{
  "id": "astro-ph/9908199",
  "version": "v1",
  "published": "1999-08-18T15:03:06.000Z",
  "updated": "1999-08-18T15:03:06.000Z",
  "title": "The Cooling Flow to Accretion Flow Transition",
  "authors": [
    "Eliot Quataert",
    "Ramesh Narayan"
  ],
  "comment": "emulateapj.sty, 10 pages incl. 5 figures, to appear in ApJ",
  "doi": "10.1086/308171",
  "categories": [
    "astro-ph"
  ],
  "abstract": "Cooling flows in galaxy clusters and isolated elliptical galaxies are a source of mass for fueling accretion onto a central supermassive black hole. We calculate the dynamics of accreting matter in the combined gravitational potential of a host galaxy and a central black hole assuming a steady state, spherically symmetric flow (i.e., no angular momentum). The global dynamics depends primarily on the accretion rate. For large accretion rates, no simple, smooth transition between a cooling flow and an accretion flow is possible; the gas cools towards zero temperature just inside its sonic radius, which lies well outside the region where the gravitational influence of the central black hole is important. For accretion rates below a critical value, however, the accreting gas evolves smoothly from a radiatively driven cooling flow at large radii to a nearly adiabatic (Bondi) flow at small radii. We argue that this is the relevant parameter regime for most observed cooling flows. The transition from the cooling flow to the accretion flow should be observable in M87 with the {\\it Chandra X-ray Observatory}.",
  "revisions": [
    {
      "version": "v1",
      "updated": "1999-08-18T15:03:06.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "cooling flow",
      "accretion flow transition",
      "central black hole",
      "large accretion rates",
      "global dynamics depends"
    ],
    "tags": [
      "journal article"
    ],
    "note": {
      "typesetting": "TeX",
      "pages": 10,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 518984
    }
  }
}