Effects of site-specific substitution of 5-fluorouridine on the stabilities of duplex DNA and RNA.

The effects of 5-fluorouridine (FUrd) and 5-fluorodeoxyuridine (FdUrd) substitution on the stabilities of duplex RNA and DNA have been studied to determine how FUrd substitution in nucleic acids may alter the efficiency of biochemical processes that require complementary base pairing for molecular recognition. The parent sequence, 5'-GCGAAUUCGC, contains two non-equivalent uridines. Eight oligonucleotides (four RNA and four DNA) were prepared with either zero, one or two Urd substituted by FUrd. The stability of each self-complementary duplex was determined by measuring the absorbance at 260 nm as a function of temperature. Tm values were calculated from the first derivative of the absorbance versus temperature profiles and values for delta H0 and delta S0 were calculated from the concentration dependence of the Tm. Individual absorbance versus temperature curves were also analyzed by a parametric approach to calculate thermodynamic parameters for the duplex to single-stranded transition. Analysis of the thermodynamic parameters for each oligonucleotide revealed that FUrd substitution had sequence-dependent effects in both A-form RNA and B-form DNA duplexes. Conservation of helix geometry in FUrd-substituted duplexes was determined by CD spectroscopy. FUrd substitution at a single site in RNA stabilized the duplex (delta delta G37 = 0.8 kcal/mol), largely due to more favorable stacking interactions. FdUrd substitution at a single site in DNA destabilized the duplex (delta delta G37 = 0.3 kcal/mol) as a consequence of less favorable stacking interactions. All duplexes melt via single cooperative transitions.     

Thermodynamics of ribonuclease T1 denaturation.

Differential scanning calorimetry has been used to investigate the thermodynamics of denaturation of ribonuclease T1 as a function of pH over the pH range 2-10, and as a function of NaCl and MgCl2 concentration. At pH 7 in 30 mM PIPES buffer, the thermodynamic parameters are as follows: melting temperature, T1/2 = 48.9 +/- 0.1 degrees C; enthalpy change, delta H = 95.5 +/- 0.9 kcal mol-1; heat capacity change, delta Cp = 1.59 kcal mol-1 K-1; free energy change at 25 degrees C, delta G degrees (25 degrees C) = 5.6 kcal mol-1. Both T1/2 = 56.5 degrees C and delta H = 106.1 kcal mol-1 are maximal near pH 5. The conformational stability of ribonuclease T1 is increased by 3.0 kcal/mol in the presence of 0.6 M NaCl or 0.3 M MgCl2. This stabilization results mainly from the preferential binding of cations to the folded conformation of the protein. The estimates of the conformational stability of ribonuclease T1 from differential scanning calorimetry are shown to be in remarkably good agreement with estimates derived from an analysis of urea denaturation curves.     

Nearest-neighbor thermodynamics and NMR of DNA sequences with internal A.A, C.C, G.G, and T.T mismatches

Thermodynamic measurements are reported for 51 DNA duplexes with A.A, C.C, G.G, and T.T single mismatches in all possible Watson-Crick contexts. These measurements were used to test the applicability of the nearest-neighbor model and to calculate the 16 unique nearest-neighbor parameters for the 4 single like with like base mismatches next to a Watson-Crick pair. The observed trend in stabilities of mismatches at 37 degrees C is G.G > T.T approximately A.A > C.C. The observed stability trend for the closing Watson-Crick pair on the 5' side of the mismatch is G.C >/= C.G >/= A.T >/= T.A. The mismatch contribution to duplex stability ranges from -2.22 kcal/mol for GGC.GGC to +2.66 kcal/mol for ACT.ACT. The mismatch nearest-neighbor parameters predict the measured thermodynamics with average deviations of DeltaG degrees 37 = 3.3%, DeltaH degrees = 7. 4%, DeltaS degrees = 8.1%, and TM = 1.1 degrees C. The imino proton region of 1-D NMR spectra shows that G.G and T.T mismatches form hydrogen-bonded structures that vary depending on the Watson-Crick context. The data reported here combined with our previous work provide for the first time a complete set of thermodynamic parameters for molecular recognition of DNA by DNA with or without single internal mismatches. The results are useful for primer design and understanding the mechanism of triplet repeat diseases.     

