dorsal/arxiv
View SchemaRayleigh-B\'{e}nard convection in a homeotropically aligned nematic liquid crystal
| Authors | Leif Thomas, Werner Pesch, Guenter Ahlers |
|---|---|
| Categories | |
| ArXiv ID | patt-sol/9805009 |
| URL | https://arxiv.org/abs/patt-sol/9805009 |
| DOI | 10.1103/PhysRevE.58.5885 |
Abstract
We report experimental results for convection near onset in a thin layer of a homeotropically aligned nematic liquid crystal heated from below as a function of the temperature difference $\Delta T$ and the applied vertical magnetic field $H$ and compare them with theoretical calculations. The experiments cover the field range $8 \alt h \equiv H/ H_{F} \alt 80$ ($H_F =$ is the Fr\'eedericksz field). For $h$ less than a codimension-two field $h_{ct} \simeq 46$ the bifurcation is subcritical and oscillatory, with travelling- and standing-wave transients. Beyond $h_{ct}$ the bifurcation is stationary and subcritical until a tricritical field $h_t= 57.2$ is reached, beyond which it is supercritical. The bifurcation sequence as a function of $h$ found in the experiment confirms the qualitative aspects of the theoretical predictions. However, the value of $h_{ct}$ is about 10% higher than the predicted value and the results for $k_c$ are systematically below the theory by about 2% at small $h$ and by as much as 7% near $h_{ct}$. At $h_{ct}$, $k_c$ is continuous within the experimental resolution whereas the theory indicates a 7% discontinuity. The theoretical tricritical field $h_t^{th} = 51$ is somewhat below the experimental one. The fully developed flow above $R_c$ for $h < h_{ct}$ is chaotic. For $h_{ct} < h < h_t$ the subcritical stationary bifurcation also leads to a chaotic state. The chaotic states persist upon reducing the Rayleigh number below $R_c$, i.e. the bifurcation is hysteretic. Above the tricritical field $h_t$, we find a bifurcation to a time independent pattern which within our resolution is non-hysteretic.
{
"annotation_id": "ec97384f-f28a-4f9d-a90e-8e990c1acd09",
"date_created": "2026-03-02T18:00:29.402000Z",
"date_modified": "2026-03-02T18:00:29.402000Z",
"file_hash": "90b99a1159800e0d472a46716b8af1dab6bc095bee5d54eb415ea614a2eb1cf1",
"private": false,
"record": {
"abstract": "We report experimental results for convection near onset in a thin layer of a\nhomeotropically aligned nematic liquid crystal heated from below as a function\nof the temperature difference $\\Delta T$ and the applied vertical magnetic\nfield $H$ and compare them with theoretical calculations. The experiments cover\nthe field range $8 \\alt h \\equiv H/ H_{F} \\alt 80$ ($H_F =$ is the\nFr\\\u0027eedericksz field). For $h$ less than a codimension-two field $h_{ct} \\simeq\n46$ the bifurcation is subcritical and oscillatory, with travelling- and\nstanding-wave transients. Beyond $h_{ct}$ the bifurcation is stationary and\nsubcritical until a tricritical field $h_t= 57.2$ is reached, beyond which it\nis supercritical. The bifurcation sequence as a function of $h$ found in the\nexperiment confirms the qualitative aspects of the theoretical predictions.\nHowever, the value of $h_{ct}$ is about 10% higher than the predicted value and\nthe results for $k_c$ are systematically below the theory by about 2% at small\n$h$ and by as much as 7% near $h_{ct}$. At $h_{ct}$, $k_c$ is continuous within\nthe experimental resolution whereas the theory indicates a 7% discontinuity.\nThe theoretical tricritical field $h_t^{th} = 51$ is somewhat below the\nexperimental one. The fully developed flow above $R_c$ for $h \u003c h_{ct}$ is\nchaotic. For $h_{ct} \u003c h \u003c h_t$ the subcritical stationary bifurcation also\nleads to a chaotic state. The chaotic states persist upon reducing the Rayleigh\nnumber below $R_c$, i.e. the bifurcation is hysteretic. Above the tricritical\nfield $h_t$, we find a bifurcation to a time independent pattern which within\nour resolution is non-hysteretic.",
"arxiv_id": "patt-sol/9805009",
"authors": [
"Leif Thomas",
"Werner Pesch",
"Guenter Ahlers"
],
"categories": [
"patt-sol",
"nlin.PS"
],
"doi": "10.1103/PhysRevE.58.5885",
"title": "Rayleigh-B\\\u0027{e}nard convection in a homeotropically aligned nematic liquid crystal",
"url": "https://arxiv.org/abs/patt-sol/9805009"
},
"schema_id": "dorsal/arxiv",
"source": {
"execution_id": "30ae544b-c0fc-488e-a840-25188b9ddc6c",
"id": "arXiv Dataset IDs",
"type": "Model",
"variant": "snapshot-2026-03-01",
"version": "0.1.0"
},
"user_id": 1000002
}