Evidence for long-range interactions in DNA. Analysis of melting curves of block polymers d(C15A15)·d(T15G15), d(C20A15)·d(T15G20), and d(C20A10)·d(T10G20)

The influence of one DNA region on the stability of an adjoining region (telestability) was examined. Melting curves of three block DNA's, d(C₁₅A₁₅)·d(T₁₅G₁₅), d(C₂₀A₁₅)·d(T₁₅G₂₀), and d(C₂₀A₁₀)·d(T₁₀G₂₀) were analyzed in terms of the nearest neighbor Ising model. Comparisons of predicted and experimental curves were made in 0.01 M and 0.1 M sodium ion solutions. The nearest neighbor formalism was also employed to analyze block DNA transition in the presence of actinomycin, a G·C specific molecule. The results show that nearest neighbor base-pair interaction cannot predict the melting curves of the block DNA's. Adjustments in theoretical parameters to account for phosphate repulsion assuming a B conformation throughout the DNA's do not alter this conclusion. Changes in the theoretical parameters, which provide good overall agreement, are consistent with a substantial stabilization of the A·T region nearest the G·C block. The melting temperature T A·T for the average A·T pari in d(C₂₀A₁₀)·d(T₁₀G₂₀), with 10 A·T pairs, appears to be 4°C greater than T_A·T for d(C₁₅A₁₅)·d(T₁₅G₁₅) and d(C₂₀A₁₅)·d(T₁₅G₂₀), both with 15 A·T pairs. Actinomycin bound to the G·C end effectively stabilizes the A·T end by 9°C. These results indicate a long-range contribution to the interactions governing DNA stability. A possible mechanism for these interactions will be discussed.     

An analysis of the sequence dependence of the structure and energy of A- and B-DNA models using molecular mechannics

Molecular-mechanics calculations have been carried out on the base-paired hexanucleoside pentaphosphates d(TATATA)₂, d(ATATAT)₂, d(A₆)·d(T₆), d(CGCGCG)₂, d(GCGCGC)₂, and d(C₆)·d(G₆) in both A- and B-DNA geometries. The calculated relative energies of these polymers are consistent with the relative stabilities of the polymers found experimentally. In particular, the results of our calculations support the observation that the homopolymer d(A)_n·d(T)_n is more stable in a B-DNA conformation, while the homopolymer d(G)_n·d(C)_n is more stable in an A-DNA conformation. The molecular interactions responsible for these differential stabilities include both inter- and intrastrand base stacking, as well as base–phosphate interactions. While definitive experiments on the heteropolymer stabilities have not yet been carried out, the results of our calculations also suggest a greater stability of the purine-3′,5′-pyrimidine sequence over the pyrimidine-3′,5′-purine sequence in both the A- and B-conformations. The reason for this greater stability lies in the importance of the inherent directionality (5′ → 3′ vs 3′ → 5′) of phosphate–base and base–base interactions. The largest conformation change observed on energy refinement is sugar repuckering, which occurs mainly on pyrimidine-attched sugars and only in the B-DNA geometry. We suggest a molecular mechanism, specifically, differential base–sugar steric interactions involving neighboring sugars, to explain why this repuckering occurs more with d(A₆)·d(T₆) than with other isomers.     

Conformational Preferences of Modified Nucleoside N(4)-Acetylcytidine, ac4C Occur at “Wobble” 34th Position in the Anticodon Loop of tRNA

