Kinetic and thermodynamic characterization of DNA duplex–hairpin interconversion for two DNA decamers: d(CAACGGGTTG) and d(CAACCCGTTG)

The duplex–hairpin interconversion of two DNA decamers, d(CAACGGGTTG) and d(CAACCCGTTG), has been characterized thermodynamically and kinetically by using uv-melting and nmr relaxation methods. Separately, each decamer shows slow exchange between hairpin and duplex conformations. The hairpin conformations have melting points of 47 and 50°C, respectively, and exhibit similar thermodynamic stabilities. The enthalpies of duplex formation, measured by nmr, were found to be very similar (ΔH_DH = 26 ± 3 kcal/mole) for both decanters at low salt concentrations (< 50 mM NaCl). However, as the salt concentration was increased the behavior of ΔH_DH, and kinetics is significantly different for each decamer. The d(CAACGGGTTG) decamer forms a duplex containing two central G·G mismatches at high salt and DNA concentration. Based upon the measurement of high interconversion activation energies and a decrease in hairpin formation rate with increasing salt, the interconversion between hairpin and duplex was concluded to proceed by complete strand dissociation. In contrast, the d(CAAC-CCGTTG) decamer was determined to form a duplex with two centrally located C·C mismatches at pH values less than 6.2, consistent with the formation of a hemiprotonated C⁺·C mismatch. At pH values greater than 6.4, the hairpin–duplex equilibrium is almost completely shifted toward the hairpin conformation at DNA concentrations of 0.5–7.0 mM and salt concentrations of 10–100 mM. The interconversion of duplex and hairpin conformations was ascertained by means of both kinetic and thermodynamic measurements to proceed by a slightly different mechanism than its complementary decamer. Although the interconversion proceeds by complete strand separation as suggested by high duplex-hairpin interconversion activation enthalpies, the increasing hairpin formation rate with increasing ionic strength as well as the ΔH_DH, dependence on sail indicate that an intermediate internally bulged duplex (no C⁺·C formation) is stabilized by increasing ionic strength. These data support an interconversion mechanism where an intermediate internally bulged duplex may be the rate limiting step before strand separation. © 1995 John Wiley & Sons, Inc.     

Hairpin Formation of d(CGCG-TA-CGCG), d(CGCG-TG-CGCG) and Their Cytosine Methylated Analogs

Abstract

Hairpin formations of decamers d(CGCG-TA-CGCG), d(CGCG-TG-CGCG), and their m⁵dC analogs are evidenced by the existence of biphasic absorbance melting profiles in which the lower transition temperature increases with increasing oligomer concentration, whereas the higher melting temperature is concentration independent. The corresponding temperature dependent CD intensity at 285 nm exhibits a maximum around 55°C. These observations are consistent with the interpretation that the lower temperature transition corresponds to the duplex to hairpin transformation while the melting of hairpins into single strands constitutes the higher temperature transition. The CD spectrum of the hairpin conformation appears to be characterized by a couplet with nearly equal positive and negative intensities at 285 and 255 nm, respectively, while a significantly smaller intensity at 285 nm is apparent for the duplex form. The hairpin conformation is suspected to contain a two-nucleotide loop. Titrations with NaCl further suggest that, in contrast to the TA sequence, the TG sequence with wobble base pairing favors Z formation under high salt conditions.     

2D 1H and 31P NMR Spectra and Distorted A-DNA-Like Duplex Structure of a Phosphorodithioate Oligonucleotide

