AI Chat Paper
Note: Please note that the following content is generated by AMiner AI. SciOpen does not take any responsibility related to this content.
{{lang === 'zh_CN' ? '文章概述' : 'Summary'}}
{{lang === 'en_US' ? '中' : 'Eng'}}
Chat more with AI
PDF (599.3 KB)
Collect
Submit Manuscript AI Chat Paper
Show Outline
Outline
Show full outline
Hide outline
Outline
Show full outline
Hide outline
Research Article | Open Access

Recent analytic development of the dynamic Q-tensor theory for nematic liquid crystals

Department of Mathematics and Statistics, Old Dominion University, Norfolk, VA 23529, USA
Show Author Information

Abstract

Liquid crystals are a typical type of soft matter that are intermediate between conventional crystalline solids and isotropic fluids. The nematic phase is the simplest liquid crystal phase, and has been studied the most in the mathematical community. There are various continuum models to describe liquid crystals of nematic type, and Q-tensor theory is one among them. The aim of this paper is to give a brief review of recent PDE results regarding the Q-tensor theory in dynamic configurations.

References

【1】
【1】
 
 
Electronic Research Archive
Pages 2220-2246

{{item.num}}

Comments on this article

Go to comment

< Back to all reports

Review Status: {{reviewData.commendedNum}} Commended , {{reviewData.revisionRequiredNum}} Revision Required , {{reviewData.notCommendedNum}} Not Commended Under Peer Review

Review Comment

Close
Close
Cite this article:
Xu X. Recent analytic development of the dynamic Q-tensor theory for nematic liquid crystals. Electronic Research Archive, 2022, 30(6): 2220-2246. https://doi.org/10.3934/era.2022113

15

Views

0

Downloads

4

Crossref

2

Web of Science

4

Scopus

Received: 18 September 2021
Revised: 13 December 2021
Accepted: 14 December 2021
Published: 15 June 2022
©2022 the Author(s), licensee AIMS Press.

This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)