Conformational preferences of modified nucleoside, N(4)-acetylcytidine, ac⁴C have been investigated using quantum chemical semi-empirical RM1 method. Automated geometry optimization using PM3 method along with ab initio methods HF SCF (6-31G**), and density functional theory (DFT; B3LYP/6-31G**) have also been made to compare the salient features. The most stable conformation of N(4)-acetyl group of ac⁴C prefers “proximal” orientation. This conformation is stabilized by intramolecular hydrogen bonding between O(7)···HC(5), O(2)···HC2′, and O4′···HC(6). The “proximal” conformation of N(4)-acetyl group has also been observed in another conformational study of anticodon loop of E. coli elongator tRNA^Met. The solvent accessible surface area (SASA) calculations revealed the role of ac⁴C in anticodon loop. The explicit molecular dynamics simulation study also shows the “proximal” orientation of N(4)-acetyl group. The predicted “proximal” conformation would allow ac⁴C to interact with third base of codon AUG/AUA whereas the ‘distal’ orientation of N(4)-acetyl cytidine side-chain prevents such interactions. Single point energy calculation studies of various models of anticodon–codon bases revealed that the models ac⁴C₍₃₄₎(Proximal):G₃, and ac⁴C₍₃₄₎(Proximal):A₃ are energetically more stable as compared to models ac⁴C₍₃₄₎(Distal):G₃, and ac⁴C₍₃₄₎(Distal):A₃, respectively. MEPs calculations showed the unique potential tunnels between the hydrogen bond donor–acceptor atoms of ac⁴C₍₃₄₎(Proximal):G₃/A₃ base pairs suggesting role of ac⁴C in recognition of third letter of codons AUG/AUA. The “distal” conformation of ac⁴C might prevent misreading of AUA codon. Hence, this study could be useful to understand the role of ac⁴C in the tertiary structure folding of tRNA as well as in the proper recognition of codons during protein biosynthesis process.     

CD studies of double-stranded polydeoxynucleotides composed of repeating units of contiguous homopurine residues

Double-stranded synthetic polydeoxynucleotides of the general form poly[d(G_nC_n)] · poly[d(G_nC_n)], poly[d(G_nC)] · poly[d(GC_n)], and poly[d(A_nT_n)] · poly[d(A_nT_n)] have been synthesized. When n = 4 or larger, the CD spectra of polymers of the form poly[d(G_nC_n)] · poly[d(G_nC_n)] or poly[d(G_nC)] · poly[d(GC_n)] closely resemble the spectrum of poly[dG] · poly[dC], suggesting that a string of four continguous guanosine residues is sufficient to induce a conformation resembling that of the polypurine · polypyrimidine. With polymers of the form poly[d(A_nT_n)] · poly[d(A_nT_n)], however, the CD spectrum only gradually approaches that of poly[dA] · poly[dT].     

A molecular mechanical study of netropsin-DNA interactions

We present molecular mechanical calculations on the complexes of netropsin with dA₆·dT₆, d(TATATA)₂, d(CGCGCG)₂, and d(CGCGAATTCGCG)₂. The complexes were model built using computer graphics and then completely energy refined. Our calculations are consistent with the observed AT preference for netropsin and suggest that mixed sugar pucker geometries should be more stable than uniform in netropsin complexes with poly[d(A-T)]·poly[d(A-T)] and poly(dA)·poly(dt). The netropsin·d(TATATA) and netropsin·dA₆·dT₆ complexes are significantly different in structure, leading to a possible reason why the observed thermodynamics of netropsin-association with poly[d(A-T)]·poly[d(A-T)] and with poly(dA)·poly(dT) are so different. We also model built and energy refined a structure of netropsin-d(CGCGAATTCGCG)₂ using as a guide the nmr data of Patel [(1982) Proc. Natl. Acad. Sci. USA, 79 , 6424–6428] and found a three-dimensional structure qualitatively consistent with the NOE enhancements observed by him. After our calculations were completed, we learned of an x-ray structure of a netropsin:d(CGCGAATTCGCG)₂ complex, and we compared the structure found in our calculation with the x-ray structure.     

Base-pair exchange kinetics of the imino and amino protons of the 3′-phenazinium tethered DNA-RNA duplex,r(5′GAUUGAA3′):d(5′TCAATC3′-Pzn), and their comparison with those of B-DNA duplex

