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Interstellar bubbles. II - Structure and evolution
Abstract
The detailed structure of the interaction of a strong stellar wind with the interstellar medium is presented. First, an adiabatic similarity solution is given which is applicable at early times. Second, a similarity solution is derived which includes the effects of thermal conduction between the hot (about 1 million K) interior and the cold shell of swept-up interstellar matter. This solution is then modified to include the effects of radiative energy losses. The evolution of an interstellar bubble is calculated, including the radiative losses. The quantitative results for the outer-shell radius and velocity and the column density of highly ionized species such as O VI are within a factor 2 of the approximate results of Castor, McCray, and Weaver (1975). The effect of stellar motion on the structure of a bubble, the hydrodynamic stability of the outer shell, and the observable properties of the hot region and the outer shell are discussed.
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“Clearly, the outflow becomes slower quickly in the presence of a CGM over a time scale of ∼ Myr.”
From The Fermi/eROSITA bubbles: a look into the nuclear outflow from the Milky Way (2024) · cites this paper as Weaver et al. 1977
In the citing paper
“The dynamical time-scale of the actual expansion would depend on the speed of the shock driven by this hot gas and can be much lower (Castor et al. 1975; Weaver et al. 1977).”
From The Fermi/eROSITA bubbles: a look into the nuclear outflow from the Milky Way (2024) · cites this paper as Weaver et al. 1977
In the citing paper
“The higher value of σ compared to a blast wave case is due to a higher fraction of thermal energy stored in wind-driven bubbles (Weaver et al. 1977).”
From The Fermi/eROSITA bubbles: a look into the nuclear outflow from the Milky Way (2024) · cites this paper as Weaver et al. 1977
In the citing paper
“Shocks driven by a constant energy source (namely, winds) are also self-similar and can be represented by the equation 10 with the modification Eb = L t , where L is the power of the energy source (Castor et al. 1975; Weaver et al. 1977).”
From The Fermi/eROSITA bubbles: a look into the nuclear outflow from the Milky Way (2024) · cites this paper as Weaver et al. 1977
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On the contribution of charge-exchange induced X-ray emission in the ISM and ICM
Lallement, R. (2004) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20035625 · Cited by 89
“Alternately, the shock may be stronger and the shocked gas fully ionized, but radiative cooling in the dense swept-up shell may cause rapid recombination if the density is high enough (Weaver et al. 1977).”
BackgroundInfluentialMartin, C., & Bouché, N. (2009) · Max Planck Digital Library · Cited by 89
Lynds, R. C., Tolstoy, E., O’Neil, E. J., et al. (1998) · The Astronomical Journal · doi:10.1086/300409 · Cited by 89
Polarized radio filaments outside the Galactic plane
Vidal, M., Dickinson, C., Davies, R. D., & Leahy, J. P. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv1328 · Cited by 88
“This idea has been suggested by a number of authors, (see e.g.Weaver et al. 1977; Heiles et al. 1980).”
ResultProchaska, J. X., Dessauges-Zavadsky, M., Ramirez-Ruiz, E., & Chen, H. (2008) · The Astrophysical Journal · doi:10.1086/590529 · Cited by 87
“…increases gradually, while the wind velocity decreases slightly, which results in an almost constant mechanical luminosity Lw = 1 2 Ṁwv 2 w. (1) This behavior allows us to easily compute the time evolution of the main-sequence bubble using the analytical solutions given by Weaver et al. (1977).”
MethodKinematics of massive star ejecta in the Milky Way as traced by26Al
Kretschmer, K., Diehl, R., Krause, M., Burkert, A. M., Fierlinger, K., Gerhard, O., Greiner, J., & Wang, W. (2013) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201322563 · Cited by 88
“Mostly formed in groups (Lada & Lada 2003), they create superbubbles up to kpc in size (Jaskot et al. 2011; Weaver et al. 1977), and drive large scale outflows (von Glasow et al. 2013).”
BackgroundH I shells in the outer Milky Way
Ehlerová, S., & Palouš, J. (2005) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20034389 · Cited by 87
Izotov, Y. I., Thuan, T. X., & Guseva, N. G. (2007) · The Astrophysical Journal · doi:10.1086/522923 · Cited by 86
“Theoretical studies of the interaction of large OB associations with the interstellar medium (Weaver et al. 1977; McCray & Kafatos 1987; Mac Low & McCray 1988) predict that multiple SN events can create a large and low-density stellar wind bubble which pushes out a supershell of denser ionized…”
BackgroundBLACK HOLE POWERED NEBULAE AND A CASE STUDY OF THE ULTRALUMINOUS X-RAY SOURCE IC 342 X-1
Cseh, D., Corbel, S., Kaaret, P., et al. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/749/1/17 · Cited by 85
“We follow the formalism developed by Weaver et al. (1977) and Ostriker & McKee (1988) describing the hydrodynamic structure of a bubble.”
