determined by small-angle neutron scattering. The transition seen by some investigators at between 2.9 and 7.5 mM ionic strength is not observed by small-angle neutron scattering in either type of nucleosome particle. The two contrasts measured (H2O and D2O) indicate that only small conformational changes occur in the protein core, but the DNA is partially unfolded below the transition point. Patterson inversion of the data and analysis of models indicate that the DNA in both types of particle is unwinding from the ends, leaving about one turn of supercoiled DNA bound to the histone core in approximately its normal (compact) conformation. The mechanism of unfolding appears to be similar for both types of particles and in both cases occurs at the same ionic strength. The unfolding observed for nucleosomes in this study is in definite disagreement with extended superhelical models for the DNA and also disagrees with models incorporating an unfolded histone core.     

Precollapse of T7 DNA by spermidine at low ionic strength: A linear dichroism and intrinsic viscosity study

At low salt ([Na⁺] = 10^?3M), spermidine is capable of transforming DNA from a highly extended random coil to a compact particle. The transition takes place at a spermidine concentration of around 25 μM and the compact particle has been previously studied in considerable detail for several different DNAs. The objective of the present study is to see what effect, if any, spermidine has on T7 DNA conformation prior to collapse using flow dichroism and intrinsic viscosity. We conclude that increasing the spermidine concentration from 0 to the collapse transition point (above 20 μM) makes DNA increasingly nondraining. Furthermore, the persistence length dropped from 785 (±42) to 560 (±32) to 445 (±26) Å on increasing the ambient spermidine concentration from 0 to 1 to 10 μM. These results are in good agreement with counterion condensation theory and Odijk's theory of the electrostatic contribution to the persistence length of DNA. Nonetheless, it is concluded that counterion condensation is not entirely responsible for DNA collapse and that crosslinking promotes the transition to the compact state.     

Electric and flow linear dichroism of unfolded and condensed chromatin: a comparative study at low and intermediate ionic strength

Identical samples containing polynucleosomal chains of chicken erythrocyte (CE) and Ehrlich ascites tumour (EA) chromatin were studied under various ionic conditions with regard to electric linear dichroism (ELD) and flow linear dichroism (FLD). Both orientation techniques consistently confirmed that, in the limit of very low ionic strength and in the absence of multivalent cations, the reduced linear dichroism of chromatin is negative in the DNA-base absorption band, as expected for an extended zig-zag polynucleosomal conformation. With increasing electrolyte content, both ELD and FLD decreased drastically in amplitude, but in contrast to the ELD which remains negative in an intermediate range of low ionic strength (0.1-0.5 mM Mg2+) the FLD changes sign and becomes positive. The ELD and FLD amplitudes decrease with higher Mg2+ concentrations and FLD even vanishes in the region of 0.2-0.4 mM; both signals are positive above 0.4-0.5 mM Mg2+. The origin of the dissimilarities between ELD and FLD observations is still not fully understood. Several possibilities are considered: ELD signals are more influenced than FLD by the presence of short chromatin chains, nucleosomes and small pieces of naked DNA, while FLD is more susceptible to the presence of large, easily orientable, scattering aggregates. Different preferred orientation directions of the chromatin fibre with respect to electric and hydrodynamic fields may also be involved. Finally, FLD and ELD probably "see" different features of the chromatin structure.