{
  "annotation_id": "6d429f00-6780-435d-bbe5-a737c4632dd6",
  "date_created": "2026-03-02T18:00:28.667000Z",
  "date_modified": "2026-03-02T18:00:28.667000Z",
  "file_hash": "aef78b00daa1573c72752444a636f35d8e14047daef89a25125aa0354f6d3836",
  "private": false,
  "record": {
    "abstract": "Realistic boundaries of finite heat conductivity Realistic boundaries of\nfinite heat conductivity for thermoconvection in a Rayleigh-B\\\u0027enard setup with\nmagnetized ferrofluids are investigated. A linear stability analysis of the\nconductive state is performed with a shooting method. It shows that the\ncritical wave number is for any magnetic field stronly influenced by the\nconductivity of the boundaries. Linear as well as nonlinear coefficients of a\nGinzburg Landau amplitude equation for convection shortly above the onset are\nevaluated as functions of the magnetic Rayleigh number, the boundary\nconductivities, and the fluid Prandtl number.",
    "arxiv_id": "patt-sol/9810008",
    "authors": [
      "A. Recktenwald",
      "M. Luecke"
    ],
    "categories": [
      "patt-sol",
      "nlin.PS"
    ],
    "doi": "10.1016/S0304-8853(98)00185-1",
    "journal_ref": "J. Magn. Magn. Mater. 188, 326 - 332 (1998)",
    "title": "Thermoconvection in magnetized ferrofluids: the influence of boundaries   with finite heat conductivity",
    "url": "https://arxiv.org/abs/patt-sol/9810008"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1b8aa3c2-75c8-4f86-9857-dca230d47fa5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}