Dispersion of Latex Particles in a Nematic Solution. 2. Phase Diagram and Elastic Properties

Langmuir ◽  
1996 ◽  
Vol 12 (16) ◽  
pp. 3789-3792 ◽  
Author(s):  
V. A. Raghunathan ◽  
P. Richetti ◽  
D. Roux
2009 ◽  
Vol 283-286 ◽  
pp. 559-564 ◽  
Author(s):  
M. Vázquez da Silva ◽  
João M.P.Q. Delgado

Cold-set gels of whey protein isolate (WPI) were produced. The cold gelation was induced through the addition of magnesium chloride whose cation is an alternative to the most common cations used in this kind of gelation. A phase diagram for denatured WPI in magnesium was determined by varying protein and salt concentrations. In this diagram the protein and cation concentrations varied from 0.3 to 8.0 wt % and 1 to 75 mM, respectively. The viscoelastic behaviour of the WPI was analysed, whereas gels elastic properties were measured by means of texture tests. Mathematical manipulation of the experimental data relative to the puncture tests was made in order to obtain the Young’s modulus for each cold-set gel.


1985 ◽  
Vol 34 (5) ◽  
pp. 667
Author(s):  
YAO YU-SHU ◽  
WANG RU-JU ◽  
WANG JI-FANG ◽  
HE SHOU-AN ◽  
ZHANG LIANG-KUN

1990 ◽  
Vol 12 (3) ◽  
pp. 235-240 ◽  
Author(s):  
H Vollmayr ◽  
R Kree ◽  
A Zippelius

2003 ◽  
Vol 81 (6) ◽  
pp. 797-804 ◽  
Author(s):  
G Quirion ◽  
A Kelly ◽  
S Newbury ◽  
F S Razavi ◽  
J D Garrett

It is now well-established that the strong anisotropy in the magnetic properties of the intermetallic compounds UT2Si2, where T stands for a transition metal, is responsible for their rich magnetic phase diagram. However, within that series of compounds, UNi2Si2 is one that shows an unusual sequence of magnetically ordered states. Thus, to better understand its unusual properties, we have investigated the elastic properties of UNi2Si2 as a function of temperature, magnetic field, and pressure. In all three magnetic phases, our measurements indicate that the sound-velocity temperature dependence is dominated by the magnetoelastic coupling. Moreover, the analysis of the temperature dependence for the incommensurate longitudinal spin-density wave phase is consistent with a critical exponent β = 0.38 ± 0.01. We also present the magnetic phase diagram for UNi2Si2 obtained at 0 and 8 kbar. Our investigation reveals that the triple-point coordinates (Tp, Hp) decrease with pressure at a rate of dTp/dP = –0.1 K/kbar and dHp/dP = –0.1 T/kbar, respectively. PACS Nos.: 75.30.kz, 62.20.Dc, 62.50.+p, 75.40.Cx


2003 ◽  
Vol 68 (14) ◽  
Author(s):  
Yoshiki Nakanishi ◽  
Takuo Sakon ◽  
Mitsuhiro Motokawa ◽  
Michiaki Ozawa ◽  
Takashi Suzuki ◽  
...  

Author(s):  
I. Stapff ◽  
G. Weidemann ◽  
C. Schellenberg ◽  
M. Regenbrecht ◽  
S. Akari ◽  
...  

1989 ◽  
Vol 116 (1) ◽  
pp. 287-293 ◽  
Author(s):  
O. G. Vlokh ◽  
A. V. Kityk ◽  
O. M. Mokry ◽  
V. G. Grybyk

Author(s):  
Earl R. Walter ◽  
Glen H. Bryant

With the development of soft, film forming latexes for use in paints and other coatings applications, it became desirable to develop new methods of sample preparation for latex particle size distribution studies with the electron microscope. Conventional latex sample preparation techniques were inadequate due to the pronounced tendency of these new soft latex particles to distort, flatten and fuse on the substrate when they dried. In order to avoid these complications and obtain electron micrographs of undistorted latex particles of soft resins, a freeze-dry, cold shadowing technique was developed. The method has now been used in our laboratory on a routine basis for several years.The cold shadowing is done in a specially constructed vacuum system, having a conventional mechanical fore pump and oil diffusion pump supplying vacuum. The system incorporates bellows type high vacuum valves to permit a prepump cycle and opening of the shadowing chamber without shutting down the oil diffusion pump. A baffeled sorption trap isolates the shadowing chamber from the pumps.


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