276 research outputs found
Structural variability and the incoherent addition of scattered intensities in single-particle diffraction
X-ray lasers may allow structural studies on single particles and biomolecules without crystalline periodicity in the samples. We examine here the effect of sample dynamics as a source of structural heterogeneity on the resolution of the reconstructed image of a small protein molecule. Structures from molecular-dynamics simulations of lysozyme were sampled and aligned. These structures were then used to calculate diffraction patterns corresponding to different dynamic states. The patterns were incoherently summed and the resulting data set was phased using the oversampling method. Reconstructed images of hydrated and dehydrated lysozyme gave resolutions of 3.7 Å and 7.6 Å, respectively. These are significantly worse than the root-mean-square deviation of the hydrated ͑2.7 Å for all atoms and 1.45 Å for C-␣ positions͒ or dehydrated ͑3.7 Å for all atoms and 2.5 Å for C-␣ positions͒ structures. The noise introduced by structural dynamics and incoherent addition of dissimilar structures restricts the maximum resolution to be expected from direct image reconstruction of dynamic systems. A way of potentially reducing this effect is by grouping dynamic structures into distinct structural substates and solving them separately
The cooperative behaviour of antimicrobial peptides in model membranes
A systematic analysis of the hypothesis of the antimicrobial peptides' (AMPs) cooperative action is performed by means of full atomistic molecular dynamics simulations accompanied by circular dichroism experiments. Several AMPs from the aurein family (2.5,2.6, 3.1), have a similar sequence in the first ten amino acids, are investigated in different environments including aqueous solution, trifluoroethanol (TFE), palmitoyloleoylphosphatidylethanolamine (POPE), and palmitoyloleoylphosphatidylglycerol (POPG) lipid bilayers. It is found that the cooperative effect is stronger in aqueous solution and weaker in TFE. Moreover, in the presence of membranes, the cooperative effect plays an important role in the peptide/lipid bilayer interaction. The action of AMPs is a competition of the hydrophobic interactions between the side chains of the peptides and the hydrophobic region of lipid molecules, as well as the intra peptide interaction. The aureins 2.5-COOH and 2.6-COOH form a hydrophobic aggregate to minimize the interaction between the hydrophobic group and the water. Once that the peptides reach the water/lipid interface the hydrophobic aggregate becomes smaller and the peptides start to penetrate into the membrane. In contrast, aurein 3.1-COOH forms only a transient aggregate which disintegrates once the peptides reached the membrane, and it shows no cooperativity in membrane penetratio
Auger Electron Cascades in Water and Ice
Secondary electron cascades can induce significant ionisation in condensed
matter due to electron-atom collisions. This is of interest in the context of
diffraction and imaging using X-rays, where radiation damage is the main
limiting factor for achieving high resolution data. Here we present new results
on electron-induced damage on liquid water and ice, from the simulation of
Auger electron cascades. We have compared our theoretical estimations to the
available experimental data on elastic and inelastic electron-molecule
interactions for water and found the theoretical results for elastic cross
sections to be in very good agreement with experiment. As a result of the
cascade we find that the average number of secondary electrons after 100 fs in
ice is about 25, slightly higher than in water, where it is about 20. The
difference in damage between ice and water is discussed in the context of
sample handling for biomolecular systems.Comment: 19 pages, 8 figures. Includes slight corrections to the version
submitted for publicatio
Space-time evolution of electron cascades in diamond
Here we describe model calculations to follow the spatio-temporal evolution
of secondary electron cascades in diamond. The band structure of the insulator
has been explicitly incorporated into the calculations as it affects
ionizations from the valence band. A Monte-Carlo model was constructed to
describe the path of electrons following the impact of a single electron of
energy E 250 eV. The results show the evolution of the secondary electron
cascades in terms of the number of electrons liberated, the spatial
distribution of these electrons, and the energy distribution among the
electrons as a function of time. The predicted ionization rates (5-13 electrons
in 100 fs) lie within the limits given by experiments and phenomenological
models. Calculation of the local electron density and the corresponding Debye
length shows that the latter is systematically larger than the radius of the
electron cloud. This means that the electron gas generated does not represent a
plasma in a single impact cascade triggered by an electron of E 250 eV energy.
This is important as it justifies the independent-electron approximation used
in the model. At 1 fs, the (average) spatial distribution of secondary
electrons is anisotropic with the electron cloud elongated in the direction of
the primary impact. The maximal radius of the cascade is about 50 A at this
time. As the system cools, energy is distributed more equally, and the spatial
distribution of the electron cloud becomes isotropic. At 90 fs maximal radius
is about 150 A. The Monte-Carlo model described here could be adopted for the
investigation of radiation damage in other insulators and has implications for
planned experiments with intense femtosecond X-ray sources.Comment: 26 pages, latex, 13 figure
Инфекционно-токсический шок в акушерстве и гинекологии
ШОК ТОКСИЧЕСКИЙ /ДИАГН /ПАТОФИЗИОЛ /ТЕРСЕПТИЦЕМИЯИНФЕКЦИЯ /ОСЛЖЕНСКИЕ БОЛЕЗНИ /ОСЛ /СМЕРТНАБОРТ КРИМИНАЛЬНЫЙБАКТЕРИАЛЬНЫЕ ИНФЕКЦИИ /ОСЛГИСТЕРЭКТОМИЯГИНЕКОЛОГИЧЕСКИЕ ХИРУРГИЧЕСКИЕ ОПЕРАЦИ
Virus Capsid Dissolution Studied by Microsecond Molecular Dynamics Simulations
Dissolution of many plant viruses is thought to start with swelling of the capsid caused by calcium removal following infection, but no high-resolution structures of swollen capsids exist. Here we have used microsecond all-atom molecular simulations to describe the dynamics of the capsid of satellite tobacco necrosis virus with and without the 92 structural calcium ions. The capsid expanded 2.5% upon removal of the calcium, in good agreement with experimental estimates. The water permeability of the native capsid was similar to that of a phospholipid membrane, but the permeability increased 10-fold after removing the calcium, predominantly between the 2-fold and 3-fold related subunits. The two calcium binding sites close to the icosahedral 3-fold symmetry axis were pivotal in the expansion and capsid-opening process, while the binding site on the 5-fold axis changed little structurally. These findings suggest that the dissociation of the capsid is initiated at the 3-fold axis
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