MethodThe trouble with the Local Bubble
Welsh, B. Y., & Shelton, R. L. (2009) · Astrophysics and Space Science · doi:10.1007/s10509-009-0053-3 · Cited by 85
Shining a light on galactic outflows: photoionized outflows
Chisholm, J., Tremonti, C., Leitherer, C., Chen, Y., & Wofford, A. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw178 · Cited by 84
“…different “scaling relations”, or how the outflow properties (like mass outflow rate and outflow velocity) scale with host galaxy properties (Castor et al. 1975; McKee & Ostriker 1977; Weaver et al. 1977; Ferrara & Tolstoy 2000; Springel & Hernquist 2003; Murray et al. 2005; Hopkins et al. 2012).”
BackgroundExpanding bubbles in Orion A: [C II] observations of M 42, M 43, and NGC 1977
Pabst, C. H. M., Goicoechea, J. R., Teyssier, D., et al. (2020) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202037560 · Cited by 84
“In this depiction, we have calculated the expected kinetic energy of a stellar wind bubble using the analytical model developed by Weaver et al. (1977), Ekin ' 6 11 Lwt, (20) and the pressure-driven expansion of ionized gas (Spitzer 1978), Mshell ' 4π 3 R3S,0µn0 ( 1 + 7t 4ts )12/7 , (21) Ekin ' 1 2…”
BackgroundMethodResultInfluentialA dynamical model of supernova feedback: gas outflows from the interstellar medium
Lagos, C. D. P., Lacey, C., & Baugh, C. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt1696 · Cited by 70
ULTRAFAINT DWARF GALAXIES—THE LOWEST-MASS RELICS FROM BEFORE REIONIZATION
Bland-Hawthorn, J., Sutherland, R. S., & Webster, D. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/807/2/154 · Cited by 83
“The evolutionary phases of an explosive wind are well understood analytically (Weaver et al. 1977), although we see additional substructure due to the complexity of the initial medium.”
BackgroundROSAT and ASCA Observations of W50 Associated with the Peculiar Source SS 433
Safí-Harb, S., & Öğelman, H. (1997) · The Astrophysical Journal · doi:10.1086/304274 · Cited by 83
A binary merger model for the formation of the Supernova 1987A triple-ring nebula
Morris, T., & Podsiadlowski, P. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.15114.x · Cited by 82
“However, the equations of motion can be reduced to a straightforward numerical integration (Weaver et al. 1977) for the density and velocity profile in Region B.”
BackgroundMethodMeyer, D. M.-A., Mackey, J., Langer, N., et al. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu1629 · Cited by 82
“3 of Weaver et al. 1977) and of moving stars (see fig.”
BackgroundInfluentialDISRUPTION OF MOLECULAR CLOUDS BY EXPANSION OF DUSTY H II REGIONS
Kim, J., Kim, W., & Ostriker, E. C. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/819/2/137 · Cited by 82
Pang, X., Li, Y., Yu, Z., Tang, S.-Y., Dinnbier, F., Kroupa, P., Pasquato, M., & Kouwenhoven, M. B. N. (2021) · The Astrophysical Journal · doi:10.3847/1538-4357/abeaac · Cited by 84
“After the first stars have formed, the gas surrounding the OCs is rapidly removed by stellar radiation (Krumholz & Matzner 2009; Dinnbier & Walch 2020), stellar winds (Weaver et al. 1977), or supernovae (McKee & Ostriker 1977).”
BackgroundFormation of 'bullets' by hydrodynamical instabilities in stellar outflows
Stone, J. M., Xu, J., & Mundy, L. G. (1995) · Nature · doi:10.1038/377315a0 · Cited by 81
THE INTERACTION OF THE FERMI BUBBLES WITH THE MILKY WAY’S HOT GAS HALO
Miller, M. J., & Bregman, J. N. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/829/1/9 · Cited by 91
“The Bubbles as a Confined Galactic Wind We treat the bubbles in the framework of a continuous galactic outflow/superbubble with self-similar SedovTaylor solutions (e.g., Castor et al. 1975; Weaver et al. 1977; Mac Low & McCray 1988; Veilleux et al. 2005).”
MethodBlowing in the Milky Way Wind: Neutral Hydrogen Clouds Tracing the Galactic Nuclear Outflow
Di Teodoro, E. M., McClure-Griffiths, N. M., Lockman, F. J., Denbo, S. R., Endsley, R., Ford, H. A., & Harrington, K. (2018) · The Astrophysical Journal · doi:10.3847/1538-4357/aaad6a · Cited by 79
“Under the assumption that 10-20% of the total energy goes into kinetic energy (e.g., Weaver et al. 1977; Walch & Naab 2015), the total kinetic power available is about 3− 6× 1039 erg s−1, a value similar to that found from the Hi clouds.”
BackgroundAGN feedback in dwarf galaxies?