Thermodynamics of RNA duplexes with tandem mismatches containing a uracil-uracil pair flanked by C.G/G.C or G.C/A.U closing base pairs

The thermodynamics governing the denaturation of RNA duplexes containing 8 bp and a central tandem mismatch or 10 bp were evaluated using UV absorbance melting curves. Each of the eight tandem mismatches that were examined had one U-U pair adjacent to another noncanonical base pair. They were examined in two different RNA duplex environments, one with the tandem mismatch closed by G.C base pairs and the other with G.C and A.U closing base pairs. The free energy increments (Delta Gdegrees(loop)) of the 2 x 2 loops were positive, and showed relatively small differences between the two closing base pair environments. Assuming temperature-independent enthalpy changes for the transitions, (Delta Gdegrees(loop)) for the 2 x 2 loops varied from 0.9 to 1.9 kcal/mol in 1 M Na(+) at 37 degrees C. Most values were within 0.8 kcal/mol of previously estimated values; however, a few sequences differed by 1.2-2.0 kcal/mol. Single strands employed to form the RNA duplexes exhibited small noncooperative absorbance increases with temperature or transitions indicative of partial self-complementary duplexes. One strand formed a partial self-complementary duplex that was more stable than the tandem mismatch duplexes it formed. Transitions of the RNA duplexes were analyzed using equations that included the coupled equilibrium of self-complementary duplex and non-self-complementary duplex denaturation. The average heat capacity change (DeltaC(p)) associated with the transitions of two RNA duplexes was estimated by plotting DeltaH degrees and DeltaS degrees evaluated at different strand concentrations as a function of T(m) and ln T(m), respectively. The average DeltaC(p) was 70 +/- 5 cal K(-)(1) (mol of base pairs)(-)(1). Consideration of this heat capacity change reduced the free energy of formation at 37 degrees C of the 10 bp control RNA duplexes by 0.3-0.6 kcal/mol, which may increase Delta Gdegrees(loop) values by similar amounts.     

The first example of a Hoogsteen base-paired DNA duplex in dynamic equilibrium with a Watson-Crick base-paired duplex--a structural (NMR), kinetic and thermodynamic study.

