Nucleation of ordered solid phases of proteins via a disordered high-density state: Phenomenological approach

2005 ◽  
Vol 122 (17) ◽  
pp. 174905 ◽  
Author(s):  
Weichun Pan ◽  
Anatoly B. Kolomeisky ◽  
Peter G. Vekilov
2004 ◽  
Vol 129-130 ◽  
pp. 551-553
Author(s):  
Shin Muroya ◽  
Atsushi Nakamura ◽  
Chiho Nonaka

2004 ◽  
Vol 153 ◽  
pp. 51-59 ◽  
Author(s):  
Shin Muroya ◽  
Atsushi Nakamura ◽  
Chiho Nonaka

Author(s):  
Daniel Mariedahl ◽  
Fivos Perakis ◽  
Alexander Späh ◽  
Harshad Pathak ◽  
Kyung Hwan Kim ◽  
...  

Here we report about the structural evolution during the conversion from high-density amorphous ices at ambient pressure to the low-density state. Using high-energy X-ray diffraction, we have monitored the transformation by following in reciprocal space the structure factor S OO ( Q ) and derived in real space the pair distribution function g OO ( r ). Heating equilibrated high-density amorphous ice (eHDA) at a fast rate (4 K min –1 ), the transition to the low-density form occurs very rapidly, while domains of both high- and low-density coexist. On the other hand, the transition in the case of unannealed HDA (uHDA) and very-high-density amorphous ice is more complex and of continuous nature. The direct comparison of eHDA and uHDA indicates that the molecular structure of uHDA contains a larger amount of tetrahedral motives. The different crystallization behaviour of the derived low-density amorphous states is interpreted as emanating from increased tetrahedral coordination present in uHDA. This article is part of the theme issue ‘The physics and chemistry of ice: scaffolding across scales, from the viability of life to the formation of planets'.


2014 ◽  
Vol 21 (8) ◽  
pp. 082511 ◽  
Author(s):  
H. Saitoh ◽  
Y. Yano ◽  
Z. Yoshida ◽  
M. Nishiura ◽  
J. Morikawa ◽  
...  

1992 ◽  
Vol 63 (1) ◽  
pp. 163-165 ◽  
Author(s):  
J. A. Brand ◽  
J. E. Furst ◽  
T. J. Gay ◽  
L. D. Schearer
Keyword(s):  

1989 ◽  
Vol 109 (3) ◽  
pp. 1037-1046 ◽  
Author(s):  
R Einstein ◽  
C A Gabel

Mouse L-cells that contain the cation-independent (CI) mannose 6-phosphate (Man 6-P)/insulin-like growth factor (IGF) II receptor endocytose acid hydrolases and deliver these enzymes to lysosomes. The postendocytic loss of the Man 6-P recognition marker from the cell-associated acid hydrolases was assessed by CI-Man 6-P receptor affinity chromatography. 125I-labeled acid hydrolases internalized by L-cells grown at high density were delivered to lysosomes but were not dephosphorylated. In contrast, the same 125I-labeled hydrolases internalized by L-cells maintained at low density were delivered to lysosomes and were extensively dephosphorylated. The dephosphorylation at low density required 5 h for completion suggesting that the phosphatase responsible for the dephosphorylation is located within the lysosomal compartment. Transition from the high to low density state was rapid and was not inhibited by cycloheximide. Medium substitution experiments indicated that serum factors were necessary to maintain the L-cells in the dephosphorylation-competent (low density) state, and that serum-free conditions led to a dephosphorylation-incompetent (high density) state. Addition of IGF II to cells in serum-free medium allowed acid hydrolases subsequently introduced by endocytosis to be dephosphorylated. The results indicate that the removal of the Man 6-P recognition marker from endocytosed acid hydrolases is regulated by serum factors in the growth medium, including IGF II.


2014 ◽  
Vol 70 (a1) ◽  
pp. C897-C897
Author(s):  
Laurent Gagné-Dumais ◽  
Catherine Aldous ◽  
Serge Desgreniers

Mixing different molecular species at high density may yield weakly bound compounds or van der Waals solids. These novel solids are stabilized by the application of high pressure and differ in physical properties from solids formed by pure molecular species at comparable thermodynamic conditions. In this contribution, we address the importance in studying the miscibility in dense molecular mixtures and present results of the formation of binary methane-nitrogen compounds at low temperature and high pressure. Methane and nitrogen, with similar potentials and molecular sizes, are expected to be partly miscible in the condensed state. Indeed, binary van der Waals solid phases of methane and nitrogen do occur with the application of pressure. Using single crystal and powder X-ray diffraction with synchrotron radiation, and vibrational spectroscopy, the pressure-concentration phase diagram for this system has been explored from 1 to 16 GPa at room temperature. The existence of novel van der Waals solid phases for samples with concentrations above 10% (methane per volume) is demonstrated. For example, at 7.6 GPa and at room temperature, whereas pure nitrogen and methane exist in a cubic (Pm3n) and in a rhombohedral structure (R-3/m), respectively, our study indicates that a methane-nitrogen sample with ~ 40% methane by volume exhibits, under the same conditions, a novel phase with a tetragonal symmetry with lattice parameters a ~ 11.9 Å and c ~ 6.2 Å. Other novel structures in methane-nitrogen samples with different concentrations under varying pressure conditions have also been observed and will be discussed.


Sign in / Sign up

Export Citation Format

Share Document