Abstract

Assignment of the ¹H and ³¹P NMR spectra of a phosphorodithioate modified oligonucleotide decamer duplex, d(CGCTTpS^? ₂AAGCG)₂ (10-mer-S; a site of dithioate substitution is designated with the symbols pS^? ₂), was achieved by two-dimensional homonuclear TOCSY, NOES Y and ¹H-³¹P Pure Absorption phase Constant time (PAC) heteronuclear correlation spectroscopy. In contrast to the parent palindromic decamer sequence (1) which has been shown to exist entirely in the duplex B-DNA conformation under comparable conditions (100 mM KCI), the dithiophosphate analogue forms a hairpin loop. However, the duplex form of the dithioate oligonucleotide can be stabilized at lower temperatures, higher salt and strand concentration. The solution structure of the decamer duplex was calculated by an iterative hybrid relaxation matrix method (MORASS) combined with 2D NOESY-distance restrained molecular dynamics. These backbone modified compounds, potentially attractive antisense oligonucleotide agents, are often assumed to possess similar structure as the parent nucleic acid complex. Importantly, the refined structure of the phosphorodithioate duplex shows a significant deviation from the parent unmodified, phosphoryl duplex. An overall bend and unwinding in the phosphorodithioate duplex is observed. The structural distortion of the phosphorodithioate duplex was confirmed by comparison of helicoidal parameters and groove dimensions. Especially, the helical twists of the phosphorodithioate decamer deviate significantly from the parent phosphoryl decamer. The minor groove width of phosphorodithioate duplex 10-mer-S varies between 8.4 and 13.3 Å which is much wider than those of the parent phosphoryl decamer d(CGCTTAAGCG)₂ (4.2～9.4Å). The larger minor groove width of 10-mer-S duplex contributes to the unwinding of the backbone and indicates that the duplex has an overall A-DNA-like conformation in the region surrounding the dithiophosphate modification.     

Helix-coil dynamics of a Z-helix hairpin

The helix–coil transition of a Z-helix hairpin formed from d(C-G)₅T₄(C-G)₅ has been characterized by equilibrium melting and temperature jump experiments in 5M NaClO₄ and 10 mM Na₂HPO₄, pH 7.0. The melting curve can be represented by a simple all-or-none transition with a midpoint at 81.6 ± 0.4°C and an enthalpy change of 287 ± 15 kJ/mole. The temperature jump relaxation can be described by single exponentials at a reasonable accuracy. Amplitudes measured as a function of temperature provide equilibrium parameters consistent with those derived from equilibrium melting curves. The rate constants of Z-helix formation are found in the range from 1800 s^?1 at 70°C to 800 s^?1 at 90°C and are associated with an activation enthalpy of ?(50 ± 10) kJ/mole, whereas the rate constants of helix dissociation are found in the range from 200 s^?1 at 70°C to 4500 s^?1 at 90°C with an activation enthalpy +235 kJ/mole. These parameters are consistent with a requirement of 3–4 base pairs for helix nucleation. Apparently nucleation occurs in the Z-helix conformation, because a separate slow step corresponding to a B to Z transition has not been observed. In summary, the dynamics of the Z-helix–coil transition is very similar to that of previously investigated right-handed double helices.     

The Duplex-Harpin Conformational Transition of d(CGCGCGATCGCGCG) and d(CGCGCGTACGCGCG): A Thermodynamic and Kinetic Study

Abstract

We have studied the duplex-hairpin conformational transition in two perfectly palindromic sequences, d(CGCGCGATCGCGCG)(I) and d(CGCGCGTACGCGCG)(II), by means of UV-melting, electrophoretic and T-jump experiments. Both tetradecamers exhibit biphasic thermal profiles. The lower temperature transition is concentration dependent whereas the higher temperature transition is not. The former transition has been characterized by gel electrophoresis and shows two distinct bands, whose intensity depends on temperature. This behavior is due to the occurrence of a slow premelting interconversion between the duplex and hairpin forms in both tetradecamers. The kinetics of hairpin formation from the duplex is studied by T-jump experiments. Relaxation spectra are well reproduced by a single relaxation time with rate constants characterized by a high temperature coefficient. In 10 mM NaCl, the duplex-hairpin conversion of I is characterized by an apparent activation energy of 96 ± 6 kcal/mol, a value rather close to the expected denaturation enthalpy. In 1 mM NaCl a value slightly lower has been obtained. The rate of duplex-hairpin interconversion has been found to decrease as the salt concentration is raised. These data suggest that the transformation from the duplex to the hairpin form should imply a transition state with a simultaneous breaking of most base pairs, if not total strand separation.     

An NMR Study of the Polymorphous Behavior of the Mismatched DNA Octamer d(m5C-G-m5C-G-T-G-m5C-G) in Solution. The B,Z, and Hairpin Forms

Abstract

The polymorphism exhibited by the mismatched octamer d(m ⁵C-G-m⁵C-G-T-G-m⁵C-G), as a function of the temperature, DNA concentration and ionic strength, was investigated by means of NMR spectroscopy.