A single-point substitution of the O4' oxygen by a CH2 group at the sugar residue of A6 (i.e. 2'-deoxyaristeromycin moiety) in a self-complementary DNA duplex, 5'-d(C1G2C3G4A5A6T7T8C9G10C11G12)2(-3), has been shown to steer the fully Watson-Crick basepaired DNA duplex (1A), akin to the native counterpart, to a doubly A6:T7 Hoogsteen basepaired (1B) B-type DNA duplex, resulting in a dynamic equilibrium of (1A)<==>(1B): Keq = k1/k(-1) = 0.56+/-0.08. The dynamic conversion of the fully Watson-Crick basepaired (1A) to the partly Hoogsteen basepaired (1B) structure is marginally kinetically and thermodynamically disfavoured [k1 (298K) = 3.9 0.8 sec(-1); deltaHdegrees++ = 164+/-14 kJ/mol; -TdeltaS degrees++ (298K) = -92 kJ/mol giving a deltaG degrees++ 298 of 72 kJ/mol. Ea (k1) = 167 14 kJ/mol] compared to the reverse conversion of the Hoogsteen (1B) to the Watson-Crick (1A) structure [k-1 (298K) = 7.0 0.6 sec-1, deltaH degrees++ = 153 13 kJ/mol; -TdeltaSdegrees++ (298K) = -82 kJ/mol giving a deltaGdegrees++(298) of 71 kJ/mol. Ea (k-1) = 155 13 kJ/mol]. Acomparison of deltaGdegrees++(298) of the forward (k1) and backward (k-1) conversions, (1A)<==>(1B), shows that there is ca 1 kJ/mol preference for the Watson-Crick (1A) over the double Hoogsteen basepaired (1B) DNA duplex, thus giving an equilibrium ratio of almost 2:1 in favour of the fully Watson-Crick basepaired duplex. The chemical environments of the two interconverting DNA duplexes are very different as evident from their widely separated sets of chemical shifts connected by temperature-dependent exchange peaks in the NOESY and ROESY spectra. The fully Watson-Crick basepaired structure (1A) is based on a total of 127 intra, 97 inter and 17 cross-strand distance constraints per strand, whereas the double A6:T7 Hoogsteen basepaired (1B) structure is based on 114 intra, 92 inter and 15 cross-strand distance constraints, giving an average of 22 and 20 NOE distance constraints per residue and strand, respectively. In addition, 55 NMR-derived backbone dihedral constraints per strand were used for both structures. The main effect of the Hoogsteen basepairs in (1B) on the overall structure is a narrowing of the minor groove and a corresponding widening of the major groove. The Hoogsteen basepairing at the central A6:T7 basepairs in (1B) has enforced a syn conformation on the glycosyl torsion of the 2'-deoxyaristeromycin moiety, A6, as a result of substitution of the endocyclic 4'-oxygen in the natural sugar with a methylene group in A6. A comparison of the Watson-Crick basepaired duplex (1A) to the Hoogsteen basepaired duplex (1B) shows that only a few changes, mainly in alpha, sigma and gamma torsions, in the sugar-phosphate backbone seem to be necessary to accommodate the Hoogsteen basepair.     

The conformational study of two carbocyclic nucleosides: why carbocyclic nucleic acids (CarNAs) form more stable duplexes with RNA than DNA does

Replacement of the furanose moiety of DNA with a cyclopentane ring produces a modified sugar analogue: Carbocyclic nucleic acid (CarNA). UV melting-temperature experiments demonstrate that the incorporation of 2'-deoxycarbaguanosine ((c)G) and 2'-deoxyaristeromycin ((c)A) of carbocyclic nucleosides into a DNA strand increases the stability of the CarNA/RNA hybrid. Circular Dichroism (CD) study indicates that the CarNA/RNA hybrid adopts an A-like conformation. To elucidate the molecular basis of the increased stability of the CarNA/RNA, the conformation of (c)G and (c)A were examined by (1)H NMR conformational analysis of (3)J(HH) coupling constants and ab initio molecular orbital (MO) calculations. These results show that the populations of N-type of (c)G and (c)A are higher than those of dG and dA, respectively, at different temperatures [For example, 37% (N%) of (c)G vs. 28%of dG, 36% (N%) of (c)A vs. 25% of dA at 278 K], which suggest that the cyclopentane rings of (c)G and (c)A prefer the N-type conformation in two-state N-S pseudorotional equilibrium in comparison with the furanose rings of dG and dA. The DeltaH degrees of (c)G (DeltaH degrees = - 0.43 kcal mol(-1)) and (c)A (DeltaH degrees = - 0.41kcal mol(-1)) are lower than that of dG (dG = - 1.8 kcal mol(-1)) and dA (dA = - 1.0 kcal mol(-1)), respectively, which suggest that the gauche effect in the (c)A and (c)G driving N-S pseudorotional equilibrium to S-type is reduced by replacement of the 4'-oxygen by a CH(2) group. These results suggest that the preferred N-type of the (c)G and (c)A leads to the A-like conformation, which contributes to the stability of CarNA/RNA hybrid.     

Spectroscopic and calorimetric investigation on the DNA triplex formed by d(CTCTTCTTTCTTTTCTTTCTTCTC) and d(GAGAAGAAAGA) at acidic pH.

