Thermal dissociation of streptavidin homotetramer in the gas phase: Subunit loss versus backbone fragmentation

2013 ◽  
Vol 345-347 ◽  
pp. 97-103 ◽  
Author(s):  
Elena N. Kitova ◽  
Igor Sinelnikov ◽  
Lu Deng ◽  
John S. Klassen
2001 ◽  
Vol 210-211 ◽  
pp. 215-222 ◽  
Author(s):  
Ben Garcia ◽  
Javier Ramirez ◽  
Sandy Wong ◽  
Carlito B. Lebrilla

2001 ◽  
Vol 105 (18) ◽  
pp. 4446-4457 ◽  
Author(s):  
Jesse H. Kroll ◽  
Shailesh R. Sahay ◽  
James G. Anderson ◽  
Kenneth L. Demerjian ◽  
Neil M. Donahue

2017 ◽  
Vol 52 (4) ◽  
pp. 204-209 ◽  
Author(s):  
Y. Kostyukevich ◽  
A. Kononikhin ◽  
I. Popov ◽  
E. Nikolaev

2002 ◽  
Vol 13 (12) ◽  
pp. 1432-1442 ◽  
Author(s):  
Natalia Felitsyn ◽  
Elena N. Kitova ◽  
John S. Klassen

2011 ◽  
Vol 42 (3) ◽  
pp. 568-574 ◽  
Author(s):  
Duygu Ağaoğulları ◽  
Özge Balcı ◽  
İsmaİl Duman ◽  
M. Lütfİ Öveçoğlu

2013 ◽  
Vol 18 (4) ◽  
pp. 314-321 ◽  
Author(s):  
Leonid Zhdanov ◽  
Vladyslav Kovalenko ◽  
Nataliya Strelenko ◽  
Yevgenia Chvertko

A method of settlement of the process of thermal dissociation of oxides in reaction zone during the submerged arc welding and welding deposition is presented. Combined non-linear equations for definition of gas-vapour mixture composition were developed. They describe the dissociation of MeO, MeO2 and Me2O3 types of oxides. Calculations of the processes of oxide dissociation were performed for the oxides that are commonly included into welding fluxes. Their results and analysis are presented. The method proposed appeared to be adequate and applicable for analysis of processes during submerged arc operation that run in the gas phase.


Author(s):  
Richard E. Hartman ◽  
Roberta S. Hartman ◽  
Peter L. Ramos

The action of water and the electron beam on organic specimens in the electron microscope results in the removal of oxidizable material (primarily hydrogen and carbon) by reactions similar to the water gas reaction .which has the form:The energy required to force the reaction to the right is supplied by the interaction of the electron beam with the specimen.The mass of water striking the specimen is given by:where u = gH2O/cm2 sec, PH2O = partial pressure of water in Torr, & T = absolute temperature of the gas phase. If it is assumed that mass is removed from the specimen by a reaction approximated by (1) and that the specimen is uniformly thinned by the reaction, then the thinning rate in A/ min iswhere x = thickness of the specimen in A, t = time in minutes, & E = efficiency (the fraction of the water striking the specimen which reacts with it).


Author(s):  
E. G. Rightor

Core edge spectroscopy methods are versatile tools for investigating a wide variety of materials. They can be used to probe the electronic states of materials in bulk solids, on surfaces, or in the gas phase. This family of methods involves promoting an inner shell (core) electron to an excited state and recording either the primary excitation or secondary decay of the excited state. The techniques are complimentary and have different strengths and limitations for studying challenging aspects of materials. The need to identify components in polymers or polymer blends at high spatial resolution has driven development, application, and integration of results from several of these methods.


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