Dashyan, G., Silk, J. I., Mamon, G. A., et al. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx2716 · Cited by 80
“Following an approach similar to MNRAS 000, 1–6 (2017) Weaver et al. (1977) and Koo & McKee (1990), the set of equations giving the radius of the shell and the internal energy of the gas is { d dt (Mshell(R) ÛRR) = 2Eth + Mshell ÛR 2 + Egrav,t , Ein + Egrav,0 = Eth + 1 2 Mshell ÛR2 + Egrav,t ,…”
BackgroundMethodFast and inefficient star formation due to short-lived molecular clouds and rapid feedback
Kruijssen, J. M. D., Schruba, A., Chevance, M., Longmore, S. N., Hygate, A. P. S., Haydon, D. T., McLeod, A. F., Dalcanton, J. J., Tacconi, L. J., & Dishoeck, E. F. (2019) · RePEc: Research Papers in Economics · Cited by 78
The photometric evolution of FU Orionis objects: disc instability and wind-envelope interaction
Clarke, C. J., Lodato, G., Melnikov, S., et al. (2005) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2005.09231.x · Cited by 79
“The evolution of a wind expanding into a quasi-spherical density distribution is initially approximately adiabatic (e.g., Weaver et al. 1977), i.e. the combined thermal energy of the wind blown cavity and the kinetic energy of the swept up shell of shocked medium together increase at a rate set by…”
BackgroundMarcolini, A., Strickland, D., D’Ercole, A., Heckman, T. M., & Hoopes, C. G. (2005) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2005.09343.x · Cited by 79
“…initially low-ionization gas being conductively evaporated, the Ovi column density may be increased by a factor of ∼ 3 from the equilibrium case (Weaver et al. 1977; Indebetouw & Shull 2004), as the region of Ovi ions extends into lower density and kinetically hotter material (the gas is…”
BackgroundMethodInfluentialThe effect of stellar winds on the formation of a protocluster
Dale, J. E., & Bonnell, I. A. (2008) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2008.13802.x · Cited by 79
“Weaver et al. (1977) introduce two zones in this region – an inner shell of hot shocked wind and an outer shell of shocked ISM separated by a contact discontinuity.”
BackgroundRadioactive26Al from the Scorpius-Centaurus association
Diehl, R., Lang, M., Martin, P., Ohlendorf, H., Preibisch, T., Voss, R., Jean, P., Roques, J. P., von Ballmoos, P., & Wang, W. (2010) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201014302 · Cited by 79
“Stellar winds and explosions are expected to create interacting gas shells (Weaver et al. 1977), merging of hot cavities may form superbubbles (Tenorio-Tagle & Bodenheimer 1988; Mac Low & McCray 1988; Cho & Kang 2008).”
BackgroundConstraints on gamma-ray burst and supernova progenitors through circumstellar absorption lines
van Marle, A. J., Langer, N., & García-Segura, G. (2005) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20053520 · Cited by 78
“In principle, the evolution of main sequence and WolfRayet bubbles are influenced – although weakly – by various stellar and interstellar medium parameters (Weaver et al. 1977).”
BackgroundMethodwarpfield 2.0: feedback-regulated minimum star formation efficiencies of giant molecular clouds
Rahner, D., Pellegrini, E. W., Glover, S. C. O., et al. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty3295 · Cited by 77
“More details are provided in Weaver et al. (1977).”
BackgroundInfluentialWind bubbles within H ii regions around slowly moving stars
Mackey, J., Gvaramadze, V. V., Mohamed, S., et al. (2014) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201424716 · Cited by 77
“Both Weaver et al. (1977) and Capriotti & Kozminski (2001) derive criteria determining when a wind bubble can trap the H ii region, finding that strong winds (i.e. high mass stars) in dense gas are the most favourable scenario.”
BackgroundInfluentialForming a constant density medium close to long gamma-ray bursts
van Marle, A. J., Langer, N., Achterberg, A., et al. (2006) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20065709 · Cited by 77
“The mechanical luminosity of the star, Lw = 1 2 Ṁw V 2 w, (2) is a measure of the mechanical energy that the star puts into the CSM.”
BackgroundMethodInfluentialHow multiple supernovae overlap to form superbubbles
Yadav, N., Mukherjee, D., Sharma, P., & Nath, B. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw2522 · Cited by 49
“The superbubble pressure as a function of time, according to the adiabatic model of Weaver et al. (1977), is ∼ 34ρ3 2 sb, which at the end of cluster lifetime becomes psb, late kB ∼ 1.7 × 105 K cm−3N2/5OB,4η 2/5 mech,−2τ −6/5 OB,30n 3/5 g0,1, (20) where mechanical efficiency has been scaled to 0.01.”
BackgroundMethodInfluentialRadiatively Driven Winds and the Shaping of Bipolar Luminous Blue Variable Nebulae
Dwarkadas, V. V., & Owocki, S. P. (2002) · The Astrophysical Journal · doi:10.1086/344257 · Cited by 77
“This situation is quite different from the Weaver et al. (1977) model, which applies to a nebula that has already settled into an energyconserving stage, with a strong reverse shock heating a bubble of high pressure that drives an outward expansion of a thin shell of swept-up ambient material.”
