Circular dichroism studies of the B goes to A conformational transition in seven small DNA restriction fragments containing the Escherichia coli lactose control region.

The B goes to A conformational transition caused by high ethanol concentrations was studied for seven DNA restriction fragments with overlapping and known sequences. Since the DNAs are homogeneous and range in GC content from 44-63%, they permit an evaluation of the influence of DNA sequence and base composition on the B goes to A transition. Moreover, their small size (80-301 bp) minimizes precipitation artifacts. The B- form spectra (in low salt) and the transition toward the C- form (in ethanol concentrations below the B goes to A transition) agree with prior measurements on chromosomal DNAs and are similar for all seven DNAs. At higher ethanol concentrations (80%), all fragments undergo a transition to the A- form as judged by the large increase of the positive CD band at 270 nm. Difference spectra among the fragments reveal minor differences between the A- form spectra. The ethanol concentration necessary to cause this transition is 72 +/- 2% for all fragments, thus excluding a preference of the CAP-, E. coli RNA polymerase-, or lac repressor-binding sequences for the A- form. The kinetics of the B goes to A transition in 80% ethanol are biphasic; the initial rapid transition is an intramolecular B goes to A form shift and the slower transition is an aggregation (but not precipitation) of the DNA     

Different effects of polylysine and polyarginine on the transition to a condensed state of DNA in polyethyleneglycol/salt solution.

Circular dichroism spectroscopy has been used to investigate the influence of polylysine and polyarginine on the transition to a condensed state of DNA brought about by high concentrations of polyethyleneglycol and salt. From the dependence on DNA concentration of the CD signals, the anomalous CD of free DNA in polyethyleneglycol/salt solution was attributed to the intermolecular association of DNA molecules. The CD spectral changes in polyethyleneglycol/salt solution of the DNA - polylysine complex were indistinguishable from those of free DNA while the DNA-polyarginine complex suffered much smaller spectral changes as compared with free DNA, at low DNA concentrations where time-independent CD spectra were observed in polyethyleneglycol/salt solution for both the complexed and free DNA. The repression of the spectral change by the latter complex was more remarkable at higher ratios of polyarginine to DNA. The facts indicate that, whereas polylysine binding has little influence on the intermolecular structural transition of double-stranded DNA into a compact molecular configuration in polyethyleneglycol/salt solution, polyarginine binding has an effect of inhibiting the transition.     

Alcohol-induced changes of beta-lactoglobulin-retinol-binding stoichiometry

It has been demonstrated using CD that ethanol induces important secondary structure changes of beta-lactoglobulin. CD spectra indicate that beta-lactoglobulin secondary structure, which is mainly composed of beta-strands, becomes mostly alpha-helical under the influence of the solvent polarity changes. The midpoint of beta-strand/alpha-helix transition in beta-lactoglobulin is observed at dielectric constant approximately 60 (35% ethanol; v/v). According to CD measurements, the ethanol-dependent secondary structure changes are reversible. The alkylation of lysines epsilon-NH2 in beta-lactoglobulin weakens the central beta-barrel structure, since the beta-strand/alpha-helix transition midpoint of alkylated beta-lactoglobulin is shifted to lower ethanol concentration (25% ethanol; v/v). beta-Lactoglobulin structural changes are triggering the dissociation of the beta-lactoglobulin-retinol complex as judged from complete quenching of its fluorescence in ethanol concentration greater than 30% (v/v). However, in 20% ethanol (v/v), beta-lactoglobulin still retains most of its native secondary structure as shown by CD and, in this condition, one beta-lactoglobulin molecule binds an additional second retinol molecule. This suggests that the highly populated species observed around 20% ethanol (v/v) might represent an intermediate state able to bind two molecules of retinol.     

