The dynamic solvation of the fluorescent probe, coumarin 153, is measured in five room-temperature ionic liquids using different experimental techniques and methods of data analysis. With time-resolved stimulatedemission and time-correlated single-photon counting techniques, it is found that the solvation is comprised of an initial rapid component of ∼55 ps. In all the solvents, half or more of the solvation is completed within 100 ps. The remainder of the solvation occurs on a much longer time scale. The emission spectra of coumarin 153 are nearly superimposable at all temperatures in a given solvent unless they are obtained using the supercooled liquid, suggesting that the solvents have an essentially glassy nature. The physical origin of the two components is discussed in terms of the polarizability of the organic cation for the faster one and the relative diffusional motion of the cations and the anions for the slower one. A comparison of the solvation response functions obtained from single-wavelength and from spectral-reconstruction measurements is provided. Preliminary fluorescence-upconversion measurements are presented against which the appropriateness of the single-wavelength method for constructing solvation correlation functions and the use of stimulated-emission measurements is considered. These measurements are consistent with the trends mentioned above, but a comparison indicates that the presence of one or more excited states distorts the stimulated-emission kinetics such that they do not perfectly reproduce the spontaneous emission data. Fluorescence-upconversion results indicate an initial solvation component on the order of ∼7 ps. December 2, 2003; In Final Form: April 20, 2004 The dynamic solvation of the fluorescent probe, coumarin 153, is measured in five room-temperature ionic liquids using different experimental techniques and methods of data analysis. With time-resolved stimulatedemission and time-correlated single-photon counting techniques, it is found that the solvation is comprised of an initial rapid component of ∼55 ps. In all the solvents, half or more of the solvation is completed within 100 ps. The remainder of the solvation occurs on a much longer time scale. The emission spectra of coumarin 153 are nearly superimposable at all temperatures in a given solvent unless they are obtained using the supercooled liquid, suggesting that the solvents have an essentially glassy nature. The physical origin of the two components is discussed in terms of the polarizability of the organic cation for the faster one and the relative diffusional motion of the cations and the anions for the slower one. A comparison of the solvation response functions obtained from single-wavelength and from spectral-reconstruction measurements is provided. Preliminary fluorescence-upconversion measurements are presented against which the appropriateness of the single-wavelength method for constructing solvation correlation functions and the use of stimulated-emission measurements is considered. These...

Cell-derived GPMVs (giant plasma-membrane vesicles) enable investigation of lipid phase separation in a system with appropriate biological complexity under physiological conditions, and in the present study were used to investigate the cholesterol-dependence of domain formation and stability. The cholesterol level is directly related to the abundance of the liquid-ordered phase fraction, which is the majority phase in vesicles from untreated cells. Miscibility transition temperature depends on cholesterol and correlates strongly with the presence of detergent-insoluble membrane in cell lysates. Fluorescence correlation spectroscopy reveals two distinct diffusing populations in phase-separated cell membrane-derived vesicles whose diffusivities correspond well to diffusivities in both model systems and live cells. The results of the present study extend previous observations in purified lipid systems to the complex environment of the plasma membrane and provide insight into the effect of cholesterol on lipid phase separation and abundance.

Even though nanostructures of various shapes and sizes can be controlled by microemulsions, there is substantial difficulty in understanding their growth mechanism. The evolution of nanostructures from the time of mixing of reactants to their final stage is a heterogeneous process involving a variety of intermediates. To obtain a deeper insight into these kinetic steps, we studied the slow growth kinetics (extending over eight days) of iron oxalate nanorods inside the polar core of water-in-oil microemulsion droplets made of cetyltrimethylammonium bromide/1-butanol/isooctane. Fluorescence correlation spectroscopy (FCS), dynamic light scattering (DLS), and transmission electron microscopy (TEM) have been employed to monitor the nanostructure growth at (near) the single-droplet level and in an ensemble. Analyzing FCS data with suitable kinetic model we obtain transient dimer lifetime (28 μs) and the droplet fusion rates (and fusion tendency) on each day as the reaction proceeds. The droplet fusion rate is found to directly control the nanorod growth in microemulsion solution and attains its maximum value (3.55 × 10(4) s(-1)) on day 6, when long nanorods are found in TEM data, implying that more and more reactants are fed into the growing system at this stage. Combining FCS, DLS, and TEM results, we find three distinct periods in the entire growth process: a long nucleation-dominant nanoparticle growth period which forms nanoparticles of critical (average) size of ∼53 nm, followed by a short period where isotropic nanoparticles switch to anisotropic growth to form nanorods, and finally elongation of nanorods and growth (and shrinking) of nanoparticles.

