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A semi-analytic dynamical friction model for cored galaxies
We present a dynamical friction model based on Chandrasekhar's formula that reproduces the fast inspiral and stalling experienced by satellites orbiting galaxies with a large constant density core. We show that the fast inspiral phase does not owe to resonance. Rather, it owes to the background...
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Published in: | Monthly notices of the Royal Astronomical Society 2016-11, Vol.463 (1), p.858-869 |
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container_title | Monthly notices of the Royal Astronomical Society |
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creator | Petts, J. A. Read, J. I. Gualandris, A. |
description | We present a dynamical friction model based on Chandrasekhar's formula that reproduces the fast inspiral and stalling experienced by satellites orbiting galaxies with a large constant density core. We show that the fast inspiral phase does not owe to resonance. Rather, it owes to the background velocity distribution function for the constant density core being dissimilar from the usually assumed Maxwellian distribution. Using the correct background velocity distribution function and our semi-analytic model from previous work, we are able to correctly reproduce the infall rate in both cored and cusped potentials. However, in the case of large cores, our model is no longer able to correctly capture core-stalling. We show that this stalling owes to the tidal radius of the satellite approaching the size of the core. By switching off dynamical friction when r
t(r) = r (where r
t is the tidal radius at the satellite's position), we arrive at a model which reproduces the N-body results remarkably well. Since the tidal radius can be very large for constant density background distributions, our model recovers the result that stalling can occur for M
s/M
enc ≪ 1, where M
s and M
enc are the mass of the satellite and the enclosed galaxy mass, respectively. Finally, we include the contribution to dynamical friction that comes from stars moving faster than the satellite. This next-to-leading order effect becomes the dominant driver of inspiral near the core region, prior to stalling. |
doi_str_mv | 10.1093/mnras/stw2011 |
format | article |
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t(r) = r (where r
t is the tidal radius at the satellite's position), we arrive at a model which reproduces the N-body results remarkably well. Since the tidal radius can be very large for constant density background distributions, our model recovers the result that stalling can occur for M
s/M
enc ≪ 1, where M
s and M
enc are the mass of the satellite and the enclosed galaxy mass, respectively. Finally, we include the contribution to dynamical friction that comes from stars moving faster than the satellite. This next-to-leading order effect becomes the dominant driver of inspiral near the core region, prior to stalling.</description><identifier>ISSN: 0035-8711</identifier><identifier>EISSN: 1365-2966</identifier><identifier>DOI: 10.1093/mnras/stw2011</identifier><language>eng</language><publisher>London: Oxford University Press</publisher><subject>Constants ; Density ; Friction ; Galaxies ; Mathematical models ; Probability distribution ; Satellites ; Stalling ; Stars & galaxies ; Velocity ; Velocity distribution</subject><ispartof>Monthly notices of the Royal Astronomical Society, 2016-11, Vol.463 (1), p.858-869</ispartof><rights>2016 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society 2016</rights><rights>Copyright Oxford University Press, UK Nov 21, 2016</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c364t-6a7525d0017f2d0ab031d609435818f5b68ccc39e94e13fbd6dd97d88197dd963</citedby><cites>FETCH-LOGICAL-c364t-6a7525d0017f2d0ab031d609435818f5b68ccc39e94e13fbd6dd97d88197dd963</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,1598,27901,27902</link.rule.ids><linktorsrc>$$Uhttps://dx.doi.org/10.1093/mnras/stw2011$$EView_record_in_Oxford_University_Press$$FView_record_in_$$GOxford_University_Press</linktorsrc></links><search><creatorcontrib>Petts, J. A.</creatorcontrib><creatorcontrib>Read, J. I.</creatorcontrib><creatorcontrib>Gualandris, A.</creatorcontrib><title>A semi-analytic dynamical friction model for cored galaxies</title><title>Monthly notices of the Royal Astronomical Society</title><description>We present a dynamical friction model based on Chandrasekhar's formula that reproduces the fast inspiral and stalling experienced by satellites orbiting galaxies with a large constant density core. We show that the fast inspiral phase does not owe to resonance. Rather, it owes to the background velocity distribution function for the constant density core being dissimilar from the usually assumed Maxwellian distribution. Using the correct background velocity distribution function and our semi-analytic model from previous work, we are able to correctly reproduce the infall rate in both cored and cusped potentials. However, in the case of large cores, our model is no longer able to correctly capture core-stalling. We show that this stalling owes to the tidal radius of the satellite approaching the size of the core. By switching off dynamical friction when r