The equimolar mixture of d(CTCTTCTTTCTTTTCTTTCTTCTC) (dY24) and d(GAGAAGAAAGA) (dR11) [designated (dY24).(dR11)], forms at pH = 5 a DNA triplex, which mimicks the H-DNA structure. The DNA triplex was identified by the following criteria: (i) dY24 and dR11 co-migrate in a poly-acrylamide gel, with a mobility and a retardation coefficient comparable to those observed for an 11-triad DNA triplex, previously characterized in our laboratories (1); (ii) the intercalator ethidium bromide shows a poor affinity for (dR11).(dY24) at pH = 5, and a high affinity at pH = 8; (iii) the (dR11).(dY24) mixture is not a substrate for DNase I at pH = 5; (iv) the CD spectrum of (dR11).(dY24), at pH = 5, is consistent with those previously reported for triple-stranded DNA. The (dR11).(dY24) mixture exhibits a thermally induced co-operative transition, which appears to be monophasic, reversible and concentration dependent. This transition is attributed to the disruption of the DNA triplex into single strands. The enthalpy change of the triplex-coil transition was measured by DSC (delta Hcal = 129 +/- 6 kcal/mol) and, assuming a two-state model, by analysis of UV-denaturation curves (average of two methods delta HUV = 137 +/- 13 kcal/mol). Subtracting from delta Hcal of triplex formation the contributions due to the Watson-Crick helix and to the protonation of the C-residues, we found that each pyrimidine binding into the major groove of the duplex, through a Hoogsteen base pair, is accompanied by an average delta H = -5.8 +/- 0.6 kcal/mol. The effect on the stability of the (dR11).(dY24) triplex due to the substitution of a T:A:T triad with a T:T:T one was also investigated.     

Expression, purification, and characterization of a recombinant ribonuclease H from Thermus thermophilus HB8.

Thermus thermophilus ribonuclease H was overexpressed and purified from Escherichia coli. The determination of the complete amino acid sequence allowed modification of that predicted from the DNA sequence, and the enzyme was shown to be composed of 166 amino acid residues with a molecular weight of 18,279. The isoelectric point of the enzyme was 10.5, and the specific absorption coefficient A0.1%(280) was 1.69. The enzymatic and physicochemical properties as well as the thermal and conformational stabilities of the enzyme were compared with those of E. coli RNase HI, which shows 52% amino acid sequence identity. Comparison of the far and near UV circular dichroism spectra suggests that the two enzymes are similar in the main chain folding but different in the spatial environments of tyrosine and tryptophan residues. The enzymatic activities of T. thermophilus RNase H at 37 and 70 degrees C for the hydrolysis of either an M13 DNA/RNA hybrid or a nonanucleotide duplex were approximately 5-fold lower and 3-fold higher, respectively, as compared with E. coli RNase HI at 37 degrees C. The melting temperature, Tm, of T. thermophilus RNase H was 82.1 degrees C in the presence of 1.2 M guanidine hydrochloride, which was 33.9 degrees C higher than that observed for E. coli RNase HI. The free energy changes of unfolding in the absence of denaturant, delta G[H2O], of T. thermophilus RNase H increased by 11.79 kcal/mol at 25 degrees C and 14.07 kcal/mol at 50 degrees C, as compared with E. coli RNase HI.     

Thermodynamic parameters for loop formation in RNA and DNA hairpin tetraloops.

