Studies of viomycin, an anti-tuberculosis antibiotic: copper(ii) coordination, DNA degradation and the impact on delta ribozyme cleavage activity.

Viomycin is a basic peptide antibiotic, which is among the most effective agents against multidrug-resistant tuberculosis. In this paper we provide the characteristics of its acid base properties, coordination preferences towards the Cu(ii) ions, as well as the reactivity of the resulting complexes against plasmid DNA and HDV ribozyme. Careful coordination studies throughout the wide pH range allow for the characterisation of all the Cu(ii)-viomycin complex species. The assignment of proton chemical shifts was achieved by NMR experiments, while the DTF level of theory was applied to support molecular structures of the studied complexes. The experiments with the plasmid DNA reveal that at the physiological levels of hydrogen peroxide the Cu(ii)-viomycin complex is more aggressive against DNA than uncomplexed metal ions. Moreover, the degradation of DNA by viomycin can be carried out without the presence of transition metal ions. In the studies of antigenomic delta ribozyme catalytic activity, viomycin and its complex are shown to modulate the ribozyme functioning. The molecular modelling approach allows the indication of two different locations of viomycin binding sites to the ribozyme.

Genomic imprinting mechanisms in embryonic and extraembryonic mouse tissues.

Imprinted genes in mice and humans mainly occur in clusters that are associated with differential DNA methylation of an imprint control element (ICE) and at least one nonprotein-coding RNA (ncRNA). Imprinted gene silencing is achieved by parental-specific insulator activity of the unmethylated ICE mediated by CTCF (CCCTC-binding factor) binding, or by ncRNA expression from a promoter in the unmethylated ICE. In many imprinted clusters, some genes, particularly those located furthest away from the ICE, show imprinted expression only in extraembryonic tissues. Recent research indicates that genes showing imprinted expression only in extraembryonic tissues may be regulated by different epigenetic mechanisms compared with genes showing imprinted expression in extraembryonic tissues and in embryonic/adult tissues. The study of extraembryonic imprinted expression, thus, has the potential to illuminate novel epigenetic strategies, but is complicated by the need to collect tissue from early stages of mouse development, when extraembryonic tissues may be contaminated by maternal cells or be present in limited amounts. Research in this area would be advanced by the development of an in vitro model system in which genetic experiments could be conducted in less time and at a lower cost than with mouse models. Here, we summarize what is known about the mechanisms regulating imprinted expression in mouse extraembryonic tissues and explore the possibilities for developing an in vitro model.

Structure and dynamics of adenosine loops in RNA bulge duplexes as revealed by linked application of thermodynamics, spectrofluorimetry and simulation of molecular dynamics.

Structure and dynamics of adenosine loops in RNA bulge duplexes was studied using time-resolved spectrofluorimetry and in aqua simulation of molecular dynamics. Thermodynamics revealed that 2-aminopurine riboside is an non-invasive fluorescent probe when built within the bulge region of chemically synthesized RNA duplexes.

Conformational dynamics of a 5S rRNA hairpin domain containing loop D and a single nucleotide bulge.

Molecular modeling and molecular dynamics have been employed to study the conformation and flexibility of a 15-nucleotide fragment of the plant 5S rRNA containing loop D and a single uridine bulge. Two different model built initial structures were used: one with the bulge localized inside the helical stem and another with the bulge pointing out from the helix. Several independent 700-ps-long trajectories in aqueous solution with Na(+) conterions were produced for each starting structure. The bulge nucleotide inside the helix stayed in two main conformations, both of which affected the geometry of the stem part opposite the bulge. When the bulge nucleotide was located outside the helix, we found high base mobility and local backbone flexibility. The dynamics of the hydrogen bond network and conformational changes from a direct to a water mediated hydrogen bond in the sheared G-A basepair in the tetraloop was described. Our results correlate with lead ion induced cleavage patterns in 5S rRNA. Sites resistant to nonspecific lead cleavage appeared in all our simulations as the most rigid fragments independent of the localization of the bulge nucleotide.

