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Volumn 288, Issue 5471, 2000, Pages 1617-1620

Gone with the wind: The origin of SO galaxies in clusters

Author keywords

[No Author keywords available]

Indexed keywords

HYDROGEN;

EID: 0034596049     PISSN: 00368075     EISSN: None     Source Type: Journal    
DOI: 10.1126/science.288.5471.1617     Document Type: Article
Times cited : (608)

References (42)
  • 19
    • 4043100253 scopus 로고    scopus 로고
    • V. Quilis, J. Ma. Ibánez, D. Sáez, Astrophys. J. 469, 11 (1996). The numerical code used in this report is a 3D Eulerian code on a fix cartesian grid. This code is based on modern high-resolution shock-capturing (HRSC) techniques, a general denomination for a recently developed family of methods to solve hyperbolic systems of equations such as the hydrodynamic equations. Our code is similar to PPM (piecewise parabolic method) but with some particular features. It has four key ingredients: (i) conservative formulation, numerical quantities are conserved up to the numerical order of the method, (ii) the reconstruction procedure, which allow to recover the distribution of the quantities inside the computational cells, (iii) the Riemann solver, which solves the evolution of discontinuities between cell interfaces, and (iv) the advancing in time, designed to be consistent with the conservation properties. HRSC schemes have the following advantages: (i) they do not suffer from numerical artifacts such as artificial viscosity, (ii) they can resolve strong shocks extremely well, typically in one or two cells, (iii) strong gradients are perfectly modeled, and (iv) they work very well in low-density regions and are high-order in smooth regions of the flow.
    • (1996) Astrophys. J. , vol.469 , pp. 11
    • Quilis, V.1    Ibánez, J.Ma.2    Sáez, D.3
  • 21
    • 0002498980 scopus 로고    scopus 로고
    • and references therein
    • MC's are structures much smaller than the maximum numerical resolution that we can achieve (100 parsecs). Therefore, they cannot be modeled in our simulations as components of the ISM which it is described as exponential disk of cold HI. Nevertheless, we can conclude that MC's are not relevant to the ram-pressure stripping suffered by the HI component due to their small size and high density. Several previous studies, such as A. C. Raga, J. Cantó, S. Curiel, and S. Taylor [Mon. Not. R. Astron. Soc. 295, 738 (1998), and references therein] justify this statement. Raga et al. carried out an analytical and numerical study of the interaction of MC's with winds. If we apply their conclusions to the typical parameters adopted here, the clouds would remain unaltered, that is, MC's do not suffer ram-pressure stripping by the interaction with the ICM. A second possible effect of MC's embedded in the flow is to shield the HI component from the ICM. This effect is also negligible due to the small covering factor of MC's. Their cross sections are < 1% of the area of one of our numerical cells; thus, they would act like single points in a fluid.
    • (1998) Mon. Not. R. Astron. Soc. , vol.295 , pp. 738
    • Raga, A.C.1    Cantó, J.2    Curiel, S.3    Taylor, S.4
  • 22
    • 0343410127 scopus 로고    scopus 로고
    • note
    • α photons.
  • 23
    • 0343410126 scopus 로고    scopus 로고
    • -1, and no holes, are not able to remove the bulk of this material. Simulations with high ICM velocity and density but with a smooth ICM with no holes retain small HI disk with sizes of 3 kpc after 100 My. The more realistic cases including a nonuniform ISM exhibit massive gas losses with almost no HI component remaining after 100 My. Only the strict edge-on cases are weakly affected by the stripping processes, but this configuration for several orbits is expected to be quite rare. Results of one simulation including 10 small holes and inhomogeneous density are shown as mpeg movies at www.sciencemag.org/feature/data/ 1050370.shl.
  • 24
    • 0342974817 scopus 로고    scopus 로고
    • note
    • Ram pressure stripping removes the outer disk gas in a time scale of 20 My. Turbulence and viscous stripping operate over the entire surface of the disk and are effective at removing the diffuse HI even from regions of the disk that are above the threshold for ram pressure effects. These latter processes operate over a longer time scale and are effective at depleting the diffuse HI from the central disk in a time scale of the order of the crossing time for the ICM through the ISM (Fig. 2).
  • 29
    • 0343846064 scopus 로고    scopus 로고
    • note
    • 8 years); (ii) even for galaxies moving with a relative angle of 20° to the ICM, all the gas is stripped (Fig. 1); and (iii) the form of the galactic orbits, typically with pericenters <500 kpc and an average relation apocenter:pericenter approximately 6:1, in clusters and all possible orientations respect the ICM.
  • 32
    • 0342974816 scopus 로고    scopus 로고
    • note
    • Indirect evidence for cluster-galaxy hydrodynamic interactions is frequently observed in head-tail radio galaxies with escaping radio-jets that are stripped backwards by the ICM. This long-lived synchrotron emission may arise within the stripped and subsequently ionized plasma that is in pressure equilibrium with the ICM, supported by the original disk magnetic field that is entangled with the stripped disk material [Web fig. 1 (41)].
  • 37
    • 0000715742 scopus 로고
    • 7 years, then the decline in the molecular gas content of infalling galaxies is as rapid as the rate of HI removal by the stripping process. Initially, this seems at odds with the observations of J. D. P. Kenney and J. S. Young [Astrophys. J. 344, 171 (1989)], who found that bright HI-deficient spirals in the Virgo cluster contained similar masses of molecular H to counterparts of the same morphological type in the field. This apparently suggests that molecular clouds must have a lifetime that is considerably longer than the stripping time scale. However, we note that this comparison is made at a fixed morphology. Morphology is strongly dependent on the star formation rate, in the sense that galaxies with low star formation rate will be classified as earlier type. Thus, it is unlikely that galaxies with similar morphology will exhibit large differences in CO content. Rather, a large deficiency in CO will result in a galaxy with low star formation rate and earlier morphological type. It is then hard to disentangle any deficiency in CO content due to stripping from the reduction in CO content expected for the change in morphological type. It is encouraging, nevertheless, that galaxies of earlier type match more closely the curve in Kenney and Young's data expected if the molecular and atomic gas contents decline at similar rates.
    • (1989) Astrophys. J. , vol.344 , pp. 171
    • Kenney, J.D.P.1    Young, J.S.2
  • 41
    • 0342540537 scopus 로고    scopus 로고
    • Supplementary material is available at www. sciencemag.org/feature/data/1050370.shl.
  • 42
    • 0343410125 scopus 로고    scopus 로고
    • note
    • V.Q. is a Marie Curie research fellow of the European Union (grant HPMF-CT-1999-00052). During the first part of this work, V.Q. was supported by a fellowship of the Spanish SEUID (Ministerio de Educación y Cultura) and partially by Spanish DGES (grant PB96-0797). B.M. is a Royal Society research fellow. Numerical simulations were carried out as part of the Virgo Consortium and the UK Computational Cosmology Consortium.


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