Film formation process of natural rubber latex particles: roles of the particle size and distribution of non-rubber species on film microstructure

Author(s):  
Manus Sriring ◽  
Adun Nimpaiboon ◽  
Sirirat Kumarn ◽  
Keiko Higaki ◽  
Yuji Higaki ◽  
...  
Author(s):  
Kanjanee Nawamawat ◽  
Jitladda T. Sakdapipanich ◽  
Chee C. Ho ◽  
Yujie Ma ◽  
Jing Song ◽  
...  

2019 ◽  
Vol 304 (9) ◽  
pp. 1900283
Author(s):  
Manus Sriring ◽  
Adun Nimpaiboon ◽  
Nattanee Dechnarong ◽  
Sirirat Kumarn ◽  
Yuji Higaki ◽  
...  

2008 ◽  
Vol 286 (8-9) ◽  
pp. 1049-1059 ◽  
Author(s):  
A. Bogner ◽  
A. Guimarães ◽  
R. C. O. Guimarães ◽  
A. M. Santos ◽  
G. Thollet ◽  
...  

2017 ◽  
Vol 5 ◽  
pp. 63-71 ◽  
Author(s):  
Mitsuru Furuya ◽  
Naoki Shimono ◽  
Kazuyuki Yamazaki ◽  
Ryota Domura ◽  
Masami Okamoto

1955 ◽  
Vol 28 (3) ◽  
pp. 918-921
Author(s):  
Manfred Gordon ◽  
James S. Taylor

Abstract Kinetic evidence is presented for the occurrence in Hevea latex particles of a trace substance that retards the hydrochlorination reaction. No retardation effect is observed with synthetic polyisoprene latex. The chemical nature of the retarder in Hevea latex particles is not known, but it is likely to be a basic substance. Its retardation action reflects its power to deactivate the reactive precursor of the hydrochlorination reaction, which is interpreted as a form of ion pair (H+, Cl−). A constant amount of the precursor is deactivated by the retarder, irrespective of the temperature or the pressure of the hydrochlorination reaction.


2021 ◽  
pp. 110740
Author(s):  
Waraporn Wichaita ◽  
Duangkamol Promlok ◽  
Narissara Sudjaipraparat ◽  
Supang Sripraphot ◽  
Teeraporn Suteewong ◽  
...  

1947 ◽  
Vol 20 (2) ◽  
pp. 602-606 ◽  
Author(s):  
R. H. Kelsey ◽  
E. E. Hanson

Abstract The preparation of natural and synthetic rubber latex specimens for examination with an electron microscope is difficult because the individual particles are easily deformed and, under the usual conditions of specimen preparation, the particles tend to agglomerate. Von Ardenne and Beischer and others used a method which consisted of depositing a drop of highly diluted latex on a collodion film and allowing the drop to dry completely. In some instances the drop was withdrawn again into a glass capillary. It was found that in either case the latex particles were flattened at their areas of contact with the collodion film. The collodion film method was tried in this laboratory with the same poor results observed by Hendricks, Wildman, and McMurdee. Figure 1 is an electron micrograph of a natural rubber latex particle deposited by evaporating latex diluted 200 to 1 on a collodion film. The film has broken and curled to give a profile view of the particle which is observed to be badly flattened at its area of contact with the film. Figure 2 is a typical electron micrograph of natural rubber latex particles deposited on a collodion film. The blurred outlines of the particles are explained by the effect shown in Figure 1. It was obviously impossible to make good particle-size measurements from micrographs of this type. It was found further that severe aggregation of particles usually took place when a drop of the diluted latex was dried down. The latex particles which were left behind when the drop was removed with a glass capillary usually were not badly agglomerated, but it was felt that there was some possibility that the latex particles might adhere selectively according to size to the collodion film. An attempt was made to reduce the amount of agglomeration by incorporating in the diluting water various amounts of such wetting or dispersing agents as sodium oleate, orvis paste, Aerosol-OT, and ammonium caseinate. None of these materials helped very much in reducing the agglomeration of particles. It was found also in this study that very often the latex particles appeared granular around their edges due to foreign material being swept in during the evaporation of the water and crystallizing out upon the surface of the particle. This effect may also be observed in Figure 1.


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