1,325 research outputs found
The mosaics of Mars: As seen by the Viking Lander cameras
The mosaics and derivative products produced from many individual high resolution images acquired by the Viking Lander Camera Systems are described: A morning and afternoon mosaic for both cameras at the Lander 1 Chryse Planitia site, and a morning, noon, and afternoon camera pair at Utopia Planitia, the Lander 11 site. The derived products include special geometric projections of the mosaic data sets, polar stereographic (donut), stereoscopic, and orthographic. Contour maps and vertical profiles of the topography were overlaid on the mosaics from which they were derived. Sets of stereo pairs were extracted and enlarged from stereoscopic projections of the mosaics
Replacement of PBNA in HB and HC polymers used in SRM propellant and liner
The antioxidant phenyl-beta-naphthylamine (PBNA) was used in both HB and HC polymers. The sole (domestic) supplier of PBNA has withdrawn this product from the market, primarily because of suspected health hazards. Commercially available substitute(s) were selected and qualified for use in the two polymers
Response to the letter by Udo Bonnet
Peer Reviewedhttps://deepblue.lib.umich.edu/bitstream/2027.42/153273/1/nmo13715_am.pdfhttps://deepblue.lib.umich.edu/bitstream/2027.42/153273/2/nmo13715.pd
Pathways to folding, nucleation events and native geometry
We perform extensive Monte Carlo simulations of a lattice model and the Go
potential to investigate the existence of folding pathways at the level of
contact cluster formation for two native structures with markedly different
geometries. Our analysis of folding pathways revealed a common underlying
folding mechanism, based on nucleation phenomena, for both protein models.
However, folding to the more complex geometry (i.e. that with more non-local
contacts) is driven by a folding nucleus whose geometric traits more closely
resemble those of the native fold. For this geometry folding is clearly a more
cooperative process.Comment: Accepted in J. Chem. Phy
Relevant distance between two different instances of the same potential energy in protein folding
In the context of complex systems and, particularly, of protein folding, a
physically meaningful distance is defined which allows to make useful
statistical statements about the way in which energy differences are modified
when two different instances of the same potential-energy function are used.
When the two instances arise from the fact that different algorithms or
different approximations are used, the distance herein defined may be used to
evaluate the relative accuracy of the two methods. When the difference is due
to a change in the free parameters of which the potential depends on, the
distance can be used to quantify, in each region of parameter space, the
robustness of the modeling to such a change and this, in turn, may be used to
assess the significance of a parameters' fit. Both cases are illustrated with a
practical example: the study of the Poisson-based solvation energy in the
Trp-Cage protein (PDB code 1L2Y).Comment: 20 pages, 6 figures, LaTeX file, elsart style. v1: Aknowledgments
modified. v2: y-values of fig. 5 and 6 corrected. v3: Journal-ref added,
aknowledgements modified and fig. 1 and 2 correcte
The effect of local thermal fluctuations on the folding kinetics: a study from the perspective of the nonextensive statistical mechanics
Protein folding is a universal process, very fast and accurate, which works
consistently (as it should be) in a wide range of physiological conditions. The
present work is based on three premises, namely: () folding reaction is a
process with two consecutive and independent stages, namely the search
mechanism and the overall productive stabilization; () the folding kinetics
results from a mechanism as fast as can be; and () at nanoscale
dimensions, local thermal fluctuations may have important role on the folding
kinetics. Here the first stage of folding process (search mechanism) is focused
exclusively. The effects and consequences of local thermal fluctuations on the
configurational kinetics, treated here in the context of non extensive
statistical mechanics, is analyzed in detail through the dependence of the
characteristic time of folding () on the temperature and on the
nonextensive parameter .The model used consists of effective residues
forming a chain of 27 beads, which occupy different sites of a D infinite
lattice, representing a single protein chain in solution. The configurational
evolution, treated by Monte Carlo simulation, is driven mainly by the change in
free energy of transfer between consecutive configurations. ...Comment: 19 pages, 3 figures, 1 tabl
Exploring the Levinthal limit in protein folding
According to the thermodynamic hypothesis, the native state of proteins is uniquely defined by their amino acid sequence. On the other hand, according to Levinthal, the native state is just a local minimum of the free energy and a given amino acid sequence, in the same thermodynamic conditions, can assume many, very different structures that are as thermodynamically stable as the native state. This is the Levinthal limit explored in this work. Using computer simulations, we compare the interactions that stabilize the native state of four different proteins with those that stabilize three non-native states of each protein and find that the nature of the interactions is very similar for all such 16 conformers. Furthermore, an enhancement of the degree of fluctuation of the non-native conformers can be explained by an insufficient relaxation to their local free energy minimum. These results favor Levinthal's hypothesis that protein folding is a kinetic non-equilibrium process.FCT - Foundation for Science and Technology, Portugal [UID/Multi/04326/2013]; Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP); Conselho Nacional de Desenvolvimento Cientia co e Tecnologico (CNPq
Soliton concepts and the protein structure
Structural classification shows that the number of different protein folds is
surprisingly small. It also appears that proteins are built in a modular
fashion, from a relatively small number of components. Here we propose to
identify the modular building blocks of proteins with the dark soliton solution
of a generalized discrete nonlinear Schrodinger equation. For this we show that
practically all protein loops can be obtained simply by scaling the size and by
joining together a number of copies of the soliton, one after another. The
soliton has only two loop specific parameters and we identify their possible
values in Protein Data Bank. We show that with a collection of 200 sets of
parameters, each determining a soliton profile that describes a different short
loop, we cover over 90% of all proteins with experimental accuracy. We also
present two examples that describe how the loop library can be employed both to
model and to analyze the structure of folded proteins.Comment: 7 pages 6 fig
Highly Designable Protein Structures and Inter Monomer Interactions
By exact computer enumeration and combinatorial methods, we have calculated
the designability of proteins in a simple lattice H-P model for the protein
folding problem.
We show that if the strength of the non-additive part of the interaction
potential becomes larger than a critical value, the degree of designability of
structures will depend on the parameters of potential. We also show that the
existence of a unique ground state is highly sensitive to mutation in certain
sites.Comment: 14 pages, Latex file, 3 latex and 6 eps figures are include
CRANKITE: a fast polypeptide backbone conformation sampler
Background: CRANKITE is a suite of programs for simulating backbone conformations of polypeptides and proteins. The core of the suite is an efficient Metropolis Monte Carlo sampler of backbone conformations in continuous three-dimensional space in atomic details.
Methods: In contrast to other programs relying on local Metropolis moves in the space of dihedral angles, our sampler utilizes local crankshaft rotations of rigid peptide bonds in Cartesian space.
Results: The sampler allows fast simulation and analysis of secondary structure formation and conformational changes for proteins of average length
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