Kinetics of Surfactant Adsorption at Fluid-Fluid Interfaces: Surfactant Mixtures

The adsorption at the interface between an aqueous solution of several surface-active agents and another fluid (air or oil) phase is addressed theoretically. We derive the kinetic equations from a variation of the interfacial free energy, solve them numerically and provide an analytic solution for the simple case of a linear adsorption isotherm. Calculating asymptotic solutions analytically, we find the characteristic time scales of the adsorption process and observe the behavior of the system at various temporal stages. In particular, we relate the kinetic behavior of the mixture to the properties of its individual constituents and find good agreement with experiments. In the case of kinetically limited adsorption, the mixture kinetics is found to be considerably different from that of the single-surfactant solutions because of strong coupling between the species.Comment: 19 pages, 7 figures, to be published in Langmui

Swelling of particle-encapsulating random manifolds

We study the statistical mechanics of a closed random manifold of fixed area and fluctuating volume, encapsulating a fixed number of noninteracting particles. Scaling analysis yields a unified description of such swollen manifolds, according to which the mean volume gradually increases with particle number, following a single scaling law. This is markedly different from the swelling under fixed pressure difference, where certain models exhibit criticality. We thereby indicate when the swelling due to encapsulated particles is thermodynamically inequivalent to that caused by fixed pressure. The general predictions are supported by Monte Carlo simulations of two particle-encapsulating model systems -- a two-dimensional self-avoiding ring and a three-dimensional self-avoiding fluid vesicle. In the former the particle-induced swelling is thermodynamically equivalent to the pressure-induced one whereas in the latter it is not.Comment: 8 pages, 6 figure

Nanoscale surface relaxation of a membrane stack

Recent measurements of the short-wavelength (~ 1--100 nm) fluctuations in stacks of lipid membranes have revealed two distinct relaxations: a fast one (decay rate of ~ 0.1 ns^{-1}), which fits the known baroclinic mode of bulk lamellar phases, and a slower one (~ 1--10 \mu s^{-1}) of unknown origin. We show that the latter is accounted for by an overdamped capillary mode, depending on the surface tension of the stack and its anisotropic viscosity. We thereby demonstrate how the dynamic surface tension of membrane stacks could be extracted from such measurements.Comment: 4 page

Stability of Quasicrystals Composed of Soft Isotropic Particles

Quasicrystals whose building blocks are of mesoscopic rather than atomic scale have recently been discovered in several soft-matter systems. Contrary to metallurgic quasicrystals whose source of stability remains a question of great debate to this day, we argue that the stability of certain soft-matter quasicrystals can be directly explained by examining a coarse-grained free energy for a system of soft isotropic particles. We show, both theoretically and numerically, that the stability can be attributed to the existence of two natural length scales in the pair potential, combined with effective three-body interactions arising from entropy. Our newly gained understanding of the stability of soft quasicrystals allows us to point at their region of stability in the phase diagram, and thereby may help control the self-assembly of quasicrystals and a variety of other desired structures in future experimental realizations.Comment: Revised abstract, more detailed explanations, and better images of the numerical minimization of the free energ

Mating rituals of the Spotted Turtle

This is where the abstract of this record would appear. This is only demonstration data

Correlated particle dynamics in concentrated quasi-two-dimensional suspensions

We investigate theoretically and experimentally how the hydrodynamically correlated lateral motion of particles in a suspension confined between two surfaces is affected by the suspension concentration. Despite the long range of the correlations (decaying as 1/r^2 with the inter-particle distance r), the concentration effect is present only at short inter-particle distances for which the static pair correlation is nonuniform. This is in sharp contrast with the effect of hydrodynamic screening present in unconfined suspensions, where increasing the concentration changes the prefactor of the large-distance correlation.Comment: 13 page

