{"title":"On the formation of cores in accreting filaments and the impact of ambient environment on it","authors":"S. V. Anathpindika, J. Di Francesco","doi":"arxiv-2409.09431","DOIUrl":null,"url":null,"abstract":"Recent numerical works, including ours, lend credence to the thesis that\nambient environment, i.e., external pressure, affects star-forming ability of\nclouds & filaments. In continuation with our series of papers on the subject we\nexplore this thesis further by developing hydrodynamic simulations of accreting\nfilaments confined by external pressures in the range $10^{4 -7}$ $K\\ cm^{-3}$.\nOur findings are-\\textbf{(i)} irrespective of linemass, filaments fragment to\nyield spheroidal cores. Initially sub-critical filaments in low to intermediate\nexternal pressure environments form broad cores which suggests, weakly\nself-gravitating filaments must fragment via \\emph{collect-and-collapse} mode\nto form broad cores. Transcritical filaments, by contrast, become susceptible\nto Jeans-type instability and form pinched cores; \\textbf{(ii)} ambient\nenvironment bears upon physical properties of filaments including their {\\small\nFWHM$_{fil}$}. Only those initially suffused with subsonic turbulence in Solar\nNeighbourhood-like environs, however, have {\\small FWHM$_{fil}$}$\\sim$ 0.1\n$pc$. In high pressure environs they not only have smaller widths, but become\nseverely eviscerated. On the contrary, filaments suffused with initially\nsupersonic turbulence are typically broader; \\textbf{(iii)} quasi-oscillatory\nnature of velocity gradients is ubiquitous along filament lengths and its\nmagnitude generally increases with increasing pressure. The periodicity of the\nvelocity gradients approximately matches the fragmentation lengthscale of\nfilaments; \\textbf{(iv)} oscillatory features of the radial component of the\nvelocity gradient are a unreliable proxy for detecting signatures of accretion\nonto filaments; \\textbf{(v)} filaments at either extreme of external pressure\nare inefficient at cycling gas into the dense phase which could reconcile the\ncorresponding inefficiency of star-formation in such environments.","PeriodicalId":501187,"journal":{"name":"arXiv - PHYS - Astrophysics of Galaxies","volume":"20 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Astrophysics of Galaxies","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.09431","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Recent numerical works, including ours, lend credence to the thesis that
ambient environment, i.e., external pressure, affects star-forming ability of
clouds & filaments. In continuation with our series of papers on the subject we
explore this thesis further by developing hydrodynamic simulations of accreting
filaments confined by external pressures in the range $10^{4 -7}$ $K\ cm^{-3}$.
Our findings are-\textbf{(i)} irrespective of linemass, filaments fragment to
yield spheroidal cores. Initially sub-critical filaments in low to intermediate
external pressure environments form broad cores which suggests, weakly
self-gravitating filaments must fragment via \emph{collect-and-collapse} mode
to form broad cores. Transcritical filaments, by contrast, become susceptible
to Jeans-type instability and form pinched cores; \textbf{(ii)} ambient
environment bears upon physical properties of filaments including their {\small
FWHM$_{fil}$}. Only those initially suffused with subsonic turbulence in Solar
Neighbourhood-like environs, however, have {\small FWHM$_{fil}$}$\sim$ 0.1
$pc$. In high pressure environs they not only have smaller widths, but become
severely eviscerated. On the contrary, filaments suffused with initially
supersonic turbulence are typically broader; \textbf{(iii)} quasi-oscillatory
nature of velocity gradients is ubiquitous along filament lengths and its
magnitude generally increases with increasing pressure. The periodicity of the
velocity gradients approximately matches the fragmentation lengthscale of
filaments; \textbf{(iv)} oscillatory features of the radial component of the
velocity gradient are a unreliable proxy for detecting signatures of accretion
onto filaments; \textbf{(v)} filaments at either extreme of external pressure
are inefficient at cycling gas into the dense phase which could reconcile the
corresponding inefficiency of star-formation in such environments.