Biomedical subjects

A S Benight

Publications and source records attributed to A S Benight.

At least 37 records · Page 2Linked to original sources

PubMed1997

The question of long-range allosteric transitions in DNA.

The question of long-range allosteric transitions of DNA secondary structure and their possible involvement in transcriptional activation is discussed in the light of new results. A variety of recent evidence strongly supports a fluctuating long-range description of DNA secondary structure. Balanced equilibria between two or more different secondary structures, and the occurrence of very large domain sizes, have been documented in several instances. Long-range allosteric effects stemming from changes in sequence or secondary structure over a small region of the DNA have been observed to extend over distances up to hundreds of base pairs in some cases. The discovery that coherent bending strain beyond a threshold level in small (N < or = 250 base pairs (bp)] circular DNAs significantly alters the DNA secondary structure has important implications, especially for transcriptional activators that either bend the DNA directly or are involved in the formation of DNA loops of sufficiently small size (N < or = 250 bp). Whether the RNA polymerase is activated primarily via protein: protein contacts, as is widely believed, or instead via a bend-induced allosteric transition of the DNA in such a small loop, is now an open question. Binding of the transcriptional activator Sp1 to linear DNA induces a remarkably long-range change in its secondary structure, and catabolite activator protein binding to a supercoiled DNA behaves similarly, though possibly for different reasons. Compelling evidence for a bend-induced long-range structural transmission effect of the transcriptional activator integration host factor on RNA polymerase activity was recently reported. These results may augur a new paradigm in which allosteric transitions of duplex DNA, as well as of the proteins, are involved in the regulation of transcription.

Allosteric Site↗

PubMed1996

DNA and RNA oligomer sequences from the 3' noncoding region of the chicken glutamine synthetase gene from intramolecular hairpins.

The DNA sequence of the chicken glutamine synthetase gene contains an A.T-rich stretch of approximately 1500 base pairs in the 3' noncoding regions of exon 7 [Pu, H., & Young, A. P. (1989) Gene 18, 169-175]. Within this region several palindromic sequences occur that could conceivably form intramolecular structures. One such perfect inverted repeat sequence resides between positions 2605 and 2623. To investigate the hairpin-forming potential for this sequence, optical and calorimetric melting and gel electrophoresis studies have been performed on the following synthetically prepared DNA and RNA oligomer subsequences: DNA, 5'd-T-T-T-T-T-T-A-A-T-A-A-T-T-A-A-A-A-A-A-3'; and RNA, 5'r-U-U-U-U-U-U-A-A-U-A-A-U-U-A-A-A-A-A-A-3'. The DNA strand corresponds to the coding strand sequence while the RNA strand represents the transcribed mRNA. Results of melting analysis of these 19-base, partially self-complementary strands performed in 115 mM Na+ yielded evaluations of their thermodynamic transition parameters. These values are consistent with the melting of unimolecular structures, presumably hairpins. Thermodynamic parameters evaluated by analysis of the optical melting transitions assuming a two-state model and measured directly by differential scanning calorimetry agreed within experimental error. Therefore, melting behavior of the hairpins is all-or-none like. The DNA hairpin is slightly more stable than the RNA hairpin with melting enthalpy delta H0 = 41.2 +/- 3.8 kcal/mol and entropy delta S0 = 133 +/- 11 cal/K.mol (eu) compared to delta H0 = 32.0 +/- 6.0 kcal/mol and entropy delta S0 = 105 +/- 20 eu for the RNA. Gel electrophoretic analysis of these oligomers alone and in various mixtures with their DNA and RNA complementary strands was also performed. Consistent with interpretations of melting results, these experiments revealed both strands alone preferentially form intramolecular hairpin structures. In mixtures in which their complementary strands are in vast molar excess (stoichiometric ratios > 10:1), the intramolecular structures are converted to intermolecular duplexes. For the DNA and RNA strands examined, the conversion is not complete until over a 1000-fold excess of the complementary strand is added. Semiquantitative analysis of gel electrophoretograms enabled evaluations of the relative free energies of the hairpin and duplex states as a function of complementary strand concentration. With the finding that these sequences preferentially form hairpins, potential roles these structures could play in regulatory activities are considered.

Animals↗

PubMed1996

Isolation, characterization, and magnesium-induced self-association kinetics of discrete aggregates of RecA protein from Escherichia coli.

