Escin belongs to a large class of natural biosurfactants, called saponins, that are present in more than 500 plant species. Saponins are applied in the pharmaceutical, cosmetics, and food and beverage industries due to their variously expressed bioactivity and surface activity. In particular, escin adsorption layers at the air-water interface exhibit an unusually high surface elastic modulus (>1100 mN/m) and a high surface viscosity (ca. 130 N·s/m). The molecular origin of these unusual surface rheological properties is still unclear. We performed classical atomistic dynamics simulations of adsorbed neutral and ionized escin molecules to clarify their orientation and interactions on the water surface. The orientation and position of the escin molecules with respect to the interface, the intermolecular interactions, and the kinetics of molecular aggregation into surface clusters are characterized in detail. Significant differences in the behavior of the neutral and the charged escin molecules are observed. The neutral escin rapidly assembles in a compact and stable surface cluster. This process is explained by the action of long-range attraction between the hydrophobic aglycones, combined with intermediate dipole-dipole attraction and short-range hydrogen bonds between the sugar residues in escin molecules. The same interactions are expected to control the viscoelastic properties of escin adsorption layers.

Locked nucleic acids (LNAs) exhibit a modified sugar fragment that is restrained to the C3'-endo conformation. LNA-containing duplexes are rather stable and have a more rigid structure than DNA duplexes, with a propensity for A-conformation of the double helix. To gain detailed insight into the local structure of LNA-modified DNA oligomers (as a foundation for subsequent exploration of the electron-transfer capabilities of such modified duplexes), we carried out molecular dynamics simulations on a set of LNA:DNA 9-mer duplexes and analyzed the resulting structures in terms of base step parameters and the conformations of the sugar residues. The perturbation introduced by a single locked nucleotide was found to be fairly localized, extending mostly to the first neighboring base pairs; such duplexes featured a B-type helix. With increasing degree of LNA modification the structure gradually changed; the duplex with one complete LNA strand assumed a typical A-DNA structure. The relative populations of the sugar conformations agreed very well with NMR data, lending credibility to the validity of the computational protocol.

Four three-dimensional (3D) pyrene-fused N -heteroacenes ( P1 – P4 ) are designed and synthesized. From P1 to P4 , their lengths are extended in an iterative way, where the thiadiazole unit can be reduced to diamine and the obtained diamines can be further condensed with the diketones with a thiadiazole unit. Compared to their two-dimensional counterparts, the solubility of these 3D pyrene-fused N -heteroacenes is improved by this 3D covalent linkage with two-dimensional units. The diameters of P1 – P4 are 3.66, 6.06, 8.48 and 10.88 nm, respectively, and these 3D molecules are characterized by 1 H, 13 C and 2D NMR, MS, UV–vis, PL and CV spectra. Our strategy shows a promising way to large 3D pyrene-fused N -heteroacenes.

The electronic coupling is one of the key parameters governing electron hole transfer along DNA helices. In this study, we established the first comprehensive data base of electronic coupling elements, calculated at the ab initio level. The data set comprises all possible Watson-Crick base pair dimers, both in standard A-DNA and B-DNA geometries. We also quantified the sensitivity of the coupling elements with respect to geometry changes by varying each of the six standard base step parameters, which specify the relative orientation of neighboring base pairs. We compare the couplings in a systematic way by discussing variations in the coupling magnitude due to geometry or nucleotide sequence in the dimer, and we analyze how the structure affects the electronic coupling in terms of general and dimer-specific trends. Furthermore, we studied how the coupling changes when one introduces the chemically modified base 7-deazaguanine in the corresponding base-pair dimers. Finally, on the basis of the calculated coupling elements, we suggest a model duplex with an enhanced capacity for hole transfer.

Classical molecular dynamics simulations are employed to monitor the aggregation behavior of six bile salts (nonconjugated and glycine- and taurine-conjugated sodium cholate and sodium deoxycholate) with concentration of 10 mM in aqueous solution in the presence of 120 mM NaCl. There are 150 ns trajectories generated to characterize the systems. The largest stable aggregates are analyzed to determine their shape, size, and stabilizing forces. It is found that the aggregation is a hierarchical process and that its kinetics depends both on the number of hydroxyl groups in the steroid part of the molecules and on the type of conjugation. The micelles of all salts are similar in shape-deformed spheres or ellipsoids, which are stabilized by hydrophobic forces, acting between the steroid rings. The differences in the aggregation kinetics of the various conjugates are rationalized by the affinity for hydrogen bond formation for the glycine-modified salts or by the longer time needed to achieve optimum packing for the tauro derivatives. Evidence is provided for the hypothesis from the literature that the entirely hydrophobic core of all aggregates and the enhanced dynamics of the molecules therein should be among the prerequisites for their pronounced solubilization capacity for hydrophobic substances in vivo.

Calculations for model oligomers of the emeraldine salt with UBLYP/6-31G*/PCM are performed. The models differ in number of monomers, in the position of the counterions (Cl(-)), and in multiplicity. The molecular features affected most prominently by the protonation, namely, structure, energetics, and electron and spin density partitioning are analyzed. The results show unequivocally that the studied molecular characteristics are essentially size independent. The octamer profiles of all parameters are repeated in the dodecamer and the hexadecamer. The bipolaronic forms are energetically more favorable than the polaronic ones within the chosen protocol. The electronic structure in the intermediate multiplicities differs from the bipolaronic and polaronic periodicity. The geometrical changes and electron density redistribution upon increase of multiplicity illustrate the pathway of intramolecular bipolaron-polaron conversion. The orbital analysis rationalizes the observed behavior of the oligomers.

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