Searcharxiv⌕ Search

arXiv · physics/0510220

Structural Transition of Actin Filament in a Cell-Sized Water Droplet with a Phospholipid Membrane

Abstract

Actin filament, F-actin, is a semiflexible polymer with a negative charge, and is one of the main constituents on cell membranes. To clarify the effect of cross-talk between a phospholipid membrane and actin filaments in cells, we conducted microscopic observations on the structural changes in actin filaments in a cell-sized (several tens of micrometers in diameter) water droplet coated with a phospholipid membrane such as phosphatidylserine (PS; negatively-charged head group) or phosphatidylethanolamine (PE; neutral head group) as a simple model of a living cell membrane. With PS, actin filaments are distributed uniformly in the water phase without adsorption onto the membrane surface between 2 and 6 mM Mg2+, while between 6 and 12 mM Mg2+, actin filaments are adsorbed onto the inner membrane surface. With PE, actin filaments are uniformly adsorbed onto the inner membrane surface between 2 and 12 mM Mg2+. With both PS and PE membranes, at Mg2+ concentrations higher than 12 mM, thick bundles are formed in the bulk water droplet accompanied by the dissolution of actin filaments from the membrane surface. The attraction between actin filaments and membrane is attributable to an increase in the translational entropy of counterions accompanied by the adsorption of actin filaments onto the membrane surface. These results suggest that a microscopic water droplet coated with phospholipid can serve as an easy-to-handle model of cell membranes.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

M. Hase, K. Yoshikawa. 2005-10-25. Structural Transition of Actin Filament in a Cell-Sized Water Droplet with a Phospholipid Membrane. https://doi.org/10.1063/1.2174004

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Unravelling carbene moiety role in the N-heterocyclic carbene-phosphinidenes coordination chemistry: bonding and reactivity in gold chemistry

The coordination properties of the emerging class of N-heterocyclic carbene-phosphinidene (NHCP) ligands have been reported to be strongly affected by the carbene (NHC) moiety, but a clear understanding remains strikingly limited. In this work the bonding features and reactivity of 13 NHCP gold hydride complexes, [NHCPAuH], bearing different classes of NHCs have been systematically explored and compared to carbene analogues, using a consistent computational protocol. The analyses reveal that, although the $π$-acceptor ability trend of NHCPs qualitatively parallels that of NHCs, the $σ$-donor ability trend reverses, with more $σ$-donating NHC moieties generating less $σ$-donating NHCP ligands. Concurrently, the nature of the NHC moiety impacts the coordination geometry at the P center, with the CNHC-P-Au bond angle appearing as a structural descriptor to monitor and/or design NHCP ligands with desired $σ$-donor properties. The NHCPs stronger $σ$-donor and weaker $π$-acceptor abilities compared to NHCs and their unique structural flexibility and electronic adaptability have been showcased to be directly controlled by the carbene moiety via modulation of the HOMO lone pair energy and its atomic phosphorous 3p character. The reactivity of [NHCPAuH] complexes with CO2, taken as a probe for potential NHCP applications in small molecule activation processes, demonstrates qualitatively similar mechanisms, with remarkably different activation barriers, which directly correlate with the NHCPs $σ$-donor ability, thus reflecting the high tunability of their bonding properties. This work provides insights and perspectives on the design principle of NHCP ligands, with a spotlight on the pivotal role of NHC moiety in modulating their electronic and steric properties, offering opportunities for burgeoning applications across diverse fields.

physics.chem-ph↗

Third-Order Algebraic Diagrammatic Construction Renormalized by Particle-Particle Ladders

The algebraic diagrammatic construction (ADC) of the electronic self-energy is based on Møller--Plesset perturbation theory. Its vertices contain bare energy denominators that do not capture renormalization of Hartree--Fock excitations through excited-state correlations. As we show here, replacing the Møller--Plesset amplitudes by amplitudes obtained from Epstein--Nesbet (EN) partitioning of the electronic Hamiltonian overcomes this deficiency at no extra cost by introducing dressed denominators that resum to infinite order the diagonal elements of ladder diagrams described by the pair propagator in the particle-particle $T$-matrix approximation. Third-order ADC with EN-dressed denominators leads to an almost fourfold increase in accuracy compared to standard ADC(3) on a challenging benchmark set for ionization potentials of closed-shell molecules, reaching an accuracy between that of equation-of-motion coupled cluster with singles and doubles (EOM-CCSD) and with singles, doubles, and triples. For open-shell systems, EN-ADC(3) halves the error of ADC(3) for weakly spin-contaminated molecules, outperforming EOM-CCSD, and still improves on ADC(3) for strongly spin-contaminated ones, for which EOM-CCSD remains more accurate.

physics.chem-ph↗

A Geometry-Induced Finite Warburg element for Reversible Diffusion Impedance at Microdisk Electrodes

A compact analytical representation is developed for the diffusion impedance of a disk electrode under reversible conditions, obtained by transforming the chronoamperometric relaxation function into the frequency domain. A Padé approximant is constructed for the uniform-concentration boundary condition, preserving the finite low-frequency diffusion resistance of the steady-state disk current and the high-frequency Cottrell regime. It is extended to reactions in which both oxidized and reduced species contribute, with unequal diffusion coefficients and surface concentrations. Its accuracy is quantified against converged numerical solutions, including an exact solution of the coupled problem with finite-rate kinetics. The approximant reproduces the Saito resistance and the $45^{\circ}$ Warburg phase exactly; its modulus is within 0.6\% of the converged solution for $ωa^2/D\le12$ and 7\% below the Cottrell amplitude at high frequency. The uniform-concentration and uniform-flux boundary conditions both give a diffusion impedance of geometric origin, but differ by up to 11\% in modulus because each couples differently to the spreading diffusion field; a criterion based on the rate constant and the disk radius delineates where each applies. The exact solution shows that this crossover is broad and that the decomposition into a charge-transfer resistance and a diffusion impedance is accurate to about 5\% for $1\le2k^0a/D\le100$. Fitted to a published spectrum of a platinum microdisk, it reproduces the reported diffusion coefficient within 1\%, while the two limiting elements lie 4.8\% below and 4.1\% above it. The element is a practical tool for microdisk impedance analysis.

physics.chem-ph↗