Dehydrated circular DNA: Circular dichroism of molecules in ethanolic solutions

We have measured the ultraviolet CD spectra for covalently closed and linear forms of phage PM2 DNA in solution. We find that increased concentrations of salt or ethanol (up to 50% ethanol by weight) depress the long-wavelength positive CD bands in the spectra of both forms of DNA, although the spectrum of the native covalently closed DNA always has a slightly larger magnitude of these bands than does the spectrum of the linear DNA. In addition, both DNAs are equally capable of undergoing a transition to the A conformation in 70–80% ethanol at low Na⁺ concentrations. Thus, the constraint imposed by the covalent closure of a DNA molecule does not seem to hinder its conformational response to these changing solution conditions. Lang [(1973) J. Mol. Biol. 78 , 247–254] has found by electron microscopy that T7 DNA has an inherent ability to condense into compact particles, suggested to be supercoils of multiple order. Both covalently closed and linear forms of PM2 DNA also become condensed when the DNA, in 0.2M ammonium acetate and 1 mM EDTA, is exposed to ethanol and subsequent drying on specimen grids [Lang, D., Taylor, T. N., Dobyan, D. C. & Gray, D. M. (1976) J. Mol. Biol. 106 , 97–107]. Under similar conditions, in solutions of 0.2M ammonium acetate and 1 mM EDTA to which ethanol is added, we have measured the CD spectra of both covalently closed and linear forms of DNA. Below ethanol concentrations at which the DNA obviously precipitates, the CD spectra of both forms have reduced long-wavelength positive CD bands.     

Structural transitions of deoxyribonucleic acid in aqueous electrolyte solutions. I. Reference spectra of conformational limits.

The circular dichroism properties of calf thymus DNA have been examined at 27 degrees over the wavelength range of 215-300 nm in aqueous solutions of NaCl, KCl, LiCl, CsCl, and NH4Cl at pH 7. The concentrations of these electrolytes were varied from 0.01 to ca. 5-10 m. The spectral changes induced by changes in concentration of NaCl and KCl and all but the highest concentrations of NH4Cl as well as lower concentrations of Cstcl and LiCl could be represented by a common two-state transition involving the conversion of the typical conservative spectrum commonly seen in dilute solutions of these salts to a nonconservative spectrum similar to that obtained by Tunis-Schneider and Maestre ((1970), J. Mol. Biol. 52, 521) for the C form of DNA. At higher concentrations of CsCl, LiCl, and NH4Cl, an additional component, resembling an A type spectrum, was required to account for the observed CD changes with changing concentration of electrolyte. Relying on the published spectra of the B, the C, and the A forms of DNA by Tunis-Schneider and Maestre for identification and approximate values of the molecular ellipticities of these forms, we have analyzed these spectral transitions by two least mean squares methods in order to obtain accurate reference spectra of aqueous "B", C, and "A" conformations of calf thymus DNA. The results obtained suggest that although the C form in solution is identical with that obtained in film, the aqueous B conformational limit is not identical with the crystallographic Watson-Crick structure. In addition, the A form generated in solution under our experimental conditions appears to be more similar to that assumed by low molecular weight Escherichia coli DNA at 75% relative humidity rather than calf thymus DNA at the same relative humidity.     

Thermodynamics of the B to Z transition in poly(dGdC)

The thermodynamics of the B to Z transition in poly(dGdC) was examined by differential scanning calorimetry, temperature-dependent absorbance spectroscopy, and CD spectroscopy. In a buffer containing 1 mM Na cacodylate, 1 mM MgCl₂, pH 6.3, the B to Z transition is centered at 76.4°C, and is characterized by ΔH_cal = 2.02 kcal (mol base pair)^?1 and a cooperative unit of 150 base pairs (bp). The t_m of this transition is independent of both polynucleotide and Mg²⁺ concentrations. A second transition, with ΔH_cal = 2.90 cal (mol bp)^?1, follows the B to Z conversion, the t_m of which is dependent upon both the polynucleotide and the Mg²⁺ concentrations. Turbidity changes are concomitant with the second transition, indicative of DNA aggregation. CD spectra recorded at a temperature above the second transition are similar to those reported for ψ(–)-DNA. Both the B to Z transition and the aggregation reaction are fully and rapidly reversible in calorimetric experiments. The helix to coil transition under these solution conditions is centered at 126°C, and is characterized by ΔH_cal = 12.4 kcal (mol bp)^?1 and a cooperative unit of 290 bp. In 5 mM MgCl₂, a single transition is seen centered at 75.5°C, characterized by ΔH_cal = 2.82 kcal (mol bp)^?1 and a cooperative unit of 430 bp. This transition is not readily reversible in calorimetric experiments. Changes in turbidity are coincident with the transition, and CD spectra at a temperature just above the transition are characteristic of ψ(–)-DNA. A transition at 124.9°C is seen under these solution conditions, with ΔH_cal = 10.0 kcal (mol bp)^?1 and which requires a complex three-step reaction mechanism to approximate the experimental excess heat capacity curve. Our results provide a direct measure of the thermodynamics of the B to Z transition, and indicate that Z-DNA is an intermediate in the formation of the ψ-(–) aggregate under these solution conditions.     

