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TINY-SCALE NEUTRAL STRUCTURE Tiny-Scale Atomic Structure (TSAS) –Observations, THEN and NOW –Pressure problem –Interpretive Solutions Tiny-Scale Molecular.

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Presentation on theme: "TINY-SCALE NEUTRAL STRUCTURE Tiny-Scale Atomic Structure (TSAS) –Observations, THEN and NOW –Pressure problem –Interpretive Solutions Tiny-Scale Molecular."— Presentation transcript:

1 TINY-SCALE NEUTRAL STRUCTURE Tiny-Scale Atomic Structure (TSAS) –Observations, THEN and NOW –Pressure problem –Interpretive Solutions Tiny-Scale Molecular Structure (SAMS) –Observations –Interpretative aspects: “Stones”, “Clumpuscules” –The “Missing/Dark Matter”? Carl Heiles, Astronomy, UC Berkeley

2 TSAS OBSERVATIONS THEN – 1990’S

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11 The single descriptive word was... UBIQUITOUS

12 TSAS OBSERVATIONS NOW – 2000’S

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19 (Also: Minter, Balser, Kartalepe 2005; PSR B0329+54)

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21 Today’s picture Pulsar HI absorption spectra is less rosy than yesteryear’s! It indicates that TSAS is NOT SO UBIQUITOUS! HOWEVER... VLBI still shows structure against 3 sources, one of which is both time- and space-variable! OPTICAL ABSORPTION LINES are still going strong (sensitive to ionization fraction)!

22 TSAS --- INTERPRETIVE ISSUES

23 MAX MIN PRESSURE CONSTRAINT/THERMAL EQUILIBRIUM The THERMAL P CNM > MIN (MICROphysics requirement). The Boulares/Cox Hydrostatic Limit is strict for long-lived structures MACROphysics requirement). CONCLUSION: If in equilibrium, the CNM thermal pressure must lie between MIN and Hydrostatic--a range of about 10. (from Wolfire et al 2003) Galactic Hydrostatic Equilibrium Limit

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25 To avoid high TSAS pressure, we want... * Low Temperature * High Anisotropy (High G) High G means L || >> L perp :

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28 IF TSAS IS DISCRETE QUASISTATIC STRUCTURES… T low, ~16 K L ┴ ~30 AU P/k ~ 4000 cm -3 K L || = G L ┴ ~ 190 AU

29 HOW ABOUT G? ARECIBO/GALFA PROVIDES NEW EVIDENCE FOR ANISOTROPY AT LARGER SCALES: * A PANCAKE (sheet) * A CIGAR (filament)

30 Knapp/Verschuur cloud: 17 K; a very thin sheet (0.03 pc).

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33 GALFA data of this 150 sq deg region: Vlsr = 5 to 12 km/s Note the long, straight filaments!

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37 (from Jenkins and Tripp)

38 How about possibilities other than discrete structures in pressure equilibrium? 1. Discrete structures, but highly overpressured (Tripp—stay tuned!) 2. Velocity gradients plus 21-cm line scintillation lead to apparent variations in 21-cm line opacity (Gwinn—not present at this meeting) 3. Simply the random pileup of column density/velocity along the line of sight—will produce observable fluctuations if the turbulent spectrum is flat enough (Deshpande; not present at this meeting).

39 SAMS OBSERVATIONS Heithausen discovered isolated Tiny-Scale MOLECULAR Structures. He christened them... SAMS – Small-Area Molecular Structures

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44 at 100 pc, n(H2) ~ 500000 per cc; R ~ 200 AU; M ~ 100 M(Jup; V_exp ~ 0.3 km/s

45 SAMS OBSERVED PROPERTIES Intrinsic CO linewidth ~ 0.4 km/s Vel gradient ~ 1 km/s over 6000 AU N(H) ~ few x 10 19 (HI? H 2 ? X factor?) Radius ~ few hundred AU n(H) ~ few x 10 4 or more cm -3 At T ~ 10 K, BIG PRESSURE PROBLEM! Mass ~ few x 10 -4 Suns or ~ 1 Jupiter Dense clouds oscillate in Z, period 240 Myr Cloud velocities low (few km/s)

46 THEORETICAL/INTERPRETIVE ISSUES A cloud should “drop like a stone”, oscillate in Galactic z-gravity Period 240 Myr Vz,max = 2.5 km/s for Zmax = 100 pc, commensurate with observed low velocities But this “stone” picture implies a cohesive object. Self-gravity seems the only mechanism!

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48 SUMMARY OF PFENNIGER/COMBES Argue that ISM is hierarchical and fractal Set minimum size by equating cooling time to free-fall time: the “CLUMPUSCULE” Clumpuscule properties are similar to observed molecular clumps!

49 ‘MISSING MATTER” – “DARK MATTER”? Pfenniger/Combes1994: Clumpuscules Walker/Wardle 1998: ISRF ionizes outside of clumpsicules and produces ESE lenses (Ionized Structure: Rickett, stay tuned!) –Ionized clumpsicule covering fraction 0.7% –1000 times more clumpuscules than stars! –Solves “missing/dark matter” problem! Gerhard/Silk 1996 also postulate small molecular clouds—cosmology only.

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51 OVERALL SUMMARY—TSAS * Discrete structures in quasi-equilibriuim—favored by VLBI and my prejudice; needs Low T, High G * Discrete structures, Overpressured >> Galactic hydrostatic pressure. (Tripp) * Multiscale contributions from turbulent spectrum (Deshpande) OVERALL SUMMARY—SAMS * Discrete clumpuscules (Heithausen and Dirsch et al. data, 2002/2004) * If ESE, they are the dark matter (Pfenniger/Combes 1993; Walker/Wardle 1998)!

52 S mall I onized and N eutral S tructures (in the Diffuse ISM) [by Carl Heiles]: SINS V ital I nterstellar R egions: T iny, U nexpected, E xpanding S tructures [by Lou Hobbs]: VIRTUES


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