Dynamic and static intensity light scattering techniques were employed to identify conditions allowing preparation of homogeneous solutions of distinct oligomeric states of RecA protein. These hydrodynamically distinguishable oligomer populations of RecA protein were obtained in homogeneous pure quantities sufficient for physical studies. Results indicate two fairly narrow distributions of RecA oligomers comprised on average of 42 +/- 3 and 18 +/- 1 RecA monomers. These structures, denoted RecA42 and RecA18, respectively, could be obtained reproducibly in milligram quantities and were stable for at least one week. This enabled reliable characterizations of their hydrodynamic properties by dynamic and total intensity light scattering. These measurements revealed RecA42 had an average translational diffusion coefficient, D20(L) = 8 +/- 2 x 10(-8) cm2/s, molecular weight, M(r) = 1.6 +/- 0.1 x 10(6), and radius of gyration, RG = 465 +/- 29 A. The smaller aggregate, RecA18, had D20(S) = 20.5 +/- 2.5 x 10(-8) cm2/s, M(r) = 7.0 +/- 0.4 x 10(5), and RG = 300 +/- 20 A. Heating RecA18 at 37 degrees C overnight resulted in conversion to a species with hydrodynamic properties indistinguishable from RecA42, called RecA18/42. Conversion of RecA42 to RecA18 occurred almost instantaneously by 50% dilution at 38 degrees C or very slowly with incubation at 4 degrees C for at least 39 days. Self-association reactions of the three starting oligomeric states (RecA18, RecA42, and RecA18/42) induced by MgCl2 were monitored at several temperatures by dynamic light scattering. Results of these experiments provided evaluations of kinetic activation parameters of the self-association reactions. The activation parameters found for each starting oligomeric state of the protein were significantly different, revealing the variable influence of MgCl2 on the activation barriers to RecA self-association. Highly aggregated equilibrium solutions that ultimately form in solutions of each starting oligomeric species, incubated in MgCl2 at 38 degrees C for four days, were characterized by total intensity light scattering. Interpretations of these data in terms of characteristic behavior of random polymers suggests the surface morphologies of these highly associated equilibrium states formed from RecA42 and RecA18/42 are similar but contrast with that of RecA18. Calculated values of the translational diffusion coefficient D0 were obtained for oligomeric structures modeled as helical arrays of connected monomer spheres. Best agreement with experimentally determined diffusion coefficients required that constituent monomer spheres of RecA42 have radii 33-40% larger than the monomer spheres of RecA18. Results suggest the hydrodynamically distinct oligomeric forms of RecA may reside in conformational states with different surface exposure of hydrophobic residues, which results in substantial differences in local solvation/hydration.

Bacterial Proteins↗

PubMed1996

Studies of DNA dumbbells. VI. Analysis of optical melting curves of dumbbells with a sixteen-base pair duplex stem and end-loops of variable size and sequence.

Optical melting curves of 22 DNA dumbbells with the 16-base pair duplex sequence 5'-G-C-A-T-C-A-T-C-G-A-T-G-A-T-G-C-3' linked on both ends by single-strand loops of A, or C, sequences (iota = 2, 3, 4, 6, 8, 10, 14). T sequences (iota = 2, 3, 4, 6, 8, 10), and G iota sequences (iota = 2, 4) were measured in phosphate buffered solvents containing 30, 70, and 120 mM Na+. For dumbbells with loops comprised of at least three nucleotides, stability is inversely proportional to end-loop size. Dumbbells with loops comprised of only two nucleotide bases generally have lower stabilities than dumbbells with three base nucleotide loops. Experimental melting curves were analyzed in terms of the numerically exact (multistate) statistical thermodynamic model of DNA dumbbell melting previously described (T. M. paner, M. Amaratunga & A. S. Benight (1992), Biopolymers 32, 881). Theoretically calculated melting curves were fitted to experimental curves by simultaneously adjusting model parameters representing statistical weights of intramolecular hairpin loop and single-strand circle states. The systematically determined empirical parameters provided evaluations of the energetics of hairpin loop formation as a function of loop size, sequence, and salt environment. Values of the free energies of hairpin loop formation delta Gloop(n > iota) and single-strand circles, delta Gcir(N) as a function of end-loop size, tau = 2-14, circle size, N = 32 + 2 iota, and loop sequence were obtained. These quantities were found to depend on end-loop size but not loop sequence. Their empirically determined values also varied with solvent ionic strength. Analytical expressions for the partition function Q(T) of the dumbbells were evaluated using the empirically evaluated best-fit loop parameters. From Q(T), the melting transition enthalpy delta H, entropy delta S, and free energy delta G, were evaluated for the dumbbells as a function of end-loop size, sequence, and [Na+]. Since the multistate analysis is based on the numerically exact model, and considers a statistically significant number of theoretically possible partially melted states, it does not require prior assumptions regarding the nature of the melting transition, i.e., whether or not it occurs in a two-state manner. For comparison with the multistate analysis, thermodynamic transition parameters were also evaluated directly from experimental melting curves assuming a two-state transition and using the graphical van't Hoff analysis. Comparisons between results of the multistate and two-state analyses suggested dumbbells with loops comprised of six or fewer residues melted in a two-state manner, while the melting processes for dumbbells with larger end-loops deviate from two-state behavior. Dependence of thermodynamic transition parameters on [Na+] as a function of loop size suggests single-strand end-loops have different counterion binding properties than the melted circle. Results are compared with those obtained in an earlier study of dumbbells with the slightly different stem sequence 5'-G-C-A-T-A-G-A-T-G-A-G-A-A-T-G-C-3' linked on the ends by T iota loops (iota = 2, 3, 4, 6, 8, 10, 14).

