Concentration dependent phase behavior and collapse dynamics of PNIPAM microgel by dielectric relaxation

2017 ◽  
Vol 19 (23) ◽  
pp. 15433-15443 ◽  
Author(s):  
Man Yang ◽  
Chunyan Liu ◽  
Kongshuang Zhao

Concentration dependent phase behavior of microgel: the dense system underwent a phase transition from colloidal crystal to liquid and to phase separation (above); the dilute system only underwent a transition from liquid to phase separation (below).

Soft Matter ◽  
2022 ◽  
Author(s):  
Paul Pullara ◽  
Ibraheem Alshareedah ◽  
Priya Banerjee

Liquid-liquid phase separation (LLPS) of multivalent biopolymers is a ubiquitous process in biological systems and is of importance in bio-mimetic soft matter design. The phase behavior of biomolecules, such as...


RSC Advances ◽  
2016 ◽  
Vol 6 (12) ◽  
pp. 9693-9708 ◽  
Author(s):  
Ashkan Shoja Chaykar ◽  
Fatemeh Goharpey ◽  
Jafar Khademzadeh Yeganeh

We investigate the effect of nanoparticles and radiation dose on interactions in the PVME-based nanogel system and its phase behavior (swelling/deswelling behavior and phase separation mechanism) by rheological and FTIR measurements.


Soft Matter ◽  
2017 ◽  
Vol 13 (39) ◽  
pp. 7161-7171 ◽  
Author(s):  
Hernan Garate ◽  
King-Wo Li ◽  
Denis Bouyer ◽  
Patrick Guenoun

Phase separation of thermo-responsive polymers in solution is a complex process, whose understanding is improved by following the dynamical modes as the transition is approached.


2017 ◽  
Vol 114 (49) ◽  
pp. 12906-12909 ◽  
Author(s):  
Ricard Alert ◽  
Pietro Tierno ◽  
Jaume Casademunt

Mixed-order phase transitions display a discontinuity in the order parameter like first-order transitions yet feature critical behavior like second-order transitions. Such transitions have been predicted for a broad range of equilibrium and nonequilibrium systems, but their experimental observation has remained elusive. Here, we analytically predict and experimentally realize a mixed-order equilibrium phase transition. Specifically, a discontinuous solid–solid transition in a 2D crystal of paramagnetic colloidal particles is induced by a magnetic field H. At the transition field Hs, the energy landscape of the system becomes completely flat, which causes diverging fluctuations and correlation length ξ∝|H2−Hs2|−1/2. Mean-field critical exponents are predicted, since the upper critical dimension of the transition is du=2. Our colloidal system provides an experimental test bed to probe the unconventional properties of mixed-order phase transitions.


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