| Hauptseite > Publikationsdatenbank > Nonequilibrium Phase Transitions and Equilibrium Textures of Charged Chiral Rods (fd-Viruses) > print |
| 001 | 152205 | ||
| 005 | 20240619083458.0 | ||
| 037 | _ | _ | |a FZJ-2014-01961 |
| 041 | _ | _ | |a English |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a Kang, Kyongok |0 P:(DE-Juel1)130749 |b 0 |e Corresponding Author |u fzj |
| 245 | _ | _ | |a Nonequilibrium Phase Transitions and Equilibrium Textures of Charged Chiral Rods (fd-Viruses) |
| 260 | _ | _ | |a Libertyville, Ill. |c 2014 |b David Publ. |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1397043460_8373 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a article |2 DRIVER |
| 520 | _ | _ | |a Both non-equilibrium phase transitions and equilibrium textures of interacting charged chiral rods are explored, where thick electric double layers are present in the suspensions of charged chiral fibrous (fd) viruses at a low ionic strength. We first start with the electric phase/state diagram, illustrating dynamic frequency responses at the concentration of isotropic-nematic (I-N) coexistence, leading to various field-induced phases/states. As a low frequency response, two sharp transitions of chiral-nematic phases and dynamical states are induced, while as one transition is found to a homeotropic phases that is stabilized at a high-frequency. The characterizations of field-induced phases/states, and critical slowing down behaviors in the non-equilibrium criticality are discussed, by means of image-time correlation, dynamic light scattering and electric birefringence. For the equilibrium phase behaviors, depolarized optical morphology is studied with their texture dynamics, as an increase of rod concentration for a long equilibration time (80-100 h). Structure arrest has been observed by dynamic light scattering, above a glass transition concentration. Below the glass transition concentration, chiral-nematic textures are equilibrated at low, but above the I-N coexistence concentration. At higher, near to the glass transition concentration, another type of the equilibrium is reached as “domain” textures (of the helical domains) . Whether there will be a thermodynamic access of the density in orientational domains in these equilibrated textures in the interaction of charged chiral rods would be an interesting issue. |
| 536 | _ | _ | |a 451 - Soft Matter Composites (POF2-451) |0 G:(DE-HGF)POF2-451 |c POF2-451 |f POF II |x 0 |
| 773 | _ | _ | |0 PERI:(DE-600)2702036-8 |n 1 |p 26-35 |t Journal of physical science and application |v 4 |y 2014 |x 2159-5348 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/152205/files/FZJ-2014-01961.pdf |z Published final document. |y Restricted |
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| 914 | 1 | _ | |y 2014 |
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