Base Composition↗

PubMed1993

Tetramethylammonium does not universally neutralize sequence dependent DNA stability.

Effects of different concentrations of Tetramethylammonium on the thermostability of six DNA dumbbells with similar well defined sequences have been investigated. Each molecule has a 16 base pair duplex stem linked on both ends by T4 single strand loops. Only the sequence of the four central base pairs distinguishes one molecule from the next. The distinguishing central sequences are, [A-T-A-T], [T-A-T-A], [A-A-A-A], [C-G-C-G], [G-C-G-C] and [G-G-G-G] situated between the sequences: 5'-G-T-A-T-C-C-[]-G-G-A-T-A-C-3' which are the same in all molecules. Optical melting curves collected on these molecules as a function of TMA concentration over the range from 0.09 M to 4.5 M revealed there is no single concentration of TMA where all these molecules exhibit the same melting temperature.

Base Sequence↗

PubMed1993

Sequence dependence of the free energy of B-Z junction formation in deoxyoligonucleotides.

The NaCl-induced transition from the right-handed B form to a hybrid form containing both left and right-handed DNA, joined by a B-Z junction, was investigated. Transition curves were constructed from circular dichroism spectra collected as a function of NaCl concentration for a series of 16 bp deoxyoligonucleotides. The sequence of the series (one strand of the duplex) was: 5'CGCGCGCGAMNGACTG, where C indicates m5dC, and -MN- was varied to include the possible Py:Py stacks: -CC-, -CT-, -TC- and -TT-. Transition curves for the conversion of all deoxyoligonucleotides were found to be biphasic. Singular value decomposition was used to analyze the experimental circular dichroism spectra obtained as a function of NaCl, and showed that the transition was not a simple two-state process, but rather required at least three species to account for the experimental data. A sequential three-state model, B<-->I<-->BZ, was derived and applied to analyze experimental transition curves. Non-linear least-squares analysis was used to evaluate the salt-dependent equilibrium constants for each step in the sequential reaction model. The results indicate that the free energy change for B-Z junction formation (delta Gj) depends on the dinucleotide sequence near the junction. At a Na activity of 5, delta Gj values ranging from +1.2 to +1.7 kcal mol-1 were determined, depending on the sequence near the junction. delta Gj was found to be strongly dependent on salt concentration, with its magnitude decreasing with increasing Na activity. In addition to studies on linear duplex molecules, the B to BZ transition was also investigated in "dumbbell" forms of selected sequences. In these molecules, the ends were covalently linked by a single-stranded T4 segment. These studies show that junction formation is energetically more costly in dumbbells than in their linear counterparts. A striking correlation was found between delta Gj and two independent conformational properties of the dinucleotide steps that were introduced into the linear duplex molecules. These are the free energy of unstacking and the estimated free energy change for the conversion of the dinucleotide from the B to the A conformation. The more stable against unstacking, or the more resistant to the B to A conversion, the sequence near the junction site is, the more costly is B-Z junction formation. These correlations reveal that the DNA sequence near the junction apparently must be pliable in order to accommodate the unusual structure of the junction.(ABSTRACT TRUNCATED AT 400 WORDS)

Base Composition↗

PubMed1993

Studies of DNA dumbbells. IV. Preparation and melting of a DNA dumbbell with the 16 base-pair sequence 5'G-T-A-T-C-C-C-T-C-T-G-G-A-T-A-C3' linked on the ends by dodecyl chains.

