recent progress in modelling of accretion discs in am cvn
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Recent Progress in Modelling of Accretion Discs in AM CVn Stars Thorsten Nagel D.-J. Kusterer, T. Rauch, D. Semionov, K. Werner Institut fr Astronomie und Astrophysik Kepler Center for Astro and Particle Physics Universitt Tbingen Sept.


  1. Recent Progress in Modelling of Accretion Discs in AM CVn Stars Thorsten Nagel D.-J. Kusterer, T. Rauch, D. Semionov, K. Werner Institut für Astronomie und Astrophysik Kepler Center for Astro and Particle Physics Universität Tübingen Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  2. Outline Modelling of NLTE Accretion Discs Model grid for AM CVn systems Model vs. CE 315 Accretion Disc Wind – First Steps Summary Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  3. Modelling of NLTE Accretion Discs Assumptions: geometrically thin α-disc (Shakura & Sunyaev 1973) axial symmetry Divide disc into set of concentric rings Each ring: plane-parallel radiating slab Calculate detailed vertical structure and synthetic spectrum with AcDc (Accretion Disc code, Nagel et al. 2004 ) Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  4. Modelling of Accretion Discs hydrostatic equilibrium (gas and radiation pressure) radiative equilibrium (full line blanketing, no convection) NLTE rate equations radiation transfer eqs. (irradiation by primary can be considered) Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  5. Modelling of Accretion Discs Vertical structure and spectrum for each disc ring Integration of all disc ring intensities, rotational broadening ⇒ NLTE accretion disc spectra for different inclinations disc spectrum can be used as input for our accretion disc wind models Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  6. Modelling of Accretion Discs Input parameters mass and radius of central object mass accretion rate radial extension of accretion disc Reynolds number chemical abundances (→ donor star) irradiation: temperature/spectrum of central object irradiation angle Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  7. Model grid for AM CVn stars mass of primary: 0.6, 0.8, 1.0, 1.2 and 1.4 M ☺ mass accretion rate: 10 -8 , 10 -9 , 10 -10 , 10 -11 M ☺ /yr variation of C, N, O, Si abundances radially extended to the tidal radius (if possible) five inclination angles Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  8. Model grid for AM CVn stars Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  9. Variation of primary mass Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  10. Variation of mass-accretion rate Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  11. Variation of chem. abundances Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  12. Variation of chem. abundances Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  13. Variation of inclination Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  14. Influence of irradiation by primary Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  15. Influence of irradiation by primary Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  16. Spectroscopic detection of primary so far only one directly spectroscopical detection of white dwarf primary (Sion et al. 2006) in which systems should we look, in which wavelength range ? Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  17. Spectroscopic detection of primary Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  18. Models vs. Observation: CE 315 (spectrum by Ruiz et al. 2001) Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  19. Models vs. Observation: CE 315 (spectrum by Ruiz et al. 2001) Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  20. Models vs. Observation: CE 315 Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  21. Accretion Disc Wind P Cygni profile (Wade 2002) Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  22. Accretion Disc Wind WOMPAT: Wind mOdel in Monte carlo Parallel rAdiative Transfer (D. Kusterer 2008, PhD Thesis) parallelized Monte Carlo code LTE occupation numbers iterative solution of temperature and ionisation structure calculated disc spectrum or blackbody as input Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  23. Accretion Disc Wind Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  24. Accretion Disc Wind Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  25. Summary grid of accretion disc models: 0.6 - 1.4 M ☺ 10 -8 - 10 -11 M ☺ /y reproduction of absorption and emission line spectra for high and low state irradiation by the primary seems to have almost no effect onto the spectrum Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

  26. Summary spectroscopic detection of primary best possible in UV indication of underabundance of Si in CE315 (also no Si found in X-ray [Ramsay et al. 2006] and UV [Gänsicke et al. 2003]) Monte Carlo based accretion disc wind Sept. 4th 2008 2 nd Int. Workshop on AM CVn Stars 1 – 5 Sept. 2008 Cape Town, South Africa

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