Conformational change in a single molecular species, beta3, of beta-conglycinin in acidic ethanol solution

Several physicochemical experiments were done to obtain further information on the conformational changes occurring in beta-conglycinin in acidic-ethanol solution, using a single molecular species of this protein, beta3. By far-UV circular dichroism (CD), a transition from beta-sheet to alpha-helical structure was observed upon addition of acidic-ethanol, and the alpha-helix content was found to reach 76% in 70% ethanol (pH 2). From analyses of near-UV CD and difference absorption spectra, it was found that the tertiary structure of the beta3 species was significantly altered at ethanol concentrations between 10 and 20%. The profiles of binding of 1-anilinonaphthalene-8-sulfonic acid to the beta3 species during acidic-ethanol denaturation were indicative of the existence of intermediate conformers in the molten globule-like denaturation state. By measuring Fourier transform infrared spectra and estimating the Stokes radius by dynamic light scattering, the beta3 molecules were found to aggregate with an increase in ethanol concentration.     

On the flexibility of the boundaries between the A-form and B-form sections in DNA molecule.

The degree of orientation of DNA in a flow has been studied within the interval of the B - A transition induced by ethanol. The orientation of the B DNA (60-65% ethanol, v/v) and that of the A DNA (80-82% ethanol) are nearly identical. This means that both conformations have similar persistence lengths and that there is no aggregation in the course of formation of the A form. Within the transition range (65-78% ethanol) the orientation attains a sharp minimum which coincides with the half-transition point (73% ethanol). The cooperative character of the B - A transition presupposes the existence of boundaries between the alternating sections of the A and B conformations that may entail an increased flexibility of the DNA molecule and a corresponding drop of orientation. Theory predicts an elliptical dependence of the number of boundaries on the proportion of the A form. The experimental degree of orientation follows the same pattern. Quantitative evaluation shows that the flexibility of a boundary is small, so that several dozen of boundaries are required to simulate free rotation.     

Fine structure in the B-A transition of native DNA

The B-A transition caused by high ethanol concentrations has been studied by the multi-dimensional spectrophotometer equipped with the computer-controlled microbullet. When ethanol concentration is increased, the CD signal at 270 nm of linearized ColEl DNA exhibits a biphasic transition; the first broad one and the second sharp one. The B-A transition of the ColEl DNA is much broader than that of alternative copolymers with shorter lengths. In addition, each PvuII restriction fragment of ColEl DNA has a different transition curve. Therefore the stability of the B-A transition varies along a long DNA molecule. The second transition is speculated to be caused by aggregation. When ethanol concentration is decreased, on the other hand, only a single transition shifted to lower ethanol concentration is observed. Thus the B-A transition curve has a hysteresis. A slow dissociation rate of the aggregation seems to cause the hysteresis.     

A study of the B-A transition in DNA by gel electrophoresis

A procedure is developed for studying the B-A transition in DNA using gel electrophoresis. The starting point has been the idea that the junction between the A and B sections, which appear within the transition interval would increase the mobility of the DNA molecules. Indeed, the mobility of DNA in a gel is shown to increase in the middle of the B-A transition due to the formation of the largest possible number of boundaries between the B and A forms. The middle of the B-A transition in supercoiled DNA appears to be shifted against the middle of the transition in open circular (as well as linear) DNA by about 1.3% towards lower ethanol concentrations under the influence of the superhelical stress.     