The preparation and melting of a 16 base-pair duplex DNA linked on both ends by C12H24 (dodecyl) chains is described. Absorbance vs temperature curves (optical melting curves) were measured for the dodecyl-linked molecule and the same duplex molecule linked on the ends instead by T4 loops. Optical melting curves of both molecules were measured in 25, 55, and 85 mM Na+ and revealed, regardless of [Na+], the duplex linked by dodecyl loops is more stable by at least 6 degrees C than the same duplex linked by T4 loops. Experimental curves in each salt environment were analyzed in terms of the two-state and multistate theoretical models. In the two-state, or van't Hoff analysis, the melting transition is assumed to occur in an all-or-none manner. Thus, the only possible states accessible to the molecule throughout the melting transition are the completely intact duplex and the completely melted duplex or minicircle. In the multistate analysis no assumptions regarding the melting transition are required and the statistical occurrence of every possible partially melted state of the duplex is explicitly considered. Results of the analysis revealed the melting transitions of both the dodecyl-linked molecule and the dumbbell with T4 end loops are essentially two state in 25 and 55 mM Na+. In contrast, significant deviations from two-state behavior were observed in 85 mM Na+. From our previously published melting data of DNA dumbbells with Tn end loops where n = 2, 3, 4, 6, 8, 10, 14 [T. M. Paner, M. Amaratunga, and A. S. Benight, (1992) Biopolymers, Vol. 32, pp. 881-892] and the dumbbell with T4 end loops of this study, a plot of d(Tm)/d ln [Na+] was constructed. Extrapolation of this data to n = 1 intersects with the value of d (Tm)/d ln [Na+] obtained for the alkyl-linked dumbbell, suggesting the salt-dependent stability of the alkyl-linked molecule behaves as though the duplex of this molecule were linked by end loops comprised of a single T residue.

Base Sequence↗

PubMed1993

Studies of DNA dumbbells. V. A DNA triplex formed between a 28 base-pair DNA dumbbell substrate and a 16 base linear single strand.

CD spectra and melting curves were collected for a 28 base-pair DNA fragment in the form of a DNA dumbbell (linked on both ends by T4 single-strand loops) and the same DNA sequence in the linear form (without end loops). The central 16 base pairs (bp) of the 28-bp duplex region is the poly(pu) sequence: 5'-AGGAAGGAGGAAAGAG-3'. Mixtures of the dumbbell and linear DNAs with the 16-base single-strand sequence 5'-TCCTTCCTCCTTTCTC-3' were also prepared and studied. At 22 degrees C, CD measurements of the mixtures in 950 mM NaCl, 10 mM sodium acetate, 1 mM EDTA, pH 5.5, at a duplex concentration of 1.8 microM, provided evidence for triplex formation. Spectroscopic features of the triplexes formed with either a dumbbell or linear substrate were quite similar. Melting curves of the duplex molecules alone and in mixtures with the third strand were collected as a function of duplex concentration from 0.16 to 2.15 microM. Melting curves of the dumbbell alone and mixtures with the third strand were entirely independent of DNA concentration. In contrast, melting curves of the linear duplex alone or mixed with the third strand were concentration dependent. At identical duplex concentrations, the dumbbell alone melts approximately 20 degrees C higher than the linear duplex. The curve of the linear duplex displayed a significant pretransition probably due to end fraying. On melting curves of mixtures of the dumbbell or linear duplex with the third strand, a low temperature transition with much lower relative hyperchromicity change (approximately 5%) was observed. This transition was attributed to the melting of a new molecular species, e.g., the triplex formed between the duplex and single-strand DNA molecules. In the case of the dumbbell/single-strand mixture, these melting transitions of the triplex and the dumbbell were entirely resolvable. In contrast, the melting transitions of the linear duplex and the triplex overlapped, thereby preventing their clear distinction. To analyze the data, a three-state equilibrium model is presented. The analysis utilizes differences in relative absorbance vs temperature curves of dumbbells (or linear molecules) alone and in mixtures with the third strand.(ABSTRACT TRUNCATED AT 400 WORDS)

Base Sequence↗

PubMed1992

Dynamic light scattering investigations of human erythrocyte spectrin.