BackgroundThe low rate of Galactic pevatrons
Cristofari, P., Blasi, P., & Amato, E. (2020) · Astroparticle Physics · doi:10.1016/j.astropartphys.2020.102492 · Cited by 76
Interaction of a Pulsar Wind with the Expanding Supernova Remnant
Jun, B. I. (1997) · CERN Document Server (European Organization for Nuclear Research) · Cited by 76
REGULATION OF BLACK HOLE WINDS AND JETS ACROSS THE MASS SCALE
King, A. L., Miller, J. M., Raymond, J., et al. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/762/2/103 · Cited by 75
“Instead, if we combine the intensity measurements of Russell et al. (2007) with the shock wave models of Raymond et al. (1988) and the theory of interstellar bubbles blown by a continuous energy input (Castor et al. 1975; Weaver et al. 1977), we can get a tighter constraint on the power estimate.”
BackgroundInfluentialMcLeod, A. F., Dale, J. E., Evans, C. J., et al. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2696 · Cited by 75
“6), indicating that these are consistent with the standard bubble model (Weaver et al. 1977).”
ResultRadio lobes and X-ray hotspots in the microquasar S26
Soria, R., Pakull, M. W., Broderick, J. W., et al. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.17360.x · Cited by 75
“However, the mass of X-ray-emitting gas is an order of magnitude less than the total mass of the swept-up interstellar medium, that is, the swept-up shell is not significantly depleted by evaporation into the hot region, in agreement with the self-similar approximation of Weaver et al. (1977).”
Background3D simulations of Betelgeuse’s bow shock
Mohamed, S., Mackey, J., & Langer, N. (2012) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201118002 · Cited by 75
“For stationary stars, the wind-ISM interface is expected to be a spherical shell as shown, for example, by the analytic and hydrodynamic models of Weaver et al. (1977) and GarciaSegura et al. (1996), respectively.”
MethodStewart, S. G., Fanelli, M. N., Byrd, G. G., et al. (2000) · The Astrophysical Journal · doi:10.1086/308241 · Cited by 75
“…acts on only one side of a molecular cloud where as large-scale triggering describes the process by which a centralized source destroys the remainder of its parental molecular cloud, creating a void in the gas and a dense ridge of swept up material carried to large distances (Weaver et al. 1977).”
BackgroundPlanetary Nebulae: Sources of Enlightenment
Kwitter, K., & Henry, R. (2021) · Publications of the Astronomical Society of the Pacific · doi:10.1088/1538-3873/ac32b1 · Cited by 51
Landecker, T. L., Reich, W., Reid, R. I., Reich, P., Wolleben, M., Kothes, R., Uyanıker, B., Gray, A. D., Rizzo, D. D., Fürst, E., et al. (2010) · Astronomy and Astrophysics · doi:10.1051/0004-6361/200913921 · Cited by 74
THE EMISSION-LINE SPECTRA OF MAJOR MERGERS: EVIDENCE FOR SHOCKED OUTFLOWS
Soto, K. T., Martin, C. L., Prescott, M. K. M., & Armus, L. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/757/1/86 · Cited by 81
“The simplest model for the initial response of the interstellar gas to this feedback is based on stellar wind bubbles (Weaver et al. 1977; Shull & McKee 1979).”
Supernova Blast Waves in Low‐Density Hot Media: A Mechanism for Spatially Distributed Heating
Tang, S., & Wang, Q. D. (2005) · The Astrophysical Journal · doi:10.1086/430875 · Cited by 74
“After a couple of 106 years, fast stellar winds start to play a major role in heating and shaping the medium, creating a low-density hot bubble (Weaver et al. 1977), probably even before the explosion of the first SN in the association.”
BackgroundBroten, N. W., MacLeod, J. M., & Vallée, J. P. (1988) · Astrophysics and Space Science · doi:10.1007/bf00639497 · Cited by 74
The Fine–Scale Structure of the neutral Interstellar Medium in nearby GalaxiesPreprint
Bagetakos, I., Brinks, E., Walter, F., de Blok, W. J. G., Usero, A., Leroy, A. K., Rich, J. W., & Kennicutt, R. C. (2011) · Cited by 72
Supernova blast waves in wind-blown bubbles, turbulent, and power-law ambient media
Haid, S., Walch, S., Naab, T., Seifried, D., Mackey, J., & Gatto, A. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw1082 · Cited by 71
“The expansion radius r s,B of a wind-blown bubble from a constant stellar wind without heat transfer is given by (Weaver et al. 1977; Pittard 2013) r s,B(t) = ( 125 154π )1/5 ( Lω ρ 0,uni )1/5 t3/5 (22) where ρ 0,uni is the density of the initial homogeneous ambient medium with µ = 1.”
