6533b85ffe1ef96bd12c1253

RESEARCH PRODUCT

Structure, stability, and fragmentation of sodium bis(2-ethylhexyl)sulfosuccinate negatively charged aggregates in vacuo by MD simulations.

Giovanna LonghiAlberto CeselliLeopoldo CerauloSandro L. ForniliVincenzo Turco LiveriSergio Abbate

subject

SodiumSupramolecular chemistryMolecular Conformationchemistry.chemical_elementFragmentation patternsMolecular Dynamics SimulationAOTNa Self-assembling Charged reverse micelles Molecular dynamics simulation (MD) Supramolecular aggregates in vacuo Fragmentation patternsMicelleMolecular dynamicsSurface-Active AgentsPulmonary surfactantStructural BiologyAotNa; self-assembling; charged revrse micelle; Molecular Dynamics simulations; Supramolecular aggregates in vacuo; Fragmentation patternsSpectroscopyAlkylMicellesSettore CHIM/02 - Chimica Fisicachemistry.chemical_classificationIonsDioctyl Sulfosuccinic AcidAggregation numberAotNacharged revrse micelleself-assemblingSupramolecular aggregates in vacuoCrystallographychemistryThermodynamicsMolecular Dynamics simulationsCounterion

description

Negatively charged supramolecular aggregates formed in vacuo by n bis(2-ethylhexyl)sulfosuccinate (AOT(-)) anions and n + n(c) sodium counterions (i.e., [AOT(n) Na(n+nc)](nc)) have been investigated by molecular dynamics (MD) simulations for n = 1 to 20 and n(c) = -1 to -5. By comparing the maximum excess charge values of negatively and positively charged AOTNa aggregates, it is found that the charge storage capability is higher for the latter systems, the difference decreasing as the aggregation number increases. Statistical analysis of physical properties like gyration radii and moment of inertia tensors of aggregates provides detailed information on their structural properties. Even for n(c) = -5, all stable aggregates show a reverse micelle-like structure with an internal core, including sodium counterions and surfactant polar heads, surrounded by an external layer consisting of the surfactant alkyl chains. Interestingly, the reverse micelle-like structure is retained also in proximity of fragmentation. Moreover, the aggregate shapes may be approximated by elongated ellipsoids whose longer axis increases with n and |n(c)|. The fragmentation patterns of a number of these aggregates have also been examined and have been found to markedly depend on the aggregate charge state. The simulated fragmentation patterns of a representative aggregate show good agreement with experimental data obtained using low collision voltages.

10.1007/s13361-014-0942-8https://pubmed.ncbi.nlm.nih.gov/24969925