Dynamic light scattering measurements were performed on spectrin from human erythrocytes in 25 mM Tris buffer at pH 7.6 with 100 mM NaCl and 5 mM EDTA. Measurements were made on spectrin solutions prepared as dimers and tetramers over the temperature range from 23 to 41 degrees C, as a function of the square of the scattering vector (K2) over the range of 0.7 x 10(10) cm-2 less than or equal to K1 less than or equal to 20 x 10(10) cm-2. Analysis of the autocorrelation functions collected for these solutions revealed the presence of two predominant motional components over the entire range of K2. Plots of the diffusion coefficients (D20) of these components, with viscosity and temperature corrected to water at 20 degrees C, as a function of K2 indicated three rather distinct regions, flat regions at low and high K2 joined by a sloping intermediate region. At small K2 (less than or equal to 4 x 10(10) cm-2) the D20 values were (7.3 +/- 2.0) x 10(-8) cm2/s for the slow component and (20.3 +/- 2.0) x 10(-8) cm2/s for the fast component. At large K2 (greater than or equal to 10 x 10(10) cm-2) the values increased to (13.0 +/- 2.0) x 10(-8) cm2/s for the slow component and (39.4 +/- 2.0) x 10(-8) cm2/s for the fast component. In the intermediate K2 region, D20 is a linear function of K2 and appears as a transition between the low and high K2 regions.(ABSTRACT TRUNCATED AT 250 WORDS)

Diffusion↗

PubMed1992

A semi-micromethod for the determination of the extinction coefficients of duplex and single-stranded DNA.

We have developed a rapid and convenient procedure for the determination of concentrations and extinction coefficients of oligo- and polynucleotides. It offers significant advantages over other methods in terms of precision and the ability to detect artifactual or erroneous results. Samples are first completely digested with appropriate enzymes to mononucleotides and nucleosides. Using the multicomponent linear regression capabilities of commonly available spreadsheet programs, the absorbance spectrum of the digest can be analyzed as a linear combination of the contribution of the possible constituent monomers. If all the spectral components present have been included, the analysis yields the concentration of each of the monomer species whose sum is the concentration (in monomer units) of the original undigested sample. When combined with the predigest absorbance spectrum, the extinction coefficients of the intact sample can then be calculated. The analysis also yields the fractional base composition of the oligomer or polymer. The extensive spectral data provided by digital read-outs of modern spectrophotometers permit the application of sensitive tests of the goodness of fit, thus facilitating the detection of artifacts and sample inhomogeneity. Both single-strand and duplex structures can be analyzed comfortably in sample sizes of 25 to 35 nmol (total) of mononucleotides with a precision of 1%. The concentrations obtained by this method agree, on the average, within 0.2% with those determined by phosphate analysis of the same sample. The method also yields the base composition with an accuracy of ca. 5% for high-molecular-weight polymers and 2% for short oligomers (15-20 bp) when compared to the predicted values.

Base Composition↗

PubMed1992

Studies of DNA dumbbells. I. Melting curves of 17 DNA dumbbells with different duplex stem sequences linked by T4 endloops: evaluation of the nearest-neighbor stacking interactions in DNA.