BackgroundInfluentialDwarkadas, V. V. (2004) · CERN Document Server (European Organization for Nuclear Research) · Cited by 72
SpitzerIRS Observations of the Galactic Center: Shocked Gas in the Radio Arc Bubble
Simpson, J. P., Colgan, S. W. J., Cotera, A. S., Erickson, E. F., Hollenbach, D. J., Kaufman, M. J., & Rubin, R. H. (2007) · The Astrophysical Journal · doi:10.1086/522295 · Cited by 69
The many sides of RCW 86: a Type Ia supernova remnant evolving in its progenitor's wind bubble
Broersen, S., Chiotellis, A., Vink, J., et al. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu667 · Cited by 71
“7 of Weaver et al. (1977).”
Star formation efficiency as a function of metallicity: from star clusters to galaxies
Dib, S., Piau, L., Mohanty, S., & Braine, J. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.18966.x · Cited by 72
“…bubbles which take into account the interaction of the expanding bubble with a surrounding confining medium were developed by Castor et al. (1975), Weaver et al. (1977), Shull (1980), Koo & McKee (1992a,b) and Cantó et al. (2000), and recently included in global molecular cloud simulations by…”
BackgroundUnusual CO Line Ratios and Kinematics in the N83/N84 Region of the Small Magellanic Cloud
Bolatto, A. D., Leroy, A. K., Israel, F. P., et al. (2003) · The Astrophysical Journal · doi:10.1086/377230 · Cited by 71
“From the interstellar bubble model of Weaver et al. (1977), we find that the age, t, of the bubble is related to its radius, Rs, in parsecs and its expansion velocity, Vs, in km s 1 by t ¼ 6 105Rs=Vs.”
BackgroundFujita, A., Martin, C., MacLow, M. M., et al. (2002) · CERN Document Server (European Organization for Nuclear Research) · Cited by 71
ATOMIC HYDROGEN IN A GALACTIC CENTER OUTFLOW
McClure-Griffiths, N. M., Green, J. A., Hill, A. S., Lockman, F. J., Dickey, J. M., Gaensler, B. M., & Green, A. J. (2013) · The Astrophysical Journal · doi:10.1088/2041-8205/770/1/l4 · Cited by 70
“Assuming the ratio of ratio of kinetic energy of the H i clouds to the total input wind energy is ∼ 0.2 (Weaver et al. 1977), as often assumed for superbubbles, the required wind energy input was ∼ 8 × 1052 ergs over the past 106 yrs.”
InfluentialExpanding bubbles in Orion A: [CII] observations of M 42, M 43, and NGC 1977
Pabst, C. H. M., Goicoechea, J. R., Teyssier, D., et al. (2020) · Kölner Universitäts PublikationsServer (Universität zu Köln) · Cited by 70
Interstellar Medium Abundances in the Pegasus Dwarf Irregular Galaxy
Skillman, E. D., Bomans, D. J., & Kobulnicky, H. A. (1997) · The Astrophysical Journal · doi:10.1086/303464 · Cited by 70
Spatially Resolved Observations of the Galactic Center Source IRS 21
Tanner, A. M., Ghez, A. M., Morris, M., Becklin, E. E., Cotera, A. S., Ressler, M. E., Werner, M. W., & Wizinowich, P. L. (2002) · The Astrophysical Journal · doi:10.1086/341470 · Cited by 66
“…mass-loss rate in units of 10 6 M yr 1, vw is the stellar wind velocity in units of 108 cm s 1, v is the motion of the star through the Northern Arm in units of 106 cm s 1, lH is the mean molecular weight, and nH is the gas density of the Northern Arm in units of cm s 1 (Weaver et al. 1977).”
BackgroundRamirez‐Ruiz, E., Garcia‐Segura, G., Salmonson, J. D., & Perez‐Rendon, B. (2005) · The Astrophysical Journal · doi:10.1086/432433 · Cited by 68
Multiwavelength features of Fermi bubbles as signatures of a Galactic wind
Sarkar, K. C., Nath, B., & Sharma, P. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv1806 · Cited by 56
“The snapshot clearly shows the structure of a standard stellar wind scenario (Weaver et al. 1977).”
BackgroundChandraobservation of NGC 4449: analysis of the X-ray emission from a dwarf starburst galaxy
Summers, L. K., Stevens, I. R., Strickland, D., et al. (2003) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2003.06590.x · Cited by 69
“The less intense bulging of the emission seen to the ESE and WNW could be indicative of a bipolar outflow along the minor axis of the galaxy as would be expected from standard superbubble models (Weaver et al. 1977).”
BackgroundMethodSupernova 1996cr: SN 1987A’s Wild Cousin?
Bauer, F. E., Dwarkadas, V. V., Brandt, W. N., et al. (2008) · The Astrophysical Journal · doi:10.1086/589761 · Cited by 68
“Such transitions typically lead to the formationof a wind-blown bubble (e.g., Weaver et al. 1977; Garcia-Segura et al. 1996a,b), and numerous researchers have explored the subsequent interaction between the complex CSM associated with a bubble and the SN blast wave (e.g., Chevalier & Liang 1989;…”
BackgroundMethodTHE ORIGIN AND KINEMATICS OF COLD GAS IN GALACTIC WINDS: INSIGHT FROM NUMERICAL SIMULATIONS
Fujita, A., Martin, C. L., Low, M. M., et al. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/698/1/693 · Cited by 68
“Weaver et al. (1977) argued that the density in the hot interior of bubbles in uniform gas is dominated by conductive evaporation from the dense shell.”