We determined the melting temperatures (Tm) and thermodynamic parameters of 15 RNA and 19 DNA hairpins at 1 M NaCl, 0.01 M sodium phosphate, 0.1 mM EDTA, at pH 7. All these hairpins have loops of four bases, the most common loop size in 16S and 23S ribosomal RNAs. The RNA hairpins varied in loop sequence, loop-closing base pair (A.U, C.G, or G.C), base sequence of the stem, and stem size (four or five base pairs). The DNA hairpins varied in loop sequence, loop-closing base pair (C.G, or G.C), and base sequence of the four base-pair stem. Thermodynamic properties of a hairpin may be represented by nearest-neighbor interactions of the stem plus contributions from the loop. Thus, we obtained thermodynamic parameters for the formation of RNA and DNA tetraloops. For the tetraloops we studied, a free energy of loop formation (at 37 degrees C) of about +3 kcal/mol is most common for either RNA or DNA. There are extra stable loops with delta G degrees 37 near +1 kcal/mol, but the sequences are not necessarily the same for RNA and DNA. The closing base pair is also important; changing from C.G to G.C lowered the stability of several tetraloops in both RNA and DNA. These values will be useful in predicting RNA and DNA secondary structures.     

Deoxycytidine methylation does not affect DNA.RNA hybrid formation or B-A transitions of (dG)n.(dC)n sequences.

Optical thermal denaturation and circular dichroism (CD) experiments were performed with the following non-selfcomplementary duplex DNA, RNA and DNA.RNA hybrids: (I) dGAG3C3G3CTC.dGAGC3G3C3TC, (II) dGAG3m5C3G3m5CTC.dGAGm5C3G3m5C3TC, (III) rGAG3C3G3CUC.rGAGC3G3C3UC, (IV) dGAG3C3G3CTC.rGAGC3G3C3UC, (V) rGAG3C3G3CUC.dGAGC3G3C3TC, (VI) dGAG3m5C3G3m5CTC.rGAGC3G3C3UC, (VII) rGAG3C3G3CUC.dGAGm5C3G3m5C3TC. Duplex stabilities (delta G degrees at 60 degrees C) increase in the order: I less than IV less than II = V = VI less than VII less than III. Large enthalpic stabilization is associated with intrastrand stacking of guanosine (rG) residues. CD spectroscopy indicates B-form conformations for the unmethylated and methylated DNA (I,II), A-form geometry for the RNA (III), and DNA.RNA hybrid (IV - VII) conformations resembling but not identical to A-RNA. C5-methyldeoxycytidine does not significantly influence DNA conformation, DNA.RNA hybrid formation, or the ability of DNA to adopt an A-type conformation in trifluoroethanol solutions.     

Spectroscopic analysis of DNA base-pair opening by Escherichia coli RNA polymerase. Temperature and ionic strength effects

The interaction of Escherichia coli RNA polymerase with poly[d(A-T)] and poly[d-(I-C)] was studied by difference absorption spectroscopy at temperatures, from 5 to 45 degrees C in the absence and presence of Mg2+. The effect of KCl concentration, at a fixed temperature, was studied from 12.5 to 400 mM. Difference absorption experiments permitted calculation of the extent of DNA opening induced by RNA polymerase and estimation of the equilibrium constant associated with the isomerization from a closed to an open RNA polymerase-DNA complex. delta H0 and delta S0 for the closed-to-open transition with poly[d(A-T)] or poly[d(I-C)] complexed with RNA polymerase are significantly lower than the values associated with the helix-to-coil transition for the free polynucleotides. For the RNA polymerase complexes with poly[d(A-T)] and poly[d(I-C)] in 50 mM KCl, delta H0 approximately 15-16 kcal/mol (63-67 kJ/mol) and delta S0 approximately 50-57 cal/K per mol (209-239 J/K per mol). The presence of Mg2+ does not change these parameters appreciably for the RNA polymerase-poly[d(A-T)] complex, but for the RNA polymerase-poly[d(I-C)] complex in the presence of Mg2+, the delta H0 and delta S0 values are larger and temperature-dependent, with delta H0 approximately 22 kcal/mol (92 kJ/mol) and delta S0 approximately 72 cal/K per mol (approx. 300 J/K per mol) at 25 degrees C, and delta Cp0 approximately 2 kcal/K per mol (approx. 8.3 kJ/K per mol). The circular dichroism (CD) changes observed for helix opening induced by RNA polymerase are qualitatively consistent with the thermally induced changes observed for the free polynucleotides, supporting the difference absorption method. The salt-dependent studies indicate that two monovalent cations are released upon helix opening. For poly[d(A-T)], the temperature-dependence of enzyme activity correlates well with the helix opening, implying this step to be the rate-determining step. In the case of poly[d(I-C)], the same is not true, and so the rate-determining step must be a process subsequent to helix opening.     