Seventeen DNA dumbbells were constructed that have duplex sequences ranging in length from 14 to 18 base pairs linked on the ends by T4 single-strand loops. Fifteen of the molecules have the core duplexes with the sequences 5'G-T-A-T-C-C-(W-X-Y-Z)-G-G-A-T-A-C3', where (W-X-Y-Z) represents a unique combination of A.T, T.A, G.C, and C.G base pairs. The remaining two molecules have the central sequence (W-X-Y-Z) = A-C and A-C-A-C-A-C. These duplex sequences were designed such that the central sequences include different combinations of the 10 possible nearest-neighbor (n-n) stacks in DNA. In this sense the set of molecules is complete and serves as a model system for evaluating sequence-dependent local stability of DNA. Optical melting curves of the samples were collected in 25, 55, 85, and 115 mM [Na+], and showed, regardless of solvent ionic strength, that the transition temperatures of the dumbbells vary by as much as 14 degrees for different molecules of the set. Results of melting experiments analyzed in terms of a n-n sequence-dependent model allowed evaluation of nine independent linear combinations of the n-n stacking interactions in DNA as a function of solvent ionic strength. Although there are in principle 10 possible different n-n interactions in DNA, these 10 are not linearly independent and therefore can not be uniquely determined. For molecules with ends, there are 9 linearly independent combinations, as opposed to circular or semiinfinite repeating copolymers where only 8 linear combinations of the 10 possible n-n interactions are linearly independent. The n-n interactions are presented as combinations of the deviations from average stacking for the 5'-3' base-pair doublets, delta Gi, and reveal several interesting features: (1) Titratable changes in the values of delta Gi with changing salt environment are observed. In all salts the most stable unique combination is delta G4 = (delta GGpC+delta GCpG)/2, and the least stable is the GpG/CpC stack, delta G2 = delta GGpG/CpC. (2) The chi 2 values of the fits of the evaluated delta Gi's to experimental data increased with decreasing [Na+], suggesting that significant interactions beyond nearest neighbors become more pronounced, particularly at 25 nM Na+.(ABSTRACT TRUNCATED AT 400 WORDS)

Base Sequence↗

PubMed1992

Studies of DNA dumbbells. II. Construction and characterization of DNA dumbbells with a 16 base-pair duplex stem and Tn end loops (n = 2, 3, 4, 6, 8, 10, 14).

The preparation and characterization of DNA dumbbells that contain the 16 base-pair duplex sequences 5'G-C-A-T-A-G-A-T-G-A-G-A-A-T-G-C3' (set 1) and 5'G-C-A-T-C-A-T-C-G-A-T-G-A-T-G-C3' (set 2) are reported. The dumbbells of set 1 have the duplex stem nucleated on both ends by Tn (n = 2, 3, 4, 6, 8, 10, and 14) loops. The dumbbells of set 2 have Tn (n = 2, 4, 8, 10) end loops. For the molecules of set 1, effects of end loop size on the electrophoretic mobility, CD and UV absorbance spectra, and cleavage by restriction enzymes, were investigated. Effects of loop size on the CD spectra and restriction enzyme cleavage of the molecules of set 2 were also examined. Optical melting curves of the molecules of set 1 were collected as a function of sodium ion concentration from 30 to 120 mM. These investigations revealed that as loop size decreases, the electrophoretic mobilities, rates of enzyme cleavage, and optical melting temperatures increase. For end loops with at least three T's the observed increases are inversely proportional to loop size. The behavior of the dumbbell with T2 end loops departs from this linear dependence and is anomalous in every experimental context. For molecules with end loops comprised of at least four T's CD spectra were virtually indistinguishable. However, these spectra differed considerably from the CD spectrum of the T2-looped molecule. The CD spectrum of the dumbbell with T3 end loops displayed features common to the dumbbells with larger loops and T2 end loops. Thermodynamic evidence that the terminal G.C base pairs (bps) nucleating the T2 end loops were intact was obtained from a comparison of the melting temperature of this molecule with that of a DNA dumbbell containing the 14 central bps of the set 1 duplex sequence linked instead by end loops comprised of the four base sequence, C-T-T-C. The tm of this latter molecule was determined to be 9 degrees C less than that of the former dumbbell assumed to contain a 16-bp stem and T2 end loops.(ABSTRACT TRUNCATED AT 400 WORDS)

Base Composition↗

PubMed1992

Studies of DNA dumbbells. III. Theoretical analysis of optical melting curves of dumbbells with a 16 base-pair duplex stem and Tn end loops (n = 2, 3, 4, 6, 8, 10, 14).