It is shown that this partly self-complementary DNA fragment, under conditions of low DNA concentration (0.4 mM) and low ionic strength, exclusively prefers to adopt a monomeric hairpin form, which consists of a stem of three Watson-Crick-type base pairs and a loop of only two residues. This in striking contrast with earlier intimations in literature, which postulated that in oligonucleotides loop formations containing only two residues are sterically impossible. Moreover, the hairpin form displays an unusual stability in comparison with previously reported hairpins. AT_m of 332 K and a ΔH° of—130 kj · mol^?1 were calculated for the hairpin to random coil transition.

At high DNA concentration (8 mM)and/or upon the addition of sodium chloride the hairpin form occurs in slow exchange with a B-DNA dimer structure (approximately 20% at 270 K, no added salt), which comprises two central GxT-mismatched base pairs with the bases as major tautomers.

At higher ionic strength (> 100 mM NaCI), or upon the addition of methanol, a third species appears, which is in slow exchange with both the B dimer and the hairpin form. This third species could be identified with a Z DNA form, comprising two GxT mismatches with the bases as major tautomers, with the guanine bases syn and the cytosine and thymine bases anti.     

Thermodynamics of the slow–fast transition in bacteriophage T2L

We have measured the thermodynamic parameters of the slow-fast tail-fiber reorientation transition on T2L bateriophage. Proportions of the virus in each form were determined from peak-height measurements in sedimention-velocity runs and from average diffusion coefficients obtained by quasielastic laser light scattering. Computer simulation of sedimentation confirmed that there were no undetected intermediates in the transition, which was analyzed as a two-state process. Van't Hoff-type plots of the apparent equilibrium constant and of the pH midpoint of the transition as function of reciprocal temperature led to the following estimates of the thermodynamic parameters for the transition at pH 6.0 and 20°C: ΔH° = ?139 ± 18Kcal mol^?1, ΔS° = ?247 ± 46 cal K^?1 mol^?1, and ΔG° = ?66 ± 22 kcal mol^?1. Per mole of protons taken up in the transition, the analogous quantities were ?15.9 ± 1.7 kcal mol^?1, ?26.3 ± 2.2 cal K^?1 mol^?1, and ?8.22 ± 1.8 kcal mol^?1. The net number of protons taken up was about 8.5 ± 1.5. The large values of the thermodynamic functions are consistent with a highly cooperative reaction and with multiple interactions between the fibres and the remainder of the phage. The negative entropy of the transition is probably due to immobilization of the fibres.     

Thermodynamic parameters for the helix-coil thermal transition of ribonuclease-S-peptide and derivatives from 1H-NMR data

Values for the thermodynamic quantities, ΔH° = 11.8 ± 2.0 Kcal/mole and ΔS° = 43.6 ± 6.0 e.u., of the 3-13 helix–coil equilibrium of isolated S-peptide (19 residue N-terminal fragment of ribonuclease A) in aqueous solution (3 m M, 1M NaCl, pD 5.4) have been determined from a joint analysis of the Thr 3γ, Ala 6β, Phe 8meta, and Phe 8para ¹H chemical shift vs temperature curves (?7 to 80°C) in several aqueous–trifluorethanol mixtures. Chemical shifts in the coil and in the helix have been determined for up to 16 protons belonging to the 3-13 fragment. Thermodynamic parameters have also been determined for C-peptide (13 residue fragment) and a number of S-peptide derivatives. From the variation of the values of the thermodynamic parameters at pD 2.5, 5.4, and 8.0, a quantitation of the two helix-stabilizing side-chain interactions can be made: (1) Δ(ΔH°) ? 5 Kcal/mole and Δ(ΔS°) ? 18 e.u. for the salt bridge Glu 2^? … Arg 10⁺ and (2) Δ(ΔH°) ? 3 Kcal/mole and Δ(ΔS°) = 9 e.u. for the one in which the His 12⁺ imidazolium group is involved, presumably a partial stacking with the Phe 8 side chain.     

