lysozyme crystal
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2019 ◽  
Vol 19 (10) ◽  
pp. 5955-5960 ◽  
Author(s):  
Haruhiko Koizumi ◽  
Satoshi Uda ◽  
Katsuo Tsukamoto ◽  
Kenji Hanada ◽  
Ryo Suzuki ◽  
...  

2019 ◽  
Vol 283 ◽  
pp. 652-659 ◽  
Author(s):  
I.Zh. Bezbakh ◽  
V.P. Ginkin ◽  
V.V. Safronov ◽  
V.I. Strelov ◽  
B.G. Zakharov

Crystals ◽  
2018 ◽  
Vol 8 (11) ◽  
pp. 400 ◽  
Author(s):  
Yong Yu ◽  
Kai Li ◽  
Hai Lin ◽  
Ji-Cheng Li

Space is expected to be a convection-free, quiescent environment for the production of large-size and high-quality protein crystals. However, the mechanisms by which the diffusion environment in space improves the quality of the protein crystals are not fully understood. The interior of a microfluidic device can be used to simulate a microgravity environment to investigate the protein crystallization mechanism that occurs in space. In the present study, lysozyme crystals were grown in a prototype microchannel device with a height of 50 μm in a glass-polydimethylsiloxane (PDMS)-glass sandwich structure. Comparative experiments were also conducted in a sample pool with a height of 2 mm under the same growth conditions. We compared the crystal morphologies and growth rates of the grown crystals in the two sample pools. The experimental results showed that at very low initial supersaturation, the morphology and growth rates of lysozyme crystals under the simulated microgravity conditions is similar to that on Earth. With increasing initial supersaturation, a convection-free, quiescent environment is better for lysozyme crystal growth. When the initial supersaturation exceeded a threshold, the growth of the lysozyme crystal surface under the simulated microgravity conditions never completely transform from isotropic to anisotropic. The experimental results showed that the convection may have a dual effect on the crystal morphology. Convection can increase the roughness of the crystal surface and promote the transformation of the crystal form from circular to tetragonal during the crystallization process.


Structure ◽  
2018 ◽  
Vol 26 (4) ◽  
pp. 667-675.e3 ◽  
Author(s):  
Hongyi Xu ◽  
Hugo Lebrette ◽  
Taimin Yang ◽  
Vivek Srinivas ◽  
Sven Hovmöller ◽  
...  

2017 ◽  
Vol 50 (4) ◽  
pp. 985-993 ◽  
Author(s):  
Ti-Yen Lan ◽  
Jennifer L. Wierman ◽  
Mark W. Tate ◽  
Hugh T. Philipp ◽  
Veit Elser ◽  
...  

Recently, there has been a growing interest in adapting serial microcrystallography (SMX) experiments to existing storage ring (SR) sources. For very small crystals, however, radiation damage occurs before sufficient numbers of photons are diffracted to determine the orientation of the crystal. The challenge is to merge data from a large number of such `sparse' frames in order to measure the full reciprocal space intensity. To simulate sparse frames, a dataset was collected from a large lysozyme crystal illuminated by a dim X-ray source. The crystal was continuously rotated about two orthogonal axes to sample a subset of the rotation space. With the EMC algorithm [expand–maximize–compress; Loh & Elser (2009).Phys. Rev. E,80, 026705], it is shown that the diffracted intensity of the crystal can still be reconstructed even without knowledge of the orientation of the crystal in any sparse frame. Moreover, parallel computation implementations were designed to considerably improve the time and memory scaling of the algorithm. The results show that EMC-based SMX experiments should be feasible at SR sources.


2015 ◽  
Vol 41 (4) ◽  
pp. 327-338 ◽  
Author(s):  
Ivaylo L. Dimitrov ◽  
Feyzim V. Hodzhaoglu ◽  
Dobryana P. Koleva

2014 ◽  
Vol 70 (a1) ◽  
pp. C1661-C1661
Author(s):  
Ryuta Mizutani ◽  
Yusuke Shimizu ◽  
Rino Saiga ◽  
Go Ueno ◽  
Yuki Nakamura ◽  
...  

Time-resolved visualization of the soaking process of tetragonal lysozyme crystal was performed by synchrotron radiation microtomography. Mother liquor containing hexachloroplatinate was introduced into a capillary bearing lysozyme crystals to visualize crystals undergoing soaking. The platinum distribution was first observed in the superficial layer of crystal and then gradually penetrated into the crystal core. The crystal structure of the platinum derivative in each soaking period was determined by time-resolved crystallography. A total of five platinum sites were identified in Bijvoet difference maps. These sites were classified into two groups on the basis of the time dependence of electron density development. A soaking process model consisting of binding-rate-driven and equilibrium-driven layers is proposed to describe the results. This study suggests that the structures of soaked crystals vary depending on the crystal position from which diffractions were taken.


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