Spatial distribution functions as a tool in the analysis of ribonucleic acids hydration--molecular dynamics studies.

The spatial distribution functions (SDFs) determined as three-dimensional density distribution of hydrogen and oxygen atoms of water in a local coordinate system linked with RNA molecule are used to study details of the spatial structure of aqueous solution around selected parts of RNA duplexes: r(CGCGCG)2 and 2'-O-Me(CGCGCG)2. The influence of the 2'-O-methylation on the hydration pattern of RNA helical fragments is visualized at the atomic level.

A molecular dynamics computer simulation study of nucleotide analogues. Comparison of the hydration pattern of dithymidine phosphate with those of the dithymidine methylphosphonate diastereomers.

The hydration pattern of thymidyl(3'->5') thymidine 1 and those of Rp and Sp diastereomers of the corresponding methylphosphonate analogue 2, have been studied using Molecular Dynamics (MD) computer simulation. It was found that the methylphosphonate modification leads to significant changes in the coordination of water molecules around the internucleotidic linkage and these, in turn, affect the hydration pattern of other parts of the molecule. The most notable differences between Rp and Sp diastereomers 2a and 2b were found to occur at the deoxyribose moieties of the nucleosid-5'-yl units.

Hydration of C-H groups in natural dithymidine nucleotide and its methylphosphonate analogues.

In this paper we report our preliminary studies on the hydration pattern of selected C-H groups in natural thymidyl(3'-5)thymidine and its Rp and Sp-methylphosphonate analogues using Molecular Dynamic simulations in aqueous solutions. The methyl groups attached to the phosphorus center (P-Me) in methylphosphonate analogues are hydrated by water molecules as efficiently as the hydrophilic P=O group in the natural dithymidine nucleotide and better than the neutral P=O functions in these compounds, although the nature of the hydration is different. The C5-Me centers of the 3'-yl units seem to be better hydrated in the methylphosphonate analogues than in the natural dithymidine phosphate and than other centers of the thymine bases in methylphosphonate analogues. Due to chirality of the phosphorus center, the C5-Me group of the 5'-yl unit in the Sp diastereomer coordinates more water than that in the Rp diastereomer. The C6-H group in the 5'-yl unit of the Sp diastereomer exhibits a specific interaction with water.

Bicyclic [b]-heteroannelated pyridazine derivatives. Part 6. Aromatization of some tetrahydrotriazolo[4,3-b]pyridazine derivatives with potential activity as benzodiazepine receptor ligands.

Aromatization of the pyridazine ring in 8-aryl-7,8-dihydro-3-trifluoromethyltriazolo[4,3-b]pyridazin -6(5H)-ones in the reaction with a phosphorus pentachloride-phosphorus oxychloride mixture yielded the corresponding 6-chloro compounds. Since halogenation at C-7 was accompanied by an instant 7,8-dehydrohalogenation, the reaction with bromine gave the 7,8-dehydro analogs with no change of the carbonyl function at C-6. Benzoylation yielded the O-benzoyl derivative as found by X-ray crystallography. Substitution of chlorine at C-6 for an amine or thioether function was effected in the reactions with hydrazine, amines, and thiophenols. In vitro tests revealed low affinity of the compounds for the benzodiazepine receptor.

Mg2+ dependence of the structure and thermodynamics of wheat germ and lupin seeds 5S rRNA.

The formation and stability of structural elements in two 5S rRNA molecules from wheat germ (WG) and lupin seeds (LS) as a function of Mg2+ concentration in solution was determined using the adiabatic differential scanning microcalorimetry (DSC). The experimentally determined thermodynamic parameters are compared with calculations using thermodynamic databases used for prediction of RNA structure. The 5S rRNA molecules which show minor differences in the nucleotide sequence display very different thermal unfolding profiles (DSC profiles). Numerical deconvolution of DSC profiles provided information about structural transformations that take place in both 5S rRNA molecules. A comparative analysis of DSC data and the theoretical thermodynamic models of the structure was used to establish a relationship between the constituting transitions found in the melting profiles and the unfolding of structural domains of the 5S rRNA and stability of its particular helical elements. Increased concentrations of Mg2+ ions induces additional internal interactions stabilising 5S rRNA structures found at low Na+ concentrations. Observed conformational transitions suggest a structural model in which the extension of helical region E dominates over the postulated tertiary interaction between hairpin loops. We propose that helix E is stabilised by a sequence of non-standard pairings extending this helix by the formation of tetra loop e and an almost total reduction of loop d between helices E and D. Two hairpin structures in both 5S rRNA molecules: the extended C-C' and the extended E-E'-E" hairpins appear as the most stable elements of the structure. The cooperativity of the unfolding of helixes in these 5S rRNA molecules changes already at 2 mM Mg2+.