The dynamics of the opening-closing of the constituent base-pairs as well as of the exchange kinetics of the base-paired imino and amino protons with water in a DNA-RNA hybrid, [^5′r(G¹A²U³U⁴G⁵A⁶A⁷)^3′]:^5′p[d(T⁸C⁹A¹⁰A¹¹T¹²C¹³)]^3′-Pzn] duplex (I), are reported here in details for the first time. The exchange kinetics of amino and imino protons in the DNA-RNA hybrid (duplex I) have been compared with identical studies on the following B-DNA duplexes: d(C¹G²T³A⁴C⁵G⁶)₂ (II), d[p(^5′T¹G²T³T⁴T⁵G⁶ G⁷C⁸)^3′]:d[p(^5′C⁹C¹⁰A¹¹A¹²A¹³C¹⁴A¹⁵)^3′] (III), d(C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶)₂ (IV) and d(C¹G²C³G⁴C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶C¹⁷G¹⁸C¹⁹G²⁰)₂ (V). This comparative study shows that the life-times τ_o of various base-pairs in the DNA-RNA hybrid (I) varies in the range of ∼ 1 ms, and they are quite comparable to those of the shorter B-DNA duplexes (II) and (III), but very different from the τ_o of the larger duplexes (IV) and (V): the τ_o for the base pair of T¹¹ and T¹² residues in the 20-mer (duplex V) are 2.9 ± 2.3 ms and 23.2 ± 8.9 ms, respectively, while the corresponding τ_o in the 12-mer (duplex IV) are 2.8 ± 2.2 ms and 17.4 ± 5.4 ms. It has also been shown that the total energy of activation (E_a) assessed from the exchange rates of both imino and amino protons, representing energetic contributions from both base-pair and helix opening-closing as well as from the exchange process of the imino protons from the open state with the bound water, is close to the E_a of the short B-DNA duplex (E_a ≈ 28–47 kcal/mol).     

Shape readout of AT‐rich DNA by carbohydrates

Gene expression can be altered by small molecules that target DNA; sequence as well as shape selectivities are both extremely important for DNA recognition by intercalating and groove‐binding ligands. We have characterized a carbohydrate scaffold (1) exhibiting DNA “shape readout” properties. Thermodynamic studies with 1 and model duplex DNAs demonstrate the molecule's high affinity and selectivity towards B* form (continuous AT‐rich) DNA. Isothermal titration calorimetry (ITC), circular dichroism (CD) titration, ultraviolet (UV) thermal denaturation, and Differential Scanning Calorimetry were used to characterize the binding of 1 with a B* form AT‐rich DNA duplex d[5′‐G₂A₆T₆C₂‐3′]. The binding constant was determined using ITC at various temperatures, salt concentrations, and pH. ITC titrations were fit using a two‐binding site model. The first binding event was shown to have a 1:1 binding stoichiometry and was predominantly entropy‐driven with a binding constant of approximately 10⁸ M^?1. ITC‐derived binding enthalpies were used to obtain the binding‐induced change in heat capacity (ΔC_p) of ?225 ± 19 cal/mol·K. The ionic strength dependence of the binding constant indicated a significant electrolytic contribution in ligand:DNA binding, with approximately four to five ion pairs involved in binding. Ligand 1 displayed a significantly higher affinity towards AT‐tract DNA over sequences containing GC inserts, and binding experiments revealed the order of binding affinity for 1 with DNA duplexes: contiguous B* form AT‐rich DNA (d[5′‐G₂A₆T₆C₂‐3′]) >B form alternate AT‐rich DNA (d[5′‐G₂(AT)₆C_2‐3′]) > A form GC‐rich DNA (d[5′‐A₂G₆C₆T₂‐3′]), demonstrating the preference of ligand 1 for B* form DNA. © 2013 Wiley Periodicals, Inc. Biopolymers 101: 720–732, 2014.     

