Extended frequency range depolarized light scattering study of N-acetyl-leucine-methylamide-water solutions

We have studied the influence of the amphiphilic model peptide N-acetyl-leucine-methylamide (NALMA) on the dynamics of water using extended frequency range depolarized light scattering (EDLS), between 0.3 GHz and 36 THz. This technique allowed us to separate solute from solvent dynamics and bulk from hydration water, providing both characteristic times and relative fractions. In the temperature range 5-65 °C, a retardation factor from 9 to 7 is found for water hydrating NALMA. Moreover, in the same range, a hydration number from 62 to 50 is observed, corresponding to more than two hydration layers. This strong perturbation suggests the existence of a collective effect of amphiphilic molecules on surrounding water molecules.     

The density dependence of the depolarized light scattering at high frequencies in rare gas fluids

Measurements of the depolarized light scattering spectra of venon at densities between 0.3 and 2.65 times the critical density are presented. The second moments are compared with the second moments of the scattering functions S(k, ω) of argon at corresponding densities. A conclusion is drawn about the wavevector of the modes that contribute to the high-frequency part of the spectra that are observed at high, liquid densities.     

Reorientational motion and orientational correlation functions in weakly associated organic liquids by depolarized Rayleigh scattering

Depolarized Rayleigh scattering of weakly associated organic liquids was investigated, giving the reorientational correlation of molecules. There is a high probability for reversal of the initial direction of angular velocity during collisions. This behaviour can be explained as librational motion damped by the diffusional mechanism.     

Polarized and depolarized dynamic light scattering of concentrated polystyrene solutions

Polarized and depolarized dynamic light scattering have been used to examine the dynamics of concentrated polystyrene solutions in dioctyl phthalate and toluene. Time-temperature superposition of the depolarized intensity correlation functions gave master curves covering more than 10 decades on the time scale. Polarized correlation functions are resolved into relaxational and diffusive components having different temperature dependences. When the relaxation rate of the concentration fluctuations approaches the reorientational relaxation rate, the concentration fluctuations become q-independent i.e. the diffusional relaxation is rate-determined by the backbone mobility. With a small molecule solvent as toluene, however, a part of the concentration fluctuations relaxes faster than the orientational relaxation, i.e., the diffusion occurs in the free volume within the “frozen” network.     

Effect of solvent on depolarized light scattering in dilute polymer solutions

An optical model of a system in which both polymer segments and solvent molecules are described as point dipoles has been used to calculate the intensity of light depolarized in scattering. The final expression consists of six terms, the physical meaning of which is briefly discussed. An approximation procedure has been worked out for the calculation of two interaction terms due to deviations of the local field in solution from the Lorentz–Lorenz field; the terms have been calculated for simple models of flexible and rigid molecules. Their dependence on molecular weight appears to be approximately the same as the intrinsic anisotropy of the polymer molecule; their contribution is nonzero even for a solvent isorefractive with the polymer.     

In situ measurements of nanotube dimensions in suspensions by depolarized dynamic light scattering

We show that the dimensions of carbon nanotubes (CNTs) in suspension can be characterized by depolarized dynamic light scattering. Taking advantages of this in situ technique, we investigate in detail the influence of sonication procedures on the length and diameter of CNTs in surfactant solutions. Sonication power is shown to be particularly efficient at unbundling nanotubes, whereas a long sonication time at low power can be sufficient to cut the bundles with limited unbundling. We finally demonstrate the influence of CNT dimensions on the electrical properties of CNT fibers. Slightly varying the sonication conditions, and thereby the suspended nanotube dimensions, can affect the fibers conductivity by almost 2 orders of magnitude.     

Low frequency motions of water isolated in low temperature matrices

Far infrared spectra of monomer H₂O, D₂O, HOD in argon and nitrogen and of H₂O in krypton and methane are recorded at different temperatures. Assignments of the bands to rotational and translational motions are given for argon and krypton on the basis of rotational constants, derived from mid infrared vibration rotation matrix spectra. Motions of water in nitrogen are interpreted as librations around the OH bond axes, because the HOD spectra do not fit the picture of librations around the proper rotational axes.     

Influence of the potential on the intensity of depolarized light scattering ; in dense liquid argon

The depolarized light scattering intensity of argon at the triple point is calculated by molecular dynamics using the two-body Bobetic-Barker potential. The result differs from that obtained with a Lennard-Jones potential by no more than 15%.     

The three-body correlation spectral moments in depolarized interaction-induced light scattering of H2 at 297 K

The three-body correlation spectral moments of depolarized interaction-induced light scattering have been measured in normal H₂ at 297 K by means of an analysis of the density behaviour of the spectra between 10 and 300 cm⁻¹. Comparison with classical calculation shows a major discrepancy for the second moment which is attributed to the anisotropic properties of the interacting molecules.     

