4.5 Article

Experimental device to measure the ionic conductivity anisotropy in liquid crystal hydrogel based in [EMIM] alkyl sulfate Ionic Liquids

Journal

FLUID PHASE EQUILIBRIA
Volume 555, Issue -, Pages -

Publisher

ELSEVIER
DOI: 10.1016/j.fluid.2021.113353

Keywords

2D experimental device; Ionic liquid; Hydrogel; Electrical conductivity; Anisotropy; Liquid crystal

Funding

  1. Ministerio de Economia y Competitividad (MINECO)
  2. FEDER Program [MAT2017-89239-C2-1P, MAT2017-89239-C2-2-P, RED2018-102679-T]
  3. Xunta de Galicia
  4. FEDER [GRC 508 ED431C 2020/10]
  5. Universidade da Coruna/CISUG

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A device was built to measure the electrical conductivity anisotropy in a liquid crystal formed from the gelation of an ionic liquid. The gel state exhibited a striped pattern of a giant mesophase, and the electrical conductivity showed a significant difference between directions parallel and perpendicular to the observed stripes. This research is important for understanding the charge transport mechanism in ionic liquids and semi-solid conductors.
We have built an experimental device with the aim to measure the expected electrical conductivity anisotropy in a liquid crystal, obtained from the gelation of the ionic liquid 1-ethyl-3-methyl imidazolium decyl sulfate, [EMIM][DSO4]. This ionic liquid has the particularity that it transits to a semi-solid gel state at room temperature when it contains water, naturally adsorbed from the environment until a balance is reached between the concentration of water in the IL and the atmospheric humidity grade. The quantity of water adsorbed to form the hydrogel at room temperature varies from about 5 to 30 wt %, each composition giving place to different smectic phases. In the gel state, the ionic liquid ions and the water molecules self-organize into micro-sized mesophases that resemble the structures of a liquid crystal. Our device is a closed 2D sample holder (with sides 150 times longer than its thickness), with a single narrow window open to the atmosphere, and four copper contacts on the sides. The dried ionic liquid is tempered at 40 degrees C to increase its fluidity when injected into the cavity, and then, it can only adsorb water through the narrow opening. Thus, water adsorption is unidirectional and slow, so the transition of the IL to the gel phase happens progressively. A metastable giant mesophase appears as an orientated macrodomain in the form of a striped pattern. In this state, we measure the electrical conductivity of the confined film in directions parallel and perpendicular to the observed strips, finding a difference of up to 26% between both values of the conductivity. If the sample freezes (below 10 degrees C) or it liquefies (above 50 degrees C) the meso structure is broken and the observed anisotropy destroyed. We can return the sample to gel state by varying the temperature, but the ordered macroscopic state is no longer recovered. This research must give clues to solve the charge transport mechanism quiz in ionic liquids and semi-solid coductors. (C) 2021 The Author(s). Published by Elsevier B.V.

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