Molecular Dynamics Simulation of 7, 8-dihydro-8-Oxoguanine DNA

Abstract

To elucidate the effect of guanine lesion produced by the oxidative damage on DNA, 1 nanosecond molecular dynamics simulations of native and oxidized DNA were performed. The target DNA molecules are dodecamer duplex d(CGCGAATTCGCG)2 and its derivative duplex d(C₁G₂C₃(8-oxoG)₄A₅A₆T₇T₈C₉G₁₀C₁₁G₁₂)·d(C₁₃G₁₄C₁₅G₁₆A₁₇A₁₈T₁₉T₂₀C21_G22C₂₃G₂₄), which has one oxidized guanine, 7, 8-dihydro-8-oxoguanine (8-oxoG), at the fourth position. The local structural change due to the lesion of 8-oxoG and the global dynamic structure of the 8-oxoG DNA were studied. It was found that the 8-oxoG DNA remained structurally stable during the simulation due to newly produced hydrogen bonds around the (8-oxoG)₄ residue. However, there were distinguishable differences in structural parameters and dynamic property in the 8-oxoG DNA. The conformation around the (8- oxoG)₄ residue departed from the usual conformation of native DNA and took an unique conformation of ?-ζ in B_II conformation and χ in high anti orientation at the (8-oxoG)₄ residue, and adopted a very low helical twist angle at the C₃:G₂₂—(8-oxoG)₄:C₂₁ step. Further analysis by principal component analysis indicated that the formation of the hydrogen bonds around the (8-oxoG)₄ residue plays a role as a trigger for the conformational transition of the 8-oxoG DNA in the conformational space.     

Molecular interactions of the quinone electron acceptors QA,QB, and QC in photosystem II as studied by the fragment molecular orbital method

Molecular interactions of the three plastoquinone electron acceptors, Q_A, Q_B, and Q_C, in photosystem II (PSII) were studied by fragment molecular orbital (FMO) calculations. Calculations at the FMO-MP2/6-31G level using PSII models deduced from the X-ray structure of the PSII complexes from Thermosynechococcus elongatus provided the binding energies of Q_A, Q_B, and Q_C as ?56.1, ?37.9, and ?30.1 kcal/mol, respectively. The interaction energies with surrounding fragments showed that the contributions of lipids and cofactors were 0, 24 and 45 % of the total interaction energies for Q_A, Q_B, and Q_C, respectively. These results are consistent with the fact that Q_A is strongly bound to the PSII protein, whereas Q_B functions as a substrate and is exchangeable with other quinones and herbicides, and the presence of Q_C is highly dependent on PSII preparations. It was further shown that the isoprenoid tail is more responsible for the binding than the head group in all the three quinones, and that dispersion forces rather than electrostatic interactions mainly contribute to the stabilization. The relevance of the stability and molecular interactions of Q_A, Q_B, and Q_C to their physiological functions is discussed.     

Genetic Relationships Within and Between Capsicum Species

Genetic relationships were estimated among 24 accessions belonging to 11 species of Capsicum, using 2,760 RAPD markers based on touch-down polymerase chain reactions (Td-RAPD-PCR). These markers were implemented in analyses of principal coordinates, unweighted pair group mean average, and 2,000 bootstrap replications. The accessions were divided into four groups, corresponding to previously described Capsicum complexes: C. annuum complex (C_A), C. baccatum complex (C_B), C. pubescens complex (C_P), and C. chacoense accessions (C_A/_B). Their overall mean genetic similarity index was 0.487 ± 0.082, ranging from 0.88 to 0.32, based on Jaccard’s coefficient. The highest genetic variation was observed among the accessions in C_P; the accessions in C_B had a low level of variation as judged from the standard deviations of the genetic similarity indices. Based on the Td-RAPD-PCR markers, the 24 accessions were divided into four major groups, three of which corresponded to the three distinct Capsicum complexes. Accessions of C. chacoense were found to be equally related to complexes C_A, C_B, and C_P.     

The Residence Time of the Bound Water in the Hydrophobic Minor Groove of the Carbocyclic-Nucleoside Analogs of Dickerson-Drew Dodecamers

