Specific Features of the Rheological Behavior of a Protic Oligomeric Ionic Liquid of Cationic Type with Basic Sites of Two Types in the Region of the Solid–Liquid Transition

The structure and rheological behavior of a reactive oligomeric ionic liquid (OIL) have been studied. The OIL has a linear structure and contains ionic fragments of two types at both ends of oligo(ethylene oxide) chain. The ionic fragments are represented by secondary amino groups and nitrogen-conta...

Full description

Saved in:
Bibliographic Details
Published inColloid journal of the Russian Academy of Sciences Vol. 81; no. 6; pp. 804 - 816
Main Authors Shumskii, V. F., Shevchenko, V. V., Gumennaya, M. A., Getmanchuk, I. P., Stryutskii, A. V., Klimenko, N. S., Davidenko, V. V., Ignatova, T. D., Syrovets, A. P., Vorontsova, L. A.
Format Journal Article
LanguageEnglish
Published Moscow Pleiades Publishing 01.11.2019
Springer Nature B.V
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:The structure and rheological behavior of a reactive oligomeric ionic liquid (OIL) have been studied. The OIL has a linear structure and contains ionic fragments of two types at both ends of oligo(ethylene oxide) chain. The ionic fragments are represented by secondary amino groups and nitrogen-containing heterocycles protonated with ethane sulfonic acid. The results obtained using rotational rheometry in different dynamic regimes indicate that, in the linear region of deformation at temperatures T < 20°C, this OIL exhibits the behavior of an elastic solidlike body. The components of the complex shear modulus ( G  ' ~ 10 7 Pa and G  '' ~ 10 6 Pa) are independent of frequency ω and temperature. At the same time, its complex dynamic viscosity is independent of temperature and decreases with an increase in ω (in logarithmic coordinates, the dependence is linear and has a slope close to unity, which is a formal sign of the existence of a yield stress). At T ≤ 20°C in the nonlinear region of periodic deformation, a crossover is observed in the amplitude dependences of G  ' and G  '', which indicates that the critical shear stress is reached. As a result, the OIL passes into the liquid state ( G  '' > G  '). The boundary, which is located at nearly 30°C, is characterized by equality between G  ' and G  '' in a wide range of strain amplitudes. The structural transformations induced by thermal and mechanical energies have been explained using a hypothesis of the existence of micellar structures and a “normal micelle–reverse micelle” transition in the OIL, as well as changes in micelle shapes. The analysis of the temperature dependences for the viscoelastic characteristics and scattered light intensity, as well as the data of DSC and optical microscopy, has led to the hypothesis that at, T = 21–28°C, the OIL may occur in an ordered state similar to the liquid-crystalline one.
ISSN:1061-933X
1608-3067
DOI:10.1134/S1061933X19050132