Volume and sound velocity changes associated with coil- transition of poly(S-carboxymethyl L-cysteine) in aqueous solution

The measurements were made for the volume and the sound velocity changes (ΔV and ΔU) on titrating the sodium salt of poly (S-carboxymethyl L -cysteine) with dilute HCl. For the reaction, ? COO^? + H⁺ → ? COOH, ΔV per mole of H⁺ bound was + 12. 7 ml and +11. 4 ml in salt-free and 0. 2 M NaCl solutions, respectively. Corresponding ΔU was about ?13 cm/sec in salt-free polymer solution where 11.5 mM carboxylate ion reacts with equimolar hydrogen ion. ΔV associated with the coil-to-β transition was found to be +2. 35 ml in H₂O and +1. 90 ml in 0. 2 M NaCl per mole of amino acid residue, respectively. These values are larger than those obtained for the coil-to-helix transition of poly (L -glutamic acid). ΔU for the transition was about ?30 cm/sec in salt-free solution of polymer concentration 0.0115 mole/liter. Possible sources of ΔV and ΔU for reaction; coil → β, are (1) the formation of void volume and (2) the changes in the extent of solvation in amide linkage and in side chain.     

Salt-dependent conformational transitions in the self-complementary deoxydodecanucleotide d(CGCAATTCGCG): Evidence for hairpin formation

Differential scanning calorimetry (DSC), temperature-dependent uv-absorption spectroscopy, and temperature-dependent CD were used to monitor and characterize the salt-dependent, thermally induced structural transitions in the deoxydodecanucleotide d(CGCGAATTCGCG). At the high oligomer concentrations required for DSC, the calorimetric scans revealed a single, monophasic transition curve at all salt concentrations. Based on previous nmr melting studies under similar conditions, we conclude that these monophasic transitions correspond to the cooperative duplex-to-single-strand conversion of the dodecamer. By contrast, at the lower oligomer concentrations used for the spectroscopic studies, the shapes of the uv and CD melting curves were found to depend on the concentration of the added salt. At high salt (≥0.1M Na⁺), a single, monophasic transition curve was observed. At lower salt (?0.01M Na⁺), the CD and uv melting curves exhibit biphasic behavior. Based on the concentration dependence, the enthalpy, and the cooperativity of each transition in the biphasic curve, we conclude that at low salt and low oligomer concentrations, the dodecamer melts in a sequential manner involving initial disruption of a duplex structure and subsequent disruption of a hairpin structure.     

The interaction of collagen with the hydrophobic fluorescent probe-2-p-toluidinylnaphthalene-6-sulfonate.

Three kinds of fluorescence enhancement result from the interaction of 2-p-toluidinylnaphthalene-6-sulfonate and calf-skin collagen. They are negatively cooperative, independent, and highly cooperative fluorescence enhancement. In the independent region at pH 3.7, the binding number is about 36 moles of 2-p-toluidinylnaphthalene-6-sulfonate per mole of tropocollagen with a binding constant of 2.0 × 10⁴ M^?1; with ΔG = ?5.7 kcal/mole, ΔH = ?4.0 kcal/mole, and ΔS = 6 e.u. The pH dependence of fluorescence of native collagen shows that the deprotonated forms of the β and γ carboxyl groups of aspartic and glutamic acid decrease the intensity, possibly by charge repulsion of the negatively charged sulfonate group of 2-p-toluidinylnaphthalene-6-sulfonate. The positive charge of lysine is found to be unimportant in the interaction of 2-p-toluidinylnaphthalene-6-sulfonate with collagen. Fluorescence enhancement is caused mainly by the hydrophobic interactions of 2-p-toluidinylnaphthalene-6-sulfonate and collagen. Salt bridge formation between basic and acidic side chains in very low salt concentration may be detectable by 2-p-toluidinylnaphthalene-6-sulfonate fluorescence.     