Summary

The residence time of the bound water molecules in the antisense oligodeoxyribonucleotides containing 7′-α-methyl (T_Me). carbocyclic thymidines in duplex (I), d⁵′(¹C²G³C⁴G⁵A⁶A⁷T_Mc ⁸T_Mc ⁹C¹⁰G¹¹C¹²G)₂ ³′, and 6′-a-hydroxy (T_OH) carbocyclic thymidines in duplex (II), d⁵′(¹C³G³C⁴G⁵A_OH ⁶ A_OH ⁷T_OH ⁸ T_OH ⁹C¹⁰G¹¹C¹²G)₂3, have been investigated using a combination of NOESY and ROESY experiments. Because of the presence of 7′-α-methyl groups of T_Me in the centre of the minor groove in duplex (I), the residence time of the bound water molecule is shorter than 0.3 ns. The dramatic reduction of the residence time of the water molecule in the minor groove in duplex (I) compared with the natural counterpart has been attributed to the replacement of second shell of hydration and disruption of hydrogen-bonding with 04′ in the minor groove by hydrophobic α-methyl groups, as originally observed in the X-ray study. This effect could not be attributed to the change of the width of the minor groove because a comparative NMR study of the duplex (I) and its natural counterpart showed that the widths of their minor grooves are more or less unchanged (r.m.s.d change in the core part is <0.63Å). For duplex (II) with polar 6′-α-hydroxyl groups pointed to the minor groove, the correlation time is much longer than 0.36ns as a result of the stabilising hydrogen-bonding interaction with N3 or 02 of the neighbouring nucleotides.     

The First Example of a Hoogsteen Basepaired DNA Duplex in Dynamic Equilibrium with a Watson-Crick Basepaired Duplex—A Structural (NMR), Kinetic and Thermodynamic Study

Abstract

A single-point substitution of the O4′ oxygen by a CH₂ group at the sugar residue of A ⁶ (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 A ⁶:T⁷ Hoogsteen basepaired (1B) B-type DNA duplex, resulting in a dynamic equilibrium of (1A)→←(1B): K_eq = 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; δH°? = 164±14 kJ/mol;-TδS°? (298K) = ?92 kJ/mol giving a δG₂₉₈°? 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, δH°? = 153±13 kJ/mol;-TδS°? (298K) = ?82 kJ/mol giving a δG₂₉₈°? of 71 kJ/mol. Ea (k-1) = 155±13 kJ/mol]. A comparison of δG₂₉₈°? 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 A ⁶: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 A ⁶:T⁷ basepairs in (1B) has enforced a syn conformation on the glycosyl torsion of the 2′- deoxyaristeromycin moiety, A ⁶, as a result of substitution of the endocyclic 4′-oxygen in the natural sugar with a methylene group in A ⁶. A comparison of the Watson-Crick basepaired duplex (1A) to the Hoogsteen basepaired duplex (1B) shows that only a few changes, mainly in α, σ and γ torsions, in the sugar-phosphate backbone seem to be necessary to accommodate the Hoogsteen basepair.     

Theoretical investigations of the H···π and X (X = F,Cl, Br,I)···π complexes between hypohalous acids and benzene

The H···π and X (X = F, Cl, Br, I)···π interactions between hypohalous acids and benzene are investigated at the MP2/6-311++G(2d,2p) level. Four hydrogen-bonded and three halogen-bonded complexes were obtained. Ab initio calculations indicate that the X···π interaction between HOX and C₆H₆ is mainly electrostatically driven, and there is nearly an equal contribution from both electrostatic and dispersive energies in the case of XOH–C₆H₆ complexes. Natural bond orbital (NBO) analysis reveals that there exists charge transfer from benzene to hypohalous acids. Atom in molecules (AIM) analysis locates bond critical points (BCP) linking the hydrogen or halogen atom and carbon atom in benzene.     

A Single Carbocyclic Nucleotide Substitution in a 12mer DNA Gives a Hoogsteen Basepaired Duplex (Till 38°C) and a Hairpin (Till 65°C). A 600 MHz NMR Spectroscopic Study

Abstract

The impact of intramolecular stereoelectronic effects has been examined by comparison of the solution structures of natural oligo-DNA duplex, 5′(¹C²G³C⁴G⁵A⁶A⁷T⁸T⁹C¹⁰G¹¹C¹²G)₂ ³′, and its carbocyclic-nucleotide analogues in which the pentose sugar in 2′-dA residue is replaced with its carbocyclic counterpart (i.e. 2′-deoxyaristeromycin). Based on the NMR evidences, it has been shown, that 2′-deoxyaristeromycin analog exists in a dynamic equilibrium between the two forms of duplexes, one with W-C bp and the second with Hoogsteen bp in ca 1:1 ratio at lower temperature (below 35°C) and as hairpin at higher temperature (from ～40° – 60°C).     

