Transport passif

Résumé

Passive transport is a type of membrane transport that does not require energy to move substances across cell membranes. Instead of using cellular energy, like active transport, passive transport relies on the second law of thermodynamics to drive the movement of substances across cell membranes. Fundamentally, substances follow Fick's first law, and move from an area of high concentration to one of low concentration because this movement increases the entropy of the overall system. The rate of passive transport depends on the permeability of the cell membrane, which, in turn, depends on the organization and characteristics of the membrane lipids and proteins. The four main kinds of passive transport are simple diffusion, facilitated diffusion, filtration, and/or osmosis. Passive transport follows Fick's first law. Diffusion Diffusion is the net movement of material from an area of high concentration to an area with lower concentration. The difference of concentration between the two areas is often termed as the concentration gradient, and diffusion will continue until this gradient has been eliminated. Since diffusion moves materials from an area of higher concentration to an area of lower concentration, it is described as moving solutes "down the concentration gradient" (compared with active transport, which often moves material from area of low concentration to area of higher concentration, and therefore referred to as moving the material "against the concentration gradient"). However, in many cases (e.g. passive drug transport) the driving force of passive transport can not be simplified to the concentration gradient. If there are different solutions at the two sides of the membrane with different equilibrium solubility of the drug, the difference in the degree of saturation is the driving force of passive membrane transport. It is also true for supersaturated solutions which are more and more important owing to the spreading of the application of amorphous solid dispersions for drug bioavailability enhancement.

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https://fr.wikipedia.org/wiki/Transport_passif

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Publications associées (2)

Concepts associés (18)

Cours associés (10)

Séances de cours associées (53)

MOOCs associés (2)

Hydrated lipid bilayer membranes and their asymmetry play a fundamental role in living cells by maintaining and regulating concentration gradients between cells, their environment, and their compartments. They achieve this not only through various channels and transporters, but also by being inherently semi-permeable to various molecules, including water and ions. However, molecular information about passive ion transport, as well as the complex structure of membrane hydration remain elusive, mainly due to a lack of experimental methods that can access this information, and relate it to micro- and macroscopic membrane properties. In this work, we study the molecular structure of lipid bilayer membranes and ion transport across them with high throughput wide-field second harmonic (SH) microscopy by utilizing water as the contrast agent. We show that by detecting small amounts of asymmetry in the structure of interfacial water, it is possible to measure the distribution of charged species across the membrane with high sensitivity. We apply this surface-selective technique to measure ion-lipid-water interactions, track ion transport, and quantify electro-chemical surface properties at the interfaces of lipid bilayer membranes in the form of giant unilamellar vesicles (GUVs). We start by improving the throughput of wide field SH microscopy in order to probe low-asymmetry interfaces with high contrast in a label-free manner. To do this, we design a custom optical parametric amplifier (OPA) with a tunable output in the 670-1000 nm range, up to a 1 MHz repetition rate, and an ultra-short 23 fs pulse duration. We then experimentally demonstrate the achieved throughput improvement. Next, we establish a way to probe interfacial hydration of GUVs. We quantify the surface properties of vesicles composed of different ratios of zwitterionic and anionic lipids, and show that only a few percent of anionic headgroups are ionized. We also observe spatial and temporal fluctuations in surface properties, and demonstrate that these fluctuations are universally found in lipid bilayer systems.Following that, we demonstrate a direct link between membrane potential fluctuations and divalent ion transport. Molecular dynamics simulations reveal that these fluctuations reduce the free energy cost of transient pore formation and increase the ion flux across an open pore. These transient pores can act as conduits for ion transport, which we SH image for a series of divalent cations (Cu2+, Ca2+, Ba2+, Mg2+) passing through GUV membranes. Combining the experimental and computational results, we show that permeation through pores formed via an ion-induced electrostatic field is a viable mechanism for unassisted ion transport.Then, we focus on unassisted Ca2+ translocation in more detail. We vary the hydrophobic core of bilayer membranes and observe different types of behavior in high throughput wide-field SH images. Ca2+ translocation is observed through mono-unsaturated membranes, significantly reduced upon adding cholesterol, and completely inhibited for branched and poly-unsaturated membranes. We propose, using molecular dynamics simulations, that ion transport occurs through ion induced transient pores, which require non-equilibrium membrane restructuring. This results in different transport rates at different locations and suggests that the hydrophobic structure of lipids plays a much more sophisticated regulating role than previously thought.

EPFL2022

Single-molecule motions of oligoarginine transporter conjugates on the plasma membrane of Chinese hamster ovary cells

Hui Wang

To explore the real-time dynamic behavior of molecular transporters of the cell-penetrating-peptide (CPP) type on a biological membrane, single fluorescently labeled oligoarginine conjugates were imaged interacting with the plasma membrane of Chinese hamster ovary (CHO) cells. The diffusional motion on the membrane, characterized by single-molecule diffusion coefficient and residence time (tau R), defined as the time from the initial appearance of a single-molecule spot on the membrane (from the solution) to the time the single molecule disappears from the imaging focal plane, was observed for a fluorophore-labeled octaarginine (a model guanidinium-rich CPP) and compared with the corresponding values observed for a tetraarginine conjugate (negative control), a lipid analogue, and a fluorescently labeled protein conjugate (transferrin-Alexa594) known to enter the cell through endocytosis. Imaging of the oligoarginine conjugates was enabled by the use of a new high-contrast fluorophore in the dicyanomethylenedihydrofuran family, which brightens upon interaction with the membrane at normal oxygen concentrations. Taken as a whole, the motions of the octaarginine conjugate single molecules are highly heterogeneous and cannot be described as Brownian motion with a single diffusion coefficient. The observed behavior is also different from that of lipids, known to penetrate cellular membranes through passive diffusion, conventionally involving lateral diffusion followed by membrane bilayer flip-flop. Furthermore, while the octaarginine conjugate behavior shares some common features with transferrin uptake (endocytotic) processes, the two systems also exhibit dissimilar traits when diffusional motions and residence times of single constructs are compared. Additionally, pretreatment of cells with cytochalasin D, a known actin filament disruptor, produces no significant effect, which further rules out unimodal endocytosis as the mechanism of uptake. Also, the involvement of membrane potential in octaarginine-membrane interaction is supported by significant changes in the motion with high [K(+)] treatment. In sum, this first study of single transporter motion on the membrane of a living cell indicates that the mode by which the octaarginine transporter penetrates the cell membrane appears to either be a multimechanism uptake process or a mechanism different from unimodal passive diffusion or endocytosis.

2008