Structural transitions of calf thymus DNA in concentrated LiCl solutions

The solubility, sedimentation, circular dichroism, and absorption spectral characteristics of calf thymus DNA have been examined in concentrated solutions of LiCl (6-13 m) at 25 to 27 degree C. At all concentrations of LiCl, the DNA is base stacked and exhibits normal hypochromicty, At the upper end of this range of LiCl concentrations, DNA aggregates and ultimately precipitates completely from solution between 13 and 14 m LiCl. This aggregation process is dependent on concentration, base composition, and molecular weight of DNA. The sedimentation velocity data taken together with the absorbance spectral data suggest that the aggregation process leading to the formaiton of large structures beings at approximately equal to 9 m. Prior to the onset of aggregation, the circular dichroism (CD) spectra can be adequately fitted by a linear combination of contributions of the B, C, and A forms of DNA (Hanlon, S., Brudno, S., Wu, T. T., and Wolf, B. (1975), Biochemistry 14, 1648). Above 9 m LiCl, both factor analysis and a primitive version of matrix rank order analysis indicate that at least one additional spectral component is required to account for the observed CD spectra above 260 nm. The general shape of this additional component or distortion resembles the psi form of DNA.     

A Study of the B-A Transition in DNA by Gel Electrophoresis

Abstract

A procedure is developed for studying the B-A transition in DNA using gel electrophoresis. The starting point has been the idea that the junction between the A and B sections, which appear within the transition interval would increase the mobility of the DNA molecules. Indeed, the mobility of DNA in a gel is shown to increase in the middle of the B-A transition due to the formation of the largest possible number of boundaries between the B and A forms. The middle of the B-A transition in supercoiled DNA appears to be shifted against the middle of the transition in open circular (as well as linear) DNA by about 1.3% towards lower ethanol concentrations under the influence of the superhelical stress.     

Conformational origin of the aggregation of recombinant human factor VIII

Aggregation of proteins is a major problem in their use as drugs and is also involved in a variety of pathological diseases. In this study, biophysical techniques were employed to investigate aggregate formation in the pharmaceutically important protein, recombinant human factor VIII (rhFVIII). Recombinant human factor VIII incubated in solution at 37 degrees C formed soluble aggregates as detected by molecular sieve chromatography and dynamic light scattering. This resulted in a corresponding loss of biological activity. Fluorescence and CD spectra of the thermally stressed rhFVIII samples did not, however, suggest significant differences in protein conformation. To identify conformational changes in rhFVIII that may be involved in rhFVIII aggregation, temperature and solutes were used to perturb the native structure of rhFVIII. Far-UV CD and FTIR studies of rhFVIII as a function of temperature revealed conformational changes corresponding to an increase in intermolecular beta-sheet content beginning at approximately 45 degrees C with significant aggregation observed above 60 degrees C. Fluorescence and DSC studies of rhFVIII also indicated conformational changes initiating between 45 and 50 degrees C. An increase in the exposure of hydrophobic surfaces was observed beginning at approximately 40 degrees C, as monitored by increased binding of the fluorescent probe, bis-anilinonaphthalene sulfonic acid (bis-ANS). Perturbation by various solutes produced several transitions prior to extensive unfolding of rhFVIII. In all cases, a common transition, characterized by an increase in the wavelength of the fluorescence emission maximum of rhFVIII from approximately 330 to 335 nm, was observed during thermal and solute perturbation of factor VIII. Moreover, this transition was correlated with an increased association of factor VIII upon incubation at 37 degrees C in the presence of various solutes. These results suggest that association of rhFVIII in solution was initiated by a small transition in the tertiary structure of the protein which produced a nucleating species that led to the formation of inactive soluble aggregates.     