Hexamer oligonucleotide topology and assembly under solution phase NMR and theoretical modeling scrutiny

The entire family of noncomplementary hexamer oligodeoxyribonucleotides d(GCXYGC) (X and Y = A, G, C, or T) were assessed for topological indicators and equilibrium thermodynamics using a priori molecular modeling and solution phase NMR spectroscopy. Feasible modeled hairpin structures formed a basis from which solution structure and equilibria for each oligonucleotide were considered. ¹H and ³¹P variable temperature‐dependent (VT) and concentration‐dependent NMR data, NMR signal assignments, and diffusion parameters led to d(GCGAGC) and d(GCGGGC) being understood as exceptions within the family in terms of self‐association and topological character. A mean diffusion coefficient D_{298 K} = (2.0 ± 0.07) × 10^?10 m² s^?1 was evaluated across all hexamers except for d(GCGAGC) (D_{298 K} = 1.7 × 10^?10 m² s^?1) and d(GCGGGC) (D_{298 K} = 1.2 × 10^?10 m² s^?1). Melting under VT analysis (T_m = 323 K) combined with supporting NMR evidence confirmed d(GCGAGC) as the shortest tandem sheared GA mismatched duplex. Diffusion measurements were used to conclude that d(GCGGGC) preferentially exists as the shortest stable quadruplex structure. Thermodynamic analysis of all data led to the assertion that, with the exception of XY = GA and GG, the remaining noncomplementary oligonucleotides adopt equilibria between monomer and duplex, contributed largely by monomer random‐coil forms. Contrastingly, d(GCGAGC) showed preference for tandem sheared GA mismatch duplex formation with an association constant K = 3.9 × 10⁵M^?1. No direct evidence was acquired for hairpin formation in any instance although its potential existence is considered possible for d(GCGAGC) on the basis of molecular modeling studies. © 2010 Wiley Periodicals, Inc. Biopolymers 93: 1023–1038, 2010. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

Design of Peptides Using α,β-Dehydro-residues: Synthesis,Crystal Structure and Molecular Conformation of N-Boc-L-Val-ΔPhe–ΔPhe-L-Ala-OCH3

To obtain general rules of peptide design using α,β-dehydro-residues, a sequence with two consecutive ΔPhe-residues, Boc-L -Val-ΔPhe–ΔPhe- L -Ala-OCH₃, was synthesized by azlactone method in solution phase. The peptide was crystallized from its solution in an acetone/water mixture (70:30) in space group P6₁ with a=b=14.912(3) Å, c= 25.548(5) Å, V=4912.0(6) ų. The structure was determined by direct methods and refined by a full matrix least-squares procedure to an R value of 0.079 for 2891 observed [I?3σ(I)] reflections. The backbone torsion angles ?₁=?54(1)°, ψ₁= 129(1)°, ω₁=?177(1)°, ?₂ =57(1)°, ψ₂=15(1)°, ω₂ =?170(1)°, ?₃=80(1)°, ψ₃ =7(2)°, ω₃=?177(1)°, ?₄ =?108(1)° and ψ^T₄=?34 (1)° suggest that the peptide adopts a folded conformation with two overlapping β-turns of types II and III′. These turns are stabilized by two intramolecular hydrogen bonds between the CO of the Boc group and the NH of ΔPhe³ and the CO of Val¹ and the NH of Ala⁴. The torsion angles of ΔPhe² and ΔPhe³ side chains are similar and indicate that the two ΔPhe residues are essentially planar. The folded molecules form head-to- tail intermolecular hydrogen bonds giving rise to continuous helical columns which run parallel to the c-axis. This structure established the formation of two β-turns of types II and III′ respectively for sequences containing two consecutive ΔPhe residues at (i+2) and (i+3) positions with a branched β-carbon residue at one end of the tetrapeptide.     

Cis-Trans equilibrium and kinetic studies of acetyl-L-proline and glycyl-L-proline

By means of carbon-13 nmr (at 25 MHz) the trans/cis conformer ratio in glycyl-L -proline has been measured in aqueous (D₂O) solution over the temperature range 33–96°C. It is found that ΔH⁰ = ?4.2 kJ/mole and ΔS⁰ = ?9.7 J/mole/K. Measurements of the T₁ values for the proline ring carbons yielded values consistent with a fast puckering process involving both the β- and γ-carbons. Measurements of the rate of cis-trans conformational interconversion in glycyl-L -proline, using complete line-shape analysis for the glycyl α-carbon resonance, gave values for the trans → cis isomerization as follows: ΔH^≠ = 83.5 ± 0.2 kJ/mole; ΔS^≠ = 0.0 ± 10 J/mole/K. A more approximate determination from coalescence temperature observations gave a value of ΔG^≠ of 82.0 ± 0.4 kJ/mole for this process in acetyl-L -proline in aqueous solution. The presence of 12M NaSCN lowered this barrier by ca. 2.6 kJ/mole. Such measurements are relevant to present theoretical models of the denaturation-renaturation processes in proteins, in which proline residues may play a key role.     