A consideration of orientational correlation functions,time-dependent distribution functions and pictorial representations of the orientational motions of molecules.

The relationships between experimental quantities which arise due to the dynamics of molecules and the underlying time-correlation functions and time-dependent distribution functions are considered, with special emphasis being given to reorientational motions as detected by dielectric and closely related techniques. It is shown that pictorial representations of angular motion (small-step diffusion, free rotation, collision-interrupted rotation) may be given in terms of three and two dimensional diagrams of the time-dependent orientation distribution functions and that these afford a physical insight and appreciation of the averaged motions of ensembles of molecules.     

Time evolution of density fluctuation in supercritical region. I. Non-hydrogen-bonded fluids studied by dynamic light scattering

The time evolution of the density fluctuation of molecules inhomogeneously dispersing in a mesoscopic volume is investigated by dynamic light scattering in several fluids in supercritical states. This study is the first time-domain investigation to compare the dynamics of density fluctuation among several fluids. The samples used are non-hydrogen-bonded fluids in the supercritical states: CHF(3), C(2)H(4), CO(2), and xenon. These four molecules have different properties but are of similar size. Under these conditions, the relationship between dynamic and static density inhomogeneities is studied by measuring the time correlation function of the density fluctuation. In all cases, this function is characterized by a single exponential function, decaying within a few microseconds. While the correlation times in the four fluids show noncoincidence, those values agree well with each other when scaled to a dimensionless parameter. From the results of this scaling based on the Kawasaki theory and Landau-Placzek theory, the relation between dynamics and static structures is analyzed, and the following four insights are obtained: (i) viscosity is the main contributor to the time evolution of density fluctuation; (ii) the principle of corresponding state is observed by the use of time-domain data; (iii) the Kawasaki theory and the Landau-Placzek theory are confirmed to be applicable to polar, nonpolar, and nondipolar fluids that have no hydrogen bonding, at temperatures relatively far from critical temperature; and (iv) the density fluctuation correlation length and the value of density fluctuation are estimated from the time-domain data and agree with the values from other experiments and calculations.     

Shear small-angle light scattering studies of shear-induced concentration fluctuations and steady state viscoelastic properties

We aimed at elucidating the influence of shear-induced structures (shear-enhanced concentration fluctuations and/or shear-induced phase separation), as observed by rheo-optical methods with small-angle light scattering under shear flow (shear-SALS) and shear-microscopy, on viscoelastic properties in semidilute polystyrene (PS) solutions of 6.0 wt % concentration using dioctyl phthalate (DOP) as a Theta solvent and tricresyl phosphate (TCP) as a good solvent. In order to quantify the effects of the shear-induced structures, we conducted a numerical analysis of rheological properties in a homogeneous solution based on the constitutive equation developed by Kaye-Bernstein, Kearsley, and Zapas (K-BKZ). In the low-to-intermediate shear rate gamma region between tau(w) (-1) and tau(e) (-1), where tau(w) and tau(e) are, respectively, terminal relaxation time and the relaxation time for chain stretching, the steady state rheological properties, such as shear stress sigma and the first normal stress difference N(1), for the PS/DOP and PS/TCP solutions are found to be almost same and also well predicted by the K-BKZ equation, in spite of the fact that there is a significant difference in the shear-induced structures as observed by shear-SALS and shear-microscopy. This implies that the contribution of the concentration fluctuations built up by shear flow to the rheological properties seems very small in this gamma region. On the other hand, once gamma exceeds tau(e) (-1), sigma and N(1) for both PS/DOP and PS/TCP start to deviate from the predicted values. Moreover, when gamma further increases and becomes higher than gamma(a,DOP) (sufficiently higher than tau(e) (-1)), above which rheological and scattering anomalies are observed for PS/DOP, sigma and N(1) for PS/DOP and PS/TCP are significantly larger than those predicted by K-BKZ. Particularly, a steep increase of sigma and N(1) for PS/DOP above gamma(a,DOP) is attributed to an excess free energy stored in the system via the deformation of interface of well-defined domains, which are aligned into the stringlike structure developed parallel to the flow axis, and stretching of the chains connecting the domains in the stringlike structures. Thus, we advocate that the effect of shear-induced structures should be well considered on the behavior of sigma and N(1) at the high gamma region above tau(e) (-1) in semidilute polymer solutions.     