Thermodynamic parameters for an expanded nearest-neighbor model for the formation of RNA duplexes with single nucleotide bulges

Thirty-four RNA duplexes containing single nucleotide bulges were optically melted, and the thermodynamic parameters deltaH degrees, deltaS degrees, deltaG degrees (37), and T(M) for each sequence were determined. Data from this study were combined with data from previous thermodynamic data [Longfellow, C. E., Kierzek, R., and Turner, D. H. (1990) Biochemistry 29, 278-85] to develop a model that will more accurately predict the free energy of an RNA duplex containing a single nucleotide bulge. Differences between purine and pyrimidine bulges as well as differences between Group I duplexes, those in which the bulge is not identical to either neighboring nucleotide, and Group II duplexes, those in which the bulge is identical to at least one neighboring nucleotide, were considered. The length of the duplex, non-nearest-neighbor effects, and bulge location were also examined. A model was developed which divides sequences into two groups: those with pyrimidine bulges and those with purine bulges. The proposed model for pyrimidine bulges predicts deltaG degrees (37,bulge) = 3.9 kcal/mol + 0.10deltaG degrees (37,nn) + beta, while the model for purine bulges predicts deltaG degrees (37,bulge) = 3.3 kcal/mol - 0.30deltaG degrees (37,nn) + beta, where beta has a value of 0.0 and -0.8 kcal/mol for Group I and Group II sequences, respectively, and deltaG degrees (37,nn) is the nearest-neighbor free energy of the base pairs surrounding the bulge. The conformation of bulge loops present in rRNA was examined. Three distinct families of structures were identified. The bulge loop was either extrahelical, intercalated, or in a "side-step" conformation.     

Probing the conformation of a human apolipoprotein C-1 by amino acid substitutions and trimethylamine-N-oxide.

To test, at the level of individual amino acids, the conformation of an exchangeable apolipoprotein in aqueous solution and in the presence of an osmolyte trimethylamine-N-oxide (TMAO), six synthetic peptide analogues of human apolipoprotein C-1 (apoC-1, 57 residues) containing point mutations in the predicted alpha-helical regions were analyzed by circular dichroism (CD). The CD spectra and the melting curves of the monomeric wild-type and plasma apoC-1 in neutral low-salt solutions superimpose, indicating 31 +/- 4% alpha-helical structure at 22 degrees C that melts reversibly with T(m,WT) = 50 +/- 2 degrees C and van't Hoff enthalpy deltaH(v,WT)(Tm) = 18 +/- 2 kcal/mol. G15A substitution leads to an increased alpha-helical content of 42 +/- 4% and an increased T(m,G15A) = 57 +/- 2 degrees C, which corresponds to stabilization by delta deltaG(app) = +0.4 +/- 1.5 kcal/mol. G15P mutant has approximately 20% alpha-helical content at 22 degrees C and unfolds with low cooperativity upon heating to 90 degrees C. R23P and T45P mutants are fully unfolded at 0-90 degrees C. In contrast, Q31P mutation leads to no destabilization or unfolding. Consequently, the R23 and T45 locations are essential for the stability of the cooperative alpha-helical unit in apoC-1 monomer, G15 is peripheral to it, and Q31 is located in a nonhelical linker region. Our results suggest that Pro mutagenesis coupled with CD provides a tool for assigning the secondary structure to protein groups, which should be useful for other self-associating proteins that are not amenable to NMR structural analysis in aqueous solution. TMAO induces a reversible cooperative coil-to-helix transition in apoC-1, with the maximal alpha-helical content reaching 74%. Comparison with the maximal alpha-helical content of 73% observed in lipid-bound apoC-1 suggests that the TMAO-stabilized secondary structure resembles the functional lipid-bound apolipoprotein conformation.     

