1 / 19

Lecture 10: Bubbles and PNe September 26, 2011

Lecture 10: Bubbles and PNe September 26, 2011. III. Conduction Layer. Probe the thermal conduction layer High ions produced by thermal collisions. O VI N V C IV Si IV. UV Probes of the 10 5 K Gas. C IV N V O VI

adriel
Download Presentation

Lecture 10: Bubbles and PNe September 26, 2011

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Lecture 10:Bubbles and PNeSeptember 26, 2011

  2. III. Conduction Layer • Probe the thermal conduction layer • High ions produced by thermal collisions O VI N V C IV Si IV

  3. UV Probes of the 105 K Gas C IV N V O VI ll (Å)1548, 1550 1238, 1242 1031, 1037 Obs. HST STIS HST STIS FUSE I.P. (eV) 47.9 77.5 138.1 T (K) 1.0105 1.8105 3.0105 Teff (K) >35,000 >75,000 >125,000

  4. Interface of the WR Bubble S308 N V C IV S II Boroson et al. 1997, ApJ, 478, 638

  5. S 308 - ideal for conduction study Boroson et al. (1997) detected N V absorption from the conduction layer. HST STIS observation of N V and C VI emission was scheduled, but STIS died. FUSE observations of O VI were awarded, and it died, too. Spitzer can observe Ne V, but it ran out cryogen. HD 50896 * R: HG: [O III]B: X-ray

  6. FUSE Observations of NGC 6543 Gruendl, Chu, Guerrero 2004, ApJL

  7. III. Conduction Layer • Probe the thermal conduction layer • High ions produced by thermal collisions • NGC 6543: given the boundary conditions • of hot interior and warm shell, thermal • conduction appears to be consistent, but • does not explain the low X-ray luminosity. Gruendl, Chu, Guerrero 2004, ApJL

  8. Stars and Nebulae: Evolving Together Steffen & Schönberner (2006)

  9. Stars and Nebulae: Evolving Together Steffen & Schönberner (2006)

  10. Interacting-Wind Model of PNe

  11. Hot Gas in Planetary Nebulae X-ray emission detected by Chandra & XMM-Newton NGC 2392 NGC 6543 NGC 7026 Guerrero et al. (2005) Chu et al. (2001) Gruendl et al. (2006)

  12. Hot Gas in Planetary Nebulae X-ray emission detected by Chandra & XMM-Newton 2.7x106 K 3.0x106 K 1.7x106 K T = 1-3 x 106 K n  100 cm-3

  13. To Ensure Detection of Diffuse X-rays • Closed shell or lobes to confine hot gas. • Stellar winds – P Cygni profiles • Nearby, no large extinction • OVI, NV lines from interface layer • NGC 246, NGC 3132 - no high ions, no X-rays • High ions and diffuse X-rays from • IC 418, NGC 2392, NGC 6826, NGC 7009

  14. FUSE - Nebular OVIEmission NGC 7293 (Helix) NGC 6543 (Cat’s Eye) Star Inside Nebula O VI 1032 O VI 1037 Ly 1026 Outside Nebula Stellar P Cygni profile fast stellar wind Nebular O VI emission hot gas from shocked wind

  15. O VI of PNe detected in X-rays

  16. O VI of PNe not detected in X-rays

  17. Pressure-driven bubble with heat conduction at interface  Bubble dynamics does not matchLx (obs) / Lx (expected) = 10-1 to 10-3    • Adjust fast wind • wind velocity • mass loss rate Dynamically mix nebular material (mass-loading) Reduce heat conduction

  18. What Next? Swept-up Shell Reasonably well understood Interface (conduction) layer Spatially-resolved high-dispersion UV spectra are needed Hot interior Spatially-resolved high-resolution X-ray spectra are needed

More Related