Structure Sensitivity of Amino Proton Exchange in 2′ - and 5′ - Guanosine Monophosphate Dianions

Abstract

Proton NMR line broadening methods were used to determine the rates of amino proton exchange for disordered 2′ - and 5′ - GMP dianions in aqueous solutions containing tetramethylammonium (TMA⁺) cations. Replacing TMA⁺ with Na⁺ does not substantially alter the exchange rates, provided that H-bonded, Na⁺-directed tetramer structures are absent. Activation enthalpies (kcal/mol) and entropies (eu) for 2′ - GMP are: ΔH^# = 18.5 ± 1.3, ΔS^# = 9.6 ± 4.2 for theTMA⁺ salt atpH 8.10, and ΔH^# = 14.7 ± 2.6, ΔS^# = -3.7 ± 8.0 for the Na⁺ salt at pH 8.11. Extrapolated values of pseudo first-order rate constants at 25° Care in the range of k = 1–10 sec^?1. At suitable concentrations and temperatures, the Na⁺ salts of both 2′ - and 5′ - GMP formed stacked and unstacked tetramer units. Relative to the exchange kinetics observed for the disordered nucleotide, the exchange process in the tetramer units was catalyzed in half the amino protons and inhibited in the other half. The catalytic process (k < 10³ sec^?3) has been attributed to amino protons not involved in interbase H-bonding, where as the inhibited process (k > 10^?1 sec^?1) was assigned to those protons which do form such bonds. The structure-catalyzed process in both the stacked and unstacked tetramers was manifested by a loss of NMR amino proton intensity due to weighted time-averaging with the resonance for bulk water. A bridging water molecule between an amino proton and a phosphate on an adjacent nucleotide in the tetramer unit may provide a mechanistic pathway for the structure-catalyzed process.     

Calorimetric studies of oxyhemoglobin dissociation. I. Reaction of sodium dithionite with oxygen

Calorimetric studies of the reduction of free oxygen in solution by sodium dithionite are in agreement with a stoichiometry of 2 moles Na₂S₂O₄ per mole of oxygen. The reaction is biphasic with ΔH_t - 118±7 kcal mol^?1 (?494 ± 29 kJ mol^?1). The initial phase of the reaction proceeds with an enthalpy change of ca ?20 kcal (?84 kJ) and occurs when 0.5 moles of dithionite have been added per mole dioxygen present. This could be interpreted as the enthalpy change for the addition of a single electron to form the superoxide anion. Further reduction of the oxygen to water by one or more additional steps is accompanied by an enthalpy change of ca ?100 kcal (?418. 5 kJ). Neither of these reductive phases is consistent with the formation of hydrogen peroxide as an intermediate. The reduction of hydrogen peroxide by dithionite in 0.1 M phosphate buffer, pH 7.15, is a much slower process and with an enthalpy change of ca ? 74 kcal mol^?1 (?314 kJ mol^?1). Dissociation of oxyhemoglobin induced by the reduction of free oxygen tension with dithionite also shows a stoichiometry of 2 moles dithionite per mole oxygen present and an enthalpy change of ca. ?101 ±9 kcal mol^?1 (?423± 38 kJ mol^?1). The difference in the observed enthalpies (reduction of dioxygen vs. oxyhemoglobin) has been attributed to the dissociation of oxyhemoglobin, which is 17 kcal mol^?1 (71 kJ mol^?1).     

