TY - JOUR
T1 - Instability of supersonic cold streams feeding galaxies - IV. Survival of radiatively cooling streams
AU - Mandelker, Nir
AU - Nagai, Daisuke
AU - Aung, Han
AU - Dekel, Avishai
AU - Birnboim, Yuval
AU - Van Den Bosch, Frank C.
N1 - Publisher Copyright:
© 2020 The Author(s).
PY - 2020
Y1 - 2020
N2 - We study the effects of Kelvin-Helmholtz Instability (KHI) on the cold streams that feed massive haloes at high redshift, generalizing our earlier results to include the effects of radiative cooling and heating from a UV background, using analytic models and high resolution idealized simulations. We currently do not consider self-shielding, thermal conduction, or gravity. A key parameter in determining the fate of the streams is the ratio of the cooling time in the turbulent mixing layer which forms between the stream and the background following the onset of the instability, tcool, mix, to the time in which the mixing layer expands to the width of the stream in the non-radiative case, tshear. This can be converted into a critical stream radius, Rs, crit, such that Rs/Rs,crit = tshear/tcool, mix. If Rs < Rs, crit, the non-linear evolution proceeds similarly to the non-radiative case studied by Mandelker et al. If Rs > Rs,crit, which we find to almost always be the case for astrophysical cold streams, the stream is not disrupted by KHI. Rather, background mass cools and condenses on to the stream, and can increase the mass of cold gas by a factor of ∼3 within 10 stream sound crossing times. The mass entrainment induces thermal energy losses from the background and kinetic energy losses from the stream, which we model analytically. Roughly half of the dissipated energy is radiated away from gas with T < 5 × 104 K, suggesting much of it will be emitted in Ly α.
AB - We study the effects of Kelvin-Helmholtz Instability (KHI) on the cold streams that feed massive haloes at high redshift, generalizing our earlier results to include the effects of radiative cooling and heating from a UV background, using analytic models and high resolution idealized simulations. We currently do not consider self-shielding, thermal conduction, or gravity. A key parameter in determining the fate of the streams is the ratio of the cooling time in the turbulent mixing layer which forms between the stream and the background following the onset of the instability, tcool, mix, to the time in which the mixing layer expands to the width of the stream in the non-radiative case, tshear. This can be converted into a critical stream radius, Rs, crit, such that Rs/Rs,crit = tshear/tcool, mix. If Rs < Rs, crit, the non-linear evolution proceeds similarly to the non-radiative case studied by Mandelker et al. If Rs > Rs,crit, which we find to almost always be the case for astrophysical cold streams, the stream is not disrupted by KHI. Rather, background mass cools and condenses on to the stream, and can increase the mass of cold gas by a factor of ∼3 within 10 stream sound crossing times. The mass entrainment induces thermal energy losses from the background and kinetic energy losses from the stream, which we model analytically. Roughly half of the dissipated energy is radiated away from gas with T < 5 × 104 K, suggesting much of it will be emitted in Ly α.
KW - Galaxies: evolution
KW - Galaxies: formation
KW - Hydrodynamics
KW - Instabilities
UR - http://www.scopus.com/inward/record.url?scp=85098416246&partnerID=8YFLogxK
U2 - 10.1093/MNRAS/STAA812
DO - 10.1093/MNRAS/STAA812
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AN - SCOPUS:85098416246
SN - 0035-8711
VL - 494
SP - 2641
EP - 2663
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 2
ER -