Evaporation induced self-assembly of imogolite nanotubes in levitation: exploring phase transitions and material shaping

05 February 2024, Version 1
This content is a preprint and has not undergone peer review at the time of posting.

Abstract

Evaporation-induced self-assembly (EISA) is a versatile method for generating organized superstructures from colloidal particles, offering diverse design possibilities through the manipulation of colloid size, shape, substrate nature, and environmental conditions. While some work highlighted the importance of the choice of the substrate, this parameter is often overlooked in many EISA studies. In this work, we compare the self-assembly of lyotropic liquid crystals by EISA on hydrophilic or hydrophobic substrates, and by acoustic levitation (absence of substrate). We focus on imogolite nanotubes, a model colloidal system of 1D charged objects, due to their tunable morphology and rich liquid-crystalline phase behavior. We demonstrate the feasibility to obtain phase transitions in levitating droplets and on hydrophobic substrate, whereas self-assembly was limited on hydrophilic supports. Moreover, the aspect ratio of the nanotubes proves to be a pivotal factor, influencing both transitions and the resulting materials shape and surface. Besides material shaping, acoustic levitation emerges as a promising method for studying phase transitions, toward the rapid establishment of phase diagrams from diluted to highly concentrated states using a limited volume of sample.

Keywords

hydrophilic substrate
hydrophobic substrate
acoustic levitation
aspect ratio
anisotropic colloids
drying without substrate

Supplementary materials

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Supporting Information
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Supporting Information
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Video S1: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT M (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S1: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT M (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S2: Accelerated movie of the 2D SAXS patterns of the 1 µL droplet of Ge-DWINT M (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S2: Accelerated movie of the 2D SAXS patterns of the 1 µL droplet of Ge-DWINT M (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S3: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT S (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S3: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT S (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S4: Accelerated movie of the 2D SAXS patterns of the 1 µL droplet of Ge-DWINT S (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S4: Accelerated movie of the 2D SAXS patterns of the 1 µL droplet of Ge-DWINT S (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S5: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT L (Φinitial = 0.15%) during in-situ SAXS measurements.
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Video S5: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT L (Φinitial = 0.15%) during in-situ SAXS measurements.
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Title
Video S6: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT L (Φinitial = 0.15%) during in-situ SAXS measurements.
Description
Video S6: Accelerated movie of the evaporation of 1 µL droplet of Ge-DWINT L (Φinitial = 0.15%) during in-situ SAXS measurements.
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