1991
DOI: 10.1093/mnras/250.2.278
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Spiral modes driven by narrow features in angular-momentum density

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Cited by 105 publications
(144 citation statements)
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“…In the above models, the evolution of the spiral arms is governed by the winding of the arms, which leads to breaks and bifurcations of the spiral arms. Sellwood & Lin (1989) and Sellwood & Kahn (1991) instead argued that the dynamics originate from multiple wave modes of Figure 10. Evolution of spiral arm on α −δ plane for T rot = 12.0 − 12.5.…”
Section: Swing Amplified Spiralsmentioning
confidence: 99%
“…In the above models, the evolution of the spiral arms is governed by the winding of the arms, which leads to breaks and bifurcations of the spiral arms. Sellwood & Lin (1989) and Sellwood & Kahn (1991) instead argued that the dynamics originate from multiple wave modes of Figure 10. Evolution of spiral arm on α −δ plane for T rot = 12.0 − 12.5.…”
Section: Swing Amplified Spiralsmentioning
confidence: 99%
“…The RWI (Lovelace et al 1999;Li et al 2000Li et al , 2001 has been studied and discussed in various situations of differentially rotating discs, from galactic discs (Lovelace & Hohlfeld 1978;Sellwood & Kahn 1991) to microquasar and protoplanetary discs (Papaloizou & Pringle 1985;Lovelace et al 1999). It can be seen as the form that the Kelvin-Helmholtz instability takes in differentially rotating discs, and has a similar instability criterion: it requires an extremum in a vorticity-related quantity, defined in a non-magnetised thin disc as (Li et al 2000)…”
Section: Rossby Wave Instabilitymentioning
confidence: 99%
“…Only a small bump or depression in L(r) leads to the growth of a global disc mode (Sellwood 2013). When the self-gravity of the disc is strong, the RWI is observed to occur at radii where L is a minimum rather than a maximum (Sellwood and Kahn 1991;Sellwood 2012Sellwood , 2013 as predicted by Lovelace and Hohlfeld (1978).…”
Section: Vortices In Self-graviating Discsmentioning
confidence: 87%
“…For disc galaxies L → σΩ/κ 2 (Lovelace and Hohlfeld 1978), where κ is the radial epicyclic angular frequency given below equation 3. The RWI in disc galaxies consisting predominanly of stars has been observed and studied in many different cases using N −body simulations (Sellwood and Kahn 1991;Sellwood 2012;Sellwood 2013). Only a small bump or depression in L(r) leads to the growth of a global disc mode (Sellwood 2013).…”
Section: Vortices In Self-graviating Discsmentioning
confidence: 99%