2014A&A...571A..95F


Query : 2014A&A...571A..95F

2014A&A...571A..95F - Astronomy and Astrophysics, volume 571A, 95-95 (2014/11-1)

On the probability distribution function of the mass surface density of molecular clouds. II.

FISCHERA J.

Abstract (from CDS):

The probability distribution function (PDF) of the mass surface density of molecular clouds provides essential information about the structure of molecular cloud gas and condensed structures out of which stars may form. In general, the PDF shows two basic components: a broad distribution around the maximum with resemblance to a log-normal function, and a tail at high mass surface densities attributed to turbulence and self-gravity. In a previous paper, the PDF of condensed structures has been analyzed and an analytical formula presented based on a truncated radial density profile, ρ(r)=ρc/(1+(r/r0)2)n/2 with central density ρc and inner radius r0, widely used in astrophysics as a generalization of physical density profiles. In this paper, the results are applied to analyze the PDF of self-gravitating, isothermal, pressurized, spherical (Bonnor-Ebert spheres) and cylindrical condensed structures with emphasis on the dependence of the PDF on the external pressure pext and on the overpressure q–1=pc/pext, where pc is the central pressure. Apart from individual clouds, we also consider ensembles of spheres or cylinders, where effects caused by a variation of pressure ratio, a distribution of condensed cores within a turbulent gas, and (in case of cylinders) a distribution of inclination angles on the mean PDF are analyzed. The probability distribution of pressure ratios q–1 is assumed to be given by P(q–1)∝q–k1/(1+(q0/q)γ)(k1+k2)/γ, where k1, γ, k2, and q0 are fixed parameters. The PDF of individual spheres with overpressures below ∼100 is well represented by the PDF of a sphere with an analytical density profile with n=3. At higher pressure ratios, the PDF at mass surface densities Σ≪Σ(0), where Σ(0) is the central mass surface density, asymptotically approaches the PDF of a sphere with n=2. Consequently, the power-law asymptote at mass surface densities above the peak steepens from Psph(Σ)∝Σ–2 to Psph(Σ)∝Σ–3. The corresponding asymptote of the PDF of cylinders for the large q–1 is approximately given by Pcyl(Σ)∝Σ–4/3/SQRT(1-(Σ/Σ(0))2/3). The distribution of overpressures q–1 produces a power-law asymptote at high mass surface densities given by <Psph(Σ)>∝Σ–2k2–1 (spheres) or <Pcyl(Σ)>∝Σ–2k2 (cylinders).

Abstract Copyright:

Journal keyword(s): ISM: clouds - methods: statistical - ISM: structure - methods: analytical

Simbad objects: 14

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Number of rows : 14
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2021
#notes
1 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1148 0
2 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 3747 0
3 NAME Ori A MoC 05 38 -07.1           ~ 2774 0
4 NAME Ori B MoC 05 41 43.0 -01 54 44           ~ 1225 0
5 NAME Rosette Molecular Cloud MoC 06 34.7 +04 02           ~ 237 0
6 NAME Musca Cld 12 23 -71.3           ~ 170 0
7 NAME Coalsack Nebula DNe 12 31 19 -63 44.6           ~ 247 0
8 NAME Lupus I Cld 15 43 02.1 -34 09 06           ~ 245 0
9 NAME Lupus III SFR 16 09.6 -39 03           ~ 290 0
10 NAME Lupus V MoC 16 21 -37.5           ~ 57 0
11 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3198 1
12 LDN 204 DNe 16 47 47.3 -12 05 16           ~ 52 0
13 LDN 1228 DNe 20 57 13 +77 35.8           ~ 122 0
14 IC 5146 OpC 21 53 24 +47 16.0           ~ 408 2

    Equat.    Gal    SGal    Ecl

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2021.07.30-04:04:23

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