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Claudio J Margulis

Publications and source records attributed to Claudio J Margulis.

5 recordsLinked to original sources

A study of the time-resolved fluorescence spectrum and red edge effect of ANF in a room-temperature ionic liquid.

In a recent article, we have analyzed using molecular dynamics simulations the steady-state red edge effect (REE) observed by Samanta and co-workers when the fluorescent probe 2-amino-7-nitrofluorene (ANF) is photoexcited at different wavelengths in 1-butyl-3-methylimidazolium ([BMIM+]) hexafluorophosphate ([PF6-]). In this letter, we predict the time- and wavelength-dependent emission spectra of ANF in the same ionic solvent. From the analysis of our simulated data, we are able to derive an approximate time scale for reorganization of the solvent around the solute probe. The effect that slow varying local liquid environments have on the overall time-dependent signal is also discussed.

Letter↗

Heterogeneity in a room-temperature ionic liquid: persistent local environments and the red-edge effect.

In this work, we investigate the slow dynamics of 1-butyl-3-methylimidazolium hexafluorophosphate, a very popular room-temperature ionic solvent. Our study predicts the existence of heterogeneity in the liquid and shows that this heterogeneity is the underlying microscopic cause for the recently reported "red-edge effect" (REE) observed in the study of fluorescence of the organic probe 2-amino-7-nitrofluorene. This theoretical work explains in microscopic terms the relation between REE and dynamic heterogeneity in a room-temperature ionic liquid (IL). The REE is typical of micellar or colloidal systems, which are characterized by microscopic environments that are structurally very different. In contrast, in the case of this room-temperature IL, the REE occurs because of the long period during which molecules are trapped in quasistatic local solvent cages. This trapping time, which is longer than the lifetime of the excited-state probe, together with the inability of the surroundings to adiabatically relax, induces a set of site-specific spectroscopic responses. Subensembles of fluorescent molecules associated with particular local environments absorb and emit at different frequencies. We describe in detail the absorption wavelength-dependent emission spectra of 2-amino-7-nitrofluorene and show that this dependence on lambda(ex) is characteristic of the IL and, as is to be expected, is absent in the case of a normal solvent such as methanol.

Cations↗

Why is the partial molar volume of CO2 so small when dissolved in a room temperature ionic liquid? Structure and dynamics of CO2 dissolved in [Bmim+] [PF6(-)].

When supercritical CO2 is dissolved in an ionic liquid, its partial molar volume is much smaller than that observed in most other solvents. In this article we explore in atomistic detail and explain in an intuitive way the peculiar volumetric behavior experimentally observed when supercritical CO2 is dissolved in 1-butyl-3-methylimidazolium hexafluorophosphate ([Bmim+] [PF6(-)]). We also provide physical insight into the structure and dynamics occurring across the boundary of the CO2 ionic liquid interface. We find that the liquid structure of [Bmim+] [PF6(-)] in the presence of CO2 is nearly identical to that in the neat ionic liquid (IL) even at fairly large mole fractions of CO2. Our simulations indicate, in agreement with experiments, that partial miscibilities of one fluid into the other are very unsymmetrical, CO2 being highly soluble in the ionic liquid phase while the ionic liquid is highly insoluble in the CO2 phase. We interpret our results in terms of the size and shape of spontaneously forming cavities in the ionic liquid phase, and we propose that CO2 occupies extremely well-defined locations in the IL. Even though our accurate prediction of cavity sizes in the neat IL indicates that these cavities are small compared with the van der Waals radius of a single carbon or oxygen atom, CO2 appears to occupy a space that was for the most part a priori "empty".

Journal Article↗

Conformational dynamics of sialyl Lewisx in aqueous solution and its interaction with selectinE. A study by molecular dynamics.

Three dimensional structures of sialyl Lewis(x) (SLe(x)) in aqueous solution and bound to selectinE are described based on an exhaustive conformational analysis and several long molecular dynamics simulations using different glycosidic regions as starting conformations. It appears from this study that when the oligosaccharide is free in solution the NeuNAcalpha(2-3)Gal segment favors glycosidic conformation in three different regions in the (Phi,Psi) plane with propensity of populations in the ratio 1:8:1. Each one of these structures is characteristically stabilized by specific hydrogen bonding interaction between NeuNAc and Gal. On the other hand, the Gal-GlcNAc-Fuc segment can exist in four different conformational states. Based on the topology of SLe(x) we are able to predict that out of all the allowed conformations in solution only two of these structures possess a geometry that would fit without steric clashes into the binding location of selectinE. In both of these binding modes, segment Gal-GlcNAc-Fuc adopts a unique conformation. The only difference between the two SLe(x) conformers that can successfully bind to selectinE is given by two possible regions in glycosidic space in the fragment NeuNAcalpha(2-3)Gal. A large conformational departure from the crystallographic data is observed for two lysine residues at the binding site of selectinE. These two residues play an important role when SLe(x) binds selectinE in aqueous solution. These findings help reconcile the X-ray data, in which these residues appear to be 1 nm away from SLe(x), with recent liquid NMR data reporting couplings between these protein residues and the sugar.

Crystallography, X-Ray↗

Hydrophobic collapse in multidomain protein folding.

We performed molecular dynamics simulations of the collapse of a two-domain protein, the BphC enzyme, into a globular structure to examine how water molecules mediate hydrophobic collapse of proteins. In the interdomain region, liquid water persists with a density 10 to 15% lower than in the bulk, even at small domain separations. Water depletion and hydrophobic collapse occur on a nanosecond time scale, which is two orders of magnitude slower than that found in the collapse of idealized paraffin-like plates. When the electrostatic protein-water forces are turned off, a dewetting transition occurs in the interdomain region and the collapse speeds up by more than an order of magnitude. When attractive van der Waals forces are turned off as well, the dewetting in the interdomain region is more profound, and the collapse is even faster.

Computer Simulation↗