Optical melting curves of seven DNA dumbbells with the 16 base-pair duplex sequence 5'G-C-A-T-A-G-A-T-G-A-G-A-A-T-G-C3' linked on both ends by Tn (n = 2, 3, 4, 6, 8, 10, and 14) loops measured in 30, 70, and 120 mM Na+ are analyzed in terms of the numerically exact statistical thermodynamic model of DNA melting. The construction and characterization of these molecules were described in the previous paper (Amaratunga et al., 1992). As was recently reported for hairpins (T. M. Paner, M. Amaratunga, M. J. Doktycz, and A. S. Benight, 1990, Biopolymers, Vol. 29, pp. 1715-1734) theoretically calculated melting curves were fitted to experimental curves by simultaneously adjusting the parameters representing loop and circle formation to optimize the fits. The systematically determined empirical parameters provide evaluations of the free energies of hairpin loop formation delta Gloop (n) and single-strand circles delta Gcircle (N), as a function of end loop size, n = 2-14, and circle size, N = 32 + 2n. The dependence of these quantities on solvent ionic strength over the range from 30 to 120 mM Na+ was evaluated. An approximately analytical expression for the partition function Q(T) of the dumbbells was formulated that allowed a means for determining the transition enthalpy delta H degrees and entropy delta S degrees for every dumbbell, revealing the dependence of these quantities on loop size. In this multistate approach a manifold of partially melted intermediate microstates are considered and therefore no assumptions regarding the nature of the melting transitions (that they are two-state) are required. The transition thermodynamic parameters were also determined from a van't Hoff analysis of the melting curves. Comparisons between the results of the multistate analysis and the two-state van't Hoff analysis revealed significant differences for the dumbbells with larger end loops, indicating that the melting transitions of the larger looped dumbbells deviate considerably from two-state behavior. Results are then compared with published melting studies of much larger DNA dumbbells (D. B. Naritsin and Y. L. Lyubchenko, 1990, Journal of Biomolecular Structure and Dynamics, Vol. 8, pp. 1-13), of small hairpins (Paner et al., 1990; M. J. Doktycz, T. M. Paner, M. Amaratunga and A. S. Benight, 1990, Biopolymers, Vol. 30, pp. 829-845) and another dumbbell (A. S. Benight, J. M. Schurr, P. F. Flynn, B. R. Reid, and D. E. Wemmer, 1988) Journal of Molecular Biology, Vol. 200, pp. 377-399).(ABSTRACT TRUNCATED AT 400 WORDS)

Base Composition↗

PubMed1992

How many numbers are required to specify sequence-dependent properties of polynucleotides?

There are 10 unique dinucleotides of double-stranded DNA, but only 8 independent nearest-neighbor energies that occur in circular DNA, as shown by D. M. Gray and I. Tinoco [(1970) Biopolymers 9, 223-244]. We extend that analysis to include end effects, and show that the number of unique dinucleotide pairs (including ends) is 14, but there are only 12 independent energies. We discuss how these 12 energies (or spectra or any other pairwise additive property) can be measured and displayed, and how they should and should not be compared between experimenters. As an example, we analyzed the recently reported melting curves [M.J. Doktycz et al. (1992) Biopolymers, 32, 849-864.] of 16 DNA dumbbells in two different Na+ environments. This analysis reveals a new means for evaluating end effects and the emergence of longer than nearest-neighbor interactions at low salt concentration.

Base Composition↗

PubMed1990

Kinetic analysis of the pre-equilibrium steps in the self-assembly of RecA protein from Escherichia coli.

Total intensity light scattering is employed to investigate the self-assembly kinetics of RecA protein. Reaction conditions are employed where the kinetics of self-assembly are slow enough to yield reliable scattered intensity measurements over the range of scattering angles from 40 to 130 degrees as a function of time. From these measurements the time-dependent behavior of the weight average molecular weight, Mr, and radius of gyration, RG, of the associating protein species as a function of [MgCl2], [NaCl], [RecA], and pH was determined. The temperature dependence of RecA self-assembly was also investigated and allowed an evaluation of the activation thermodynamic parameters of association. Results reveal RecA self-assembly is bi-phasic under all conditions examined. The first phase, referred to as "filamentation" is second-order in [RecA] and occurs via a quasi linear condensation scheme with an Arrhenius activation energy of 88.6 kcal/mol. Filamentation assembly involves the uptake of one proton, one MgCl2, the release of five to six NaCls, and is driven by the release of approximately 70 water molecules. The evaluated activation parameters of the first kinetic phase are consistent with the proposition that linear self-assembly of RecA protein into ordered filaments is entropically driven. The second kinetic phase, referred to as "bundling" is greater than second-order in both [RecA] and [MgCl2], is considerably slower that filamentation assembly, and is apparently initiated by 2nd order collisions of linear filaments.

Escherichia coli↗

PubMed1990

Energetics of B-Z junction formation in a sixteen base-pair duplex DNA.