Salt bridge exchange binding mechanism between streptavidin and its DNA aptamer – thermodynamics and spectroscopic evidences

Protein‐nucleic acids binding driven by electrostatic interactions typically are characterized by the release of counter ions, and the salt‐inhibited binding association constant (K_a) and the magnitude of exothermic binding enthalpy (ΔH). Here, we report a non‐classical thermodynamics of streptavidin (SA)–aptamer binding in NaCl (140–350 mM) solutions near room temperatures (23–27 °C). By using isothermal titration calorimetry (ITC) and circular dichroism (CD)/fluorescence spectroscopy, we found that the binding was enthalpy driven with a large entropy cost (ΔH ?20.58 kcal mol^?1, TΔS ?10.99 kcal mol^?1, and K_a 1.08 × 10⁷ M^?1 at 140 mM NaCl 25 °C). With the raise of salt concentrations, the ΔH became more exothermic, yet the K_a was almost unchanged (ΔH ?26.29 kcal mol^?1 and K_a 1.50 × 10⁷ M^?1 at 350 mM NaCl 25 °C). The data suggest that no counter Na⁺ was released in the binding. Spectroscopy data suggest that the binding, with a stoichiometry of 2, was accompanied with substantial conformational changes on SA, and the changes were insensitive to the variation of salt concentrations. To account for the non‐classical results, we propose a salt bridge exchange model. The intramolecular binding‐site salt bridge(s) of the free SA and the charged phosphate group of aptamers re‐organize to form the binding complex by forming a new intermolecular salt bridge(s). The salt bridge exchange binding process requires minimum amount of counter ions releasing but dehydration of the contacting surface of SA and the aptamer. The energy required for dehydration is reduced in the case of binding solution with higher salt concentration and account for the higher binding exothermic mainly. Copyright © 2013 John Wiley & Sons, Ltd.     

Kinetics of the renaturation of yeast tRNA3 leu.

Yeast tRNA₃^Leu is one of several tRNA molecules which can adopt a stable, biologically inactive, denatured conformation. The circular dichroism of the native and denatured conformers differs, providing the basis for the present study of the mechanism for the renaturation process. Conversion of the denatured structure to the native takes place in two steps: a rapid change occurring immediately on addition of Mg⁺⁺, followed by a slower, strongly temperature-dependent step which returns the molecule to its biologically active state. Optimal kinetic data for the second step could be obtained at 285 nm. Analysis of the time dependence of Δε₂₈₅ by the Guggenheim method demonstrated that this step follows first-order kinetics. The temperature dependence of the rate constants over the range 32–41°C yielded the following parameters for the rate-limiting step: E_a = 69 kcal/mole, ΔH^? = 69 kcal/mole, and ΔS^? = 146 cal/mole deg. Values of this magnitude are typical of order—order transitions in nucleic acids.     

The stereodynamics of 1,2‐dipropyldiaziridines

N‐alkylated trans‐diaziridines are an intriguing class of compounds with two stereogenic nitrogen atoms which easily interconvert. In the course of our investigations of the nature of the interconversion process via nitrogen inversion or electrocyclic ring opening ring closure, we synthesized and characterized the three constitutionally isomeric diaziridines 1,2‐di‐n‐propyldiaziridine 1 , 1‐isopropyl‐2‐n‐propyldiaziridine 2 , and 1,2‐diisopropyldiaziridine 3 to study the influence of the substituents on the interconversion barriers. Enantiomer separation was achieved by enantioselective gas chromatography on the chiral stationary phase Chirasil‐β‐Dex with high separation factors α (1‐isopropyl‐2‐n‐propyldiaziridine: 1.18; 1, 2‐diisopropyldiaziridine: 1.24; 100°C 50 kPa He) for the isopropyl substituted diaziridines. These compounds showed pronounced plateau formation between 100 and 150°C, and peak coalescence at elevated temperatures. The enantiomerization barriers ΔG? and activation parameters ΔH? and ΔS? were determined by enantioselective dynamic gas chromatography (DGC) and direct evaluation of the elution profiles using the unified equation implemented in the software DCXplorer. Interestingly, 1‐isopropyl‐2‐n‐propyldiaziridine and 1,2‐diisopropyldiaziridine exhibit similar high interconversion barriers ΔG? (100°C) of 128.3 ± 0.4 kJ mol^?1 and 129.8 ± 0.4 kJ mol^?1, respectively, which indicates that two sterically demanding substituents do not substantially increase the barrier as expected for a distinct nitrogen inversion process. Chirality, 2010. © 2009 Wiley‐Liss, Inc.