In vitro study of stability and amyloid-fibril formation of two mutants of human stefin B (cystatin B) occurring in patients with EPM1

Myoclonus epilepsy of type 1 (EPM1) is a rare monogenic progressive and degenerative epilepsy, also known under the name Unverricht-Lundborg disease. With the aim of comparing their behavior in vitro, wild-type (wt) human stefin B (cystatin B) and the G4R and the R68X mutants observed in EPM1 were expressed and isolated from the Escherichia coli lysate. The R68X mutant (Arg68Stop) is a peptide of 67 amino acids from the N terminus of stefin B. CD spectra have shown that the R68X peptide is not folded, in contrast to the G4R mutant, which folds like wild type. The wild type and the G4R mutant were unfolded by urea and by trifluoroethanol (TFE). It has been shown that both proteins have closely similar stability and that at pH 4.8, where a native-like intermediate was demonstrated, TFE induces unfolding intermediates prior to the major transition to the all-alpha-helical state. Kinetics of fibril formation were followed by Thioflavin T fluorescence while the accompanying changes of morphology were followed by the transmission electron microscopy (TEM). For the two folded proteins the optimal concentration of TFE producing extensive lag phases and high fibril yields was predenaturational, 9% (v/v). The unfolded R68X peptide, which is highly prone to aggregate, formed amyloid fibrils in aqueous solution and in predenaturing 3% TFE. The G4R mutant exhibited a much longer lag phase than the wild type, with the accumulation of prefibrillar aggregates. Implications for pathology in view of the higher toxicity of prefibrillar aggregates to cells are discussed.     

Alcohol induced structural and dynamic changes in β-lactoglobulin in aqueous solution: A neutron scattering study

Structural and dynamic properties of β-lactoglobulin (β-LG) were revealed as a function of alcohol concentration in ethanol- and trifluoroethanol(TFE)-water mixtures with circular dichroism (CD), small-angle neutron scattering (SANS) and quasi-elastic neutron scattering (QENS). The CD spectra showed that an increase in TFE concentration promotes the formation of the β-sheet structure of β-LG. The SANS-intensities were fitted using form factors for two attached spheres for the native and native-like states of the protein. At higher alcohol concentrations, where aggregation takes place, a form factor modelling diffusion limited colloidal aggregation (DLCA) was employed. The QENS-data were analyzed in terms of internal motions for all alcohol concentrations. While low concentrations of TFE (10% (v/v)) lead to an increase of the mean square amplitudes of vibrations and a retention of a native-like structure - but not to an increase of the characteristic radius of proton diffusion processes a. Addition of 20% (v/v) of TFE induces aggregation, going along with a further increase of . Further increase of TFE concentration to 30% (v/v) changes the nanoscale structure of the oligomeric nucleate, but induces no further significant changes in . The present study underlines the necessity of methods sensitive to the dynamics of a system to obtain a complete picture of a molecular process.     

Poly(L–lysine)–DNA interactions in NaCl solutions: B → C and B → ψ Transitions

Thermal denaturation and circular dichroism (CD) properties of poly(L -lysine)–DNA complexes vary greatly when these complexes are prepared differently, that is, whether by NaCl-gradient dialysis starting from 2.0 M NaCl or by direct mixing at low salt. These differing properties were investigated in more detail by examining complexes, made by direct mixing in the presence of various concentrations of NaCl, both before and after the NaCl was dialyzed out of the complex solution. The precipitation curves of DNA due to polylysine binding indicate that such binding is noncooperative at zero salt; from 0.1 up to 1.0 M NaCl they exhibit varying degrees of cooperatively. Starting from zero salt, as the NaCl concentration used for complex formation is increased, both the CD and the melting properties of the complexes are shifted from those of directly mixed at zero salt to those of reconstitution: in the CD spectra there is a gradual shift from a B → C transition to a B → ψ transition; thermal denaturation results show a gradual increase in the melting temperatures of both free DNA (t_m) and polylysine-bound DNA (t′_m). The progressive shift from B → C to B → ψ suggests a close relationship between these two transitions. Large aggregates of the complexes do not warrant the appearance of ψ-type CD spectra: ψ-spectra have been obtained in the supernatants of polylysine–DNA complexes made and measured at 1.0 M NaCl while slightly perturbed CD spectra in B → C transition have been observed in turbid solutions of fully covered complexes made at very low salt. If the complexes are made at intermediate salts and dialyzed to a very low salt, although up to 60% of the DNA is still bound by polylysine, the CD spectra of the complexes are shifted back to the B-type CD characteristic of pure DNA.     