The structure of the cytoplasmic dynein tail

Cytoplasmic dynein is a molecular motor that moves cargos along microtubules. Dynein, together with its large co-factor dynactin, is responsible for the vast majority of traffic towards the centre of the cell. The largest subunit of the dynein complex is called the dynein heavy chain (DHC). The DHC includes a C-terminal motor domain, which converts ATP hydrolysis into mechanical force, an N-terminal tail domain, and a flexible linker domain to join the two together. An intermediate chain (DIC) and light intermediate chain (DLIC) bind directly to the DHC tail, while light chains (DLCs) bind to the DIC. This tail complex is important for both cargo binding as well as homodimerisation of the DHC, which is necessary for processive movement. Previous studies suggest that the DLCs play an important role in homodimerisation, but it remains unclear how else the DHCs are held together. Using S. cerevisiae as a model system, I co-expressed all four dynein subunits and purified functional dynein motors. In this background, I found that truncating the DHC to include only the first 1004 residues (out of the total 4092) eliminates the motor domain as well as the flexible linker domain, while preserving binding to the DIC, DLIC and DLC. However, truncating just another 50 residues off of the C-terminus led to a loss of all accessory subunits. I developed a protocol for expressing and purifying large quantities of the 1004 residue construct, thus I provide the first description of a recombinant dynein tail domain. Using negative stain electron microscopy (EM), I also present the first 3D structural information for the tail region of the cytoplasmic dynein motor. I then describe a construct including only the first 557 residues of the DHC, which dimerises despite not being able to bind any of the other subunits. I present a crystal structure of this smaller DHC fragment, which shows that the N-terminal 180 residues of the DHC constitute an intricate dimerisation domain made up of a β-sheet sandwiched between α-helices. Not only is this the first crystal structure of any part of the DHC N-terminus, but it reveals a previously undocumented dimerisation domain within the DHC itself. Furthermore, information garnered from this crystal structure allowed for interpretation of a recent cryo-EM structure of a triple complex containing the dynein tail, dynactin and the cargo adaptor BICD2 (TDB) that was solved by my colleagues in the Carter group. Only by docking the DHC N-terminus crystal structure within the TDB EM density did it become clear that the N-terminus of the DHC is responsible for the majority of the contacts the dynein tail makes with both dynactin and BICD2. Therefore the work that I present here sheds new light on the unexpected importance of the DHC N-terminus and allows two important conclusions to be made. First, the N-terminal 180 residues of the DHC constitute a dimerisation domain of its own. Second, the next ~400 residues of the DHC form a domain that plays a key role in the complex interface between dynein, dynactin and BICD2.This work was funded by the Medical Research Council, UK (grant number MC_UP_A025_1011) and the Cambridge Overseas Trust, UK

A combination of high concentrations of serum triglyceride and non-high-density-lipoprotein-cholesterol is a risk factor for cardiovascular disease in subjects with abnormal glucose metabolism - The Hoorn Study

Aims/hypothesis. Type 2 diabetes is not only associated with hyperglycaemia, but also with disorders of lipid metabolism. The aim of this study was to investigate the association of triglyceride and non-HDL-cholesterol concentrations with cardiovascular disease in subjects with normal and abnormal glucose metabolism. Methods. Subjects were 869 men and 948 women aged 50 to 75 who participated in the Hoorn Study, a population-based cohort study that started in 1989. Glucose metabolism was determined by a 75 g OGTT. High fasting triglyceride and non-HDL-cholesterol concentrations were defined as above the median of the study population. Results. After 10 years of follow-up, the age- and sex-adjusted hazard ratios for cardiovascular disease were 1.35 (1.11-1.64) and 1.71 (1.40-2.08) for high triglycerides and high non-HDL-cholesterol, respectively, after mutual adjustment. After stratification for glucose metabolism status, the hazard ratios for cardiovascular disease for non-HDL-cholesterol were 1.70 (1.31-2.21) in normal glucose metabolism and 1.56 (1.12-2.18) in abnormal glucose metabolism. Triglycerides were not a risk factor in subjects with normal glucose metabolism, with a hazard ratio of 0.94 (0.73-1.22), but in subjects with abnormal glucose metabolism, the hazard ratio for cardiovascular disease was 1.54 (1.07-2.22). In subjects with abnormal glucose metabolism, the hazard ratio for the combined presence of high triglycerides and non-HDL-cholesterol was 2.12 (1.35-3.34). Conclusion. Our data suggest that in people with abnormal glucose metabolism, but not in those with normal glucose metabolism, high triglyceride concentration could be associated with the risk of cardiovascular disease, particularly in people with high non-HDL-cholesterol