BackgroundInfluentialSelf-citationSequential explosions of supernovae in an ob association and formation of a superbubble
Tomisaka, K., Habe, A., & Ikeuchi, S. (1981) · Astrophysics and Space Science · doi:10.1007/bf00648941 · Cited by 68
Cosmic ray production in superbubbles
Vieu, T., Gabici, S., Tatischeff, V., et al. (2022) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stac543 · Cited by 67
Search for OB stars running away from young star clusters
Gvaramadze, V. V., Kniazev, A. Y., Kroupa, P., et al. (2011) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201117746 · Cited by 67
“One can, therefore, expect to find some of the runaways via detection of their associated bow shocks – the natural attributes of supersonically moving stars (Baranov et al. 1971; Weaver et al. 1977).”
BackgroundThe H i Kinematics and Distribution of Four Blue Compact Dwarf Galaxies
Thuan, T. X., Hibbard, J. E., & Levrier, F. (2004) · The Astronomical Journal · doi:10.1086/422431 · Cited by 67
“According to Weaver et al. (1977), in the standard superbubble model, the time evolution of the radius of the dense shell of swept-up ambient material is given by R ¼ (65:9 pc)L0:238 n 0:20 t0:66 , where L38 is the mechanical luminosity injected by the starburst in units of 1038 ergs s 1, n0 is the…”
Bipolar outflows and the evolution of stars
Frank, A. (1999) · New Astronomy Reviews · doi:10.1016/s1387-6473(99)00005-6 · Cited by 67
“In what follows I borrow liberally from a number of excellent treatments of spherical WBB theory (Pikel’ner 1968, Dyson & de Vries 1972, Weaver et al. 1977, Kwok et al. 1978, Dyson & Williams 1981, Kahn 1983, Koo & McKee 1992) When a stellar wind “turns on” it initially expands ballistically until…”
BackgroundWhich feedback mechanisms dominate in the high-pressure environment of the central molecular zone?
Barnes, A. T., Longmore, S. N., Dale, J. E., Krumholz, M. R., Kruijssen, J. M. D., & Bigiel, F. (2020) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/staa2719 · Cited by 67
“For the Weaver et al. (1977) solution, we use wind luminosities of Lwind = 10 L , 100 L and 4000 L , which cover the measured range within G0.”
BackgroundMethodInfluentialSpatially resolved Spitzer-IRS spectral maps of the superwind in M82
Beirão, P., Armus, L., Lehnert, M. D., et al. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv1101 · Cited by 66
“As it expands, it sweeps up and shocks ambient material, creating an outflowing “superwind” (Castor et al. 1975; Weaver et al. 1977).”
BackgroundYeh, S., & Matzner, C. D. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/757/2/108 · Cited by 66
“Indeed, Ugeom can easily be computed from the self-similar solutions of Koo & McKee (1992): using L = (1 + β)Sēi and evaluating for the case of a steady wind in a uniform medium (Weaver et al. 1977), Ugeom = 2Uem = 2.2kBTi 3(1 + β)ēi ṘIF fwvw .”
BackgroundMethodInterpreting the star formation efficiency of nearby molecular clouds with ionizing radiation
Geen, S., Soler, J. D., & Hennebelle, P. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx1765 · Cited by 66
Stellar population of the superbubble N 206 in the LMC
Ramachandran, V., Hamann, W. ‐., Hainich, R., et al. (2018) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201832816 · Cited by 66
The Stellar Population and Star Clusters in the Unusual Local Group Galaxy IC 10
Hunter, D. A. (2001) · The Astrophysical Journal · doi:10.1086/322399 · Cited by 66
“If the ambient gas density9A.7, is 1 cm~3, a single massive star could easily blow a holen0this size in a few Myr (Weaver et al. 1977 ; McCray & Kafatos 1987), so there is no problem producing this shell with stars in clusters 4-2 or 4-1.”
BackgroundNESTED SHELLS REVEAL THE REJUVENATION OF THE ORION–ERIDANUS SUPERBUBBLE
Ochsendorf, B. B., Brown, A. G. A., Bally, J., & Tielens, A. G. G. M. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/808/2/111 · Cited by 65
“In the classical picture of an expanding superbubble, a dense, neutral shell will wrap around the 104 K region created by the reverse shock traced by bright Hα emission (Weaver et al. 1977).”
BackgroundInfluentialEverett, J. E., & Churchwell, E. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/713/1/592 · Cited by 65
“One can see that (as in Weaver et al. 1977), the luminosity increases with time, in contrast to the model with dust cooling presented in Figure 12.”