Conformational analysis of galanin using end to end distance distribution observed by Förster resonance energy transfer.

The structural dynamics of the flexible neuropeptide galanin in solution were studied by Förster resonance energy transfer measurements at different temperatures by time-resolved fluorescence spectroscopy to determine its conformational heterogeneity. Endogenous tryptophan at position 2 acted as the fluorescent donor and the non fluorescent acceptor dinitrophenyl or the fluorescent acceptor dansyl were selectively attached to lysine 25 in porcine galanin. The coexistence of different structures of the neuropeptide galanin in trifluoroethanol solution was revealed by the model independent analysis of the distribution of relaxation times from the time-resolved resonance energy transfer data. Multiple conformational states are reflected by distinct end-to-end distance populations. The conformations differ in mean donor-acceptor distance by about 15, and are consistent with the extended and folded backbone conformations of two alpha-helical regions separated by a flexible hinge. The effect that the labelling of galanin has on binding to the receptor was also evaluated. DNP-galanin showed the same high affinity to galanin receptors as unlabelled galanin, whereas DNS-galanin had significantly reduced affinity.

Dynamics of the peptide hormone motilin studied by time resolved fluorescence spectroscopy.

Time resolved fluorescence was used to study the dynamics on the nanosecond and subnanosecond time scale of the peptide hormone motilin. The peptide is composed of 22 amino acid residues and has one tyrosine residue in position 7, which was used as an intrinsic fluorescence probe. The measurements show that two rotational correlation times, decreasing with increasing temperature, are needed to account for the fluorescence polarization anisotropy decay data. Viscosity measurements combined with the fluorescence measurements show that the rotational correlation times vary approximately as viscosity with temperature. The shorter rotational correlation time (0.08 ns in an aqueous solution with 30% hexafluoropropanol, HFP at 20 degrees C) should be related to internal movement of the tyrosine side chain in the peptide while the longer rotational correlation time (2.2 ns in 30% HFP at 20 degrees C) describes the motion of the whole peptide. In addition, the interaction of motilin or the derivative motilin (Y7F) -23W (with tyrosine substituted by phenylalanine and with a tryptophan fluorophore added to the C-terminal) with negatively charged phospholipid vesicles (DOPG) was studied. The results show the development of a long anisotropy decay time which reflects partial immobilization of the peptide by interaction with the vesicles.

The interaction of pyrene labeled diacylglycerol with protein kinase C in mixed micelles.

The binding of protein kinase C (PKC) to pyrene-labeled diacylglycerol (pDG) has been studied in a mixed micellar system by monitoring resonance energy transfer from excited tryptophans to pyrene with time-correlated single photon counting. The average lifetime of the excited state of the tryptophans in PKC showed a clear dependence on the mole percentage pDG in micelles in contrast with pyrene-labeled phosphatidylcholine (pPC). The binding data has been analyzed to a simple model which encompasses the size of the micelles and the binding constant of the pDG-PKC complex. From our data, though, these quantities cannot be determined independently. If we have no size information on the micelles we can determine a lower boundary of this quantity compatible with the data. When the micellar size is known, a binding constant for the DG-PKC complex can be extracted. The presented analytical approach can be applied to other systems in which lipid-protein interactions must be quantified.

Site specific point mutation changes specificity: a molecular modeling study by free energy simulations and enzyme kinetics of the thermodynamics in ribonuclease T1 substrate interactions.