We report analysis of the NaCl-induced B-Z transition in a 16 base-pair duplex DNA with sequence designed such that when NaCl is increased the left half of the molecule undergoes the B-Z transition while the right half remains in the B-form. An equilibrium thermodynamic model based on the body of available published experimental data and the recent theoretical work of Soumpasis, which indicate, in the salt range above approximately 0.9 M-NaCl, the transition free-energy of B-Z conversion in DNA is a linear function of the NaCl concentration, is employed. Analysis of the B-Z transition of the junction-containing molecule indicates the B-Z junction formed in this 16 base-pair DNA is composed of approximately three base-pairs and has a free energy of formation of approximately 4.7 kcal/mol junction. These values for the junction are in excellent agreement with published estimates of B-Z junction size and energy derived from much longer DNA pieces.

Base Sequence↗

PubMed1990

B to Z transitions of the short DNA hairpins formed from the oligomer sequences: d[(CG)3X4(CG)3] (X = A, T, G, C).

Circular Dichroism (CD) spectra were collected as a function of sodium perchlorate concentration [NaClO4] for the set of DNA hairpins formed from the oligomer sequences d[(CG)3X4(CG)3] where X = A, T, G or C. Over the range in salt concentration from 0 to 4.0 M NaClO4, the CD spectra invert in a manner characteristic of the B to Z transition. A factor analysis routine is described and employed to determine the least number of basis spectra required to fit the measured spectra of each hairpin over the entire salt range examined. In every case, linear combinations of only two sub-spectra fit the experimental spectra of the hairpins with greater than 98% accuracy, indicating the spectrally monitored structural transitions are two-state. From the relative weights of the individual sub-spectra, B-Z transition curves are constructed. The transitions are analyzed in terms of a simple two-state equilibrium model which yields an evaluation of the transition free-energy, delta GB-Z, as a function of NaClO4 concentration. At 1.0 M NaClO4 and 21 degrees C, delta GB-Z = 5.4, 4.9, 3.6 and 2.3 kcal/mole for the G4, T4, A4 and C4 loop hairpins, respectively.

Base Sequence↗

PubMed1990

Structure and dynamics of M13mp19 circular single-strand DNA: effects of ionic strength.

Dynamic and static light scattering, CD, and optical melting experiments have been conducted on M13mp19 viral circular single-strand DNA as a function of NaCl concentration. Over the 10,000-fold range in concentration from 100 microM to 1.0 M NaCl, the melting curves and CD spectra indicate an increase in base stacking and stability of stacked regions with increased salt concentration. Analysis of dynamic light scattering measurements of the single-strand DNA solutions as a function of K2 from 1.56 to 20 X 10(10) cm-2 indicates the collected autocorrelation functions are biexponential, thus revealing the presence of two decaying dynamic components. These components are taken to correspond to (1) global translational motions of the molecular center of mass and (2) motions of the internal molecular subunits. From the evaluated relaxation rates of these components, diffusion coefficients D0 and Dplat are determined. The center of mass translational diffusion coefficient D0, varies in a nonmonotonic manner, by 10%, from 3.75 X 10(-8) to 3.39 X 10(-8) cm2/s over the NaCl concentration range from 100 microM to 1.0 M. Likewise, the radius of gyration RG, obtained from static light scattering experiments, varies by 15% from 699 to 830 A over the same NaCl range Dplat, the diffusion coefficient of the internal subunits, displays a different dependence on the NaCl concentration and decreases, by nearly 22% in a titratable fashion, from 12.46 X 10(-8) to 10.26 X 10(-8) cm2/s, when the salt is increased from 100 microM to 1.0 M. A semiquantitative interpretation of these results is provided by analysis of the light scattering data in terms of the circular Rouse-Zimm chain. Rouse-Zimm model parameters are estimated from the experimental results, assuming the circular chains are composed of a fixed number of Gaussian segments, N + 1 = 15. The rms displacement of the internal segments, b, is estimated to be the smallest (442 A) in 100 mM NaCl. Increases of b to 467 A in 100 microM and 524 A in 1.0 M NaCl are observed. Meanwhile, the hypothetical friction factor of the internal subunits, f, progressively increases as the NaCl concentration is raised. It is inferred from the evaluated Rouse-Zimm model parameters that both the static flexibility of the circular chain and diffusive displacements of the internal subunits decrease with increases in NaCl concentration from 100 mM to 1.0 M.(ABSTRACT TRUNCATED AT 400 WORDS)

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