BackgroundMethodResultInfluentialAnalysis and Modeling of the Multi-wavelength Observations of the Luminous GRB 190114C
Fraija, N. I., Dichiara, S., Pedreira, A. C. C. D. E. S., Galván-Gaméz, A., Becerra, R. L., Duran, R. B., & Zhang, B. (2019) · The Astrophysical Journal Letters · doi:10.3847/2041-8213/ab2ae4 · Cited by 65
“Therefore, a transition phase between the stratified to uniform medium is expected at a distance larger than & 10−2 pc (Weaver et al. 1977; Castor et al. 1975; Fryer et al. 2006).”
BackgroundCosmological Feedback from High‐Redshift Dwarf Galaxies
Fujita, A., Low, M. M., Ferrara, A., et al. (2004) · The Astrophysical Journal · doi:10.1086/422861 · Cited by 65
“…is tc = 3kTs/4n0Λ(Ts), with postshock electron number density 4n0 and shocked temperature Ts = (3µs/16k)v 2 shock, where µs is the mass per particle in the ionized ISM, and vshock is shock velocity given by a similarity solution of a bubble in a uniform density medium n0 by Weaver et al. (1977).”
BackgroundMethodInfluentialMolecular Hydrogen in the Direction of ζ Orionis A
Jenkins, E. B., & Peimbert, A. (1997) · The Astrophysical Journal · doi:10.1086/303694 · Cited by 65
Hydrodynamical simulations of Galactic fountains – I. Evolution of single fountains
Melioli, C., Brighenti, F., D’Ercole, A., & Pino, E. M. D. G. D. (2008) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2008.13446.x · Cited by 64
Wind bubbles within H ii regions around slowly moving starsPreprint
Mackey, J., Gvaramadze, V. V., Mohamed, S., et al. (2014) · Cited by 64
FEEDBACK: a SOFIA Legacy Program to Study Stellar Feedback in Regions of Massive Star Formation
Schneider, N., Simon, R., Guevara, C., et al. (2020) · Publications of the Astronomical Society of the Pacific · doi:10.1088/1538-3873/aba840 · Cited by 63
“The resulting overpressure of this plasma leads to the formation of dense swept-up shells on the surfaces of surrounding clouds (Weaver et al. 1977).”
BackgroundBarnes, A. T., Watkins, E. J., Meidt, S. E., et al. (2023) · The Astrophysical Journal Letters · doi:10.3847/2041-8213/aca7b9 · Cited by 63
“According to the classical Weaver et al. (1977) model of expanding bubbles, v R t0.”
X-Shooting ULLYSES: Massive stars at low metallicity
Vink, J. S., Mehner, A., Crowther, P. A., et al. (2023) · Astronomy and Astrophysics · doi:10.1051/0004-6361/202245650 · Cited by 63
Zhou, P., & Vink, J. (2017) · Astronomy & Astrophysics · doi:10.1051/0004-6361/201731583 · Cited by 47
“In particular, massive stars are known to create large wind-blown bubbles of several tens of parsecs in size (Weaver et al. 1977; Chevalier 1999).”
BackgroundA Morphological Diagnostic for Dynamical Evolution of Wolf-Rayet Bubbles
Gruendl, R. A., Chu, Y., Dunne, B. C., et al. (2000) · The Astronomical Journal · doi:10.1086/316830 · Cited by 63
“…of morphology observed in WR rings, analytic models and numerical simulations have been put forward for windblown bubbles in di†erent media : in a homogeneous ISM (e.g., Weaver et al. 1977), in a cloudy ISM (McKee, van Buren, & Lazare† 1984), and in a circumstellar medium & Mac Low 1995a, 1995b).”
BackgroundApellániz, J. M., Pérez, E., & Más-Hesse, J. M. (2004) · The Astronomical Journal · doi:10.1086/422925 · Cited by 63
“As a matter of fact, any of the four cavities in NGC 604 could have been created by the kinetic energy released into their surroundings by only one or a few massive stars (as opposed to the 200 here) in a period of 3 Myr if Weaver et al. (1977) models were applicable here.”
BackgroundKimura, S. S., Murase, K., & Bartos, I. (2021) · The Astrophysical Journal · doi:10.3847/1538-4357/ac0535 · Cited by 62
Dwarkadas, V. V. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.18001.x · Cited by 62
“The fast wind sweeps the ambient medium or slower wind into a dense shell, whose density can be extremely high if the wind shock is radiative (see Figure 1), and the swept-up mass collapses into a very thin dense shell bordered by a radiative shock (Weaver et al. 1977; Dwarkadas 2005).”
Background(周平), P. Z., (陳陽), Y. C., (張智昱), Z.-Y. Z., et al. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/826/1/34 · Cited by 62
“16 in Weaver et al. 1977), which could be consistent with the suggestion that the SNR is evolving in a uniform medium (Badenes et al. 2007; Yamaguchi et al. 2014).”
BackgroundResultInfluentialAccretion of pristine gas and dilution during the formation of multiple-population globular clusters
D’Ercole, A., D'Antona, F. A., & Vesperini, E. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw1583 · Cited by 62
“Before describing the interaction of the GC wind with the surrounding medium, we briefly summarize the evolution of a “standard” spherical bubble, that is, a bubble powered by a constant luminosity wind and expanding through a local uniform gas (Weaver et al. 1977).”