1H NMR assignment and melting temperature study of cis-syn and trans-syn thymine dimer containing duplexes of d(CGTATTATGC).d(GCATAATACG)

The preparation and spectroscopic characterization of duplex decamers containing site-specific cis-syn and trans-syn thymine dimers are described. Three duplex decamers, d(CGTATTATGC).d(GCATAATACG), d(CGTAT[c,s]TATGC).d(GCATAATACG), and d(CGTAT[t,s]TATGC).d(GCATAATACG), were prepared by solid-phase phosphoramidite synthesis utilizing cis-syn and trans-syn cyclobutane thymine dimer building blocks (Taylor et al., 1987; Taylor & Brockie, 1988). NMR spectra (500 MHz 2D 1H and 202 MHz 1D 31P) were obtained in "100%" D2O at 10 degrees C, and 1D exchangeable 1H spectra were obtained in 10% D2O at 10 degrees C. 1H NMR assignments for H5, H6, H8, CH3, H1', H2', and H2" were made on the basis of standard sequential NOE assignment strategies and verified in part by DQF COSY data. Comparison of the chemical shift data suggests that the helix structure is perturbed more to the 3'-side of the cis-syn dimer and more to the 5'-side of the trans-syn dimer. Thermodynamic parameters for the helix in equilibrium coil equilibrium were obtained by two-state, all or none, analysis of the melting behavior of the duplexes. Analysis of the temperature dependence of the T5CH3 1H NMR signal gave delta H = 44 +/- 4 kcal and delta S = 132 +/- 13 eu for the trans-syn duplex. Analysis of the concentration and temperature dependence of UV spectra gave delta H = 64 +/- 6 kcal and delta S = 178 +/- 18 eu for the parent duplex and delta H = 66 +/- 7 kcal and delta S = 189 +/- 19 eu for cis-syn duplex. It was concluded that photodimerization of the dTpdT unit to give the cis-syn product causes little perturbation of the DNA whereas dimerization to give the trans-syn product causes much greater perturbation, possibly in the form of a kink or dislocation at the 5'-side of the dimer.     

Calorimetric and spectroscopic investigation of drug--DNA interactions: II. Dipyrandium binding to poly d(AT).

We report the first calorimetric investigation of steroid diamine binding to a DNA duplex. Absorption spectroscopy, batch calorimetry, and differential scanning calorimetry (DSC) have been used to detect, monitor, and thermodynamically characterize the binding of the steroid diamine, dipyrandium, to poly d(AT). The following thermodynamic data for the binding in 16 mM Na+ at 25 degrees C have been obtained: delta G degree = -6.5 kcal/mol, delta H degree = +4.2 kcal/mol, and delta S = +36 e.u. We interpret the endothermic binding enthalpy in terms of steroid-induced conformational changes in the duplex (e.g. "kinking"). The large positive entropy is interpreted in terms of binding-induced release of bound water and condensed sodium ions. The salt-dependence of the binding constant is interpreted in terms of dipyrandium site-binding involving only one of the two charged ends of the steroid. The optical and DSC curves for the unsaturated steroid-poly d(AT) complexes exhibit biphasic behavior. A comparison of the van't Hoff and the calorimetric transition enthalpies reveals that steroid binding reduces the cooperativity of the transition.     

Purine-purine mismatches in RNA helices: evidence for protonated G.A pairs and next-nearest neighbor effects.

