Abstract
A coupled phase-field and hydrodynamic model is introduced to describe a two-phase, weakly compressible smectic (layered phase) in contact with an isotropic fluid of different density. A non-conserved smectic order parameter is coupled to a conserved mass density in order to accommodate non-solenoidal flows near the smectic-isotropic boundary arising from density contrast between the two phases. The model aims to describe morphological transitions in smectic thin films under heat treatment, in which arrays of focal conic defects evolve into conical pyramids and concentric rings through curvature dependent evaporation of smectic layers. The model leads to an extended thermodynamic relation at a curved surface that includes its Gaussian curvature, non-classical stresses at the boundary and flows arising from density gradients. The temporal evolution given by the model conserves the overall mass of the liquid crystal while still allowing for the modulated smectic structure to grow or shrink. A numerical solution of the governing equations reveals that pyramidal domains are sculpted at the center of focal conics upon a temperature increase, which display tangential flows at their surface. Other cases investigated include the possible coalescence of two cylindrical stacks of smectic layers, formation of droplets, and the interactions between focal conic domains through flow.
Original language | English (US) |
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Pages (from-to) | 6140-6159 |
Number of pages | 20 |
Journal | Soft Matter |
Volume | 17 |
Issue number | 25 |
DOIs | |
State | Published - Jun 30 2021 |
Bibliographical note
Funding Information:This research has been supported by the Minnesota Supercomputing Institute, and by the Extreme Science and Engineering Discovery Environment (XSEDE), 82 which is supported by the National Science Foundation under Grant No. ACI-1548562. EV thanks the support from the Doctoral Dissertation Fellowship and from the Aerospace Engineering and Mechanics department, University of Minnesota. This research is also supported by the National Science Foundation under Grant No. DMR-1838977. Part of the work of JV was done during the ACTIVE20 program at the Kavli Institute for Theoretical Physics which is funded by the National Science Foundation under Grant No. NSF PHY-1748958.
Funding Information:
This research has been supported by the Minnesota Supercomputing Institute, and by the Extreme Science and Engineering Discovery Environment (XSEDE),82 which is supported by the National Science Foundation under Grant No. ACI-1548562. EV thanks the support from the Doctoral Dissertation Fellowship and from the Aerospace Engineering and Mechanics department, University of Minnesota. This research is also supported by the National Science Foundation under Grant No. DMR-1838977. Part of the work of JV was done during the ACTIVE20 program at the Kavli Institute for Theoretical Physics which is funded by the National Science Foundation under Grant No. NSF PHY-1748958.
Publisher Copyright:
© The Royal Society of Chemistry 2021.
PubMed: MeSH publication types
- Journal Article