Study of the low-frequency motions in poly(ethylene terephthalate) (PET) by neutron inelastic scattering

By neutron inelastic scattering, a complex low-frequency spectrum is obtained for PET. This is attributed to the complicated structure of the monomer unit, a large number of intramolecular modes being possible. Most of them were identified using infrared and Raman data. Some indication of the presence of intermolecular modes below 200 cm^?1 was found in the dependence of resolution and intensity on temperature in this frequency domain. The existence of these intermolecular modes was further supported by the spectra obtained from oriented or annealed crystalline samples.     

Low angle laser light scattering and photon correlation spectroscopy in surfactant vesicles

Using low angle laser light scattering, weight averaged molecular weights, M?_w, diffusion coefficients, and hydrodynamic radii, R_H, have been determined for completely synthetic surfactant vesicles, prepared by ultrasonic irradiation of dioctadecyldimethylammonium chloride. DODAC, and dihexadecylphosphate. DHP dispersion. Both the M?_w and R_H values were found to decrease exponentially as a function of sonication time. At the limit, M?_w and R_H for DODAC vesicles are 12.6 × 10⁶ dalton and 396 Å, and those for DHP vesicles are 23 × 10⁶ dalton and 595 Å. Calculations indicate both vesicles to be prolates.     

Collective membrane motions of high and low amplitude, studied by dynamic light scattering and micro-interferometry

Undulations of lipid bilayers were experimentally studied for the two limiting cases of high and weak lateral tension using two well established model systems: freely suspended planar lipid bilayers, so-called black lipid membranes (BLM) for high-tension studies and large unilamellar vesicles (LUV) for measurements at weak tension. This variation in tension results in changes of undulation amplitudes from several hundred nm (LUV) down to 1 nm (BLM), thus requiring different physical methods for their detection. We have employed microinterferometric techniques (RICM) for studying the regime of weak tension and dynamic light scattering (DLS) for that of high tension. The dedicated DLS set-up allowed the measurements of undulations over a wide wave vector range of 250 < q/cm-1 < 35,000 cm-1. This enabled the observation of collective membrane modes in two regimes, the oscillating one at low q and the overdamped regime at high q. The transition between both regimes at the bifurcation point is rather abrupt and depends on the lateral tension of the bilayer, as is demonstrated by comparing the dispersion curves of pure lipid and of lipid-cholestrol BLMs over the same q-range. The DLS measurements allowed a critical test of a hydrodynamic theory of the dispersion behaviour of membrane collective modes under tension. The DLS measurements are compared with RICM results of undulatory excitations of giant vesicles weakly adhering to substrates in the 10(-6)-2.5 x 10(-7) m wavelength regime and at low frequencies (0.1-25 Hz). Experimental evidence for the strong decrease in the relaxation rate by the hydrodynamic coupling of the membrane with the wall is established.     

Micellar structures of block‐copolymers with ordered cores in dilute solution as studied by polarized and depolarized light scattering

The hierarchical self‐assembly behaviors of a series of amphiphilic liquid crystalline block copolymers (pEG_mAz_n), consisting of poly(ethylene glycol) (pEG) block and liquid crystalline polymer block (pAz) of poly{11‐[4‐(4‐butylphenylazo) phenoxy]‐undecyl methacrylate} containing an azobenzenzene mesogen, in the selective solvent diethyleneglycol, which is good for pEG block, were studied by polarized and depolarized light scattering. It was found that these copolymers can form micellar particles with internal ordered structures of optical anisotropy. Depending on the relative lengths of the blocks, the obtained micellar structures show optical anisotropies with different geometrical anisotropies. The higher composition of pAz‐core blocks leads to the larger aggregate. The lower‐molecular‐weight copolymers tend to form the long and thin strings, which show rather the larger size with larger aggregation number. Even at the similar composition of pAz‐core block, copolymers with different chain lengths can form the core of the different aggregating structures with the different molecular orientations. It was also found that the addition of a small amount of the surfactant, C₁₂E₂₅, makes the string‐like aggregate shorter. © 2007 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 45: 1333–1343, 2007     

Static light scattering from poly(ethylene oxide) in methanol

Static light scattering measurements were performed on dilute solutions of monodisperse poly(ethylene oxide) (PEO) in methanol at 25°C. PEOs of five different molecular weights ranging from nominal M_w = 8.6 × 10⁴ to 9.13 × 10⁵ were used. Linear Zimm plots were obtained for all the PEO samples: no downturn was observed at small angles, indicating that no large aggregates of PEO molecules exist in the solution. From the plots, values of the weight-average molecular weight, M_w, the radius gyration, R_G, and the second virial coefficient, A₂, were successfully determined for respective PEOs. Observed relationship between R_G and M_w indicates that methanol is certainly a good solvent for the polymer. © 1996 John Wiley & Sons, Inc.