Lamellar-to-Onion Transition with Increasing Temperature under Shear Flow in a Nonionic Surfactant/Water System

Langmuir ◽  
2010 ◽  
Vol 26 (6) ◽  
pp. 3835-3842 ◽  
Author(s):  
Yuriko Kosaka ◽  
Makiko Ito ◽  
Youhei Kawabata ◽  
Tadashi Kato
2012 ◽  
Vol 372 (1) ◽  
pp. 32-39 ◽  
Author(s):  
Luigi Gentile ◽  
Bruno F.B. Silva ◽  
Sandor Balog ◽  
Kell Mortensen ◽  
Ulf Olsson

2004 ◽  
pp. 9-15
Author(s):  
T. Kato ◽  
K. Minewaki ◽  
K. Miyazaki ◽  
Y. Kawabata ◽  
T. Shikata ◽  
...  

Langmuir ◽  
2004 ◽  
Vol 20 (9) ◽  
pp. 3504-3508 ◽  
Author(s):  
Tadashi Kato ◽  
Koji Minewaki ◽  
Youhei Kawabata ◽  
Masayuki Imai ◽  
Yoshiaki Takahashi

2003 ◽  
Vol 398 (1) ◽  
pp. 157-167 ◽  
Author(s):  
Luigi Coppola ◽  
Raffaella Gianferri ◽  
Isabella Nicotera ◽  
Cesare Oliviero

Langmuir ◽  
2006 ◽  
Vol 22 (26) ◽  
pp. 10951-10957 ◽  
Author(s):  
Ying Wang ◽  
Michael C. Holmes ◽  
Marc S. Leaver ◽  
Andrew Fogden

2008 ◽  
Vol 18 (2) ◽  
pp. 23050-1-23050-7 ◽  
Author(s):  
Anne Pitkowski ◽  
Taco Nicolai ◽  
Dominique Durand

Abstract Small micellar casein particles were formed in aqueous solutions of native casein after addition of polyphosphate. These so-called submicelles aggregated and gelled with a rate that increased with increasing temperature. The evolution of the viscosity during this process was determined at constant shear rate or shear stress. When applying a small shear stress the viscosity increased strongly until the shear rate became immeasurably slow, but when the applied shear stress exceeded a critical value (σc) the aggregates broke up and the viscosity reached a maximum. At longer times the viscosity decreased rapidly at first, followed by a very slow decrease. σc was independent of the shear rate and heating temperature, but increased strongly with increasing casein concentration. At constant shear rate the stress remained close to σc, but fluctuated irregularly. After cessation of shear flow, gels were formed rapidly. Oscillation shear measurements for σ > σc showed a strongly non-linear response at the time of maximum viscosity.


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