Thermodynamic parameters are presented for 12 different RNA duplexes containing A.A, A.G, G.A and G.G mismatches flanked by C-G base pairs. UV melting studies were conducted under three different buffer conditions in order to evaluate the effects of salt concentration and pH on the stability of each mismatch-containing duplex. The main findings are: (i) the mismatches have a wide range of effects on duplex stability, decreasing delta G degrees 37 of denaturation by approximately 0-7 kcal/mol; (ii) the nearest-neighbor assumption commonly used to calculate helix stability breaks down for G.A mismatches; and (iii) G.A mismatches separated by 2 bp form a protonated structure.     

High- and low-temperature unfolding of human high-density apolipoprotein A-2.

Human plasma apolipoprotein A-2 (apoA-2) is the second major protein of the high-density lipoproteins that mediate the transport and metabolism of cholesterol. Using CD spectroscopy and differential scanning calorimetry, we demonstrate that the structure of lipid-free apoA-2 in neutral low-salt solutions is most stable at approximately 25 degrees C and unfolds reversibly both upon heating and cooling from 25 degrees C. High-temperature unfolding of apoA-2, monitored by far-UV CD, extends from 25-85 degrees C with midpoint Th = 56 +/- 2 degrees C and vant Hoff's enthalpy delta H(Th) = 17 +/- 2 kcal/mol that is substantially lower than the expected enthalpy of melting of the alpha-helical structure. This suggests low-cooperativity apoA-2 unfolding. The apparent free energy of apoA-2 stabilization inferred from the CD analysis of the thermal unfolding, delta G(app)(25 degrees) = 0.82 +/- 0.15 kcal/mol, agrees with the value determined from chemical denaturation. Enhanced low-temperature stability of apoA-2 observed upon increase in Na2HPO4 concentration from 0.3 mM to 50 mM or addition of 10% glycerol may be linked to reduced water activity. The close proximity of the heat and cold unfolding transitions, that is consistent with low delta G(app)(25 degrees), indicates that lipid-free apoA-2 has a substantial hydrophobic core but is only marginally stable under near-physiological solvent conditions. This suggests that in vivo apoA-2 transfer is unlikely to proceed via the lipid-free state. Low delta H(Th) and low apparent delta Cp approximately 0.52 kcal/mol.K inferred from the far-UV CD analysis of apoA-2 unfolding, and absence of tertiary packing interactions involving Tyr groups suggested by near-UV CD, are consistent with a molten globular-like state of lipid-free apoA-2.     

Structural studies of N- and C-terminally truncated human apolipoprotein A-I

Apolipoprotein A-I (apoA-I) plays an important structural and functional role in lipid transport and metabolism. This work is focused on the central region of apoA-I (residues 60-183) that is predicted to contain exclusively amphipathic alpha-helices. Six N- and/or C-terminally truncated mutants, delta(1-41), delta(1-59), delta(198-243), delta(209-243), delta(1-41,185-243), and delta(1-59,185-243), were analyzed in their lipid-free state in solution at pH 4.7-7.8 by far- and near-UV CD spectroscopy. At pH 7.8, all mutants show well-defined secondary structures consisting of 40-52% alpha-helix. Comparison of the alpha-helix content in the wild type and mutants suggests that deletion of either the N- or C-terminal region induces helical unfolding elsewhere in the structure, indicating that the terminal regions are important for the integrity of the solution conformation of apoA-I. Near-UV CD spectra indicate significant tertiary and/or quaternary structural changes resulting from deletion of the N-terminal 41 residues. Reduction in pH from 7.8 to 4.7 leads to an increase in the mutant helical content by 5-20% and to a large increase in thermal unfolding cooperativity. Van't Hoff analysis of the mutants at pH 4.7 indicates melting temperatures T(m) ranging from 51 to 59 degrees C and effective enthalpies deltaH(v)(T(m)) = 35 +/- 5 kcal/mol, similar to the values for plasma apoA-I at pH 7.8 (T(m) = 57 degrees C, deltaH(v) = 32 kcal/mol). Our results provide the first report of the pH effects on the secondary, tertiary, and/or quaternary structure of apoA-I variants and indicate the importance of the electrostatic interactions for the solution conformation of apoA-I.