t(r) = r (where r
t is the tidal radius at the satellite's position), we arrive at a model which reproduces the N-body results remarkably well. Since the tidal radius can be very large for constant density background distributions, our model recovers the result that stalling can occur for M
s/M
enc ≪ 1, where M
s and M
enc are the mass of the satellite and the enclosed galaxy mass, respectively. Finally, we include the contribution to dynamical friction that comes from stars moving faster than the satellite. This next-to-leading order effect becomes the dominant driver of inspiral near the core region, prior to stalling.</description><subject>Constants</subject><subject>Density</subject><subject>Friction</subject><subject>Galaxies</subject><subject>Mathematical models</subject><subject>Probability distribution</subject><subject>Satellites</subject><subject>Stalling</subject><subject>Stars & galaxies</subject><subject>Velocity</subject><subject>Velocity distribution</subject><issn>0035-8711</issn><issn>1365-2966</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqN0EtLxDAQwPEgCq6rR-8FL16ik6R54WlZfMGCFz2XbJJKlrZZkxbdb2_3AYIXvWQI_BiGP0KXBG4IaHbbdsnk29x_UiDkCE0IExxTLcQxmgAwjpUk5BSd5bwCgJJRMUF3syL7NmDTmWbTB1u4TWfaYE1T1CnYPsSuaKPz4zemwsbkXfFuGvMVfD5HJ7Vpsr84zCl6e7h_nT_hxcvj83y2wJaJssfCSE65AyCypg7MEhhxAnTJuCKq5kuhrLVMe116wuqlE85p6ZQi4-u0YFN0vd-7TvFj8Lmv2pCtbxrT-TjkiijOmdRE639QJhmA1DDSq190FYc0ZtgpqkpJ6VbhvbIp5px8Xa1TaE3aVASqbfVqV706VP85IA7rP-g3BG-CzA</recordid><startdate>20161121</startdate><enddate>20161121</enddate><creator>Petts, J. A.</creator><creator>Read, J. I.</creator><creator>Gualandris, A.</creator><general>Oxford University Press</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7TG</scope><scope>KL.</scope></search><sort><creationdate>20161121</creationdate><title>A semi-analytic dynamical friction model for cored galaxies</title><author>Petts, J. A. ; Read, J. I. ; Gualandris, A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c364t-6a7525d0017f2d0ab031d609435818f5b68ccc39e94e13fbd6dd97d88197dd963</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Constants</topic><topic>Density</topic><topic>Friction</topic><topic>Galaxies</topic><topic>Mathematical models</topic><topic>Probability distribution</topic><topic>Satellites</topic><topic>Stalling</topic><topic>Stars & galaxies</topic><topic>Velocity</topic><topic>Velocity distribution</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Petts, J. A.</creatorcontrib><creatorcontrib>Read, J. I.</creatorcontrib><creatorcontrib>Gualandris, A.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><jtitle>Monthly notices of the Royal Astronomical Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Petts, J. A.</au><au>Read, J. I.</au><au>Gualandris, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A semi-analytic dynamical friction model for cored galaxies</atitle><jtitle>Monthly notices of the Royal Astronomical Society</jtitle><date>2016-11-21</date><risdate>2016</risdate><volume>463</volume><issue>1</issue><spage>858</spage><epage>869</epage><pages>858-869</pages><issn>0035-8711</issn><eissn>1365-2966</eissn><abstract>We present a dynamical friction model based on Chandrasekhar's formula that reproduces the fast inspiral and stalling experienced by satellites orbiting galaxies with a large constant density core. We show that the fast inspiral phase does not owe to resonance. Rather, it owes to the background velocity distribution function for the constant density core being dissimilar from the usually assumed Maxwellian distribution. Using the correct background velocity distribution function and our semi-analytic model from previous work, we are able to correctly reproduce the infall rate in both cored and cusped potentials. However, in the case of large cores, our model is no longer able to correctly capture core-stalling. We show that this stalling owes to the tidal radius of the satellite approaching the size of the core. By switching off dynamical friction when r
t(r) = r (where r
t is the tidal radius at the satellite's position), we arrive at a model which reproduces the N-body results remarkably well. Since the tidal radius can be very large for constant density background distributions, our model recovers the result that stalling can occur for M
s/M
enc ≪ 1, where M
s and M
enc are the mass of the satellite and the enclosed galaxy mass, respectively. Finally, we include the contribution to dynamical friction that comes from stars moving faster than the satellite. This next-to-leading order effect becomes the dominant driver of inspiral near the core region, prior to stalling.</abstract><cop>London</cop><pub>Oxford University Press</pub><doi>10.1093/mnras/stw2011</doi><tpages>12</tpages></addata></record> |
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subjects | Constants Density Friction Galaxies Mathematical models Probability distribution Satellites Stalling Stars & galaxies Velocity Velocity distribution |
title | A semi-analytic dynamical friction model for cored galaxies |
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