Condensation prevails over B-A transition in the structure of DNA at low humidity

B-A transition and DNA condensation are processes regulated by base sequence and water activity. The constraints imposed by interhelical interactions in condensation compromise the observation of the mechanism by which B and A base-stacking modes influence the global state of the molecule. We used a single-molecule approach to prevent aggregation and mechanical force to control the intramolecular chain association involved in condensation. Force-extension experiments with optical tweezers revealed that DNA stretches as B-DNA under ethanol and spermine concentrations that favor the A-form. Moreover, we found no contour-length change compatible with a cooperative transition between the A and B forms within the intrinsic-force regime. Experiments performed at constant force in the entropic-force regime with magnetic tweezers similarly did not show a bistable contraction of the molecules that could be attributed to the B-A transition when the physiological buffer was replaced by a water-ethanol mixture. A total, stepwise collapse was found instead, which is characteristic of DNA condensation. Therefore, a low-humidity-induced change from the B- to the A-form base-stacking alone does not lead to a contour-length shortening. These results support a mechanism for the B-A transition in which low-humidity conditions locally change the base-stacking arrangement and globally induce DNA condensation, an effect that may eventually stabilize a molecular contour-length reduction.     

Phosphorus NMR spectra of natural DNA fragments in the course of the B-to-A conformational transition

Changes in the ³¹P-nmr spectra of sonicated natural DNA fragments were investigated in ethanol solutions where the fragments underwent, as checked by CD, the B-to-A conformational transition. The study produced the following conclusions: (1) The high DNA concentrations used for the ³¹P-nmr measurements promote the transition compared to dilute solutions that are commonly used for CD measurements. (2) The B-to-A transition was reflected in a cooperative downfield shift of the DNA ³¹P-nmr resonance, consistent with unwinding of the double helix. (3) Prior to the transition, the changes in chemical shift of double-and single-stranded DNAs were almost identical. It thus appears that the effect of ethanol on the geometry and hydration of phosphodiester linkages does not depend heavily on DNA base–base interactions. (4) The A-form resonances were 30–40% narrower than the B-form resonances, which is attributed to marked sequence-dependent variations in the latter conformation and to their reduction in the former. (5) The B-form DNA aggregated in the concentrated ³¹P-nmr samples in the presence of ethanol, judged from a milky opalescence of the solution and a substantial broadening of its ³¹P-nmr resonance. The broadening abruptly disappeared as soon as DNA adopted the A-form so that DNA, in dependence on the secondary structure, showed different tendencies to condense in the presence of ethanol. The condensation increased cooperativity of the B-to-A interconversion.     

Alcohol induced B-A transition of DNAs with different base compositions studied by circular dichroism

The circular dichroic (CD) spectra of natural DNAs (from Cl. perfringens, T2 phage, calf thymus, E. coli, and M. lysodeikticus) as well as duplexes of synthetic DNAs (poly(dA) X poly(dT), poly(dA-dT), and poly(dG-dC] were measured in water-ethanol mixtures with 0.3 mM NaCl. A conformational change from the B to the A form was observed for the natural DNAs on adding ethanol. The ethanol concentration that induces the transition and the extent of the change in the CD spectrum are different for the five natural DNAs depending on their GC contents. The higher the GC content is, the more easily the transition to the A form takes place. The results indicate that the GC content of a DNA is an important factor for induction of the B-A transition. The results for the synthetic DNAs show that their properties cannot be inferred by simple extrapolation of those of natural DNAs. Coexisting ions and the molecular weight of a DNA were also found to affect the induction of the B-A transition.