Tetraplex Formation of d(GGGGGTTTTT): 1H NMR Study in Solution

Abstract

The oligonucleotide d(G₅T₅) can in principle form a fully matched duplex with G · T pairing and/or a tetraplex. Non-denaturing gel electrophoresis, circular dichroism and NMR experiments show that the tetraplex is exclusively formed by this oligomer in solution. In the presence of its complementary strand d(A₅C₅) at low temperature, d(G₅T₅) forms the tetraplex over the normally expected Watson-Crick duplex. However, when d(G₅T₅) and d(A₅C₅) are mixed together in equimolar amounts and heated for several minutes at 85°C, and then allowed to cool, the product was essentially the Watson-Crick duplex. The lack of resolution in the 500 MHz ¹H NMR spectra and the presence of extensive spin diffusion do not allow us to derive a quantitative structure for the tetraplex from the NMR data. However, we find good qualitative agreement between the NOESY and MINSY data and a theoretically derived stereochemically sound structure in which the G's and T's are part of a parallel tetraplex.     

Skeletal ontogeny of the vertebral column and of the fins in shi drum Umbrina cirrosa (Teleostei: Perciformes: Sciaenidae), a new candidate species for aquaculture

The osteological development of the vertebral column and fins in shi drum Umbrina cirrosa was studied in order to improve knowledge for its introduction in Mediterranean aquaculture. The osteological development was studied in 171 individuals, of total length (L_T) from 2·7 to 30·2 mm that were reared under the mesocosm technique. Vertebral ontogeny starts at 3·4 and 4·0 mm L_T, with the formation of the first cartilaginous neural and haemal arches, and spines, respectively, and is completed with the full attainment of epicentrals (12·5 mm L_T). The formation of vertebral centra occurs between 4·1 and 7·4 mm L_T. Pectoral supports are the first fin elements to develop (3·0 mm L_T), followed by those of the caudal fin (3·8 mm L_T), pelvic fin (3·9 mm L_T) and finally by those of the dorsal and anal fins (4·5 mm L_T). The caudal fin is the first to develop fin rays and attain the full count of principal fin rays (4·5–6·8 mm L_T), but the last to be fully completed with the formation of procurrent fin rays (6·9–17·5 mm L_T). The next fins starting to present rays are the dorsal (5·3 mm L_T) and the pectoral fins (5·6 mm L_T), while the anal and pelvic fins are the last (5·7 mm L_T). Following the caudal principal fin rays (6·8 mm L_T), the dorsal, anal (6·9 mm L_T), pelvic (7·4 mm L_T) and pectoral fins (9·8 mm L_T) are the next with fully completed ray counts. Aggregation of qualitative changes, such as the appearance of cartilages, the beginning and the complement of the ossification process and the full complement of elements in U. cirrosa were measured as cumulative frequency counts. These measurements reveal three ontogenetic intervals: one very developmentally active period during early life stages (from 3 to 5·9 mm L_T), a second slower developmental period (from 6·0 to 8·9 mm L_T) and finally a period of ontogeny more focused on structure refinement up to metamorphosis and settlement (>9·0 mm L_T).     

Relativistic theoretical studies on hydrogen bonds and the electronic structure of aqueous solvated bis(uranyl) complex: an insight into explicit and/or implicit solvent effects

To understand the chemical behavior of uranyl complexes in water, a bis-uranyl [(phen)(UO₂)(μ₂–F)(F)]₂ (A; phen?=?phenanthroline, μ₂?=?doubly bridged) and its hydrated form A?·?(H₂O)_n (n?=?2, 4 and 6) were examined using scalar relativistic density functional theory. The addition of water caused the phen ligands to deviate slightly from the U₂(μ₂–F)₂ plane, and red-shifts the U–F-terminal and U?=?O stretching vibrations. Four types of hydrogen bonds are present in the optimized hydrated A?·?(H₂O)_n complexes; their energies were calculated to fall within the range 4.37–6.77 kcal mol^-1, comparable to the typical values of 5.0 kcal mol^-1 reported for hydrogen bonds. An aqueous environment simulated by explicit and/or implicit models lowers and re-arranges the orbitals of the bis-uranyl complex.

