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The Impact of Dust on a Stellar Wind-Blown Bubbles

Ed Churchwell & John Everett University of Wisconsin Oct. 12-15, 2008 Lowell Observatory Flagstaff, AZ. The Impact of Dust on a Stellar Wind-Blown Bubbles. Outline N49-A Stellar Wind-Blown Bubble. Dust observed within this wind-blown bubble MIR/Radio Image

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The Impact of Dust on a Stellar Wind-Blown Bubbles

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  1. Ed Churchwell & John Everett University of Wisconsin Oct. 12-15, 2008 Lowell Observatory Flagstaff, AZ The Impact of Dust on a Stellar Wind-Blown Bubbles

  2. OutlineN49-A Stellar Wind-Blown Bubble • Dust observed within this wind-blown bubble • MIR/Radio Image • 24µm/70µm brightness ratios • Modelling the dust: • Dust properties in wind shocks? • How long does dust survive? • Importance of grains on bubble properties • Summary

  3. N49 4.5(B), 8.0(G), 24(R) µm Image

  4. N49 IR/Radio Image

  5. Image of Wind-Blown Bubbles a la Weaver et al. 1977

  6. Dust models approximately fit the data:24/70µm Brightness Distributions

  7. As a first approximation, we model N49 as a static, uniform-temperature, dusty bubble using Cloudy (Ferland, 1998) and Cloudy_3D (Morisset, 2004). Key parameters for the models are: Dust Model Properties

  8. Can Dust Survive in the Bubble? Dust Properties in Wind-Blown Bubbles • Grain Temperatures • Sputtering Timescales • Grain Residence times • Average Grain Charge • Dust Cooling Fraction

  9. Grain Temperatures: Little Sublimation Graphites slightly warmer than the silicates at same radius and grain size Larger grains cooler than smaller grains at same radius and grain size Decrease in temp with radius only ~20-30%

  10. Sputtering: Very Long Timescales Grains not significantly sputtered in hot, post-shocked wind bubble (Sputtering timescales about same for graphite & silicates.)‏

  11. Wind Drag: Driving Small Grains Out Grains with radii < 0.05 µm are driven out of the wind-blown bubble in less than ~105 years. This shows that the advection of dust due to wind drag is the most important process for dust longevity.

  12. Grain Charge: Grains Help With Cooling High stellar luminosity & low density drives grains to have significant positive charges over most of parameter space.

  13. Dust Cooling Fraction Dust dominates the cooling until Compton cooling becomes important at large luminosities and small densities.

  14. Issues • 24µm emission => Dust exists within HII regions • Dust residence timescales are small relative to the age of bubbles =>Why are grains in HII regions? • Need a continuous source of grains • Perhaps from embedded neutral condensations? • Entrainment of neutral condensations from the PDR of the HII region?

  15. Diagram of a Dusty Wind-Blown Bubble

  16. Summary • Dust Impacts on wind-blown HII regions • Dust is strongly positively charged • Dust dominates cooling • Temperatures lower than in absence of dust • Radii smaller for age and ambient density than expected in absence of dust => age estimates not simply related to size and ambient ISM density • Ionization structure => looks like a cooler central star than the actual star • MIR-FIR brightness much greater than in absence of dust • Theoretically only grains of size ≥ 0.2µm survive long enough to play an important role, however we seem to see grains of all sizes • Kinematic impacts due to dust? • Relative dust drift velocities are fairly large

  17. Comparison:[NeII], [NeIII], PAH(11.3µm)‏

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