Macromolecular crowding is one of the key characteristics of the cellular environment and therefore, is intimately coupled to the process of protein folding in vivo. While previous studies have provided invaluable insight into the effect of crowding on the stability and folding rate of protein tertiary structures, very little is known about how crowding affects protein folding dynamics at the secondary structure level. Herein, we examine the thermal stability and folding-unfolding kinetics of three small folding motifs, i.e., a 34-residue α-helix, a 34-residue cross-linked helix-turn-helix, and a 16-residue β hairpin, in the presence of two commonly used crowding agents, Dextran 70 (200 g/L) and Ficoll 70 (200 g/L). We find that these polymers do not induce any appreciable changes in the folding kinetics of the two helical peptides, which is somewhat surprising as the helix-coil transition kinetics have been shown to depend on viscosity. Also to our surprise and in contrast to what has been observed for larger proteins, we find that crowding leads to an appreciable decrease in the folding rate of the shortest β-hairpin peptide, indicating that besides the excluded volume effect, other factors also need to be considered when evaluating the net effect of crowding on protein folding kinetics. A model considering both the static and dynamic effects arising from the presence of the crowding agent is proposed to rationalize these results.

The amide I' band of a polypeptide is sensitive not only to its secondary structure content but also to its environment. In this study we show how degrees of hydration affect the underlying spectral features of the amide I' band of two alanine-based helical peptides. This is achieved by solubilizing these peptides in the water pool of sodium bis(2-ethylhexyl)sulfosuccinate reverse micelles with different water contents or w0 values. In agreement with several earlier studies, our results show that the amide I' band arising from a group of dehydrated helical amides is centered at approximately 1650 cm-1, whereas hydration shifts this frequency toward lower wavenumbers. More importantly, temperature-dependent infrared studies further show that these helical peptides undergo a thermally induced conformational transition in reverse micelles of low w0 values (e.g., w0=6), resulting in soluble peptide aggregates rich in antiparallel beta-sheets. Interestingly, however, increasing w0 or water content leads to an increase in the onset temperature at which such beta-aggregates begin to form. Therefore, these results provide strong evidence suggesting that dehydration facilitates aggregate formation and that removal of water imposes a free energy barrier to peptide association and aggregation, a feature that has been suggested in recent simulation studies focusing on the mechanism of beta-amyloid formation.

It is well known that water plays a crucial role in the folding, dynamics and function of proteins. Here we provide further evidence showing that the aggregation kinetics of peptides also depend strongly on their hydration status. Using reverse micelles as a tool to modulate the accessible number of water molecules and infrared spectroscopy and transmission electron microscopy as means to monitor aggregate formation, we show that the rate of aggregation of two amyloid forming peptides increases significantly under conditions where limited hydration of the peptide molecule is expected to occur. These results are not only in accord with recent computer simulations indicating that the expulsion of interfacial water molecules is a key event in the dimerization/oligmerization of amyloid β (Aβ) peptides, but also have implications for amyloid formation in vivo where molecular crowding is expected to influence the solvation status of proteins.

Sperm whale myoglobin (Mb) and soybean leghemoglobin (Lba) are two small, monomeric hemoglobins that share a common globin fold but differ widely in many other aspects. Lba has a much higher affinity for most ligands, and the two proteins use different distal and proximal heme pocket regulatory mechanisms to control ligand binding. Removal of the constraint provided by covalent attachment of the proximal histidine to the F-helices of these proteins decreases oxygen affinity in Lba and increases oxygen affinity in Mb, mainly because of changes in oxygen dissociation rate constants. Hence, Mb and Lba use covalent constraints in opposite ways to regulate ligand binding. Swapping the F-helices of the two proteins brings about similar effects, highlighting the importance of this helix in proximal heme pocket regulation of ligand binding. The F7 residue in Mb is capable of weaving a hydrogen-bonding network that holds the proximal histidine in a fixed orientation. On the contrary, the F7 residue in Lba lacks this property and allows the proximal histidine to assume a conformation favorable for higher ligand binding affinity. Geminate recombination studies indicate that heme iron reactivity on picosecond timescales is not the dominant cause for the effects observed in each mutation. Results also indicate that in Lba the proximal and distal pocket mutations probably influence ligand binding independently. These results are discussed in the context of current hypotheses for proximal heme pocket structure and function.

Reverse micelles formed by sodium bis(2-ethylhexyl) sulfosuccinate (AOT) in isooctane (IO) and water have long been used as a means to provide a confined aqueous environment for various applications. In particular, AOT reverse micelles have often been used as a template to mimic membrane-water interfaces. While earlier studies have shown that membrane-binding peptides can indeed be incorporated into the polar cavity of AOT reverse micelles where they mostly fold into an alpha-helical structure, the underlying interactions leading to the ordered conformation are however not well understood. Herein, we have used circular dichroism (CD) and infrared (IR) spectroscopies in conjunction with a local IR marker (i.e., the CN group of a non-natural amino acid, p-cyano-phenylalanine) and a global IR reporter (i.e., the amide I' band of the peptide backbone) to probe the conformation as well as the hydration status of an antimicrobial peptide, mastoparan x (MPx), in AOT reverse micelles of different water contents. Our results show that at, w0=6, MPx adopts an alpha-helical conformation with both the backbone and hydrophobic side chains mostly dehydrated, whereas its backbone becomes partially hydrated at w0=20. In addition, our results suggest that the amphipathic alpha-helix so formed orients itself in such a manner that its positively charged, lysine-rich, hydrophilic face points toward the negatively charged AOT head groups, while its hydrophobic face is directed toward the polar interior of the water pool. This picture is in marked contrast to that observed for the binding of MPx to phospholipid bilayers wherein the hydrophobic surface of the bound alpha-helix is buried deeper into the membrane interior.