N-substituted ethylcarbamate complexes of thorium(IV) and lanthanum(III) nitrates

N-substituted ethylcarbamates form with thorium nitrate the complexes Th(NO₃)₄·3RHNC(O)OC₂H₅ (where R = CH₃, C₂H₅, C₆H₅(CH₃)CH) and with lanthanum nitrate the complexes La(NO₃)₃· 2RR′NC(O)OC₂H₅·3H₂O (where R = CH₃, C₂H₅, C₆H₅(CH₃)CH; R′ = H and R = CH₃, C₆H₅; R′ = C₂H₅ or R = R′ = CH₃). In addition the anhydrous La(NO₃)₃·3(C₂H₅)₂NC(O)OC₂H₅ has been isolated. From the IR spectra it is deduced that the carbamates coordinate the metal through the carbonyl oxygen atom and that the nitrato groups act as chelated ligands. ¹H nmr spectral data of the complexes are reported and discussed.     

Selectively 13C-enriched DNA: Evidence from 13C1′ relaxation rate measurements of an internal dynamics sequence effect in the lac operator

Summary In order to study some internal dynamic processes of the lac operator sequence, the ¹³C-labeled duplex 5d(C₀G₁C₂T₃C₄A₅C₆A₇A₈T₉T₁₀) · d(A₁₀A₉T₈T₇G₆T₅G₄A₃G₂C₁G₀)3 was used. The spreading of both the H1 and C1 resonances brought about an excellent dispersion of the ¹H1-¹³C1 correlations. The spinlattice relaxation parameters R(C_z), R(C_x,y) and R(H_zC_z) were measured for each residue of the two complementary strands, except for the 3-terminal residues which were not labeled. Variation of the relaxation rates was found along the sequence. These data were analyzed in the context of the model-free formalism proposed by Lipari and Szabo [(1982) J. Am. Chem. Soc., 104, 4546–4570] and extended to three parameters by Clore et al. [(1990) Biochemistry, 29, 7387–7401; and (1990) J. Am. Chem. Soc., 112, 4989–4991]. A careful analysis using a least-squares program showed that our data must be interpreted in terms of a three-parameter spectral density function. With this approach, the global correlation time was found to be the same for each residue. All the C1-H1 fragments exhibited both slow (_s = 1.5) and fast (_f = 20 ps) restricted libration motions (S _inf2 ^sups =0.74 to 1.0 and S _inf2 ^supf =0.52 to 0.96). Relaxation processes were described as governed by the motion of the sugar relative to the base and in terms of bending of the whole duplex. The possible role played by the special structure of the AATT sequence is discussed. No evident correlation was found between the amplitude motions of the complementary residues. The 5-terminal residues showed large internal motions (S²=0.5), which describe the fraying of the double helix. Global examination of the microdynamical parameters S _inf2 ^supf and S _inf2 ^sups along the nucleotide sequence showed that the adenine residues exhibit more restricted fast internal motions (S _inf2 ^supf =0.88 to 0.96) than the others, whereas the measured relaxation rates of the four nucleosides in solution were mainly of dipolar origin. Moreover, the fit of both R(C_z) and R(HzC_z) experimental relaxation rates using an only global correlation time for all the residues, gave evidence of a supplementary relaxation pathway affecting R(C_x,y) for the purine residues in the (53) G₄A₃ and A₁₀A₉T₈T₇ sequences. This relaxation process was analyzed in terms of exchange stemming from motions of the sugar around the glycosidic bond on the millisecond time scale. It should be pointed out that these residues gave evidence of close contacts with the protein in the complex with the lac operator [Boelens et al. (1987) J. Mol. Biol., 193, 213–216] and that these motions could be implied in the lac-operator-lac-repressor recognition process.