We have theoretically and experimentally studied the binding of two different ligands to wild-type ribonuclease T1 (RNT1) and to a mutant of RNT1 with Glu-46 replaced by Gln. The binding of the natural substrate 3'-GMP has been compared with the binding of a fluorescent probe, 2-aminopurine 3'-monophosphate (2AP), and relative free energies of binding of these ligands to the mutant and the wild-type (wt) enzyme have been calculated by free energy perturbation methods. The free energy perturbations predict that the mutant RNT1-Gln-46 binds 2AP better than 3'GMP, in agreement with experiments on dinucleotides. Four free energy perturbations, forming a closed loop, have been performed to allow the detection of systematic errors in the simulation procedure. Because of the larger number of atoms involved, it was necessary to use a much longer simulation time for the change in the protein, i,e., the perturbation from Glu to Gln, than in the perturbation from 3'-GMP to 2AP. Finally the structure of the binding site is analyzed for understanding differences in catalytic speed and binding strength.

Comparative calorimetric studies on the dynamic conformation of plant 5S rRNA: II. Structural interpretation of the thermal unfolding patterns for lupin seeds and wheat germ.

Thermal unfolding of 5S rRNA from wheat germ (WG) and lupin seeds (LS) was studied in solution. Experimental curves of differential scanning calorimetry (DSC) were resolved into particular components according to the thermodynamic model of two-state transitions. The DSC temperature profiles for WG and LS differ significantly in spite of very high similarities in the sequence of both molecules. Those results are interpreted according to a model of the secondary and tertiary molecular structure of 5S rRNA. A comparison of the 'nearest neighbour' model of interaction with the experimental thermodynamic results enables a complete interpretation of the process of the melting of its structures. In light of our observations, the crucial differences between both DSC melting profiles are mainly an outcome of different thermodynamic properties of the first helical fragment 'A' made up of 9 complementary base pairs. It contains 6 differences in the nucleotide sequence of both types of molecules, which still retain 9-meric double helixes. The temperature stability of his helix in WG is much lower than of the LS one. Moreover, the results supply evidence for a strong specific tertiary interaction between the two hairpin loops 'c' and 'e' in both 5S rRNA molecules, modulated by small differences in the thermodynamic properties of both 5S rRNA.

Spectroscopic investigations of the single tryptophan residue and of riboflavin and 7-oxolumazine bound to lumazine apoprotein from Photobacterium leiognathi.

Spectroscopic techniques have been applied to investigate the conformation, local structure, and dynamic properties of the apoprotein of the lumazine protein from Photobacterium leiognathi and the holoprotein reconstituted with either the natural ligand 6,7-dimethyl-8-ribityllumazine or the closely related analogues riboflavin and 6-methyl-7-oxo-8-ribityllumazine (7-oxolumazine). The analogues are bound similarly to the natural prosthetic group. They exhibit similar shifts on binding in their absorption and fluorescence spectra, single-exponential fluorescence decays, and no independent motion from the protein as evident from a long-lived anisotropy decay (single-exponential phi = 10 ns, 20 degrees C) and high initial anisotropy. Steady-state anisotropy measurements result in similar KD's (40 nM, 20 degrees C, 50 mM inorganic phosphate) for all ligands. Circular dichroism in the far-UV region (190-250 nm) indicates no change in secondary structure on binding to the apoprotein. In the spectral region of 250-310 nm relatively large changes occur, indicating changes in the environment of the tyrosine and tryptophan residues. The single tryptophan residue shows a three-exponential decay of its fluorescence in both the apoprotein and the holoprotein. Radiationless energy transfer also occurs from the tryptophan to the bound ligand, especially evident with 7-oxolumazine. We have designed a new method for evaluation of the rate constant of energy transfer by measuring the (picosecond) rise time of the acceptor fluorescence. The anisotropy decay of the tryptophan residue shows two correlation times, a short one (phi approximately equal to 0.4 ns) representing rapid but restriced oscillation of this residue and a longer one (phi 2 = 5-7 ns, 20 degrees C) representing the motion of a larger segment of the protein.