BackgroundInfluentialWeisz, D. R., Skillman, E. D., Cannon, J. M., Dolphin, A. E., Kennicutt, R. C., Lee, J. C., & Walter, F. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/704/2/1538 · Cited by 61
“The origin of these ISM features has long been attributed to stellar feedback from massive stars, i.e., stellar winds and Type II supernovae (SNe; Weaver et al. 1977; Cash et al. 1980; McCray & Kafatos 1987; Tenorio-Tagle & Bodenheimer 1988, and references therein).”
Dynamical Evolution and Ionization Structure of an Expanding Superbubble: Application to W4
Basu, S., Johnstone, D., & Martin, P. G. (1999) · The Astrophysical Journal · doi:10.1086/307125 · Cited by 62
“The Interior TemperatureThe bubble temperature Tb is obtained from the model of Weaver et al. (1977).”
BackgroundMethodInfluentialGamma‐Ray Burst Afterglows in Pulsar‐Wind Bubbles
Königl, A., & Granot, J. (2002) · The Astrophysical Journal · doi:10.1086/340941 · Cited by 62
“This effect, which has been considered in the study of interstellar bubbles (e.g., Weaver et al. 1977), would be strongly suppressed if the magnetic field were strictly transverse to the flow direction, as is assumed in our model.”
BackgroundTHE ASTROSPHERE OF THE ASYMPTOTIC GIANT BRANCH STAR IRC+10216
Sahai, R., & Chronopoulos, C. (2010) · The Astrophysical Journal Letters · doi:10.1088/2041-8205/711/2/l53 · Cited by 61
“Furthermore, once a complete balance has been established between the ram pressures of the stellar wind and the ISM, the leading edge of the astropause remains a fixed distance ahead of the moving star (Weaver et al. 1977).”
BackgroundMethodHot Gas in the Circumstellar Bubble S308
Chu, Y., Guerrero, M. A., Gruendl, R. A., et al. (2003) · The Astrophysical Journal · doi:10.1086/379607 · Cited by 61
“In the bubble model of Weaver et al. (1977), the fast stellar wind encounters an inner, stagnation shock and the shocked stellar wind provides the thermal pressure to drive the expansion of the nebular shell.”
BackgroundMethodInfluentialAmbient Interstellar Pressure and Superbubble Evolution
Oey, M. S., & Garcı́a-Segura, G. (2004) · The Astrophysical Journal · doi:10.1086/421483 · Cited by 61
“The model predicts that the interior pressure evolves as (e.g., Weaver et al. 1977), Pi/k = 1.83 × 10 5 L 2/5 38 n 3/5t −4/5 6 cm −3 K .”
BackgroundMethodInfluentialFraija, N. I., Vereš, P., Zhang, B., Duran, R. B., Becerra, R. L., Zhang, B., Lee, W. H., Watson, A. M., Ordaz-Salazar, C., & Galván-Gaméz, A. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa8a72 · Cited by 62
“The dynamics of the wind-to-ISM transition phase was originally introduced by Weaver et al. (1977) and Castor et al. (1975).”
BackgroundTriggered Star Formation inside the Shell of a Wolf–Rayet Bubble as the Origin of the Solar System
Dwarkadas, V. V., Dauphas, N., Meyer, B. S., et al. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa992e · Cited by 60
HS 0837+4717 – a metal-deficient blue compact galaxy with large nitrogen excess
Pustilnik, S., Kniazev, A., Pramskij, A., et al. (2004) · Astronomy and Astrophysics · doi:10.1051/0004-6361:20035646 · Cited by 60
“The latter is tdyn = 0.6 Rshell/Vshell=13.7 Myr (Weaver et al. 1977).”
BackgroundInfluential
Metadata
- Authors
- Weaver, R., McCray, R., Castor, J., Shapiro, P., & Moore, R.
- Venue
- The Astrophysical Journal
- Publisher
- American Astronomical Society
- Published
- 1977-12
- Volume
- 218
- Pages
- 377
- ISSN
- 0004-637X (ISSN-L)
- 1538-4357
- OpenAlex
- W2089390834
- Cited by
- 1,736
- References
- 0
- Citations by year
- 2026: 49 · 2025: 74 · 2024: 77 · 2023: 70 · 2022: 81 · 2021: 73 · 2020: 67 · 2019: 58 · 2018: 69 · 2017: 52 · 2016: 68 · 2015: 47 · 2014: 76 · 2013: 70 · 2012: 64
- FWCI
- 11.64
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- The Astrophysical Journal (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Astrophysics and Star Formation Studies
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Stellar, planetary, and galactic studies
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Astrophysics and Cosmic Phenomena
- Keywords
- interstellar bubbles, stellar winds, interstellar medium, heat conduction, radiative losses, hot interstellar gas, stellar kinematics, hydrodynamic stability
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